diff --git a/.gitignore b/.gitignore index f4532824a..959717130 100644 --- a/.gitignore +++ b/.gitignore @@ -26,6 +26,7 @@ examples/python/**/*.xml docs/build docs/source/_images/*.pdf docs/source/_images/*.aux +docs/source/pythonapi/generated/ # Source build build diff --git a/.travis.yml b/.travis.yml index b406a1013..6aed183a0 100644 --- a/.travis.yml +++ b/.travis.yml @@ -27,7 +27,7 @@ before_install: - conda config --set always_yes yes --set changeps1 no - conda update -q conda - conda info -a - - conda create -q -n test-environment python=$TRAVIS_PYTHON_VERSION numpy scipy h5py pandas + - conda create -q -n test-environment python=$TRAVIS_PYTHON_VERSION numpy scipy h5py=2.5 pandas - source activate test-environment # Install GCC, MPICH, HDF5, PHDF5 @@ -44,10 +44,10 @@ before_script: - git clone --branch=master git://github.com/bhermanmit/nndc_xs nndc_xs - cat nndc_xs/nndc.tar.gza* | tar xzvf - - rm -rf nndc_xs - - export CROSS_SECTIONS=$PWD/nndc/cross_sections.xml - - wget http://web.mit.edu/smharper/Public/multipole_lib.tar.gz - - tar -xzf multipole_lib.tar.gz - - export MULTIPOLE_LIBRARY=$PWD/multipole_lib + - export OPENMC_CROSS_SECTIONS=$PWD/nndc/cross_sections.xml + - git clone --branch=master git://github.com/smharper/windowed_multipole_library.git wmp_lib + - tar xzvf wmp_lib/multipole_lib.tar.gz + - export OPENMC_MULTIPOLE_LIBRARY=$PWD/multipole_lib - cd .. script: diff --git a/data/get_multipole_data.py b/data/get_multipole_data.py index cb87865a8..b5126bc0a 100755 --- a/data/get_multipole_data.py +++ b/data/get_multipole_data.py @@ -23,13 +23,13 @@ except ImportError: cwd = os.getcwd() sys.path.insert(0, os.path.join(cwd, '..')) -baseUrl = 'http://web.mit.edu/smharper/Public/' -files = ['multipole_lib.tar.gz'] +baseUrl = 'https://github.com/smharper/windowed_multipole_library/blob/master/' +files = ['multipole_lib.tar.gz?raw=true'] checksums = ['9f0307132fe5beca78b8fc7a01fb401c'] block_size = 16384 # ============================================================================== -# DOWNLOAD FILES FROM ATHENA LOCKER +# DOWNLOAD FILES FROM GITHUB REPO filesComplete = [] for f in files: @@ -44,23 +44,26 @@ for f in files: file_size = req.length downloaded = 0 + # Remove GitHub junk from the file name. + fname = f[:-9] if f.endswith('?raw=true') else f + # Check if file already downloaded - if os.path.exists(f): - if os.path.getsize(f) == file_size: - print('Skipping ' + f) - filesComplete.append(f) + if os.path.exists(fname): + if os.path.getsize(fname) == file_size: + print('Skipping ' + fname) + filesComplete.append(fname) continue else: if sys.version_info[0] < 3: - overwrite = raw_input('Overwrite {0}? ([y]/n) '.format(f)) + overwrite = raw_input('Overwrite {0}? ([y]/n) '.format(fname)) else: - overwrite = input('Overwrite {0}? ([y]/n) '.format(f)) + overwrite = input('Overwrite {0}? ([y]/n) '.format(fname)) if overwrite.lower().startswith('n'): continue # Copy file to disk print('Downloading {0}... '.format(f), end='') - with open(f, 'wb') as fh: + with open(fname, 'wb') as fh: while True: chunk = req.read(block_size) if not chunk: break @@ -69,14 +72,15 @@ for f in files: status = '{0:10} [{1:3.2f}%]'.format(downloaded, downloaded * 100. / file_size) print(status + chr(8)*len(status), end='') print('') - filesComplete.append(f) + filesComplete.append(fname) # ============================================================================== # VERIFY MD5 CHECKSUMS print('Verifying MD5 checksums...') for f, checksum in zip(files, checksums): - downloadsum = hashlib.md5(open(f, 'rb').read()).hexdigest() + fname = f[:-9] if f.endswith('?raw=true') else f + downloadsum = hashlib.md5(open(fname, 'rb').read()).hexdigest() if downloadsum != checksum: raise IOError("MD5 checksum for {} does not match. If this is your first " "time receiving this message, please re-run the script. " @@ -87,12 +91,13 @@ for f, checksum in zip(files, checksums): # EXTRACT FILES FROM TGZ for f in files: - if not f in filesComplete: + fname = f[:-9] if f.endswith('?raw=true') else f + if not fname in filesComplete: continue # Extract files - with tarfile.open(f, 'r') as tgz: - print('Extracting {0}...'.format(f)) + with tarfile.open(fname, 'r') as tgz: + print('Extracting {0}...'.format(fname)) tgz.extractall(path='wmp/') # Move data files down one level diff --git a/docs/source/_templates/myclass.rst b/docs/source/_templates/myclass.rst new file mode 100644 index 000000000..a0560f93a --- /dev/null +++ b/docs/source/_templates/myclass.rst @@ -0,0 +1,7 @@ +{{ fullname }} +{{ underline }} + +.. currentmodule:: {{ module }} + +.. autoclass:: {{ objname }} + :members: diff --git a/docs/source/conf.py b/docs/source/conf.py index 6ca551a43..38661cdb3 100644 --- a/docs/source/conf.py +++ b/docs/source/conf.py @@ -24,13 +24,8 @@ except ImportError: from mock import Mock as MagicMock -class Mock(MagicMock): - @classmethod - def __getattr__(cls, name): - return Mock() - MOCK_MODULES = ['numpy', 'h5py', 'pandas', 'opencg'] -sys.modules.update((mod_name, Mock()) for mod_name in MOCK_MODULES) +sys.modules.update((mod_name, MagicMock()) for mod_name in MOCK_MODULES) # If extensions (or modules to document with autodoc) are in another directory, @@ -48,6 +43,8 @@ extensions = ['sphinx.ext.autodoc', 'sphinx.ext.napoleon', 'sphinx.ext.mathjax', 'sphinx.ext.autosummary', + 'sphinx.ext.intersphinx', + 'sphinx.ext.viewcode', 'sphinx_numfig', 'notebook_sphinxext'] @@ -65,7 +62,7 @@ master_doc = 'index' # General information about the project. project = u'OpenMC' -copyright = u'2011-2015, Massachusetts Institute of Technology' +copyright = u'2011-2016, Massachusetts Institute of Technology' # The version info for the project you're documenting, acts as replacement for # |version| and |release|, also used in various other places throughout the @@ -122,20 +119,13 @@ pygments_style = 'tango' # -- Options for HTML output --------------------------------------------------- -# The theme to use for HTML and HTML Help pages. Major themes that come with -# Sphinx are currently 'default' and 'sphinxdoc'. -if on_rtd: - html_theme = 'default' - html_logo = '_images/openmc200px.png' -else: - html_theme = 'haiku' - html_theme_options = {'full_logo': True, - 'linkcolor': '#0c3762', - 'visitedlinkcolor': '#0c3762'} - html_logo = '_images/openmc.png' +# The theme to use for HTML and HTML Help pages +if not on_rtd: + import sphinx_rtd_theme + html_theme = 'sphinx_rtd_theme' + html_theme_path = [sphinx_rtd_theme.get_html_theme_path()] -# Add any paths that contain custom themes here, relative to this directory. -#html_theme_path = ["_theme"] +html_logo = '_images/openmc200px.png' # The name for this set of Sphinx documents. If None, it defaults to # " v documentation". @@ -248,4 +238,12 @@ latex_elements = { #Autodocumentation Flags #autodoc_member_order = "groupwise" #autoclass_content = "both" -#autosummary_generate = [] +autosummary_generate = True + +napoleon_use_ivar = True + +intersphinx_mapping = { + 'python': ('https://docs.python.org/3', None), + 'numpy': ('http://docs.scipy.org/doc/numpy/', None), + 'pandas': ('http://pandas.pydata.org/pandas-docs/stable/', None) +} diff --git a/docs/source/index.rst b/docs/source/index.rst index 8dba92016..54ba825e5 100644 --- a/docs/source/index.rst +++ b/docs/source/index.rst @@ -4,9 +4,10 @@ The OpenMC Monte Carlo Code OpenMC is a Monte Carlo particle transport simulation code focused on neutron criticality calculations. It is capable of simulating 3D models based on -constructive solid geometry with second-order surfaces. The particle interaction -data is based on ACE format cross sections, also used in the MCNP and Serpent -Monte Carlo codes. +constructive solid geometry with second-order surfaces. OpenMC supports either +continuous-energy or multi-group transport. The continuous-energy +particle interaction data is based on ACE format cross sections, also used +in the MCNP and Serpent Monte Carlo codes. OpenMC was originally developed by members of the `Computational Reactor Physics Group`_ at the `Massachusetts Institute of Technology`_ starting diff --git a/docs/source/methods/cross_sections.rst b/docs/source/methods/cross_sections.rst index 5126252cd..50a97d575 100644 --- a/docs/source/methods/cross_sections.rst +++ b/docs/source/methods/cross_sections.rst @@ -63,6 +63,79 @@ Other Methods A good survey of other energy grid techniques, including unionized energy grids, can be found in a paper by Leppanen_. +--------------------------------- +Windowed Multipole Representation +--------------------------------- + +In addition to the usual pointwise representation of cross sections, OpenMC +offers support for an experimental data format called windowed multipole (WMP). +This data format requires less memory than pointwise cross sections, and it +allows on-the-fly Doppler broadening to arbitrary temperature. + +The multipole method was introduced by [Hwang]_ and the faster windowed +multipole method by [Josey]_. In the multipole format, cross section resonances +are represented by poles, :math:`p_j`, and residues, :math:`r_j`, in the complex +plane. The 0K cross sections in the resolved resonance region can be computed +by summing up a contribution from each pole: + +.. math:: + \sigma(E, T=0\text{K}) = \frac{1}{E} \sum_j \text{Re} \left[ + \frac{i r_j}{\sqrt{E} - p_j} \right] + +Assuming free-gas thermal motion, cross sections in the multipole form can be +analytically Doppler broadened to give the form: + +.. math:: + \sigma(E, T) = \frac{1}{2 E \sqrt{\xi}} \sum_j \text{Re} \left[i r_j + \sqrt{\pi} W_i(z) - \frac{r_j}{\sqrt{\pi}} C \left(\frac{p_j}{\sqrt{\xi}}, + \frac{u}{2 \sqrt{\xi}}\right)\right] +.. math:: + W_i(z) = \frac{i}{\pi} \int_{-\infty}^\infty dt \frac{e^{-t^2}}{z - t} +.. math:: + C \left(\frac{p_j}{\sqrt{\xi}},\frac{u}{2 \sqrt{\xi}}\right) = + 2p_j \int_0^\infty du' \frac{e^{-(u + u')^2/4\xi}}{p_j^2 - u'^2} +.. math:: + z = \frac{\sqrt{E} - p_j}{2 \sqrt{\xi}} +.. math:: + \xi = \frac{k_B T}{4 A} +.. math:: + u = \sqrt{E} + +where :math:`T` is the temperature of the resonant scatterer, :math:`k_B` is the +Boltzmann constant, :math:`A` is the mass of the target nucleus. For +:math:`E \gg k_b T/A`, the :math:`C` integral is approximately zero, simplifying +the cross section to: + +.. math:: + \sigma(E, T) = \frac{1}{2 E \sqrt{\xi}} \sum_j \text{Re} \left[i r_j + \sqrt{\pi} W_i(z)\right] + +The :math:`W_i` integral simplifies down to an analytic form. We define the +Faddeeva function, :math:`W` as: + +.. math:: + W(z) = e^{-z^2} \text{Erfc}(-iz) + +Through this, the integral transforms as follows: + +.. math:: + \text{Im} (z) > 0 : W_i(z) = W(z) +.. math:: + \text{Im} (z) < 0 : W_i(z) = -W(z^*)^* + +There are freely available algorithms_ to evaluate the Faddeeva function. For +many nuclides, the Faddeeva function needs to be evaluated thousands of times to +calculate a cross section. To mitigate that computational cost, the WMP method +only evaluates poles within a certain energy "window" around the incident +neutron energy and accounts for the effect of resonances outside that window +with a polynomial fit. This polynomial fit is then broadened exactly. This +exact broadening can make up for the removal of the :math:`C` integral, as +typically at low energies, only curve fits are used. + +Note that the implementation of WMP in OpenMC currently assumes that inelastic +scattering does not occur in the resolved resonance region. This is usually, +but not always the case. Future library versions may eliminate this issue. + .. only:: html .. rubric:: References @@ -70,8 +143,17 @@ can be found in a paper by Leppanen_. .. [Brown] Forrest B. Brown, "New Hash-based Energy Lookup Algorithm for Monte Carlo codes," LA-UR-14-24530, Los Alamos National Laboratory (2014). +.. [Hwang] R. N. Hwang, "A Rigorous Pole Representation of Multilevel Cross + Sections and Its Practical Application," *Nucl. Sci. Eng.*, **96**, + 192-209 (1987). + +.. [Josey] Colin Josey, Pablo Ducru, Benoit Forget, and Kord Smith, "Windowed + Multipole for Cross Section Doppler Broadening," *J. Comp. Phys*, + **307**, 715-727 (2016). http://dx.doi.org/10.1016/j.jcp.2015.08.013 + .. _MCNP: http://mcnp.lanl.gov .. _Serpent: http://montecarlo.vtt.fi .. _NJOY: http://t2.lanl.gov/codes.shtml .. _ENDF/B data: http://www.nndc.bnl.gov/endf .. _Leppanen: http://dx.doi.org/10.1016/j.anucene.2009.03.019 +.. _algorithms: http://ab-initio.mit.edu/wiki/index.php/Faddeeva_Package diff --git a/docs/source/methods/geometry.rst b/docs/source/methods/geometry.rst index c1be68f72..f642cca10 100644 --- a/docs/source/methods/geometry.rst +++ b/docs/source/methods/geometry.rst @@ -84,10 +84,10 @@ to fully define the surface. | Plane perpendicular | x-plane | :math:`x - x_0 = 0` | :math:`x_0` | | to :math:`x`-axis | | | | +----------------------+------------+------------------------------+-------------------------+ - | Plane perpendicular | y-plane | :math:`x - x_0 = 0` | :math:`y_0` | + | Plane perpendicular | y-plane | :math:`y - y_0 = 0` | :math:`y_0` | | to :math:`y`-axis | | | | +----------------------+------------+------------------------------+-------------------------+ - | Plane perpendicular | z-plane | :math:`x - x_0 = 0` | :math:`z_0` | + | Plane perpendicular | z-plane | :math:`z - z_0 = 0` | :math:`z_0` | | to :math:`z`-axis | | | | +----------------------+------------+------------------------------+-------------------------+ | Arbitrary plane | plane | :math:`Ax + By + Cz = D` | :math:`A\;B\;C\;D` | diff --git a/docs/source/pythonapi/ace.rst b/docs/source/pythonapi/ace.rst deleted file mode 100644 index 4810ec4bb..000000000 --- a/docs/source/pythonapi/ace.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_ace: - -========== -ACE Format -========== - -.. automodule:: openmc.ace - :members: diff --git a/docs/source/pythonapi/cmfd.rst b/docs/source/pythonapi/cmfd.rst deleted file mode 100644 index 51470069f..000000000 --- a/docs/source/pythonapi/cmfd.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_cmfd: - -==== -CMFD -==== - -.. automodule:: openmc.cmfd - :members: diff --git a/docs/source/pythonapi/element.rst b/docs/source/pythonapi/element.rst deleted file mode 100644 index 473cbba45..000000000 --- a/docs/source/pythonapi/element.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_element: - -======= -Element -======= - -.. automodule:: openmc.element - :members: diff --git a/docs/source/pythonapi/energy_groups.rst b/docs/source/pythonapi/energy_groups.rst deleted file mode 100644 index 28ca6f3fe..000000000 --- a/docs/source/pythonapi/energy_groups.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_energy_groups: - -============= -Energy Groups -============= - -.. automodule:: openmc.mgxs.groups - :members: diff --git a/docs/source/pythonapi/examples/mgxs-part-i.ipynb b/docs/source/pythonapi/examples/mgxs-part-i.ipynb index 94deeec7b..de66cbb83 100644 --- a/docs/source/pythonapi/examples/mgxs-part-i.ipynb +++ b/docs/source/pythonapi/examples/mgxs-part-i.ipynb @@ -141,15 +141,12 @@ }, "outputs": [], "source": [ + "%matplotlib inline\n", "import numpy as np\n", "import matplotlib.pyplot as plt\n", "\n", "import openmc\n", - "import openmc.mgxs as mgxs\n", - "from openmc.source import Source\n", - "from openmc.stats import Box\n", - "\n", - "%matplotlib inline" + "import openmc.mgxs as mgxs" ] }, { @@ -341,10 +338,12 @@ "settings_file.batches = batches\n", "settings_file.inactive = inactive\n", "settings_file.particles = particles\n", - "settings_file.output = {'tallies': True, 'summary': True}\n", + "settings_file.output = {'tallies': True}\n", + "\n", + "# Create an initial uniform spatial source distribution over fissionable zones\n", "bounds = [-0.63, -0.63, -0.63, 0.63, 0.63, 0.63]\n", - "settings_file.source = Source(space=Box(\n", - " bounds[:3], bounds[3:], only_fissionable=True))\n", + "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n", + "settings_file.source = openmc.source.Source(space=uniform_dist)\n", "\n", "# Export to \"settings.xml\"\n", "settings_file.export_to_xml()" @@ -423,22 +422,24 @@ "data": { "text/plain": [ "OrderedDict([('flux', Tally\n", - " \tID =\t10000\n", - " \tName =\t\n", - " \tFilters =\t\n", - " \t\tcell\t[1]\n", - " \t\tenergy\t[ 0.00000000e+00 6.25000000e-07 2.00000000e+01]\n", - " \tNuclides =\ttotal \n", - " \tScores =\t['flux']\n", - " \tEstimator =\ttracklength), ('absorption', Tally\n", - " \tID =\t10001\n", - " \tName =\t\n", - " \tFilters =\t\n", - " \t\tcell\t[1]\n", - " \t\tenergy\t[ 0.00000000e+00 6.25000000e-07 2.00000000e+01]\n", - " \tNuclides =\ttotal \n", - " \tScores =\t['absorption']\n", - " \tEstimator =\ttracklength)])" + "\tID =\t10000\n", + "\tName =\t\n", + "\tFilters =\t\n", + " \t\tcell\t[1]\n", + " \t\tenergy\t[ 0.00000000e+00 6.25000000e-07 2.00000000e+01]\n", + "\tNuclides =\ttotal \n", + "\tScores =\t['flux']\n", + "\tEstimator =\ttracklength\n", + "), ('absorption', Tally\n", + "\tID =\t10001\n", + "\tName =\t\n", + "\tFilters =\t\n", + " \t\tcell\t[1]\n", + " \t\tenergy\t[ 0.00000000e+00 6.25000000e-07 2.00000000e+01]\n", + "\tNuclides =\ttotal \n", + "\tScores =\t['absorption']\n", + "\tEstimator =\ttracklength\n", + ")])" ] }, "execution_count": 13, @@ -518,8 +519,9 @@ " Copyright: 2011-2015 Massachusetts Institute of Technology\n", " License: http://mit-crpg.github.io/openmc/license.html\n", " Version: 0.7.1\n", - " Git SHA1: ea9fb637f63f9374c7436456141afa850b84acf9\n", - " Date/Time: 2016-01-14 07:16:05\n", + " Git SHA1: eeb5091ca3a34cc85df73a3318cae2b6c7097413\n", + " Date/Time: 2016-04-13 11:24:09\n", + " MPI Processes: 1\n", "\n", " ===========================================================================\n", " ========================> INITIALIZATION <=========================\n", @@ -545,56 +547,56 @@ "\n", " Bat./Gen. k Average k \n", " ========= ======== ==================== \n", - " 1/1 1.19804 \n", - " 2/1 1.12945 \n", - " 3/1 1.15573 \n", - " 4/1 1.13929 \n", - " 5/1 1.16300 \n", - " 6/1 1.22117 \n", - " 7/1 1.19012 \n", - " 8/1 1.11299 \n", - " 9/1 1.16066 \n", - " 10/1 1.12566 \n", - " 11/1 1.20854 \n", - " 12/1 1.14691 1.17773 +/- 0.03082\n", - " 13/1 1.17204 1.17583 +/- 0.01789\n", - " 14/1 1.14148 1.16724 +/- 0.01529\n", - " 15/1 1.17272 1.16834 +/- 0.01189\n", - " 16/1 1.18575 1.17124 +/- 0.01014\n", - " 17/1 1.20498 1.17606 +/- 0.00983\n", - " 18/1 1.14754 1.17249 +/- 0.00923\n", - " 19/1 1.18141 1.17348 +/- 0.00820\n", - " 20/1 1.15074 1.17121 +/- 0.00768\n", - " 21/1 1.15914 1.17011 +/- 0.00703\n", - " 22/1 1.14586 1.16809 +/- 0.00673\n", - " 23/1 1.18999 1.16978 +/- 0.00642\n", - " 24/1 1.15101 1.16844 +/- 0.00609\n", - " 25/1 1.13791 1.16640 +/- 0.00602\n", - " 26/1 1.19791 1.16837 +/- 0.00597\n", - " 27/1 1.19818 1.17012 +/- 0.00587\n", - " 28/1 1.14160 1.16854 +/- 0.00576\n", - " 29/1 1.11487 1.16571 +/- 0.00614\n", - " 30/1 1.17538 1.16620 +/- 0.00584\n", - " 31/1 1.20210 1.16791 +/- 0.00581\n", - " 32/1 1.20078 1.16940 +/- 0.00574\n", - " 33/1 1.14624 1.16839 +/- 0.00558\n", - " 34/1 1.14618 1.16747 +/- 0.00542\n", - " 35/1 1.16866 1.16752 +/- 0.00520\n", - " 36/1 1.18565 1.16821 +/- 0.00504\n", - " 37/1 1.16824 1.16821 +/- 0.00485\n", - " 38/1 1.18299 1.16874 +/- 0.00471\n", - " 39/1 1.21418 1.17031 +/- 0.00480\n", - " 40/1 1.11167 1.16835 +/- 0.00504\n", - " 41/1 1.11545 1.16665 +/- 0.00516\n", - " 42/1 1.11114 1.16491 +/- 0.00529\n", - " 43/1 1.14227 1.16423 +/- 0.00517\n", - " 44/1 1.14104 1.16355 +/- 0.00506\n", - " 45/1 1.16756 1.16366 +/- 0.00492\n", - " 46/1 1.13065 1.16274 +/- 0.00487\n", - " 47/1 1.11251 1.16139 +/- 0.00492\n", - " 48/1 1.14731 1.16101 +/- 0.00481\n", - " 49/1 1.16691 1.16117 +/- 0.00469\n", - " 50/1 1.19679 1.16206 +/- 0.00465\n", + " 1/1 1.11184 \n", + " 2/1 1.15820 \n", + " 3/1 1.18468 \n", + " 4/1 1.17492 \n", + " 5/1 1.19645 \n", + " 6/1 1.18436 \n", + " 7/1 1.14070 \n", + " 8/1 1.15150 \n", + " 9/1 1.19202 \n", + " 10/1 1.17677 \n", + " 11/1 1.20272 \n", + " 12/1 1.21366 1.20819 +/- 0.00547\n", + " 13/1 1.15906 1.19181 +/- 0.01668\n", + " 14/1 1.14687 1.18058 +/- 0.01629\n", + " 15/1 1.14570 1.17360 +/- 0.01442\n", + " 16/1 1.13480 1.16713 +/- 0.01343\n", + " 17/1 1.17680 1.16852 +/- 0.01144\n", + " 18/1 1.16866 1.16853 +/- 0.00990\n", + " 19/1 1.19253 1.17120 +/- 0.00913\n", + " 20/1 1.18124 1.17220 +/- 0.00823\n", + " 21/1 1.19206 1.17401 +/- 0.00766\n", + " 22/1 1.17681 1.17424 +/- 0.00700\n", + " 23/1 1.17634 1.17440 +/- 0.00644\n", + " 24/1 1.13659 1.17170 +/- 0.00654\n", + " 25/1 1.17144 1.17169 +/- 0.00609\n", + " 26/1 1.20649 1.17386 +/- 0.00610\n", + " 27/1 1.11238 1.17024 +/- 0.00678\n", + " 28/1 1.18911 1.17129 +/- 0.00647\n", + " 29/1 1.14681 1.17000 +/- 0.00626\n", + " 30/1 1.12152 1.16758 +/- 0.00641\n", + " 31/1 1.12729 1.16566 +/- 0.00639\n", + " 32/1 1.15399 1.16513 +/- 0.00612\n", + " 33/1 1.13547 1.16384 +/- 0.00599\n", + " 34/1 1.17723 1.16440 +/- 0.00576\n", + " 35/1 1.09296 1.16154 +/- 0.00622\n", + " 36/1 1.19621 1.16287 +/- 0.00612\n", + " 37/1 1.12560 1.16149 +/- 0.00605\n", + " 38/1 1.17872 1.16211 +/- 0.00586\n", + " 39/1 1.17721 1.16263 +/- 0.00568\n", + " 40/1 1.13724 1.16178 +/- 0.00555\n", + " 41/1 1.18526 1.16254 +/- 0.00542\n", + " 42/1 1.13779 1.16177 +/- 0.00531\n", + " 43/1 1.15066 1.16143 +/- 0.00516\n", + " 44/1 1.12174 1.16026 +/- 0.00514\n", + " 45/1 1.17479 1.16068 +/- 0.00501\n", + " 46/1 1.14146 1.16014 +/- 0.00489\n", + " 47/1 1.20464 1.16135 +/- 0.00491\n", + " 48/1 1.15119 1.16108 +/- 0.00479\n", + " 49/1 1.17938 1.16155 +/- 0.00468\n", + " 50/1 1.15798 1.16146 +/- 0.00457\n", " Creating state point statepoint.50.h5...\n", "\n", " ===========================================================================\n", @@ -604,27 +606,27 @@ "\n", " =======================> TIMING STATISTICS <=======================\n", "\n", - " Total time for initialization = 1.1720E+00 seconds\n", - " Reading cross sections = 9.0300E-01 seconds\n", - " Total time in simulation = 1.7319E+01 seconds\n", - " Time in transport only = 1.7310E+01 seconds\n", - " Time in inactive batches = 1.9120E+00 seconds\n", - " Time in active batches = 1.5407E+01 seconds\n", - " Time synchronizing fission bank = 2.0000E-03 seconds\n", - " Sampling source sites = 2.0000E-03 seconds\n", - " SEND/RECV source sites = 0.0000E+00 seconds\n", + " Total time for initialization = 4.6300E-01 seconds\n", + " Reading cross sections = 1.2100E-01 seconds\n", + " Total time in simulation = 1.6504E+01 seconds\n", + " Time in transport only = 1.6479E+01 seconds\n", + " Time in inactive batches = 1.9620E+00 seconds\n", + " Time in active batches = 1.4542E+01 seconds\n", + " Time synchronizing fission bank = 1.0000E-02 seconds\n", + " Sampling source sites = 4.0000E-03 seconds\n", + " SEND/RECV source sites = 3.0000E-03 seconds\n", " Time accumulating tallies = 0.0000E+00 seconds\n", - " Total time for finalization = 1.0000E-03 seconds\n", - " Total time elapsed = 1.8507E+01 seconds\n", - " Calculation Rate (inactive) = 13075.3 neutrons/second\n", - " Calculation Rate (active) = 6490.56 neutrons/second\n", + " Total time for finalization = 0.0000E+00 seconds\n", + " Total time elapsed = 1.6977E+01 seconds\n", + " Calculation Rate (inactive) = 12742.1 neutrons/second\n", + " Calculation Rate (active) = 6876.63 neutrons/second\n", "\n", " ============================> RESULTS <============================\n", "\n", - " k-effective (Collision) = 1.16131 +/- 0.00453\n", - " k-effective (Track-length) = 1.16206 +/- 0.00465\n", - " k-effective (Absorption) = 1.16096 +/- 0.00364\n", - " Combined k-effective = 1.16120 +/- 0.00325\n", + " k-effective (Collision) = 1.15984 +/- 0.00411\n", + " k-effective (Track-length) = 1.16146 +/- 0.00457\n", + " k-effective (Absorption) = 1.16177 +/- 0.00380\n", + " Combined k-effective = 1.16105 +/- 0.00364\n", " Leakage Fraction = 0.00000 +/- 0.00000\n", "\n" ] @@ -750,8 +752,8 @@ "\tDomain Type =\tcell\n", "\tDomain ID =\t1\n", "\tCross Sections [cm^-1]:\n", - " Group 1 [6.25e-07 - 20.0 MeV]:\t6.81e-01 +/- 1.88e-01%\n", - " Group 2 [0.0 - 6.25e-07 MeV]:\t1.40e+00 +/- 5.91e-01%\n", + " Group 1 [6.25e-07 - 20.0 MeV]:\t6.81e-01 +/- 2.69e-01%\n", + " Group 2 [0.0 - 6.25e-07 MeV]:\t1.40e+00 +/- 5.93e-01%\n", "\n", "\n", "\n" @@ -779,7 +781,7 @@ { "data": { "text/html": [ - "
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" ], "text/plain": [ - " cell energy [MeV] nuclide \\\n", - "0 1 (0.0e+00 - 6.3e-07) total \n", - "1 1 (6.3e-07 - 2.0e+01) total \n", + " cell energy low [MeV] energy high [MeV] nuclide \\\n", + "0 1 0.00e+00 6.25e-07 total \n", + "1 1 6.25e-07 2.00e+01 total \n", "\n", - " score mean std. dev. \n", - "0 (((absorption / flux) / (total / flux)) + ((sc... 1 0.007741 \n", - "1 (((absorption / flux) / (total / flux)) + ((sc... 1 0.002619 " + " score mean std. dev. \n", + "0 (((absorption / flux) / (total / flux)) + ((sc... 1.00e+00 7.76e-03 \n", + "1 (((absorption / flux) / (total / flux)) + ((sc... 1.00e+00 3.74e-03 " ] }, "execution_count": 26, @@ -1187,7 +1201,7 @@ "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython2", - "version": "2.7.10" + "version": "2.7.6" } }, "nbformat": 4, diff --git a/docs/source/pythonapi/examples/mgxs-part-ii.ipynb b/docs/source/pythonapi/examples/mgxs-part-ii.ipynb index 593d53647..6ed5cd38d 100644 --- a/docs/source/pythonapi/examples/mgxs-part-ii.ipynb +++ b/docs/source/pythonapi/examples/mgxs-part-ii.ipynb @@ -34,14 +34,16 @@ "name": "stderr", "output_type": "stream", "text": [ - "/usr/lib/pymodules/python2.7/matplotlib/__init__.py:1173: UserWarning: This call to matplotlib.use() has no effect\n", + "/usr/local/lib/python2.7/dist-packages/matplotlib-1.5.1+1178.ga40c9ec-py2.7-linux-x86_64.egg/matplotlib/__init__.py:884: UserWarning: axes.color_cycle is deprecated and replaced with axes.prop_cycle; please use the latter.\n", + " warnings.warn(self.msg_depr % (key, alt_key))\n", + "/usr/local/lib/python2.7/dist-packages/matplotlib-1.5.1+1178.ga40c9ec-py2.7-linux-x86_64.egg/matplotlib/__init__.py:1362: UserWarning: This call to matplotlib.use() has no effect\n", "because the backend has already been chosen;\n", "matplotlib.use() must be called *before* pylab, matplotlib.pyplot,\n", "or matplotlib.backends is imported for the first time.\n", "\n", " warnings.warn(_use_error_msg)\n", - "/usr/local/lib/python2.7/dist-packages/IPython/kernel/__main__.py:11: QAWarning: pyne.rxname is not yet QA compliant.\n", - "/usr/local/lib/python2.7/dist-packages/IPython/kernel/__main__.py:11: QAWarning: pyne.ace is not yet QA compliant.\n" + "/usr/local/lib/python2.7/dist-packages/IPython/kernel/__main__.py:9: QAWarning: pyne.rxname is not yet QA compliant.\n", + "/usr/local/lib/python2.7/dist-packages/IPython/kernel/__main__.py:9: QAWarning: pyne.ace is not yet QA compliant.\n" ] } ], @@ -52,10 +54,8 @@ "\n", "import openmc\n", "import openmc.mgxs as mgxs\n", - "from openmc.source import Source\n", - "from openmc.stats import Box\n", "import openmoc\n", - "from openmoc.compatible import get_openmoc_geometry\n", + "from openmoc.opencg_compatible import get_openmoc_geometry\n", "import pyne.ace\n", "\n", "%matplotlib inline" @@ -286,10 +286,12 @@ "settings_file.batches = batches\n", "settings_file.inactive = inactive\n", "settings_file.particles = particles\n", - "settings_file.output = {'tallies': True, 'summary': True}\n", + "settings_file.output = {'tallies': True}\n", + "\n", + "# Create an initial uniform spatial source distribution over fissionable zones\n", "bounds = [-0.63, -0.63, -0.63, 0.63, 0.63, 0.63]\n", - "settings_file.source = Source(space=Box(\n", - " bounds[:3], bounds[3:], only_fissionable=True))\n", + "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n", + "settings_file.source = openmc.source.Source(space=uniform_dist)\n", "\n", "# Activate tally precision triggers\n", "settings_file.trigger_active = True\n", @@ -450,8 +452,8 @@ " Copyright: 2011-2015 Massachusetts Institute of Technology\n", " License: http://mit-crpg.github.io/openmc/license.html\n", " Version: 0.7.1\n", - " Git SHA1: 263266f4f8807fd38c6ac282fae259ae73fa1eee\n", - " Date/Time: 2016-01-20 18:12:40\n", + " Git SHA1: eeb5091ca3a34cc85df73a3318cae2b6c7097413\n", + " Date/Time: 2016-04-13 11:59:39\n", " MPI Processes: 1\n", "\n", " ===========================================================================\n", @@ -478,91 +480,87 @@ "\n", " Bat./Gen. k Average k \n", " ========= ======== ==================== \n", - " 1/1 1.22593 \n", - " 2/1 1.24245 \n", - " 3/1 1.24545 \n", - " 4/1 1.21868 \n", - " 5/1 1.22429 \n", - " 6/1 1.22607 \n", - " 7/1 1.21456 \n", - " 8/1 1.23816 \n", - " 9/1 1.25060 \n", - " 10/1 1.22806 \n", - " 11/1 1.19821 \n", - " 12/1 1.19897 1.19859 +/- 0.00038\n", - " 13/1 1.22119 1.20612 +/- 0.00754\n", - " 14/1 1.20701 1.20634 +/- 0.00533\n", - " 15/1 1.24784 1.21464 +/- 0.00927\n", - " 16/1 1.22413 1.21622 +/- 0.00773\n", - " 17/1 1.25050 1.22112 +/- 0.00817\n", - " 18/1 1.22006 1.22099 +/- 0.00707\n", - " 19/1 1.22813 1.22178 +/- 0.00629\n", - " 20/1 1.22791 1.22239 +/- 0.00566\n", - " 21/1 1.22729 1.22284 +/- 0.00514\n", - " 22/1 1.19867 1.22083 +/- 0.00510\n", - " 23/1 1.23796 1.22214 +/- 0.00488\n", - " 24/1 1.22412 1.22228 +/- 0.00452\n", - " 25/1 1.22638 1.22256 +/- 0.00421\n", - " 26/1 1.22181 1.22251 +/- 0.00394\n", - " 27/1 1.19055 1.22063 +/- 0.00415\n", - " 28/1 1.20683 1.21986 +/- 0.00399\n", - " 29/1 1.21689 1.21971 +/- 0.00378\n", - " 30/1 1.23670 1.22056 +/- 0.00368\n", - " 31/1 1.21396 1.22024 +/- 0.00352\n", - " 32/1 1.21389 1.21995 +/- 0.00337\n", - " 33/1 1.24649 1.22111 +/- 0.00342\n", - " 34/1 1.23204 1.22156 +/- 0.00330\n", - " 35/1 1.20768 1.22101 +/- 0.00322\n", - " 36/1 1.22271 1.22107 +/- 0.00309\n", - " 37/1 1.21796 1.22096 +/- 0.00298\n", - " 38/1 1.23842 1.22158 +/- 0.00293\n", - " 39/1 1.23080 1.22190 +/- 0.00285\n", - " 40/1 1.23572 1.22236 +/- 0.00279\n", - " 41/1 1.21691 1.22218 +/- 0.00271\n", - " 42/1 1.24616 1.22293 +/- 0.00272\n", - " 43/1 1.21903 1.22282 +/- 0.00264\n", - " 44/1 1.22967 1.22302 +/- 0.00257\n", - " 45/1 1.22053 1.22295 +/- 0.00250\n", - " 46/1 1.24087 1.22344 +/- 0.00248\n", - " 47/1 1.20251 1.22288 +/- 0.00248\n", - " 48/1 1.20331 1.22236 +/- 0.00246\n", - " 49/1 1.22724 1.22249 +/- 0.00240\n", - " 50/1 1.24798 1.22313 +/- 0.00243\n", - " Triggers unsatisfied, max unc./thresh. is 1.32110 for scatter-p1 in tally 10054\n", - " The estimated number of batches is 80\n", + " 1/1 1.20332 \n", + " 2/1 1.22209 \n", + " 3/1 1.24309 \n", + " 4/1 1.22833 \n", + " 5/1 1.21786 \n", + " 6/1 1.22005 \n", + " 7/1 1.20894 \n", + " 8/1 1.22071 \n", + " 9/1 1.21279 \n", + " 10/1 1.22198 \n", + " 11/1 1.22287 \n", + " 12/1 1.25490 1.23888 +/- 0.01602\n", + " 13/1 1.20224 1.22667 +/- 0.01532\n", + " 14/1 1.23375 1.22844 +/- 0.01098\n", + " 15/1 1.23068 1.22889 +/- 0.00851\n", + " 16/1 1.23073 1.22920 +/- 0.00696\n", + " 17/1 1.25364 1.23269 +/- 0.00684\n", + " 18/1 1.20820 1.22963 +/- 0.00667\n", + " 19/1 1.23138 1.22982 +/- 0.00588\n", + " 20/1 1.20682 1.22752 +/- 0.00574\n", + " 21/1 1.23580 1.22827 +/- 0.00525\n", + " 22/1 1.24190 1.22941 +/- 0.00492\n", + " 23/1 1.23125 1.22955 +/- 0.00453\n", + " 24/1 1.21606 1.22859 +/- 0.00430\n", + " 25/1 1.23653 1.22912 +/- 0.00404\n", + " 26/1 1.23850 1.22970 +/- 0.00383\n", + " 27/1 1.20986 1.22853 +/- 0.00378\n", + " 28/1 1.25277 1.22988 +/- 0.00381\n", + " 29/1 1.23334 1.23006 +/- 0.00361\n", + " 30/1 1.24345 1.23073 +/- 0.00349\n", + " 31/1 1.21565 1.23001 +/- 0.00339\n", + " 32/1 1.20555 1.22890 +/- 0.00342\n", + " 33/1 1.22995 1.22895 +/- 0.00327\n", + " 34/1 1.19763 1.22764 +/- 0.00339\n", + " 35/1 1.22645 1.22760 +/- 0.00325\n", + " 36/1 1.23900 1.22803 +/- 0.00316\n", + " 37/1 1.24305 1.22859 +/- 0.00309\n", + " 38/1 1.22484 1.22846 +/- 0.00298\n", + " 39/1 1.20986 1.22782 +/- 0.00294\n", + " 40/1 1.23764 1.22814 +/- 0.00286\n", + " 41/1 1.20476 1.22739 +/- 0.00287\n", + " 42/1 1.21652 1.22705 +/- 0.00280\n", + " 43/1 1.21279 1.22662 +/- 0.00275\n", + " 44/1 1.20210 1.22590 +/- 0.00276\n", + " 45/1 1.22644 1.22591 +/- 0.00268\n", + " 46/1 1.22907 1.22600 +/- 0.00261\n", + " 47/1 1.24057 1.22639 +/- 0.00257\n", + " 48/1 1.21610 1.22612 +/- 0.00251\n", + " 49/1 1.22199 1.22602 +/- 0.00245\n", + " 50/1 1.20860 1.22558 +/- 0.00243\n", + " Triggers unsatisfied, max unc./thresh. is 1.25496 for flux in tally 10050\n", + " The estimated number of batches is 73\n", " Creating state point statepoint.050.h5...\n", - " 51/1 1.22253 1.22311 +/- 0.00237\n", - " 52/1 1.24330 1.22359 +/- 0.00236\n", - " 53/1 1.23251 1.22380 +/- 0.00231\n", - " 54/1 1.21133 1.22352 +/- 0.00228\n", - " 55/1 1.24503 1.22399 +/- 0.00228\n", - " 56/1 1.22013 1.22391 +/- 0.00223\n", - " 57/1 1.23877 1.22423 +/- 0.00220\n", - " 58/1 1.23793 1.22451 +/- 0.00218\n", - " 59/1 1.21018 1.22422 +/- 0.00215\n", - " 60/1 1.22417 1.22422 +/- 0.00211\n", - " 61/1 1.23094 1.22435 +/- 0.00207\n", - " 62/1 1.23310 1.22452 +/- 0.00204\n", - " 63/1 1.22488 1.22453 +/- 0.00200\n", - " 64/1 1.22702 1.22457 +/- 0.00196\n", - " 65/1 1.18834 1.22391 +/- 0.00204\n", - " 66/1 1.23112 1.22404 +/- 0.00200\n", - " 67/1 1.21611 1.22390 +/- 0.00197\n", - " 68/1 1.22513 1.22392 +/- 0.00194\n", - " 69/1 1.21741 1.22381 +/- 0.00191\n", - " 70/1 1.22484 1.22383 +/- 0.00188\n", - " 71/1 1.19662 1.22338 +/- 0.00190\n", - " 72/1 1.23315 1.22354 +/- 0.00187\n", - " 73/1 1.22796 1.22361 +/- 0.00185\n", - " 74/1 1.21417 1.22346 +/- 0.00182\n", - " 75/1 1.21020 1.22326 +/- 0.00181\n", - " 76/1 1.23413 1.22343 +/- 0.00179\n", - " 77/1 1.22184 1.22340 +/- 0.00176\n", - " 78/1 1.20309 1.22310 +/- 0.00176\n", - " 79/1 1.23458 1.22327 +/- 0.00174\n", - " 80/1 1.20724 1.22304 +/- 0.00173\n", - " Triggers satisfied for batch 80\n", - " Creating state point statepoint.080.h5...\n", + " 51/1 1.21850 1.22541 +/- 0.00237\n", + " 52/1 1.22833 1.22548 +/- 0.00232\n", + " 53/1 1.20239 1.22494 +/- 0.00233\n", + " 54/1 1.24876 1.22548 +/- 0.00234\n", + " 55/1 1.20670 1.22506 +/- 0.00232\n", + " 56/1 1.24260 1.22545 +/- 0.00230\n", + " 57/1 1.21039 1.22512 +/- 0.00228\n", + " 58/1 1.23929 1.22542 +/- 0.00225\n", + " 59/1 1.21357 1.22518 +/- 0.00221\n", + " 60/1 1.23456 1.22537 +/- 0.00218\n", + " 61/1 1.23963 1.22565 +/- 0.00215\n", + " 62/1 1.24020 1.22593 +/- 0.00213\n", + " 63/1 1.22325 1.22587 +/- 0.00209\n", + " 64/1 1.22070 1.22578 +/- 0.00205\n", + " 65/1 1.22423 1.22575 +/- 0.00201\n", + " 66/1 1.22973 1.22582 +/- 0.00198\n", + " 67/1 1.21842 1.22569 +/- 0.00195\n", + " 68/1 1.19552 1.22517 +/- 0.00198\n", + " 69/1 1.21475 1.22500 +/- 0.00196\n", + " 70/1 1.21888 1.22489 +/- 0.00193\n", + " 71/1 1.19720 1.22444 +/- 0.00195\n", + " 72/1 1.23770 1.22465 +/- 0.00193\n", + " 73/1 1.23894 1.22488 +/- 0.00191\n", + " Triggers unsatisfied, max unc./thresh. is 1.00243 for flux in tally 10050\n", + " The estimated number of batches is 74\n", + " 74/1 1.22437 1.22487 +/- 0.00188\n", + " Triggers satisfied for batch 74\n", + " Creating state point statepoint.074.h5...\n", "\n", " ===========================================================================\n", " ======================> SIMULATION FINISHED <======================\n", @@ -571,27 +569,27 @@ "\n", " =======================> TIMING STATISTICS <=======================\n", "\n", - " Total time for initialization = 4.3200E-01 seconds\n", - " Reading cross sections = 9.1000E-02 seconds\n", - " Total time in simulation = 2.2239E+02 seconds\n", - " Time in transport only = 2.2234E+02 seconds\n", - " Time in inactive batches = 1.3715E+01 seconds\n", - " Time in active batches = 2.0867E+02 seconds\n", - " Time synchronizing fission bank = 2.3000E-02 seconds\n", - " Sampling source sites = 1.7000E-02 seconds\n", - " SEND/RECV source sites = 6.0000E-03 seconds\n", - " Time accumulating tallies = 2.0000E-03 seconds\n", - " Total time for finalization = 9.0000E-03 seconds\n", - " Total time elapsed = 2.2288E+02 seconds\n", - " Calculation Rate (inactive) = 7291.29 neutrons/second\n", - " Calculation Rate (active) = 1916.88 neutrons/second\n", + " Total time for initialization = 4.0100E-01 seconds\n", + " Reading cross sections = 8.8000E-02 seconds\n", + " Total time in simulation = 2.3897E+02 seconds\n", + " Time in transport only = 2.3892E+02 seconds\n", + " Time in inactive batches = 1.6456E+01 seconds\n", + " Time in active batches = 2.2251E+02 seconds\n", + " Time synchronizing fission bank = 1.8000E-02 seconds\n", + " Sampling source sites = 1.3000E-02 seconds\n", + " SEND/RECV source sites = 4.0000E-03 seconds\n", + " Time accumulating tallies = 0.0000E+00 seconds\n", + " Total time for finalization = 1.2000E-02 seconds\n", + " Total time elapsed = 2.3943E+02 seconds\n", + " Calculation Rate (inactive) = 6076.81 neutrons/second\n", + " Calculation Rate (active) = 1797.66 neutrons/second\n", "\n", " ============================> RESULTS <============================\n", "\n", - " k-effective (Collision) = 1.22327 +/- 0.00148\n", - " k-effective (Track-length) = 1.22304 +/- 0.00173\n", - " k-effective (Absorption) = 1.22407 +/- 0.00129\n", - " Combined k-effective = 1.22373 +/- 0.00113\n", + " k-effective (Collision) = 1.22358 +/- 0.00179\n", + " k-effective (Track-length) = 1.22487 +/- 0.00188\n", + " k-effective (Absorption) = 1.22300 +/- 0.00114\n", + " Combined k-effective = 1.22347 +/- 0.00106\n", " Leakage Fraction = 0.00000 +/- 0.00000\n", "\n" ] @@ -636,7 +634,7 @@ "outputs": [], "source": [ "# Load the last statepoint file\n", - "sp = openmc.StatePoint('statepoint.080.h5')" + "sp = openmc.StatePoint('statepoint.074.h5')" ] }, { @@ -650,7 +648,7 @@ "cell_type": "code", "execution_count": 16, "metadata": { - "collapsed": true + "collapsed": false }, "outputs": [], "source": [ @@ -718,25 +716,25 @@ "\tDomain ID =\t10000\n", "\tNuclide =\tU-235\n", "\tCross Sections [barns]:\n", - " Group 1 [0.821 - 20.0 MeV]:\t3.31e+00 +/- 1.88e-01%\n", - " Group 2 [0.00553 - 0.821 MeV]:\t3.97e+00 +/- 1.24e-01%\n", - " Group 3 [4e-06 - 0.00553 MeV]:\t5.50e+01 +/- 2.02e-01%\n", - " Group 4 [6.25e-07 - 4e-06 MeV]:\t8.83e+01 +/- 3.56e-01%\n", - " Group 5 [2.8e-07 - 6.25e-07 MeV]:\t2.90e+02 +/- 4.54e-01%\n", - " Group 6 [1.4e-07 - 2.8e-07 MeV]:\t4.49e+02 +/- 4.10e-01%\n", - " Group 7 [5.8e-08 - 1.4e-07 MeV]:\t6.87e+02 +/- 2.56e-01%\n", - " Group 8 [0.0 - 5.8e-08 MeV]:\t1.44e+03 +/- 2.82e-01%\n", + " Group 1 [0.821 - 20.0 MeV]:\t3.30e+00 +/- 2.19e-01%\n", + " Group 2 [0.00553 - 0.821 MeV]:\t3.96e+00 +/- 1.32e-01%\n", + " Group 3 [4e-06 - 0.00553 MeV]:\t5.52e+01 +/- 2.31e-01%\n", + " Group 4 [6.25e-07 - 4e-06 MeV]:\t8.83e+01 +/- 2.96e-01%\n", + " Group 5 [2.8e-07 - 6.25e-07 MeV]:\t2.90e+02 +/- 4.64e-01%\n", + " Group 6 [1.4e-07 - 2.8e-07 MeV]:\t4.49e+02 +/- 4.22e-01%\n", + " Group 7 [5.8e-08 - 1.4e-07 MeV]:\t6.87e+02 +/- 2.97e-01%\n", + " Group 8 [0.0 - 5.8e-08 MeV]:\t1.44e+03 +/- 2.91e-01%\n", "\n", "\tNuclide =\tU-238\n", "\tCross Sections [barns]:\n", - " Group 1 [0.821 - 20.0 MeV]:\t1.06e+00 +/- 2.30e-01%\n", - " Group 2 [0.00553 - 0.821 MeV]:\t1.21e-03 +/- 2.25e-01%\n", - " Group 3 [4e-06 - 0.00553 MeV]:\t5.82e-04 +/- 3.09e+00%\n", - " Group 4 [6.25e-07 - 4e-06 MeV]:\t6.54e-06 +/- 3.27e-01%\n", - " Group 5 [2.8e-07 - 6.25e-07 MeV]:\t1.07e-05 +/- 4.39e-01%\n", - " Group 6 [1.4e-07 - 2.8e-07 MeV]:\t1.55e-05 +/- 4.12e-01%\n", - " Group 7 [5.8e-08 - 1.4e-07 MeV]:\t2.30e-05 +/- 2.57e-01%\n", - " Group 8 [0.0 - 5.8e-08 MeV]:\t4.24e-05 +/- 2.81e-01%\n", + " Group 1 [0.821 - 20.0 MeV]:\t1.06e+00 +/- 2.56e-01%\n", + " Group 2 [0.00553 - 0.821 MeV]:\t1.21e-03 +/- 2.55e-01%\n", + " Group 3 [4e-06 - 0.00553 MeV]:\t5.77e-04 +/- 3.67e+00%\n", + " Group 4 [6.25e-07 - 4e-06 MeV]:\t6.54e-06 +/- 2.74e-01%\n", + " Group 5 [2.8e-07 - 6.25e-07 MeV]:\t1.07e-05 +/- 4.55e-01%\n", + " Group 6 [1.4e-07 - 2.8e-07 MeV]:\t1.55e-05 +/- 4.25e-01%\n", + " Group 7 [5.8e-08 - 1.4e-07 MeV]:\t2.30e-05 +/- 2.97e-01%\n", + " Group 8 [0.0 - 5.8e-08 MeV]:\t4.24e-05 +/- 2.90e-01%\n", "\n", "\n", "\n" @@ -771,14 +769,14 @@ "\tDomain Type =\tcell\n", "\tDomain ID =\t10000\n", "\tCross Sections [cm^-1]:\n", - " Group 1 [0.821 - 20.0 MeV]:\t2.52e-02 +/- 2.19e-01%\n", - " Group 2 [0.00553 - 0.821 MeV]:\t1.51e-03 +/- 1.22e-01%\n", - " Group 3 [4e-06 - 0.00553 MeV]:\t2.06e-02 +/- 2.02e-01%\n", - " Group 4 [6.25e-07 - 4e-06 MeV]:\t3.31e-02 +/- 3.56e-01%\n", - " Group 5 [2.8e-07 - 6.25e-07 MeV]:\t1.09e-01 +/- 4.54e-01%\n", - " Group 6 [1.4e-07 - 2.8e-07 MeV]:\t1.69e-01 +/- 4.10e-01%\n", - " Group 7 [5.8e-08 - 1.4e-07 MeV]:\t2.58e-01 +/- 2.56e-01%\n", - " Group 8 [0.0 - 5.8e-08 MeV]:\t5.40e-01 +/- 2.82e-01%\n", + " Group 1 [0.821 - 20.0 MeV]:\t2.52e-02 +/- 2.44e-01%\n", + " Group 2 [0.00553 - 0.821 MeV]:\t1.51e-03 +/- 1.30e-01%\n", + " Group 3 [4e-06 - 0.00553 MeV]:\t2.07e-02 +/- 2.31e-01%\n", + " Group 4 [6.25e-07 - 4e-06 MeV]:\t3.31e-02 +/- 2.96e-01%\n", + " Group 5 [2.8e-07 - 6.25e-07 MeV]:\t1.09e-01 +/- 4.64e-01%\n", + " Group 6 [1.4e-07 - 2.8e-07 MeV]:\t1.69e-01 +/- 4.22e-01%\n", + " Group 7 [5.8e-08 - 1.4e-07 MeV]:\t2.58e-01 +/- 2.97e-01%\n", + " Group 8 [0.0 - 5.8e-08 MeV]:\t5.40e-01 +/- 2.91e-01%\n", "\n", "\n", "\n" @@ -804,17 +802,6 @@ "collapsed": false }, "outputs": [ - { - "name": "stderr", - "output_type": "stream", - "text": [ - "/usr/local/lib/python2.7/dist-packages/numpy/lib/shape_base.py:872: DeprecationWarning: using a non-integer number instead of an integer will result in an error in the future\n", - " return c.reshape(shape_out)\n", - "/usr/local/lib/python2.7/dist-packages/numpy/lib/shape_base.py:872: DeprecationWarning: using a non-integer number instead of an integer will result in an error in the future\n", - " return c.reshape(shape_out)\n", - "/usr/local/lib/python2.7/dist-packages/openmc-0.7.1-py2.7.egg/openmc/mgxs/mgxs.py:1303: FutureWarning: sort(columns=....) is deprecated, use sort_values(by=.....)\n" - ] - }, { "data": { "text/html": [ @@ -838,8 +825,8 @@ " 1\n", " 1\n", " H-1\n", - " 0.234022\n", - " 0.003645\n", + " 0.234115\n", + " 0.003568\n", " \n", " \n", " 127\n", @@ -847,8 +834,8 @@ " 1\n", " 1\n", " O-16\n", - " 1.560305\n", - " 0.006280\n", + " 1.563707\n", + " 0.005953\n", " \n", " \n", " 124\n", @@ -856,8 +843,8 @@ " 1\n", " 2\n", " H-1\n", - " 1.588025\n", - " 0.002815\n", + " 1.594129\n", + " 0.002369\n", " \n", " \n", " 125\n", @@ -865,8 +852,8 @@ " 1\n", " 2\n", " O-16\n", - " 0.285147\n", - " 0.001392\n", + " 0.285761\n", + " 0.001676\n", " \n", " \n", " 122\n", @@ -874,8 +861,8 @@ " 1\n", " 3\n", " H-1\n", - " 0.010776\n", - " 0.000186\n", + " 0.011089\n", + " 0.000248\n", " \n", " \n", " 123\n", @@ -892,8 +879,8 @@ " 1\n", " 4\n", " H-1\n", - " 0.000023\n", - " 0.000010\n", + " 0.000000\n", + " 0.000000\n", " \n", " \n", " 121\n", @@ -928,13 +915,13 @@ ], "text/plain": [ " cell group in group out nuclide mean std. dev.\n", - "126 10002 1 1 H-1 0.234022 0.003645\n", - "127 10002 1 1 O-16 1.560305 0.006280\n", - "124 10002 1 2 H-1 1.588025 0.002815\n", - "125 10002 1 2 O-16 0.285147 0.001392\n", - "122 10002 1 3 H-1 0.010776 0.000186\n", + "126 10002 1 1 H-1 0.234115 0.003568\n", + "127 10002 1 1 O-16 1.563707 0.005953\n", + "124 10002 1 2 H-1 1.594129 0.002369\n", + "125 10002 1 2 O-16 0.285761 0.001676\n", + "122 10002 1 3 H-1 0.011089 0.000248\n", "123 10002 1 3 O-16 0.000000 0.000000\n", - "120 10002 1 4 H-1 0.000023 0.000010\n", + "120 10002 1 4 H-1 0.000000 0.000000\n", "121 10002 1 4 O-16 0.000000 0.000000\n", "118 10002 1 5 H-1 0.000000 0.000000\n", "119 10002 1 5 O-16 0.000000 0.000000" @@ -997,18 +984,18 @@ "\tDomain ID =\t10000\n", "\tNuclide =\tU-235\n", "\tCross Sections [cm^-1]:\n", - " Group 1 [6.25e-07 - 20.0 MeV]:\t7.81e-03 +/- 4.75e-01%\n", - " Group 2 [0.0 - 6.25e-07 MeV]:\t1.82e-01 +/- 1.89e-01%\n", + " Group 1 [6.25e-07 - 20.0 MeV]:\t7.73e-03 +/- 5.06e-01%\n", + " Group 2 [0.0 - 6.25e-07 MeV]:\t1.82e-01 +/- 2.05e-01%\n", "\n", "\tNuclide =\tU-238\n", "\tCross Sections [cm^-1]:\n", - " Group 1 [6.25e-07 - 20.0 MeV]:\t2.17e-01 +/- 1.31e-01%\n", - " Group 2 [0.0 - 6.25e-07 MeV]:\t2.53e-01 +/- 2.08e-01%\n", + " Group 1 [6.25e-07 - 20.0 MeV]:\t2.17e-01 +/- 1.44e-01%\n", + " Group 2 [0.0 - 6.25e-07 MeV]:\t2.53e-01 +/- 2.57e-01%\n", "\n", "\tNuclide =\tO-16\n", "\tCross Sections [cm^-1]:\n", - " Group 1 [6.25e-07 - 20.0 MeV]:\t1.45e-01 +/- 1.50e-01%\n", - " Group 2 [0.0 - 6.25e-07 MeV]:\t1.74e-01 +/- 2.66e-01%\n", + " Group 1 [6.25e-07 - 20.0 MeV]:\t1.46e-01 +/- 1.60e-01%\n", + " Group 2 [0.0 - 6.25e-07 MeV]:\t1.75e-01 +/- 2.94e-01%\n", "\n", "\n", "\n" @@ -1026,16 +1013,6 @@ "collapsed": false }, "outputs": [ - { - "name": "stderr", - "output_type": "stream", - "text": [ - "/usr/local/lib/python2.7/dist-packages/numpy/lib/shape_base.py:872: DeprecationWarning: using a non-integer number instead of an integer will result in an error in the future\n", - " return c.reshape(shape_out)\n", - "/usr/local/lib/python2.7/dist-packages/numpy/lib/shape_base.py:872: DeprecationWarning: using a non-integer number instead of an integer will result in an error in the future\n", - " return c.reshape(shape_out)\n" - ] - }, { "data": { "text/html": [ @@ -1057,48 +1034,48 @@ " 10000\n", " 1\n", " U-235\n", - " 20.828127\n", - " 0.098842\n", + " 20.611692\n", + " 0.104237\n", " \n", " \n", " 4\n", " 10000\n", " 1\n", " U-238\n", - " 9.582295\n", - " 0.012550\n", + " 9.585358\n", + " 0.013808\n", " \n", " \n", " 5\n", " 10000\n", " 1\n", " O-16\n", - " 3.157358\n", - " 0.004725\n", + " 3.164190\n", + " 0.005049\n", " \n", " \n", " 0\n", " 10000\n", " 2\n", " U-235\n", - " 485.217649\n", - " 0.916465\n", + " 485.413426\n", + " 0.996410\n", " \n", " \n", " 1\n", " 10000\n", " 2\n", " U-238\n", - " 11.176081\n", - " 0.023196\n", + " 11.190386\n", + " 0.028731\n", " \n", " \n", " 2\n", " 10000\n", " 2\n", " O-16\n", - " 3.788167\n", - " 0.010090\n", + " 3.794859\n", + " 0.011139\n", " \n", " \n", "\n", @@ -1106,12 +1083,12 @@ ], "text/plain": [ " cell group in nuclide mean std. dev.\n", - "3 10000 1 U-235 20.828127 0.098842\n", - "4 10000 1 U-238 9.582295 0.012550\n", - "5 10000 1 O-16 3.157358 0.004725\n", - "0 10000 2 U-235 485.217649 0.916465\n", - "1 10000 2 U-238 11.176081 0.023196\n", - "2 10000 2 O-16 3.788167 0.010090" + "3 10000 1 U-235 20.611692 0.104237\n", + "4 10000 1 U-238 9.585358 0.013808\n", + "5 10000 1 O-16 3.164190 0.005049\n", + "0 10000 2 U-235 485.413426 0.996410\n", + "1 10000 2 U-238 11.190386 0.028731\n", + "2 10000 2 O-16 3.794859 0.011139" ] }, "execution_count": 23, @@ -1215,168 +1192,169 @@ "text": [ "[ NORMAL ] Importing ray tracing data from file...\n", "[ NORMAL ] Computing the eigenvalue...\n", - "[ NORMAL ] Iteration 0:\tk_eff = 0.574633\tres = 5.948E-317\n", - "[ NORMAL ] Iteration 1:\tk_eff = 0.679931\tres = 4.254E-01\n", - "[ NORMAL ] Iteration 2:\tk_eff = 0.660910\tres = 1.832E-01\n", - "[ NORMAL ] Iteration 3:\tk_eff = 0.658975\tres = 2.797E-02\n", - "[ NORMAL ] Iteration 4:\tk_eff = 0.642976\tres = 2.928E-03\n", - "[ NORMAL ] Iteration 5:\tk_eff = 0.625710\tres = 2.428E-02\n", - "[ NORMAL ] Iteration 6:\tk_eff = 0.606520\tres = 2.685E-02\n", - "[ NORMAL ] Iteration 7:\tk_eff = 0.587277\tres = 3.067E-02\n", - "[ NORMAL ] Iteration 8:\tk_eff = 0.568777\tres = 3.173E-02\n", - "[ NORMAL ] Iteration 9:\tk_eff = 0.551415\tres = 3.150E-02\n", - "[ NORMAL ] Iteration 10:\tk_eff = 0.535708\tres = 3.052E-02\n", - "[ NORMAL ] 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NORMAL ] Iteration 217:\tk_eff = 1.223061\tres = 1.680E-05\n", + "[ NORMAL ] Iteration 218:\tk_eff = 1.223080\tres = 1.616E-05\n", + "[ NORMAL ] Iteration 219:\tk_eff = 1.223098\tres = 1.554E-05\n", + "[ NORMAL ] Iteration 220:\tk_eff = 1.223116\tres = 1.495E-05\n", + "[ NORMAL ] Iteration 221:\tk_eff = 1.223132\tres = 1.437E-05\n", + "[ NORMAL ] Iteration 222:\tk_eff = 1.223149\tres = 1.382E-05\n", + "[ NORMAL ] Iteration 223:\tk_eff = 1.223164\tres = 1.330E-05\n", + "[ NORMAL ] Iteration 224:\tk_eff = 1.223179\tres = 1.279E-05\n", + "[ NORMAL ] Iteration 225:\tk_eff = 1.223194\tres = 1.230E-05\n", + "[ NORMAL ] Iteration 226:\tk_eff = 1.223208\tres = 1.183E-05\n", + "[ NORMAL ] Iteration 227:\tk_eff = 1.223221\tres = 1.138E-05\n", + "[ NORMAL ] Iteration 228:\tk_eff = 1.223234\tres = 1.094E-05\n", + "[ NORMAL ] Iteration 229:\tk_eff = 1.223246\tres = 1.052E-05\n", + "[ NORMAL ] Iteration 230:\tk_eff = 1.223258\tres = 1.012E-05\n" ] } ], @@ -1740,9 +1718,9 @@ "name": "stdout", "output_type": "stream", "text": [ - "openmc keff = 1.223729\n", - "openmoc keff = 1.222447\n", - "bias [pcm]: -128.2\n" + "openmc keff = 1.223474\n", + "openmoc keff = 1.223258\n", + "bias [pcm]: -21.5\n" ] } ], @@ -1831,9 +1809,9 @@ }, { "data": { - "image/png": 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NiQo+A2zbVhpS7/HHs7juuuDB588+s3PyyQURB6bT7T6mu1ai9ZoTfG5s5bMg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\nnYz04Ol8fel6baJlPT25tggrTElUAlN2J1IrGZq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N73Q6ue++BxgzZhyPPfZos+WNVcYlBxEpFZGPReSUVMdu397DrFm1dO7s5uSTS1izRjuq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\n+KP1PP8hsU6nNWku3KqsyVy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"text/plain": [ - "" + "" ] }, "metadata": {}, @@ -1879,18 +1857,7 @@ "metadata": { "collapsed": false }, - "outputs": [ - { - "name": "stderr", - "output_type": "stream", - "text": [ - "/usr/local/lib/python2.7/dist-packages/numpy/lib/shape_base.py:872: DeprecationWarning: using a non-integer number instead of an integer will result in an error in the future\n", - " return c.reshape(shape_out)\n", - "/usr/local/lib/python2.7/dist-packages/numpy/lib/shape_base.py:872: DeprecationWarning: using a non-integer number instead of an integer will result in an error in the future\n", - " return c.reshape(shape_out)\n" - ] - } - ], + "outputs": [], "source": [ "# Construct a Pandas DataFrame for the microscopic nu-scattering matrix\n", "nuscatter = xs_library[moderator_cell.id]['nu-scatter']\n", @@ -1925,9 +1892,9 @@ "outputs": [ { "data": { - "image/png": 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"text/plain": [ - "" + "" ] }, "metadata": {}, diff --git a/docs/source/pythonapi/examples/mgxs-part-iii.ipynb b/docs/source/pythonapi/examples/mgxs-part-iii.ipynb index a541efbf0..5fccc4f03 100644 --- a/docs/source/pythonapi/examples/mgxs-part-iii.ipynb +++ b/docs/source/pythonapi/examples/mgxs-part-iii.ipynb @@ -32,7 +32,7 @@ "name": "stderr", "output_type": "stream", "text": [ - "/usr/local/lib/python2.7/dist-packages/matplotlib/__init__.py:1318: UserWarning: This call to matplotlib.use() has no effect\n", + "/usr/local/lib/python2.7/dist-packages/matplotlib-1.5.1+1178.ga40c9ec-py2.7-linux-x86_64.egg/matplotlib/__init__.py:1362: UserWarning: This call to matplotlib.use() has no effect\n", "because the backend has already been chosen;\n", "matplotlib.use() must be called *before* pylab, matplotlib.pyplot,\n", "or matplotlib.backends is imported for the first time.\n", @@ -44,20 +44,16 @@ "source": [ "import math\n", "import pickle\n", + "\n", "from IPython.display import Image\n", - "import matplotlib.pylab as pylab\n", + "import matplotlib.pyplot as plt\n", "import numpy as np\n", "\n", "import openmc\n", "import openmc.mgxs\n", - "from openmc.statepoint import StatePoint\n", - "from openmc.summary import Summary\n", - "from openmc.source import Source\n", - "from openmc.stats import Box\n", - "\n", "import openmoc\n", "import openmoc.process\n", - "from openmoc.compatible import get_openmoc_geometry\n", + "from openmoc.opencg_compatible import get_openmoc_geometry\n", "from openmoc.materialize import load_openmc_mgxs_lib\n", "\n", "%matplotlib inline" @@ -392,10 +388,12 @@ "settings_file.batches = batches\n", "settings_file.inactive = inactive\n", "settings_file.particles = particles\n", - "settings_file.output = {'tallies': False, 'summary': True}\n", - "source_bounds = [-10.71, -10.71, -10, 10.71, 10.71, 10.]\n", - "settings_file.source = Source(Box(\n", - " source_bounds[:3], source_bounds[3:], only_fissionable=True))\n", + "settings_file.output = {'tallies': False}\n", + "\n", + "# Create an initial uniform spatial source distribution over fissionable zones\n", + "bounds = [-10.71, -10.71, -10, 10.71, 10.71, 10.]\n", + "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n", + "settings_file.source = openmc.source.Source(space=uniform_dist)\n", "\n", "# Export to \"settings.xml\"\n", "settings_file.export_to_xml()" @@ -420,8 +418,8 @@ "plot = openmc.Plot(plot_id=1)\n", "plot.filename = 'materials-xy'\n", "plot.origin = [0, 0, 0]\n", - "plot.width = [21.5, 21.5]\n", "plot.pixels = [250, 250]\n", + "plot.width = [-10.71*2, -10.71*2]\n", "plot.color = 'mat'\n", "\n", "# Instantiate a PlotsFile, add Plot, and export to \"plots.xml\"\n", @@ -470,7 +468,7 @@ "outputs": [ { "data": { - "image/png": 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+ "image/png": "iVBORw0KGgoAAAANSUhEUgAAAPoAAAD6AgMAAAD1grKuAAAABGdBTUEAALGPC/xhBQAAAAFzUkdC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\n", "text/plain": [ "" ] @@ -560,7 +558,7 @@ "* `NuScatterMatrixXS` (`\"nu-scatter matrix\"`)\n", "* `Chi` (`\"chi\"`)\n", "\n", - "In this case, let's create the multi-group cross sections needed to run an OpenMOC simulation to verify the accuracy of our cross sections. In particular, we will define `\"transport\"`, `\"nu-fission\"`, `\"nu-scatter matrix\"` and `\"chi\"` cross sections for our `Library`.\n", + "In this case, let's create the multi-group cross sections needed to run an OpenMOC simulation to verify the accuracy of our cross sections. In particular, we will define `\"transport\"`, `\"nu-fission\"`, `'\"fission\"`, `\"nu-scatter matrix\"` and `\"chi\"` cross sections for our `Library`.\n", "\n", "**Note**: A variety of different approximate transport-corrected total multi-group cross sections (and corresponding scattering matrices) can be found in the literature. At the present time, the `openmc.mgxs` module only supports the `\"P0\"` transport correction. This correction can be turned on and off through the boolean `Library.correction` property which may take values of `\"P0\"` (default) or `None`." ] @@ -569,12 +567,12 @@ "cell_type": "code", "execution_count": 19, "metadata": { - "collapsed": true + "collapsed": false }, "outputs": [], "source": [ "# Specify multi-group cross section types to compute\n", - "mgxs_lib.mgxs_types = ['transport', 'nu-fission', 'nu-scatter matrix', 'chi']" + "mgxs_lib.mgxs_types = ['transport', 'nu-fission', 'fission', 'nu-scatter matrix', 'chi']" ] }, { @@ -681,7 +679,7 @@ "mesh.type = 'regular'\n", "mesh.dimension = [17, 17]\n", "mesh.lower_left = [-10.71, -10.71]\n", - "mesh.width = [1.26, 1.26]\n", + "mesh.upper_right = [+10.71, +10.71]\n", "\n", "# Instantiate tally Filter\n", "mesh_filter = openmc.Filter()\n", @@ -689,9 +687,8 @@ "\n", "# Instantiate the Tally\n", "tally = openmc.Tally(name='mesh tally')\n", - "tally.add_filter(mesh_filter)\n", - "tally.add_score('fission')\n", - "tally.add_score('nu-fission')\n", + "tally.filters = [mesh_filter]\n", + "tally.scores = ['fission', 'nu-fission']\n", "\n", "# Add mesh and Tally to TalliesFile\n", "tallies_file.add_mesh(mesh)\n", @@ -737,8 +734,9 @@ " Copyright: 2011-2015 Massachusetts Institute of Technology\n", " License: http://mit-crpg.github.io/openmc/license.html\n", " Version: 0.7.1\n", - " Git SHA1: ea9fb637f63f9374c7436456141afa850b84acf9\n", - " Date/Time: 2016-01-14 08:12:09\n", + " Git SHA1: eeb5091ca3a34cc85df73a3318cae2b6c7097413\n", + " Date/Time: 2016-04-13 11:57:40\n", + " MPI Processes: 1\n", "\n", " ===========================================================================\n", " ========================> INITIALIZATION <=========================\n", @@ -765,56 +763,56 @@ "\n", " Bat./Gen. k Average k \n", " ========= ======== ==================== \n", - " 1/1 1.02650 \n", - " 2/1 1.01386 \n", - " 3/1 1.01045 \n", - " 4/1 1.05511 \n", - " 5/1 1.04873 \n", - " 6/1 1.04558 \n", - " 7/1 1.03840 \n", - " 8/1 1.02086 \n", - " 9/1 1.08845 \n", - " 10/1 1.03932 \n", - " 11/1 1.01271 \n", - " 12/1 1.03448 1.02360 +/- 0.01088\n", - " 13/1 1.04395 1.03038 +/- 0.00925\n", - " 14/1 1.05477 1.03648 +/- 0.00894\n", - " 15/1 1.00485 1.03015 +/- 0.00938\n", - " 16/1 1.04523 1.03267 +/- 0.00806\n", - " 17/1 1.01328 1.02990 +/- 0.00735\n", - " 18/1 1.01476 1.02800 +/- 0.00664\n", - " 19/1 1.01490 1.02655 +/- 0.00604\n", - " 20/1 1.00926 1.02482 +/- 0.00567\n", - " 21/1 0.98504 1.02120 +/- 0.00627\n", - " 22/1 1.00397 1.01977 +/- 0.00591\n", - " 23/1 1.02556 1.02021 +/- 0.00545\n", - " 24/1 0.99808 1.01863 +/- 0.00529\n", - " 25/1 0.99638 1.01715 +/- 0.00514\n", - " 26/1 0.99615 1.01584 +/- 0.00499\n", - " 27/1 1.01843 1.01599 +/- 0.00469\n", - " 28/1 1.00315 1.01528 +/- 0.00447\n", - " 29/1 1.00633 1.01480 +/- 0.00426\n", - " 30/1 1.02159 1.01514 +/- 0.00405\n", - " 31/1 1.03395 1.01604 +/- 0.00396\n", - " 32/1 1.02672 1.01652 +/- 0.00381\n", - " 33/1 1.03778 1.01745 +/- 0.00375\n", - " 34/1 1.03807 1.01831 +/- 0.00369\n", - " 35/1 1.07854 1.02072 +/- 0.00428\n", - " 36/1 1.03524 1.02128 +/- 0.00415\n", - " 37/1 1.03100 1.02164 +/- 0.00401\n", - " 38/1 1.03853 1.02224 +/- 0.00391\n", - " 39/1 1.04089 1.02288 +/- 0.00383\n", - " 40/1 1.02150 1.02284 +/- 0.00370\n", - " 41/1 0.98470 1.02161 +/- 0.00379\n", - " 42/1 1.00658 1.02114 +/- 0.00370\n", - " 43/1 0.98652 1.02009 +/- 0.00373\n", - " 44/1 1.02787 1.02032 +/- 0.00363\n", - " 45/1 0.98800 1.01939 +/- 0.00364\n", - " 46/1 1.00286 1.01893 +/- 0.00357\n", - " 47/1 1.02559 1.01911 +/- 0.00348\n", - " 48/1 1.03729 1.01959 +/- 0.00342\n", - " 49/1 1.02538 1.01974 +/- 0.00333\n", - " 50/1 1.01478 1.01962 +/- 0.00325\n", + " 1/1 1.03852 \n", + " 2/1 0.99743 \n", + " 3/1 1.02987 \n", + " 4/1 1.04472 \n", + " 5/1 1.02183 \n", + " 6/1 1.05263 \n", + " 7/1 0.99048 \n", + " 8/1 1.02753 \n", + " 9/1 1.03159 \n", + " 10/1 1.04005 \n", + " 11/1 1.05278 \n", + " 12/1 1.02555 1.03917 +/- 0.01362\n", + " 13/1 0.99400 1.02411 +/- 0.01699\n", + " 14/1 1.03508 1.02685 +/- 0.01232\n", + " 15/1 1.00055 1.02159 +/- 0.01090\n", + " 16/1 1.01334 1.02022 +/- 0.00900\n", + " 17/1 0.99822 1.01707 +/- 0.00823\n", + " 18/1 1.01767 1.01715 +/- 0.00713\n", + " 19/1 1.05052 1.02086 +/- 0.00730\n", + " 20/1 1.03133 1.02190 +/- 0.00661\n", + " 21/1 1.04112 1.02365 +/- 0.00623\n", + " 22/1 1.04175 1.02516 +/- 0.00588\n", + " 23/1 1.01909 1.02469 +/- 0.00543\n", + " 24/1 1.07119 1.02801 +/- 0.00603\n", + " 25/1 0.97445 1.02444 +/- 0.00665\n", + " 26/1 1.04737 1.02588 +/- 0.00638\n", + " 27/1 1.04656 1.02709 +/- 0.00612\n", + " 28/1 1.03464 1.02751 +/- 0.00578\n", + " 29/1 1.02528 1.02739 +/- 0.00547\n", + " 30/1 1.02799 1.02742 +/- 0.00519\n", + " 31/1 1.05846 1.02890 +/- 0.00516\n", + " 32/1 1.03811 1.02932 +/- 0.00493\n", + " 33/1 1.00894 1.02843 +/- 0.00480\n", + " 34/1 1.02049 1.02810 +/- 0.00460\n", + " 35/1 1.00690 1.02726 +/- 0.00450\n", + " 36/1 1.03129 1.02741 +/- 0.00432\n", + " 37/1 0.98864 1.02597 +/- 0.00440\n", + " 38/1 1.00017 1.02505 +/- 0.00434\n", + " 39/1 1.03635 1.02544 +/- 0.00421\n", + " 40/1 1.07090 1.02696 +/- 0.00434\n", + " 41/1 1.03141 1.02710 +/- 0.00420\n", + " 42/1 1.02624 1.02707 +/- 0.00406\n", + " 43/1 1.02668 1.02706 +/- 0.00394\n", + " 44/1 1.05940 1.02801 +/- 0.00394\n", + " 45/1 1.01149 1.02754 +/- 0.00385\n", + " 46/1 1.06958 1.02871 +/- 0.00392\n", + " 47/1 1.02674 1.02866 +/- 0.00381\n", + " 48/1 1.02542 1.02857 +/- 0.00371\n", + " 49/1 1.03516 1.02874 +/- 0.00362\n", + " 50/1 1.06818 1.02973 +/- 0.00366\n", " Creating state point statepoint.50.h5...\n", "\n", " ===========================================================================\n", @@ -824,27 +822,27 @@ "\n", " =======================> TIMING STATISTICS <=======================\n", "\n", - " Total time for initialization = 4.1800E-01 seconds\n", - " Reading cross sections = 1.4300E-01 seconds\n", - " Total time in simulation = 4.1206E+01 seconds\n", - " Time in transport only = 4.1193E+01 seconds\n", - " Time in inactive batches = 4.1760E+00 seconds\n", - " Time in active batches = 3.7030E+01 seconds\n", + " Total time for initialization = 4.3700E-01 seconds\n", + " Reading cross sections = 8.2000E-02 seconds\n", + " Total time in simulation = 4.7745E+01 seconds\n", + " Time in transport only = 4.7726E+01 seconds\n", + " Time in inactive batches = 3.8220E+00 seconds\n", + " Time in active batches = 4.3923E+01 seconds\n", " Time synchronizing fission bank = 3.0000E-03 seconds\n", " Sampling source sites = 2.0000E-03 seconds\n", - " SEND/RECV source sites = 1.0000E-03 seconds\n", - " Time accumulating tallies = 0.0000E+00 seconds\n", + " SEND/RECV source sites = 0.0000E+00 seconds\n", + " Time accumulating tallies = 1.0000E-03 seconds\n", " Total time for finalization = 0.0000E+00 seconds\n", - " Total time elapsed = 4.1648E+01 seconds\n", - " Calculation Rate (inactive) = 5986.59 neutrons/second\n", - " Calculation Rate (active) = 2700.51 neutrons/second\n", + " Total time elapsed = 4.8198E+01 seconds\n", + " Calculation Rate (inactive) = 6541.08 neutrons/second\n", + " Calculation Rate (active) = 2276.71 neutrons/second\n", "\n", " ============================> RESULTS <============================\n", "\n", - " k-effective (Collision) = 1.01805 +/- 0.00261\n", - " k-effective (Track-length) = 1.01962 +/- 0.00325\n", - " k-effective (Absorption) = 1.01554 +/- 0.00339\n", - " Combined k-effective = 1.01711 +/- 0.00235\n", + " k-effective (Collision) = 1.02763 +/- 0.00343\n", + " k-effective (Track-length) = 1.02973 +/- 0.00366\n", + " k-effective (Absorption) = 1.02732 +/- 0.00319\n", + " Combined k-effective = 1.02826 +/- 0.00259\n", " Leakage Fraction = 0.00000 +/- 0.00000\n", "\n" ] @@ -982,14 +980,13 @@ "name": "stderr", "output_type": "stream", "text": [ - "/home/romano/openmc/openmc/tallies.py:1642: RuntimeWarning: invalid value encountered in true_divide\n", - " self_rel_err = data['self']['std. dev.'] / data['self']['mean']\n" + "/usr/local/lib/python2.7/dist-packages/openmc-0.7.1-py2.7.egg/openmc/tallies.py:1996: RuntimeWarning: invalid value encountered in true_divide\n" ] }, { "data": { "text/html": [ - "
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\n", " \n", " \n", @@ -1220,16 +1217,16 @@ " \n", " \n", " \n", - " \n", - " \n", + " \n", + " \n", " \n", " \n", " \n", " \n", " \n", " \n", - " \n", - " \n", + " \n", + " \n", " \n", " \n", " \n", @@ -1245,8 +1242,8 @@ ], "text/plain": [ " cell group in nuclide mean std. dev.\n", - "0 10000 1 U-235 0.074383 0.000280\n", - "1 10000 1 U-238 0.005959 0.000036\n", + "0 10000 1 U-235 0.074860 0.000303\n", + "1 10000 1 U-238 0.005952 0.000035\n", "2 10000 1 O-16 0.000000 0.000000" ] }, @@ -1327,126 +1324,126 @@ "name": "stdout", "output_type": "stream", "text": [ - "[ NORMAL ] Ray tracing for track segmentation...\n", - "[ NORMAL ] Dumping tracks to file...\n", + "[ NORMAL ] Importing ray tracing data from file...\n", "[ NORMAL ] Computing the eigenvalue...\n", - "[ NORMAL ] Iteration 0:\tk_eff = 0.854316\tres = 0.000E+00\n", - "[ NORMAL ] Iteration 1:\tk_eff = 0.801593\tres = 1.522E-01\n", - "[ NORMAL ] Iteration 2:\tk_eff = 0.761131\tres = 6.380E-02\n", - "[ NORMAL ] Iteration 3:\tk_eff = 0.731467\tres = 5.066E-02\n", - "[ NORMAL ] Iteration 4:\tk_eff = 0.709897\tres = 3.910E-02\n", - "[ NORMAL ] Iteration 5:\tk_eff = 0.695111\tres = 2.954E-02\n", - "[ NORMAL ] Iteration 6:\tk_eff = 0.685967\tres = 2.085E-02\n", - "[ NORMAL ] Iteration 7:\tk_eff = 0.681511\tres = 1.317E-02\n", - "[ NORMAL ] Iteration 8:\tk_eff = 0.680926\tres = 6.520E-03\n", - "[ NORMAL ] Iteration 9:\tk_eff = 0.683509\tres = 1.046E-03\n", - "[ NORMAL ] Iteration 10:\tk_eff = 0.688659\tres = 3.848E-03\n", - "[ NORMAL ] Iteration 11:\tk_eff = 0.695861\tres = 7.565E-03\n", - "[ NORMAL ] Iteration 12:\tk_eff = 0.704674\tres = 1.048E-02\n", - "[ NORMAL ] Iteration 13:\tk_eff = 0.714726\tres = 1.269E-02\n", - "[ NORMAL ] Iteration 14:\tk_eff = 0.725701\tres = 1.428E-02\n", - "[ NORMAL ] Iteration 15:\tk_eff = 0.737329\tres = 1.537E-02\n", - "[ NORMAL ] Iteration 16:\tk_eff = 0.749388\tres = 1.604E-02\n", - "[ NORMAL ] Iteration 17:\tk_eff = 0.761691\tres = 1.637E-02\n", - "[ NORMAL ] Iteration 18:\tk_eff = 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+ "[ NORMAL ] Iteration 65:\tk_eff = 1.020246\tres = 7.562E-04\n", + "[ NORMAL ] Iteration 66:\tk_eff = 1.020903\tres = 6.981E-04\n", + "[ NORMAL ] Iteration 67:\tk_eff = 1.021509\tres = 6.445E-04\n", + "[ NORMAL ] Iteration 68:\tk_eff = 1.022069\tres = 5.948E-04\n", + "[ NORMAL ] Iteration 69:\tk_eff = 1.022586\tres = 5.489E-04\n", + "[ NORMAL ] Iteration 70:\tk_eff = 1.023063\tres = 5.064E-04\n", + "[ NORMAL ] Iteration 71:\tk_eff = 1.023503\tres = 4.671E-04\n", + "[ NORMAL ] Iteration 72:\tk_eff = 1.023909\tres = 4.308E-04\n", + "[ NORMAL ] Iteration 73:\tk_eff = 1.024284\tres = 3.973E-04\n", + "[ NORMAL ] Iteration 74:\tk_eff = 1.024629\tres = 3.663E-04\n", + "[ NORMAL ] Iteration 75:\tk_eff = 1.024948\tres = 3.377E-04\n", + "[ NORMAL ] Iteration 76:\tk_eff = 1.025241\tres = 3.113E-04\n", + "[ NORMAL ] Iteration 77:\tk_eff = 1.025512\tres = 2.869E-04\n", + "[ NORMAL ] Iteration 78:\tk_eff = 1.025761\tres = 2.644E-04\n", + "[ NORMAL ] Iteration 79:\tk_eff = 1.025991\tres = 2.436E-04\n", + "[ NORMAL ] Iteration 80:\tk_eff = 1.026203\tres = 2.244E-04\n", + "[ NORMAL ] Iteration 81:\tk_eff = 1.026398\tres = 2.067E-04\n", + "[ NORMAL ] Iteration 82:\tk_eff = 1.026578\tres = 1.904E-04\n", + "[ NORMAL ] Iteration 83:\tk_eff = 1.026743\tres = 1.754E-04\n", + "[ NORMAL ] Iteration 84:\tk_eff = 1.026895\tres = 1.615E-04\n", + "[ NORMAL ] Iteration 85:\tk_eff = 1.027036\tres = 1.487E-04\n", + "[ NORMAL ] Iteration 86:\tk_eff = 1.027165\tres = 1.369E-04\n", + "[ NORMAL ] Iteration 87:\tk_eff = 1.027284\tres = 1.260E-04\n", + "[ NORMAL ] Iteration 88:\tk_eff = 1.027393\tres = 1.160E-04\n", + "[ NORMAL ] Iteration 89:\tk_eff = 1.027494\tres = 1.068E-04\n", + "[ NORMAL ] Iteration 90:\tk_eff = 1.027587\tres = 9.825E-05\n", + "[ NORMAL ] Iteration 91:\tk_eff = 1.027672\tres = 9.041E-05\n", + "[ NORMAL ] Iteration 92:\tk_eff = 1.027751\tres = 8.319E-05\n", + "[ NORMAL ] Iteration 93:\tk_eff = 1.027823\tres = 7.654E-05\n", + "[ NORMAL ] Iteration 94:\tk_eff = 1.027889\tres = 7.042E-05\n", + "[ NORMAL ] Iteration 95:\tk_eff = 1.027950\tres = 6.478E-05\n", + "[ NORMAL ] Iteration 96:\tk_eff = 1.028007\tres = 5.959E-05\n", + "[ NORMAL ] Iteration 97:\tk_eff = 1.028058\tres = 5.481E-05\n", + "[ NORMAL ] Iteration 98:\tk_eff = 1.028106\tres = 5.041E-05\n", + "[ NORMAL ] Iteration 99:\tk_eff = 1.028150\tres = 4.636E-05\n", + "[ NORMAL ] Iteration 100:\tk_eff = 1.028190\tres = 4.263E-05\n", + "[ NORMAL ] Iteration 101:\tk_eff = 1.028227\tres = 3.920E-05\n", + "[ NORMAL ] Iteration 102:\tk_eff = 1.028261\tres = 3.604E-05\n", + "[ NORMAL ] Iteration 103:\tk_eff = 1.028292\tres = 3.314E-05\n", + "[ NORMAL ] Iteration 104:\tk_eff = 1.028321\tres = 3.047E-05\n", + "[ NORMAL ] Iteration 105:\tk_eff = 1.028347\tres = 2.801E-05\n", + "[ NORMAL ] Iteration 106:\tk_eff = 1.028371\tres = 2.575E-05\n", + "[ NORMAL ] Iteration 107:\tk_eff = 1.028394\tres = 2.367E-05\n", + "[ NORMAL ] Iteration 108:\tk_eff = 1.028414\tres = 2.175E-05\n", + "[ NORMAL ] Iteration 109:\tk_eff = 1.028433\tres = 1.999E-05\n", + "[ NORMAL ] Iteration 110:\tk_eff = 1.028450\tres = 1.838E-05\n", + "[ NORMAL ] Iteration 111:\tk_eff = 1.028466\tres = 1.689E-05\n", + "[ NORMAL ] Iteration 112:\tk_eff = 1.028481\tres = 1.552E-05\n", + "[ NORMAL ] Iteration 113:\tk_eff = 1.028494\tres = 1.426E-05\n", + "[ NORMAL ] Iteration 114:\tk_eff = 1.028507\tres = 1.310E-05\n", + "[ NORMAL ] Iteration 115:\tk_eff = 1.028518\tres = 1.204E-05\n", + "[ NORMAL ] Iteration 116:\tk_eff = 1.028528\tres = 1.106E-05\n", + "[ NORMAL ] Iteration 117:\tk_eff = 1.028538\tres = 1.017E-05\n" ] } ], @@ -1478,9 +1475,9 @@ "name": "stdout", "output_type": "stream", "text": [ - "openmc keff = 1.017105\n", - "openmoc keff = 1.020704\n", - "bias [pcm]: 359.8\n" + "openmc keff = 1.028263\n", + "openmoc keff = 1.028538\n", + "bias [pcm]: 27.5\n" ] } ], @@ -1554,20 +1551,18 @@ }, "outputs": [], "source": [ - "# Export OpenMOC's fission rates for each pin cell instance in the fuel assembly\n", - "openmoc.process.compute_fission_rates(solver)\n", + "# Create OpenMOC Mesh on which to tally fission rates\n", + "openmoc_mesh = openmoc.process.Mesh()\n", + "openmoc_mesh.dimension = np.array(mesh.dimension)\n", + "openmoc_mesh.lower_left = np.array(mesh.lower_left)\n", + "openmoc_mesh.upper_right = np.array(mesh.upper_right)\n", + "openmoc_mesh.width = openmoc_mesh.upper_right - openmoc_mesh.lower_left\n", + "openmoc_mesh.width /= openmoc_mesh.dimension\n", "\n", - "# Open the pickle file with the fission rates\n", - "fission_rates = pickle.load(open('fission-rates/fission-rates.pkl', 'rb' ))\n", - "\n", - "# Allocate array for fission rates in each fuel pin\n", - "openmoc_fission_rates = np.zeros((17, 17))\n", - "\n", - "# Extract fission rates for each fuel pin\n", - "for key, value in fission_rates.items():\n", - " lat_x = int(key.split(':')[1].split()[3][1:-1])\n", - " lat_y = int(key.split(':')[1].split()[4][:-1]) \n", - " openmoc_fission_rates[lat_x, lat_y] = value\n", + "# Tally OpenMOC fission rates on the Mesh\n", + "openmoc_fission_rates = openmoc_mesh.tally_fission_rates(solver)\n", + "openmoc_fission_rates = np.squeeze(openmoc_fission_rates)\n", + "openmoc_fission_rates = np.fliplr(openmoc_fission_rates)\n", "\n", "# Normalize to the average pin fission rate\n", "openmoc_fission_rates /= np.mean(openmoc_fission_rates)" @@ -1590,7 +1585,7 @@ { "data": { "text/plain": [ - "" + "" ] }, "execution_count": 44, @@ -1599,9 +1594,9 @@ }, { "data": { - "image/png": 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C1AQ5bCGEqAly2EIIURPksIUQoibIYQshRE1o78SZ8tJsG0t5iQkdADyaFhl9aFpmVJNF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\nhKgJA06cMbPLgdc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FXUQkIyrqIiIZiYw/GJGZDQCbKMY6bHP3l0aet/fJiYA70us4JDAryfa3pWcl8R+n2zpq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\nZOT/APiw99Nd94jXAAAAAElFTkSuQmCC\n", "text/plain": [ - "" + "" ] }, "metadata": {}, @@ -1610,15 +1605,24 @@ ], "source": [ "# Plot OpenMC's fission rates in the left subplot\n", - "fig = pylab.subplot(121)\n", - "pylab.imshow(openmc_fission_rates, interpolation='none', cmap='jet')\n", - "pylab.title('OpenMC Fission Rates')\n", + "fig = plt.subplot(121)\n", + "plt.imshow(openmc_fission_rates, interpolation='none', cmap='jet')\n", + "plt.title('OpenMC Fission Rates')\n", "\n", "# Plot OpenMOC's fission rates in the right subplot\n", - "fig2 = pylab.subplot(122)\n", - "pylab.imshow(openmoc_fission_rates, interpolation='none', cmap='jet')\n", - "pylab.title('OpenMOC Fission Rates')" + "fig2 = plt.subplot(122)\n", + "plt.imshow(openmoc_fission_rates, interpolation='none', cmap='jet')\n", + "plt.title('OpenMOC Fission Rates')" ] + }, + { + "cell_type": "code", + "execution_count": null, + "metadata": { + "collapsed": true + }, + "outputs": [], + "source": [] } ], "metadata": { diff --git a/docs/source/pythonapi/examples/pandas-dataframes.ipynb b/docs/source/pythonapi/examples/pandas-dataframes.ipynb index 60c2c1c40..388e4aaa6 100644 --- a/docs/source/pythonapi/examples/pandas-dataframes.ipynb +++ b/docs/source/pythonapi/examples/pandas-dataframes.ipynb @@ -17,19 +17,14 @@ }, "outputs": [], "source": [ + "%matplotlib inline\n", "import glob\n", "from IPython.display import Image\n", "import matplotlib.pylab as pylab\n", "import scipy.stats\n", "import numpy as np\n", "\n", - "import openmc\n", - "from openmc.statepoint import StatePoint\n", - "from openmc.summary import Summary\n", - "from openmc.source import Source\n", - "from openmc.stats import Box\n", - "\n", - "%matplotlib inline" + "import openmc" ] }, { @@ -302,12 +297,14 @@ "settings_file.batches = min_batches\n", "settings_file.inactive = inactive\n", "settings_file.particles = particles\n", - "settings_file.output = {'tallies': False, 'summary': True}\n", + "settings_file.output = {'tallies': False}\n", "settings_file.trigger_active = True\n", "settings_file.trigger_max_batches = max_batches\n", - "source_bounds = [-10.71, -10.71, -10, 10.71, 10.71, 10.]\n", - "settings_file.source = Source(space=Box(\n", - " source_bounds[:3], source_bounds[3:]))\n", + "\n", + "# Create an initial uniform spatial source distribution over fissionable zones\n", + "bounds = [-10.71, -10.71, -10, 10.71, 10.71, 10.]\n", + "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n", + "settings_file.source = openmc.source.Source(space=uniform_dist)\n", "\n", "# Export to \"settings.xml\"\n", "settings_file.export_to_xml()" @@ -382,7 +379,7 @@ "outputs": [ { "data": { - "image/png": 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+ "image/png": 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"text/plain": [ "" ] @@ -453,10 +450,8 @@ "\n", "# Instantiate the Tally\n", "tally = openmc.Tally(name='mesh tally')\n", - "tally.add_filter(mesh_filter)\n", - "tally.add_filter(energy_filter)\n", - "tally.add_score('fission')\n", - "tally.add_score('nu-fission')\n", + "tally.filters = [mesh_filter, energy_filter]\n", + "tally.scores = ['fission', 'nu-fission']\n", "\n", "# Add mesh and Tally to TalliesFile\n", "tallies_file.add_mesh(mesh)\n", @@ -483,10 +478,9 @@ "\n", "# Instantiate the tally\n", "tally = openmc.Tally(name='cell tally')\n", - "tally.add_filter(cell_filter)\n", - "tally.add_score('scatter-y2')\n", - "tally.add_nuclide(u235)\n", - "tally.add_nuclide(u238)\n", + "tally.filters = [cell_filter]\n", + "tally.scores = ['scatter-y2']\n", + "tally.nuclides = [u235, u238]\n", "\n", "# Add mesh and tally to TalliesFile\n", "tallies_file.add_tally(tally)" @@ -503,7 +497,7 @@ "cell_type": "code", "execution_count": 18, "metadata": { - "collapsed": true + "collapsed": false }, "outputs": [], "source": [ @@ -512,14 +506,13 @@ "\n", "# Instantiate tally Trigger for kicks\n", "trigger = openmc.Trigger(trigger_type='std_dev', threshold=5e-5)\n", - "trigger.add_score('absorption')\n", + "trigger.scores = ['absorption']\n", "\n", "# Instantiate the Tally\n", "tally = openmc.Tally(name='distribcell tally')\n", - "tally.add_filter(distribcell_filter)\n", - "tally.add_score('absorption')\n", - "tally.add_score('scatter')\n", - "tally.add_trigger(trigger)\n", + "tally.filters = [distribcell_filter]\n", + "tally.scores = ['absorption', 'scatter']\n", + "tally.triggers = [trigger]\n", "\n", "# Add mesh and tally to TalliesFile\n", "tallies_file.add_tally(tally)" @@ -571,8 +564,9 @@ " Copyright: 2011-2015 Massachusetts Institute of Technology\n", " License: http://mit-crpg.github.io/openmc/license.html\n", " Version: 0.7.1\n", - " Git SHA1: ea9fb637f63f9374c7436456141afa850b84acf9\n", - " Date/Time: 2016-01-14 07:08:19\n", + " Git SHA1: eeb5091ca3a34cc85df73a3318cae2b6c7097413\n", + " Date/Time: 2016-04-13 11:40:02\n", + " MPI Processes: 1\n", "\n", " ===========================================================================\n", " ========================> INITIALIZATION <=========================\n", @@ -599,35 +593,34 @@ "\n", " Bat./Gen. k Average k \n", " ========= ======== ==================== \n", - " 1/1 0.54958 \n", - " 2/1 0.67628 \n", - " 3/1 0.70618 \n", - " 4/1 0.66601 \n", - " 5/1 0.70876 \n", - " 6/1 0.69708 \n", - " 7/1 0.68623 0.69166 +/- 0.00543\n", - " 8/1 0.69159 0.69163 +/- 0.00313\n", - " 9/1 0.69908 0.69349 +/- 0.00289\n", - " 10/1 0.63865 0.68253 +/- 0.01120\n", - " 11/1 0.65439 0.67784 +/- 0.01027\n", - " 12/1 0.68518 0.67889 +/- 0.00875\n", - " 13/1 0.69507 0.68091 +/- 0.00784\n", - " 14/1 0.70129 0.68317 +/- 0.00728\n", - " 15/1 0.71336 0.68619 +/- 0.00717\n", - " 16/1 0.68725 0.68629 +/- 0.00649\n", - " 17/1 0.72579 0.68958 +/- 0.00678\n", - " 18/1 0.67149 0.68819 +/- 0.00639\n", - " 19/1 0.67771 0.68744 +/- 0.00596\n", - " 20/1 0.68035 0.68697 +/- 0.00557\n", - " Triggers unsatisfied, max unc./thresh. is 1.09851 for absorption in tally 10002\n", - " The estimated number of batches is 24\n", + " 1/1 0.55921 \n", + " 2/1 0.63816 \n", + " 3/1 0.68834 \n", + " 4/1 0.71192 \n", + " 5/1 0.67935 \n", + " 6/1 0.68274 \n", + " 7/1 0.66339 0.67307 +/- 0.00967\n", + " 8/1 0.65835 0.66816 +/- 0.00743\n", + " 9/1 0.66697 0.66786 +/- 0.00527\n", + " 10/1 0.70498 0.67528 +/- 0.00847\n", + " 11/1 0.68596 0.67706 +/- 0.00714\n", + " 12/1 0.68481 0.67817 +/- 0.00614\n", + " 13/1 0.68369 0.67886 +/- 0.00536\n", + " 14/1 0.68785 0.67986 +/- 0.00483\n", + " 15/1 0.66145 0.67802 +/- 0.00470\n", + " 16/1 0.71831 0.68168 +/- 0.00561\n", + " 17/1 0.68428 0.68190 +/- 0.00512\n", + " 18/1 0.67527 0.68139 +/- 0.00474\n", + " 19/1 0.68166 0.68141 +/- 0.00439\n", + " 20/1 0.65475 0.67963 +/- 0.00446\n", + " Triggers unsatisfied, max unc./thresh. is 1.07581 for absorption in tally 10002\n", + " The estimated number of batches is 23\n", " Creating state point statepoint.020.h5...\n", - " 21/1 0.68105 0.68660 +/- 0.00522\n", - " 22/1 0.67168 0.68572 +/- 0.00498\n", - " 23/1 0.67520 0.68514 +/- 0.00473\n", - " 24/1 0.67940 0.68483 +/- 0.00449\n", - " Triggers satisfied for batch 24\n", - " Creating state point statepoint.024.h5...\n", + " 21/1 0.64538 0.67749 +/- 0.00469\n", + " 22/1 0.73275 0.68074 +/- 0.00547\n", + " 23/1 0.71674 0.68274 +/- 0.00553\n", + " Triggers satisfied for batch 23\n", + " Creating state point statepoint.023.h5...\n", "\n", " ===========================================================================\n", " ======================> SIMULATION FINISHED <======================\n", @@ -636,28 +629,28 @@ "\n", " =======================> TIMING STATISTICS <=======================\n", "\n", - " Total time for initialization = 1.2110E+00 seconds\n", - " Reading cross sections = 9.4900E-01 seconds\n", - " Total time in simulation = 1.0453E+01 seconds\n", - " Time in transport only = 1.0440E+01 seconds\n", - " Time in inactive batches = 1.5590E+00 seconds\n", - " Time in active batches = 8.8940E+00 seconds\n", - " Time synchronizing fission bank = 4.0000E-03 seconds\n", - " Sampling source sites = 3.0000E-03 seconds\n", - " SEND/RECV source sites = 1.0000E-03 seconds\n", + " Total time for initialization = 3.7900E-01 seconds\n", + " Reading cross sections = 8.6000E-02 seconds\n", + " Total time in simulation = 8.7310E+00 seconds\n", + " Time in transport only = 8.7200E+00 seconds\n", + " Time in inactive batches = 1.3230E+00 seconds\n", + " Time in active batches = 7.4080E+00 seconds\n", + " Time synchronizing fission bank = 2.0000E-03 seconds\n", + " Sampling source sites = 1.0000E-03 seconds\n", + " SEND/RECV source sites = 0.0000E+00 seconds\n", " Time accumulating tallies = 0.0000E+00 seconds\n", " Total time for finalization = 0.0000E+00 seconds\n", - " Total time elapsed = 1.1681E+01 seconds\n", - " Calculation Rate (inactive) = 8017.96 neutrons/second\n", - " Calculation Rate (active) = 4216.33 neutrons/second\n", + " Total time elapsed = 9.1240E+00 seconds\n", + " Calculation Rate (inactive) = 9448.22 neutrons/second\n", + " Calculation Rate (active) = 5062.10 neutrons/second\n", "\n", " ============================> RESULTS <============================\n", "\n", - " k-effective (Collision) = 0.68264 +/- 0.00405\n", - " k-effective (Track-length) = 0.68483 +/- 0.00449\n", - " k-effective (Absorption) = 0.68225 +/- 0.00336\n", - " Combined k-effective = 0.68275 +/- 0.00346\n", - " Leakage Fraction = 0.34345 +/- 0.00167\n", + " k-effective (Collision) = 0.67952 +/- 0.00434\n", + " k-effective (Track-length) = 0.68274 +/- 0.00553\n", + " k-effective (Absorption) = 0.68095 +/- 0.00369\n", + " Combined k-effective = 0.67994 +/- 0.00349\n", + " Leakage Fraction = 0.34133 +/- 0.00332\n", "\n" ] }, @@ -700,7 +693,7 @@ "statepoints = glob.glob('statepoint.*.h5')\n", "\n", "# Load the last statepoint file\n", - "sp = StatePoint(statepoints[-1])" + "sp = openmc.StatePoint(statepoints[-1])" ] }, { @@ -713,7 +706,7 @@ "outputs": [], "source": [ "# Load the summary file and link with statepoint\n", - "su = Summary('summary.h5')\n", + "su = openmc.Summary('summary.h5')\n", "sp.link_with_summary(su)" ] }, @@ -774,13 +767,13 @@ "name": "stdout", "output_type": "stream", "text": [ - "[[[ 0.21161313]]\n", + "[[[ 0.1508711 ]]\n", "\n", - " [[ 0.07979747]]\n", + " [[ 0.05389822]]\n", "\n", - " [[ 0.40532194]]\n", + " [[ 0.19633 ]]\n", "\n", - " [[ 0.19458598]]]\n" + " [[ 0.12963172]]]\n" ] } ], @@ -803,13 +796,14 @@ { "data": { "text/html": [ - "
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mesh 1energy [MeV]energy low [MeV]energy high [MeV]scoremeanstd. dev.
111(0.0e+00 - 6.3e-07)0.00e+006.25e-07fission0.0001650.0000352.34e-043.54e-05
1111(0.0e+00 - 6.3e-07)0.00e+006.25e-07nu-fission0.0004030.0000855.71e-048.62e-05
2111(6.3e-07 - 2.0e+01)6.25e-072.00e+01fission0.0000770.0000047.03e-057.05e-06
3111(6.3e-07 - 2.0e+01)6.25e-072.00e+01nu-fission0.0002070.0000111.87e-041.76e-05
4121(0.0e+00 - 6.3e-07)0.00e+006.25e-07fission0.0003500.0000433.67e-043.61e-05
5121(0.0e+00 - 6.3e-07)0.00e+006.25e-07nu-fission0.0008530.0001058.94e-048.80e-05
6121(6.3e-07 - 2.0e+01)6.25e-072.00e+01fission0.0001060.0000151.04e-045.36e-06
7121(6.3e-07 - 2.0e+01)6.25e-072.00e+01nu-fission0.0002740.0000392.76e-041.40e-05
8131(0.0e+00 - 6.3e-07)0.00e+006.25e-07fission0.0005520.0000606.04e-045.57e-05
9131(0.0e+00 - 6.3e-07)0.00e+006.25e-07nu-fission0.0013460.0001461.47e-031.36e-04
10131(6.3e-07 - 2.0e+01)6.25e-072.00e+01fission0.0001480.0000081.41e-046.69e-06
11131(6.3e-07 - 2.0e+01)6.25e-072.00e+01nu-fission0.0003840.0000213.72e-041.82e-05
12141(0.0e+00 - 6.3e-07)0.00e+006.25e-07fission0.0006820.0000546.45e-044.59e-05
13141(0.0e+00 - 6.3e-07)0.00e+006.25e-07nu-fission0.0016620.0001321.57e-031.12e-04
14141(6.3e-07 - 2.0e+01)6.25e-072.00e+01fission0.0001620.0000121.82e-049.37e-06
15141(6.3e-07 - 2.0e+01)6.25e-072.00e+01nu-fission0.0004240.0000314.76e-042.47e-05
16151(0.0e+00 - 6.3e-07)0.00e+006.25e-07fission0.0009110.0000767.28e-047.49e-05
17151(0.0e+00 - 6.3e-07)0.00e+006.25e-07nu-fission0.0022210.0001861.77e-031.83e-04
18151(6.3e-07 - 2.0e+01)6.25e-072.00e+01fission0.0001780.0000131.81e-041.04e-05
19151(6.3e-07 - 2.0e+01)6.25e-072.00e+01nu-fission0.0004640.0000324.72e-042.67e-05
\n", "
" ], "text/plain": [ - " mesh 1 energy [MeV] score mean std. dev.\n", - " x y z \n", - "0 1 1 1 (0.0e+00 - 6.3e-07) fission 0.000165 0.000035\n", - "1 1 1 1 (0.0e+00 - 6.3e-07) nu-fission 0.000403 0.000085\n", - "2 1 1 1 (6.3e-07 - 2.0e+01) fission 0.000077 0.000004\n", - "3 1 1 1 (6.3e-07 - 2.0e+01) nu-fission 0.000207 0.000011\n", - "4 1 2 1 (0.0e+00 - 6.3e-07) fission 0.000350 0.000043\n", - "5 1 2 1 (0.0e+00 - 6.3e-07) nu-fission 0.000853 0.000105\n", - "6 1 2 1 (6.3e-07 - 2.0e+01) fission 0.000106 0.000015\n", - "7 1 2 1 (6.3e-07 - 2.0e+01) nu-fission 0.000274 0.000039\n", - "8 1 3 1 (0.0e+00 - 6.3e-07) fission 0.000552 0.000060\n", - "9 1 3 1 (0.0e+00 - 6.3e-07) nu-fission 0.001346 0.000146\n", - "10 1 3 1 (6.3e-07 - 2.0e+01) fission 0.000148 0.000008\n", - "11 1 3 1 (6.3e-07 - 2.0e+01) nu-fission 0.000384 0.000021\n", - "12 1 4 1 (0.0e+00 - 6.3e-07) fission 0.000682 0.000054\n", - "13 1 4 1 (0.0e+00 - 6.3e-07) nu-fission 0.001662 0.000132\n", - "14 1 4 1 (6.3e-07 - 2.0e+01) fission 0.000162 0.000012\n", - "15 1 4 1 (6.3e-07 - 2.0e+01) nu-fission 0.000424 0.000031\n", - "16 1 5 1 (0.0e+00 - 6.3e-07) fission 0.000911 0.000076\n", - "17 1 5 1 (0.0e+00 - 6.3e-07) nu-fission 0.002221 0.000186\n", - "18 1 5 1 (6.3e-07 - 2.0e+01) fission 0.000178 0.000013\n", - "19 1 5 1 (6.3e-07 - 2.0e+01) nu-fission 0.000464 0.000032" + " mesh 1 energy low [MeV] energy high [MeV] score mean \\\n", + " x y z \n", + "0 1 1 1 0.00e+00 6.25e-07 fission 2.34e-04 \n", + "1 1 1 1 0.00e+00 6.25e-07 nu-fission 5.71e-04 \n", + "2 1 1 1 6.25e-07 2.00e+01 fission 7.03e-05 \n", + "3 1 1 1 6.25e-07 2.00e+01 nu-fission 1.87e-04 \n", + "4 1 2 1 0.00e+00 6.25e-07 fission 3.67e-04 \n", + "5 1 2 1 0.00e+00 6.25e-07 nu-fission 8.94e-04 \n", + "6 1 2 1 6.25e-07 2.00e+01 fission 1.04e-04 \n", + "7 1 2 1 6.25e-07 2.00e+01 nu-fission 2.76e-04 \n", + "8 1 3 1 0.00e+00 6.25e-07 fission 6.04e-04 \n", + "9 1 3 1 0.00e+00 6.25e-07 nu-fission 1.47e-03 \n", + "10 1 3 1 6.25e-07 2.00e+01 fission 1.41e-04 \n", + "11 1 3 1 6.25e-07 2.00e+01 nu-fission 3.72e-04 \n", + "12 1 4 1 0.00e+00 6.25e-07 fission 6.45e-04 \n", + "13 1 4 1 0.00e+00 6.25e-07 nu-fission 1.57e-03 \n", + "14 1 4 1 6.25e-07 2.00e+01 fission 1.82e-04 \n", + "15 1 4 1 6.25e-07 2.00e+01 nu-fission 4.76e-04 \n", + "16 1 5 1 0.00e+00 6.25e-07 fission 7.28e-04 \n", + "17 1 5 1 0.00e+00 6.25e-07 nu-fission 1.77e-03 \n", + "18 1 5 1 6.25e-07 2.00e+01 fission 1.81e-04 \n", + "19 1 5 1 6.25e-07 2.00e+01 nu-fission 4.72e-04 \n", + "\n", + " std. dev. \n", + " \n", + "0 3.54e-05 \n", + "1 8.62e-05 \n", + "2 7.05e-06 \n", + "3 1.76e-05 \n", + "4 3.61e-05 \n", + "5 8.80e-05 \n", + "6 5.36e-06 \n", + "7 1.40e-05 \n", + "8 5.57e-05 \n", + "9 1.36e-04 \n", + "10 6.69e-06 \n", + "11 1.82e-05 \n", + "12 4.59e-05 \n", + "13 1.12e-04 \n", + "14 9.37e-06 \n", + "15 2.47e-05 \n", + "16 7.49e-05 \n", + "17 1.83e-04 \n", + "18 1.04e-05 \n", + "19 2.67e-05 " ] }, "execution_count": 25, @@ -1064,6 +1102,10 @@ "# Get a pandas dataframe for the mesh tally data\n", "df = tally.get_pandas_dataframe(nuclides=False)\n", "\n", + "# Set the Pandas float display settings\n", + "import pandas as pd\n", + "pd.set_option('display.float_format', '{:.2e}'.format)\n", + "\n", "# Print the first twenty rows in the dataframe\n", "df.head(20)" ] @@ -1077,9 +1119,9 @@ "outputs": [ { "data": { - "image/png": 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8WtJB4DlgSUTsO+qtNrMJzX1PNZ8iil62GDskxXis91hXKpXc0rBxRQIfCkaHJCLiiOaG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\ni8CTEfEFSVcDUyP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"text/plain": [ - "" + "" ] }, "metadata": {}, @@ -1102,26 +1144,18 @@ { "data": { "text/plain": [ - "" + "" ] }, "execution_count": 27, "metadata": {}, "output_type": "execute_result" }, - { - "name": "stderr", - "output_type": "stream", - "text": [ - "/usr/local/lib/python2.7/dist-packages/matplotlib/collections.py:590: FutureWarning: elementwise comparison failed; returning scalar instead, but in the future will perform elementwise comparison\n", - " if self._edgecolors == str('face'):\n" - ] - }, { "data": { - "image/png": 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33sJ/DJxVuO24MQ9WamvQqt/TnAqsrXm/Dji5hTpTgSktxNabAtTOPrNrX6VG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\nAAAASUVORK5CYII=\n", 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"text/plain": [ - "" + "" ] }, "metadata": {}, @@ -1131,7 +1165,7 @@ "source": [ "# Extract thermal nu-fission rates from pandas\n", "fiss = df[df['score'] == 'nu-fission']\n", - "fiss = fiss[fiss['energy [MeV]'] == '(0.0e+00 - 6.3e-07)']\n", + "fiss = fiss[fiss['energy low [MeV]'] == 0.0]\n", "\n", "# Extract mean and reshape as 2D NumPy arrays\n", "mean = fiss['mean'].reshape((17,17))\n", @@ -1191,7 +1225,7 @@ { "data": { "text/html": [ - "
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10000U-235scatter-Y0,00.0380270.0013503.86e-021.11e-03
110000U-235scatter-Y1,-10.0000710.0003832.75e-042.96e-04
210000U-235scatter-Y1,0-0.0005790.000250-5.55e-054.33e-04
310000U-235scatter-Y1,1-0.0001760.000282-4.22e-043.51e-04
410000U-235scatter-Y2,-20.0001050.0002245.88e-052.04e-04
510000U-235scatter-Y2,-1-0.0000770.0002211.00e-042.49e-04
610000U-235scatter-Y2,00.0001340.000181-8.09e-051.59e-04
710000U-235scatter-Y2,1-0.0001170.0003081.93e-042.14e-04
810000U-235scatter-Y2,20.0000390.0002111.12e-041.86e-04
910000U-238scatter-Y0,02.3409870.0143102.34e+001.34e-02
1010000U-238scatter-Y1,-10.0228170.0024582.32e-022.97e-03
1110000U-238scatter-Y1,00.0015890.0030517.50e-042.55e-03
1210000U-238scatter-Y1,1-0.0271460.002511-2.73e-023.28e-03
1310000U-238scatter-Y2,-2-0.0041460.001722-2.36e-031.21e-03
1410000U-238scatter-Y2,-10.0017650.002474-1.80e-041.49e-03
1510000U-238scatter-Y2,00.0060380.0019173.23e-032.25e-03
1610000U-238scatter-Y2,10.0001670.0014383.75e-031.97e-03
1710000U-238scatter-Y2,2-0.0016840.0015352.07e-031.60e-03
\n", @@ -1354,24 +1388,24 @@ ], "text/plain": [ " cell nuclide score mean std. dev.\n", - "0 10000 U-235 scatter-Y0,0 0.038027 0.001350\n", - "1 10000 U-235 scatter-Y1,-1 0.000071 0.000383\n", - "2 10000 U-235 scatter-Y1,0 -0.000579 0.000250\n", - "3 10000 U-235 scatter-Y1,1 -0.000176 0.000282\n", - "4 10000 U-235 scatter-Y2,-2 0.000105 0.000224\n", - "5 10000 U-235 scatter-Y2,-1 -0.000077 0.000221\n", - "6 10000 U-235 scatter-Y2,0 0.000134 0.000181\n", - "7 10000 U-235 scatter-Y2,1 -0.000117 0.000308\n", - "8 10000 U-235 scatter-Y2,2 0.000039 0.000211\n", - "9 10000 U-238 scatter-Y0,0 2.340987 0.014310\n", - "10 10000 U-238 scatter-Y1,-1 0.022817 0.002458\n", - "11 10000 U-238 scatter-Y1,0 0.001589 0.003051\n", - "12 10000 U-238 scatter-Y1,1 -0.027146 0.002511\n", - "13 10000 U-238 scatter-Y2,-2 -0.004146 0.001722\n", - "14 10000 U-238 scatter-Y2,-1 0.001765 0.002474\n", - "15 10000 U-238 scatter-Y2,0 0.006038 0.001917\n", - "16 10000 U-238 scatter-Y2,1 0.000167 0.001438\n", - "17 10000 U-238 scatter-Y2,2 -0.001684 0.001535" + "0 10000 U-235 scatter-Y0,0 3.86e-02 1.11e-03\n", + "1 10000 U-235 scatter-Y1,-1 2.75e-04 2.96e-04\n", + "2 10000 U-235 scatter-Y1,0 -5.55e-05 4.33e-04\n", + "3 10000 U-235 scatter-Y1,1 -4.22e-04 3.51e-04\n", + "4 10000 U-235 scatter-Y2,-2 5.88e-05 2.04e-04\n", + "5 10000 U-235 scatter-Y2,-1 1.00e-04 2.49e-04\n", + "6 10000 U-235 scatter-Y2,0 -8.09e-05 1.59e-04\n", + "7 10000 U-235 scatter-Y2,1 1.93e-04 2.14e-04\n", + "8 10000 U-235 scatter-Y2,2 1.12e-04 1.86e-04\n", + "9 10000 U-238 scatter-Y0,0 2.34e+00 1.34e-02\n", + "10 10000 U-238 scatter-Y1,-1 2.32e-02 2.97e-03\n", + "11 10000 U-238 scatter-Y1,0 7.50e-04 2.55e-03\n", + "12 10000 U-238 scatter-Y1,1 -2.73e-02 3.28e-03\n", + "13 10000 U-238 scatter-Y2,-2 -2.36e-03 1.21e-03\n", + "14 10000 U-238 scatter-Y2,-1 -1.80e-04 1.49e-03\n", + "15 10000 U-238 scatter-Y2,0 3.23e-03 2.25e-03\n", + "16 10000 U-238 scatter-Y2,1 3.75e-03 1.97e-03\n", + "17 10000 U-238 scatter-Y2,2 2.07e-03 1.60e-03" ] }, "execution_count": 29, @@ -1405,8 +1439,8 @@ "name": "stdout", "output_type": "stream", "text": [ - "[[[ 0.00153535 0.0143096 ]\n", - " [ 0.00021107 0.00135025]]]\n" + "[[[ 0.00159927 0.01341406]\n", + " [ 0.00018637 0.00111048]]]\n" ] } ], @@ -1474,13 +1508,13 @@ "name": "stdout", "output_type": "stream", "text": [ - "[[[ 0.04318886]]]\n" + "[[[ 0.05767856]]]\n" ] } ], "source": [ "# Get the relative error for the scattering reaction rates in\n", - "# the first 30 distribcell instances \n", + "# the first 10 distribcell instances \n", "data = tally.get_values(scores=['scatter'], filters=['distribcell'],\n", " filter_bins=[(i,) for i in range(10)], value='rel_err')\n", "print(data)" @@ -1503,7 +1537,7 @@ { "data": { "text/html": [ - "
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576288absorption0.0001190.0000161.25e-049.59e-06
577288scatter0.0184820.0008612.01e-026.75e-04
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" ], "text/plain": [ - " distribcell score mean std. dev.\n", - "558 279 absorption 0.000102 0.000016\n", - "559 279 scatter 0.013889 0.000964\n", - "560 280 absorption 0.000087 0.000012\n", - "561 280 scatter 0.014347 0.000652\n", - "562 281 absorption 0.000087 0.000010\n", - "563 281 scatter 0.014283 0.000715\n", - "564 282 absorption 0.000111 0.000012\n", - "565 282 scatter 0.016374 0.000865\n", - "566 283 absorption 0.000090 0.000008\n", - "567 283 scatter 0.015839 0.000795\n", - "568 284 absorption 0.000103 0.000012\n", - "569 284 scatter 0.017182 0.000660\n", - "570 285 absorption 0.000111 0.000014\n", - "571 285 scatter 0.017565 0.000862\n", - "572 286 absorption 0.000125 0.000014\n", - "573 286 scatter 0.018128 0.000931\n", - "574 287 absorption 0.000124 0.000016\n", - "575 287 scatter 0.017253 0.000902\n", - "576 288 absorption 0.000119 0.000016\n", - "577 288 scatter 0.018482 0.000861" + " distribcell score mean std. dev.\n", + "558 279 absorption 8.19e-05 7.82e-06\n", + "559 279 scatter 1.33e-02 6.19e-04\n", + "560 280 absorption 1.00e-04 7.93e-06\n", + "561 280 scatter 1.40e-02 5.61e-04\n", + "562 281 absorption 9.52e-05 7.08e-06\n", + "563 281 scatter 1.51e-02 6.50e-04\n", + "564 282 absorption 9.85e-05 9.47e-06\n", + "565 282 scatter 1.53e-02 4.63e-04\n", + "566 283 absorption 1.08e-04 1.34e-05\n", + "567 283 scatter 1.65e-02 7.04e-04\n", + "568 284 absorption 1.13e-04 7.91e-06\n", + "569 284 scatter 1.67e-02 5.51e-04\n", + "570 285 absorption 1.23e-04 9.53e-06\n", + "571 285 scatter 1.88e-02 7.25e-04\n", + "572 286 absorption 1.44e-04 1.34e-05\n", + "573 286 scatter 1.90e-02 7.07e-04\n", + "574 287 absorption 1.26e-04 8.66e-06\n", + "575 287 scatter 1.97e-02 7.23e-04\n", + "576 288 absorption 1.25e-04 9.59e-06\n", + "577 288 scatter 2.01e-02 6.75e-04" ] }, "execution_count": 33, @@ -1713,7 +1747,7 @@ { "data": { "text/html": [ - "
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5771000301000116001000210000288scatter2.01e-026.75e-04
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" ], "text/plain": [ - " level 1 level 2 level 3 distribcell score \\\n", - " cell univ lat cell univ \n", - " id id id x y z id id \n", - "0 10003 0 10001 0 0 0 10002 10000 0 absorption \n", - "1 10003 0 10001 0 0 0 10002 10000 0 scatter \n", - "2 10003 0 10001 0 1 0 10002 10000 1 absorption \n", - "3 10003 0 10001 0 1 0 10002 10000 1 scatter \n", - "4 10003 0 10001 0 2 0 10002 10000 2 absorption \n", - "5 10003 0 10001 0 2 0 10002 10000 2 scatter \n", - "6 10003 0 10001 0 3 0 10002 10000 3 absorption \n", - "7 10003 0 10001 0 3 0 10002 10000 3 scatter \n", - "8 10003 0 10001 0 4 0 10002 10000 4 absorption \n", - "9 10003 0 10001 0 4 0 10002 10000 4 scatter \n", - "10 10003 0 10001 0 5 0 10002 10000 5 absorption \n", - "11 10003 0 10001 0 5 0 10002 10000 5 scatter \n", - "12 10003 0 10001 0 6 0 10002 10000 6 absorption \n", - "13 10003 0 10001 0 6 0 10002 10000 6 scatter \n", - "14 10003 0 10001 0 7 0 10002 10000 7 absorption \n", - "15 10003 0 10001 0 7 0 10002 10000 7 scatter \n", - "16 10003 0 10001 0 8 0 10002 10000 8 absorption \n", - "17 10003 0 10001 0 8 0 10002 10000 8 scatter \n", - "18 10003 0 10001 0 9 0 10002 10000 9 absorption \n", - "19 10003 0 10001 0 9 0 10002 10000 9 scatter \n", + " level 1 level 2 level 3 distribcell score \\\n", + " cell univ lat cell univ \n", + " id id id x y z id id \n", + "558 10003 0 10001 16 9 0 10002 10000 279 absorption \n", + "559 10003 0 10001 16 9 0 10002 10000 279 scatter \n", + "560 10003 0 10001 16 8 0 10002 10000 280 absorption \n", + "561 10003 0 10001 16 8 0 10002 10000 280 scatter \n", + "562 10003 0 10001 16 7 0 10002 10000 281 absorption \n", + "563 10003 0 10001 16 7 0 10002 10000 281 scatter \n", + "564 10003 0 10001 16 6 0 10002 10000 282 absorption \n", + "565 10003 0 10001 16 6 0 10002 10000 282 scatter \n", + "566 10003 0 10001 16 5 0 10002 10000 283 absorption \n", + "567 10003 0 10001 16 5 0 10002 10000 283 scatter \n", + "568 10003 0 10001 16 4 0 10002 10000 284 absorption \n", + "569 10003 0 10001 16 4 0 10002 10000 284 scatter \n", + "570 10003 0 10001 16 3 0 10002 10000 285 absorption \n", + "571 10003 0 10001 16 3 0 10002 10000 285 scatter \n", + "572 10003 0 10001 16 2 0 10002 10000 286 absorption \n", + "573 10003 0 10001 16 2 0 10002 10000 286 scatter \n", + "574 10003 0 10001 16 1 0 10002 10000 287 absorption \n", + "575 10003 0 10001 16 1 0 10002 10000 287 scatter \n", + "576 10003 0 10001 16 0 0 10002 10000 288 absorption \n", + "577 10003 0 10001 16 0 0 10002 10000 288 scatter \n", "\n", " mean std. dev. \n", " \n", " \n", - "0 0.000113 0.000013 \n", - "1 0.017337 0.000749 \n", - "2 0.000204 0.000021 \n", - "3 0.027631 0.001348 \n", - "4 0.000319 0.000025 \n", - "5 0.040052 0.001427 \n", - "6 0.000388 0.000022 \n", - "7 0.048578 0.001561 \n", - "8 0.000511 0.000030 \n", - "9 0.057903 0.001988 \n", - "10 0.000481 0.000033 \n", - "11 0.061211 0.001989 \n", - "12 0.000542 0.000045 \n", - "13 0.070888 0.002497 \n", - "14 0.000587 0.000047 \n", - "15 0.078107 0.002794 \n", - "16 0.000627 0.000033 \n", - "17 0.082031 0.001740 \n", - "18 0.000667 0.000028 \n", - "19 0.088516 0.002037 " + "558 8.19e-05 7.82e-06 \n", + "559 1.33e-02 6.19e-04 \n", + "560 1.00e-04 7.93e-06 \n", + "561 1.40e-02 5.61e-04 \n", + "562 9.52e-05 7.08e-06 \n", + "563 1.51e-02 6.50e-04 \n", + "564 9.85e-05 9.47e-06 \n", + "565 1.53e-02 4.63e-04 \n", + "566 1.08e-04 1.34e-05 \n", + "567 1.65e-02 7.04e-04 \n", + "568 1.13e-04 7.91e-06 \n", + "569 1.67e-02 5.51e-04 \n", + "570 1.23e-04 9.53e-06 \n", + "571 1.88e-02 7.25e-04 \n", + "572 1.44e-04 1.34e-05 \n", + "573 1.90e-02 7.07e-04 \n", + "574 1.26e-04 8.66e-06 \n", + "575 1.97e-02 7.23e-04 \n", + "576 1.25e-04 9.59e-06 \n", + "577 2.01e-02 6.75e-04 " ] }, "execution_count": 34, @@ -2119,7 +2153,7 @@ "df = tally.get_pandas_dataframe(summary=su, nuclides=False)\n", "\n", "# Print the last twenty rows in the dataframe\n", - "df.head(20)" + "df.tail(20)" ] }, { @@ -2132,7 +2166,7 @@ { "data": { "text/html": [ - "
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count289.000000289.0000002.89e+022.89e+02
mean0.0004190.0000244.19e-042.24e-05
std0.0002370.0000102.42e-049.14e-06
min0.0000150.0000031.90e-053.44e-06
25%0.0002070.0000172.02e-041.56e-05
50%0.0004150.0000234.05e-042.20e-05
75%0.0006150.0000306.07e-042.89e-05
max0.0009010.0000559.19e-044.95e-05
\n", "
" ], "text/plain": [ - " mean std. dev.\n", - " \n", - " \n", - "count 289.000000 289.000000\n", - "mean 0.000419 0.000024\n", - "std 0.000237 0.000010\n", - "min 0.000015 0.000003\n", - "25% 0.000207 0.000017\n", - "50% 0.000415 0.000023\n", - "75% 0.000615 0.000030\n", - "max 0.000901 0.000055" + " mean std. dev.\n", + " \n", + " \n", + "count 2.89e+02 2.89e+02\n", + "mean 4.19e-04 2.24e-05\n", + "std 2.42e-04 9.14e-06\n", + "min 1.90e-05 3.44e-06\n", + "25% 2.02e-04 1.56e-05\n", + "50% 4.05e-04 2.20e-05\n", + "75% 6.07e-04 2.89e-05\n", + "max 9.19e-04 4.95e-05" ] }, "execution_count": 35, @@ -2242,15 +2276,15 @@ "name": "stdout", "output_type": "stream", "text": [ - "Mann-Whitney Test p-value: 0.456115837774\n" + "Mann-Whitney Test p-value: 0.303583331507\n" ] } ], "source": [ - "# Extract tally data from pins in the pins divided along y=x diagonal \n", + "# Extract tally data from pins in the pins divided along y=-x diagonal\n", "multi_index = ('level 2', 'lat',)\n", - "lower = df[df[multi_index + ('x',)] + df[multi_index + ('y',)] < 16]\n", - "upper = df[df[multi_index + ('x',)] + df[multi_index + ('y',)] > 16]\n", + "lower = df[df[multi_index + ('x',)] > df[multi_index + ('y',)]]\n", + "upper = df[df[multi_index + ('x',)] < df[multi_index + ('y',)]]\n", "lower = lower[lower['score'] == 'absorption']\n", "upper = upper[upper['score'] == 'absorption']\n", "\n", @@ -2280,15 +2314,15 @@ "name": "stdout", "output_type": "stream", "text": [ - "Mann-Whitney Test p-value: 4.59783355073e-42\n" + "Mann-Whitney Test p-value: 6.038663783e-42\n" ] } ], "source": [ - "# Extract tally data from pins in the pins divided along y=-x diagonal\n", + "# Extract tally data from pins in the pins divided along y=x diagonal \n", "multi_index = ('level 2', 'lat',)\n", - "lower = df[df[multi_index + ('x',)] > df[multi_index + ('y',)]]\n", - "upper = df[df[multi_index + ('x',)] < df[multi_index + ('y',)]]\n", + "lower = df[df[multi_index + ('x',)] + df[multi_index + ('y',)] < 16]\n", + "upper = df[df[multi_index + ('x',)] + df[multi_index + ('y',)] > 16]\n", "lower = lower[lower['score'] == 'absorption']\n", "upper = upper[upper['score'] == 'absorption']\n", "\n", @@ -2316,17 +2350,17 @@ "name": "stderr", "output_type": "stream", "text": [ - "/usr/local/lib/python2.7/dist-packages/ipykernel/__main__.py:4: SettingWithCopyWarning: \n", + "/usr/local/lib/python2.7/dist-packages/IPython/kernel/__main__.py:4: SettingWithCopyWarning: \n", "A value is trying to be set on a copy of a slice from a DataFrame.\n", "Try using .loc[row_indexer,col_indexer] = value instead\n", "\n", - "See the the caveats in the documentation: http://pandas.pydata.org/pandas-docs/stable/indexing.html#indexing-view-versus-copy\n" + "See the caveats in the documentation: http://pandas.pydata.org/pandas-docs/stable/indexing.html#indexing-view-versus-copy\n" ] }, { "data": { "text/plain": [ - "" + "" ] }, "execution_count": 38, @@ -2335,9 +2369,9 @@ }, { "data": { - "image/png": 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lFF22YsUKr6ur9/Hjp3pd3SkFV0uljlFXV++jRx+RMb7mtnBsTktadVpV1YSs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\navaycuWdAJHPaE1aN/DMxN7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DHPbPqAORFIssKZjZMjObY2azzGxGVHFI6ryz7B36dO0TdRiSrELgkOdiT8eT\nOiPKMwUHTnL3w9396AjjkBTYuXsnU5ZP4aTck6IORZK1AViXBwe8EXUkkkJRNx9p3OQ6YubKmXRp\n1oVWjVtFHYpURuEgOHR01FFICtWL8NgOTDKzXcBj7j4iwlgkJK+++iqbNm3i5a9fpsPODjzzzDNR\nhySV8Z9z4Sc3QcNvYVvUwUgqRJkUjnf3VWbWCnjLzBa4+5Tilf37949vmJeXR35+fhQxhmLq1KlR\nhxCqxPpdeeWNbNmSz44Bs8n+uCvvfqY7ZWuVLfvGHpma9wJ8AgUFBVFHVC2Z9n9v3rx5zJ8/v0b3\nGVlScPdVwb/rzOxF4GggnhSef/75qEJLiYEDB0YdQqiK63f99bezoeh+aH8Mu595nR1bdwMtow1O\nKqdwEPQcAZ9kxuc2E+pQnpp4ZGok1xTMrJGZ5QTzjYFTiPV1kEzUYQ58fRBsbRF1JFIVn/aNPWOh\nSdSBSCpEdaG5DTDFzD4BPgRecfeJEcUiYes6HZaqK2qttXNvWHAmdI86EEmFSJqP3H0p0COKY0sE\ncj+ED26LOgqpjsJB8JMno45CUiDqLqmS4Tx7N3QohM9PjDoUqY6lP4IcWPDVgqgjkZApKUiotrfb\nCqsPhu05UYci1eHZUAij5+iehUynpCCh2t5pMyzSWUJGKITRhaNx18ipmUxJQUK1rfNmWHxC1GFI\nTVgFe9Xbi2krNHJqJlNSkNB8sfELdu+9E1aq20qmmP/MfI6//HjMLD5JZlFSkNBMXDyRBisaxdqj\nJTMULoFDWkLWdvQAnsykpCCheXPxmzT8olHUYUhN2tA1diPiAW9GHYmERElBQrFr9y4mLZkUO1OQ\nzDLnAo2cmsGUFCQUM76cQYemHcj+LsoxFyUU886FA1+HBkVRRyIhUFKQUIz/dDx9D+obdRgShs0t\nYzcj5r0YdSQSAiUFCcXLn77MGd3OiDoMCYuakDKWkoLUuNXbV7Nh6waO6nBU1KFIWBb2hQ4zNHJq\nBlJSkBo387uZ9OvWjyzTxytj7WgEn/bTyKkZSP9rpcZ9tOkjNR3VBXMugEOjDkJqmpKC1Ki1361l\nxfYV9Omq5ydkvKV9oCl8+tWnUUciNUhJQWrUuHnj6NG4Bw3rNYw6FAmbZ8Pc2CB5kjmUFKRGFRQW\ncFzOcVGHIakyB56a/RS7du+KOhKpIUoKUmM+3/A5C75awKGN1NBcZ6yCdjntmLBwQtSRSA1RUpAa\nM3buWM6mJdosAAAJv0lEQVTJP4d6pruY65Jrjr6G4R8OjzoMqSFKClIj3J2nC59m4KEDow5FUqx/\nfn8WfLWAwjWFUYciNUBJQWrE9BXT2bZzGyd21lPW6poG2Q244sgreHDGg1GHIjVASUFqxGMzH2Po\nEUP10JU6augRQ3lu3nOs3rQ66lCkmpQUpNrWb1nPy5++zCU9Lok6FIlImyZtuODQC7j3g3ujDkWq\nSUlBqm3U7FGcdsBptGzUMupQJEI3nXATI2eNZN1366IORapBSUGqZceuHdw//X6u7XVt1KFIxDo2\n7ch5h5zHfdPuizoUqQYlBamWsXPHsn+L/enVsVfUoUgauPmEm3n848dZWbQy6lCkipQUpMp27d7F\nn6b+iZtPuDnqUCRNdGnehSE9h3Dr27dGHYpUkZKCVNnowtE026sZJ+93ctShSBq55cRbeGPRG8xc\nOTPqUKQKlBSkSrbs2MJv3/4tfzn5L+qGKiU0bdiUu/rcxeWvXs7O3TujDkcqSUlBquQvH/yFI9sf\nyXGdNPidfN/gHoPZZ+99+PPUP0cdilSSkoJU2ty1c3lwxoMMP03j3UjZzIwRfUdw//T7+XjVx1GH\nI5WgpCCVsm3nNga/PJi7+txFx6Ydow5H0ljnZp15+KcP0//Z/ny1+auow5EkKSlIpVzz+jV0btaZ\nIT2HRB2K1ALnHnIu5x1yHj9/7uds3bk16nAkCUoKkrT7pt3H+8vf54kzntDFZUnaXX3uYt9G+3LO\ns+ewfdf2qMORPVBSkKQM/3A4D854kIkXTKRpw6ZRhyO1SHZWNgVnF9AguwF9x/Rl/Zb1UYckFYgk\nKZjZqWa2wMw+M7OboohBkrNt5zaufu1qHvnoEd6+6G06NesUdUhSC9XPrs+z5z5LXss8ev29ly4+\np7GUJwUzywYeAk4F8oHzzSwv1XFEad68eVGHkJQpn0/hiMePYEXRCqZfOp2uLbomVa621E9Sq15W\nPf566l8ZdtIwTht9Gte/eX3KB8/TZ3PPojhTOBpY5O7L3H0HMBY4I4I4IjN//vyoQyjXlh1bGDdv\nHH1G9eHily7mt71/yws/f4FmezVLeh/pXD+J3sBDB1J4RSGbd2ym20PduPLVK5n2xTTcPfRj67O5\nZ1E8TLcD8EXC6xWARlNLMXenaHsRyzYsY8n6JcxdO5epX0xl+orpHNHuCC7pcQnndz+f+tn1ow5V\nMlDrxq159PRH+W3v3/LErCcY/PJg1m9dT+8uvenVoRcH7XsQB+5zIO1y2tGsYTN1bEihKJJC+D8H\n0tjwD4czNXcqPx39UxyP/zoqni/9b0XrPPhTJrtut+/m223fsmHrBr7d9i171duLLs27sH+L/em2\nbzeG9hzKU2c+RavGrWqsvtnZ0KTJULKymgTxbKeoqMZ2L7Vcx6Yd+d0Pf8fvfvg7Pt/wOVOWT+Gj\nlR/xzrJ3+Ozrz1i9aTVbdm6hxV4taNqwKQ3rNaRBdgMaZsf+bZDdIJ4wDCsxD3xv3czcmZxecHqJ\ndZVx+RGX87ODflYTVU9blopTthIHNDsGGObupwavfwPsdvc/JWxTpxOHiEhVuXu1TquiSAr1gE+B\nHwMrgRnA+e6uxj4RkYilvPnI3Xea2VXAm0A2MFIJQUQkPaT8TEFERNJXZHc0m9k+ZvaWmS00s4lm\n1ryc7f5hZmvMrLAq5aNSifqVeSOfmQ0zsxVmNiuYTk1d9OVL5sZDMxserJ9tZodXpmyUqlm3ZWY2\nJ3ivZqQu6uTtqX5mdrCZTTOzrWb268qUTQfVrF8mvH+Dgs/lHDObamaHJVu2BHePZAL+DNwYzN8E\n/LGc7U4EDgcKq1I+netHrPlsEZAL1Ac+AfKCdbcD10ddj2TjTdjmp8BrwXwvYHqyZWtr3YLXS4F9\noq5HNevXCjgS+APw68qUjXqqTv0y6P07FmgWzJ9a1f97UY591A8YFcyPAs4sayN3nwKUNVhKUuUj\nlEx8e7qRL906Zydz42G83u7+IdDczNomWTZKVa1bm4T16fZ+Jdpj/dx9nbt/BOyobNk0UJ36Favt\n7980d98YvPwQ6Jhs2URRJoU27r4mmF8DtKlo4xDKhy2Z+Mq6ka9Dwuurg9PBkWnSPLaneCvapn0S\nZaNUnbpB7P6bSWb2kZml47jiydQvjLKpUt0YM+39uxR4rSplQ+19ZGZvAW3LWHVr4gt39+rcm1Dd\n8lVVA/WrKOZHgDuC+TuBe4m90VFK9m+czr+4ylPdup3g7ivNrBXwlpktCM5y00V1/n/Uht4o1Y3x\neHdflQnvn5n9CPgFcHxly0LIScHdTy5vXXDxuK27rzazdsDaSu6+uuWrrQbq9yWQOOxoJ2JZHHeP\nb29mfwcm1EzU1VJuvBVs0zHYpn4SZaNU1bp9CeDuK4N/15nZi8RO2dPpSyWZ+oVRNlWqFaO7rwr+\nrdXvX3BxeQRwqruvr0zZYlE2H40HLg7mLwZeSnH5sCUT30fAgWaWa2YNgPOCcgSJpNhZQGEZ5VOt\n3HgTjAcugvjd6xuCZrRkykapynUzs0ZmlhMsbwycQnq8X4kq8/cvfTaU7u8dVKN+mfL+mVln4AXg\nAndfVJmyJUR4NX0fYBKwEJgINA+WtwdeTdhuDLE7n7cRaxcbXFH5dJkqUb/TiN3hvQj4TcLyp4A5\nwGxiCaVN1HUqL17gMuCyhG0eCtbPBnruqa7pMlW1bsB+xHp0fALMTce6JVM/Yk2hXwAbiXXuWA40\nqQ3vXXXql0Hv39+Br4FZwTSjorLlTbp5TURE4vQ4ThERiVNSEBGROCUFERGJU1IQEZE4JQUREYlT\nUhARkTglBanTzGy3mf0z4XU9M1tnZulwB7lIyikpSF33HXCIme0VvD6Z2BAAuoFH6iQlBZHYaJI/\nC+bPJ3YXvUFs2AOLPejpQzP72Mz6Bctzzex9M5sZTMcGy08ys3fN7Dkzm29mT0dRIZGqUlIQgWeA\nAWbWEDiU2Fj0xW4FJrt7L6AP8Bcza0RsOPST3f0IYAAwPKFMD+BaIB/Yz8yOR6SWCHWUVJHawN0L\nzSyX2FnCq6VWnwL0NbMbgtcNiY0yuRp4yMx+AOwCDkwoM8ODUVPN7BNiT7yaGlb8IjVJSUEkZjxw\nD/BDYo9tTHS2u3+WuMDMhgGr3P1CM8sGtias3pYwvwv9P5NaRM1HIjH/AIa5+39KLX8TuKb4hZkd\nHsw2JXa2ALHhtLNDj1AkBZQUpK5zAHf/0t0fSlhW3PvoTqC+mc0xs7nA74PlDwMXB81D3YBNpfdZ\nwWuRtKWhs0VEJE5nCiIiEqekICIicUoKIiISp6QgIiJxSgoiIhKnpCAiInFKCiIiEqekICIicf8f\nReuGFnegfMcAAAAASUVORK5CYII=\n", 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DlnoznkkeyJPJ/qpSks3oorJstUPi00rHX03uFWEkUtbX3oa7Sn7FgYX/j5ML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\nSUVORK5CYII=\n", "text/plain": [ - "" + "" ] }, "metadata": {}, @@ -2408,7 +2442,7 @@ "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython2", - "version": "2.7.10" + "version": "2.7.6" } }, "nbformat": 4, diff --git a/docs/source/pythonapi/examples/post-processing.ipynb b/docs/source/pythonapi/examples/post-processing.ipynb index 7fbca6864..0dc18d5a2 100644 --- a/docs/source/pythonapi/examples/post-processing.ipynb +++ b/docs/source/pythonapi/examples/post-processing.ipynb @@ -15,16 +15,12 @@ }, "outputs": [], "source": [ + "%matplotlib inline\n", "from IPython.display import Image\n", "import numpy as np\n", "import matplotlib.pyplot as plt\n", "\n", - "import openmc\n", - "from openmc.statepoint import StatePoint\n", - "from openmc.source import Source\n", - "from openmc.stats import Box\n", - "\n", - "%matplotlib inline" + "import openmc" ] }, { @@ -273,9 +269,11 @@ "settings_file.batches = batches\n", "settings_file.inactive = inactive\n", "settings_file.particles = particles\n", - "source_bounds = [-0.63, -0.63, -0.63, 0.63, 0.63, 0.63]\n", - "settings_file.source = Source(space=Box(\n", - " source_bounds[:3], source_bounds[3:]))\n", + "\n", + "# Create an initial uniform spatial source distribution over fissionable zones\n", + "bounds = [-0.63, -0.63, -0.63, 0.63, 0.63, 0.63]\n", + "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n", + "settings_file.source = openmc.source.Source(space=uniform_dist)\n", "\n", "# Export to \"settings.xml\"\n", "settings_file.export_to_xml()" @@ -350,7 +348,7 @@ "outputs": [ { "data": { - "image/png": "iVBORw0KGgoAAAANSUhEUgAAAPoAAAD6AgMAAAD1grKuAAAABGdBTUEAALGPC/xhBQAAACBjSFJN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\nFMTl8QAAAABJRU5ErkJggg==\n", + "image/png": "iVBORw0KGgoAAAANSUhEUgAAAPoAAAD6AgMAAAD1grKuAAAABGdBTUEAALGPC/xhBQAAAAFzUkdC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\nVDExOjMyOjU1LTA0OjAwoL4U5gAAAABJRU5ErkJggg==\n", "text/plain": [ "" ] @@ -408,9 +406,8 @@ "\n", "# Create mesh tally to score flux and fission rate\n", "tally = openmc.Tally(name='flux')\n", - "tally.add_filter(mesh_filter)\n", - "tally.add_score('flux')\n", - "tally.add_score('fission')\n", + "tally.filters = [mesh_filter]\n", + "tally.scores = ['flux', 'fission']\n", "tallies_file.add_tally(tally)" ] }, @@ -461,8 +458,9 @@ " Copyright: 2011-2015 Massachusetts Institute of Technology\n", " License: http://mit-crpg.github.io/openmc/license.html\n", " Version: 0.7.1\n", - " Git SHA1: ea9fb637f63f9374c7436456141afa850b84acf9\n", - " Date/Time: 2016-01-14 07:02:06\n", + " Git SHA1: eeb5091ca3a34cc85df73a3318cae2b6c7097413\n", + " Date/Time: 2016-04-13 11:32:56\n", + " MPI Processes: 1\n", "\n", " ===========================================================================\n", " ========================> INITIALIZATION <=========================\n", @@ -489,106 +487,106 @@ "\n", " Bat./Gen. k Average k \n", " ========= ======== ==================== \n", - " 1/1 1.04894 \n", - " 2/1 1.01711 \n", - " 3/1 1.05357 \n", - " 4/1 1.03052 \n", - " 5/1 1.06523 \n", - " 6/1 1.06806 \n", - " 7/1 1.05161 \n", - " 8/1 1.04199 \n", - " 9/1 1.05010 \n", - " 10/1 1.04617 \n", - " 11/1 1.04894 \n", - " 12/1 1.06806 1.05850 +/- 0.00956\n", - " 13/1 1.05002 1.05567 +/- 0.00620\n", - " 14/1 1.03471 1.05043 +/- 0.00683\n", - " 15/1 1.01803 1.04395 +/- 0.00837\n", - " 16/1 1.05588 1.04594 +/- 0.00712\n", - " 17/1 1.07503 1.05010 +/- 0.00731\n", - " 18/1 1.02786 1.04732 +/- 0.00691\n", - " 19/1 1.00071 1.04214 +/- 0.00800\n", - " 20/1 1.05587 1.04351 +/- 0.00729\n", - " 21/1 1.03886 1.04309 +/- 0.00660\n", - " 22/1 1.04335 1.04311 +/- 0.00603\n", - " 23/1 1.04057 1.04292 +/- 0.00555\n", - " 24/1 1.01976 1.04126 +/- 0.00540\n", - " 25/1 1.05811 1.04238 +/- 0.00515\n", - " 26/1 1.02351 1.04120 +/- 0.00496\n", - " 27/1 1.05261 1.04188 +/- 0.00471\n", - " 28/1 1.03355 1.04141 +/- 0.00446\n", - " 29/1 1.02797 1.04071 +/- 0.00428\n", - " 30/1 1.03758 1.04055 +/- 0.00406\n", - " 31/1 1.04883 1.04094 +/- 0.00388\n", - " 32/1 1.03557 1.04070 +/- 0.00371\n", - " 33/1 1.02947 1.04021 +/- 0.00358\n", - " 34/1 1.03651 1.04006 +/- 0.00343\n", - " 35/1 1.03331 1.03979 +/- 0.00330\n", - " 36/1 1.05947 1.04054 +/- 0.00326\n", - " 37/1 1.05093 1.04093 +/- 0.00316\n", - " 38/1 1.06787 1.04189 +/- 0.00319\n", - " 39/1 1.01451 1.04095 +/- 0.00322\n", - " 40/1 1.02351 1.04037 +/- 0.00317\n", - " 41/1 1.04826 1.04062 +/- 0.00307\n", - " 42/1 1.04228 1.04067 +/- 0.00298\n", - " 43/1 1.03214 1.04041 +/- 0.00290\n", - " 44/1 1.04950 1.04068 +/- 0.00282\n", - " 45/1 1.06616 1.04141 +/- 0.00284\n", - " 46/1 1.07039 1.04221 +/- 0.00287\n", - " 47/1 1.00292 1.04115 +/- 0.00299\n", - " 48/1 1.04477 1.04125 +/- 0.00291\n", - " 49/1 1.03360 1.04105 +/- 0.00284\n", - " 50/1 1.04783 1.04122 +/- 0.00277\n", - " 51/1 1.03985 1.04119 +/- 0.00271\n", - " 52/1 1.02507 1.04080 +/- 0.00267\n", - " 53/1 1.03477 1.04066 +/- 0.00261\n", - " 54/1 1.00412 1.03983 +/- 0.00268\n", - " 55/1 1.02239 1.03945 +/- 0.00265\n", - " 56/1 1.04308 1.03952 +/- 0.00259\n", - " 57/1 1.05534 1.03986 +/- 0.00256\n", - " 58/1 1.06667 1.04042 +/- 0.00257\n", - " 59/1 1.06458 1.04091 +/- 0.00256\n", - " 60/1 1.00304 1.04015 +/- 0.00262\n", - " 61/1 1.05038 1.04036 +/- 0.00258\n", - " 62/1 1.02904 1.04014 +/- 0.00254\n", - " 63/1 1.00249 1.03943 +/- 0.00259\n", - " 64/1 1.01779 1.03903 +/- 0.00257\n", - " 65/1 1.05335 1.03929 +/- 0.00254\n", - " 66/1 1.06231 1.03970 +/- 0.00253\n", - " 67/1 1.02382 1.03942 +/- 0.00250\n", - " 68/1 1.03796 1.03939 +/- 0.00245\n", - " 69/1 1.03672 1.03935 +/- 0.00241\n", - " 70/1 1.02926 1.03918 +/- 0.00238\n", - " 71/1 1.05834 1.03950 +/- 0.00236\n", - " 72/1 1.04332 1.03956 +/- 0.00232\n", - " 73/1 1.05613 1.03982 +/- 0.00230\n", - " 74/1 1.01963 1.03950 +/- 0.00228\n", - " 75/1 1.02228 1.03924 +/- 0.00226\n", - " 76/1 1.04842 1.03938 +/- 0.00223\n", - " 77/1 1.02157 1.03911 +/- 0.00222\n", - " 78/1 1.02810 1.03895 +/- 0.00219\n", - " 79/1 1.05030 1.03912 +/- 0.00216\n", - " 80/1 1.02391 1.03890 +/- 0.00214\n", - " 81/1 1.02488 1.03870 +/- 0.00212\n", - " 82/1 1.04957 1.03885 +/- 0.00210\n", - " 83/1 1.03499 1.03880 +/- 0.00207\n", - " 84/1 1.05922 1.03907 +/- 0.00206\n", - " 85/1 1.05898 1.03934 +/- 0.00205\n", - " 86/1 1.02242 1.03912 +/- 0.00204\n", - " 87/1 1.03278 1.03904 +/- 0.00201\n", - " 88/1 1.06134 1.03932 +/- 0.00201\n", - " 89/1 1.04521 1.03940 +/- 0.00198\n", - " 90/1 1.04277 1.03944 +/- 0.00196\n", - " 91/1 1.04214 1.03947 +/- 0.00193\n", - " 92/1 1.05610 1.03967 +/- 0.00192\n", - " 93/1 1.04531 1.03974 +/- 0.00190\n", - " 94/1 1.01534 1.03945 +/- 0.00190\n", - " 95/1 1.03971 1.03945 +/- 0.00187\n", - " 96/1 1.07183 1.03983 +/- 0.00189\n", - " 97/1 1.07214 1.04020 +/- 0.00191\n", - " 98/1 1.03710 1.04017 +/- 0.00188\n", - " 99/1 1.02532 1.04000 +/- 0.00187\n", - " 100/1 1.03965 1.04000 +/- 0.00185\n", + " 1/1 1.04359 \n", + " 2/1 1.04244 \n", + " 3/1 1.03020 \n", + " 4/1 1.03630 \n", + " 5/1 1.06478 \n", + " 6/1 1.05450 \n", + " 7/1 1.02369 \n", + " 8/1 1.03614 \n", + " 9/1 1.05193 \n", + " 10/1 1.02886 \n", + " 11/1 1.05011 \n", + " 12/1 1.04597 1.04804 +/- 0.00207\n", + " 13/1 1.07035 1.05548 +/- 0.00753\n", + " 14/1 1.06150 1.05698 +/- 0.00554\n", + " 15/1 1.07094 1.05977 +/- 0.00512\n", + " 16/1 1.05131 1.05836 +/- 0.00441\n", + " 17/1 1.04733 1.05679 +/- 0.00405\n", + " 18/1 1.08130 1.05985 +/- 0.00465\n", + " 19/1 1.02559 1.05605 +/- 0.00560\n", + " 20/1 1.03399 1.05384 +/- 0.00547\n", + " 21/1 1.04617 1.05314 +/- 0.00500\n", + " 22/1 1.06981 1.05453 +/- 0.00477\n", + " 23/1 1.05270 1.05439 +/- 0.00439\n", + " 24/1 1.02487 1.05228 +/- 0.00458\n", + " 25/1 1.05905 1.05273 +/- 0.00429\n", + " 26/1 1.07658 1.05422 +/- 0.00428\n", + " 27/1 1.03455 1.05307 +/- 0.00418\n", + " 28/1 1.00971 1.05066 +/- 0.00462\n", + " 29/1 1.06111 1.05121 +/- 0.00440\n", + " 30/1 1.01777 1.04954 +/- 0.00450\n", + " 31/1 1.04718 1.04942 +/- 0.00428\n", + " 32/1 1.03340 1.04870 +/- 0.00415\n", + " 33/1 1.04570 1.04857 +/- 0.00397\n", + " 34/1 1.02728 1.04768 +/- 0.00390\n", + " 35/1 1.02852 1.04691 +/- 0.00382\n", + " 36/1 1.03242 1.04636 +/- 0.00371\n", + " 37/1 1.01479 1.04519 +/- 0.00376\n", + " 38/1 1.06045 1.04573 +/- 0.00366\n", + " 39/1 1.03810 1.04547 +/- 0.00354\n", + " 40/1 1.05281 1.04571 +/- 0.00343\n", + " 41/1 1.03941 1.04551 +/- 0.00332\n", + " 42/1 1.04049 1.04535 +/- 0.00322\n", + " 43/1 1.04586 1.04537 +/- 0.00312\n", + " 44/1 1.05437 1.04563 +/- 0.00304\n", + " 45/1 1.03445 1.04531 +/- 0.00297\n", + " 46/1 1.05104 1.04547 +/- 0.00289\n", + " 47/1 1.00773 1.04445 +/- 0.00299\n", + " 48/1 1.06879 1.04509 +/- 0.00298\n", + " 49/1 1.06625 1.04564 +/- 0.00295\n", + " 50/1 1.02641 1.04515 +/- 0.00292\n", + " 51/1 1.05701 1.04544 +/- 0.00286\n", + " 52/1 1.02868 1.04504 +/- 0.00282\n", + " 53/1 1.04592 1.04506 +/- 0.00275\n", + " 54/1 1.05757 1.04535 +/- 0.00271\n", + " 55/1 1.02329 1.04486 +/- 0.00269\n", + " 56/1 1.04116 1.04478 +/- 0.00263\n", + " 57/1 1.01990 1.04425 +/- 0.00263\n", + " 58/1 1.06202 1.04462 +/- 0.00260\n", + " 59/1 1.03550 1.04443 +/- 0.00255\n", + " 60/1 1.01383 1.04382 +/- 0.00258\n", + " 61/1 1.04111 1.04377 +/- 0.00253\n", + " 62/1 1.02061 1.04332 +/- 0.00252\n", + " 63/1 1.00456 1.04259 +/- 0.00257\n", + " 64/1 1.02277 1.04222 +/- 0.00255\n", + " 65/1 1.04544 1.04228 +/- 0.00251\n", + " 66/1 1.04487 1.04233 +/- 0.00246\n", + " 67/1 1.02699 1.04206 +/- 0.00243\n", + " 68/1 1.06160 1.04240 +/- 0.00241\n", + " 69/1 1.02989 1.04218 +/- 0.00238\n", + " 70/1 1.03107 1.04200 +/- 0.00235\n", + " 71/1 1.06571 1.04239 +/- 0.00234\n", + " 72/1 1.03444 1.04226 +/- 0.00231\n", + " 73/1 1.05059 1.04239 +/- 0.00228\n", + " 74/1 1.03352 1.04225 +/- 0.00224\n", + " 75/1 1.03707 1.04217 +/- 0.00221\n", + " 76/1 1.02994 1.04199 +/- 0.00219\n", + " 77/1 1.05416 1.04217 +/- 0.00216\n", + " 78/1 1.03794 1.04211 +/- 0.00213\n", + " 79/1 1.04652 1.04217 +/- 0.00210\n", + " 80/1 1.05715 1.04239 +/- 0.00208\n", + " 81/1 1.08146 1.04294 +/- 0.00212\n", + " 82/1 1.02159 1.04264 +/- 0.00211\n", + " 83/1 1.01968 1.04233 +/- 0.00211\n", + " 84/1 1.05577 1.04251 +/- 0.00209\n", + " 85/1 1.07808 1.04298 +/- 0.00211\n", + " 86/1 1.03943 1.04293 +/- 0.00209\n", + " 87/1 1.03431 1.04282 +/- 0.00206\n", + " 88/1 1.02414 1.04258 +/- 0.00205\n", + " 89/1 1.02316 1.04234 +/- 0.00204\n", + " 90/1 1.03342 1.04223 +/- 0.00202\n", + " 91/1 1.02781 1.04205 +/- 0.00200\n", + " 92/1 1.01293 1.04169 +/- 0.00201\n", + " 93/1 1.04347 1.04171 +/- 0.00198\n", + " 94/1 1.05357 1.04186 +/- 0.00196\n", + " 95/1 1.04740 1.04192 +/- 0.00194\n", + " 96/1 1.05215 1.04204 +/- 0.00192\n", + " 97/1 1.06667 1.04232 +/- 0.00192\n", + " 98/1 1.04926 1.04240 +/- 0.00190\n", + " 99/1 1.05386 1.04253 +/- 0.00188\n", + " 100/1 1.05088 1.04262 +/- 0.00186\n", " Creating state point statepoint.100.h5...\n", "\n", " ===========================================================================\n", @@ -598,27 +596,27 @@ "\n", " =======================> TIMING STATISTICS <=======================\n", "\n", - " Total time for initialization = 3.6000E-01 seconds\n", - " Reading cross sections = 1.0600E-01 seconds\n", - " Total time in simulation = 2.5756E+02 seconds\n", - " Time in transport only = 2.5751E+02 seconds\n", - " Time in inactive batches = 9.7270E+00 seconds\n", - " Time in active batches = 2.4783E+02 seconds\n", - " Time synchronizing fission bank = 2.1000E-02 seconds\n", - " Sampling source sites = 1.3000E-02 seconds\n", - " SEND/RECV source sites = 8.0000E-03 seconds\n", - " Time accumulating tallies = 1.3000E-02 seconds\n", - " Total time for finalization = 1.4600E-01 seconds\n", - " Total time elapsed = 2.5809E+02 seconds\n", - " Calculation Rate (inactive) = 5140.33 neutrons/second\n", - " Calculation Rate (active) = 1815.75 neutrons/second\n", + " Total time for initialization = 3.8100E-01 seconds\n", + " Reading cross sections = 8.6000E-02 seconds\n", + " Total time in simulation = 2.4400E+02 seconds\n", + " Time in transport only = 2.4395E+02 seconds\n", + " Time in inactive batches = 8.3260E+00 seconds\n", + " Time in active batches = 2.3567E+02 seconds\n", + " Time synchronizing fission bank = 1.6000E-02 seconds\n", + " Sampling source sites = 6.0000E-03 seconds\n", + " SEND/RECV source sites = 7.0000E-03 seconds\n", + " Time accumulating tallies = 1.9000E-02 seconds\n", + " Total time for finalization = 1.7400E-01 seconds\n", + " Total time elapsed = 2.4458E+02 seconds\n", + " Calculation Rate (inactive) = 6005.28 neutrons/second\n", + " Calculation Rate (active) = 1909.46 neutrons/second\n", "\n", " ============================> RESULTS <============================\n", "\n", - " k-effective (Collision) = 1.03912 +/- 0.00160\n", - " k-effective (Track-length) = 1.04000 +/- 0.00185\n", - " k-effective (Absorption) = 1.04240 +/- 0.00156\n", - " Combined k-effective = 1.04078 +/- 0.00127\n", + " k-effective (Collision) = 1.04214 +/- 0.00161\n", + " k-effective (Track-length) = 1.04262 +/- 0.00186\n", + " k-effective (Absorption) = 1.04338 +/- 0.00158\n", + " Combined k-effective = 1.04278 +/- 0.00122\n", " Leakage Fraction = 0.00000 +/- 0.00000\n", "\n" ] @@ -663,7 +661,7 @@ "outputs": [], "source": [ "# Load the statepoint file\n", - "sp = StatePoint('statepoint.100.h5')" + "sp = openmc.StatePoint('statepoint.100.h5')" ] }, { @@ -718,18 +716,18 @@ { "data": { "text/plain": [ - "array([[[ 0.4107676 , 0. ]],\n", + "array([[[ 0.40945685, 0. ]],\n", "\n", - " [[ 0.40849402, 0. ]],\n", + " [[ 0.40939021, 0. ]],\n", "\n", - " [[ 0.41014343, 0. ]],\n", + " [[ 0.410625 , 0. ]],\n", "\n", " ..., \n", - " [[ 0.41049467, 0. ]],\n", + " [[ 0.41130501, 0. ]],\n", "\n", - " [[ 0.40982242, 0. ]],\n", + " [[ 0.41228849, 0. ]],\n", "\n", - " [[ 0.40996987, 0. ]]])" + " [[ 0.41420317, 0. ]]])" ] }, "execution_count": 20, @@ -765,30 +763,30 @@ { "data": { "text/plain": [ - "(array([[[ 0.00456408, 0. ]],\n", + "(array([[[ 0.00454952, 0. ]],\n", " \n", - " [[ 0.00453882, 0. ]],\n", + " [[ 0.00454878, 0. ]],\n", " \n", - " [[ 0.00455715, 0. ]],\n", + " [[ 0.0045625 , 0. ]],\n", " \n", " ..., \n", - " [[ 0.00456105, 0. ]],\n", + " [[ 0.00457006, 0. ]],\n", " \n", - " [[ 0.00455358, 0. ]],\n", + " [[ 0.00458098, 0. ]],\n", " \n", - " [[ 0.00455522, 0. ]]]),\n", - " array([[[ 1.95085625e-05, 0.00000000e+00]],\n", + " [[ 0.00460226, 0. ]]]),\n", + " array([[[ 1.64748193e-05, 0.00000000e+00]],\n", " \n", - " [[ 1.78129859e-05, 0.00000000e+00]],\n", + " [[ 1.70922989e-05, 0.00000000e+00]],\n", " \n", - " [[ 1.89709648e-05, 0.00000000e+00]],\n", + " [[ 1.67622385e-05, 0.00000000e+00]],\n", " \n", " ..., \n", - " [[ 1.56286612e-05, 0.00000000e+00]],\n", + " [[ 1.69274948e-05, 0.00000000e+00]],\n", " \n", - " [[ 1.65813279e-05, 0.00000000e+00]],\n", + " [[ 1.57842763e-05, 0.00000000e+00]],\n", " \n", - " [[ 1.67530331e-05, 0.00000000e+00]]]))" + " [[ 2.06590062e-05, 0.00000000e+00]]]))" ] }, "execution_count": 21, @@ -820,7 +818,7 @@ "output_type": "stream", "text": [ "Tally\n", - "\tID =\t10000\n", + "\tID =\t10001\n", "\tName =\t\n", "\tFilters =\t\n", " \t\tmesh\t[10000]\n", @@ -868,7 +866,7 @@ { "data": { "text/plain": [ - "" + "" ] }, "execution_count": 24, @@ -877,9 +875,9 @@ }, { "data": { - "image/png": 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Yr9Q/xbCa5inP2+SJ4KTLV8U3aTi8XB17kj98LomVU/C3m4z611GcPRqyly4a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\nLjAFNhpx8reeoGFzET+yyjCzlBb9bL7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iMlLCwDArSILGbeUwvcIabqNCCTsKTUKkKeDF\nqZaYEG9yMXMeLwUOSbdZo4dNqYusHsFLAS+t8PxuYQ0H1QcumA1smAhsZbvYqHTT07uMQy0/7KH7\nA2NqvwPnUR8xb5qT61d5hK8wP2uyZbxbqrA2S4uGFthaGnY7+/5umrRl7XKGVc9oq9PuMULb+S0A\nt1i35cMt0wJ6i6lb+nb7OYXdi92eBK+4ygk5wXGxn0L8OMnng5RvFmisvL9gqw+CPXTAzk6H0MtB\nUu4wZclNwfDyMfHbnHW9Rdi1jUcosmQeYc3s4V+Gf5sjwi1SQpgQaZqCwmXhFJt0kibEmzyOKjVI\nGp2ktzopVL1sq3FunjyCw1PGTg0XJY5znWFhnnPqn5Kgh1scAcCbKrBxxWSi5y5nY2/STYIkHWQJ\n0s0aH8+8zIn8LUS3wWogRsyzxT/l9wgX8gRTBcSaTj4aJO/w4RaLNHN2Cqs+To5eo+GXeYmPYrKJ\nnToBstipksXPPQ5yWLqDTdJwkcFHHok6VZwwZaJMaUTceTBMUKv8zM6XWPPFSLpDyB4NYiAbGsOO\nWXZoZQXsYBsbNfpYxkkFb7bM/oUcnoaTfJ8DZ7zClLSPy9IxNqUYaUJUcWAg0kOCCTZJ7eaaXmKA\nb4jP8xhv8Qwvs0wfTUWm4ZO47DzGhtLBc7zAV5qfYY0uBmyLjI/f5sDYXexGldUvXWHMU+eycIov\nD3+W/JCPsJjiI3yH41znRfFZHFQ5otwiPRAiKGQZ5z4+CvSHlxGDBnaxwn3GmGaUAZYIkmGNbnpI\nkMfPyzzD2sYAjlSTsdgMBdX7N4y8vzfL3E+FGPitAT723/wmQ6+9xVXdpE6LmSrsacjtICzTmvCr\nsTeRaEka1sSf2FbXKpN2+22yB9IWsFogawXZaLTkFasf64HRbu16tsLehCRtf63zW7p6yoDVhsnR\nN36X0POP8uLn/zWL/3KZ9B9u/C3u3gfLHjpgG2mZyht+phqH0WIK4j6de8EJIrYkG0YXc5tj2MQa\n/6Tj9znbuER/I0G9niDpCbFq6yJJB04q2KoNLm6dJxBIg27SXJTxxnIEe3fwerL4lDyd2hZPp1+j\nV13hddJkmWCyMc6t+hGedbzI/u55nD9SZaMrxnWOo1Knky32M4eIgehvsmzroq+xTjiZo7Tt4ds9\nz1JzOwjKOcb1SXocy/x3/N9s0cEV6SxTNh8Hm/fpaGwQUXe4yQwH8BNhh0g1S09lm85KGj0Im9Eo\niU90k+5spYeq4qDr0CYdvTtocQmPu4h3sIARESl7baCY5A660AYENCQuB0+RpIOmqfB6+QnCQop+\n1wrhXA5/uoSsGbgSNQq4WO3uI1zKMtJc4KXwR7FJdWJsUcVBGRcr9HKMG7uLIbsRMCji4SLnWKOL\ngJyj7rRhl6oEybBOF4PyIgeocY6LiKKJIJqoNLgmznNOKOKlwBHxJhI6efyY0EoFQMujY6PRxezc\nAbQ5lYWNUUIfT3K8+zrP1l/BqVXIyT78rjxeCjR3f4YyGiIm+5mhsu2jkPBTPW2nguthD90Pvdn8\ncPhzIgO+28R/5SuEbkxi6I13AaQFABbgtjNhpa3cqmPfbVtjD4wt2cMCbNhj6pbUYu7Waa/naGtr\nSSrtGvZ75Zl2KabWdp72sPd2QDf1BsGbkzz2L36HoQP7WPxXEW79J6jn/3b384NgD3+JMFeWgeYk\nm8U4FY8Te7NK01RQs02imynWzRpx3zrPCC+zr7qEo1angZ2K4SSPjxIePBSJGCnWG/3kdD+GKbRk\nBleaodAM3bReoQNmjlFtBp+U23UrspHRg6xU+ijWfXTaN5g4epM5hijXXPgyRXS/hGTTGWvMsmjr\nY92I0Z3Ywl2v4HTWWTN6WLL3IdoN1okRKabwbRVxB0ts2btZC/QRkLOMNaeJNlOs6W78hkBUT1HV\n3ThKDcZXZtgqh1mK9DA9vp+aaMcwJUTDpB5XycfdJKUoml/GYVbZ35ijLqrkZS+1uA0HNQxELppn\nSTR7kRom95vjDMiLZAgS0vP4KGMqDdS0hiSZ5Lp9xI0k/doKI+YsboqESLNJJ8v0PZCObDSo4aCO\njRz+BwsJ6KZEw7DhlsoUaK3WHpW2CZMiuDvxq9CksfuzLuFGxCBEmhApatiZ5CD3GSFAFht1KrqL\n3GaI5FqMZK6DZ5vfYp+2yNHqHZJChLqo0s0aIgYGIm5KFHYXTu5nhaIrSNoXxisVKTb+nmH/debt\ng+5jOoeHtxi8ewf/H196kMfD+mtJH+3yhAXYFqOV2ZtghD3Gq/JuZtxuUtumttVt0ALaZtsxcfdz\no60NvBvA21m61NbGAn4L2K2t3XPFuZpk6I9fJPgvzuA4OEHxqQjrN2TyK+8rQPbvzB7+ijMn7/HP\nPv4qXzJ/krscxBRETqhXefTm2/i+WaX4D/6EYsxJ2XSh5A226eCV7ifQxZZ+aSLgI4/PmSe+b517\n4kHu1w9gTIgEfBnGmOI0l6niYF3p4o3YIziFMknu0UeeMCkaho0vrv0Mh1y3+cTo15DQGEot8/zF\nl/m9U/+Y6x1ejm1PYgRVSnkPxlsi7AfnQIWD8iQaIgsM8U2eJ7MaxTan80uP/j6x4Dqd7lVSgp9m\n3sbI9iKF5qMktRjRcpYvOc9jmBI/tfgVoitp8j1+Ns52M6TOMWZO0dnYwtmsUxD8bLliXBDOk9Ii\n/Gbmf0FyCCz6B8kRQKGJjMYl8yzT5XHqaTf7OyaJupJs0okWkKliwwxMgWkiFgzsRo1qUMVjpvlV\n6d/RRCFDkBscQ6VOhiCzjJAizDZRBAwOc4dxJukgSXdji3hhhynfPup2G9Vd3/QaNu5zgBFm8FBg\njR4u4eFVfrGVQ5ssfazwBBeo0Eo9++N8mTGmMJC4IZ4hf9xL7GCCTzm+wlONC5hNkUv+U6za44TI\n7Ppw73CQu8wwQhkXXvKcfOQSom7gtpd4LfXRhz10P9S27xNw/pdrdP7aBdxvLCHR8uCw5Ih2LdoC\nXEsaMdo+t4OoScvlT6KV5bod6EXezYrb27W77LV7hMAeA7cYt0AL1Ou77SztWuPdDwhLHrGCdKwJ\nT4nWWwDsRVPWAfn/uUHnExk+/jvP8dp/8HL99/8esL+rKXITl1IhleogXYtho85qRx8X+wSKz/kY\nj9/BIxXQBYlCwMmGEGVG2o+IgZ8cB7jPfQ4wrY2xUe4iYwtQbTgwtkXWpvt4U3mS5WMDuAIlnFKF\nQWmBGElSbNNkBK9S4AnvBVJiB4PKHGe4zDH9Jj53gdoRCTGoYW/UkJIG14TjXHA+zmvnnuKj4ZeZ\n8NzmlH6ZVaGbC0I3yWoMr79EbCzJq9VniJU2eM75AgdXptFMhXcix1HkJp2ZLaRJg/WD3VSCNtKn\nPOiCTMbtQ5QMVBrogsSiMkBvdZNAPs+JpdssRIZIdnQw5R2mQ96in2WmcLJDhDIu+oQVwo40ekgl\nYEuxX5jjEHfIiz6W3X1cjThwHokjyRqCojFcXyRfi/DHzZ/F704TcSbZopPZ0hjJaieP+S9wXL6O\nbGpMigfoZbW1Og4FfJUC6madoD3NiH2GIFk2iZElQBUHKnWcVKngpI8l+nmBd3jkQdCMnXor7SwL\nDxbXjSrbdO1foWETcHmK/CXPsUYP494p7qgH2RBiSBgc4g4BslRw0rOziawJpKIhCqoXAwk7NWzu\nysMeuh9KkztUQr8Yp8s1SfTfvoJ6ZwOx3HjAZmGPNbfnArGiCy1PDotlW0zbqqvwVwNhLN26PQDG\nAvB21mvwVyUMi9GrvFuvlnm3RGI9aN77UGl/2FjntlwK28ulcgP77U2k33qN6MDTdP6rcVJ/tEVz\n26r54bCHDtg1wUHC7GGn1kGh5MdhVLmmnGbSN872uQjr5Ri9lQQOV5ltb4QNutggjoSGjkjn7uTY\nfHmI2ckDBHtSeN1FitUwO5sxclqQjbEYMf8G/SyzjwVs1BHRW37OcoZH5bfIufyM1GcZz9zHsAuk\n1DCvhx9Hs0vYqxVuiYe4ZR7hov0sb448hqkaeKU0Hc0dfGYeN2UEfYvRwDTD0Xku7jyBo1nltHmZ\n7so6KXuIhWA/Ae7RX0nTKCtUNQdlr53KAZUSHtL40Xclh6Lgpio5sIk66CKBQo5R7wxp0c+Cqx+n\nUaJPX2ZeHEYTZEwEOoVNZJsGNtB3gauJTBOZNVsX17xxyvsOEyZNHyv062tUmm7eqJ8nZE8ywn0A\n6podoSJwwJxmwnUbh6OC38xiE+rIaKQI08SOzdRQzCZxNuk3V7gkPEKGIGWc6LtDR0ckRJYRZrnM\naQRMBEwyBHFSoY9ltuhEQqcpK8S7E0g0HkgmBdkHskmKEDkClHBzuHwXt1lGd8p4GlU89RKGKVHG\nRVn3UKz6sCnVv27Y/XBawId9n5eRgzUGLi/i+aNbwF+d1GsHy3Z92opatACbtrJ2YG3vQ+bd7Nlg\nD9QtKUVq68sKnLHqN3m3i58F0ip7mroVcWldr9Xeusb3BtgI76nzoL/1IuIf3qH3l4eonN5HcbiD\nZrMA2Q+PqP3QAXtL6eDb8gGqnTK2YplqxsG3557HG87iGU1zb+kYXiXP4OgMLlquWiXc2KkxzzBv\n8Rg26iibGnxRZPjj83Q+vk6mO0bDYcNGjSH/HAEpg4MaRTzcZYJJFM4h0k0CD6VWNr7MJqHJIvcm\nRnjB/Dj/8dY/48cmvky4M8lvTPwbZKnJQGOZe8ljXA6cQw5ojKuTeCnwk8IXsbnrDJtz9LHCiehV\nRMHAIxbIDzupiQoRY4eB8gpDjjrZp1x47Vk8CDioUsBHBSc5/KzRjdsscbR5kxnXKNddR4h1bdEr\nL9HNMt/gRyloPvyNIgWHF5dU4iD3uMlRtokioSNgkCTK2zzCKa5QwMcCXuAAgyzioUjO6cHlKPGU\n+W12xDA17PSxQo93Da9Q5Il7F6mE7SyNDDDBXXL4ucxp7nCIbv8aP+L+Bk1FwWFW8RoFyqKLlBAh\nh4914hiISOis0UWJ82QIoaGwxAApQvjJ4aTCDhFW6WWGESa4S5RttogRY4sYm4RIU8KNgImPPOMr\n0xxoztIcE1iO9jPFMDnJj45Mvubn+uIZHo+8+rCH7ofPDh/AfbSDx3/n1+hfuvIu3bd9AtBgDwCt\n9xSZlq+z1caSJyzAtADQAj877w6QsRi45TXSDpbQkiUs+QLe7SJo7beDNeyFplvpWuHdAG9NYlp6\nN7zbT9z67o62NiZw6I9fIvB2jqmnfoeSugmvvfPX3NQPlj10wO6WEojCCB61QGnDS/VtD8W6h0ZI\nobzjonzLi94tURu100Ni1xfXQZIO1rPdLM6OMNJ/n87IBs2P2QgN7SCVdLhm4oiXcR4okLX7yRUD\nSCUTPSwxqC5g12pcvXUGu6PGoX03OXR7ErMm8mb/I3y79Bxv5J9kvdLNhtZFBZV5BhkUl+hRE4T9\nWc7IlzhVvUKHtsO8OkDWFsApVtg2WwvtRoUkaUK8w2kMm0QRDxkzyDxeSkofXe5VRAwUmrzNOao4\nmGsO83b5UQYci5RUN4vSACtiPxtCHJdS5iwX2c8sIjpZyc+K2kuXsE4WP2kzzJnqNUwBMnYfHdkU\nC8IgXw58ejeYRUAkh4fCgzwoNdGGhwJ+smzRQYZgK1hHTKA4GrzVc4aoLUm0uc0d+TA5wUcNBwW8\nZKQAO1IYHQkJg4wYpCI4cVHCtrsyTRE3WYLUKaHtDqUmChWc2KixQbwVnk6BXlaJsUWA7O7qNjUS\nWg8yGi75GmFSxOtbDBRWGVIX2XFFeVE8j01qYBPqHOUmIgZNw8ZH6m9i08p86WEP3g+NeYFxHl9J\n8HTty/TMT6IWSw+AywJhy3/5vdKEZe2qrgXUFnhaQGoBfq2tL2vyr92X2gLIdl3begBYoGpdg3Xu\n9/plW0BtyTXvDdZp9x5p9xO3tmbbNVr5uauAkSsRmb/Pf2v/v7iwdZqLnAKmaOUL/GDbQwdsj1BE\nNAzi4gZCScTYUCm7XBhFieaajUAqQ29wuZUhj0UUmiTpoGI4SRcj5OeD1DxOXMMJjjx3HbtQpbTu\nIZhKQ4+BM1pAQyad7qCU8SH5moTVHSRd58biCQy/gDpQ4dzmFQSbwMK+Pm4vHWa10UfAn0ZXReqm\nHZdexilVCCkposH7nKxf4WjtFsFKgYLbw4JtgApOCoIXCY0gGWo4WGKQEm6qOKhh567SIKk+yQHu\nc5C7KDS5ywRuStQMB/W6jawaZEYYIS95qeGgYjpJG0ECQpZeMUGAHLoksClFCbNDHRsJs5fnqy/h\nlzMs2brpqW6hiBoSxgPW7SVBJ1sEyWAC+d18zS0fEtduEIqKiUhVtXO99wAntGsMa7NsmzEyUgC3\nVMRNK8imtZiTuyVFCC5ShDARcFLBaVYQTJO0GEJhkR4SZAg+uA91bGzTwQ4R+ll6oGcvG/2kCVIS\n3CzVB3EaVSJSioZNJaRlOVe+hOaTueMa58+kz3JUuMlxbtDPMk7KeMQyUUeOO8r4wx66Hxpz2gT6\nIypPZy/z3NLnWaO11K0FmrAnJVhM2PJZbvfCaAfR9pBxjT3mbMkY1qRgex8W+Fvg2Q7I7ROQzbZ6\n7b7U7RGM1vkskG6fuLTaim3HDN7N1KEFzhb7t/q3WLujsMUzb38eKQDZnn/A8rZIpd7+2Phg2kMH\n7Jv6UUKNEZ5TX+DA4Smm+8e4WTuCoYh0udY58vRNTtmucIZ3uMExrnOca5xgs9ZJVghjDEpMi2OI\neY2fC3yBkuRmM9rJYz/1HRoOddfFqMGkeoQ7rqNsSHHuMoEhTpOPeWm4FO4qE8w+Psgx4Trnhdcx\nuyWGO6bZMDo5Yb+GT8zjd+RoCComAinCXFePUjPtPFV8i359GQ2BBQYfeDCUcCOjcZzrDxijT8hj\ntxu4XT6WGCTMDhLrBMgwwgx+NceTode4LU4wy340ZHpJoBky3y5/DEnV6bWv7oIq2KmTJEoTmSjb\nqGIdu1AjKKbZioaponKCa5Rx0UQhRIpOVEKkkNFYZB+bdHKVkzipMMQ8T/EqCk1ShPFRoCkp5PHx\nyfy3mFWGuOQ9wSCL9LNEN2tMcpAkHaQIs0w/Jdx4KHKkeZugmeYN9XE62OJ5lukhwVVOMs0oOfwU\n8VDEQ9bwYwitn9pLtWfISCFsSp2dahRv4SrHqvdI94RJuwOsxGOkxAh3xHESQg+DtFLcLrAPMHE7\nygwOLbItBf+6YfdDZYPRJf7dz/wJ5o1lrr20l2EP3p0C1WKZEnuZ9Cy/6vbgmXZQtBI9WeHn7Uy1\nXaaQ2vatz1Zq1PZJTpGWRGH1X2ora5c22r1JbLRC1dvD4O1t12eVW5q51YfStt9s23RaUtB94Ny5\nr/PI8dv8+h8+xuSqnx96wA6IWVShwd3KBA3NwY4tiuaUcduK+B0ZinjI4UfAxEmZ8G5Ojp3NGGZJ\npKN3DY+9QK9tlV4hwTJ9yIrGYGSRNEEyBFFpMOycxivlWRD7KRluHJLAx/q/haGIaIJA1utnmlFk\nNOxqhUPqLSa4zUhzDl+5wIHqLJvuKNuOSMsTQnCwke2k+ecyoUAOaXiegKNANupjJxriKicJkuGY\ndoPgWh5fqYiDKtfqLiLSJCXcuCnTsZxi5NU5YsNbuP0ljMwqYW+WA745ak47K94eVuw9nFdfo19a\npoj7AVN1GFV6S+sMSisYKviKBUxFQPdKFJVW6lcJnZPaVTRkVgAXZeJsEiTNS/qzvGOeIS2FGBCW\nsFN7cL9KuFmml7nKfm6XjvOo+hZ+NcNh7lDDjpsSOhJzDHGPgxTx4iOPmxKbdGIUZQJakWA4w436\nAP85eYZkuQNnoMTRwE1clFuyFl3ogoSXIhWcuOUSefxkjCBBe5o0AX7f9o+pKQqSqJFSQ/Szgn83\nJ8sOUS7Un6SS8xB1bzFuv8e4Po1H/PvQdAD7s53YjrgorGxCIv0AiC0f6vbFBCyGaoGzlZnP0pwt\n2cPJHnNt9/6w9i1vEYsNW6APf5XJw568YjFoa0JRYy845735stvD4a2JT3i3f7cVOWlp49ZEZztr\nt8xi2ba2a6kD2eU0RtCG/afjOG56qb74wY6GfOiA3SVuIMgppspjlKs+RA28/ix9+hJDuSWWXX3M\nKCP0s4yGRBfrOKmwmBuh2nBxKHoDv5Kll0TrNd/0UjLdDIhLVHBiIiKjM2Kf4rDtFn+pfRzRNFCF\nEp+O/BmK0GSOIUwEJrWDrDe6mLDdoVtK4KJCTE8SqOXpym8TVFP4HJ2s0UOGAELWhJfB0V3DbtSJ\n27eZFEaYio5wlwn6WeaIcQslqePbKRIhRUfdyyDz7BAhTIrOtS2Of/kOwnMG+j4RbUVhMLbCQHwV\np7/KK/p5ym4Hx93XcUklFhhinS7KuPAYJc5WrhFTNqkpMs26jarpQqPlNSKj4aLMsDFHCTcVhmii\noNLARYWC4WHLiKFITfzk8JMjQxC/mUc2dXJCgLn6KFrJhi1e5Unbdzih32BKHKEqONikk22ibNNB\nlgBdrOPRStSqDmyFJg5q9Jhr/EWjl3dyv4CSafKM+pccDtwmSOZBAiddkKhjo4CXPnUVwxDJfzTn\ngwAAIABJREFUaX4CjgxJZ5jP8wucEd4hTIpFBug3l+lnmQnhHiv0sqQNsJHrZ0K4xUEmCefzVN3O\nhz10P+DWCg+JHXETO9Fk6osCgeUWkFkSgSVTWFp0u55tyQcWuLYHuVgRiDVakoLVnzXBaD0M6uyB\nfDuztfpvd8GzHgqwF6zT7lFiseR2r5T272ElnrKOS+/p33rgWJGU7Q8BC+SV3e/WrnGv3YNcWaTz\nt1WypoPFF5381SnSD449fLc+bHSJGU57LyO5DZxmlQF5gYml++y/u8CXznya+c5BXuA5ulgjyjYx\ntnD15uk3avyC9AW2iJGgh2/yPFONUZq6woB9CVVsECbFAItE2cYm1BFlnRIeZs0Mg9ureNU8/kiW\ndeIsFob4xvJn6BtYJRco8i2eZ1BdJOjPUnM78ClZ1N1swEMs0OtI4NhXpXZMoXFOxj1Zw62XGGCR\nH+EvKOLlHfkMNwaP8UjXZX5d+vc4dsp0Gpt0ieuoNBB9BkxA/bBE7pCH5PEYs8owDdXGcfk6E7fv\nMZhaYv7xPu54D5GghwEWW0mZpAb5kBOEECXJxfWek/iEHI9wCSdVOkhyhFu8ojzN25xlnTXu00kB\nL0XcCLLJ4+YbJIRuxpjiUd4iRBp/o0SjaQMHjHsnkZw6T6vfYaQxh7daQXOpLCqDpAlxjrc5zG0u\n8CQGItFsip+7+0U6ejdoxCT6pSUGnXnGe79BLL5FyJZimyjXONHKcUKePD4S9JCgm5NcIy5ssi1H\nSdajdAhJztsuMCgs0kESF2X263PoSOyTFzjFZSSHwWLvPg4XJzm8dQ9vvYhL+WGPdHTz/5H35kGW\nned53+/sd9/v7dv73j3Ts/XMADMDDAACIrhTJGNTtkiZYkxLcpw/4lRKLqssxVVOlKqILpcdJ3HF\niuNYkVyURFqhSXEnSIDAADMAZp+enu7p9fZyb/fd9+0s+ePOQZ9pgtrIARHxrerq2+ee851zu08/\n33ue73mfF2b4wB98nQ99+Rtsp7NvgZvGAfg6GxA4rUltqsKmFuCAr25zQH04TaDgwCvbzpKdFqlO\nGsYGRDujbx+6HruE3Flk48z87acCp+SvxUHmj+PzOP237QlGcYxl27zaxTf2sTZtM7S7z7nf/Ff8\nae1D/C4fBpaBd6fU75EDdoJ94kKWafk+Gm06qLRwUfYHyA+Gkd1d6lUfS9k5ToT+b2a9qzQ0jeng\ncs/IXugioeOmiYTORelVRMGgI6istSdpdD084/4Bk+YaLr1Dn5ZlUxxmDZ1N9zCDstgDgm6DjDBI\nf3ibFXWSIgE02qyJE6yLFj65xigGw8Y2w817xKw8UbmA+lSXxpRKM6lhtkXEQG/BcY0JygTJCTGK\nwTBZK0pKGKSjFCkKIW5yinHWGRF3QIWWVyMXjrDENFsMo9CljUzSzJKo55FqBkuuOdJqP1FyDLPF\ngJDGK9XooJAXYrRdCjW8bJtDDK5mCIo1mpMqqtDBQ4MYeTqMUiZIgn1mmytECwVymzEmfGtMJVZw\nh2vkxDhZK86ZnZtMeVdphxSmymuYlsSiNktbVEmu7zF6bYfxC2vUBt2UCdFFwaV1uJs4Qjnk6TU4\nFsJ4pDqD7i2auLjbmqNd0+j37CKLXdq9NsM08FDFT5Y4LUHDRMQltYkJeUaEFGv1KVaYpc+7y5C4\nzWgnxfnqVbKeKE1NY959nUljHS8V9jxRUu5hem2EfjYjMtLkxM9vMvz6EuYb62/RFC4OPKSdftY2\nxws/3AwADnhkO1u2s12bh7YtUW2QdlZDHvYAsakYJ1Xxdq3FnE5/zozffs9ZvOOkWJxqEKcSxHm8\nfR6dh+V/zsnLzsqVdgdhaZ3xx5d49hNHufXVJoXUD//O3w3xyAE7buQQ2yZD8jZusUleiHKLk6T7\n+tnsGyZHlG5ao7PmZWQszaiyzYI2zYiaooGHDEm6qIQo4aPKEfkeGm2+wYfZbg/TarrxanUSeg5f\nq0VczCLJBhp+VsIzmCacb+7QV85TkwPcGb/EClMUCHORSyxylEbLTTy3j9fbICYXmK/fwW22EEUT\n4RxYAYGuJtGdkGmLCpYlUNGDlMQwLcnFiJrCT5U1JmhaC+wbSV6TLxCkjCmJ1NweWqJKU/dStCKY\nkohLbCJigsfC7WkxW10l4c1iqQINvKh0GbB2CRolqkYQ3VQYlnZoyi7uW9P0L+VxmTUqQR8D/l1O\nareosI2fXpOBae7zZO11ZjZW4QdADMxZ6MwJ7PsTrFrjfDDzAnpEIBOI4y23WNfGeDXyOAPsMrG1\nwcTXUjSHFYxklEFph3ZXI+0a4E+Pf4DTXCdGjnXGgRsEKLPMNEvto0gtk2fUlzAVkQ1hjPoDoyYX\nbTbNUSxBQBW6+NUaSTLErBxfLvwtNoRRprz3OCYuMKOvcjZ7i/+U+Bjr2jBP8Bq6TyTti5Gmn0Vm\ngFce9e37Lg2Z+GCTn/+7d5DbKe6/0ctcffRA12n6Dw8DGjxsp+oEL7ujjF25KB8axym3c/pRHx7T\neV6nQ5+Tb7apDWfmb792yvScZk52Vu8Efrts/e2KZ6xD253vOwtvdHpNEILzm3z0s6+QvjpNIWVT\nI++ueOSAfbtykp27v8DLA88QDeZIuPZ4nDexEFhjgmVmmPKu8xuj/4JLsQu84TlBhDw3mEehyylu\nEiPLHkm+xCe5ylkG6S0MPOf5HqqrzZJ8hF1pkD4hy2OV68xZK8y3ZJ4ycvhLNYKrDaSbJmafTPPj\nHua5iYzOBqOc5wqTN+8T+Wd7hN/XwP28QWHcj08U8dbrqFtWjytWG7h3Da765rkeOsnP7b5MyrXB\ny31P4KdCgn26popW0Unmsswkl3mMN4kOZ/nBLz3BnLbEkewag/UsG/EhKkEvHTS6brX3X1IAn69G\nfzDNKBvIdNkRBvHLVcKZMo+t3cKMiGwnBliMTSEkwbXYpv9/yxP8ZJXY8RwDpImzziqT/B6fJag3\nmJFXYRLYA/EWqH6L4+ElJuQt3GNVdr1JsnIMkrAijrHJCH3ssX5ylJd+/Rk+5P0OjUqQr4R/nrXU\nLANGms9O/TtMUWSTUW5xEpUbHOEebTQS3iw+V42nzEukjBG25OHeAipNhsxt7jWPMCxucdF9iVuc\nJEiZOWsR/26VqFDgwuBrIMB+J0GkUMMbqAFwk1OEKKHSoUKABj/LHHYS7e4o/f/gi1R3dqhxsAhn\n0FNlOxUVtp+GnYVrHKg2nD7TtgOeszTdzmBt/tjO2g8Dh1OP7axItPd3AqhTYmeDp23YZEsGmxzw\n6vY+Hg4WN216xObAbZB2Xod9Xrtc3TaZsiclm/6xjae0r+0i3JCQlp8HQsCdP+fv8M7HIwdsZHD5\nmoTUEi3RxQrTDLNNU3ez0D3GjLrMsDvF/cQE1z0nKUpBpljBTxUvdfJE6KKwwyBrTFAhgLfV5Km9\nV8kFoqyHR0nTj0+o0REVThdvE5ByeC2VVSYoKWGigRL9Q2ny4TAD7HKC2zTw8F3ei0KXpLTHsCfF\nrn+EDf8AdZeLQXGbocYO4f0GuEFPKOTdARR0phobTBtrqHRI0U/rgb45L0S5Jx8hqA7yPr7DJCuU\nvSG+4vkolWaQE607eM0GRSlEzfQy0d2kHvSwMJpgWxxk150kTIEGHvr2sgxlMwSSDfyVJkreYCk2\nTdN0M1VYJxePoHdFBoxd2l6N7dYwy0UNb8PLiCdFjBwhT4FCMkjG30fcnyeeziNeBd9sDXWuSSOg\nsqUMclM4RdKVwaLH3ct0qYYClP1+hFfAL9VIPLVP1t1PrJ7jVHqBS+ELrHkmHvyJdRLtCs9kL3HD\nf4qqz0e8WqCjueiX04iYGEjogsyWNIwgWoiYzLLE0fQ9xhdTDLm28CRqnON1hs0tKoqPr8Y+xGuV\nJ9jvRpkdWCQm5XDRYpshavge+a37bo3oXIfJ2QLmt/ah0XgLhJ2ZsA2QdvbpBC97UQ8OuGdnpaCd\nbR9WfIj0wM7p1HeYT3YaOzkzfae80EnNOP237TE0HjZ1gh9WtzjVIPZ1O8vRnddhX5fTOtaZvb/l\np7LbwCxnmX5/nnpJZvP7vOvi0VMi/n0Gp69yhmssGzO83H6Ga9ZZqh0/u51+Pif9exqqh98O/mNc\nNImRo0KAYyzgpc4mo+jI5IhjICLTJdQsc+b+Lf505ENcCZ9niG1kdDqGilkV6HpE6orG68Lz3Ase\nIRws8vjR1+ljn1E2meI+e/TRxkWRMKWhKMN/J8e9o3PcGjiGJrYwBQEfDVxVk1ZboawEyCSTROtl\njlWX8Lib1DUXR4wlboonKQqhXsMFfxwlMsh/zb/BQuCadZZvmR+g7dbIecLEybLIERTd4JnWZXLB\nEDfiJ3nFfAqX1CRsFcgZcY6vL/HYzZtwAUxDoK56eTM6T1gu85Hdb/Ot0efYHukjcC5PRfSxUpzh\njdw4AzWN93m+yQUuo4S6rIaGucJ5Hk9eJ3qvgPlFiWZEph5TqRBgWZ/lkvEUs8oSx8XbnOUqGZLI\nps5kew3v1ToutckHLn6bgYE0gWIdz1KHNXmaZc80I6To0sbbajC/cZf00AB7ngRiUyQoVBl2bxGk\n1CvWEdzcd03TRmOXAS5yidNbtwh8o8HAZ7YJTOWZZJWkkWHJNcu/nfocN19/jOB2lePx24wJm/is\nKqvS5Fs0y89eCIycyXD2kxWqlzoYvXzirezT5p/hYRC1QfDwIp9t/u8MnQONtZNvtmVxtuLE2ZfR\nqfrgwZhux/hOasJWl2iOcRUOytDdPMxNO6/LzpKd260Hxzbp0UJOoyvnoqQNzvZTh9NTW3ywrevv\ncOG/vAarE2x+38W7Lf5CgC0IggS8CWxblvXzgiBEgD8CRunRP3/LsqzS25+gV6TxNfMj7KUHyKwO\nU6nGONV/jb9/4t+yIk+xwRhe6pzlKqNs4qOG8mAeHmKHcdaxEIizzyC7BHwV/vf5X0N3SzzLi5x4\nUFEoqQbSWJuiHKAqe3hcfIML1mUmrVW8Qp17whG+zCfIEUOlQ5Q8QUpUwj6++sQHGN3Z5hdvfAmm\nTXSfSCXgY/upIdpeFRGDPvZYcB3lK+JH+XTjiyRqWU6XFjD6ZNbc42SJE2EVGOQLfIoSIXJCjCPi\nPRShyxoTXOc0DTyEpBLf9b6H49VF3rv/MqdrC3w99n5uBY/z2c3/yKnind5/oQ7VmJfcQIiLXCZQ\nq4MEgmBSF9ykxGGGhC1+wf9HuAdqjISeIE2SVSbJkGSJWa5xhoC3yuzMIru/OkA3Kr9lk3op9QwL\n6/NMnV5hLTLBmzzGDMscqSxzdGuF6FABIywwLqyzzjjbvkG+cORvsuUewP+gIrJFC90r8vrcaXzu\nMs+Z38ffqbKl9rPJKHmihCgSpcAAu71GB9ygio+XZ57k1c9Z3Bw6QQ0vX+BTTEqr1OnJF3H1Jixd\nkFFKBoF2E3+8RkP+yVAiP869/c5Hr+Xt+EubPL26x91y66Hs2QbiOgdSPo9ju9OrwwZW+1g4AHuT\nAwrFKQ20j3FmrDZwujhQcDjHt8O5AGlLD20qwrlACQ/3fHTSOva1OmkUkYOqTluO6OTHBceYThC3\nKRN7fLvYJ1Bqcv6fv0yn1uA/86zjqHdH/EUz7H9IrzDI/+Dn3wC+Y1nW5wVB+McPfv6NtztwtzhI\n9XaSwfEt+uVd3J4OQ9Y2J7w3mFRX2KcPAwkPTZ6sv8podgspZdIZU8klotzXJlCELj5qJMiSJINL\nadGMqfip9n6mRaxSIFIu4XE1KSpBWoKLE4276KJEXXOzT4JVJskTZYNRglRQ6GAiUtJC3O+bpL+R\nIZHK4v1+ndqwh/3RGPvxPuSOTrhYJuIrosmtXg+UVQFDlDBiIpMLGwR9NfaH4jS2Upxb7lCa9pMT\nYsjonBRuYSH0GgMgMcwWw+YWkWaR1eo0t2vz+OQKq8Ik68Y4bUXD7IN6WGMrMoIRAp+3jL9WwhIk\nttQBuqqMShdZ0HsFLUqdQW8NRe2ywwAaHfZJUNGDnKjdZYAMbbeL5aNT7IiDlAnSwE1QKXHR+wrj\n0gYFQqTpJ0SJGWOVAT3D4vQMjZBGmBwTpQ1CxRpGXsQ/WqUdV/FSp4xGXnDjlxskxQw+o4Za7eCS\n24QoIWLQwMOOOcjp8i3GmxsMmtv8SewTrIXGEUMmDdwYSKwySVEI46LFENuk3JNUCXKDU8yIKyAL\nLAszFAn/2Df/j3tvv+MRD8KxWczbJtabu8j6AZg6i1RsKkPnQOUBB8ZJ9jF25nm4utGmQZx0hdMH\nxObCD+9vF6OIh44xeBj2Dkv4uoe229m4/d3ez3nNhwtz7OPt65EO7eecmJwFQM7rNwGjbWC8kcYc\nsOC5E/DmzXeVxcifC9iCIAwBHwb+J+C/e7D5Y8B7Hrz+PeBFfsRNfXf3ONFvBnn+U/8BeajDTnKQ\n9/NtJHRSjHDOeh2X1aKkhzmeXSZ+LQ9fAz4BNy6c4Fvq83iF+lvl4E3chChx7kEHcx2ZZXOG4N51\nZtbXEfosCv0xupbCaHmbReUof+j+22RIYiISZx8BizYqJhI1/BjIdFDJjkfIVGNM/q9N/KdbWO8r\nUfbn6SvlGSxmaA+LHHXfI17LEb5SJD8SYnV2lGNfWWbWs4bwPovOgsEnkzdpTUp8R3yeHWGQKHky\nJKnjZZgtzlpXmessEs3X+KfV/5H/Q/o1BkfXqQsepK7OK6PncY1XmTbv8z3xIkkzw3PG96kFfOyL\nfWwzRB0PUXJEyZMjToUAJWRchCgSQUfBQmCivc7n0n9AWC2SDibZcE3wkvg0WwxzkVd4bvgFTg7f\nomwGuavPkSdGU3RTVoPoEYkX409Rdvl4tvMiJ9MLxO4WEW5A6+MursdOErSq3LMCZDoxntr7KuWw\nl5IWwChLxNUsp/Ub6JLID4T3cEU/w3+/+zucyC5Q6gTZOj3Cbe0EIatEVMjjooVlCezRR4QCF61X\nWXUdYUMa5zu8j6nACm1R5gc8TfAnoJP9ce/tdzqk8QjKf3WB/d8OcjffK9d2AqENPE7ttNNbw16o\nczYxsJvcOkHdzpKdmbW9cGkDMo7vzuzVzu5txYkNtk55IRxw5zUOutB4eZhuOUx7OM2rnAoU537O\n45yvnZpyZ4d3J6XTBZoWXG/D+kwf7l85T+s3voz1/yfABv4l8I8AZ6VCn2VZew9e7wF9P+rgDxrf\n5NPt79AxLcr4GcakjpcYOU5bNxioZdFSHboL+wSSNQgC5wANzIpIJ6KyxRAmIqNsImFwn2lucIph\ntjnZvs3szioBuUx6OkpssYxpiLQFF98MP09G7MNLvWcryhbnuUyRCGWCVPEToYCL1oMMfh8l3IXn\n4Ltzz3J9+iQj6gZmREZROoTTFQayOaKVCurZJuawH90t872PPIMoWYTiRbZPL5F/ukO4VWRI28Yt\nN3HTZNJaBaAm+BivpxA7Iq/HzpCMpPgEX2RdHWWCCn3SHm1R47JwgUXxKBXBjyFKfE94L6Yg4qJJ\nkDKLHOUNHucFnqefNBEK6CxznsucQ6SGjwoBQkoFIdqlpcqInjbnpMvoiKwwxQWuMMYGWqfN2PoO\nyXSBM9U7iHMm/liFVlzkgvYqrIuMvbANjxvU5tz4ui1i4RzHWwtczLxOrdlgvhNE22uTVqZZCM2w\ndWSE0a0UE5dSNOZVJoKr5OQYK8OjrCTG2LRGiQayDNZ2uZF9nL/b97tctF4llimhI6O0ukRLeW4P\nzpPpizOhrDCn3+OkeYe/o/0BomDyrb/SLf+Tu7ff6TgRvsmvPPYdrgaWHjJccn7Zxk52ZtyiB9zO\nZgOHC12cC3A2lWKDtZNacHpl20oOe1Gz4RjLzsSd/iF2dntYRWJnv05eXXTsYx7aZk849nj2k8Rh\n6d/hlmNtHi6xN+nRRS3HezY/3gXOxV/kmdO/xm97qmyQeNu/x08j/kzAFgTho8C+ZVnXBUF49u32\nsSzLEgThRzqmvPnVS6T9IuZlgYF5P8m5CDfx4gESVpNI28C300JbqsIYtP0qZd2Pp9xgb7lEKnSJ\nmlgkS402GuVmkJIBRc8mO+IWxW6a7dIeLqGF1baQXzVpxQtsWC02zFHqUgYv6wQpkabCC9SxyCOY\nIBkme5KEaJp4Ww328y2W8i18ZYO7uR1SawJpLceKWCDc7eArWii7TcRiA3MQap4SRXGVjahOVfMi\nWRLNRZ2g1cJXMCn3bVAMFMkpUUY2dwh0yjRH3Gy2WlhtiR1rj5zvMpZ7kUTHi0tqIioNSihUTAvZ\nNECy0Mw2W902tCxUuYPi63CdDdK00ZFJUCBEmd1LLbxs4qHR67HYtCi0m3yZFoZboKQJbCJQ5Taw\nwOsUuUUbTdcI5rr4Snm05g6dVRVLA1HXqfm3kfYtlq5WaacVrCBoeYuV/H3anhRKYZWtyxZvbuVY\nEDtsxfbZCfegoH+/RV+xTXvFpKDdpmHu8wfGEPtmkhIeYuo6ze4+VnWFTOBFVoxblHIl9pQ4HVPF\n36iyEX8VM5jGJdzhT27f5v9a3McS/piOoP6oW+4vFD/+vX0ZHjSEgPiDr0cZIt3lPSqfv05ms87r\nPNxM4HCVoc3xwsPZJRzI4eCg5ZedqTobHTjleyZwm4clek6VhTOTtXlmJ1XjXNg8rCyxwdn5WZz6\n6pv8sKb6cLGNUxduTxjO8x/2RLHVKB0OJh5ny7H+a+uMfH4HIzNKD9oftSlU9sHXnx1/Xob9JPAx\nQRA+TO8JJyAIwu8De4IgJC3LygiC0A/s/6gBjv/me3B/+uN8ht+nnzQlNL7O+2nhwsMGs9xkZm2V\nscu7WPOwMdLHS74nOcFtmrgpMMsTvIaEi9/l17h1/yz1kp/Z47cZcC8yRJxpghzbWGLwlRSrS+Dz\nVvGe1Nn5L46R9UU5wj0usMoefXyRv8/TvMzj7WucKN/nvn+cTlvh6EoG+Y8MWACmgalFGmfWWR8f\nxOXqEnjwJ/ZcF/C+/qCtUKtBG53rzyW4PTbBujFOaPcu/yBW70k4L1a49fgw/yH6SS7+1pc5v/Mm\n+ue6SAaIaeD+Oq/M97E1E+KDuy9QC7jZi0WJkifSquBuddj29eFutunP5mAFspEw9x8bw2COCEO4\naOF9YK9aJsj0p0WSZKjjZf7eAlN7WxCDYr+Pa5EjfI3f4gxXeT/f5gbvofOgKClJmiljhUljjZQ8\nhDvVYfzaDgsX+hEEi2Mnagju7lvPrMvj0ArB0TKotwx+sdWk9d+INJN5ipLJBqO4iBJEoYWLaLcA\nzR0+W/48r7efQcSg27/CsHeD95PiA4Q4V/cyli3zf8Y+wqZvkJO8StD8AIP08cvCNcqfPgcmfLj1\nDRaUWd6rvvbn3uCP7t6+AJz4cc7/lwwPsfUlnv7dK+xiMccBJWIv0Nkl2Kpju73w6OUAYA16agqB\nHiVhSwKdNINd9Wh/2WD2IR7mieGAUrCzZdMxhg2qznC68tk/2xmxncXbNAkPjv853r64xv6MtjTR\nBubDXuA82G5brtq0T4sejWP7e9sxetdi8q7Fv6MPOMNB07F3Kv7Z2279MwHbsqx/AvwTAEEQ3gP8\numVZnxEE4fPAZ4HfefD9yz9qjNP6Ld5XSjO+t4FbaNLyFehGv8uGNkLZCpEoFQhpFSpPupBCBgG5\nyBPt17BkkaIUJkCFW5xAAM5wjbnkPdRolyl1GTcNAo0qx5aXqX0jx6XvwFQU1JM+yhEP065lJMZZ\nY5IuCjI6k9Yqc0vLjJZ3ELwW/V/ap3VDoLBlsrIJXRnOz0ApFqPi8pP4VgFlvE1nTmJLGiY8UmZI\n3UWuWogGCBqI4Z7OuC766EaibJ+2GFIykAQfNWZZJuQvI8ggLYI+KdKYcpFLRtkO95NWktxKzFFV\nfJQIMM192ooLQ5JZkI4ytJsmfqPIxtFhVodGWWWcGj6i9GRwM0trWKbArimTxMRHjTxRulGZhtvN\ndjBJ1hOhgp9P8qVeBSYik6wSKZToK+Uo9AdQVB2LXkf6StxH6vE+qmEPWRK8fuocZ+WrDIg7WIJI\n6MUy6o6ONG72VCtjoNUspM0OJg2UQYNgt8ZwLYNhSihah7ZL5rPhf8+gleJNzjKkbXHBuMKHO19j\n5M4uRSvCv577GP2uHYZZx0RCFEzS6UH+lxd/He1Uk8BckWVtBkOQgL86YP8k7u13LgSYmKcs+ri9\n9gUa5sNA7bQihYPM0qmnLnNAEdhKEt5mDNv2yFkJedj72gZMZwZrc8+2Y54NpHaWbGuxnXSM7Q/i\nPN6W3TmVI87FQ9ExjpMGsp8onJm4za17OJiIbImj8/PYnLs98ej0uLCCKFOPTYLnLGz8WMnBTyz+\nsjps+3fxPwN/LAjC3+OB9OlHHeClzoxVxm9WUTtd/GaDqeAqgmawzTCSZWDoEkLLoCgE6Mgqiq6z\nzDQbjCFgkSNOo+3Bl28w5N8iHtlHRkejQ8CqEDaKdFJNzAUIfAQax7yUyj5G5A4+apQIUSSMnyr9\npFGNDmZLhLZAoFhDbkikNQ8NoYOgd7HaYFVEhH2L4G4dUe1SiATYTgzRCatEfHm6FTcyBoJmUfX4\naKNhCRb77hh3x6KYbgnDI9GquzixdpfIXpGG4WZPSFBw+2lFFVzxNg1cNHHR9PXEThI6WeKUpSC6\nJJOmH0uUiaglSn0+CpEQOwzSxM2QscPp9i2mNjYoEUSwxigSxtJF4s08TZebHXeSNiqCCRG9xJi0\nSVEIUzaDjLVTDGXTBNM1SuHj6JKC3LZQxQ66pWCZAv5SnYbSJO1VaXlUKoqXGj4CUgO6LUqin2LC\nIn3MTVzOozZ1BEtgxxzEVe8SyNVp+TQqmod9OQaCwZi0gl8sMVTd5fHKm1yovEm5HOJGcJ5ve9/L\nLwn/kSF2KBPEJ9QwLYHNzhii0cEnlKlJXpLs/ahb7q8af+l7+x0LAQLnvLhkL7mUgN45AKcHbz+k\nf3ZmlnaVn+1fbb/vzE6dPh82mB529jtczu5c7LTHVBzvO7lr+/psoLePNRzvO8/lBF2qF2qoAAAg\nAElEQVT7nPZEYx7aH8f7zn2dKhLnZ3YW7Tid/Zw9JG2NdkEWkKdc+Ae9VDd5+LHgpxR/YcC2LOsl\n4KUHrwvA83+R49blMW6FZGaDS0TzJZQ8mIjEyBMWShTDAaSUwZGvrnL/k9NsHR2gIXt4mafJEWOM\nDdw0yZb6+OrlX+Dpue8zeWSJl3maM1zjA55vUZ13MTLTYDqhIz0JuVkP5ddDbDKKSK8Lt4GEiIkq\ntFk9OkInrXDhxjWEj1oYf0+j6U9w8l8XiHy3jFSB5OUs1raAOGX2/oK3FHafHIQQDGo7bMTGcNEi\nTJEtYYgqfvxUWaaPV3wTZLx9NAQPQ1d2ed+/fBH1XpfU0SG+eeY57kem8Qp1fpE/xEcNLzUmWSFE\niRIhXuZpGnhw0WuKuzvZR3qsjwvyq4QpYiLRRSHQqnE2ewtp32RX6ydvxXiJp5hqrfGrqd/jZt8x\n1r2jPJ9+Cbe7Qdcv0vRoFIQIZSPEE7lr9O3kqWc87B9JEFUUXFWDsFJCSptEX65iRQSOhtd4JnyZ\n2ojKfijKNsPwUQvN7OAXa6wU4PL5QZ5r/4BgrUbFDPCi9Cx6/TVOl2+RHQ6xEpjgujXPH9Q+wzFp\ngf9W+1eMb+wSWqsgZASW3jvNjYnjZIQkOwwyxQqTrNFHhoH+bUZ+aYuUOEIdb8/rhLW/0g3/k7y3\n36kQBIuRj64y4VrB9f+ayJ2DjNV2xHNK8GxwsrNIJ89rg6atyICHwc/lGM8GRjtLt8d3Gi8dzlTt\nrNqmJZxUifMpoE0PFO1tb0c42AZWtuWrTfvYihLbnc+penHKFuFgAdIuR285fh/O34vN1wv0JjcR\nQDWJP76PenaDxS+9zQX+FOKRVzre4Tht6wxmW2RM22Smf4WiFmSsusmZ4k1eiV8gPdxP5yMym8lh\nKvhR6fDB5ncpWmGuuufJCjEqAT/jp5c5El5givtkifWa29aDKDcs9u6a7FdgLg9i3UQz21zMXWFH\nHuBa6BT9pHHTpIGbCXENNdzk7slpwr4CireLS2mjPaUje+g9D4UszEGBylE3ak1HbJhoUgdvrom3\n0KEx5GXPk2CDMd7gcfboQ6FLlxQ1wceSMMM093FNNLj7qzOMfmGbiFnkPfnXmN9cQKnoDHqyMLLI\nUHiH+H4Z93aLbqNL4zEfjaAbCYMuMpYooNEmXKrRL2Zx+1ssCkdRNJ2r0ZNEn8jTESUSr+7xc7xA\nSCtzc2COtDtBU3bxZmye6UurJNJZmh/3kI3GWZUmuBSpIR6xyI3G2AoOEJdztEIam8oQ6dgg+XMx\nTnuvM+raJKhWGBDSGE2NBdcxduV+QpT5EN8gL0W4qp4hJuYIKDVqlpdz8hVm5GVkwSS6XUGWV4lZ\nZcbZpRZ2s+g+witDz5AI5JhvXGexb5agVeU367+DV6uyKY/ydT5MilG8Yp2q6CNfj1HWg+z4h/CK\njT/v1vtrFe+VX+CsvEiZLgY9ULFL0uFh32p78dDOlm1LU3sh0QY4m7qwAVvnoOjFqad2yuBs4IYD\nesJWlzjpEBvY7UnCLoZxls07r+NwdaZTBWKPh+M8TuWKbdHkvB4nh23THHbW71wYtT1F4GH3PwHw\n0OWEdAdJjnKPgXdDgv3oAbtAmKucRTG76KqM5mqxxTCWITLTWSNtDlCMBqhEfeyRREcmSImnrcsE\njCpf0T9CUQohuC2GxjcZZJskGUZIEWxXiJWKeLY71A2TegKMBnjXGoRSJqPFLLWIjyp+xlnHR40a\nXuKlPH6q7AwNoHWbhLpt/M06+pREzePBc7WJaFlYkoBhijT9Go2AG0nVcWU7eHbahAJVarKPfbXX\nRVxHJkAFL3Vi3TyuVptRc4uYmqP2mB99U8JdbOGljq9RR6oatC0X0U6Bvk4GX6GBvGLiybVJjuxT\n0EIYLoE6XgwkBCxk3SAhZfFRRkanJAWpej14kzW8ep3hdo0Lrfu0FZVXwhdR6OCjyn4gSn8tQzKV\nRWhZ6JZEQQzzqvcCHa/6oMWYTIY+NpSePet9aYabrnlKcT9nfNdIsI/UMCiaYdYZZ5d+4uQedMfx\nkBVi3FWOEFAqeGlwnDuMuHZp+TTudY4QbJU4Ltxl2r3CfWGCN8TTbEcGaEY0BtkkT4SAXuOCeYW0\nlSBvRSiaEfxilVCrhLbXwVvvUJAjvacF9XAt3V/fELA4uXuHee0ul80etDkLSexHfafqAt6e33Wq\nMJxA6FRW4Hjffu3MSA8XxjipFXuyOFzY4vS9s7Nt5/U7NeNOxcdhbxDJsb8dzq7tTlB1UjLOIqHD\n9InTHMp5rGYajBW3CGUWgAHeDfHIAbuPPTpilU96vsQcd9Fo80V+gcXAEfBZpKRhSgRZZ5w8vS7d\nPqr43TWqup8rrcdJaFkG1R3cNLEQ6KAiACdKi/xc9mXURAff0zAyDooK1st5Bq9KFD4yTn1SY5r7\nzLKEnyoVy8/QUgbF0qme8xGqVokWqlAS2BgeoDWsMbWXQt3oIt83COYbZB6LsXUySVeSEXQLV6PN\nmb1bRKQit+Imx1jARYtJ1niRPZ6tpzi5vYjS7CLqJpYoIF8wSIUG+Xri/TBm4jXrBIQKR8wlxhsb\nSJYFBgTqVT6y/m3uuaa4OnyKPNGe4ZVYpxT2EkGmKyoMss2ImcKn13Bv68gVmMxaDOZhKzhAw+vm\nqLDBMNtkieOfqyFHdaJqnqS+j0dp9iZSOiTJ0MJFihFyxJnjLsKWQOOFEPUPB6hMBVDosuCe7ZXq\nCBES7BOhyHVOA0skybDCFFHyjLFBmCI+X41Mfx//VPwtzolX+EfSvyCjRVGUFk/yKse5g4mE3Tmn\nJrt5zXcWF23GzTWebX+fRfUIrT0Pj3/5JrJisDee4MXBJ8mpP0M9HS3wvNjBK7dBP1g4c9Iih82O\nbACHA87YBjv7kd9Fj1qwVRrOxUDbuMm2WnUWlzg5c7sJwmFgtHgYXLuHttvncjr2ORcbnX7e9vXb\nTxP2pGF/RmcXGfvzOvXeNkDbk9LbFZvbE42LgycJTbfwLbYIlmvvCv4a3gHAVuiiUaUgRPhe43l2\nG0MkAmk8ap2sGKOKD4UuA+wiYZIhySZjvCw8DRJEtTxHpUVGSKEjs8okdzhOnggeX4tgX4WTwgJ+\ndw1hWqKo+VBKOrLRINRXYooVBvRdClKEjqDSxx6au417t8PIn6bxm3VElwURi66o0lTdWAEBCtC5\nBtmyBdk6UbFEe9rFvcQMpiRyUr9LyCwyxDZlgoSMMie7d1gyuwy3JHx79YPnQDewC2GhzBNDb4Bp\nYXhESjM+tJ0uSspCADYnhlk+NslWYpi+9j7nF67SP5bhde9j3DFPYFQ19qUBXg+coY2KIuj4pSpq\nXCcQrJINrbAQiFNUQ4QpEv9Ogeh+mc7PqxQGgxQjQUwfdCWZCdbQaLPYPcpSd5bnte9yQbpME09v\nzaCvj8iTRT5a+BoTK6u0p2QQLDLdfm7X5hnxbBBT8zxuvEHT3OUJGuzRh48a/WaaaLvMqjDJrcAJ\nznOFM/evoy6aRAcqVEa81AY8DO9maMhutvv7qeFjmyE2hDE+aHyTkb1t4jdLpOeq1BWTYKiKVm/j\n2m/z7M1LbE4OPupb990TFpRvWBQEi5bxsPzMWdzyYNeHKgBtIHIuRjqzWJsb1vhhrw4bbA9TCfb5\n7Qa4tieHM4N1ntPZEgx+eJJxarZtE6a3K1O31So2qDuzahuM7fFskLbpGCfVIhza35mxOzPutg6d\nNYtO5rAw8acXjxywLVOkY6hsiGNkjSSZ9iCftBbxUGOdcSoE8NBARsdoybRwU3EF2GQU1eyidgxk\nw0QQBUyvyKY4yh696sU9b4wVZQzN7JAQsyjeDjvePiTDZH8jy2pgEk1vEROy3LJOIgs6I6TYjfTj\nKbZJbOyju2UakohbbmNIEoYsYYbBCoIhQyMP2r6JVuziNershRJUffPEcgV8agWNNgn2SXRzDFXT\nBEwNVXRRlb00RA+SaBCVi3QbMlqrxSn3bYSWRcPtJtXXT73sY6l2BDXcYS8eZyfWz9XQPGd2bnB6\n/waWbrLNAJuMkddj7FqDXOF8byIU2rilJt2oQoAKu4Em21IMtdNhSN4mkKkipEDqmjRCKgVvlPtM\n0bVk3DSZ4y4VM8CuMcBxFjhuLiB3DcrNIDlXjCOn7/Ke668SqFbYZAC1qbPdKtFtq6iuLjFyTFkr\nrHVLnKqWyUoZ2oqKZrbxZNo0LC811cfz0gtMbm2g3DIJrdegKdBOuFDqBrqqkiNGF4WCEWGxfYwz\n0g2KjQip1BTNERnfQBV9SkDZFvBUGxzdXsYV/VnhsHsQuJ8SyXAAoDZYOasXna5z8LCMTuZhIHs7\nvtsGMjsrdS7O2cdJjrGdRTNO7td24XOqM5wLfM4Jx1nmbmf3zgnHCdgtxzZn5my9zTabrzc4kCoe\nliY6k2Ynb/6WnNGE8n5PJHGwnPrTBe9HDthN08VKa46OS+Go9x7vd3+TuLRPmn6yxMkTZZshlqwj\nbOz3muUODm8wKmzQbHi5svEMK9U5/O4yyeNb+NSeNG+ETc5wjbiyzx8m/yYJssyIS+wK/ZSkMK9o\n2/xh/R8yIm/ysdCXuS6cJsE+p4Vr/OfkxxEjFn/71B/TEl24Wh0ms1sIggUuC30IjE+A9gSMLsLm\nTIKdE/2cdN1gkaPck45yNzaNJrRoozHKBkOtDGJBoKl72I32YZ0TWLSOEmjV+FDhuxQmA3RViZiV\nQ81buKstJje3+EL8F/ju7HP0SXu8d/El3vfai7ieatEYcPG9xNMUtDARCvyy+Pu8FnmCFCO00DjO\nbcIU6aKyxjibjLLFOOHtXY637tCZFal/zENaj1MOBehvZxEbEv8Dn6LkCTLpWeWDfJM59S4jSopZ\nYYnBZhpvsYO5tks94KJ0yot/rkxJCLHFMKd27jKv3+FjE19mXrnOlLBCRk6iVxskVkpE3VWuJ46z\nbg0w+nqaM7mbHDPvoXnbKGq353/3bfDrddTHu6yMjLKiTLLOOGGKBBp1ljPH+V7f81yNPs53znyY\nX4v/Gz4W+BMaZxUkr4FruwsyqOo7Xcjw0woNiwCbqER52DrUKY+zaQTb98OGFZsCsD1BnE56Thc/\nJyjj2G5nn3b26zRRsvdzLh7a5d3Q0z8fLlyxO9nYlIgTlO3PpHKQTTurHm1Vic2XOxcV4WElinPx\n0T6308fEWfRjd2+3JySbajGALUBABcL01Oy2cvynE48csLtNjWomTHkwRMeloCPxQun9pKV+agE3\ncbLoLZU7lWNU7kUIaiW8Q3VEwSSgVXgscZnVwCRdRSEkFvHQ6C3cUWOPJHtCko6sUMdNUQ8xm19F\nxiDXqTGnvoSqtkCACn42K+NsZqZYkI4R9WUZTOxwonyXsFlhK5Gk7PGRl8KkPc8RclVwB1tUI36C\nrjJjxW38V2owKuE502Kiu8Fd8SiXpCf4G/wn2q486Wgc1WogdS2W3RPc5Sg+pcGolCLlHqKlaAzp\nW8SVPKFQFaXbIRnYZc63QAcVfUAk6wlzw3USWdEZUrYpEqZCgAIRGpIbhQ4W4Kfao1EYZZkZ/FQZ\nYoekvoegC70JMRAjIyRJMcLTvIaLDsVWjK3qCG5BZzicJulJU1dcxIwcrm4bxTBoJlUaPo2yFSRg\n1qkLfu4yx5SawpRE8nKEG8I8LdPF08YruOptxKKJHhdouVRqlpf2rAzDBi1BRlLayGkLsyBQe5+b\n/SNxtrUhdtQ+blVPcSVzkfmBq+iqSDS8x5i2hmiYpONx7rsm2TJH6GvkMWNQD6p0BZlO5NH33nh3\nRACYpUmABgc+Gk4dtg1etjTN1jzboGhvs537nJm5c2HQmYHa4Ofc5qQUnFmysyzd6T3iXNhsOfax\nwdK5MOl87eS1D9MddvbsBHpnY2DnBHE43q603ZmJOxdo4aD7jUUQmKNnRfDXHLANXcLXbOIz6rQs\nN/f1aa40nqCueomRxksdU5eR6xbDtRQBs4SIiYTZa4wbWKMU8dGRVY6Ki0gYWA9um3I3hKBbjGgp\nfEYNf6POkcoyCSHHesfieNeiKAfpoOCiRbrdz7XceQQFXLTYj/UhNe+gGDrbiSR6V4Z6rw9hRCzi\nddVJjyeYb9yhfzOLeNcgIWcRTpsku1luyadYt8bp6hq6LFOOejCFFqYuUyJECxeiaZHtRMlVYjRl\nF0q8gyLqqEoHl8tiurOMP19hKThDLhJhIzDKy+rTjFnrDAo7VPFTJgjACL3ekW00IhSp4CdDkjJB\nYuQYZptIt0qrq7Er9JMXIg/6Hx7hSOc+E80NBknTbnkIt8uMubcYMdepWF5Et0kVHw1FoNrnYlsb\nYNWawK+3aOOiQoCOT8E0BQxBIk0/0XaexF4OrdHGMgW6ioglgaGKFI4F0KwOuiBjyQbCGybqlsXW\nBwdYGR4nZY0iti3qZT97uX4aUQ9hf4Hz2ivMcI96x0c0sMeeFmfJmOVk/R7dkEQzoGIgs50bhAet\n4v56hx+YxsT/0IKZDVpwkBk7eWBbueHkpZ18t8Tb0yM2iDknBieF4FxchIcVHvY57XG6HAC/s/DG\nSX8cBlF4uLjGHst0HAcHWb/AD0sJDx8HD1+38+twsY1zUjpQovQmTdiGn3zB1l8qHjlgy/4OT0y9\nxCn1BivdSb7beS/T0VVicg4XTSoE8HsqfGrw9zgdvk5G7OP/ET/DWd5EbAh8afOj6P0wF73NE7yK\njxoFolzjDE/k3+CpymvURxTclQ6efIt60kXe5cdSShxZuE8roFE67eUYd3GH23AKJMFghmU+3Pk6\n3bBKRoqhizJDuxmiuSXOqTeRXAaGTyCbCCK4YXcihu9XaqTcQ9wTZ8l40yDoPGO+zHhhi4RcoBRt\ns6MmWfMMM0Kqp6TIlDjx0j3mlxcwoiLCL3dxr3VQ0zpiyCKYaaJZJtsfGOJP6x/npfxzNEdlkr4M\nXUkhTT8iJhOsMcgOCfYJU0ShwzZDxMkyyA7DbFEAzKyIVDNxnez5SYco08RNZKdI/94enzv9u5Tj\nAYJmmZC8j7bcJrQCt548SiEaxvJIqHKb+0xxSbiIx99ihE2e5mXC3iyiZfIp4QuEKNK/v0/gKw2E\nNoh9Ft57XWJjRQqjEW7LJ5iprTHVWqMY8tEecWFqFi+HnqaMj1EjxanUXZ7hVZ6d/x4+rYZGExmd\nZWbZUoZ5IvgaXVHhvjXFYnIKUTIwEPFT5Svf+hvAG4/69n0XhAtIIKC9BVZOHtgJTHaW6PS9tvdz\ngq/meP8wheL0p7ZpAudiopPrtq/FpkCcHLB9bU5eW3Ccy874GxwAtD2myg9n7arjWJuycFI4dtjU\nh5NTd163U/6ocFDkY3P/HQ4opoOnARWIcqBT+enFIwfsGj5cQpPb9+dZ7U6z7x1gMJkmKuc4zm0s\nRETRRFU7tFSNlD7CXr2PG9o8XqVJIFJkwrXCY1xhgjUkDEQsgpTRPSIFIYAo6ZTdIZphL25vlYhc\noKvUEAZ0PKaOvN9lPLhBW9PIy1GG2CZi5lkyZtmRBtgT+ygT5KPerzNc2cG/VaUx7KLW50ET2xii\niO4SqSU9Pa0yY3ilOh1UOqZC1h1FkxrolsCifpSV2icJWFWe9LzCqLKNP1hHHDQxQw84vBJYZYn6\nhAst3yFcKHO8co+m5scdbXJVnccn1JDRMRFR6BI0K0xX1hkqbeMt17E0gXooiJ6UiZOlz9yjo9fZ\nH45S0YO05V7JO024mL7CeCaFv1jjwvIb1EbdCAmDQKfGRmCMe2NHMNxQkXxUpQCD7OCl3svopQoy\nXSR0qoqXYLnKqXt38SZquOQW+nEBsyogKFbPm6WbpV7y8gP/RSS118D4NfEcoVCZMS2F5m4RxEAQ\nLUrBAAGpzHHvbbRuh3S3n8vKecoEaQpuVKnDqe5tju/dZfBGhu4Rkb2pOFc4jzH1Zz38/nWKHqwq\niA8t5sEPl3Q77Uptfwy7EtKZbTt9QOzs2N7HuchoA6Kz4MXOOg875Dkz5sOUiODYZgOO4DiPsyjH\nCfL2mPb+bg4A2XJst2HUqbG2x3Bm0vZ1O+kUJ9d9QIE8XDV58PzydoLAdzYeOWCX2iEKxRhvLF2k\n2IygRtrUAn4kt864tc5UeY2OoHA/OM0VznPPPEKr5eaOfJyYK8/owCrPWS9w1rqKV6jTQUOjzQgp\nzACsB0bwUierxMn7IkwJK4BFQe2SnpYJZaqEVuuMDacoR4LsefqIkUMQLV4RL7LJKBmSlAgxHl1n\nsLuDuCpRU920QjIa7QftykzqeMgTJUcM6UHuUhJDrAXGsDDxWxXS3QG2GheRTIsx9f8j772DJEnP\nM79f+vK+urq62pvp7vHe7c4O1oBYWIIACNEdqaMUIYlH8RhxokRJoT8khhQ6hY466EKhuzjyeDzy\nGLQASGIB8Ba7WKzB7s6O99097V11eW/T6I+a3M5p7Ikgl4OdCL4RFd1TnZlfVs/Xz/fm8z3P+y7T\n9d+kMy1jjQt03RJtTUJSoBVwsz6WINyu0mcVmK4vMhRY51DiKv+GXyRIGQ8NLAQELFxmk5HcBkNb\nmxh5Ad0n47MauPpbhJsl4p0cpWaVyugoW1oCFy3qphet0WVm+waRehHF0EluZKgHNDp9Eq5ul7X4\nMK8Pn+c4VxGAKv7exm93i0Qzy6i8hqkItBUXdcFHsFxn4GoGccqkOyFRvahiXDFh24IYhMwKsVqR\nsifMhtZG0jq8wxliUhbZ1WFUX8HURSqin/t9kwSFMvusBRL1HEvCJC8FP00/abzUEbA4l7vEx+6+\ngfAdqLjdVCZ9zDHNwJm/D3QI2DmljPlIx/K9tT72Zqh2s1weHmv3V4RdSZ2drcJuFruXFnDy5U76\nw85AnVSMfS9OoHTK8ODRrNiWBdrf71Wu4LgOPFra1Qm69n3bC4Lz5zYQO2kY52ak02a/txPNbkpg\ns+gfvbzv8atEql4u3XiKmhSAHZCuGvSNZtCjCtc7xxn5Vho8FpkfjzPOEoJi0Qj2MluZLjoSSXOb\nhLXDHWk/piDipcFhbhC0KoiWyYo4yqixwgnzClk5zj1hP+8yhp8YR3O3OH/5MlMrKzAl0jjpZoxl\nuigsMAWAhwbDrHFfnOF+fJbsxT4GPBvMcJ8j3EDAxEB9vzu6jE4/aYKUyREjSwwJnVFhmYOu2/x4\n5F/gos2kvICoGuyMhClZYYpimLLixzwmkTH6eMt1joHpbU4mr/FC+TWMDqh0+DQvIWLSxEXWjOMW\nmpimiFUQ6HhkKgdc5KQ4lmbwaV4idT9DNF9kJW0xVlkhFs9iIHGgPk/bdHHjwAEm15dJltI8GB/F\njIBXqOFytYiKGY5xjXGW3u+jaCISTFeZubGIK9GklAwQGCzT394h1iggNEyYB7Mj0oq6MG/p8K4J\nz0Du6RA7o1H6lS3CFAg+tK8HKDNobBIvlZAtg7LHx791/QPSUoJ5a5rPp1/CJzQYCqyzJIzjpsnT\nvEn4jSLCDWAa6gkvYHGOt58UH8OPIFpAlg5tdHrKC41eeVRbrtZ5+G8nVeLcWDQfXsVZL8O2CDjp\nC7vZgcWuLtupuoBHM1Uc17CBzq6E51Sd2Hy2ncnbpp+9iwzsgnCHR5UdAj9oQXcuCDju1b4n55i2\n9NFZSdCkZyKyS6va13Ee38vIO0CBH32J1R+Mxw7YjbSf5lAEBgwYMRE0C7e7SRuNRXGcwlAQj1bH\nQmTUWqZdclNY7UMdbCFFuuiizGXhJBn6uCfMcrZ4iYOtOcLBHGU1SEbqQ0YnLBTxC1Xe5QzvcYoH\nbDJBGF+4gTxrInt0OmGZCWuRgfkdsKA5dZmxq6u0Om7k022kDQu9olJOBHHRQKbLAlN4aOChjkKX\nftL4ujVSG2nqbi+j/SuImPipIGPglyoc1O8wkV/F7WrQcSusekfeLxDlpkE0mMdPBRMJv7dCQC2y\nKSdpuRVqeAhS6mULusFndr5FSQtSDgd50DfGkjLMSnSIICXClAhTwB2qozQ6iGUIXq3jSrRo71fw\nWh06kkbB76c5oLIUGuFWfD8JNY2LBpflE2ySIkeMAhFq+CgRYpAN+rUMgUiZetDDjjvOfWYIS2Vi\nrmKPziuDtGnivdvG8kPzuII6rqMEOwTFIsOsEdkp0lfMYQ7LWB6LvBDlvnqQOBnGpCUQehn9ijDC\n9cBh/EKV48IVGnhwmy2e6rxLf2Gn95c6DkZYootKG5X59gxPROXTxx5VYB6R6iMbjs42YE6+2s4M\nbTu4s2ToXorBmSE7N/T2ZqCa4zxnpmoDqrNQlD2+E4ztsZybijjec97TXlkhjnNs+Z2tiLHDqc12\nbkY6P699jL0xaUsMu45rO6kTcN5XBZgDKnzU8fgz7JwHUdVx9VWxhmTEroURlajjpaOobD3dRx9Z\nPNSJWnncpRb5W32I7g5SqAMifE+8iJsmOWKczV9hurBIQ1G5Kx9gQZ7gILdRhC4lMcRd9nOLQ2TQ\nKeHhQWqcxdQYYQqMssqseY/o7RKq2cE3Xsb3RhujLLN1NEZ8rtQzdhyGrdE+FqJjvGecwkudfjFN\nSCsyKq4QbFfov5WjEm0xEVnEIzeQTR2jIyObXiLlEgfv3afZ72I9McCGN8XGwzZnUfIMsgHWJltm\nimPlK8w077PgnaagRTAskf5uGlE0cetNfjr9xyz4Jvle6ClWY4NsS0ne4yQXeB2VOdw0qIx5kZUu\nVreDettA3DQRBkwkycRrNpip32fTN8BieJJFcQIvNQQsrggnWDImKBtBSnKQmuXHNESekb/HbHAO\nYwYyvgh31Wne5AJRpUDEX8TT16tJIlcMgrcbmGMa5X/kJlSt4u9UkLIdTE0ksNrAne5wKx6h6vFi\niBJvBp5myFjnOV3ARESjQ1dQuTxwjKS5zVh3mX3SPBGjzMn2NUSfRSkVxBoVKAZCZInzgCleybwA\n/C+Pe/o+AdEDCw+V9/ue2KBoc9pOZYTBrsXDzqLNPS+7ZogTHJ0d0a09xzqr4aVsA0IAACAASURB\nVMEuJWNTCDaI2ouGE5zh0czbWZfE3HNtJ8DuBXMbVO17tWkQHPdrH2ef71yEbNONszlCk136x2nj\nd1YZ7C1WFXqdTf4eADZJE9/BIuf73qKm+HhgTbGojTPCCtPMcYeDVFljkgXuizOU+3380gtfIR8M\nk5XibJNkgkW81Ht6Y6VK1ePjuvsAd+RZygQRMckJMbYYICSUiJIDoEqAGn52SPApXiJKjrBQRIl3\nqVp+7ktjTCmrBJQaKh1EzF5l9zmI1kq4g/cZzW8iGSZiwKB43IceENE7EtYDgfBWBTXYJTcSRC11\nid7LE6/6SZRrWHcErgwcYSucwCfUOM/3CVDBTZM6Hkxd4fPVl9B+p4D0Zp2DH7/H8oUxMlNRxpY3\n6ARktpIJ3tl3klCnys9u/wnaO21uRg+Sfi7R60pDkQQ7mEh0PCrEwPwYYFq4rxoI7p4A0rOjMzyR\nRpmCTW8KSTLRUTjMTVYL47yXP8+xoUt0mm7mt/cTHP0GfVYWoSCyqo5yXTnKJes0EaGAp92iP/sa\noqL3uh3GoFIOsNFOENxcQL5r4FvtMC5ssnk4yfVzh3kt8AwCJsOsc4HXmcsd4L/d+ArGpMlQcJUj\nXGeFMa41TpBLJ/ls4qvM+O6w6e3j/gszrHZGaMc00lqCNAkKhMn8ZeyxT90nI9oIFBiiwwg9YZlO\nL3u2Adt+/LcBtMWuhM9Z3AnHcc5M0qYOnBZ3HOc7qQKnxM55vJ1l25t2dgbulBg6GWAbvO1FBR6l\ndJwcuD22vajYapEPyqTtc+HRe3U+Fdhct7rnOHtsW0miASnATxso8mjJqY8mHjtghzwlDieust99\nB0OSiFlZbjaOkRUTDLvXWGeIImE2GGSVEULuEhfcr7PIJDJdNNqImHRQSbFJM6BxV5vmtrYfXZQZ\naq0TXylATQBDJqjUkRMmadocZocSYYqEEbGQTAO30aQ5pNKxFELdGuJBA6Nt4RYbKLEutQkvq4FB\nYoE8MSVH0FdmQ0jxwD/JqjSIgEFELWLMqGQ7Se7VDuA2SswwR0rI0iFO1fKDZRFsV2i0XehKT7tc\nIsQWSdYZoi24mVSWGQ/oDETKeKUym3ToiCqGR0RSDTxWg0i7iGZ20DWJYLzBcGCFs7xDiDJlgqTp\nR0ZHclvciKYZnXCTKGYYvb/BncEZymqQk6vX8LqauPvalFwh2pKKjkyFAHk9Rq7Vh2iConQQvTpR\nKU+oXsLKSFy+e5ob0eN4zjWYY5qIp8jB0XvIko5W7RK5W8KqChjIYMBGYJDCcIgUm6wODPFe/ARt\nNIqtCFutIS76vku/ss1Rz1W2pTgJdhhlhVVGaUhuTDfkpSjzwj425RTF/jDrjWFubx9hKLKK313j\nRvo4hQePu4fikxI9KImPmPQJsL0GhtkDZSdY2Zmxk7rYC9j2sXvlcE4JnQ1mzvOdGagzm3fqq/da\nw+3rOYHQjr3ZLOyqSpwLAI6fOYtF7W18sFfT7axrArvUjVPuZy9Q9u/O2XzB7j4jiBCIQcxjwspH\nz1/DjwCw++VtzvtyxMkSpshB8w6LlVnyah/r7iEUU2eeIKviMBYCJ7jCx3kZ3VAwLZmwWGRRGKct\naBziNtlwhDI+1hhmH/Mcrd0k9U4Gz2aTKWMFfJA4mWGRAJ+k0gNHNBS66LqKWu+SjYcQDYv9xQXq\nZxU6moSqd5CSJoV4gLdTJzlg3sHXLSGbJvPqON/RnmOBSSIUmfLN0/iUm++mP84fbP08z4l/hRz4\nKofH7lFciZBWYpC8xf7OHJFykeu+/Txgkh0SZIj3OsbIHvr8O/zUj32V6UPrmKpAO65RUX3sjEQJ\nGBXC9RL7l5ZY86e4OTnLgadvEyPD891XWZZGuSEe4U2eIkEGwW3xdmQFdyjGifp1+oUcryeeYtkz\nynR7HrFiUKyFWY6PYSKQpp8CEdaVISS3jiGJuP11BoPLJKxt/MUqRknixp8fZ2VwnCPnL7MojHMr\nfJCVUykk0cB/o47nzSbigIkmtRC9FnOnJrkb3cdF8zWWhWEeMMEUD8g2klwqnCesFnkx+E1+0vfH\nfEt6EcOUmTSXuCEdIeXeIJl6jy0GWOcFwhQZYRWrJnLj7gmOzlxnf/Q235z/PHUr/Lin7pMTAviP\nCQRkAXHTwjR7mawTfJ1UguJ4OUud2lmqym4W+agaYvdaNmA7qQ541BFpW8Th0U1HJ5dt65qdhZbs\n7NhpAxcdx9pA7OTW7Q1Tm5d30i57i1rZ4GwDsN30wPkUYt+/fU/OOtu2Nb4jgzIB2oAAqzz6+PER\nxWMH7L5Ymlt8iqd4q0c7iC2GIsssCuM8MCdoFoIExDL7I3cpE6REiH/Pz3J/4yCZRj+EDUaCywTd\nJd7lDM/xKse4RpAyDTzcMfYzVNnB42n2nl+ioAx20Tba+M0afqGGX6jioYGW7aBeg1iljNAGQbBo\nPe0hPxGkIgcYKWyh1dqkEls0VA8L0gR9VpYBcYOLvEaU/Pt9FA1EBsNrnHK/xUXPd0mwzZwwTiqz\nyfHiJs0LMhlPnA1PioIQJkMfeaIYyIyy+r69PqLm6YYlSjEfTZ+CAFQIENqokrhXQN3skgqmCTRr\n+LxVFL2LWRdRp3SssEALF3U8jLLCU7zFC3jxRJusPdtPIFhiOjOH2u7wZvA8bwydI6CWaaOxTT/L\njNMOyEy67xHSigywSZ+VYba5gNfdxDwKPzvwb5nwnOaGcJgZ5jjWus5sfhECBrVhN3d+bZLcu23q\nkg/TJ5LQdtA7AgNbOZ7zv8ZwbJUFpjjjf5tjriusaUO8Ij7PA2GS053LjFVW8RUbTA0s4fK3GWCL\nIGUkDMZZooqfRsjD1Ok7rPsGyKkh3McqJAZ1tv754569T0gI0HhGpaZpdF5qIXZ3nYhOcHLaqu3v\nnRm3k9rYm3nbYRtJbLOJTUPsldL9x/TSHX4w47VVIk69tU3rOM+1N/7srjd22LI7eyO1zaMVADXH\n+U7Znj1ulUfrjzgFek5teOPhy/1wfEUWaM/I1A+54Ks8EfHYATvsLqJRZ4cEhW6ETkcj6CoyIT2g\nYvlZkkJUakGKxRi+RAXV1yZHjJSyQVQtsC6lGBC2UBttrm6f4k4kS8KT4Vj2Bi3FhdmUULzd3v+g\nH1gFWdPRzA6ecouUuM1R73UakoeyEqQQCPce3bomuiTyrnaKrBBlWphDMC0wetOsJbqo1f30L2RJ\nBHNY/RJva+cRRYMaPtL0I2oG55Tvc6JwjZico+F1ESxW6Mu2aR+UWFAnyQtRhtrbZOUEHUmlg8oo\nK4QoscgEaV+CgrSOqBl0RY0SITTaJM0cHqMNErjUJoLLYE0dAhGiegGPWCdGjhg5ZuoLTFoPuG0V\nUdAoukJsp3o9q92NBgtHJ7g3vo8N3wBhij2u/uGfSVzNkFI32M89gpRR6VAVfcy5p8gGIviSZYaF\nFa5zhGOdG5ztvocmt2iIGq2gRuO4m9p9mXw1inFFIjGYxTtQJ1isEa6VCDdKeF1t1r2DbHqT1PGw\nziDbJBkSNhEkKKhxZLHL/uo9JraWqSk+LJ+AL1ZmTpymqyrIic7DR26D/vgWVlz4e2FMB7AQuDlw\nEM0l0RWvYj2EXmfN57066L01N5zORGddDpvasLPpvQYWZ1JpA6RzM9A5vg2sTjmfDY5OyZ0TVJ33\nbf98r5nGuVjsNcE4XZbOzVI7q3fW4baP2zueMyuHXQqlLUqshofY6t/PkxKPHbB9VDnINd7mHHda\nh8hX4nwm9nVOSFdAADFkcT93gHffuMCzz/0VSd8KEgafTr6ElzrfFl4kZuXIbiWovBXlraMXkAd1\nPnvjPzAY3ICwgJB6+OtvAF8F+WkddaCDO92lX1ohmdriG9qn2YoniUWz6KKMKrQJUeTrfI4iYc7x\nNpq3TZUgZUJoZhMt1yH4lw20mQ7ZZyTejpzHJTYpEWbFHGVQ2OC8/jaTa6t43VWqE26UahcxZ6G2\nTO5LsxiWzBcqL5Hzx1gXBymZIQJiBZfQ4h3Oovi7JF1bzJYeYKCQVvqRMGgE17DGwQxLNOMy+akA\nr3AByTI5zSX62GHCesA2SV4svErEKnDJCnOfGQpWBNXsIIs6Vp/A9754vlcCgCpN3Ch0iZJHRyZM\ngX0scJyr5IhzmRN0XQolgtzlAKe4RAsXgmVysn6dY9YNcgk/O0I/DTx4qdPGSybTR+ePFPrO5el7\nLo+hS1g5kdByg6fil/jGUIRL3tO0cNFBpSwE+a52kYbm4Vb0ID/DH3Bq6TLH37iD4LcojgSYj4zS\nFrX3i18d5Db7mMdERDU6vPW4J+8TEhbwsvFx8sYI57mFjvG+Jhse5ZWdumNbH21ztrbxxN60c5ZM\ndSov9mbRdtig5mx04DTR2Bmws+Srs0KesxmBk7O2x3NSG3vdjPYTgr1ZaIO1XT7VSZnsdWPuzdj3\nhq3HtlUknYf/riBz3TxM1XgO6++wh+iHiccO2B6a2C2uZtx38cs11pUhPNT5pPVtzhYv890rL/Cb\nv/vfII93aYx6WGWYB7kZ3GYTX7zIldIZNtIjNCpe+jqbxDo5pLROI+Ci3S8T6DaRbxtwC4hDK+Wi\nZnnpmmVEE9xNnbPCJcyySGSxwo2ZA2RiMQxEzvIOOyR4hedp9bsJ1SucT79DsFrBXWmhnu4yPzzB\n5eAR9klzNPDQaHv5ycWvUfd5eW/wJCvjY/RL26SkDTqjDepHIOsNk5C3cW91EN8ymTl1n7XQIN++\n8zmWxycZTi1zjGuodLgrzRAOFIlLac7zffxUibeyNBoeXh8+TzoUp4PCNgNM1RcZL2ygKW18cpeA\n9B36xQwVxUdV8LPAFErJ4Iv3vs7KyDClpJ/T3Utk5Tg7Uh9uWuhItHAxxBoiFgEq+KiRaGcZaWyx\n4BvFozSYZJFXeJ7r+hFWmyNc0o7hlquoQhMAA4kHTOJhmaHBVe79yiQj/g3UaIdX489SNgJ4jDr7\ntAVqbjdj1jKnjPfwC1UKUoSvGT9BmSBPSW+h0aEa9MMBwAeNqIc1cZgbHGGZMYZZw0OD1kOn6+n3\nrvDbj3vyPilhCWx8Y4yIbHC8K76fSXZ4tN6Hk8+26QUbKPc6/Nzsyv9ssHXK3GyruhP47Sx8b9ME\nyTGGDdRORYiTEnEqNuxSsXYmboOy0+TjHFOhl5PVHOPguKYzM7fHtekfG8idTx9OyaPzSeL9z9iR\nyF9OkE6Pwd8XwK6WA7hoodDFL1fpkzPMsQ/BEJjtzuEzm2wFUvRNbqP7JEwEhtjgHf0pFEPnJ/gT\ndoQUuC2eG32ZwdAKY+oihWQIQdRxZZtQtWCFXvXDfeCKt/CmBZRir5+S2Gcy2NlCyIJ0T6AzoNHq\nevBebnOi/zqlRJjN6AA7rgSmJJKsZQgYZUruIG8MnudeZIpV1xAKXbzU8Vp1DnXvsqBPsC4OkQtF\nqeNGtVpUYz7qcRMxbTGlLqHUuzRdGmkpQV6I4ZHqFIQwYJBghzYaaTHBFe0YYYqEKGEiYBkCeldm\nPZDimuso2UacA9ptUsY2oVYV2qBpXdz+Jg2Ph6blwl+tUWoFMAS51wtRKNJEpShEaOHCTZMkafJE\nyRInS5wIBSJmkUClRlzPg5QjQxixbbKv/oBF3yQlMURMyFFXPTyQxxlkAxctPEaDSKdMrJknRZOl\nEyMoRgefUaetSpRFL2W8RMkSrpQ4l7vEGe+7hNQSFQJsLg6TdcUYme45T1e9I1wa6xJxFci5IswL\nU9Tw4aVOlDx97NBPGgWdAfHvCyECWFC51KAlNojq1vsdUWzXns3LOsF1bwa914jiVFDYwLW364rk\neNmZrbM8q1Ph4dwodI6xF2Cci4Z9D9YHfN0LovaY8KhByF5U7Iwddp8AdB6lSZzKFnuRcPZytN/v\n0svKfbpFd6FNZavxRGw4wg8J2IIghIDfopf/WMA/BBaAP6JXln4F+LJlWaW95y5tTvAJcg+zIxcF\nIoiYxDsFJmob3AlOUf+kyuyL16kJHgbp8J/wR+Q8MbqWwpeEP8UbrpMPR/nF2X+DIUgUiDD/yTFm\n39OZfS3X+w3feXgXp6EvkmVoW8C/qmP6oXsI1JqFmAdzS8BoSrjvt9j3j1YQP2HCx4Ez8N3Y0+TV\nMEqwix4XWHQN8b8qv0ZHUImTBSDFJsPKGq5UC0OR3gdCA4m64KPgDVHttJl8Z43haJrGkEbmM0H+\nTPoJbnKY5899ix2hnzT9XOMY+7mLSodv8Bn2Mc8s9ygSQsUiShkXLTabKd4sP8OLsW8zq9ztNeKr\nQ1eQqIRdrJNCyZvs257nVqnNfP8gS2eG8Ap1RAx+T/1ZfNSYYIkQZVYZ5nUucpPDfIzXON99h/BK\nDcWjU5vQCIolvLk2gysZfnHyd2iEXXR9Mi/zY2wwSIgSKm36ujlOFm+TK+r0pyMsjYyQVhNElALP\n8l22SbLGEF7qjG5uMHxnG2G/BSHwNvP82le/wnp/kuvT+5ljhmuuI3yv/wInuIKAxW0O0UeGUVYo\nEmaCJY5wgzJBMqf6PuTU/3Dz+kcbFixeI8Ac+zG4zG4bLdhVWNiqB5uWsMHMchxrh12ZrkaPWrGr\n9tkg6DS62LVJ7HraH4RdToWywG7mb9+DbTXXH44Jj7oVYRdwbcrDVoTsrUViF7WyFxFnLRDb+u56\nOI5tPbd/B5LjWNuO36X3xGE9HLMGDAKzpo5nZxG48gGf+KOJHzbD/grwTcuyviQIgkwPMv5H4GXL\nsv4PQRD+O+DXH74eiW5K4vXORa5snEX06Az2r3CK95DVDr/l/XnOLl1iWNvEO1bnC42/AAv+pfpf\nEnIViQoFXhY+ziYpwlaRgFHB916TgVs5uhWF+oybK88fpGO6GEikGZnegElQRR1XHaRBi3wozIaU\nYPz+BmZLYv3zA4zOrRF8u4qomQg1i1wlwq3Afv6s/iW2K0naQTcHlRvEzDy/lvu/qLp9ZH0RXucC\nSWubA9zmr3zPUZN8PM2bmIgEqBA3ssS2CwTLBpmzIZa0cYreEKKos6MnyFtRVpVRppnjILdZZYQh\n1kixSZJtYuSIk6GfbRKBHbqCSFXzcUq8xKelbzKpLPBq8zle1T/Bz4b/HV5vhbc4xxQLDPo2ySVD\npILrSHRoCi48NAg8bGwwyAYjrFDDR54o1XaAykqUjD/JWmKYwEgVv1ylJarkhBilgIEy3kHxtsjQ\nx3WOYiASJUcTFwo63na956rcBhaBAZDVLm69RaDSZEuTqHoDhCmSHwiiuyQGjCzuuRbcB6HPwjvV\nIMUWEYosMsEbXMBAYjy7wn9147fxeusU+kK8MXKOsFVCMQwWtCluCYeAVz7s/P9bz+sffbRRTnQJ\n/ZKC+s+6KHet98EHdru7OI0ie8MGNltpYVf0s4HTzixtwMTxPuwCusVu9xenJNAOZ+Zs91O0y6g6\nNybte3KqPZwLjFNB4rwfmwKyAd2md+zPb59j0yhON6PdEcdZetW+T9sdCiA9qyD+nB/hN4CVj94w\nY8dfC9iCIASBC5Zl/QKAZVk6UBYE4XPAxYeH/S7wGh8wscWggY6ManSoNAOsV0YZ8mzQlhU2tSQt\nXFhGr2UBpkDFCnCLQ5xULuMSm6wyQoUAggFv1i4y3ZhnpLJBciNDeipGNhVhw5VCdXUYiW+ADJZb\nwBREKkMusr4YG3IKU1ZRIh0ah1Sm5leJVksQhu6ARDus0Mkr+I06FbXJWjxFQt7E023gtlqErQJh\ncnyPZxAxCVgVDF3CQ4OEsk2OGH6qxMhhGBIr7iEWR4dRGgZdVApCGMOS0Kw2JSuEW2gSJ8saQ0Sb\nBab0RXSvhCp2EDDJEqfl8aCoOpYCh7jFOS7xQBxjURrnmnqET5VCyJ02ZU8QHYmq5mMtMMiUu0OS\nbbqoKEaXZC3NifXr1ONu0okkbTSqBMCy6DfS9Hd28Ol1WkGNkuhnh34qBDA1kZwWIUaeAhEWmCJG\njn7ShKwym0KKbWGAlJphU82w5EqyJQwwyAY+q0bLcpG3Yg8t+QLtoIbl20HLdZDkAG3FhXe8jpA0\nSO5kqIR87GgJREzqeJHbBud2LqF4u6SVPoqpAAP5NGpDpznioa56P9TE/7Dz+kcfBrlYjDc/9knK\nv/0awkM3r3Pjzn78d/5R646vToONE+jtsGkNmwe2+V7nJp645/wPWhjs6zjHdNbcdoLwXoei053o\npFrsn9vn2xSO/QTg3My0r71XPeMc36k1dwK2fc/bAyOkL5yj6i/wKCP/0cYPk2GPAVlBEH4HOELv\n+eBXgYRlWXb7hR16RuUfCC8NnlVfZXBinbeyF3l37Slaoy6e832HL0hfpTDlZ06YIE+Ur2i/jITO\nsLJKgZ78bowVGni41TnMH2d/js8d+hpfPvSHXLj9LgOeDFqmy0ZyiG5U6S2XVWgENUpBlcWpJEUh\nQkP08vrZKZJs86zwXbwzzV7xrW2o/5gLbV+TZ996k2eG32FnPM47HEdG54Eyzv8d/8dc5DXO8i5N\nPGwJSTJmH59Nf5uKx8e9gUlKhHDRIiwVWR9I8QcTP8kbXOA3cr9B0lrjD4e/SEzJodKhgYcCEep4\nucZxjudvMVt5wMp4Ct0lUSTEX/DjlJQQEbnAGeFdJtsreJttVrzjiC6dL0b+kIPfuUtC3SH45SJt\nQWWNEe7jJkScONle1t+tMbyyyfTvr/Cbz/8KX3vxs1zgDVpohLUiR6Zv8FzjdS6W32IzFOeOepo3\nucAUC7TRWGKcJNtotFHpsMUALqvFJ81v8b+Lv84b/mc4dvAqudlXqD09y6o0wqfMbxIQy6yGR7gv\nTHGX/T0dNu8yJG2wEe9nJ5pg53Q/49IS41srDF9Lc+/oDMv9Y4iYpOln05PDHBPBhJia4xPGX+G6\nq1PLBOjvSyOpHzrr+VDz+qOI66Xj/PK1/4mj1c9zhNcfqR1X4wd12PYjvk0JuOhlnG7HMTbw2aYX\ng142bGfae80tTi58ry57L/XS4VHzy96NQTujt+3vdjbuNO/YmbPdxssZ9nVajs9in2tTPl3HtXk4\nns2/Czxqy3fKHd/OXOBrl36TZu1/4EkKwbL+/9l0QRBOAm8D5y3Lek8QhH9OT4v+y5a1azcTBKFg\nWVZkz7lW6OQYqWGBOj7Mqf10x48w4lpBzhk0Vn0k921QDfm5a81SbwZw02TIu0qYPAGquGixyihr\nnWEy1QSDnnX2K3c5WbuCKJo0FDeGJtJnZkl2dpBaUNG8vHZd5sx5kRYuSkKYLhISJm4ahOpVXOUW\nYt5CieoIbotOUybj7qPq8aOobcJmEcOSeVs6w5ixyoi5ynX5KOF2kX2lRXzzdZaio9yaPMDkm0sk\nSRPcV+bV2xqDF4ZZ96cYaq4DAsuuEapCgDpemrhJskWACjX8xFp5fEaNjDvOUGWDvkaWq7Ej3Ddm\nSbcGGPBvcKp7hbPV98iKMQquEFWPl+TONrqgsNI/TPChTf07b3k5+ZRClBxtXETNPP56DSMtcy18\nlPnYFEHKtHBRq/sQ7ojsD9zl6Pg1CnKImuinhYaMTgMveaIEKOOljosWbpq9UgGWSU3wYyISpMRb\nb4nIT51CR2LGmmPamser17kqHueGfJhRVrAQ0C2ZU8Zlgq0yektDDHTxtJsE8g1W4oPkvWHaaNxl\nP3JX52LjDRK5HBptakMubl5VuHFfY8s9QEdU2fn6u1iW9UFP5X/9xP+Q8xoG6LWOAog/fD3m8Ptg\naIBTG3/AJ5trpLuPbpg5NxmdIOnMKJ3dV/b+4pyWcRc/mG3fAk4+PMYGxw/aINybddvZtj2GU8Nt\nv+eU9znVJAA3gWOOsZy8tq1e2WtTh11Xo3Mx0ByfySkdtI8xgQEJ7oSO8vX4i7D8JrQ//H7JXx/Z\nhy877n/g3P5hMuwNYMOyLLsf058C/z2QFgSh37KstCAISSDzQSfHfuWnOfXTg1iSQFaIUyTMCSSW\nr09y6bVPE/3kywTGGsTNCfrLAn1ChpmQwbjQwYNEjhhVzpLTpxmsy4RcJXzaGFMYdFDJGzGUms6U\ntMCMouBqG5QUP1tenS/+VBVTsNgRFHRkioTZZIApFohSwEJELAs0DA/pUIyMeBgXCh/nZSYLedRS\ng+PtMkNKjZS3xe1omXi9xORaBdENL01Msnr2k3xx/V8zSwvjogdLaPK5z26TjzepCx5yQpQpKUID\nDyVCbNNPEg8JdvBRQ2pHqRkjzLv28dTm9zmdy5Da58Xb3cfbpQvkfS5U4y/5WGODiJGn7If5RBiJ\nQXZI0OEwfWQoEMGHyce+XGZ/t8R2O47q9oNmPXRYjhAhRYUgBhKdvEbaGmR4MMKZiyXWXYMYkoCH\nJnmiFAlTtfyMlVYICWUImfioYSKSJc4Iq/jNGoXuMEumjP9nThOgzLFWnUPtEhGpiKhOUlbPchyF\n+51ZrreP81Py/8bHqq8zkE9Tj7qR6ibedVichVJcR0DnpXqClu7horTAvrU6wY5OYZ+HkZ8/Qlw4\nzTv6OdYZYkc9+jf7m/g7nNdwFjj0Ycb/m0dVhrtuxkYifOZwh1uXs3RaxvvqDKcd3QY8p4rClvnZ\n9aidygqntE5hlyrZW/f6Ezxak8TO4m2eWHZcz1ljZC8o22Bsy+3+Y7U9bCXMp3jUBGNn6M52aPam\nIuxy3DZg29X67KcIp8qGh/9uAIZL4vDROEo9xddvxYB+envSP+r4nz/w3b8WsB9O3HVBEPZZljUP\nvEBPk3EH+AXgnz78+oHFiTNGgtfrz/Bl7x8jyzorjHCPWTKDScznBYqxEMNCifPS95kN3WOALbxC\nHY022yR5wCRFIoTkEof8t3AJLYKUMZBo42K7leKl+c9zIHqTF8e+gUdpoggdaixRFSFAhQQ7LDHO\nBoPMs48wJQQsKgS54j/BPWZIi0kKRBhinbO8DesS0StFLt59G2lUxzgukvDt4PE00EdADoPi7cnq\n8r8a5AFDNF0ecgvr6GGT8fo6hiCQUaPghj4ytFG5xjHqPXEgCl2OFm+TE24CKwAAIABJREFUqGeJ\nD2aJDOQoJnzoisRp620OqLf5f5f/Mdc9x/nm0As8130VRepgILFJiho+BtjiHrPkiBLh+xxoPeBc\n4TLGtsTOSITV/hRZ+phmjgPc6XVrYYuh8DrLPzPGTOkBpzauMj80ypannzw9fbqHOglzhxfuvY4l\nwWtnnuIyJ3HT5DleJUucV7ov8Of5L5Ds/J88zyWGWGd/dp5Auc5r4+epKV7GWGaZcebLs2xmR/mz\n4S8hhC2+6PozvDstpJsWvAv+cBUzbtHEzX+69fsEynXc3iaEdHBb9HXyZKR+drR+Pq98ncvWSeb/\ntn8Lfwfz+qOJnsZi8ekhXvnSFOp/8U1crfr7nWjsr04pnuvhmTbY2XzyXvrCaVYR2FWa2ADupFv2\ncsN2diqxq7awNxjtazrPd/ZktAHYXnDsY+zO7zao2kAOj2bsCrubj07+2tnqy+a57UXJXlzsMZw1\nw2shF2/8+lPcWJyAf1LjSeKv4YdXifzXwL8XBEGlpwf4h/R+t38sCMJ/xkP50wedeFp6F1kZ4nLt\nNP3qNl/W/oTx4hrbxgBvDy1RcIdQ6HKYm9RFLzskGGKddYbIESNOljxRtjqD3KichJyAx6yxOTFI\nWQ+zVR2k0a8S8eeYaC8RnS/hWm6z9Z0i/dUu1VKHlYJI+xfaBPeXGWOZscY6yXaaVtfFcmCcsc4q\nn15+mcqAF3e8zpi1gq9Qx2pA96KAEBBQXDp9xSLloI8VzzD9cobJ/AJfXvkao4MriMEuZU3HlEU6\nWQnlPZ3C8SiNITdR8txlP92qypmVa7BlYcgS5jmTit9HxQowtbZMWCzSdivUYn5uZY6wtjHKZGKO\n2cgdYnKWq+JR+vQ8k41VBE0gK3Vp42KKBcIU2UbnT+99ibv5Q/zc+O8SVfI02y4W1S4dQUWjzdPW\nm7RwkRb7WfGN0CdkUdRWz1qPmxxxNhnES50ZcZ57I/swBIkAFZ7bep2W6eLmwBEKYphtKQkBk5ic\n47i+TKqRQXF1qLlcBNQKkmBQIsQ6Q+RbMToljbWBYW55DzLuWSIV28Y6KJKLxsj2R8jQK6d7LHaT\nGc88XqvKkm+YddcgFTPIjhxHo9cg2CW0/g6m/99+Xn90YbF6Pck7zVF+rPYdZOqPbADupTuckOOs\nP+JsXmBvuDlrgDhNJs7NQCcw2tdy1jJxtthycs7O3pF7izXZ48AuuNsLDHvGtYHVHsdenOzP4uxS\nY4fzc4mO69k6bR0o01vcolWNb/7eCa6V+ulVfHqy4ocCbMuybgCnPuBHL/x15+6T5nBpd/kPzRcZ\nMLa4aL3OoeZ9dtQ4/lCBtzmHjxoxcmToo0wQD3VWGaFECC/1Hkdrhlho70cvKyh6m4weRe3qKJbB\nYP8q0437zC7PEbtdQrvd5dpdiFWhlYbOjoT2Y3X69meIUCRq5IlWS3hyTYZHNvBT4xOFl2lEFcyW\nQCKzg9o0aSZU6s9oUAJttUsgW6fu89KIeOmqMsnSNsl8Bilq0OnKqOU2WlFAzsmwA62uRldUcNGT\nxgkVkekbD/BuN2hFFLKnglwJHKdIlP3Z+0RrRYpqCDWgk64nuVM8zIWpVwm7CxRqMTbdSQpCFp/R\nomMpGEhU8eOhgY8aHVS+W/sYq/VRvuD6I2JWHlejy3Z9AL+rQkLbYUDYYksYoESIHRJU1AC6KFKW\nA+jIhCjhoYFKB0nQ2YkmUY0OE61F9m8vUOiGWfaN0PK6ERWDEd8yXrmOZBlIHRNDlWi5VATJpIGH\nHFFkurilBpKq0xI1CkKEdXmQWthLLexjeXoMHZl210Wt4eeebx9mALytKnfVGe4pswiYWFh4qXOb\nAxzQ7/1N5/rf6bz+KCN3x82D9Tifmo0hbLVobzcfUXVY7MrZ6uzSDbYZxsk3O/lcZz9E+EGg/CB6\nw76W06zipCWcWa8N2HZm6yw8ZQOp/b1Te+0Ef1t6Z3+mvUWunNUEnfTLXiWNLW+0760GaANu3MkY\nD17uY6Xi50mMx+50LBNiUMxxOvQOSWGbsuCnGZNxiTXGWcJLnRJBNhjEQx0T6WGN5y4dVN7lDDPc\n46B2k0CiDBGBpuliXt7H8+pf8rzvFe5IBzhw9z6J1wtIotkrApUCxiDRB0EssvEydXQMJLLeCJ2S\nyszqIvFoluagytUzB1GUDtHtIsNf36F5SKP2tAvRZ/Z2W74HbEC8USAsl1Emu1TOeMk/FcSv1vC8\n2iT+2xViAYifEDA+AwlvBq3dZsOd5BjXCNTqqPMd2Afdoyo5VxwdGZe7QWtapDMv4kq3mDHuURwL\nIqW6bLv7uZE/RmUrzGfHv0reH+Xfef8BR4TrvebDxDCRaOAhzw28Zyok8+u41gzkGOTUBH+69DP8\nzMDvcXD4HpfcJ1GEDtPMUcVPXM/TbXr4lvwpwmKBF/k2EzxghTHmzGle2P4eE40VVG8Htdgh1Krw\nSwu/xRtjZ7kZO0AfGe4Q4w/li+wLL3Cu9B7xfJ5X4tPcV2Zo4OFTfIu7ffspRQK9YlNsMsAW73KG\ne8yySYqjXOdM5TJPzV/izyY/x7XYUULuIreEQ5QI8pP8CWn6ucUhQGC6/uBxT90nOLYxDvhofuUI\nwr8yaf324vumGTt71ti1nttZrMEudWIf32SXe7aBTGCX2mixuwHp1OXYRh2RR2V1Tk4Zx/jOlzMj\nd7Gb5ToXC9uabl/PCbS2+sRpnLE5aXtcZ1EoyfFzmxKy1TPOBsKNTw3Q/s8P0/nVFXjHKXh8cuKx\nA7aMgSiYhKQSXuoYSDQ1jTo+SnqIfdcX0aQOtVkPhiJwV5jlq/oXSMppImKeF/k2GeKUhRBj8hKj\n8ioRs0CpE2Y/d0hKW2wIKUoDfq6eOcy2mkQSDRZrc5TbBYKhCvIZC/Jl5AWL3FSYsF7G7W6RmQlj\nBSGiFxmpbaIutvFuN1ESOtZdC/G+hXjeRGt0ezO4ArJXRx7WwQOu7Q6+d5psH03iGm8x+NlthHtt\n9IhGPhGhiwIFgYFLGZamRynGQmw824/RL2H1CURbJWCZlqqCBoZLRtAsNKHNrHqPuJpljmlueI6x\n1KcypK2hCxLzwj6ClBGwqBIgQp4YOTosEfXcZrCzgSQZzGuT3ArOEhwpEAiUcCt1RoQV2mhYCJzl\nHfxyjXn3OCvSKJskCVPkkHWLGDkWhEmUYBtXtYHrvS5GP9QGPGz6E7jdDVJsoiOj0EUQTFqSiqUI\nuIwWIaGEixYWIhotxCqIJYGL/a8z477HFgPMMU2ZIOMscbJzjYPiHfwDRUY9S3SEKb4vnKNAhKhZ\nINVNY8gymtShQJgVbfhxT90nOHSyWx7+8vc+xsduFZlmkQy72aezdogdNq+L4zj7fZs/tnleuyTp\n3poiTp22LYmzeXI7K26ym5U7lRj2+aZjTDujtzcQnZpxG3idxhqn29Fp9sFxb07A3lugCsf5ztKx\nKjAD3L05ymu/f5HsVsXx23qy4rEDtkIHLzVC9DjUFi6yYh9t04XZlgmtV4mpWawpi6asskGKvBFD\nlnTiZDjL2/wVL5IhwUFucbrxHgfqd/E0GnQDMlvBJKJgURoJMDcywWVOImJSvNmmfE8n6K4gnLRw\n3eqgZnX0KQVFr2F4ZFZnY5Tx48s3mbq/hPq9LkZTovlTGuqfdgm+VwcJ9JREe1JBzFvoKRn9gIQn\n3cK904YNgSujKdSJNvHhLNa/7tAIutnUklgIRAplRl/eYtE7Tu5kBO+zVcyihNww6DfyKLJOS1XZ\nIYGsC4Q6FVSryygrzHKPJNuE1RID/i2GpVXaqMxwv2fSQWLA2iIglIlQpMkGKZaIKkWsMNwNTHMj\nfIC+8CYSHUoE0WhjImIh0E+akhJkTpkmbSaoWL2Wan1WBh81+sQs7YhMuhBDykkEJgo0Bl2s+5Mo\nQocYOfJEiFBkhDU81KmqXnbEOG6xiZ8KKh3q+NDqXWZ3FnjB910MCb4lvciaOExYKHLEusHx5nWG\nhHWaKZkhaY0aXi5xmlrZT7hdputW0UWFtqRRIMpV4djjnrpPdORXPbzyLyaZGJjm4NQDhLVtzHbn\nfXC0gdKpvLA3B51Zt1O37QT6Ors2770NA2xgtDf23I4xnVSGk6d2ArDTgLO3G4y553xn1xpnrRP7\nfTurdhpnnFLDvQuXDey2dV8HTE1FG06ysTHDK5cmgfs8CR3SPygeO2B3UTnCTTZIUX7Im6bpZ7q9\nyHP1N7j11Cx3tH24PD0ZnAD8E+2f8bLwce6yHx2FGj4S7BChSHixQvBeAzFnUjoVIHcqhoBFjDxJ\ntllmjCJh6oKXrl8BD5iyQPGkn4rmQcTgiusIZUJI6OSIkcxmML8lwhWoxTzMRcZJPb1DSkzDDajG\nPZSf9aKdalNQopSNIAfW5wkKVYyURNqVJNQqESw3kFom7Y5GjhgjrBIr5RCuWUQuFLAw8VIn9v0S\n1e0gf/GFT7LqGqKGDz9VPrH6ChevvUliNo0RFBCAae4zlVmis+Jh7sA4O+EEHupskmLMWuaXrf+H\nP+ezLAnjZFgjjIeIu0BtRGNDTrLMGDV8LDKBhcA1jnGQWxznKtc5Sh0vBSvCZjfFppAiK8c5IVzm\nuHCNQ/8fe+8dZNl93Xd+bn45p865e3LGBAQCBAGSACmQIKmlRFGyZZlyrb1ebVCtLVe5al2q2pLt\nda0sLbWl1SqtKSoyiSQEkCAyBoPJOXWOr/v1y/G+d9P+0X0xb4aiqBU1NAjqVL3q7tc3vL7zm+89\n93u+33O4QgsvpwaOcuVT+/jJ3FeYWJ9hV+A6JSFCngQZNhhkkQe2axDn1QOsqxkUsYODSJIca/Tw\nQOQM/z2/RW9tjS+1P8afB3+SjH+dEXmeEFWUpoli2oiCgeYz6FXWeJpv8ttv/3e8UNpH/9PLFOQ4\nt51JdMfD2dVj93vpvsujBlzmxc8eZ+3IBPv/l/+d8MLqOzRCdxHOBWOXZoC7i3pwhyroltjBnUED\n92qn4Q7gtrjDS7tADHcPGeh+de8Hd7L47vaw7vtS1/buZ3aNMW523g1i7jbuueHuplGuoca9aVhA\nrifJ1/+3X+LK6Rj8xytskSXvzrj/I8I6G/SVa6wE+unIW3roMhFmZAfFa6F7ZWwZyoSpE0TAISRU\n2cV1QlTZIIWDSIA6BgpWREQfUsmlUqwkeyi1I+xevYke0JhJjZOlh4yew6fPEhkqgwHCFfD2tLmW\n2MlXlI+hKx6S4iYPcIY8CRpRL60TCnLLQC0bJF8povXpGMdF5FdtdI+HzUiceiRImQgdXcO3V6e/\nsIbfaZHW1vHJDdo+mVV/lFvBcVp48GY7BFothMMOmZVNPKd0Woc1VMUk6KkTVKpM2bfx6m28LR07\nIfH2kcNIAYNkOU8ml0PYbKHLXqoJicG1VWKVMjuiM7R0LzXFz6uR97HACEu1YebW8qQqcXrDa9zw\nTKHjIcUGEcrU8TPHKAoGCXOLYlDbDnk1ju0V6ZXWqBGkIfhZEEboYZ1J5zbxlTK2qLDZl0Bx2kht\nk1SpiBOQEBuQuVagcmud0esKgbEGOS1FhRDN7Sk4B7jIKr04HodWVGFTj1ISwxiqQlPwom/TM7RB\nKIKUdYgbZbxhHXvK4XjfSULRCutamqoQom1rmKaE4H93ya1++GEBDbKXW8Qkk8887CD5YOP63brk\n7u+72552G0bcLLgb0Ltt4PcWALuLdy7P7ao24O5eH92FyXtlfq5Cpbug2a38cM/tbqvf8zm6TTRu\ndGfoLjXTDXJuJu8Cfs8eiB10+OoFk7UrOlvPFu/euO+AHTcL0PDR8AZpylv9HwxUbisT3FImOcpp\nQlRp4aODShuNAnGGWCTQqXOrtgPRa6F52tTEIGu9acyMwKw8Rk0IEqw2eGTuNBd79nIxdWDLGNOZ\nI2guEZgyaOU0Wos+HAfWpH6e936YuFTgQd5i3JyhJEcx0xK1Zzx4xDbe13VGXlqm/XGRzgEJI6dQ\nSQTJkWKTFAYKqqfD6sE0Wr6NN7vKeHsGqWbSQmXJ308wOM6AvoyZU2nbXtSjdRIXSmjVNsu7ejB7\nJaTwlgV/wFxlqLkCVZHzI/u5eHgPmtBGXIGBxQ3kcyb5nQHmDg4yen6ZntoGliqjVA3e9B7nt2Of\nI0Eeo6WwUhykWVfohFXOcgQTmUGWsRFYsfvJOSnGmSFilonqFfoLOdYDSUSPyW7pGi3BywLD1AlQ\ntwPQEem5tU5GyBOMVohG89h1B/9iG29/GxqQvFTm1DJ0FoIwBILmYKCQpYcJpplgmhoBcnKC0/Ih\nhvyL6Cik2UDCwth+gioSJdqoElyrEa7V8aZbtMdFHt31EmlhjUscQMAmTgHN7qDFa2x8n7X34xCt\n59fRr5dI/HwGuajTul58p5Doao1dysDVP8PdMwzdrLZbReISAi74drsQ77Wkd8sCuyV03YYaqWvf\ne23s3aDr7u/y226u251pd8vz7m1Q0K166aZe6NrepWEkwD8cQxjrofF7azSXWrzb474D9orWx9eS\nJ5Bkgw4Keba0tCW2pqPUCJJmAw86IaroeFhmYIvrXs1w6bkHsI44DO6Zp9+3wlfEZ8mLCQJCnSOc\nZZ94Fc3XxlAVDBTS5Cj6I0xH9/L+fWvUjABnzQewNRFJM/m36q8yLU7Q09pgaHMdPX6NciBEkTj+\nfgPvrgrcAkV3MFoK84/3cSsyQY4UI8wTpYQHHRsBK+ywLsRJvlbEt6ZjSwJ1PQQ1iRMr53kt9RC3\nOxM8/fVvIRsWvpTOcGWVck+QDTVORQ2R7uQwVIlyJkyPsEqoU+SmsoNa0seqk6TnZoEqIaaVCWZ2\nj1MnSEGL0xdZpSKFSLLJ0zyHGHUojSRIJnvfadYUpkKUIl5arOgDXNL3c1Z8gKYWIKTU2Fu+RcIo\nsdt/m2XfAEvSIBukOcR5jutnGNjMol3rQAcmQkvYI9aWYPUk6I9qbIwnWf1EH28Kfs4d/zhrnl5y\nTpKqE0IQHV7kCa6yBxmDCBUMFHrI4qVFhnXGmSFAnRlhnFImzj7pKk+ZL5LfH6Ge8iKpJprQwUOb\nVfp4mDdIimdYVIfYFH5cpqZ/v3CY3xjkf/r9/8hnG1/kQ+LvcsHeohtEthyL99IgLji777s6Zrtr\nG5XvDheE6dq32w7end1289b3uhthC+TLXZ/DpSfcoifbP1e5M7SgG+y7zyl2be8WLw3u7t/tFlrd\n3iIBYCfw7ZOf4M8u/xTzG5e3z/bujvsO2C3JS0P1oiESo0TMKXHKPMYNYxdZo59j/tP0yFkcBGoE\n6aCSIoeCgeQzSY5s0B9dZKd0jR3c5KawgwZ+EuSRsMipSYx+DVGw+ED+VUSvhaianFRr1EM+7JrI\nQH2V1WCaoLfKbq7TwosoQd4XI2EUSRSKSLqFHDQwdwvImkOlP0Q2kmI+PsxteYIlBllmgEOc4wHj\nLMqqjaA7CBYElCbttEY2kMY332CwuETsbBn/o3X0PpXKwQAbShozKdPnX0WumnjtDngE1uReTEsl\n2cwTK1YI6zVK4zFUbxs5alA95EOPKMiCwUqwf8uSTZq4uomEgY4HjTZhpULSb1NXJ5i3h7jdmWJS\nvk1cLuCniSa1QYW6EGBJ7ueKtBsnKeJXW7RkDz6hyTgzeG2d3ZWbhM0qeV+M5GAR32wL+bkmrY9L\nOFEgCqFsg7rsZ2EsQTOqIsckMmQJOFVsQWSAFdboZZU+hlnARiRLD028LLeGyTb6mQxNE1RrdFDx\neBo0Yx6ujOxESJhIgQ4aFlfZzW2mGGCJPAmWGEQXPcjflVv9uIZDo+1wdcnkhZFjWOM2gevPodQ2\nvovK6DbYdJtpXPqhu/eGC+Jwx9qts3UjkLkb8LvB+t4Cn5tVd/c5cQG025zjZtSu3dzdrrvY6UoP\n3QJkNyXSnb27fyNd5+kGawmoB9N8a9dH+M7GMa4uuEfrVqi/O+O+AzY4xCjQxE+KDVLk+Avjk8w0\nJtB0myn1NnvkyxSI86b9MG1HY490BQcBJy1w4unXOM4p9nKFAHWC1OhljSilrY5y6gjmoMzB/GU+\nWngeOWrSEFUWUOgwRLRaY//8q5zz76HtU/DSIkSVihbmanKKg5vX6CnkaFdUWv0ylUk/4UiLDTnM\nLBmK7SgbZLgp76RIDM1qc6L+NqG5Jp5SB1m0YBBy/Ulm04PEv7jAVHEd4aLDyP55qgd95J6NcoYD\ntPDyEB0ycwXC5QaejE5OSlFpR4gWa0gLdZS6QV8mi+roBDp1CnvjiJj0V1ZZ9g9Qk4PUCBKjiI6H\nPAlW6dvi/qmy0UlzVd/DWq2PwfASgUCdGEWS2iYpLYeAjYnMTaYoD225TAUc4hQYZ4Yxe5bh4jKm\nonB9YIKdx2fJdDbx/L6O/rAHc1hCONBGvWmi3bKoDoaRqDPh3OaQcZGaFECXPOzmGq/wGN/hA/Sy\nRtPxMW+Psmo9yFptgGohyl7PZQbUJXpZI0UOw6/wqv9BhlikjxUCdp3zwmFmhHE+63yBb/FBXhbe\nD0DAqH+fdffjFFXgJC8PPsi1/Uf5x60FBhfrGJXGO/I2F+TuLUZ2DyXoBkBXHtitYW5xZ6q4jzvO\nSRdo73UYdofLT7ug260S6aZAuk0yMneeENz94M6NpVthcm8W360rb3HHvi4BhP2sjOziDx76JXLn\ns7Dw1t94dd9Ncd8BW6NNiCrDLLJJkheEDxHU6uyXL6IETZqqh2X6aeHnSvkgC84QFyIH2SNeYbdw\njY/zNRr4WKGfMWYxUGhtN4iMUCZOAQeBdkjhoncXg8oSK3If1/GzB4FEqIQ4ajHiXWDDSTAtTDDC\nPBXCXOAgw9YqqsfgTHo/OV8Sv9Tkkd43qP1OEfVUjYc/dZv2ER/rQxn2c4nDuYuE1lusTmQI5Jv0\nzW9AG3ydBv2sEKVCWLUgCmGlgolAiShVQnRQqRGkNhkCE3q1NSauztHMBvnGwQ+z6+A1jjbOkKwV\nkW7aSMsmaalIvFYj3Swx+7FxssNlDBSWGKRAnDwJrrIHCYs+XmN6ViW7OEynopE6VGBiYpowZUTn\nGIajsE+8vHXDIsIs40QpMcQiEtZWG1WxjZEQaIsa60KafCzF8LElHgme4tyOw2z4EwwNLnE7PsV1\nYSc3tClWeZPeZoaxxb9kLZHmRmqSkzzICv2EqeKnwVJ7kNO1o+iFIB1BQY7qKEqbMBX6WUHHwxKD\nvM0xTnGcvdYVPqf/HhPqDEGxxv72VZqKn7oS4C37BIsLo/d76f7oxeXrNI1l3vrln6RyKsLYb30F\nuJPRerlT6OvOuN2Wo26eabMFzO4kmm6Nczcl4Xa+czlzV2rXrShxqZUmd0DVLVLe28/ELTZ2m2m6\n+2+7oO8Oyu3mpl2wd1lol2Zxo3sU2OxnP8S1o0/Q+O0zcOPdT4N0x30H7CY+5swxpkovUFGjLARG\nKGykQHUIJTZZpZes3UPBitOWVBShw4aQYg8QpkKCTZoMUiHMBmlaeGnhZZEhelljhHliFHFUgaya\n5hYTNPFh2rNE8mU6aJxJHMRSoUiUZQZ4pPomMSoUQnHaXpUVLcNmJAGCQ6BWR561iF9tEZiu09+A\n3dYNDEtitL7A1PwMntsdfCM67YDK4mgfzYAfRenQU9kkmG/RscJcOLaP9O0s8esVJElg177bWH0S\nSavIiqePpuohyQbJQglzpk6fnMWYUFiJ9TFwfQOnLdBI+vCbOt58B2XJZKQ1TxuFOAVUOqSdDT5h\nf5mgWMMj6FjI7PRepxX1Me2ZIO1dJ8kmAepMcQuhAQ9On8LnbVFP+VkK91OWwxSJ4aOJiI0jClz3\n7UQWDELUUBQDO+0wHRzhdmCctq2xS79F0p8nopbRBQ8GCkUpylnvYVqKxjoZppmgSggZkxpBbFEk\nrhTo814jL8aZ1kaYscdImRtk5HUWGWKBYZr4WKOHULuOkrcIxBoofoNNMYFHaDHKHJskqXhi2y38\n/yHeiVIZfbbJ9PVeApkxen9uP+qLc4hrtXcIJBd43czU5aTdvtcureFmuvc6FV1OWO96T+duzXW3\nwsN9r7v5VDf42l1f3c9xb4Gym+pwz0PXsTpdx3NB2T1Wd9tUqy9I54kxltKjTN/w0p5Zg9K7U2/9\nveK+A3aZKOvmCX5i5QW8oQ51Ncji/CjeYJN4Iscq/eTsFLeMKQ75z5OUsiwJg0TtEqrToSDGqTph\nqk4QS5TeAexr7KZEFAmTIFV8tCgT4U/5NBnWCdsXSKxVWPH28q3E+/GggwOmqUBept9ZJKyVWAwO\nsiam8Tg6/c4Kg6UVoq/WSVa3qA5SMOadIWmuM5hfx7PUhhswsJRl4UQ/V57cQd5JMFxfZjS/hGcd\nCkaSFz74fp75X/+KHS9PE1eqTPyzBQTNgRrketLkY94tA4sAkUqFD7/yba4LU9w6MkkiX8HqFSgc\nCJNqFPFrOmLZZlKZJkiFHCk6jkbGznLYPMdtZZJZYYw3SPHTw69ycPgsf8TPkCCHuj184Lj5Nidy\nb3PgW9cIpJp0DstseKI8L3+QF50nyQjr2IjUCXBSOUGfs8qD5lv0mGtUxRDn4wdZI0O6nGfX4jT7\nItcYji6wEU7RokxVC/L7g5+lR9gaeHCeg1imTNLKE1YqhNQqj6qv8GjkVS52DrCg/yJn20ewLJmU\nN88VcQ91/GTIUiKK0xEQNkUsr0w+mOAtz1FEyyFo1TkinoUBOHW/F++PYJgbHdZ/bYH1f+Gn8m+e\nxJv7S7SyDk3jHdDrVoh0N+3v5qDvnQ/pArjGFjDWuSOAc6mGd6aNcwfU7+Wa751c3i3zc28U3fpt\n94ZB12fotqK3uVvR0n18uraxfQrmvl5K/+ZJsv/Zx/pvLfztL+q7KO47YKu0cRSd86P7uOrs5lpn\nFzsmrxLQash0OMgW7ylpFsutfgxBxe9v8O3iU1y2D3MwcZprjb1YpsRPhP+SohijToAHOINCBxEb\n77bCxEIiShELkXUxzeeHfxJLEglSZQc3GaivEV5voIZb1Fo+wicAuanHAAAgAElEQVQbRHdU0JIG\nsUaVv/R+hNcCj/HP9/4/REKVree4Diw1B5lLDBH3vIayv409BvImtNMaTdvHwfpV4k6eXDrMypCX\n0OQAimjQ/hmZ/IfCVMQwaU+B0NU6vACFZ2OsP5ZhN9fo7JXI9Ye5bU3SSagkpDxKxKTkizErjHLF\nu4/0/hxjA7MEUlUGLZ2oWMJf7yBjUPGHmBbGucUOSixiUyJAHT8NsmS4yEFiFJg6O8voxSW8sTYk\nwEKmQJw5Y4xbxhSPaK+hSAbzjJBhnZHaIqPrK2imjhn0EB7YuinKDRNhGsQGxFJlTjxxikUcTF3h\nxto+0pE8Y/HrzDDO3M0JNhb6+PCDLzASm31HHWLKMs96vspLuQ9xo32A31VSGHGB4/Ip/lnrD1jw\n9SH6LUrjAdpeZZsCGuLW+m4qjQj7hs+hqj9amdEPO+a+CZ11D4988lGGJqMEf+Nt4I4Ez50o41Ik\nbpbq9udwf+cCqWsH727g1OTuaTXdN4J76Q4/dzeAcouQ7nsttigYN9PvLli6AO1+7XZCuvZy90bj\n3hRM7jbPtD53mKU9e3nzVzRWz///vJjvorjvgF0iimUHebH6BMtSP3rYQyywCbbIUn2IjGeDXnmV\nj0pf57R4lDxJ/NS5Ie1FEizi5KmYYebzoySuF/AP11D7trLGDOsMOkv0GusEnAZe2uxQbtERFZbF\nNmpIR6NNPysYKNiCwJAyz7o/QVUKIHhFfJZOuFYnXisTEqus+np5a+IoQ5kl4u0Csm1S8wWoiQGW\nAz0shzLURD+JzRKGrNLfyBJ3CmiKTtO71aVOFk0cBOamhmlOeQhTwb4t4HTASgp4fFuTW6qEsRMS\nesLDKj34aBLulKn3elkKDHBJ2E9b1qgkgkiJDlUrRDRfZmp5Bn9cx4hKFMUAHtoEqOOltd3bo8U+\nLtPCQ5UgUUoENprEZsvQB03Ny2osw+vyI5zvHCbb7GdFHsQwFa7q+xjxL+AVW2SVDElxE0mxiFIi\nTBm/3ISAw6I8yFKgD0mwULCRhBYhpUqhlmDOGCcWL2Goy8g+m3Fxml5WcGyJZKVAgBZBpYlHtjjt\nHGVamiAsFBEFC1VsMyLMU1QivBx5H8v0UzXDLDZGWDUHaHc0lOsd/D0/WtzjDzsqC9AuSwQneqlm\nFHo+E2Lg9Uv4lnPvgGS3LtnNtF2gdsHy3i54buMlrWsbN+51Q3bL8LoBuJvW+OuKlu6t2NWDu7RH\ntxLF5da7R5h1c+3u8ZsDKebft59ceoKF2SSz34F25W97Fd99cd8Be94ZRdF7ePvSw6jpNpneZWQs\n1hsZLhYfIJvq4ePyl/jX/BrjvhlmGadKkGZ0ayrLM3yda/IeTuWP88Uv/iOe+ujXOdB7lhWhnz1c\n5VH7Vby6jdCBAG0eCJ+lIyrAMp/kz5ExaaPxDT7CeiDNSGCGJh4afj+FeIyx4jKJYgnq8JDvJJ5g\ng78Y+Bh7ucJBLmxrrh2ilLgdGmFOGGWZAXb5b3Csco6jxQusplJUvAH8VpNMscjI+jJXQrs5bR2l\nj1Welp6DloOeVtEfl0j6NjARWaMXABtxy8WJREP1kR1NcI0dnOYoKTa2midh8R3pCfYvXOPYly7B\nR8EJg99uMiXcJCyUmcOkzSAyFo/zEreZpEqIAZYJiVVsS8RakcjtinNhYA9/xGe41jiAWdV4LfAo\n9VaI1c0hnu3/KnpA5ZXAgxzmHEk2twu8RbSwiX1A4u3IYS769xKkhsEiac8mxwZf59yNE5xbPMrT\nh77G4OQpQpMVhpnDciQ2jQQ7V2cZt5fYFZ1mIjHN171P8bv8AnEK2MAr6oOMME+WXv5ffo4km+ht\nH6c2HiGVWCUolTn1pYeIHvoHBvv7hV6GU78G07+wn7HffIYP/fyvEVgroVjGO/ZuV0XiUgguteHq\nuLvnOra2X66ypLvPh3uMbielm7Xfa2aRu87TTc20t392reOuxK/D3WZxN8O3u7bpfgpwwVyUFEqH\ndnHqN3+ZuV9eoPB7az/Q9Xw3xP2X9ZVFjnlP8fDhN3E0ARMREZtJ702mkjepaCFWrT5+yfwNUMAR\nBWxEHuU1hpnnJjsQvA6Dk4sU/0mCw+p5nl55nsuZXfRLy9TsIM95HuVi8wjZSi8P+E6SULZGZr3O\nATZJkiNFlgxpcvwVT7FGL0knzwedb+HrNN8pR9cFPx50nuUrSGw1319ikB6yjJrzRKs1htRV5gMD\n1AjSrmkIyw7eUAtNdfC3m0imTdCoMeFM88fP/Syv2Y9z4SMHiA5XsDZVli8NMTI6g7+vyg12MsAy\nU9yij1UKxFlgiCEWyZPAQmKAZXrJotLeAs5oGSaAF0G+bON/v4G/X6cWDnKTDHH6UenwLZ5k33bP\nkAxZ9CMKp4YO8R3hA1TSIWr4qRNAdCxMW2bZHqDPv8KTynO0NQUdD2PM8setn8YQFB70nGSBYWxF\nohNTWFb6UOngo0mCPPu5tPUU06+wmBgi6i2SI8UNdhKmwsHSZQ7nL2MmBKoVP+qcxTnfIS5596Pj\noUicJn5C1DBR0GjzAGeYY5QNLUmyZw2P1gSvQ+LpLNFokex9X7zvjai9VGLmcxa18C/y/kcO8guv\n/DrLOGxyh35wqZDuMVzdZhr35Q68dTv7ueF2v+suBLa4k/m6v3Mz5m79tZuZu9Zz9xxwt2QP7jwV\ntLi7IOlm6h0gBkwJAr/z6L/klcgRNj43S/3ce+OJ7L4Dtp8Gqtwh3FMhQB3RtrnQOIzlSCTUHBYi\nWXqZYXzbdtzGMBUekt9kUFzeUjDITaKxIs2oF3+hRlCvoaGzSj9ZoZfz8gFetR5ltjmFx64xwixl\n6uRIscAQs0wwwBJpO4diWTQlP1WhjYFCVfXTCPgxbAVHgYy1TlLKkaWXeYbR0fB1WiTbBVq2HxGb\n8PYA3Y6i0PYrmJKE3DLw5A0ECzzSFldbI8iSM0iQIrfCO2jbXuQ89IlL+BDIkaSNhrhtufbaLQJO\ng3Uxw6rQSwM/fawRocw6Gfw0cGIwu2+EVHMDWTapCwFqQpAicTZJMsv4dtaroGzXzOcZIdebZrl3\ngAUGsBFRMDjCWcJqjZv+3ViSyICwzNPic2wISaqEGGWOGcbIbrddBRAlm1nvCGv00MS/1X+EJdpo\n2IjEg5sQtLHZuvE6CCwyzCiLhKjSthWEd+QHAqalUDcDSIqNIhok2aSOnwIx6ttDizu2itMWUCSD\nuC/P6MQMFT32vRfdP8Rd0ZlvUVwxKL5vnKBzlAM8S2biDEl5mYXbYFvfPW0G7gBpdxZ7r+7ZpSXc\njBju8MgufdFdBOxWhHQ7FrtNM92zFl0axej63lW3dNveBcCRITUJjjnA2ekHOOsc5cZqDF6ZBfO9\nYbS674CdimS5xlNIWOzlMjusW1zP7uemNYUYaZOI5vF5GkSkLUAodaJs1NPM+UcZ02YZZoEoRRTB\nQBRsVhI9XGAP14WdLDJMRQyTYR3BcWjZXs46RygSpsUKYcrECbDIMI/xCo9YbzLWnCPqK7GpxJkT\nRvHGWjiOSIUQU53bjBpZdFGjI6jYSEwwzXhjHm/T4MXkcSpqEA8tHASMlEA55aMkhAmutlBmqogO\nyF4Tn9DA96EK/c4Cj8sv8x0eR4l2+Oljf8II87TwUCTKdXZxhgdIscGj1mscM0/zRe2nmBdGtjoJ\nksVGZJYxfDQpJUJ8K/Yoj+99mYBQY9YzRkmIsk4GG5EFhhlmgU/xF4DDRfZzhqMsMoRKh0/wZfw0\nkLDYxTVeCj7Ofwn8LLYgcbBymY8XvsnnM58j70vgoUXUWyJHmnlG2M8lohS3ipWMMs0kXlo4FBC2\nB9LGKBJjK7uOUGaEeYrEWItl2PDF6LuRw6/rmD0y+7VLXDem+Er1WVLhTZLaJn2scol9XGcXz/MU\nPazha7S4ebOP6FCZSd9tTvAWXy9/4n4v3fdWGCa8fJIzzg7O8/v84VOf47h/meVfB7OrhUY3SHf3\ntf5eHsBuCqXJFrftHqe7V4k7LMDL3aqObvdity3eVZi4dEyTu/XW7mdyP68FiBoc+gS8VX+Qf/7r\nv4316l8BJ8F+9zsY/7Zx3wH7gH6ZPv4MEJgxx/lz4ycJpQoMzi2yeHqYcjhJe8SHb18V/UqAlu7F\nGFBY8W4NzO2gImMxxU12cZ1Vs5c/sj6DX2sQEOpEKNNGIxbbZL/vLJOem3hoMY2XElF2tm/zVOMl\ngsESHUlmxjeKINlIWCwySJoNgkIdDzpzyghZJ0OfsEoHFa3WYff1aTLiJmrY4BHPW0wHRpnThgDQ\nBS+1TpD4jQrBenPrWUwDf0dnaDHLp+N/zlXfLlbp4yAXSJGjV1iljcY6PVSIcIRz9LFKG5UFaQhL\nlNgnXKGHdUpEmWUMLy0ecM4wUMuiSW0afo3ntKepEiQhbLJBGgOVPbyNxE5qBHiTB9HoUCdAjhQD\nLDPBNCly9J/OkjxVIGKU2X/kKrVHv0ova/i8On8Wf5aXCk8SrRcYTC2xkxvs5AYjLHCao7zBQ9QJ\nMluaxLQUJmPT3GgHOFc7TMRf5nZjJ/qmH33BQ2Jgg/TEGiI2+ypXyWQLaMsGl6O7eaXvEVSvjk9o\n8lOhP6EqB1mhn9/kX5JhHUtXKRVThMJ1Qv4ymcllGj4vM/Y44+IM+8Ln+fL9XrzvtbAdHNYweZ7f\n+tYAXz3yT6l9fownv/A1hl86xQZ3hul2a6HvhTuDLVmfO5Wmzh35XYc7Rhy4u+c23G1g6R4Vdu+w\ng3tpGbfFazdoK2ypT4aBax84zjc+8wyvvTzD6rkwJi+AvfbXfPof7bjvgJ22cxzXz3C+cZiF8hiX\nWgd5evibpPybVJwo9WyQuhrCHhaQmzZeR0dVWtTEILOMUSbCWrkPw1QZjM6y6Axxgx0MssxxTjHM\nAm/YD+P1Nhn0LTLBNE18zDsm6Uaesc48U840dcdDU9SoiQGCVKnj5yp7tppRNTp0shqFQIKoVuQT\nrS+jhEw8jk68U0T2GhiaRIZ1Ck6ElW1FhzuQIWC0cWxh62paoNYNYrLBw/ZbhMNVXok+yk7hBv2s\nIGKzwDAbpEmRY4pb9LLGLKMILQGjrVEORZDkrQEOs4yRYpMdzk16nByarVPDy6w0So4UR3kbn6Hj\noUKFIh7WqTqTnLUeoEfMIlsW2VofQU+dgKdOur3JUGWFVL4Abeip59jBLRLkmVHHeU16BK2mE7NL\nNPDTyxpB6qTI8Twf5qq+j0oxStvykNTyJNhExsCxIUKJdbufNauXdkdDNVsktnvqKbaJx9ZpBjws\nRAc4Ez6EaNqEqbDDc5McSQrEWWKAhuWnakbwWS1004Pk8RFLbRJ0avQ4a6h0EL0/7u1V/65RASq8\neTOEGhwh/MwkvdoG3pgJBzdR54uIc7W7zDLdV9qlJ0zugIfrYuymO7ozZ7cgSNd78N0GmO65jfe2\nZDW4I+FzXZbSWBBrKM7yxQTXteOcCxymctNP50YRuP53vkLv5rjvgK0rHiKlJl+4/fOcnjtKqFLl\noWdP0hrXyPammT65i3InRm1ZYffkRSKhAk3RhyIYLDHARQ6wPDuKUrWQTlhYHgmP0yYnpEiRY79z\niT+xfoqUmGOfdJkR5igR46ZV58Nrp7E1gZMDD9AnLBOhTJA6furUCHKTnWyQZnM9zcZXBzCnZB5M\nneTnVv6ExJ4S1qRA87hMXQjTFH2Igk0Lddtqv4CPJpYqsXigj0SuxOT8PJSAItALvTObOIGb6Ec1\nIlJpe/qKn3lGKRPmaZ7DQKFElDQ5dq3fRlm3+ff7/hWl4NborClubXHSosJcaAAfLfzU3+kaOMo8\nBxrX0R0P55w+4jTwW3VOtY4R1sokWiWWboxT7o+hZdp8bPN5EiNFGAIMcOICDfzcZAc32MmSNMj/\n3PufmOI2JSJk6aFMhDoBWnixijLFU2ni+9eJ92XxiDppNcdk6DUOChe4GtrDmYDO+lCGMWmaw5yl\nQBxPqEHdr7Iy3ktV8hN2qnyn9TgeUedh/xv0ssYYszgIfLnzSRaEIaZ6r7LYGSSr9zDiW+Ajwjc4\nIZyiiY9v8NH7vXTf42HTuVCg8Aun+WL7OGeOHOcz/+d3GPi/3kD7jRuUt7dyJ8ts7XF3RzxXjeEO\nMLgXwL1sURtu1t3dXc/loV1u2mWYXS7bleh1m29cJYoK9AD1nxhi+hcf5k9/4X1Mvwid189gt94b\nXPX3iu8L2IIg/ArwWbau2RXg59l6EvlTtv7bLwD/jeM45b9u/9PyEWbkp5jJjSOHO6QOrdAbXSEl\n5tD8bf5yz7Ncmj3E5psZBp9cIhwrcoOdTHELPw1Oc5SegVX0lodz+mFsUUBT2ygYRDerhEot2loA\nIgXksMk5jtBBpSNe5pXUw+iSRlZIUySKgkGVED2sMWuMc6lxgKQvRyhWZvWhftRkg4C3giRb9Orr\nRK+UCdcb2EmBYLSFUAAlYuJLN6kSYoM0bVQ0uYN4tcn650FfAlMG+ZMgYtOSvcwKo4wwz1Bzif7s\nBqvxAa5HdnCFvfSwRpwiNiJqu0O0UeVp6zlOcZR5RqgSYp4R4hQQBZseskwwzSS3aeBnhX5C3q1G\nSLYgIGOxp3SdD5x9nUFriVbQS2fAQzq2xpg8yyuxh5CcEwSEBnvsq8yrAywwRIocPr3FYmuEC4FD\nyIpJwtlkR22GW8Ikfxb8JBYSR8JneHT/67STMl6xyRCLNIR5dgkaWXpQBINhY4HVpUGuXT1AKx/k\n0DNvU0zH+Lr4E+SE1HbB8wxDngV0NCRsQlQQcagRxBAVkmKeD0nPEzFq+NstwlaVfs8CSXIIBRH/\nW1/hN3/Axf+Dru0f+TBt7JqNzgaL8yJf/tUYwaufIjJgM/VPpzl85RIj37zFuTZU7buB020g1Z2F\nu4VGN9vu1nu7jklXTuhm4t3HgLsLlnTtExZgjwIrH53kyr69fPt3pyi8LFHOGSzOF9A7FnS6jenv\nzfgbAVsQhGHgc8BOx3HagiD8KfBTwG7g247j/AdBEP4V8K+3X98VM+IYRc+TmAGR/tQiU/uvE7ML\njNlzxJ0SV3v3sFAfpnotjGOD5FhEhRIjzKNYBh3DQyKWAxzmGyMMGsskhTzrcgrHEGjrHsJSDaOp\nMcMkC/4hBNkmL6zwgu8JmpYfs6GwVBtGUBzK8RCDLLHppMiaPfQ4a/SGVvHubxFVSuxyrpLzJBjK\nLdG7kYN17jzTFcDj6Ch+gxVvP3kpAUAPWaSCQeci2BI4FSC/tZ8jClhIVAnRsAIMtbKMV+fQRQ+z\ngRH6nDXiTpEFaYgVbx/tkIcReY41MiwxyAr9VAm900Y12Koj1RwS4TySZrHAMMtaLyI2JlVCVBlt\nLPChmVfwVHVyqQTmuIiitelICt8OPEGDAAnyCNs3MBCIUmbQXmK4s8jV+j4kj8UHPN8mY2ywJvQy\nxygTTDPkXyQztk6eBDoegHeMOzOME6bChH2b2dYO1gs9LGaH2du5QEPw08BHx9ZIOZvscy5jyPJ2\nwTSNBx0dLzWCDMmLaE57azivcJEB1jAtGavtYFoybd3H/vUrP9DC//tY2++dKFLNwpkveoBJouNx\n9KEI0ayF4hWZ6YvhieQJVGeIb9p0Sg517mTH3TprN7qLgS637Wqk7a73uwua3RSKCniiAv5dEu1s\nkgVxlNhGkbnEDi4OHeEN7SClSwW4dBt+jLrKfL8Mu8rWv4tPEASLLffoGvArwKPb2/wh8ArfY1Gb\nyCT9OYKP1RmTZjnABbxiC6ntkNRL2D4Ze9Qh0rvBRXkfQ9Yij8ivkyDPSmeQa5sHeCB6kt2Bq+wI\n3uSD9ZeJV4v858h/y2o6QyBRYZ94lrOrx/jCys8ztuMGQtBiwZngWu0xmo0gNBXEKxa+aI3IBzYp\nEsNQFAKxGprQZkKY4R97/5ABZxnLkXg9cpyOonBYu4jgdkIHiINmmASW23SGPDg+gShFRpijt3+D\n0EfAI4D8IWAOCEA8VOAh502mmeCWfxJnCobnVsgUczg7YdRcJGFU+GZwN/WBAN7eFqJiI+BwmHNc\nYh+9rPEgb+GlxfjGPAcuXuNbxx4j35MgySYGCk18dOgwzAJ7pGvIXgNKEC+VeGr+RV6Xj3MyfZwF\nhhFxkLC4xm4GWOYIZ6kR5JD3HI9Ir/Gr87/Kee0oD428Qccn4qfKbq4R234SuM0kOh5aeJlhnDo5\n0gzio8kAS8S8JYydCvOjI5SsCNlAmkEWeJ/zGqlOnqBVR7QdznoP0ZD99JIlQP2dLoyfkv4CA4UV\n+hn2LRDxFKhKISKFOoau8nbmEOMfW4B/cfvvvPD/Ptb2ezPmqSwu8vIvG7zV3ofiex/tT72fT3/g\neSbP/TsOfrPDyusGV/juiTHdrVHhjr7bnXbj0hmuUsRVfrjZtttQysNWIbF/r0T4t/z8wR89xufF\nX0H7nZcx/rhM+8tt9PJ57mbXfzzibwRsx3GKgiD8J2CJLarqBcdxvi0IQtpxHHdC0waQ/l7HUDAw\nRYmW14NKmwzr2/pgB802OMAlUtI6Pdo6XxOfwRAVwlQoEiOvxIhFcni0JpJgEhKqmB6BjiIxJdzC\nEkWuC7u41NpHy6fS37+Iqck0CKILGn3eFbyyjuiFW4O7KedjtL+moR/2QdqmbWiYqkxHVikKMWIU\naQh+TgsPUPFFKCYjDCuLeNUWmtwmWqqhbJr4ijoH167QSShoqTZSrI05KsOzILwBpMBKgpiFYKvB\nZH2BnC9DUYngEVv4PU28hRLve/ktro3s4ptDT3NF3EVK2CAjZ0mxuZXBWh4+Xf0SJTnKW74T1DYj\nHDIvENtZYiE4xCyjmMiotBFwqNJknl6kiEXrhI/1eoaOqLCj5ybVQAAJm4c4SRuNFl6KxIhQ3pJF\n4qALHnTFQycpMi8N8ad8mmPqadqoNPDTw9q2rnrLTRmlxBQ3eQmVk+WHqV8IcXtwB71jK/jVBnrL\nx1JzjI5PY51FCiQIyA0QoYWPeXGETeIEqLOTGzTxc43dHOcUE9UZxhaX6A+vY0cV1v1pSv44imbQ\no60hJX6wXiJ/H2v7vRkGtgGtPLSQwbLgtWneXIJb6zu4sdhHNZohP7SDnsdW2Dl0nWO8RehsE/ui\nQeEWrJhbpU0Pdxtb3MKiDESBMQV8u8HZL1M74ON1jnNjcTebrwwQWbxJcCGL9hsit65CRZiGuglN\nEWquL/LHL74fJTIG/A9s3fAqwJ8LgvDZ7m0cx3EEQfie2pnV/+PLOF86g4OIvjOAsavOTTqETBXB\n8DCrXsbnNPCaN0FpUZTSXOYGVcIUELH5Y+bNOmXKxKUCm0JhW+XxIhukWLH7mdcv4JcbJNQ8BeK0\n8GKfvIQmzKE0O7TKXmz9MsZaDOOWQOvhFtpQE4+t01IXmJZzLKOTQsTA4jy3maPCdVtiwrLxYyHa\nItSjeIs63nIT01qBIDhJgbVwCkEJEe3YXL3aAGzsBIjz0EagNCez4lnFVNYps8rVQgNPrkNnY5bn\nhiY4NaASls5hCvN4zDk65RybWpJ1X4Zg7RZZuYfLXoeNQg8Lks5SPMXquTwlLJp4EHEQsSm/uc4L\nmJzDJo3KCj5aeBmfjlKgTpUr9LGKuU3RbJJklSLzFLGo0EGlQYAq36BElJdps0IblTrrvIXDEiIO\nG+TRaAN5wsyTfzPEZukqpUtJgoNl4iObJKwCm7UOG+11WrESqEsUsUihogItPFxFp9jREZoSw1oA\nU5GZlkuUqDBaK6GtmIT9NfSwxtWgRv5mlfy1Aj6ziS2J32vJ/a3iB1/bp7ijREhuv35YsfzDO1UT\nOPkG104CiLyKBmEPgimRbGgsVn3kiRBoaTiGQcmBLBI1JDxo2EjYiNvyPBsbC4k2MSzSjoXfAKcl\n06h6OYef2w2VnCHj2BoseeD/toAZ4I9+eH/zXfHDutab26+/Ob4fJXIEOOk4TgFAEIQvAyeAdUEQ\nMo7jrAuC0APkvtcBHv8fdzPymaMsMcQGaWaReJD/QtCpMeeMYQoDjBhX+JnGbc76H6Cj7mCMrSb1\nBQbwizrFfArDqLM39Vc8Jr3CDoq00HmVERznOH0OyFg44jgyfagYtFjm2GcGWXhjnFe++CTNqA+E\nLWGQtdum7303+Ejyq0yKdRRB4Ta7iWzXxgWGybDO3nae92/UCUk1cr4kX/B+mrS9yAnzra0+IBKI\nis2y/EFMQSHSucGeC9/hZ3pKOKNbWcX5xA5++xP/hEn1FnuFK+zBJHrVxiz6mJkc4jXho6ji+/h4\n9Avsli2GNgR2/H4da6jB0jMdXrSeYUyweUyc54yRZF44ypzyBEMsspMSIhYzTLBJgiohRj6TYIpb\nJIkQYII1ejE5hgcPKiIRNhhkiQB13mYfQWpMbXPaBgobpAiToY2HJDlGkbFQmSHFAJ1tF2WFEFU0\n2lj0MYeHxMf2c3buBGPJqwzG5jlbOI6idpgMFqgrfiLCNIPEGWYejQ5lIlzgkyxN76P5epj5nTr+\n4SqhngL9qCSsUW7qOzlR+RpBp86FzM/ytPQGj5deIXO+xeZglIGv/UBjeH/AtX0cts1C/3Xiv9a5\nd0NDxZl3KJciXNP2ssQwUs2ChoNpQ5sQFhlEduKQZKuOC9DAYROBGyiso1pVpAVwNgWssyI1QjR1\nH07FhnYPEOcOw/3jdq3/3V/77vcD7JvAvxUEwVXoPAGcZqsV7j8C/v32169+rwPcru6g7uwjZyQJ\nixV2c5Ox9QU0tY2e8uChRVLKUfX6eUh6gyQbdFApL8bRrSDDI4uMeRcIqjU8QptT9nFuOZO8X3qF\nJJv0COusCT3kSNJBI7U93zxHlj00SPUVEJ6Am/4dZOt91CbCHBo/zft5iWfmv0FMK1L0R1iL9FIR\nQ1hIxCmwu36DPa3r4LcoyiFyagxUG1k0MJC5zk6SpQIHVy7xiHmKVkQjkKlS6TdZPxRnNdrHqLZE\nyrPJ49bLqHYbTdIxkWmnZAg5hGNlHrVeJmltkBY3mGOUBTW/2L8AACAASURBVO8Iw3vXaPWqzAmj\n5OQk/awwxixBtcYqfazSB0CBODOMsVIexnRkZMckQR7LUPha9ZP4fHUC3q3WZCvZQfL1FGODt5E1\nkxBVZpxxGrUgtxq7OR47SVQr4CAywDIdVERsYhTw0yBEDY0tO79bcDSRaeIjxgp7tDfoDGjoLR/L\nuSGGvP8fe28eJOl93vd9fu/V933O9NzXzszuzu7sgQUWAInTEAiRjEhJtClasiQ7SUWJ5VQqZaXs\nVFIppSpWnDgp20psJZFIStRJUSApgsRJLoAF9r7nvo+e6enp++73yh892lJkyYptDQAK86nqmuq3\np96n++1vPe/bv/d5vs8qhkeiram4qaOiUzF8fG/7JZyOJrHkbmd0mT/D7GgMLdHA8tg06VSbyLKJ\n8Ji83HoJl9HkOA9o4OJ95wVO9M2xHeqC/7C56f/B2v54YoPRAqNFu/Ynw3R9f+Z/nAd/c3SWLv7k\nJlCbTpsNgBtsuXO0a/yp02L94HHEn8dftoZ9RwjxFeA6naWom8C/BnzA7wkhfp6D0qe/aB8rjSHS\n5lmcRpMReYnHxbv0ltJILgMzDhFyOOUGu3KEYZawgXfsJ5AKEG9nmeyfYcCzipMWabpZ0I+xZg3S\nJ21iCZko+wfldZ3JJz1s08smhpXHVXGQSmzh+lyNFjL1uhMrLzManmO6eYPT+3dpuzV0oZIIZkjT\n1bE8xaarscdwY41sV4BVtZ91BnDRwEmTKl6WGcZRN+hPbzNQ3KaeclBKuFlKtSieC7Mm9RBXsiT1\nDC8a32NRHaIgB9gliR3bI2B3Jpo/a77BFPdYYYAFRtnxdPPCE2+yp0Z5336UTKOLoFyi4XARJvdw\npmWeMDU87NBNteHHbdU7vi24yBgJXq2+yAn1NhPKfURJsL3Sz0p5GCIWiqrjF2UWjVG28gOoezaS\nx2DC8YAo+zjpnFiKBLGQCFEgSQbDUMkSY0vpoUSANhpNHAi26La36Ta3ma2doGZ4eSn6MjvOBLNM\n4KOCgkHRDHE/P4XiMRhKzuOlSsS/jzzaxhfI43I2aKGxRergZJHnDcczWJLCf2b8KguMcsd1muao\n86C65Qf/3sL/q9D2EX8RfzKy9y//iX/Evxt/aR22bdu/AvzKn9mcp3NF8peS9O9Qaxk8rb3FKeUO\nLho8GBpDSDYGMhv0oaBTxct9TnDXOsUtY5rJ0RnOiFs8olx52F6to/LjxjfwGHX+tfqzaKJNHxuc\n5B4TzKCjEmMfP2WEAV++/XOYXonJ6btU8OJ1lgnHczxQJnBrFU6cuM+cNE5F8TIkVuhnnUVG+S2+\nyElljgvqNXShcptp3uZJetlEwiJPmAwJ+sMb6KOg3AFnvY1aNnE1TLqbezhdDcLvlagZbla/kGJX\nSbBLgjwRnjTeJmQVqGoefJt1gvlVIlP7mG6ZGWmSRe8AS2KYB+3jzC+fZNkzxu5Q4iA52nip8SKv\n8CKvEKJALhpBtzVWxS43+HGW1WHsoM66o4fMfozq90JU2kFaEY2Z4iSmQ9DlTFOqBdALGlYW7gyd\nQqGNlyrLB4ZPFXz4KeOlxjhz+MpNInYJMyzxmnieO5w6aKips5l/lvtvnCYxusuZk9c4od3FYoqF\nA7+RAiFyWoTHj/2AohTkHifQLZVSOUx71cv+QAJ3pIJTa7LEKBmSxNlDdlnUhJv/cf+/R/G3CPn2\nsZA4zv1/D7n/1Wr7iCM+aA6901HV2nQraVLyNg7RYo84aVdX58agLbNUOIYmtRkNzlIgjCraTEl3\nGfEu4hNl5jn2cDr4HOO0FScRKY8QNkGKDzv+WjjQ0UjT3dm3tEVPYhPDIeGlyuNcRkgWimZynbPU\nJA+r3n426KGBC40Wx2pLDJibWF6ZDVeKG+ppFqUhssTobW9yYe8Gthu2wl0YKNga6CEZY1TinjXF\nG83nWJMu01IGyBHksZFruKwGM8oxFsQoOirjzFGT3KQbKWKbeSTDohFzkpPDeKmSbGd4bfsFsp4Y\nZkSmN7RO0rGDjwp1XIQoMMEcW/Qc2LEOYKvgpo6LBl4KeJs1rG2VghWDHYnGTQ+2LEHEprYdoPqo\nn/p4Gf19F36pTLCnQHErwk6zh+GeZYoEcVNnnDkGWcFDjTJ+bIdCyfazTxQvVQLlMrMrJ3GVPLhc\ndSaH7tObWGfMOYefMie5S4gCecJkiVETbsLuHCYSkmWRL8Rot53EEhkG3EsEpCIWgixx8u0ouWqS\nsDtLVM2iePbYzPSyuj1Co9eN7Py3zeg+4oi/nhx6wjZlmaRjBxuJjJGkaIZYU/upS25sS7BYmcQp\nNzCCEpreJso+g+otXDQpEWCGSUxbpoKPRTHKA+U4QbvIeXGNYZaJkKN2YPNZIsA+0c5Vn/KAC2M3\n0FFo4+A4D/BSpYT/YMqhxj5RDBRMZPaIM9JcJ6SX6fNsUnZ6uc5pFhml29rhkeZ1Ht+6ylx0jPnw\nCA6aIMG+M0JpOMDrjaf4P8r/CUHZZFl7ilUGKZwLM8QKe1KcW0zjp8KP8Q0Kcog1Y5C+jQy1AQc7\nQ1G2SeFsNYkXstzYuEAzqTKamGW8Z46onsNVb2A4ZPrkDabsO3y18tPcFtM0fE481Ijbe7QMF0PW\nHvWqj7uz52kY7s7a4CadZcSSgLJMK+Sm3uXBMafTO7LByPA8l69+gpIVYq+n04nYwxYXuEI/axiW\nwn3zJH5XmbLkY5YJghTpq23y5oIPV7EzYHfswjxRsU+IAmX89LPOae7wDk/gNapgQFTkaMsOwiJP\ntRJCKFWSQ5uc4waBg+RuIlMyQuyVuwipOXqdGxwPPuAHK89xde8Cm9FeQo78YUv3iCM+chx6wm6j\n0cDFNc5TKETJZeOE+vfo9WzQJ20QTJSQhE3EznJ193FmUMn1hBkQa4TJc4o7XLI+wabdy4Q8y3Jr\nmJwRIeuOkZAydLFDim32iaJg4KZODQ+7dHWuyA/iq+jU8PA+j/If8Q1GWaSF8+GabZJd1v0D7Nsx\nfkz6Q+q4MZF5hjcZbG3SV9/Gp9Yoqz6yREmRpiUcfFN8hjcbz+CgxT+I/q/cVmaJEqFEgFeaLzLJ\nDF9y/yYb9GGgPFwDbzldmD0yWX+ULDEGWSGyUqa0EeLcxPtsRHuQ6DTQ3Muc4sHaKcaP36Ma8rFs\njvD2959BVxSmPnWTbVI8aJ0gW87SbIxhNwTWlgQBOjfoo3TaQuJAEDKBbtpZB8dfustLnu/wWPsK\n6pTBrHOcu0zxeb6Ogxbf4wU+yx+RaXXzT/L/iNOh6wTdHevUJLuUQ37Ux+pk5pN8//5zpE6u0+Pc\nJECJHBGmucUEMywzxERhkU/tvIqq6VwOX2Aj1stU8h6aaGGgECGHjkIDFwKboDNPIFlkVJ2nix1M\nZM6OXaFvcJVF7zDd8g//9JAjjvh35dATdqBd5mneYp8Y14zH2KmncJg1mjioml7yS1GcaoPkWJoK\nHpq4aKN13Nv0KNV6gKU74+SWIqgVC+eFFs7TGfKiY3DfxMltTuGmToQcS4x0KhgshbnCceqyC9Xf\nREVHwkLBoErHyjNLHD9l3NTJEWFXTVLGj4sG21YKA4VPSj/ASwWXWmct0cOSd5g94vSwTQMXc2Kc\niuwjLu0xps2TkzYZZIY03WTlGAYKG/Q99EYp40dHQ7V0aIJtSsi2RcTMI7uhlVDpjaxjuy3quEnT\nxbYzRSnspagGaKJRFn4qCQ9OuUkdN7l6jJ1SL+VqlPn5SbQdHXNf6dw+89D52wXusRpDPYvk7zbI\nX4e9L/i4I09j7DmJDmcJuWPM6hPcMM7SL2+QUDO8W/0E8+0JtpwpfHKBJC5kTEoEKGs+nIk6ZVmh\nVvcROnD4S9vd7OkxQnKebjmNhYymtfD6y2hKC4fWBAEx5x4BirRxUMbP7kE7fh03XqlCwrmHDazY\ng5iWgt9TRhU6nofzuo844uPFoSfsUKPE81xnlyQFYlwVFzGRO0nTkHhwa4qAu0RidAfJa+AQNTRa\n7FkJdlsplkrHaLzpRf+2yv5WknP/3fv0XlhhSYxQpOND8R3rJSaNGc5aN1jRhvBKVXx2ha1CjIIW\nIOjPskY/PWwzzS226GGWCcr4SZBBxiRDgiS7aLS5xRnmzTEky6JX26RP2cDlqXEjNMUDaZw8ERy0\nsJBo4uSseoNusUMLB16qjJqL5PQoBTVIXXZzm9N8hm/SzzoLjNLCgd+o0qg4kQMmPquCu9Vgp6uL\ntf4e4mSwEGzRwxJTtKMaQ5EF2rpKvhEmZ0eInMuhSDorxhA7e72U90JQktia6e8sg5gC1d1GCRpI\ncYv2gAPfeJnHBt5h9tUyO3+YYPGR51kNn+KtfI6f6PkaUdc+pbaf77Z+hOeV1/gF6Vf5lfI/4oY4\nQ6x7GxkdGYMudqjhoS05cGgtZMXCqTQZMNZZNftZF/3UdTdFO0RV9uKgRS3gYj4wRIwseTtAyQpS\nFj6covnwBLBDF5v04aNCiAJR9pmvH2PL7MHSJPxKmbCcJ2bt035YKnbEER8fDj1hr2SH+DXOIGGx\n0B7FrgqaphONNr3KNovHTrInx7ncvkjEnUNIcNueplIM4TOrPBf9Lnf6z7L8+BgMCFbPD1Jse5E1\nk1kxzqI5wmptsOMOtz/N0Ol5Hgu+S1G6wk8mf4U56RhLDDFIZ4lFo43Axk2dAdYO7JL8CGwGWaWP\nDVJsU9Z9rOkDlBU/20qKuuxmQYyxTxQVnT426LfWeF5/HW+pyYI6yqXQRQw2CebK/OTCN/jdY59H\njylc5DJu6lTx4qfC+zxK2puidDxAr3OdbmsHrW6z40qxpI1wnmvImMxzDCdNJpnhtHGbr838DKt7\nY1iGxMSZOSyfxLXsRZo/cMGGgHWQntIRJyzMisZw9wIDgWXcY3UeVE9RNgK47AbasRGcL5xmYmSN\n4eQlevVNHP4mDdlJwFniCe0dXmy/yonSAn/b/xtMaHdZZJiz3OQYnSWKVQa5Zp9n1p7AlCT27Rjf\n2vgcSlcTd7hGr3MTWRgs0jmx7h/cIH2St1lsjXKzNs2+L4xXqyKAaW499DIfZhnDVnjPfozM91Ok\nCml+/jP/ijvaFBXTz99t/Abftl48bOkeccRHjkNP2GWnj+vmOeyKQracxG5JVPcC7JHE4W0h+gwi\nIkuftMGoskhLOLhpnyGsrNErb3LWdYXRgVU2HAPMnx5FSrRRpebDmYVCQEAuYbo0Wj4NTW53fAuE\nStKdRqVFnEzHuxqZiu1j/eYgmq1z4cxlhGSjYNBNmkFWSbILQI+0xZ4SZ1ZM0McGfWwwZi5Qk7yk\nRRdJY5eRwhrOXIu2z0HalUTYNs5WG113ctc7wq6aoH7g2dHTSBMxCwQdJUo7YeZak0wMzNJSVbJm\nHF1zUZL9yJjkCdPCgZtObXWMLD1sYaJQLQWQt032+hO4nTW6HNv4k2VMVWY9v4/eqmNXIDKyTSS4\nh2walNMB3GqVUCBHRM4yOOmh7t8jntzFFywh08ZLhRRpavIsA/I6uq3ynnEB3Smj0SZb7MLh1nFo\nnXr4LDEsITFgr1Eq1qkuy5TP+3hcv8NE9QEb7hR1ycO8Pk5xN0yj7UZT25hxmXV9kHwjjsvdRMYi\nSaeJJtneY6S6xmx2nC2pH3tQIAVMFEnHpdRp5j3k6nHaAY24/Bc21x5xxF9bDj1hS90mFcNPOjNA\ns+RG2BZG2sGunWLfE8YTrzEpPeBZ3iBGlhwRqsLLhH+WAdYIUOT4wCu0Ek5+a/QnEGqnVXWJYbxU\n8UpVop595GETDzUMFOY5RpYteomRIMOjvM8WPWyTImdFuP7GBXxWlcem3sGnVgiJAkOsEGUfxTbw\nmHWGtRX2pSh3meIx433G9XnG7Xk8ao2r8iP42nXkHTCXNPYfD2H6YNhaplnfoyif5n8+/Yt4qeKi\nwQ/4JOOVFXrau7SCEvIctEpeHF1tltVh8nKYQiD4sEzxNqcxkOlihyJBDGSqkhc7CXLWgAWYq4zT\nZ69yoesyfV0b6Ki8Sp5csYyxqnJq+gZNl4PNrT7mL51k7OwMZyauEmMP73iF4HiOfaKU7CBl289F\nLjNsL+OwWyALrmrnWNMG6DG3yVS7uJ69yInkfXRN5hbTNHHipMlJ6R4bmQamXif64g4vSX/MU/lL\n/DPtF1i3+smUkuRmkzSLHiS3iXFBxnCo+I0aLrtJt5XmvHmNsJJnpLnMk5kr/J2bv85tx1mm+68g\nP2Zi2IL3pMe4szhNrhDju+eeY8izfNjSPeKIjxyHnrBTYotx6Tplb4CmpBCwivyi/39D+GzeUS7i\nFg0S7NJGw0LCQqKNxhoD5AnjoMmlxFMUzDBL8hDT3OIUd5jmFsDBTcImQYokyLBJLwKbAgZpuknT\njYPWwxuLi9Io/s8VqDc9/MvC32cqcJs+5zpFAniok6qmubByk3CiSF9ynXd5nMGNdew9lYWJITzO\nGufFNV52fhr3YIP++DqVkAeBTZw9dkwdoduo6IywhITFDJPcDpygbLnZUlOEp7O8oH+bptPBECuc\n4QYByrzPo9zhFCe5xzDLOGlwlUe4wgU2pT7kUJvh07NI/TbJWBq3t/OZVvVBghQZ4ivIJ/coNwKM\na3OU8GN4HMgTJvW4mz3iLDNMgRB5woyxyDP1S8Qref4f82eZbUzSbDrw9BdRfW1sS7CxMQwWnOq+\nxh3pJOt6DwPqGjU81PCwwCiuk5eZeOYuW64Ur8lPs+Qa5IrxCOk7PUgLEhfOX2ZP7WJteYgz7Zuc\n814n4dvnO8oLzOYm+drKcc6MXkX2Wwz1LKP5qnilIiXFT34nTrkeoBgLkHcl0GUHb0rPsGwPAb92\n2PI94oiPFIeesJ2igSlLjPnm8LlLtCUNPCYepcYAazRxoqJjI5gpnKSFxmhokSLBhzW5K4xQJEiY\nHAIbgY2DFvHCPmp9HWeshawZqOgsM0yOCDv2DgHiWEi0bAdmVcUWAo+3ysjIAo22m2wlgSUkTCR8\nVJivTrJWHqFf3iYu7XLOuo4uqfSKLeqyh8vy4zikBj3tLXxrNUy3xF5PlAwJXDRQhU5eC7Gu9JEt\nJwm73iam7lHHxb4jhMkwMiYDsRW8dhXZsAhYJQIU8bbq3FDOkVVjVPCxSwIBqLQReMiJCFHHHr2x\nNXyxjh2phcQ8x5Ax8VMG6iT70/iNEgklQxMHLled0yM3qEhelnfHKJtBWj4N0y/wU8Fn1sk3Y9wx\npmkYLoblBZbywzQ2XDg3m+QbcbxdZWLDafJ65wQaZR8V/cDdL0rbo9FOaliKYFYeZ4sUuqkiayam\nX0ZNtpHR0fbbjCtzHFfv43C38cllHFKThuZhqTmGy9mgy5fG7auQJE2JACE5T1Ap0pQUkKFhu1iu\njFFcjhy2dI844iPHB1CH7eCBdJwX/a+QJc4VLvB7fIEhVjjBfZYYQcJEtXVe3X6RgF3iH/p/mZvS\nNItilDI+cvk47ZaDY32X8Ug10nSzxgDPbl3i1PZ1vI9V2NRSLDHCAmPM2ePs2jpRK4pXVMhbYa7t\nPU6XnOYL3q/ipIVLa+CJ1FhkFActnuBdLu8/xfXGeUJj+zwnXmNIX+GEdp9o1z65WIhXXc+j0uap\n+g/4/PdfppVSud59ik3RS0X4sITEkq/IqudR5ndPonb9DhPqLDGyPOA4TRy8aL+CjopmGow3F8hq\nEWrCy3BpkzH3MrfVNDkizDHOPhFOcJ9udqjjxk+ZxIHb3jmu08KBjwqa2qaNxvdx0hXeRMY8qPf2\nITsNPtv/+7y++iKvL7/IbNMmOLxP0LfP22aMb1ufJi9FkGSJTwe/yZcCv8H/dPe/5eZb57FfAU4L\n1E+2yBIjrmYZYJUweWw6syA91MgXo2yuTRE/vkXBClE2fEy7bxE8V2TjXB/LDFIyIyiTBr2eDeqK\nk7eUp8gTYiCyTCp8iW/sfIFLxWcIOAt4pRqDrPI2T3IxeZkB1ti1u3hv90mK+Sh1PUD9jcBhS/eI\nIz5yHHrCDlIkA1zjPFFyPMHbeOlcXQ+xQhMnNoKgKPJS78ts7A/wT977x7jGKvjiJSLkORO5Rraa\n4MrGEyQj2/QFV+lhi9f7nuLd2KNMu29QIMQ+UY7zAJdo8I5Z5d7dFzAcEgxaSLE2stxig34mmKHf\nXqfP3mBVDLIu+rnBWXL+IPuE+YONv8WlyrMk5B1SYxtIqoWpyExIMwQpEnHkUE/qBAtFpt+8z9rp\nQVaigxSsENezDozsEwS69si7gswxwSa9JNnhWGmRwaU0VtKmEXWw7uwlL4cRlo2hyRTkEBv0EyPL\nNLcYZol3eIJZa4KK5eO0fBtddAyYLvEkTpr4KdPEiYSFjwo9bGMhATa9bOKgxX1O0IqrjHnv4zSb\nlB1eCuthjK86adcceAZaPP3cGwz75pmRJ3ENVUh6N6id8lL/shf9HYXKp318RnyTURY7XZkHzUYG\nCtpMm+KqRu7nurg4+APO+K6jCxUDhVF7kav6I9R33BjzTv6V/z/F46ygKwqf5tuEybMlUiRCadYr\ng3xr8fM81vU2ql/HQmKdfuLNfb6U+11qdogZ/SR8XSASBn+hCfsRR/w15dATdh+b9HOVe5ykToNh\nlghTIEIOB00atqtjOSoceAIVNL3J3k4cqRIm6Uwz6FvF6WpiI9irJMgYCSRdZ0xZYCUwxF4gTjdb\n1PBQIkCYPE6aWLZEut1No+ZCk5p0pbbQPC22SR14btRIsY2Tzr5XDiaZ13GzaI+yJ+LkRBgwccmd\nao2TzKHRxlIlMkMxkmmL8H6BXrYoEGSDPqp4aRsBqMOMfZyaw4vT0aDH3qbX2iRPiAAFWkLjkvIk\nulBIVXYx7s3Tk9zm9NBdKooHVbRx0MJJi24rjceoMSnNEK9mceTaVOMeNLdOjCxVvJTx00ajf3sD\n1TDI9YQoVYJk9C62w120PRpRT4YxFpitTbJV7sfYd2LnJFTLhDRUgz7KUR96QEb26BCz4VUwGhqV\nG0HkIQtXuIFGm5Sxg0abgFJizVGny3WL2cwJ9LADyWvhpoZ60HkaI0td81H2hVhQRpExcFM7MLKq\n4rRbSDWLes3Fvh1HxiRCliQ7CGxquDGQCfoKJEI75OQ4R04iR3wcOfSEfYL7PMsuv8w/7nQT0oVN\nZ1pInjB37SkAomKfBcYQEfj0xT/kOwufZWejl9D4q9QVN5qryZODb3K9fo69epy4d4+iHCRLjDJ+\nGrio4aGOmzV7gIIE+rCEuSRov+ch+EwZp7fJDl2sMMSCGKUtNNx0Jn+v00+97Ie6hHuwwKR2mwlp\nFp+oMMkMwyzTwMUOXWSUODfiU/TH1+i315kQDwCLhuSiN7aG4Vvjyt3HebPrBaYSt/jb0d9gzFxA\n87Z4bfpZToj7NISLr/DTRNnnk3uXaH/5PV567LucSd7my94vclue4hqPcIo7fNZ+mU9al2jZDtS0\nhedyi/1n/FT63Qcp3cESI6TpZuTaEsnSLr/7E5/j3fWnuFecwnc+h8tdx0eFC1yh0fTzvvwU/Biw\nBLU1L9+5+VlGxSwnn7hJzoyQr0Wp5/3wKQFzAv3/1Lj29y7ABZsRlrjQuk7cyrLk7ad+sUryOYv/\n4f1f5t39x1kN9fKS99s45BZV4eO49oDAeInVY4O4RZ2mcFLH3bErIETALlGYjdEQXpIX10lJG/Sy\nSRUfNTxUnR7+r+6fQcLmVPAGl31PUf3Gn/VgPuKIv/4cesLeJEUDwWlucyV9kWvpi4yMzTHlv02K\nbRwHnW4JMswyQVM4sYTgya63qNtu7spTLGfHUHWDH028TNERZFPtZUkaYTZ/gru502TavWiRBnay\nM5SzR2zxuPUO8wsvsNnsxXW2zIXge8TZY4ExigQZYI2T3CNNNzkibNDHaHSW7vIW19cusBnrxxlt\ncpJ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dHYwxnwF+tv9cfcZSuEhS5aY53cGpqRLyYEtZLtFQm9jTLhqLe0EU5dVUATOh\nNTA7hnhatnW5QpPmvMaTT8pH9pYCcouKizddqntVgRVtknYgt2CpaV+qs+mkUpI5VoYloX2Es21s\npFWVsi1KKXnmwrwEJP3WxoOMTckEX1sqEhT0+W5E4wtS9GO4aWmNaNsRZK4rc2RXm4YW4bbzGYxi\n7ek1Q00r/mQvSF8bOyJGXpJrWyOGzKqmA97tULgsbW/s9HCqMm7BWA37QYGDw4ulpAg0VY/8o6vS\ntmIY8y9P094t7/Vg6TLPXN6dPDu1pZj2MUOm0qsY1WWc7Hi6RX1K3mfzkEtlv/yomxMOnZyybzR3\nTmbBo3BF7mtey7J1WM4bS4LRm8hn9X6S890UDUHZsnVI0w1fyFA6J/duHQIn1OyRN87Fn7PWfoY/\nQt7OuX2nijcrTK3Tn97Jv/2hfwHA4+nnqMcyz2NiQlW8b1TWUddisiSF0ms2Jq3/6CrzVhKBJ9Jd\nDOpxm5aVH+VB3+MbD/+q3Pew4enPSKKmT/3uX+XwL18HoHPt+vf+wn9C5Vbm9i2BkMYYH5n0v2mt\n/ZyeXjbGTOvfp4GVm91rrf2MtdZ0/3szLzCQgbwV6Z9vt6DQB3N7IO8auZW5fSvsFwP8a+CUtfaz\nfX/6XeDHgZ/X///OrXZs8vmI+qjbc5Yte3gKOfg1cNpdZ2ZAc04sgfTVIOFQgyF/SKzPrcUi3rxs\nwSvDHkMnu+HnGom5G2oz6oibt3jH5TnbD7cwVqzfKOiVtqvOOKivkOZSLgnfL5QalDVU/cDoKi++\nIMnBu5kZMdBdRN1shy6qtbmRJ9DEXa2JCCev5enOZsg+tAbAsZE1Xtg8JH3JR7jKqKnbgNFntWDI\nolgq7StO4lhsD1kasgnALxsq6oh01gJi/bL1s0NECjl5TUM41S2k6iTc/IV1sXbSB7dpteTGf3nq\nCWJNkBWWLI3D4qgyVT+BXMKCTaCvTtalqoybzv4G2eNiwtf2hQwpZ377oOZev2ZpjvaKn3T58qOv\nGlYf7qUg8DRp2tITMX7Z02caoo461R2LdbrFSgyZjRuhqu8m78TcvpPEnZTJdfrv7+FrP/hLAEy6\nGVqaUbUag6N2YdNGicVdiSMCtdYdehkwQhsnMCdAPYF+lejQ/2xjEgu/bsOk7boN8bVub2hjHktL\nHdsXfvSzrP55uf5P/bef4MjPXQYgWr7penxHy3fF1I0xTwBfB07Q+z5/D3gW+C1gDriC0L42btrI\nje3Zu35jKcASAAAgAElEQVTqs1QOhuz7D/IjvPSDQRJcUziwRfsZwShiH5ozMoGKkz2+WmUri1GW\nRFz2GZmVD1uppXFPiuJtTegPPO5lIfTLJlF26TVD5YhqE9eSUigktWGSvmwf6SRVI7xciKeY4Wih\nxkZVcPfGpiivwniVWlUWl6FSjc1LwtfMzVZwVNmXl/NMzckQ1VsBnWflmvh9lSRNQKcYk7kumjK9\n0aP+dRVfdtlS1tQEblPSJ4DAOe0h/XFUDM0prQblWNLLGiy0Cs1uPYwOlB6XMkOjGQlI+kvTz/DU\n5l0APP2le8jOKwsngLKOlUlHWFX20190KZ4XfPva/1Ai1l9lJ2vZ8Q0tYvKARyCfJ8lZ49VMwl5q\nTNiEnprasklGx9iF3LJ8iDBr8LUwd33CSYpd16bcREnUp4TB9OK/+clbxtTfibn9rsfUjWHhpx4D\n4Dc/JevcIb+X/TKylpDe4tmPkYd9GjtSvZJ13ASWkeu0LjDd+l499kvb2mQxaFt7w9+77bnGkFKl\nHlubKPimjZJjH5cX2mKZfepf/A0AdvzSt+BN+A//JMrbhqlba5+G7+DBgI+82Y4NZCB/UmQwtwdy\nJ8ptSRMQBRCseAkb4tA/vsipn90NQKWawQz1LLr8eeWmvzTExgMCQWQv+biKelQOhWwo06T0akBz\nXKvYz4gF2TxbYvSEnFt9wLL32DwAF4/PEKyoY61jaA9rxsjzDqEY4ZhMhG2q0zZ0iNaELTK/nuEH\nH3wZgOeywnhZvjJCekna2xpOYdUpOJqr81fmvgnA54bfx2Ra+vXFk4fJPihsnuDpEtVdcr3NdrCa\nDMttQkETh5X3qSN3xiSpA6xHYqna95WJqtK/1EaK1IpmO5wJaY3Ju0Vph3BIg5kKISvrMm7ljOww\nPp++mz88I7CSk7YJr9yrG4amKsn3a7Tkmyw/kqN4Qfo1dCGmndNdRQfKu2Qs8ld6wWHd7JuZFcvQ\nRYFzFh9NM/tUWfvnsfo+GfzsSozT0W+5FNEc6ZYYtMx/XN9hs5dwLRztUK/2b+AH8mbEPSDRf96v\n1nll/z8HoKUBDJW4xyzpZ6g4xlBXlkvUZwWH9Jx19bhn1UeQWOLN2CbLaX8W/MQi/w79jKwl1kkf\nYkF3Ab5xyBpNbofhg5q944Wf+BUA/vKf+zjVvyowY3Tu4ncahjtCbotSL12Mqcw6rN0jH6H1wX34\nmlfFrLsJpBBsQ/mIKHLTNnhb8ofOfVXqStkrvdKDbtrF3jPsM8JA81Kw9qeF0ZE6neHCNcEJg4rB\nHBEMoLWYxfrd7b0hta2LykKQTLxOyyGlzAxi+INzwr2LlBHjb7t0NIVtnO8w8pwyQXZk+LmvCM35\nsWPn+Nbn7gUgnYKGpsc1c3GXMUhhuE51St6zOWEY3iu7fvOsBPw09rfwNCfL3BfaXPrxblZFH8q9\nz9mFrbKXfe7/ASn8+a1nDpMeFcrn/TuucyAveGNdnQjzjSGyBVG2tdBJaIydcUtrW5Tt4dklzi5M\nyniuO9RmhR3UzhlaIxpxW7MUr8h3q025SfGOIWWqrDwMld2yAOUWLPWdSiHNOfhaJSpVjlh+SMaw\ncMmhOquMm3uq5F8QqCqz2mMtuS0/ocgO5M1J9ZOP8gs/L4yW+4MODVWUXUw7BrJGa+XaqKfA+4Y7\nAsI3/BtEwft9e6Gm3usbSJsuBt97Tvfa0EJWj/uhGLlXIZe409tnWYtPl0YZJ4FNXfnNPV/guc/L\nxX/nZ/4G+d965o8elHexDHK/DGQgAxnIHSS3xVLfPORgImhpoFDqTCYpXsHBGmFdLbTLQeK+MpEh\ns6wecJMjrWHr5UMRTksdbWsOqU05ru3o5mwxlL6mgUgpMGc0F3fW0upmWAws/qYG/9zVolbWbbxn\nE5PDCQ2Fy9Lm9gEw5xUmuFsglMYsOK4GBV3NJXVJNxYLSQqEF798mNKSbh3zhjglfXEOVmk15Jlz\nQ1ucP65xLtawsSRbRnNAdhtjX02x/qRsh6/8GR8bqRm85SUpC2pzHYh0mzsR86zyzVMbDvlD0s4z\nLx/kxMw0AFNFgVZiaxjJidO0Pp9n6PVecY3/5c9/HoBfff1xoppMm9ZonNSKPfLERS78ntTkCwuG\nKFB2iwOu5tUZ/sI56cfmXpxQ+fUzAetHe9OwcVB2Co3TqSQtg3VIcrs7C1miCbXsPEOkn7A10aE5\nGwuXZSC3JNf/7vsB+Oanfik5V+9zanYtYugFE/kY2l34o88yd82NVrZ/E2gFYDuWM1kT4XLjzirC\nkNJzWdNn7dukJAHpPsgnbZweBx4SB66Loam89sRiNzEPalqS3//sL/P+/T8JwM5/+M1vH5h3udwW\npT50LqYy5+BfFOaIdcFtqBLaSIOvwSgdcEvyY44jQ/qgKp+vjROUtdjETEzphLxGfQrS80pN3NVN\nSWsJNcWuiXtVftymAYVcCGHomNALV68Mk54RWKZZD7BanMHf8Nk61KVaWqwm1Sr6CjOsF4gVrrAj\nIRtHdWEIYlITUjCjvpqjowWXK7ttgge3FnLJ8eutnXjdnDhjbQil711YZO39Ls5WNyrVUnpZoJPa\nTouvQUEYl8ljwmxZf2aKlqORoweaNC8Is2jywBrLFwTSuXSxh1tFQwp3Gcj+OWlje63Ev3rtcQAK\nX8mx8ZB0dujABhtrEq366uk5cjqbwoJNasgG25bqTk3D+wMHASlSPfyajMnm4VTy7oWrMY1pL/lW\n3Tw92/d0KJ7UWrEf2qD1wkjyHE/nBOsZjDeAX25Vzv/yo7z6o8JucXCT4J5+6eLh/Vh4jE1oQr7p\nUYaa1pA2PRglUfimdyzwiuYEMtDs5jXqg1BaN/mEjrYvxz0opmYt6T5oZ1v7mzV9+WS0hz4OaaOR\n2hhe+pRg7UfH/hb7P31nQTED+GUgAxnIQO4guS2W+tq9AmU0xVDEiYSXDIAfUzwh1mccWBxHQ+ZP\n5Ni6T6yJdEgSvGLaDrllWaHL+1y2u2Hwo2LZxqFL5W499U2f8mHdotUcHjhwGYBLWyMUUnL91pZL\nsyPOv/SKi71XLMFd+xZYrcn5zcvDpE/LLmN9QsuppWOyowJdxLFDmJW+5jNtcimBSxpRnpqkrCGz\nf5vavFi5/qbD8AMSsr/9zAShFswwfoyjKXwbdbn2gYfO8+Jrmqc4HVF9VNqendhg5cszAOSuG8oH\nxTpv72uQOamx/DNVWlpEpP6FSYbUVCo/IZCM53fYUZJdyvzJSXyFk+Kqj6lo+cAfXsbflL5snxnB\nmdJasedTAvsA6SWPnHLJU9sRGc29s3qfTLeR0zGNGRnLYNuyfbibmdEh2NCMjkdaeKsytkOv+tRm\ndec1XyTQoDVjwfum7DIymV4Rk4F8Zzn/y48CcPKT/4zI9my6rCPzrBK3E+u7C3+4iLOye9y9K+47\nThubBA9F9AccQVOfkzYxDt95N+X3WfUhhkit87TpQUKV2CGnOiHn9PjrzT7IJ6LHokl2GNZS16Cp\nCJvANq9+8p9wr/nbAOz/iTvDYr8tSj2eaVJx0qQ29KNt2ITBkt5wWb2vh4dzWbDrKABzXvOwFCHW\nhFD+pkND86kEm4bWWBeE1/YKLZrKlOmvqhQVI156WTDgu++9wmhK4ID5zkzPo35fmfi0KDDev8F4\nTq5pXR9LIikzS5qH5e4WB8YEwrm6PUR8RjrVORSx1tAcsha8o6J5Go2A3FW5t3ZXM0lna0pxEjmb\nybUId8pPa/+UKP21Rj4pTG1GmuQyolSXvzpDVtkf1oVhxcYBrCZoqV8tEBdF8datlwT9xOsyPsMH\nymR9WSSO3H+FxYq+u2O5+2GhgZ24uoO4Wy80F1N8XtruZCG1qrVdN0mCiDpZJ8mnnruuDKMxh6kv\ny1it/cgkI69oMIlHQtd0tny8qgaiFHu1asdfcmhrFaZOxlBYkPdZvddLWEsDublc/3vv5/Qn/xkg\nQUC+Mlpi4hsoiV3p2ln98MsN1EX7hq1+gnvfCK0E9CCXSM9HVhQ3iMIFUcrdBcA1Ftd0I0p7yLyD\nTdpovmGB6PYl6Ms90z0XYpNjF5MERMUYzn5SmD/HVv4mO//Rux9jH8AvAxnIQAZyB8ltsdR3fC5g\na5+ho0E+zRGThJhn1sBt91ba0eOyGnfSPcilPWwZe0CceJtPTyVBTM2JmOy8rFPthsAFrbkWnhav\naI/EGK384AURpWlh31zaGOF0S/jrOx5d5Mp15YRvZph5UJ5z5swMpqOO0L1hjzM/Jlu6D+y5yNdf\nlaT+2aseri6Xja00pin/SK25BKeEzdI8EFOfVifO1RR/7Ye/AMDvL97N5SsSy1/fzOApjHPqsjBV\nTM3DmdViA9ezbButdrS/RScvFrfpwNay7BSCsxmMMkTiYgd/RSsvLZmkkMXafdK/2lOTLN8rbTt+\njF2RG8cPrLMzK7H+V0tDZDWV8ObXpnDVs1U+FjLxh9L2+j1g1OIqXYoS1lKoG5Z2ydLYIykSTCT5\neQDaEx3QMR4+4Sbc/a1jHbLjskva8kuULkq/C9farDwgcFJzJiS9Pgg+uplUPymQy0uf+pUEFmnZ\nTuJMBBJoIqZnjffDL7W4G6bfs7ZTfY7SSuyS1juafQFKoSVhuYQW2jovAhPj02sTpN2gD2rpimsi\nmmqtByb+NgsfbswxAz24qF+6vPgImwRRpYyXOIm/8jd+kR8+/2kA8v/p2W+7/90it0WpX/8zMcQx\npqWaz4HpP5TD3PU6G4dl2x+WLJtHZPBHTloi+V1TuG5ZGBXFO7zWSw7l1Xo5UrqSfT1NU9P0xsMd\n0hdFUXUO1Qk8Za48O0Za275yJMXQK6Ictu7qsPqiBNow0SF3SYOCRh2Y1YrYNbn2668epnBW/h49\nvs1YXuCPaxfHcUYEU2imPFp7lfa4mEoSY/k1w6+flnwbxlhcLexsIkNHk1c5uW6V6DZRRZN8rTjU\n56QR49okr42zu85IQfrXbGboqFL3Mh2ilKbkrZBUCspLYSasA+nzcnFzMsLRAtgTuSrHN8QZsLWR\np3FZ8fqjDUJPfRSxkzB+SuehulO3zlMeniJB3ffNX4PLn1A2QzUmzusfXMvwS91kNtAa1fHZcGmq\nT2HyYsz2Xk2BfLaJVWbP0Cs+w+fv/Jzab1bc/Xv4P/7hryf/Dm1/znMt3m5tkpOlPxq0C3qE9DFU\n+qRuTaKY0yb69guA0Dq4fX/rKu22dYi7edaTvC72hvu6bUaYG7D47iLh0INwfHNzWKaL0WdNL/Ap\nMIZ0H10z1uWg5AT8wj/+vwH4B6984l0beTqAXwYykIEM5A6S22KpmyAiezJNWOwG4lhCzRuy+ERB\nanMijs9uiHlmpY3XENth85DH8Kty/eZDIelrAjuMvxKzdkydbpo+N7tkk+LV2XNB4uCMQodKU7fu\nkxGF85pbZNNLClnkL3sMf2QRgK0vTFOdU1ZKBPG25pnQ3UZqZ5WqevB25ussb6mT0Y+JtN+5sTq1\nbbGEp+5f4tp1MUXTd9X46wefBuCp1aO8uiztOMUQNCNiWhksUcYy9rBAQrXpALso7I8g1SHUNLxR\nNWCtIv079PErrFQF9/jgzAU+f1aKmpb3WdqjOrgKT2UuppKC0cWzLpU9Mj6vl2fJT2mN1Mj0KhhV\nfP7Ug6cA+MOr+2gjfdw8FmM11qAwUaX12tAN3yQ/b5NdWu6aQ+UuZc1cCajsVmtqu1dVqXBZ8tYA\ntIYsgVLT5z9aYuZrsg2wjqE5pg8YiAQaAOlfq/JEWgLkhIkS6bFNQv9rNk6s8n4rz+1zjrb6IJeu\n3Z3us46jPsjFv4HLHiXWtLSlaR2MTeI6Qn1qKzYJjx2gophs1ukkVn1Eb3fQfVbS75vsJlLdgKi+\nd2tai5MEKvUqMDnWcn+gc/FfV6g9qTe/y7I73hal7niWTlbS34KkxG1pEOXIyTbXP6KBJm2Dqyla\nr384oCQBiVSPtEhfEYXjrfkMn5KJ0OmLRMhd14jTvZDTQij1GcvwXcK6aF4YoZvM1606yYTIXTeJ\n8nbahuvnRVPaAx1GZgRX3lgpJthvt5pPcznHvrukVtyl5dEk3a6fCykpFFJ+eRRnj2jNxZencGbk\n+KOzZ/jdRckJc/bMDvwROf9DB09wpS4rzIuBZtfqm1+1U8M89MRZAF64sIuDs6LsPSem0ZExPHN5\nmpFxYdxcrw9ReljyvaycH02iaIfOyP/XPtzErIli9BqG1Jr+2EahdUZ8AdOvWCoaTBTORDz1FSlP\n5DYM0S6BazJnUtT3Kb7a9Im0DGCXzVLb4bDzKfnxWCfCbckzt+4LkyCjTqYH12B6xbG9BlR10fXq\nUN4ti2S7YIgyt5Rx9z0hi58WOO+be3tp4vtT4LqmxwBxeUP0ZnLcCybqSt2aPoy8N94utkcp7MPO\n0yZOrm9aN1H+oQW/GxhkurlmTA+S6ZvoTev2rsXewJDpKvWYHtYvf+u9T/fv3f45fe+G6fkQQuIE\na//1vb/LB35Cok6nP/vuYsQM4JeBDGQgA7mD5PZY6lfTOB3IrMjqu/rxFpnXdOt+MCC1X7aL0Sul\nZDtuXcvaQ3JcfDWV1MZMV00Shl7Z14GM2BzBlmI4RypUVoUh4o02kmo/Y/s2WNOQ+ThlqT0o1nHU\ncJmdlaQjj01cSopJr5TzPD59CYDfL99N+oR0oHG3WOHBuQzrJ6SOY+pjZVoaeu81YH1ErEk7ExJc\nTifj4GqahM+135ewUoIY2r70/b9fPkrrvLQTj6sTsOWyoDWQg5bh+ZOaMnXTY6Gkxa7TLRpar9PZ\n9qgXpL3NVpaNsozFkw+f5NXfkKisZMe77Sfc9fZ0mNRwtb6lcECyRS6nR/CquguZD4SxAsS+ixvI\n2DsPb/GBKdkePXt1N3FKLcI17VMbqjtkd1C4FiVWuGk61KfUadYigeeijEMgU4KNoySVnKaftpR3\nSzudDLSHv5058V4Ud3KCf/4p4V7350ZxjMFXOy7CJuyRuM9adQ3Eb0AbmtZNLOe0iW+w3LuslILp\nJKH8LjaxuLdjP9m1uljCxIKPqGs61iw6h75DavvYmmQnHXOjQ7UrUV+QU8GJvy3dQMrcmIemy6OP\nsBSc3l+SOqsY/umn/h8AfuE3P/quqqA0sNQHMpCBDOQOkttiqXs1Q+lCTKRejOn/EjD/MeWPb7k4\np8TidAzMPSVUvvUjAZW9WmuzbpNwf5Pp4C6KJRpsuLS1SEbtfqUctj2CcXGmtRdzrGsNzh+/7xn+\n7dkPyjXjLcZHBHdeOTNOPhBs+FR5iiuL4sy0ocPvrd8n1xupvQlQzIuF33IybGoRD+dKISmD1xqP\nexGgW05iCXsN2PfD4iRoRj5PPizHv3byMdhUnLjl8SMf+xYAv31SsOtHD11gvib49srpGdyKWqpj\nIZVlcYjG405SL9WZbPLEnFCzHi1e4J9Wvw+ARuSz+bBY/+N/qE7f0RZsy+7BX/UTy3d0zyblmu42\nXEt2qRcBavfJWIVOwLSO4cLyEN86J2Xxpu9dYn5BdgfdEntNYPrrMg4rD3pkFzWCdsElvS7Hm0+0\ncJfku+78SoPL3y/P92qGzqT0e/EJP/GXNHd0cJoDGwXg1M/u5h5f5ryPl2QvjPuiSJs27KUD6HME\n+vTzzLt89Z4DM6bnFI2sSbDupnVusKD7KY5dKz/E6cPjHbLmRgvd7+OuN61zg9O060yNbY/eGGMS\nuqTfF7latybZEXTbCK1NMj02raFgelz87o7FMSbJTBlby72BeN1O//09HPjUu8dS/641St/2Bxpj\n5/7fX4Agxt0UBZtZdpIteH1HhNUwea/Yxs6LkslfNUnwSmNHhK+ZF4Mtk2Tzi7MxpiQ/+Lwq2/JG\njvywTPB7JhZ5bXUKgObpoSRNQW1nhDMmyikqB7hFacPGJqlLWsw1Kb8sCj4cicnPiALr1iX1L6YZ\neV2zCu51qO/pI8xHvTw1aKHqfLFBSjne1UaKuREppJ3zW7z82h55t02Xzpy8RzYv/fPdiKmC0D9O\nnZvhoaOisJ8/s4dHDsvxcr3Aj8/KYvCflx7g5BUJXBoeqVLQPDSPjF/md87dI+9zXdg2e++dZ70m\nCrh8dpg4pdvmWm8xclu9WIDK0TZ+XtrbNb5JVetCrr4+TpSVH9OH33eSr5yR7IxdXWFrHsPHRbls\nH7R4ta7TGYrn5ZrY622520V5LkiB8G7h7U7OJoFNuaWYpSdirv71v3PLNUrfbrndNUq9nZL755e/\n8VuMO98eaOP0BRu1bHzTAJ3Q3hgMBMIFr2sQRKpPWffDJf0KuV/x9zs5+68PrZNcU9AJFVmT5HkJ\n6TlkI3pKGiRtb1eafef7F4d+LjvcyLOP3vDaXX6Fawx+0kYvrW89jvhrj/8YAJ1r17ldcqs1Sgem\nzUAGMpCB3EFyexyluZBSqc5WTRx+jXsbRHXpyvBLHtuatzx9PpukEmgNk1iOuSsuvjrrNu/tkFoV\nq2/4ZUM7L5bzxgP6arGhuiGNTMxVqF7VnN5zDaqTmis9E9JZkR1BYa5M9ZrAPzYd470u50c/ts7G\nbs0kFTlUloSH3t3ypzYMKw/qC5o4iQqNRkPuPSQhm6OpWmK11qpp5nYuAbC2VORCW1IDRG0naTN7\n9ybV0xJO39Ak68HBDdbq0o/iRJX5akmfCUs16fdmPcP/+cL3y7sFHfy0bHMfn77Ef31drPPrx6cw\nuoOIS2L5XN8YSpKfZdcd2sMyxmPHLdt75dqgbJMCGKkFn+GHZIdx/sJUkgffiw0js0L//Mbnj2HH\nNUd7Tv4frLtJ/dPUupPQNOO9dbjQ5eND6aL0a7Pgkl+QtrNLbfLzGtPwWIpI/eGxaxh63UODY9+T\ncvrTswDsdP0Eckn1wS8gFjoIV7trsb4xAVdXevCMSSz0fggl6remrUks77gvAjS2hpa6KB1jqSfc\n87DHWe9rb1v/7vTx2B1jb7imm+ArbaIE8umnOnavk/+TPOONFnpXunvqZmzJOd13jkgrVFVyAk7/\nhJAg9n/69lnqtyq3DL8YY1zgBWDeWvsDxpgR4D8Cu4HLwCettZu30I7d9c9/Ea/mEI7Ijzy15JFa\nV175fS3Sl+SXauIeVzm7bEltK1e1FrP0qHx8twl1zWQYbDhJDpnulr49HBMNy3OGRqtMFwU2OX1t\nigMzgpMtVQqU10RRTs1ssnx+TNtz8TXQpXasmeDUcd3DqckH3/kV6dP8k33bQB8yijt7TRLeux1t\nk84KXBGdLlC6Xzjzc8VNXnpFMkaml10aO3RcxnpsnaijP4xraWYflOLZl+bHeHj/ZRm3dpprW7JI\ndjouowXJe7BeyXHXlARQzVdL7CkKi6Udu7xyTSYqC8rI2dHEdhV90yN7UQazNWKJxqTfzpZPoNBX\ne38DVuVb2ZE2aMWozIJL6jFhEG1vZ2FdrokLGuzkWFzN0xKnLf5Wl/4C4azgLPlX04yckp+bdQ2t\nUhfHNxQvyzUXfsxLFoShEx6dHJz8hU+/Kfjl7ZrX2tZtg1+MH/DpU1IM/clM/Q3pAHoBR11xjbkh\nn0uXz53qOw5vwkZp9mVM7K9c5GAT3Lv/b/3QSWhd0qZXjMN5A4sl7ls8AhMnrVWslyj4lIluyA/T\nnwa4P69MV9rfgdPeL/38+q6kDUkqAd84PNsS/fCLhx/AhrcnHcU7Ab/8b8Cpvn//DPAla+0B4Ev6\n74EM5N0mg3k9kDtKbgl+McbsBL4f+AfAp/X0DwEf0uPfAL4K/PSttJe74lI9GDL9ZVn1lx+15K/p\ns6oeOS1J1xo1NMfkuF2CKU2cVh/3MLpnSq9ZjFqx1u1xm0eeEGhjcbWE+oz4s7tP8MXFQ/IPC7VQ\noIbyRi4phbb26gR2SBMJZSzFS/rMtYBgVqzfjmspvCJDd/UHdftXrBNfU3gGS2NGE3eVHbK7ZXew\na3iTC6uyC2iPRTTaYq2+9PI+0LJ9E4eWuXJRoljTTxdoCfpCZ0jsi6F71riyLA7bXTvWuVYR69x3\nYsITAsWEe5rUAnm3dBBydl2gnVyqzV+ZlHQEf+vFv0D2BYGljn3iJADfeO0AxQnx+JebeRpTWoxg\nrsxwVthE11rjtNWpbDsO2V2ylQlDl46jjqWcy0RGHLyPTl/hSxcFcnJdaW+sUONaQ/qUWewl/Krd\n18BZkl1D9ViT5rhY+OkVQ2ZNWRNZQ7skYz/zRUNb98ubRy2doW8vyfZHyds9r2+nbP7YA3wkI0Ue\nqrbTly/8xqyLN8uL7nBjfdF+eKMrXTij/1zXeZq0Y3qQS79TtGu1u6ZD0/bdo13wTZRc1+Wux0TJ\nM31iQrWaQ/rgujck+upKf+RqTncGbeswpJuMSnzju3ctW7/PBg77+u1g+WBarPP//X98H6V//ye7\nmMatYur/BPg7QKHv3KS1dlGPl4DJW32osVA85bN6vwYW+XHyw85fcglqMiG3D0CkOLpfMUnAyvbB\nGF+r3NR2GoEBAO9ymokX5N7aNemOvSsmd03u+03zMEG3CtDBJitbQqcxjsVb0vD4miE4IMq72Syw\n+kEtYJsJExjjzNoE2wdF+bh5UcadlseB98nKdPbcDkyo4dDTbfy4hw12f0u79q5wbUU0dnrFpaXX\nHDi8yvWqMHQqu2PGX5LrVxWvrzZSlIrSv8sXJvGHRHmG5RRBN0Cj7Sbb1UK6xYemhC75+etHeLmx\nG4Dp4TKbH5S+Lzfks+bG6uTTorCrmTTBdc0GeaCdVEFyqw7+koxh7FpsQ+ufjsZYDZB64MDlBN8/\nvr6D9LeUavmk4OzXT0/iT+g3O+8R6qwKzmWSQKjUpXTyayvvjZPcLyaC1fvV/3I6xtMok+FThtFX\nam8WU39b5/XtlPqPbNOwPVigeZMQ/9D2mB4YQy6BHXpKLqLHLukqd4e+ghWxl9AE+3HvN0pbP15A\n3FPOJsbvw/dDbT9Rnsb26I997JgYcwPrpqX3+SZOIB8X27ve3ng9QM6Jaffp//40Bkl/IKnelDUm\nGcGam60AACAASURBVLt6HOE7Oiaf2Kb072/6yn9i5LvCL8aYHwBWrLUvfqdrrADzNwXnjTGfMcbY\n7n9vvasDGcitSf98M8Z85jtc8z3Na21jMLcH8scqtzS3v5uj1Bjzj4C/DHSANFAEPgc8BHzIWrto\njJkGvmqtPXQrnbr/f/0lvIalMqur+TZE6qtLbVnGv6Wlzh4ZSyy3zSMQjotl6a37ZFZ6vOm2GIW4\nLcgtyg2NUa11uTtOWDPEkN0p8ILrxOwbkeeceGY/dqdYjqnXsklJterRduLQC7YMvuZcrz1cT3Ka\nZ9SabcyGjD4nFuT6+yJyV+W4XbTJ86NczOweKUu3tFHE14xw9dUcuYla0q/KvNbdvO7iPiI+uq5/\nZKa0zaVV5cs3PfIltXidmPgpOV8+GGE1k6JbCMlktV7rc0MMPbmUfIv1ssBFrUoqGdcDD10B4Ozi\nBJ7y6Dsdl6gh75M/E1C8LGO8/JChdHhd+21Z39Cdz3KKwuWevbB1nwyo0eRnhZfTVO6XHcbO3/ao\nzErb24ci/LLmjw8Nrb2aMnLbp3hWrLN2CdpHNLBsIc3ocTlsDRvSGzHP/7ufuiVn0ts9r7XNP3ZH\nqfFk7P7e2Re4N5Bx6S/XVutP4kWPDRLTs0qbfSH2/ZBGq88p2pU3slKS4hXEN00HENFjxbjYmzJn\negFCzg0QTv99b3Sqdq/vttHGSYKPHGMT2KW/jV4ysV5gk4/9Nl6+9KmXVsA1hryR0TobWn563/t1\nEG+eQ/6dklt1lH5X+MVa+3eBvwtgjPkQ8FPW2r9kjPlF4MeBn9f//86tdq6yG7AmyedRn7E9nMw3\nLH9QceeioXpIFULTTXKRuCEJyyW9bqnNaDtzEeGjMrFbC6KwbDrCaKEJm4+ol2X1cPyYK67AH6n9\nZcLXRZF2MpZwRrHfp33Wn1T8uJJOgmGicoBT1zwTV6Tj2QWPoKbH17xkkcotGJoj6rlfc1jS/Cxh\n3U8Cm8ZnN1m9Jn3JT1YpaGBTJS7i1EXhFnKi4M4vTuCqsjXrAUNTovRrbb8XcTvWZGZMoI7L5yap\nbci47frwPJcvCJrgFdtJO4TyLp18xNkF+Xu07bNzv7CDrp6ZxB/XohujfpJdM3fdsI0sJON3r5B7\nRWCZytE29Vn5bq4bk3lV3rkbOVrZY3E86evi4y4pWRdIrbkMnZXzWwcNhZdlEE0kVEqA7Xs6uH1s\nna2WXhNbto/G8O+4JXkn5vXtkPBJye55b/D15Fx/YWWXHmUvtG9geuhxxXpJgBD0gniymve6ad1e\nhCZx8vd+6KWNQ46eIu0qYQdLU3Muh0DOvKGKDSRt97eB6UWi+twIs9S6uLt1cFV5B8QJ5JOj823w\nSt26PUX+hupKUc/m69U0tRCoMy5r3IQWuseHzvdJZLn3pe+4ybut8r0EH/088DFjzDngo/rvgQzk\n3S6DeT2Qd7W8qeAja+1XETYA1tp14CNv5aGxC5lVQ+GaZmkcNnSd4lEGYs27Pf5qG68hq3x92tLR\nvNxtH6KC5rPwPUxHzs/uWaX+n8TJGOTVy5/qcdebE5Ba19wXMyGdnByP5WtsbAlzpLo3wiqLY+2x\nDkZhFve+bQrKAOl8bYrW3eLZrc4Ig2TyxTblXcq9TkF2QdrYOmKJi2JNjDzr04xkHc2UmjQ2xLLd\ne3Cdjz5yBoDTlUlePilpAlKbDkP7BC5aPyFsEetb2iVN5D9bY+G4vK+dajK0Xzjo9WYqscjzl7yk\nFupWPQP6bql0SL2qAU3Dsgtol1PEWxp8NFXlygVh4QRbDmZToZrZNmsjCpstebgKVW1WsrR3yzcZ\nmyyzdl1YOZl5j/Sqpn1o6NbaNwl8ZXIxuRNqVW1GrN2jsFUppqnsm6ETHqtPioWXKTbpFDTfzVoa\nXx3SXh0yy28t+Ojtmte3QxYeV4aQ8ZLydKHt5QWPDdSV7dHPQXcNSVbFnOn0FZDolZnrDw5y+0rL\nJRax6dzgceiHXLriYhNuum/im14T9sE8TXpO0GQn0Ac4ONiEgRPekIHSEvRBTV2uerMvB0zUt7Po\nvmNIb0eQNnECxfj06rI6TpTkhAFYeELGfO5L/ImU2xJROvqapTFqcFQZD5821Kd0IvkkE2XjcJBE\nDBbPQ3tIrrEGzLx0vTXS+7DXFv5/9t40SLLrOg/87ltzz6ysfenuqu7qFd1ANxobSYAgQYjmIkum\nJWIkezQSJcsRo5Fki3KM5FHYoiNmLNF2iKE1JibscWgsWeIicRVFQhRBLATRQO/7Wl37krVk5b68\n5c6Pc959L6ubYlMG2c1GnggEsl+9fMt9L8899zvf+U4e8fcRxS6bJAdcuNSPgTfo73o7fHmMlKOw\n60oygSzDt1KTsLhJhbOcwK6DVOizUMwqOVvxSAneJjnk2NsJl59P98LpYYZIxkE5TrCAVdLQ7qPt\nrR4L1nX+3sN1NHTeR3Ox0qJrWamnQ8rCvirycZo8CsMsflI2ocf4eCsJTByh61supbHJUsIAMXoA\nEt1KLHKzi408sI2c42TvGi5cI9lea5WuI7MhUXkfTSLZT6cRZ3qENKCqSM2yjepuZvyMN+G3aExH\nMjWsXyISSXW9Dwzjw2gQ2wkAVt5BN/bUkcs4vUKYWetcTkknrx3RVL/UHV92MPNBcvxSBwyWJnYK\nIfwj+yW8fZSLGOwtYemNYbzVTDxIUF0zQmPUIdCUAdQgOqh6AfulLtHRQeh2hUZKoGuL446KcgXm\nQXQIdFWCNlcdOi06mpKeY0a0Ohz7Vqv4VkehUoDd+5FJxZcaTNaN0SMMHVOEjJsgL+DJUJQsWjRl\nCh8x/l7F15Hl621GoCofoeiXKTRoD5a+7XXfC9bVfula17rWtfvI7kqkXnhcIr4ItNLMdHAlmhxk\nemkf257h6POL2xVEs7FfU7BI/pJEbThUaXS55ieXr6G0SXBIY5OlWh2B1R+myNu0XDiztLNftDG8\ni5gom7U42hlaEoxMrGF5jVu37S3g0TyxQWbXDqPC8rPuahwiQxHCxiJrrwy3Yc1TdOI2NNibNM3X\nd7chNhjmKElU+D4rl/LoP0hR/vmFEfTmKEKutyzV99S7mcJGiptwTNMxeh4tYLVIEXF8QcdsnSJe\nN+UBMQ7xLR/vPXgBAPD8iUOwC/SYey/4MOoUKc2NZCG20yrAYxZMdZuAcYKOXdwbKiPWxzwk5ini\nqY94ELxSSKWbGBqhldGNlT70HGXW0nwOGvP3jZkY3AQ9t0Br5uVT+2CvsupfNOgRIQtq5oMmkhP0\nR3++BzGWkWj2SlT30rH7XzHQWKdrnx+MI38Vbzl778Rl9TmAXKjxA41vU3ohq0N08tY7dF5USzet\nIwIPLAqbBJGuLbwOhkxQOESJUv+W/X2pIcaJ0nYknowWHwXbHWmoSL0uDcVsiR4vpjkdq4YoH967\nDUkkgHNMESZ7o1F7WgtXFboIC7W2jsYHJqhY7+wtZ7g37K449dwFDfENHyuP07/Hvu4hvkrOptLj\n4+q1EQCA2O3BjXOBQit0CtHuN1pLKJ2XyrUcJOvJ6An6f89wCcVzxKbRSgIjF2n73AckFmeJuSHa\nGnQWr1q+PIDJQyTac21+AF9sUHegbKqB1RVy4HpTg2BWisvYPlwNVolxzF0NNMHFSUUDiV3knGpD\nJuLHiPZn1iQ2t9ME5HmactQHR5dwjXF323SRtAi0LnD/z+WZXqWh3jzQgKbzS1m2kLpOj7P2YBOn\nVknX5ejBKVx8nio6F5/xAZ/G7SfHLuMvrlIWP9A5N/qaaAdMoaIFs8LXsaqj2RssxQXSTKPMxpu4\nOkvYff41C+XtBC2JjA9Z5K5JO+vwy/R5cpLolDOrPUie4ebabWBzHx165+daKO+gcWvlhWpYnd6U\nSC0FHZYEHM6FtDJUUQwAtQMOSrvfeo2n/3HPcfU5ijHXI9ovAeRSkaKj8XNQCWeL0HFpkKpwx49Q\nAANLiLAJtL+F5RKIdbWhIyna/F1dTSRahHVCtEeeECKwiK+6FzU76Ii3K2aK0hSBTvpisDlg9WjR\nyWXLd+zblCJo6KzE1SOyxR/ueR0AcBaP3vK9e8G68EvXuta1rt1Hdlci9doo0M5p8FiKdfb9Gka/\nHkQWJuLMllh9zEdjmLanp3TVl9Q3qZAHADRHh8Hyr/7ZHJIMgTT7KWqo73fU1NXKS2zsD2g2LvQc\nc+Bn4yqZN7B3FVMnSMJUDDdRXaWIslEyVFQcLwhUJ2kZaXKjj9QMVOTjXEtAcKMPp8+Fy9o01vEU\nWo8TzNK4mUQ8TuevrKRUFNtr19AzSrBIzbXg+syWuUwRbGPUw1NPnQcAXC4OYKVAqwc734DzGA/h\ncgLOMWLLnHpbCjqzhkRLg9amiGO+mVNaLGKQO0MtJyDy3CDEkHDGaHWQf8VGbZhlDN5zExdfJ3ZO\nOecCzD6pjQIGs5aEq6M1SM/WLcSR3kErld4YJTWvV4bQToesFZ2T1CtH4+g7T+dff8iAZHygMgGY\ndRpDoylR2smMhgogeMzj6Sbc3bdyoO9n02KxjoIjUzE6ZIRvLVXBUU6DSqA6MiyVb8uQLeJHuhwF\n2i4dCU357XRgTLXdgqei8M7vRkv/w+g4CoHEIkVDQdTuQHRsj0Iu0aKkYP+Kb6rVRkcBk9KgiRRH\nSQFWKIEJqZKjOkKVRjoOR+3Sw26usdBiMfjNJu41uytOPb4q4CSBxAw3nl2WqJMPQrNPwk3wg6hp\nqoNOddyHWQ4pToHmeOY60CxS4Y5MSwQaQ8GK0T+Zhc6UxvaOFmr5QLlIU5Kz0pCqYnN5qQeZPVS4\nU9lMIOiBlVwUaGfps/tYBbrDImKsmy48oP1+cl778uu4+jWW0r1kIvYeOl7rHUWY7KSb25ow/5rg\nhcR7yyhUCJb58MgJfHrxKI2T4WCa7809TJPBhybP46WlSQBAo21CK7D0bduG3Emvp9bS0GaoH6s2\nRo8uAgBml/PwqjQY1zb78dT2GwCA50+SxnpsuA5nmq4juS7gJviHaQpFJz13eRvSS+xsc0RZBIDm\niAfJL7twNQiX9tn+FQ+zP0zMnuOck4AngHfQmJRnMsif5cnAB2Y+EOjgA4OvMy0tp6HJNEq9KZFk\numhpEmqZLS5l4GTfWo2ntf4+haMDYWcjTUoFeehCKBihLTs1xQO2iCM15eA9CGgR7BkAHN9UuDcQ\nOuFmpKBHE7760VEVKf8+RavjmtuRIiJnS8VqVDddi1Simltglq3XEdjt9vEjcFO03V5w3Z4UHccJ\nKJ9pXUfdDyYGIMkOPto9Shvshz8zd8s577Z14Zeuda1rXbuP7K5E6tXtPoQrkKN6GzT7hEp4pW8C\nTcpfQuphwmPgGBSfuZ3zYK9xAUocqE1ww+e6ppos2DcYrhhxMTjORTlfG0AtaFiRb0OUKMo1ywJM\nn4UYdZXMbLNl4uhu6vv5mrsHkrVLdEeHXKHjB6yMVg/QukLh8ZnBOBJB/jQJlE/08WeJoQe4MUfD\nQmk38/RtB//LBOkK5/QaWi49lvcPXsAfzT8NgMr2AeDVzATWmHGj1XT43LwifdxGKUPXlCwIcIU3\nEksaZno5ISykUo9cns8ja/PSkSOY5mYMo4dWAABrrw9Cb9K+pX2eUrqsj7qojXGnqZMGig9yVyNH\nqLdJr2hIzfOzygqYzAQyZwk/2/PBazhzglYymiNg1un8S+/yVSFU8oWkuq7yLsDmNhVmVeXVIDVa\nQQFAz1UHK48GaiZvDZOJGLRIXKY+ibDDUTsStTuSkqIA0JJAgse3BS9SVu8paCIqA6DglFtK7Jk/\nLjUFkUQ1YTq6I0F06LNsPTYQ6UIUYb9EI+no8ei7YeRvRiCXQFZArSS2RPXRawrGLRYJ9Fuy8z6j\nEXpgMhG7Zdu9YN1IvWtd61rX7iO7K5F6ck5DfM2HwxWLrbyEy5/jyxJOliPYfRtw/5qi3MLjPmSO\nxbWauupo78UBe4VxbR+IT1IyrriNZv8je6dRalOEuLLHhV5jatRUDD4rGXpxqSJ8DUC5SRH8+ycv\n4sV5wq+1njYkt27zdAkrkDJ4litOT4wgSxA1/ANVlLhfZ+xCHG42OI+P7WkKOZdWs8jtpRXEb+z9\nMj5+/R/Q8RI1vG3gJgDgSn0Qj4wTT/7YJar+XF7Owcqy6uJGUkVTpb0eJDf6qA/72P8wfW+m2INE\ngJHqHpL9hPt/YOQCrtVJBqA+TsnltqejcJooim7Oh+Rkb+68gb5ztHpZNOKoT9LqoPFMCyhStGKu\n6WhzYxCxo64UON1TcQQlifX9dN2XVoYgBuizmImhEGGGOav0rBpDAg3uIas5UMqZzT6BdjaQHRCq\n4tgst5G/+BaLUbRIJA1Pcc2b0kdFBsnMcHczIhOgIfwcbSrhy1tx5zb8W6owga3ccE9tr0ljSzu7\noEdpJPqVYaI1pqo4O1vlRRUYo9ujapDRtZlKhEZUImNa0MovbK6hC6lWLB4kKqoxh4tEZLwCGqMZ\nGRdbRFym3xn93yt2V5x6s1+i3aPBolwZ7CJCHjSIew4AG9fysPp4ow88OEH88Quv7VTyAF7WhV7m\npV7Kh8WJyJ5BKp/enV7Fp14jWkhysAb9ZYIu2hla+gPU7KG3lxKRxXICVeagf+GVR1SVs9/jKGaI\nkIDHsrDrNeKaSwE0+nhi+mIe8V763BjwFb/eKOu4/CdEyhaTEhssW3Bm+3a0mSFzfmYEl01yrP5C\nHB5380nmyak6jo53jtPscSI+Bp0LsqqzfWixHEG8oOHiNHH9pSuQ6KHvNlomstyR6HxlBMfeIEVZ\nP07fS8yYYFUCuE9V4VylBGd50oeTImdrNADBTBR/OYV4nQteElKV8h942xyO5CiB9MrQLsQNmoHP\n8zU1V+PQudOTm/EhbU6wtjUIZufEVyQkOy0nDZQeoHHY/iUgvkQTd7s3jpn3s9zxwQQMVuR9q5io\nN5Xjqft+R3I0EUykMipx29ndpx5I6G5JRAYO0Y443WhyNMpbjzr7QD3Rgo8a45lJ4Si8LOrgdeHe\nVuI3cPCm8JWT3zqhbE2Qbr0W7TbwTFPqIVtHAiXeriGU6QWgJkNThkyYtKYrOMaEryAv0exMAt8r\n9hYLbbrWta517f62uxKpW5sC8u0ltM5TJOjFgNQswwh7fGR2EUTRns9SshRAakbDhTZBEEZdwOAc\nX3t7C06DomW7oKPG5f5BU4fPXH8CSNIMvb2niOuP0XZ3LYbYMEV81msZNF6mJYFlAo0JisjNgQYy\nX6djbxw0VUTZM1JCqUTb222GfnbU4NeIDljdBmRucKXjuA+jxJHI9gY203R9Bw/OYLVOHPg/v3oU\n3nWmEu4roTFF4zJyaAWHe2l1stGmfWcrPVio02pjczoH5Fi9sA1M7KMubHN9OSRO0fEag75SNZzo\nX4fFbemW6hkk55jXO8k67HXAYckFcTwLBDBHRSilS98A8mfoextHfLT76LtD2zdQaRAU40Pg+SVa\nkWzW4mjMU7VskLzV2gIOrw6GvilQeIwTr+cFHFbX1FuhdMTA8RZWBI1bYn4Ta0eYrykAyVz7Zq+G\n21S339fmr6wqumJURbDie2GDh2gUHok+nYiglx6hEkbL66Nt426nqpjVWkoawBQ+nKCiVIS66VsV\nG3GbtnTRatHA6r7ZkXhV9xzpf7q1nV60hd3WphqxLe3topICwchR45BgTCJNMiBgi4CuKeEx899f\nWcW9aHfFqQNAYzYNi2EJrSWxeZBhhoEaSrP0o5WWj97HaOCWrvcjvsiMl6SEscFFL6txJLcT1FLd\nSCBxnpxtwFdv9Xt49AFisLQ9Azpzqb2eNnCKnKfUw/29mISZZKd+JoX1Rxm81yWMOF3jWLaEkQyd\n88JlLlRqC7iD9LCtdQ2b++lrWl2Dl+KXdc2GTNMxNhoJFC4TOd8YqauuTpYUSLKsgK75cPnFf216\nHACQSTXw0qHPAgDeJz+IxTI399BjuHmFVAqN3gbaRwhOgqtDMtf+xvHtqsNTT6aOyiR7Wcbi3QTQ\n5GIvraHBZ0wdcSB+PSgykig+TTOqvhBD9ga97MteL8weWo6eu7gdP/kENed9aWUS7hDdg9PgLlKp\nlnrxWlkLBneUagwIJeUrPKC2jWEZ31Y6NM2hpJocfBPY+Vkat/IODUbz3sQ4v1fmN5u4ysD4pCkU\nLJDWyLEDVGCU1AJOduf3A+2Xpq+FnHVof6dMAKkhumrfaJFRlH1yO854tAdp1ALJ3DY09fe0Fu23\nGkInuujsRRrF19W4RBgyqucptI4m1IF8gB7pfORHlBkdCcW8q0tPdT4CgLMMm96LhUdAF37pWte6\n1rX7yu5KpN7ukdAbQmWjjbqAz8nO3HgD+hRF6rURDWtvUNIw+2ARjQ2qrnRyPvSbnN1e1lHzKFrN\nXtdQ2cXRXT8zZWoG3rhAsI2IeYhxFD4+tI5Zjdf383HEuOcpNIHWEkX7fVM+GqNcGXdFR/0d9N1z\nU6NIsgB7vI8yi/9s36v4w795LwAgeWQdoxzJF2oprHCrOpHyELtJEEVheRAaT6maJlXlamMmjXc8\nQSpwGaOFFi8h9o0Qf3wwVsFXOJGbMlsYy1JUf6U3i/R1Xs4WUkg/Fi4Ny8dpReBkfCWutb5uI8nK\ni7WdrJyXkbC4iYjUpOKp24c2UdZojLWmBo0rcfWWUMqZZkmHZL37vm2beGNjBwBgYSGP/AAnrccI\nSpou5bG+yfDQURfxWe7zOuRj7AWuI9AEcpd4yRuntoUAUBsyUB8MEqgSvkFjUd0G9J3DW87+bJNU\n8f5N/2tqmy+lUhhMar6K0E0RqjS2paaaZNB3bi39j/YQVXrmEV3yaHQe/BtgeCaivBhs96TewVP3\nt1Suaujseaq+B9HBe48eI7p/sMKIygcEx/alVFx8K8LCIeGu8HOYbEaHuqUpeLUpPfzF5iP8h3tz\nZXhXnHriYBGlUgLGFXIOA88sYP4UMSPWXx1Ca5yHNutAbtAPvjSdg8kgl4x5KD5AD7x3zxpaGwF+\nHIPGjsit0q3F8k00N+g8T0zexNkvEC6y3shADNNDsUoC9RFejrUFsozpb270wqZaIZT3etCZWWPP\nWXBYY6b/UXK2zxf2q6KYRwbncL1MjnQsvYlyL52/uZxUY+AMOECbFRHbBoRNL+TAtg2kDJo8rpQH\noKtSbZ70zDr+YP4ZAOTg395D0NLGngRWMiQ7kLxiKWVKaECc5W3T0wIBUrh+WCpaqF7msVoPJ9r6\nqIQ+RFBNZT2JHqYLlneGTS8mn74Zwk+uwADLBw8kq9ibpnFxPB2rFbrvAZtket/Y2IHhPrqohXoe\nTcblZdLF/DN0fbGCruBXowEU3k7/yJ03wgbgO12460G3KQmr/P1tBHwv2BdvkIrob/a/rvpoNqUP\nUwROWqCptFI65XYDizaKaEqh4JaoVkrYbUhTjtTcoroY1VmJRRxs4ISjnY9uZ77sLFSKUh2D7VRk\nFFIqAwvYNsF3t8I8GqRy5uaWMQiondHOUElNoK3yDBK+ugcdX5khHzKCi9/2Xu6mdeGXrnWta127\nj+yuROqbqymYSQfNPQRhLLwxAs7lwE1JGAH32Tch8xROJjJNNGoUHYuSBXud5qPihT5ghI7jJiXs\nbRQtyhmK3rXpNMw0zbjfOrMb1sP099p6DFaRIg7hEpQAANbecpgE3ZZB5hJFAINPrmB+jSJh4Qt4\newh2WVggCMdYM+GxlvvzZw7iyN5pAMBsuQfDOTre1HocvsHzqCeQG6Hto9mSWopeujaKk/w5H6/j\n0iXSRU8OUXi6kshgPElFS1/9+sP4hkmR2jvffgHlb1IxkZORiO9jUbLlNPx1esxOSqC8j6KfkV2r\nWC9Sf9MgCVl7oAWwHIGMe5At+t5zDx/Hl3IP0PdSdcwvE5x0+cQOPP4Edaa4sjaAtUtcKGb3YmqE\npAnyybpSg/zimYfofBsmCvMM4ehh5D+4dwOrDLdJPRRlayYkMlfoWnLXHVTG+PM5E01ekGRuAPWB\nu5b3v2smzxIshifCJhmmEB3NMAIYISagFBtjwlct7GIiFPoi8awwuQh0FiR5EEjzEs+RmuKgd7S5\niyRJE8JVx6n4VgjXyJChEkTcpvBVMVHFt1QSNibc26otAlDJz2ZkpRDlsgdsng4N9Q5RszBy1wGV\nHG1HICwq1GICASTc0zncy3ZXfgXpSxbqR11Ih3+1Agq/TS5IlN7O+h+n4si+TJe4sS8LLcc4WVkg\nf4mz+2kNazFuyBD3IU7SS+5z44f6uIPcEC37Nxcz8OYIL0fKh7udJ4OEDWuTrqW2nMT0McL0Ux5Q\nmeCCHteAZfEL1OMj+yodp8x0wHhBoJKhe8gMVzC9Sc6+WothzUmH98mTh17RUU2RY5uVAj+x8yQA\n4IOD5/CfXqPq0vVYCg8coCKeQIJ3qZ6BnWKq13gNmEmq7QHNM7YOVAx68fY8MoerIGir75iO5DT9\nUNbWB9Ea42KqJsvaLlvwxuggiXNxjL6XGoaeKY4ixz1f5xbzMFd4cnWAN96gBhx+zMdzzxCu++mX\nnkCai5zml/JIXCbc2+DnZ5UFcte56fgRgaD2ZGEhDwyTw4jNWQrOEpKKxQDC1Kvb6bNvSMRXaTwH\nX1rD5V/MA3+Mt5SNfJNm5NbPu0qfJK1ZqPj0bH2EkIsuBJpcBekjov0ScXIaQmceOMyaNFTQsVXL\nRbFIRLSAyb1tgVBaayvopiZNmAhxdwBoRypRtahjjpyzKUOXtRXOUZLAEYgm+F5NGhGMPqQuOjKE\nK5oQaruPsBpXh1CYugEdI6/cm0VHgXXhl651rWtdu4/sjiJ1IUQOwH8GcBCUSvtZAFcAfBLAOIBp\nAM9JKYt3crzamA/jRhxWwK54bAObGxRxJpYs2FeoJF1qwPoDvARblaptXWLVR32Ao4kVHzYzNprD\nrlqy2xuBiqOGeoHgAmtPDU6Cbtkwfbh1LhzSJZwUzdB9x3U0WNvdiwN6gw5YKGShsZ4LDImnTtAH\n9AAAIABJREFUP0ItrT5/8ggA4OiHL+DFyxS1VkpxxbL5xKOfxK+d/TG67t426jfo4HpdwGWe/uPD\ns0qH5Ud7TyF+kyLhxqgGY5TO2eDCjkd6Z1FoUeTvTyfRd5que3luBxy6TbR6gNgaHXv+a9uReISS\nkuuH02q73hDoGyL4ZzBFK5kL18ZC7nK/j/cPUTOO3z32LDTWjUfcB8YJCtLPpyB30+fY2RQ+myV4\nZeKBRUxdJWin7w1dadIIZvgYNcD7Gepnqh8bgEWXAadsqeRt/oqrZAJaaU0pWtZGBFqjNLaxWUsl\nU28+1499n1gCKd7cub3Z7/b328wXzwAAzjkJPGIFLeQ8JJhXTclTLtCKFB+1ZBihU3QeRrHJSEMK\nAEgLF/WgFCei9xITnmqkEU2aRr8b5atrEQ31WKQ031GJ11uZN1stoTlq1VDxrZDPLrVbErfR85sR\nQCraDKMuw6RqlLMOGRZ0+VIq+OWS48N44fRtr+1esTuFX34XwFeklD8uhLAAJAD8HwD+Vkr520KI\nXwfw6wB+7U4OtvuhOVw/uQ3+LtYkKaQVl8iLC3g2P1ApkL3BTq1XUxKtzZyGZIHhl5QGs8I3c7iK\ndz9yDQDw1a8S7cishA0eJgfWUGoR5GHpHuZPsD6KIVX3HfzjddSnmYLYFvCz/PK1NOwbp2YT6/kE\nCk1yrLkBOvnl4gByecLr45ajeo5+/Mb7UV8gfH/80CwujjKNMuNC52rZimuj3Kbr+v2ZZ9DqoXtO\nzBg4YxG7ZHSEcPTX13bgp7d9CwDwjcx+tLLcr7MH6H8HVZTOXx6E0xPo0wKZFwlO8nuAxjbymvaS\nCcHLb4ureYykA/MCwUpP/egp/PdpUtpK52vYt4doQNfW+5V+TAEp2Cfp3tw44C/SZDxVtAGuGG3n\nDNSHA9ojXVLt8SbkIsFDMQn0n6bjNfotFPfSD6k6rKPFFEnfAlJzvFxOhXBRc9BFP/k0bJoG5j40\nDPwHfLf2pr7b32+TLj27/+3MP8HJx/4bAECDgaoMIQJVdRr53tYlelQfxrmNP9XU30Pn6EXojWak\nSQa2QCeBRXFtR+rKiUeLlgKjCYOuOOrIo9dgira6Lg8CiWAykrcWP0WrZqP3GBOhKJgDIM2OvAZf\n5ShiWugm/+nJn8GYf+HWAbqH7DvCL0KILIB3AvgvACClbEspNwH8KEIE848B/KPv1UV2rWvfC+u+\n2127H+1OIvUJAKsA/qsQ4iEAJwD8CwCDUsol3mcZwOCdnnTub3ZA5CTcCs2RelWHvcZLHTNMJsYe\nX0dZ9qrvBfK8ZgUo7qForf+0A7NO311YS+JscpRurBYWqAST/EYjgRWOEOPTFmwOwhtDUqku1r/Z\nBzlB0azW0iFqXIyT8HB1maCTgVwVo3Fil7w2S5BLSQO0BsMFExWM9FJYGjMcTOynYao5Fg4fJl75\npZUhDGYpyn9H7ga+tEwt5crNGMwKy9ampIJi3CG+x9le/J+rH6ALF8DmQYpa9hyYx9QKUUFk0oUI\npH+vxlQA5expIHWaounaNg8bl2lsN4YJ+vKaBvx++t6l4hDSNkV7PzvxKj7+0gf5WWlojdOKZPTd\nc7g+RTCLaGgKXknOGpAc3TR7w1VQc4AjLNsFZumc9iZQOEKrlFavRLuHHkrumqZYOW5MIL5G3914\nSCK+yOyXaz5anJxu9kq43307uzf93b5blvjLLMA9ast+UyVNdQil5AiEUbsu0BGhBmhHNHEYZf2r\nVnAyTKRqESaKI7WOqDnKVomyWwLYpR2RGAgsKs3bjETyBIuEZf+64tTrHVBQwHTRhVSfrUihVBi9\nS5UENYVAUwbHDi2nGVsakLAEw2fTuNftTpy6AeBhAL8kpTwmhPhd0HJUmZRSCiFuC4IJIT4G4Dej\n2xpjHpBykD3BRTm9RMMDyMH2XODqymO9YDlkmDWoxtN6UwL8Y575EJA7w3rNsTbmz5GTCRAcoy7Q\n3EXeYWU2D7Czcw9W4bAWeHzRQO+L3LC6R6I+Tt/1TQlk6CUcGSpig4toFq/14/Mn6Xce30uAcLNh\nwfcZC6/EIDLk+Czdw0CcnPd0uRenbhB1I3nZxtLDdA+/v/E0xA06tt4QcLgYJ7GjjGqBtpttngDL\nOpJMs2z2SvVjvDI9jEO7qGLz8jcnYPAEo7lQ/Ur7/tpG4XEaUKOiYeQR8ltLx0gzRgfQZkbM3Ewf\nzA16PW68dw5mLmAKGaqfa3+simluvG2WBPreyfCPMYDYMlcA2lCcxeQ8V/RdSMLjX1Vs3YfH4tbC\nE5DMMqgNCWSnaezr/TqqIyzDWpNILPOPuifUiuk9L2E0gRkAW97Ffyel/Bhub2/6u323rOfPT+CF\n36T3+em4j6ZkhhQ0tPmzJUIHr4Noe4EphgxCaMKM4NpROCWqoRLYVr0XBZeIkLFClaFc6CZc6GIL\n+yXi6GPCjTBe9I5K162668G2kPHidVSN0vFC2qYOqOIsHQJWUEyOEEePCnfpMPACi9XlPnnyrtaR\n3sm7fSfsl3kA81LKY/zvz4B+CCtCiGE+0TCAwu2+LKX8mJRSBP99NzfQta79fSz6vv0dDh3ovttd\n+wGzO3m3v2OkLqVcFkLMCSH2SimvAHgPgIv8308D+G3+/+fv9MLsVR0tALH30W+lcbJfqRQmpiyY\ndU6OamEkZpUkPJ5Sm/0CI69QklV7dhXxPfTd6+t9qGXollKnad+1oxKaxapzmoSxSJxp1/Ax+ad0\n8OlfaKP5OBUTra2mEU9TZN++mYbXDET9JRIx2p7e2VSFE88MU/HN5z7zJHqeWqZjHB/E8jTBQIuG\nxAPvvA4AmJvrRXyGonm7KFHjHqkAsONRjnLPDuHRR+mYVcfGhSUuovoaJW+NfsDl1oheTKJn34a6\n7qC3qbm3jPY1InZbrlDwx8qTPowM3bOsx7H8LUoUB2OstwBnO91XdrCCUotC/FcLE5DMhxejTTTX\nacl05uR+CJbnbeck5uYIzkmNVlDjfqmxRBvudVqytiOrMYM7R5V3S8RWKLbI3vBRo7wwKofbqA/R\nWA2c8LHxTtpubegQzLV2EwKlfaztkfCgVXXgL3DH9r14t++WSaeN//WLPwcAuPjc73f8La/RONal\no7ZRRBr2MQ2YMLaA6v4TxMbRRhtRProDLdJ4wleJ0Jo0OmQCEpFipZzW4mMLFc0H0rtORA4gGvVv\nZdZEmTGhqmN4b54UqohIFUTJsD9rFI6qyFB6VweQ4Ei9Lh2lzGgLU43tpBNq7Nyrdqfsl18C8KfM\nDpgC8BFQlP8pIcTPgVa9z93pSXsu+dh0dGywPoqQQAB8SwHVCk1qQGOQH0pSwCb/hXYWaOVpwDe/\nvB21I+TgZdGCzt2JVp/g7iQtgf4egj+Wl3rgM70ucSmG6R/hF8htoVgm1odm+nh4hGCMVxf24ZnD\npO/w2sIOHB2hQqAzK6OolMixfeb0OwAAlgclPiZNoDVGL6++YuHaOtMYi6YqtHHjAiZXeqYe2EDM\nCF/K1QY58tVqUsnilvYzU6CoweeqWDmfRPk0OVJTB26sU/Wp5gqMHSWmTuXPR1AhPTPYBR3aAt2n\nOFxCfYUctcYaNFpbwOAJsHkqDzlIy+zhZBnVZYK1/LU4PJ5UNBdqMjbiLnb0UZ5B13w8vOMSAOAv\nXn4cMsdt7pjCOfyiQHE3HSO+qKuK0nZaKIpmaacN8SBDWzfT2PZVOkZxL1QLu/4zLYB11oWnobwv\npMl9F/amvtt30/b9Dr23Kz/WQh87cgdepNJUg8MytyXfU86MKicDWl/ozKNFSVExrKDDkS/DBs/R\nQqRkpAI0IdxQwhfowN23WhRyuQXKURBJqCvT3qIj01TQTYivB9+LiXDiakmJtBZg8QI1DhJimlAT\nny001bpu1q2qsf17vWHfZ7sjpy6lPA3gkdv86T1v7uV0rWvfX+u+21273+yuyAQsPeshf1zAmqIZ\nsvA4YC9S5C0kkFziQpNhAWuTC5RKEiXqAQ2zIrDwNM3SiUWg92sUOnoWUB+mCHroSWoIvfzyKNaY\nM24tmHDyFE20chJuhpOGho/4cYpga9t9vGFSMtOsCpxeJYji0NAS9iVJefDl5X348cfeAAB8buUJ\nAEB9xMPTj1FU/83pCejM7jAaAvVpli7IuZAsNdnql5AWF4W0TVy5QnBN7qaG6SGKvv2yiZ4xYtH0\nJGg1Uqik8A/HqSjoi8ZB1KscqeoSmRTtU1zJYOYS67rsBdI3adwqE0D6YSr6qb3WB5MLrlxu4mGu\nafCmOJJ3AaNC17pcy6DyEEsZuwKJKZYJ8AEzwSsMIVFr0/a1lQx6Y1SUlN5Rgv8KQUfak1S/s/Zg\nDm2O8JM3TST4ea8+7UBjxcj0DaBU5L6oKYEV7o6UmZKqGcbCO2117b4t0f+aDhI2eGuaO0fR5NNf\n/igu/8M/pI1SV+qNQCgtG41xNVDEClCB0u04RAHjZGt0HFhSuOpvW7npAftFh+zoR6r45pEzRpta\nRBtdOJErDs6jC6mSuc1I4wtPCnW9gRSCjxB+8bfcfxi160r3Ro/cw9Nf/ij2zL1+2/u+F+2uOPVY\nrolmb1pRDVMzQn32bKDJTZvjaxLNPFemNQA3QQM++o02Vo+QM7MqEtXRsEgloMEtv0xO0k1KVWQD\njSAIAGhPNgDuYOIVbTT7aJ+BvatYvklONbanisP9BGNc3hzAfIUFveIuPneZqieDiUGvaojr7OCm\nkzCrAf7vI7HI8IajqUIc4Qh4QYHOTAqjrwYwU8hoiQ/UUVzkRtksVvXg4CLKTAMaylSw9BpdU+NQ\nA6Upcp6j+wpYukgVqloLqNG8BGtToP4q0R7bPRJWmZflrGXfPNBA7CIdW3+siGaZPq+Vk5BuAEhK\n1MfpPode0FHlMRS6xMZm0AsPmOOxKhdSAYEI7ZNc8mpLZC5yYUnBx+ZunqCvWQqKsSoSgmGh2JpU\n0Ft9SMBJ8fisUN4FIKcevDdvdTvwsRmcei+N3VE7FKMCsAVyIXMiLBggpDo2O0S02EQo8KUL2aG9\nEsXRAyPdmKAjU/u2FZ6Bo09rTgTfDo/tb9WYkeF1BdaxPVJoFDTXTkdII0mhwQkKkSLOuxmpxNWF\nwOk2vbj7f3O6g955r1tX+6VrXeta1+4juyuReqtmwUhL1HdxkY/lIXOMI8QWYNZoFs3MtLA5SRF5\neRcQZ5bEzec0DL4YNhxW/SsHPdhrHH3HOeEy1ILcpGOYu2poMXMjfimO+i5mghg+tElivzTbJnKj\nlKArzWVxLkEc7lI1jnaFYYeGjvEDFMFfr3DxjSvwlUsHAACJooB8jGATMZNGY5A7tbQFMEoQidcw\nkOqhc1bdJBbeQxFD6qaAFaMIwTQ89IwTXPLhbaTi+NfLB3GzTFIDE5kNzHAvUs3XkBincy5fGICf\n4EiortN5AbQeaCBxksn+mkRjlOKP0a/R3xf3CrR6eQm7nMZTD10GABybHYeo0asi0y60Oo3xxgGB\ndJbuZ3//iorOF6f6sHGSVgqWDOsLRl8iGk553EZ5grYlCqQqCQD1YamUGc2aj56zvMJxJVymZNQm\nHPQep2tpp6GStkZVC6Ue3uLmLq/g5//olwAAp3/lD5AQ9N768KFzzFmXnopSNdEZrQcc7kSEORKV\n041K39q34Y9HuyMlI9K7UbVFH+E+iQjvXb9NScAtmi6RBVkzEs0HRonVTpVGXYhIUZXs+Bzce0LT\nVaLUhIaP/MGvAgCGV1695ZruZetG6l3rWte6dh+ZkPLWmfF7ekIh5MGP/g6avRKJRcbLY1Dt5Abe\nAEo7aa5p5ySSCxxNtCV85qnLZ4qQL3G/0jQQCLW1+kL8OqC9ZW/4KI+zSM+Ei57TjKlnBRpDQbd6\nwAuw8YSLiaE1db1TZwib99OeKr2HkBAsxqUbTDU8k6JKWQDmpqZyBM5wG1YipCsGw72tbxMLG4SX\nu44B+zyHswJKgCz/cAGrF4gO+YF3nQAAfGN+EhVWtDRiLnYPE9d/ej0P7zLzwYcc9LDQWHEtDWON\ncELNAdojNFjxKVtFtsE4+LZU7QAx3ILJ+vHetZS6JqskVOTtpT3YeYrUIxAttFNp1aLOXtfgcpOS\nHtZBsqo+rDIdu/CwDXuDE7ZJAZ15Z74hoHFpY21UIM7lP/UhiRQxSzH4wgoK7yIaaW2Yahou/dZH\ncbcKgYQQ8lnx43fj1Lda0KP0xT78yc6/AgDVkg0g/FhXkbpAS3b27YxayQ8j22gSNdrTs0PpMZKo\nNCHV9mhbupjwbukZ2paairijFEk/0p4uJvyOawgx+tCP+ZHtMXUdoWU1Cy0ZUYnk79pCU/mCj0x9\nCI138Uv3ffaR386+Jj9zR+/2XYFfPJv0XawqDdbmKJC7zA8+DyXFKqRQCUyzKlBn55P5Wo/6wftm\n2GTBt6Titbt95Ejr2zWINj+0FQO1Uc7iDzqIs0NqzaWQuUCPvfyQj9k1njBW47A44ekPt2Gf4gKc\ntxfVS1u5RpBDc9BH5jIvPy2oZKdvmRjfTqyZq1dGILgxiDmwjp39hDtcmh5GnZs/x6dNyJ0Eyywv\n9gDcTekrf0OsO70lkD5MLBLnZA8uVWnSsZcNtEd58pAEI/Eggus9IE0gc5Zmu/qgRM8VusjqJC+h\nBaBV6JWwEy2lxriQjyM+z9xkExD8kj+0fwZTRVadBFCvERbiD3lKB8ZLSLjJYDLk2gFfQmvROas7\nXQSvYc9VF6nrBCEVnsiroijNQeQZk8MHgOqBPlWQ5mR8pM93E6XK+Bk1fzaF179Kz+WIXVOOXIdQ\nTI+m76tEYDLCzy5xow1bABVu0hLtmATIDiZKYFtZKYHTjgmvs/GF0nMh87f0JQ0SqJqQSGvB9vAZ\nJ4RExQ+To9EORtFm0nS+oDsvFRZFpYnNiM8+2ebA6OcS94wz/26tC790rWtd69p9ZHclUo8XJKQG\nVLbxEmkN2ORy79iahiYrBWauCchgXS+hkn/CE2hnaXtmxldd5FvTOpbfRZFt3ys0E7czAtUdvLyb\naAJFShppdR3tJO1jVMNlf2zGhsXl++52Hx7tjsd3zODVwj7ax9WR5PZudYYrpAFUdnJypiHw7mdJ\nSP+Frx/GtcsUTUMLuemakLh8nmrizaqGHY8Rx/iGOQBZo+vKnLNgbzIEMRJQ94DBNCVHbwxkkD1H\n+1Z2+iqBlB8oo36cqIuWIeEyHz1W0FB/lFYB/V+IYfFZjs842rFXdLQGaJs7n8bIAVoyWeu60jNf\ne8yHZOjp0ss74e6gaP4jD30Ln56ihiG1JRupWS63HpKIrVCMlL1O3PWZDySQnonzs/QVVFYZNdDK\nUuTfe66KVh8Lrq0DrZzO9wm0WWd9ZVSH3EVjkXo1Ferwd02Zd/0mfuPXfx4A8KXf+YR6RxKaqRQb\nfeGjLgNNc6l47UE5fdOXSGoBBzyENByJDuGsrQJfdIwwgvZkZ+QcUBBv11AjITw0I5BLVP88iMJb\nErdE+8F1qQRp5HxBAtgUmoKiHOkrES8A+Le//s8AAKnrx/CDanfFqbsxgeoOCZt7yRh1iXiB5Wbj\nUE6mPixgU+U58hfb8LgXafHRtjqWWTGxuYuXUhkJa5Vuaf0heqh9JwEnxRj9gIQxTI7FaRvwyow1\nT9axuY1L9s/aqG6jBy5NCWs7YdMnF8cU+6aRtdHkoh+NWTZysAWfOynJXg9XS8T+8A0JMMdb72sj\ngC5/bOikkinxpcBkmnD89M4mTl0kakh5nwuL2TwOO8+DOxZx7gpNBpojUHsbOWl/01IAZ+VCLwSv\nKWMHN1GtkHN0RzyImwQhtbLAyNe4X+lDdH1ifxWo0H2lrlq4GidmjzHRwAazVXQAiQThOdmJJhIm\nPYs/ufwoXJeO17NvAxs6OWetLRQ7af7dzGOXEsklchxS6ApKawwK1Lj/aDuVhsa/3sq76kh+k74b\nWwkZL9qeKvYPkt7O6cmdSCx0Srl2jSz1aXJQT07+K5z8xd9V2wPH1pSeUmwkBUP6e+DqzCiqJcJC\nJUAqZ6sBHTi6HnHkgUV55WZEQjeYDHJaiHM3peiYMG4HKdiCSv6BUGUSIO2aAE5SOi9SKujJkT5i\nLKNgCh0Gu/5Df/SL2PbpHyymy+2sC790rWtd69p9ZHclUnfSQPY6FORRHxAwaBUNNwakb/IyqS6R\nnqNIcOGdNloj3Gl+2lJsDOEDFrezS8+FMEXA8lh9m46+Y0EPUwv/4b2fBAD8i1d+EmAoREwlEGP9\n8eZAyIPVaxoaNS7DFxKxo8w9b1jwWb3RS1NMkM/WUFqh6NTuraPHpgh6YawOf5Wghv58GasbJBnw\nu1feDVOn725uJjEb52rQnhK0FN2nbnjYtY8i+KAN3970Cq7PkEJXqy+MZJKzBmrbKdKJFQQqe+kY\nXt2GbvDK42YSnkXjtnHEV/evs256ez0Oo8Qwx4E2zKSj7m0yFzKCvnmWGoO4/RqKGt1bu5CAxv1c\n16omRA/zfa/ZaLOSY/4C/b88oaG4h87Ze6GNynZaMfkGkCWBSpT2SDjcMAMlG4kVGqvkMlAa58Yl\nuo/TNxnCKmuKQdW129vYb72KA/3EXz/33O+pxg+mCHtwmkIoBkgwmpYQCqqxIk0lTED9VkyElaZA\nZ0s8PxLNR9kyQUQZ44hcQ6eIWGAVaSgNd0dGue6hOTJUl3QAJDhCD/aJRSCWmOhc0e351C8AACb/\nrx/8KB24W/BLUqIlBbhnLca+XkV5J2mO9J1rYWM/OTDhAcXd3PknIWGtcDedERew6SVsVGzFlinu\nA6RGD3z4q+Qolp+UKB7kl3BDw2fWiEXy7972eXyuQBjwhcVJ+OzsxEQNGkMUvh1K9ZolgfokN8hd\nMeHn2cnc5Gu62QfJuYCY5eDsHCkm+q5Aehtd4MH8Mi7xkrNwahBPPnsKAPCKNxGOjR++fCP5Mq69\nsQMA4MXo2J/dyKjJRS6lYMfIedbGXeycJCiicHMM9jLdf8vyMThMOFdhLoF+niSEkGg5dO2bdWLw\naE0N448Qtl+opFCZpwlI5KpYa9KYVNo2duwkqpepe7hxgTQIktsqaEzR/vAFwBoujR0OYvN0LYGc\nQ2PYgzQDGqMFL0af4yuqZgRSAMLlsUg5WHwffTbWTJgcAMQMF40NZiv0ecBtHELXOm3yoyQd+6D/\nyzj7E78HgOCIhMaaRNJX2HPbDwp4QtMQkRGQITRTkULprLRkp84K1P4iQmkEuOVwhzMO3n4tAuHk\nhasmCQ8h9q5F1BbbUnZALdHrpe9JhZ1r0NQk9tCn/qUak/vFuvBL17rWta7dR3ZXInWpA5lpH7E1\nijIrOxKqi3wrG1OMF6vqQWMNbr0tkFjmhJ5nwItT/OAmJawSZ8/jEmaFPudOrgIAyjsGMfYPZgAA\n1xYGUGhQZHfSGsfpcwRjxJoCJqElKFctgJf98TlT9fds7G9ixxCpSs3WBjG0gzjm1SkqfvFsQAbQ\nxloa5gpLCgCoc9HSy199UPVOlb0S31ygCD0Ta2FhieCX7blNyBI30hh28SPvoSTXX32J1CCdHoHW\ndYqINV2ieYM+6wCml0mIzHikil0DFJFfPrcNzT56zDuPzqHcppXHWjGtEp6CE7mHjtzE5W/sonFN\nSNjM0a+PWdis0kqqP1PF4joVTQlNqnvWXsxBsFhZbNFQvHLh64gxcpOZpXFt5XU4ffy5x4dd5CYJ\nSaB8lK4pdjUGj04J3fShz/CKqSoU775yMQ+Z5qV70oF9lauiuvYdbde/eg2Prf5LAMDXf/E/IiWC\nhi0tmAh0yQOGSBgFRz/rkBF4I0yamiKM7nVQFB/sE7UgogwidlugQwJAcc1FuCIwI8lZ2ieI/EVE\nNz48SJTZEpgPH4//4UcBAJO/dX9ALlG7K0595CUH8+82MfoiDXhlm6aW3b4pkFihf8SXmyjvivP2\nEIPXm0I1XEjPSLSDVX/GhT9MWPrmEarEbOUlrlwjiECr6aj208v7+TOHVb9S39ZQ2U3fM5ct+NuJ\nrnjwfVOYLZOzXVnOoRl0FhpsqM5HjcM0G4j5OCQ3tDBWLVXl6ial2tc8VIL/OkEd9rrAoQHqdtT0\nDKynCN64ttIPGaOl4dWpYVx1WGJxO3myVKqFJlhqOOPBYDzcmizDcRjnn03iqkdje+DBWVxeIBZL\nvWnj0TGa4FxPh2WQY6320rEvLg0i/hBBNcIx4F0nOcTG5Zx6dktaCt4A3ZxuhRWlkGnozbAQKHg+\nXkzCqNG1lCboWpMLQMXW1bMMYDhnbwP5F+jeig/4CqLx1m1o/Nv0bCiMPnMTiH2IJu/WXwyiPoSu\nfRc2+nFyaB+6+av4vY8TFHPYslGV9D4EDtGHD5s/t+B3YuoRCxxvFJahop9w/2jXIcWG4f9ZkYYV\nuoBqDu0gdPAOQpgn1nEs0dFfNCqdC1D3orNt+l398q/9MsY+df8588C68EvXuta1rt1Hdlci9cUn\nTbgZD+sHaa5vHqlDLlGENnDCx+Yu5nvrcTTznNxoSaQWKLIsHtDVsl94ukqcoa0hdZwi3qCP58Tn\n6lh+G2+LA8vnCC5Br4P3HzkHAHj+2j5ofP6dj83i+gkiS09n81idYw1wTWKVk3Km5WL1JB0niCDl\n9gYSNsFJu/avKy45BOCv0rG1YhI+66DEDmzi1RN76bumhM7RrBxsIdNLXPq9fQVcLFD4GeR+XFdX\nSVMIqTjgjUoMqPLjtEKtjsO5eRzOUfJzqtaHY7PjdH7bwa4ewkUe7afWEvviS5hvE4PnU5ePQG9x\n5L2nDvD4eElfKTYaN200x1iaoFcqdpJeMiDHiFefOhlXkXjpwVAKwSzRFTaH3HDJXTFRfpZWPtlk\nE8VlTtQ6mkqmujuaSJ7m1ZsOlF6g8dEyoZZ+1747S33qNfybUz8BAEj8v2X8l4kvAoBqfWdH2uCZ\nENBURC4VzBKNznOahpoMVBq1SLGSVFF+TAgVaXtR/nokwRpwzTVAnTOGEP6JNrUwocMFzgzXAAAg\nAElEQVRkVosjPbVPwPD5qekfQvlnaMWZunZ/JUa32t2hNGZ96A2NdT8AVEz07OauOOu9SC4wG2LN\nxerDXBQ0o2Huh+ihHX30Gm4UCT9uzfWhPsKFRts2kfgrenAb+/nWRALpuUDbRGD1SCA6BLyxQs7b\nK1tIrNHDv7Hcr2iK9Zf7obFsbmpGQ22UjtlKetj/NoIxrh4ndko83sYAV3r+8MBZnLtKTt3KtDDC\nkrjTUwMwinSM6lwG5gBBF+31GDSH39q5GOwH6TjLtQz29ZNuTK9Njv5vLu1X+2prYc9Tw3ahT3El\nbFKqn8mnLj0Md40c8sjuVewfouNdXBrE6yeoUahZoXv/sgZkD1GuIB5zUOlnhs/JBBrcB9bUfFUI\nBABOmvVudteROcYMmSNNGHN0zuqhFjQWFNMTTLl8vIwS94TtydRRvkoTpz/QhrdCDrtaT8DgmSl3\nBahu5/Epx5Xzrg9LGHXaXhv14ce7lMa/r3nXpgAAlaeAp36VJGd/7xf+bwDAQ1a1o8+px8yRpNBC\npypCposH2QGNBGYK0QHZNCM0ycCCz56UHdh4cOxoU4utMEtdMoQKHada9PL88z8gCufwJ74FyI07\nGIkffOvCL13rWte6dh/ZXZHe3fHf/j1iV2No7qEluliz4Cdp9s9eMJUWiG9AQStWRaIyzuwXF2iM\nhSXF5iYnCG0JnYuIgmh26HUHbY4mpQCqo5z8sYDEMt17aQ8w+gJBA7PvN2AxG0McKsOZIshl+1fb\nWDvICofDEgafx2FdlcTuTTw+TDDGmbUR/PEDfwwA+M/rT+JL1w8CANp1E2gxs6C3gVyKoIZt6U3F\nTz89vQ32DVY7NKQqiQ+i03afh0Q/Re2G7sM9xlGuDTQHaUzsVR0thkW0kqGS0PZ4BSM54szfmO+H\nbPBqRgtoCz4MZu0MHF5BkRkvrfkUDGbC5I8WUH+eoCezItHoZ4bMuAM9Ref3HQ1mnM4vp5JhApXH\nKn9gDfk43ftiOYNWywzHxw+1fgLJ4L6zUkkJbO7W1fvR7vEQXwpZUFIDbvzrX+1K775Jpg+S1MWl\n3xzHVz/4CQDAhBGLyAu4qPth0ZJKrHY03NDQjLTT6+Std+q2WEKohKwvZQcsE7XoeYLPKS2Ggke/\ni8e/9CvY/7FpAIC3Uviu7/tetTdVelcI8a8B/BTomZwD8BEACQCfBDAOYBrAc1LK4p0cT9YMNMZc\n6AXuyGJJxBboBxxf87FxgK6755KEzrK5le064oET3idh5mhCiL+WQnk/OZDEjImgEUvuOn3Y2GfC\nYM5UYtWHx6y31JzE2hHevqihuJcpiI5U4lXlAxoyN2j/dsZQ/TO9uIS9h5yjxz06K4UUvlYkwa/+\ngTJ++sJPq/v1mYkCV1NVl74v4Hr03fPLw4hZ7ARdDTEidKC0V8JgiMYJcPmUA12nn0Z5NQUxTPc5\nuHsNa2fpR2gcLMO/Sni00+8opy1PZzGVp0lKpjz0b2PIa5pwdJFw4bMoVsxw0b5J+9plgeTjhL+v\nnRuAzmSY2qiEl6PrFnUdzz1Gmu9/dvpRGKwzX896EHyfGKFnVrzQh9UcT0DLhqKtin4PPTvomirV\nODRuRp5cDLV+yjt0xAv8Tuhh1yurIpAo+LiBO7c3+72+3yxwiHt+oYBf2fY/AQAu/8oY/vBH/isA\n4D3xOkyWxHXgKWeuReiF0aIfAB379LD+StVv3fK9VsT9mxFmiyn0DiGyF5v0Mv7yF34G+z5BuaM9\nc6//QPUUfbPtO8IvQohxAP8cwFEp5UEQ9fQnAPw6gL+VUu4G8Lf876517QfCuu911+5X+47wixAi\nD+A1AE8AKAP4HIDfA/D7AN4lpVwSQgwD+IaUcu93PKEQct9v/A7qY66aUvSqhp6LNEMXH5CqQGfs\n6y1Ux2g2b314ExVOqEFIaFwwk5wXaPHm7A0fxX0cIbBkrr6zCu1MWp0/0InRmxKNwUiRAsM8Rl2q\naL82JtTqoDwpkdlDAVtxMav0ZMqTtG972EE6T8u/yloSBicF/eUY9GGKto0LSUz+ECWkWq4Bm3ni\n566NhdOrK2CmKTJ1SraCltwURS5GRYNdpOuOFyTKE1yoVQYquxiSsnygzayhpqaKe6QA2jk+Tk2o\nMQyKg9pZqB6l8AWCpYm9rqGd42jfkOi5QN8rTQLOILNfHA1mliKudKoBJ4jOX+pBdZwHNChCWdOU\nBo2T9VWlSnxeV8VewodqkmHUJJIFuq6VxzS4XHAkE65q+tHKESd+6n+/M/jlzX6v+Zj3Ffzy7UyY\n9OPafO5hlD9EP5zfP/JneFcs7PDVCJKWQlcl+VFrSk81qgjgHA+yI5IPTIeAzfueavv42VM/AwBI\n/WUauU9S717phKu5+9XeNPhFSrkhhPhPAGYBNAA8L6V8XggxKKVc4t2WAQze6cUJD0DMR+oyQx4u\n4AeFJkkfRo1+5fVBS1WXui/n0bfMP+ynPKBC+6TnPOQv0UtTGzbRd4b2WX2OmSVLSYCx+8zxGByq\np4FVCtvgaU742dcFPN7HNySq4zwOOhCMp17VsPYkQz436B7ajkCNJW6NDRP2dd7+UA3ZNF1L8YDA\n3CYtFxstE60NwoJivQ3ox2ni0d5WhMc4uTviwR0hRylZ1jd9cB0bqwSt1A95kIxBt3wBeIESmaT/\nAGR2baJ+njs5ZXxoTFM0GkLdc8AestcF7PVwAmj10vaep5exMM367Ks6mr10jNScRJV/bG7Sh5gi\nDL4qEwr3ltt8RT+Nz3NuQ+PuUADiSzpahwhfr1sm8txU2rOEuq5UHVh4movNpgVq3PlI1Cw1AbfG\n2njXA1dAU+Z3tu/Fe/1WscCBZv/0NWT/lLb9R+MI/v3TDwEAFp+0IQ4RPPmPdp3F+7JnAQBvs70O\nBx5YQEU0ARxnOPMLpYfxheuHaIdzaYx8kwuiXjyDUfdCeC3fg/v7Qbc7gV92AfgVABMARgAkhRD/\nc3QfSeH+bcdXCPExIYQM/nsTrrlrXfs7Lfq+CSE+9m32+R96r/kY3Xe7a99Xu5N3+04SpY8AeFVK\nucoH/UsAbwewIoQYjixTb5tmllJ+DIA6uRBC1va1AE+o5sztXgmXpdri8wZMhkiE72OdJn/kLkEV\nIqWuhXPR+gENfVRDBCchkL1OUZ/23ylqroxpaAzyEr0XSjckPddGs4+26y3A3uTk404NLje+0ByB\nQLc/viywaXMxTEyq5GMQkQJQTTJ2Hp1XDatjZ5NY38vFVK5AiXVTHnv4Gq7YlNis1GJo7uATLacB\n/twzUlLHHttBnzcaCTz7wCUAwFSlF1PXqfgmedOAy1opmhOW0rfm8gDfT3pbGbUbrNviAbUJDnOT\ndD6rGDaBTqz5WD1C47wwn4dg3q+3swk/RpFa/UIGKSL8oDaiQQZtUR2A82fQqxr0ZW5SwtcU6PMA\ngJuS0GZpxSJHm2j00UESKxJugu8hp8FkJc52GqpZSTsn0XySXpbU8TSOTVFkd4fsl/+h95rP8zFs\nebfv4Lz3pUnXhfG3lCjf/rfh9hPQcAKHAQBaLAatn1Z8MhFTFUWiTitpf2UVfrOpvrsd5249z/fk\n6n9w7M1iv1wB8G+FEAnQMvU9AI4DqAH4aQC/zf///J1eWOKqjcaQDydDj6g96ECPczutigm3yAUt\nto6ABFXaC2CMHLa3GoM9Qvi1OJuGz2VoA39yBtoQOcqlD3GnnDWg/xQdozqsI1mg80w9pyPFVIlY\n0Ue9nxxFckHCSXFBy5hE9hrt48YFek+yPGlewNfps8HSJ4llAzWWabnuDSO9wO3cRnzs2U6SuNW2\njcUCwS9v3NyB0X5q66RpPvQs3U8+Xsc8QzTFlQwGRwnHP396nM6zrYKTDk0YpXISyWl6hLW9bWgs\nd+vHfMT7aKwaqwlYG3St1eksxDD9aOq9upLHzZwMqZqS9U4bgzqCn1D2jAWfHbZbiMNN0ITZf8ZH\ndZQBcU3CGWQ8p6EjMRc2qk4tMCTGQMbACR9LT9F5EksaGgMM87wYQ5vmHFTfW0X8FEFSqQUJo0HH\nKO7R1cRjbwLeIu0z+GoJhcdZBOjO7E1/r7v2d5vfbMKfm7/bl3Hf251g6qeFEP8f6IX3AZwC8P8A\nSAH4lBDi5wDMAHjue3mhXevam2nd97pr96vdEU9dSvlxAB/fsrkFim6+a3NTEr1nBDa4eYVeMmAw\nJ9kAVOm3UYdK3LVzEm6TLlfvb8K9QdnMWAvInKHS9+YT++FbtH/6Jp2rPgysH+AEnQHoDvdDPCfQ\nc4WwmJVHbRVxCy9kzrhZFxsPcuLQkOg9HigLAj5Xyqt+mY5QKo258wZcTrbqdYG6wwU9iQoWWFtl\nZGxDqTduy5Rw44skeTv642dx7SxJDMTXNGwukdqkxp2easU4WnEaK69iqibd5rKptFrGvtHC1I/S\nBQhDqqIfmfCg8+rNjDvwLV4dzRNuk5oBSk/SQPS8EFPNRcp7ffRNUIl1pR6D/RpFxwsf9ND7LU3d\nZ8BEKT/YQp3UE5C5ZKDRF6G0ANjYr8OPEeSTnfbR7KVx3TgkofPqO/lKGtUnaLWRWImjso32GTze\nxtpDLE1clCgd4OKXWkat2O7U3uz3umtduxesKxPQta51rWv3kd0VQa/2sINGxUJmFxfqPZ9Hi6sU\n3ZRU+G1pnwdrg/nWDtDzOv2h+LDA0EOUvypc7sfUTxGYHV+RaAwx3W6GcdciYFY5vSKACnerdzI+\nNg8yLfIalOhXvV9DfYzbeJUN+KyI2HNGR5NL4j0bsAgOh8nVqkY95M6X9kS6oLcF5qYo2i7eHIb2\nIEXC5aatpIjKTVtVur704iEkC/SXyl4HGtM7gwyRZnsYyFPWcLHVg9RF7i+aDmmCTtKA1mb++qqG\nx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"text/plain": [ - "" + "" ] }, "metadata": {}, @@ -1083,19 +1081,11 @@ "metadata": {}, "output_type": "execute_result" }, - { - "name": "stderr", - "output_type": "stream", - "text": [ - "/usr/local/lib/python2.7/dist-packages/matplotlib/collections.py:590: FutureWarning: elementwise comparison failed; returning scalar instead, but in the future will perform elementwise comparison\n", - " if self._edgecolors == str('face'):\n" - ] - }, { "data": { - "image/png": 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T0BgIG1rgkS7gNEPzYRg5BV5cDg+/DYkaqJwMWWEQIuDIJpRpy9C51Sy97h7qx7eFdu3Q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\nclHkFUihhRAohR0VsOwWkGqg0A3bZEiIYuCmh5lmjmRIv4cvW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UQ9gffLu/CticR/rBt/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CSgttCq5LrehW2AN556pPoN9IfJE6xO+Hwf52Xhv2IE83rMITl0DH1AsYI+7H2D4GtnyIt64Z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\n79QTVKkQcEUOyqo42jzyGW06doTwCwnwa06cNMQGWXPh4hu8LzSjU1DsNXS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f4IwNxcCDBBQ9PrtKeqEFpeeTVHnX4DRG0sP2ME0UU8VWZNcO5OZtQhnsQ1et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"text/plain": [ - "" + "" ] }, "metadata": {}, @@ -1128,7 +1118,7 @@ "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython2", - "version": "2.7.10" + "version": "2.7.6" } }, "nbformat": 4, diff --git a/docs/source/pythonapi/examples/tally-arithmetic.ipynb b/docs/source/pythonapi/examples/tally-arithmetic.ipynb index 87cdc9b66..094842895 100644 --- a/docs/source/pythonapi/examples/tally-arithmetic.ipynb +++ b/docs/source/pythonapi/examples/tally-arithmetic.ipynb @@ -15,7 +15,16 @@ "metadata": { "collapsed": false }, - "outputs": [], + "outputs": [ + { + "name": "stdout", + "output_type": "stream", + "text": [ + "The autoreload extension is already loaded. To reload it, use:\n", + " %reload_ext autoreload\n" + ] + } + ], "source": [ "%load_ext autoreload\n", "%autoreload 2" @@ -33,13 +42,7 @@ "from IPython.display import Image\n", "import numpy as np\n", "\n", - "import openmc\n", - "from openmc.statepoint import StatePoint\n", - "from openmc.summary import Summary\n", - "from openmc.source import Source\n", - "from openmc.stats import Box\n", - "\n", - "%matplotlib inline" + "import openmc" ] }, { @@ -288,10 +291,12 @@ "settings_file.batches = batches\n", "settings_file.inactive = inactive\n", "settings_file.particles = particles\n", - "settings_file.output = {'tallies': True, 'summary': True}\n", - "source_bounds = [-0.63, -0.63, -0.63, 0.63, 0.63, 0.63]\n", - "settings_file.source = Source(space=Box(\n", - " source_bounds[:3], source_bounds[3:]))\n", + "settings_file.output = {'tallies': True}\n", + "\n", + "# Create an initial uniform spatial source distribution over fissionable zones\n", + "bounds = [-0.63, -0.63, -0.63, 0.63, 0.63, 0.63]\n", + "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n", + "settings_file.source = openmc.source.Source(space=uniform_dist)\n", "\n", "# Export to \"settings.xml\"\n", "settings_file.export_to_xml()" @@ -366,7 +371,7 @@ "outputs": [ { "data": { - "image/png": "iVBORw0KGgoAAAANSUhEUgAAAPoAAAD6AgMAAAD1grKuAAAABGdBTUEAALGPC/xhBQAAACBjSFJN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\nSwQkewAAAABJRU5ErkJggg==\n", + "image/png": "iVBORw0KGgoAAAANSUhEUgAAAPoAAAD6AgMAAAD1grKuAAAABGdBTUEAALGPC/xhBQAAAAFzUkdC\nAK7OHOkAAAAgY0hSTQAAeiYAAICEAAD6AAAAgOgAAHUwAADqYAAAOpgAABdwnLpRPAAAAAxQTFRF\n////chIS6YCRTb/E6kGE+wAAAAFiS0dEAIgFHUgAAAAJcEhZcwAAAEgAAABIAEbJaz4AAALKSURB\nVGje7dpLcqQwDAbgHHE2YeEj+D4cwQucBUfo+3CEXoSp8OhuhF70T4qpKXmdr21LogK2Pj7A8QmN\nP+HDhw8fPnz48Kf6VH9G+66vy+je8k19jnf8C5dXIPv86ms56lPdjvaYbyodx3ze+XLE76cXFiD4\nzPji99z0/AJ4n1lfvJ6fnl0A6x+578efMSg1wPr172/jPO5yFXM+Ef78gdblM+WPHyguP//t1/g6\npA0wfln+ho/fwgYYn19C/xwDvwHGc9OvC+hs37DTrwuwfWanXxdQTC9Mvyygs3wjTL8uwPJpn/tN\nDbSGz7T0SBEWw4vLXzbQ6b6RoveIoO6TvPxlA63qs7z8ZQPF9F+SH22vbX8OQKf5Rtv+EgDNJ3X5\n8wZaxWd1+fMGiuFvir8bvjp8J/tGy/6jAmRvhW8fwL3vVT+o3grfPoB7r/IpALI3tz8FoJN84/NV\n873hB8UnM3xzANtf8nb4dwmg3grfFEDJO8JPE0i9Ff4pAYL3pI8mkHor/HMCeO9JH00g9SafEsh7\nT/ppARBvp48UwJnelT5SACd7O31TAlnvKx9SQCd7B58KgPO+8iMFuPWe9E8F8BveWX7bAjzX9y4/\n/Jve+fhsH6Ctv7n8PTzjvY/v9gEOHz58+PBX+6v/f/wPvnd54f3j6venE/yl769Xv7+j3x/o98/V\n32/o9+fl389Xnx+g5x/o+Qt6/oOeP6HnX+j5G3z+h54/ouefV5/foufP6Pk3ev4On/+j9w/o/Qd6\n/4Le/6D3T/D9V67Y/ZsVQBq+s+8f0ftP+P41axXguP9NWgDuu/Cdfv+N3r/D9/9TAID+A7T/Ae2/\ngPs/0P4TtP8F7r9J3AIO9P+g/Udw/9Oygbf7r9D+L7j/DO1/Q/vv4P4/tP8Q7n9E+y/h/k+0/xTu\nf4X7b+H+X7T/+BPuf3aM8OHDhw8fPnz4w/4vzcvgeY10sY0AAAAldEVYdGRhdGU6Y3JlYXRlADIw\nMTYtMDQtMTNUMTE6Mzk6MTQtMDQ6MDALPlLjAAAAJXRFWHRkYXRlOm1vZGlmeQAyMDE2LTA0LTEz\nVDExOjM5OjE0LTA0OjAwemPqXwAAAABJRU5ErkJggg==\n", "text/plain": [ "" ] @@ -418,29 +423,25 @@ "\n", "# Instantiate flux Tally in moderator and fuel\n", "tally = openmc.Tally(name='flux')\n", - "tally.add_filter(openmc.Filter(type='cell', bins=[fuel_cell.id, moderator_cell.id]))\n", - "tally.add_filter(energy_filter)\n", - "tally.add_score('flux')\n", + "tally.filters = [openmc.Filter(type='cell', bins=[fuel_cell.id, moderator_cell.id])]\n", + "tally.filters.append(energy_filter)\n", + "tally.scores = ['flux']\n", "tallies_file.add_tally(tally)\n", "\n", "# Instantiate reaction rate Tally in fuel\n", "tally = openmc.Tally(name='fuel rxn rates')\n", - "tally.add_filter(openmc.Filter(type='cell', bins=[fuel_cell.id]))\n", - "tally.add_filter(energy_filter)\n", - "tally.add_score('nu-fission')\n", - "tally.add_score('scatter')\n", - "tally.add_nuclide(u238)\n", - "tally.add_nuclide(u235)\n", + "tally.filters = [openmc.Filter(type='cell', bins=[fuel_cell.id])]\n", + "tally.filters.append(energy_filter)\n", + "tally.scores = ['nu-fission', 'scatter']\n", + "tally.nuclides = [u238, u235]\n", "tallies_file.add_tally(tally)\n", "\n", "# Instantiate reaction rate Tally in moderator\n", "tally = openmc.Tally(name='moderator rxn rates')\n", - "tally.add_filter(openmc.Filter(type='cell', bins=[moderator_cell.id]))\n", - "tally.add_filter(energy_filter)\n", - "tally.add_score('absorption')\n", - "tally.add_score('total')\n", - "tally.add_nuclide(o16)\n", - "tally.add_nuclide(h1)\n", + "tally.filters = [openmc.Filter(type='cell', bins=[moderator_cell.id])]\n", + "tally.filters.append(energy_filter)\n", + "tally.scores = ['absorption', 'total']\n", + "tally.nuclides = [o16, h1]\n", "tallies_file.add_tally(tally)" ] }, @@ -455,8 +456,8 @@ "# K-Eigenvalue (infinity) tallies\n", "fiss_rate = openmc.Tally(name='fiss. rate')\n", "abs_rate = openmc.Tally(name='abs. rate')\n", - "fiss_rate.add_score('nu-fission')\n", - "abs_rate.add_score('absorption')\n", + "fiss_rate.scores = ['nu-fission']\n", + "abs_rate.scores = ['absorption']\n", "tallies_file.add_tally(fiss_rate)\n", "tallies_file.add_tally(abs_rate)" ] @@ -471,8 +472,8 @@ "source": [ "# Resonance Escape Probability tallies\n", "therm_abs_rate = openmc.Tally(name='therm. abs. rate')\n", - "therm_abs_rate.add_score('absorption')\n", - "therm_abs_rate.add_filter(openmc.Filter(type='energy', bins=[0., 0.625]))\n", + "therm_abs_rate.scores = ['absorption']\n", + "therm_abs_rate.filters = [openmc.Filter(type='energy', bins=[0., 0.625e-6])]\n", "tallies_file.add_tally(therm_abs_rate)" ] }, @@ -486,9 +487,9 @@ "source": [ "# Thermal Flux Utilization tallies\n", "fuel_therm_abs_rate = openmc.Tally(name='fuel therm. abs. rate')\n", - "fuel_therm_abs_rate.add_score('absorption')\n", - "fuel_therm_abs_rate.add_filter(openmc.Filter(type='energy', bins=[0., 0.625]))\n", - "fuel_therm_abs_rate.add_filter(openmc.Filter(type='cell', bins=[fuel_cell.id]))\n", + "fuel_therm_abs_rate.scores = ['absorption']\n", + "fuel_therm_abs_rate.filters = [openmc.Filter(type='energy', bins=[0., 0.625e-6]),\n", + " openmc.Filter(type='cell', bins=[fuel_cell.id])]\n", "tallies_file.add_tally(fuel_therm_abs_rate)" ] }, @@ -502,8 +503,8 @@ "source": [ "# Fast Fission Factor tallies\n", "therm_fiss_rate = openmc.Tally(name='therm. fiss. rate')\n", - "therm_fiss_rate.add_score('nu-fission')\n", - "therm_fiss_rate.add_filter(openmc.Filter(type='energy', bins=[0., 0.625]))\n", + "therm_fiss_rate.scores = ['nu-fission']\n", + "therm_fiss_rate.filters = [openmc.Filter(type='energy', bins=[0., 0.625e-6])]\n", "tallies_file.add_tally(therm_fiss_rate)" ] }, @@ -520,12 +521,10 @@ "\n", "# Instantiate flux Tally in moderator and fuel\n", "tally = openmc.Tally(name='need-to-slice')\n", - "tally.add_filter(openmc.Filter(type='cell', bins=[fuel_cell.id, moderator_cell.id]))\n", - "tally.add_filter(energy_filter)\n", - "tally.add_score('nu-fission')\n", - "tally.add_score('scatter')\n", - "tally.add_nuclide(h1)\n", - "tally.add_nuclide(u238)\n", + "tally.filters = [openmc.Filter(type='cell', bins=[fuel_cell.id, moderator_cell.id])]\n", + "tally.filters.append(energy_filter)\n", + "tally.scores = ['nu-fission', 'scatter']\n", + "tally.nuclides = [h1, u238]\n", "tallies_file.add_tally(tally)" ] }, @@ -533,7 +532,7 @@ "cell_type": "code", "execution_count": 22, "metadata": { - "collapsed": true + "collapsed": false }, "outputs": [], "source": [ @@ -576,8 +575,9 @@ " Copyright: 2011-2015 Massachusetts Institute of Technology\n", " License: http://mit-crpg.github.io/openmc/license.html\n", " Version: 0.7.1\n", - " Git SHA1: ea9fb637f63f9374c7436456141afa850b84acf9\n", - " Date/Time: 2016-01-14 07:00:14\n", + " Git SHA1: eeb5091ca3a34cc85df73a3318cae2b6c7097413\n", + " Date/Time: 2016-04-13 11:39:14\n", + " MPI Processes: 1\n", "\n", " ===========================================================================\n", " ========================> INITIALIZATION <=========================\n", @@ -604,26 +604,26 @@ "\n", " Bat./Gen. k Average k \n", " ========= ======== ==================== \n", - " 1/1 1.05992 \n", - " 2/1 1.05251 \n", - " 3/1 1.05204 \n", - " 4/1 1.02100 \n", - " 5/1 1.07784 \n", - " 6/1 1.04814 \n", - " 7/1 1.02335 1.03574 +/- 0.01239\n", - " 8/1 1.02415 1.03188 +/- 0.00813\n", - " 9/1 1.10331 1.04974 +/- 0.01876\n", - " 10/1 1.05452 1.05069 +/- 0.01456\n", - " 11/1 1.07867 1.05536 +/- 0.01277\n", - " 12/1 1.04203 1.05345 +/- 0.01096\n", - " 13/1 1.04482 1.05237 +/- 0.00955\n", - " 14/1 1.04117 1.05113 +/- 0.00852\n", - " 15/1 1.07581 1.05360 +/- 0.00801\n", - " 16/1 1.04235 1.05257 +/- 0.00731\n", - " 17/1 1.02710 1.05045 +/- 0.00701\n", - " 18/1 1.01970 1.04809 +/- 0.00687\n", - " 19/1 1.01022 1.04538 +/- 0.00691\n", - " 20/1 1.01449 1.04332 +/- 0.00675\n", + " 1/1 1.03471 \n", + " 2/1 1.03257 \n", + " 3/1 1.00600 \n", + " 4/1 1.04547 \n", + " 5/1 1.02287 \n", + " 6/1 1.05752 \n", + " 7/1 1.04283 1.05017 +/- 0.00734\n", + " 8/1 1.05189 1.05074 +/- 0.00428\n", + " 9/1 1.01645 1.04217 +/- 0.00909\n", + " 10/1 1.04978 1.04369 +/- 0.00721\n", + " 11/1 1.03459 1.04218 +/- 0.00608\n", + " 12/1 1.04019 1.04189 +/- 0.00514\n", + " 13/1 1.05985 1.04414 +/- 0.00499\n", + " 14/1 1.02111 1.04158 +/- 0.00509\n", + " 15/1 1.04774 1.04219 +/- 0.00459\n", + " 16/1 1.00733 1.03902 +/- 0.00523\n", + " 17/1 1.02224 1.03763 +/- 0.00497\n", + " 18/1 1.03263 1.03724 +/- 0.00459\n", + " 19/1 1.01611 1.03573 +/- 0.00451\n", + " 20/1 1.04692 1.03648 +/- 0.00426\n", " Creating state point statepoint.20.h5...\n", "\n", " ===========================================================================\n", @@ -633,27 +633,27 @@ "\n", " =======================> TIMING STATISTICS <=======================\n", "\n", - " Total time for initialization = 1.2510E+00 seconds\n", - " Reading cross sections = 9.7600E-01 seconds\n", - " Total time in simulation = 1.5844E+01 seconds\n", - " Time in transport only = 1.5834E+01 seconds\n", - " Time in inactive batches = 2.2840E+00 seconds\n", - " Time in active batches = 1.3560E+01 seconds\n", - " Time synchronizing fission bank = 3.0000E-03 seconds\n", - " Sampling source sites = 2.0000E-03 seconds\n", + " Total time for initialization = 4.0300E-01 seconds\n", + " Reading cross sections = 8.6000E-02 seconds\n", + " Total time in simulation = 1.4439E+01 seconds\n", + " Time in transport only = 1.4430E+01 seconds\n", + " Time in inactive batches = 2.2790E+00 seconds\n", + " Time in active batches = 1.2160E+01 seconds\n", + " Time synchronizing fission bank = 2.0000E-03 seconds\n", + " Sampling source sites = 1.0000E-03 seconds\n", " SEND/RECV source sites = 1.0000E-03 seconds\n", " Time accumulating tallies = 0.0000E+00 seconds\n", " Total time for finalization = 1.0000E-03 seconds\n", - " Total time elapsed = 1.7110E+01 seconds\n", - " Calculation Rate (inactive) = 5472.85 neutrons/second\n", - " Calculation Rate (active) = 2765.49 neutrons/second\n", + " Total time elapsed = 1.4856E+01 seconds\n", + " Calculation Rate (inactive) = 5484.86 neutrons/second\n", + " Calculation Rate (active) = 3083.88 neutrons/second\n", "\n", " ============================> RESULTS <============================\n", "\n", - " k-effective (Collision) = 1.03935 +/- 0.00682\n", - " k-effective (Track-length) = 1.04332 +/- 0.00675\n", - " k-effective (Absorption) = 1.03845 +/- 0.00598\n", - " Combined k-effective = 1.04024 +/- 0.00523\n", + " k-effective (Collision) = 1.03296 +/- 0.00669\n", + " k-effective (Track-length) = 1.03648 +/- 0.00426\n", + " k-effective (Absorption) = 1.03431 +/- 0.00702\n", + " Combined k-effective = 1.03621 +/- 0.00456\n", " Leakage Fraction = 0.00000 +/- 0.00000\n", "\n" ] @@ -701,7 +701,7 @@ "outputs": [], "source": [ "# Load the statepoint file\n", - "sp = StatePoint('statepoint.20.h5')" + "sp = openmc.StatePoint('statepoint.20.h5')" ] }, { @@ -721,7 +721,7 @@ "outputs": [], "source": [ "# Load the summary file and link with statepoint\n", - 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energy [MeV]energy low [MeV]energy high [MeV]cellnuclidescore
0(0.0e+00 - 6.2e-01)06.250000e-0710000total(((absorption * nu-fission) * absorption) * (n...1.0401660.0190181.0383870.01316
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" ], "text/plain": [ - " energy [MeV] cell nuclide \\\n", - "0 (0.0e+00 - 6.2e-01) 10000 total \n", + " energy low [MeV] energy high [MeV] cell nuclide \\\n", + "0 0.00e+00 6.25e-07 10000 total \n", "\n", - " score mean std. dev. \n", - "0 (((absorption * nu-fission) * absorption) * (n... 1.040166 0.019018 " + " score mean std. dev. \n", + "0 (((absorption * nu-fission) * absorption) * (n... 1.04e+00 1.32e-02 " ] }, "execution_count": 31, @@ -1129,13 +1142,14 @@ { "data": { "text/html": [ - "
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cellenergy [MeV]energy low [MeV]energy high [MeV]nuclidescoremean
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cellenergy [MeV]energy low [MeV]energy high [MeV]nuclidescoremean
010002(1.0e-08 - 1.1e-07)1.000000e-081.080060e-07H-1scatter4.6193980.0401244.5992250.015973
110002(1.1e-07 - 1.2e-06)1.080060e-071.166529e-06H-1scatter2.0307570.0112392.0372600.011236
210002(1.2e-06 - 1.3e-05)1.166529e-061.259921e-05H-1scatter1.6584880.0097771.6625520.010280
310002(1.3e-05 - 1.4e-04)1.259921e-051.360790e-04H-1scatter1.8530020.0073781.8722010.012136
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810002(1.9e+00 - 2.0e+01)1.851749e+002.000000e+01H-1scatter0.3712800.0039490.3720220.003196
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We recommend going through the modules from Codecademy_ and/or the `Scipy lectures`_. The full API documentation serves to provide more information on a given module or class. -**Handling nuclear data:** +------------------------------------ +:mod:`openmc` -- Basic Functionality +------------------------------------ -.. toctree:: - :maxdepth: 1 +Handling nuclear data +--------------------- - ace +Classes ++++++++ -**Creating input files:** +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst -.. toctree:: - :maxdepth: 1 + openmc.XSdata + openmc.MGXSLibraryFile - cmfd - element - filter - geometry - material - mesh - nuclide - opencg_compatible - plots - settings - source - stats - surface - tallies - trigger - universe +Functions ++++++++++ -**Running OpenMC:** +.. autosummary:: + :toctree: generated + :nosignatures: -.. toctree:: - :maxdepth: 1 + openmc.ace.ascii_to_binary - executor +Simulation Settings +------------------- -**Post-processing:** +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst -.. toctree:: - :maxdepth: 1 + openmc.Source + openmc.ResonanceScattering + openmc.SettingsFile - particle_restart - statepoint - summary - tallies +Material Specification +---------------------- -**Multi-Group Cross Section Generation** +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst -.. toctree:: - :maxdepth: 1 + openmc.Nuclide + openmc.Element + openmc.Macroscopic + openmc.Material + openmc.MaterialsFile - mgxs - energy_groups - mgxs_library +Building geometry +----------------- -**Example Jupyter Notebooks:** +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.Plane + openmc.XPlane + openmc.YPlane + openmc.ZPlane + openmc.XCylinder + openmc.YCylinder + openmc.ZCylinder + openmc.Sphere + openmc.Cone + openmc.XCone + openmc.YCone + openmc.ZCone + openmc.Quadric + openmc.Halfspace + openmc.Intersection + openmc.Union + openmc.Complement + openmc.Cell + openmc.Universe + openmc.RectLattice + openmc.HexLattice + openmc.Geometry + openmc.GeometryFile + +Many of the above classes are derived from several abstract classes: + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.Surface + openmc.Region + openmc.Lattice + +Constructing Tallies +-------------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.Filter + openmc.Mesh + openmc.Trigger + openmc.Tally + openmc.TalliesFile + +Coarse Mesh Finite Difference Acceleration +------------------------------------------ + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.CMFDMesh + openmc.CMFDFile + +Plotting +-------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.Plot + openmc.PlotsFile + +Running OpenMC +-------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.Executor + +Post-processing +--------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.Particle + openmc.StatePoint + openmc.Summary + +Various classes may be created when performing tally slicing and/or arithmetic: + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.arithmetic.CrossScore + openmc.arithmetic.CrossNuclide + openmc.arithmetic.CrossFilter + openmc.arithmetic.AggregateScore + openmc.arithmetic.AggregateNuclide + openmc.arithmetic.AggregateFilter + +--------------------------------- +:mod:`openmc.stats` -- Statistics +--------------------------------- + +Univariate Probability Distributions +------------------------------------ + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.stats.Univariate + openmc.stats.Discrete + openmc.stats.Uniform + openmc.stats.Maxwell + openmc.stats.Watt + openmc.stats.Tabular + +Angular Distributions +--------------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.stats.UnitSphere + openmc.stats.PolarAzimuthal + openmc.stats.Isotropic + openmc.stats.Monodirectional + +Spatial Distributions +--------------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.stats.Spatial + openmc.stats.CartesianIndependent + openmc.stats.Box + openmc.stats.Point + +---------------------------------------------------------- +:mod:`openmc.mgxs` -- Multi-Group Cross Section Generation +---------------------------------------------------------- + +Energy Groups +------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.mgxs.EnergyGroups + +Multi-group Cross Sections +-------------------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.mgxs.MGXS + openmc.mgxs.AbsorptionXS + openmc.mgxs.CaptureXS + openmc.mgxs.Chi + openmc.mgxs.FissionXS + openmc.mgxs.NuFissionXS + openmc.mgxs.NuScatterXS + openmc.mgxs.NuScatterMatrixXS + openmc.mgxs.ScatterXS + openmc.mgxs.ScatterMatrixXS + openmc.mgxs.TotalXS + openmc.mgxs.TransportXS + +Multi-group Cross Section Libraries +----------------------------------- + +.. autosummary:: + :toctree: generated + :nosignatures: + :template: myclass.rst + + openmc.mgxs.Library + +------------------------- +Example Jupyter Notebooks +------------------------- .. toctree:: :maxdepth: 1 diff --git a/docs/source/pythonapi/material.rst b/docs/source/pythonapi/material.rst deleted file mode 100644 index 16a3af701..000000000 --- a/docs/source/pythonapi/material.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_material: - -========= -Materials -========= - -.. automodule:: openmc.material - :members: diff --git a/docs/source/pythonapi/mesh.rst b/docs/source/pythonapi/mesh.rst deleted file mode 100644 index dbecd7c31..000000000 --- a/docs/source/pythonapi/mesh.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_mesh: - -==== -Mesh -==== - -.. automodule:: openmc.mesh - :members: diff --git a/docs/source/pythonapi/mgxs.rst b/docs/source/pythonapi/mgxs.rst deleted file mode 100644 index c7084e565..000000000 --- a/docs/source/pythonapi/mgxs.rst +++ /dev/null @@ -1,66 +0,0 @@ -.. _pythonapi_mgxs: - -========================== -Multi-Group Cross Sections -========================== - -.. currentmodule:: openmc.mgxs.mgxs - ----------------------------- -Summary of Available Classes ----------------------------- - -.. autosummary:: - - MGXS - AbsorptionXS - CaptureXS - Chi - FissionXS - NuFissionXS - NuScatterXS - NuScatterMatrixXS - ScatterXS - ScatterMatrixXS - TotalXS - TransportXS - -------------------- -Class Documentation -------------------- - -.. autoclass:: MGXS - :members: - -.. autoclass:: AbsorptionXS - :members: - -.. autoclass:: CaptureXS - :members: - -.. autoclass:: Chi - :members: - -.. autoclass:: FissionXS - :members: - -.. autoclass:: NuFissionXS - :members: - -.. autoclass:: NuScatterXS - :members: - -.. autoclass:: NuScatterMatrixXS - :members: - -.. autoclass:: ScatterXS - :members: - -.. autoclass:: ScatterMatrixXS - :members: - -.. autoclass:: TotalXS - :members: - -.. autoclass:: TransportXS - :members: diff --git a/docs/source/pythonapi/mgxs_library.rst b/docs/source/pythonapi/mgxs_library.rst deleted file mode 100644 index 8ac545700..000000000 --- a/docs/source/pythonapi/mgxs_library.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_mgxs_library: - -============ -MGXS Library -============ - -.. automodule:: openmc.mgxs.library - :members: diff --git a/docs/source/pythonapi/nuclide.rst b/docs/source/pythonapi/nuclide.rst deleted file mode 100644 index 9e3214e92..000000000 --- a/docs/source/pythonapi/nuclide.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_nuclide: - -======= -Nuclide -======= - -.. automodule:: openmc.nuclide - :members: diff --git a/docs/source/pythonapi/particle_restart.rst b/docs/source/pythonapi/particle_restart.rst deleted file mode 100644 index 66ed89988..000000000 --- a/docs/source/pythonapi/particle_restart.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_particle_restart: - -================ -Particle Restart -================ - -.. automodule:: openmc.particle_restart - :members: diff --git a/docs/source/pythonapi/plots.rst b/docs/source/pythonapi/plots.rst deleted file mode 100644 index 8ad5348be..000000000 --- a/docs/source/pythonapi/plots.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_plots: - -===== -Plots -===== - -.. automodule:: openmc.plots - :members: diff --git a/docs/source/pythonapi/settings.rst b/docs/source/pythonapi/settings.rst deleted file mode 100644 index 3a3915ff5..000000000 --- a/docs/source/pythonapi/settings.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_settings: - -======== -Settings -======== - -.. automodule:: openmc.settings - :members: diff --git a/docs/source/pythonapi/source.rst b/docs/source/pythonapi/source.rst deleted file mode 100644 index 4bc770363..000000000 --- a/docs/source/pythonapi/source.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_source: - -====== -Source -====== - -.. automodule:: openmc.source - :members: diff --git a/docs/source/pythonapi/statepoint.rst b/docs/source/pythonapi/statepoint.rst deleted file mode 100644 index 737fc03fc..000000000 --- a/docs/source/pythonapi/statepoint.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_statepoint: - -========== -Statepoint -========== - -.. automodule:: openmc.statepoint - :members: diff --git a/docs/source/pythonapi/stats.rst b/docs/source/pythonapi/stats.rst deleted file mode 100644 index 58060cacb..000000000 --- a/docs/source/pythonapi/stats.rst +++ /dev/null @@ -1,58 +0,0 @@ -.. _pythonapi_stats: - -===================== -Statistical Functions -===================== - ----------------------------- -Summary of Available Classes ----------------------------- - -Univariate Probability Distributions ------------------------------------- - -.. currentmodule:: openmc.stats.univariate - -.. autosummary:: - - Univariate - Discrete - Uniform - Maxwell - Watt - Tabular - -Angular Distributions ---------------------- - -.. currentmodule:: openmc.stats.multivariate - -.. autosummary:: - - UnitSphere - PolarAzimuthal - Isotropic - Monodirectional - -Spatial Distributions ---------------------- - -.. autosummary:: - - Spatial - CartesianIndependent - Box - Point - - -Univariate Probability Distributions ------------------------------------- - -.. automodule:: openmc.stats.univariate - :members: - -Multivariate Probability Distributions --------------------------------------- - -.. automodule:: openmc.stats.multivariate - :members: diff --git a/docs/source/pythonapi/summary.rst b/docs/source/pythonapi/summary.rst deleted file mode 100644 index 9a791127b..000000000 --- a/docs/source/pythonapi/summary.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_summary: - -======= -Summary -======= - -.. automodule:: openmc.summary - :members: diff --git a/docs/source/pythonapi/surface.rst b/docs/source/pythonapi/surface.rst deleted file mode 100644 index cc31f5b3e..000000000 --- a/docs/source/pythonapi/surface.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_surface: - -======= -Surface -======= - -.. automodule:: openmc.surface - :members: diff --git a/docs/source/pythonapi/tallies.rst b/docs/source/pythonapi/tallies.rst deleted file mode 100644 index 2f24edf3a..000000000 --- a/docs/source/pythonapi/tallies.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_tallies: - -======= -Tallies -======= - -.. automodule:: openmc.tallies - :members: diff --git a/docs/source/pythonapi/trigger.rst b/docs/source/pythonapi/trigger.rst deleted file mode 100644 index 82567c2cf..000000000 --- a/docs/source/pythonapi/trigger.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_trigger: - -======= -Trigger -======= - -.. automodule:: openmc.trigger - :members: diff --git a/docs/source/pythonapi/universe.rst b/docs/source/pythonapi/universe.rst deleted file mode 100644 index fd4a3c1e2..000000000 --- a/docs/source/pythonapi/universe.rst +++ /dev/null @@ -1,8 +0,0 @@ -.. _pythonapi_universe: - -======== -Universe -======== - -.. automodule:: openmc.universe - :members: diff --git a/docs/source/usersguide/beginners.rst b/docs/source/usersguide/beginners.rst index d65ee1f83..9ecffe3f6 100644 --- a/docs/source/usersguide/beginners.rst +++ b/docs/source/usersguide/beginners.rst @@ -12,7 +12,7 @@ In a nutshell, OpenMC simulates neutrons moving around randomly in a `nuclear reactor`_ (or other fissile system). This is what's known as `Monte Carlo`_ simulation. Neutrons are important in nuclear reactors because they are the particles that induce `fission`_ in uranium and other nuclides. Knowing the -behavior of neutrons allows you to figure out how often and where fission +behavior of neutrons allows you to determine how often and where fission occurs. The amount of energy released is then directly proportional to the fission reaction rate since most heat is produced by fission. By simulating many neutrons (millions or billions), it is possible to determine the average diff --git a/docs/source/usersguide/index.rst b/docs/source/usersguide/index.rst index 5a7e7addf..0338c5cef 100644 --- a/docs/source/usersguide/index.rst +++ b/docs/source/usersguide/index.rst @@ -14,6 +14,7 @@ essential aspects of using OpenMC to perform simulations. beginners install input + mgxs_library output/index processing troubleshoot diff --git a/docs/source/usersguide/input.rst b/docs/source/usersguide/input.rst index 83f023c3c..a3e3228e4 100644 --- a/docs/source/usersguide/input.rst +++ b/docs/source/usersguide/input.rst @@ -112,9 +112,11 @@ standard deviation. The ```` element has no attributes and simply indicates the path to an XML cross section listing file (usually named cross_sections.xml). If this -element is absent from the settings.xml file, the :envvar:`CROSS_SECTIONS` -environment variable will be used to find the path to the XML cross section -listing. +element is absent from the settings.xml file, the +:envvar:`OPENMC_CROSS_SECTIONS` environment variable will be used to find the +path to the XML cross section listing when in continuous-energy mode, and the +:envvar:`OPENMC_MG_CROSS_SECTIONS` environment variable will be used in +multi-group mode. ```` Element -------------------- @@ -212,8 +214,21 @@ cross section values between. *Default*: logarithm + .. note:: This element is not used in the multi-group :ref:`energy_mode`. + .. _LA-UR-14-24530: https://laws.lanl.gov/vhosts/mcnp.lanl.gov/pdf_files/la-ur-14-24530.pdf +.. _energy_mode: + +```` Element +------------------------- + +The ```` element tells OpenMC if the run-mode should be +continuous-energy or multi-group. Options for entry are: ``continuous-energy`` +or ``multi-group``. + + *Default*: continuous-energy + ```` Element --------------------- @@ -264,6 +279,8 @@ based on the recommended value in LA-UR-14-24530_. *Default*: 8000 + .. note:: This element is not used in the multi-group :ref:`energy_mode`. + ```` Element ------------------------------- @@ -271,11 +288,24 @@ The ```` element indicates the directory containing a windowed multipole library. If a windowed multipole library is available, OpenMC can use it for on-the-fly Doppler-broadening of resolved resonance range cross sections. If this element is absent from the settings.xml file, the -:envvar:`MULTIPOLE_LIBRARY` environment variable will be used. +:envvar:`OPENMC_MULTIPOLE_LIBRARY` environment variable will be used. - .. note:: The element must also be set to "True" + .. note:: The element must also be set to "true" for windowed multipole functionality. +```` Element +--------------------------- + +The ```` element allows the user to set a maximum scattering order +to apply to every nuclide/material in the problem. That is, if the data +library has :math:`P_3` data available, but ```` was set to ``1``, +then, OpenMC will only use up to the :math:`P_1` data. + + *Default*: Use the maximum order in the data library + + .. note:: This element is not used in the continuous-energy + :ref:`energy_mode`. + .. _natural_elements: ```` Element @@ -324,10 +354,10 @@ out the file and "false" will not. *Default*: false :summary: - Writes out an ASCII summary file describing all of the user input files that + Writes out an HDF5 summary file describing all of the user input files that were read in. - *Default*: false + *Default*: true :tallies: Write out an ASCII file of tally results. @@ -355,6 +385,8 @@ or sub-elements and can be set to either "false" or "true". *Default*: true + .. note:: This element is not used in the multi-group :ref:`energy_mode`. + ```` Element ---------------------------------- @@ -414,6 +446,8 @@ attributes or sub-elements: *Defaults*: None (scatterer), ARES (method), 0.01 eV (E_min), 1.0 keV (E_max) + .. note:: This element is not used in the multi-group :ref:`energy_mode`. + ```` Element ---------------------- @@ -591,6 +625,8 @@ variable and whose sub-elements/attributes are as follows: number :math:`a` that parameterizes the distribution :math:`p(x) dx = c x e^{-x/a} dx`. + .. note:: The above format should be used even when using the multi-group + :ref:`energy_mode`. :interpolation: For a "tabular" distribution, ``interpolation`` can be set to "histogram" or "linear-linear" thereby specifying how tabular points are to be interpolated. @@ -1216,10 +1252,18 @@ Each ``material`` element can have the following attributes or sub-elements: ```` sub-elements are to be interpreted as nuclide/element densities in atom/b-cm, and the total density of the material is taken as the sum of all nuclides/elements. The "sum" option cannot be used in - conjunction with weight percents. + conjunction with weight percents. The "macro" unit is used with + a ``macroscopic`` quantity to indicate that the density is already included + in the library and thus not needed here. However, if a value is provided + for the ``value``, then this is treated as a number density multiplier on + the macroscopic cross sections in the multi-group data. This can be used, + for example, when perturbing the density slightly. *Default*: None + .. note:: A ``macroscopic`` quantity can not be used in conjunction with a + ``nuclide``, ``element``, or ``sab`` quantity. + :nuclide: An element with attributes/sub-elements called ``name``, ``xs``, and ``ao`` or ``wo``. The ``name`` attribute is the name of the cross-section for a @@ -1247,6 +1291,9 @@ Each ``material`` element can have the following attributes or sub-elements: *Default*: None + .. note:: The ``scattering`` attribute/sub-element is not used in the + multi-group :ref:`energy_mode`. + :element: Specifies that a natural element is present in the material. The natural @@ -1282,6 +1329,9 @@ Each ``material`` element can have the following attributes or sub-elements: *Default*: None + .. note:: The ``scattering`` attribute/sub-element is not used in the + multi-group :ref:`energy_mode`. + :sab: Associates an S(a,b) table with the material. This element has attributes/sub-elements called ``name`` and ``xs``. The ``name`` attribute @@ -1290,6 +1340,26 @@ Each ``material`` element can have the following attributes or sub-elements: *Default*: None + .. note:: This element is not used in the multi-group :ref:`energy_mode`. + + :macroscopic: + The ``macroscopic`` element is similar to the ``nuclide`` element, but, + recognizes that some multi-group libraries may be providing material + specific macroscopic cross sections instead of always providing nuclide + specific data like in the continuous-energy case. To that end, the + macroscopic element has attributes/sub-elements called ``name``, and ``xs``. + The ``name`` attribute is the name of the cross-section for a + desired nuclide while the ``xs`` attribute is the cross-section + identifier. One example would be as follows: + + .. code-block:: xml + + + + .. note:: This element is only used in the multi-group :ref:`energy_mode`. + + *Default*: None + .. _IUPAC Isotopic Compositions of the Elements 2009: http://pac.iupac.org/publications/pac/pdf/2011/pdf/8302x0397.pdf @@ -1376,7 +1446,8 @@ The ```` element accepts the following sub-elements: A list of universes for which the tally should be accumulated. :energy: - A monotonically increasing list of bounding **pre-collision** energies + In continuous-energy mode, this filter should be provided as a + monotonically increasing list of bounding **pre-collision** energies for a number of groups. For example, if this filter is specified as .. code-block:: xml @@ -1386,17 +1457,24 @@ The ```` element accepts the following sub-elements: then two energy bins will be created, one with energies between 0 and 1 MeV and the other with energies between 1 and 20 MeV. + In multi-group mode the bins provided must match group edges + defined in the multi-group library. + :energyout: - A monotonically increasing list of bounding **post-collision** - energies for a number of groups. For example, if this filter is - specified as + In continuous-energy mode, this filter should be provided as a + monotonically increasing list of bounding **post-collision** energies + for a number of groups. For example, if this filter is specified as .. code-block:: xml - then two post-collision energy bins will be created, one with energies - between 0 and 1 MeV and the other with energies between 1 and 20 MeV. + then two post-collision energy bins will be created, one with + energies between 0 and 1 MeV and the other with energies between + 1 and 20 MeV. + + In multi-group mode the bins provided must match group edges + defined in the multi-group library. :mu: A monotonically increasing list of bounding **post-collision** cosines @@ -1480,6 +1558,8 @@ The ```` element accepts the following sub-elements: + .. note:: This filter type is not used in the multi-group :ref:`energy_mode`. + :nuclides: If specified, the scores listed will be for particular nuclides, not the summation of reactions from all nuclides. The format for nuclides should be @@ -1659,7 +1739,8 @@ The ```` element accepts the following sub-elements: |Score | Description | +======================+===================================================+ |delayed-nu-fission |Total production of delayed neutrons due to | - | |fission. | + | |fission. This score type is not used in the | + | |multi-group :ref:`energy_mode`. | +----------------------+---------------------------------------------------+ |nu-fission |Total production of neutrons due to fission. | +----------------------+---------------------------------------------------+ @@ -1688,6 +1769,8 @@ The ```` element accepts the following sub-elements: +----------------------+---------------------------------------------------+ |inverse-velocity |The flux-weighted inverse velocity where the | | |velocity is in units of centimeters per second. | + | |This score type is not used in the | + | |multi-group :ref:`energy_mode`. | +----------------------+---------------------------------------------------+ |kappa-fission |The recoverable energy production rate due to | | |fission. The recoverable energy is defined as the | diff --git a/docs/source/usersguide/install.rst b/docs/source/usersguide/install.rst index 4075e0303..1a0569148 100644 --- a/docs/source/usersguide/install.rst +++ b/docs/source/usersguide/install.rst @@ -227,6 +227,7 @@ your PATH environment variable and subsequently uses it to determine library locations and compile flags. If you have multiple installations of HDF5 or one that does not appear on your PATH, you can set the HDF5_ROOT environment variable to the root directory of the HDF5 installation, e.g. + .. code-block:: sh export HDF5_ROOT=/opt/hdf5/1.8.15 @@ -355,7 +356,7 @@ Testing Build ------------- If you have ENDF/B-VII.1 cross sections from NNDC_ you can test your build. -Make sure the **CROSS_SECTIONS** environmental variable is set to the +Make sure the **OPENMC_CROSS_SECTIONS** environmental variable is set to the *cross_sections.xml* file in the *data/nndc* directory. There are two ways to run tests. The first is to use the Makefile present in the source directory and run the following: @@ -380,11 +381,17 @@ Cross Section Configuration --------------------------- In order to run a simulation with OpenMC, you will need cross section data for -each nuclide in your problem. Since OpenMC uses ACE format cross sections, you -can use nuclear data that was processed with NJOY_, such as that distributed -with MCNP_ or Serpent_. Several sources provide free processed ACE data as -described below. The TALYS-based evaluated nuclear data library, TENDL_, is also -openly available in ACE format. +each nuclide or material in your problem. OpenMC can be run in +continuous-energy or multi-group mode. + +In continuous-energy mode OpenMC uses ACE format cross sections; in this case +you can use nuclear data that was processed with NJOY_, such as that +distributed with MCNP_ or Serpent_. Several sources provide free processed +ACE data as described below. The TALYS-based evaluated nuclear data library, +TENDL_, is also openly available in ACE format. + +In multi-group mode, OpenMC utilizes an XML-based library format which can be +used to describe nuclide- or material-specific quantities. Using ENDF/B-VII.1 Cross Sections from NNDC ------------------------------------------- @@ -399,9 +406,10 @@ extract, and set up a confiuration file: cd openmc/data python get_nndc_data.py -At this point, you should set the :envvar:`CROSS_SECTIONS` environment variable -to the absolute path of the file ``openmc/data/nndc/cross_sections.xml``. This -cross section set is used by the test suite. +At this point, you should set the :envvar:`OPENMC_CROSS_SECTIONS` environment +variable to the absolute path of the file +``openmc/data/nndc/cross_sections.xml``. This cross section set is used by the +test suite. Using JEFF Cross Sections from OECD/NEA --------------------------------------- @@ -427,8 +435,8 @@ the following steps must be taken: 4. Additionally, you may need to change any occurrences of upper-case "ACE" within the ``cross_sections.xml`` file to lower-case. 5. Either set the :ref:`cross_sections` in a settings.xml file or the - :envvar:`CROSS_SECTIONS` environment variable to the absolute path of the - ``cross_sections.xml`` file. + :envvar:`OPENMC_CROSS_SECTIONS` environment variable to the absolute path of + the ``cross_sections.xml`` file. Using Cross Sections from MCNP ------------------------------ @@ -436,8 +444,9 @@ Using Cross Sections from MCNP To use cross sections distributed with MCNP, change the element in the ``cross_sections.xml`` file in the root directory of the OpenMC distribution to the location of the MCNP cross sections. Then, either set the -:ref:`cross_sections` in a settings.xml file or the :envvar:`CROSS_SECTIONS` -environment variable to the absolute path of the ``cross_sections.xml`` file. +:ref:`cross_sections` in a settings.xml file or the +:envvar:`OPENMC_CROSS_SECTIONS` environment variable to the absolute path of +the ``cross_sections.xml`` file. Using Cross Sections from Serpent --------------------------------- @@ -445,10 +454,21 @@ Using Cross Sections from Serpent To use cross sections distributed with Serpent, change the element in the ``cross_sections_serpent.xml`` file in the root directory of the OpenMC distribution to the location of the Serpent cross sections. Then, either set the -:ref:`cross_sections` in a settings.xml file or the :envvar:`CROSS_SECTIONS` -environment variable to the absolute path of the ``cross_sections_serpent.xml`` +:ref:`cross_sections` in a settings.xml file or the +:envvar:`OPENMC_CROSS_SECTIONS` environment variable to the absolute path of +the ``cross_sections_serpent.xml`` file. +Using Multi-Group Cross Sections +-------------------------------- + +Multi-group cross section libraries are generally tailored to the specific +calculation to be performed. Therefore, at this point in time, OpenMC is not +distributed with any pre-existing multi-group cross section libraries. +However, if the user has obtained or generated their own library, the user +should set the :envvar:`OPENMC_MG_CROSS_SECTIONS` environment variable +to the absolute path of the file library expected to used most frequently. + .. _NJOY: http://t2.lanl.gov/nis/codes.shtml .. _NNDC: http://www.nndc.bnl.gov/endf/b7.1/acefiles.html .. _NEA: http://www.oecd-nea.org diff --git a/docs/source/usersguide/mgxs_library.rst b/docs/source/usersguide/mgxs_library.rst new file mode 100644 index 000000000..a5d2ec0d0 --- /dev/null +++ b/docs/source/usersguide/mgxs_library.rst @@ -0,0 +1,302 @@ +.. _usersguide_mgxs_library: + +======================================== +Multi-Group Cross Section Library Format +======================================== + +OpenMC can be run in continuous-energy mode or multi-group mode, provided the +nuclear data is available. In continuous-energy mode, the +``cross_sections.xml`` file contains necessary meta-data for each data set, +including the name and a file system location where the complete library +can be found. In multi-group mode, this ``cross_sections.xml`` file contains +this same meta-data describing the nuclide or material, but also contains the +group-wise nuclear data. This portion of the manual describes the format of +the multi-group data library required to be used in the ``cross_sections.xml`` +file. + +Similar to the other input file types, the multi-group library is provided in +the XML_ format. This library must provide some meta-data about the library +itself (such as the number of groups and the group structure, etc.) as well as +the actual cross section data itself for each of the necessary nuclides or +materials. + +.. _XML: http://www.w3.org/XML/ + +------------------------------------------------ +MGXS Library Specification -- cross_sections.xml +------------------------------------------------ + +The multi-group library meta-data is contained within the groups_, +group_structure_, and inverse_velocities_ elements. +The actual multi-group data itself is contained within the xsdata_ element. + +.. _groups: + +```` Element +---------------------------------- + +The ```` element has no attributes and simply provides the number of +energy groups contained within the library. + + *Default*: None, this must be provided. + +.. _group_structure: + +```` Element +----------------------------- + +The ```` element has no attributes and should be provided as a +monotonically increasing list of bounding energies, in MeV, for a number of +groups. To provide proper energy boundaries, the length of the data within the +```` element should be one more than the number of groups in +the problem. For example, a two-group problem could be specified as: + +.. code-block:: xml + + 0.0 0.625E-6 20.0 + +*Default*: None, this must be provided. + +.. _inverse_velocities: + +```` Element +-------------------------------- + +The ```` element optionally indicates the average +inverse velocity corresponding to each of the groups in the problem. +This element should therefore be an array with a length which matches the +number of groups set in the groups_ element. + +*Default*: Should this be needed by the presence of an ``inverse-velocity`` +score in the ``tallies.xml`` file and not provided in this element, OpenMC +will simply convert the group mid-point energy to an inverse of the velocity +and use this information for tallying. + +.. _xsdata: + +```` Element +-------------------- + +The ```` element contains the nuclide or material-specific meta-data as +well as the actual cross section data. The following are the +attributes/sub-elements required to describe the meta-data: + + :name: + The name of the microscopic or macroscopic data set. An extension to the + name must be provided (e.g., the ``.300K`` in ``UO2.300K``). The name and + extension together must be twelve or less characters in length. This + extension must follow a period and be five characters or less in length. + similar to the equivalent in the continuous-energy ``cross_sections.xml`` + file, is used to denote variants of the particular nuclide or material of + interest (i.e. the ``UO2`` data in this example could have been generated + at a temperature of 300K). + + *Default*: None, this must be provided. + + :alias: + An alternative name to use for the microscopic or macroscopic data set. + + *Default*: If no alias is provided, it will adopt the value of ``name``. + + :kT: + The temperature times Boltzmann's constant (in units of MeV) at which the + data was generated. + + *Default*: Room temperature, 2.53E-8 MeV + + :fissionable: + This element states whether or not the data in question is fissionable. + Accepted values are "true" or "false". + + *Default*: None, this element must be provided. + + :representation: + This element provides the method used to generate and represent the + multi-group cross sections. That is, whether they were generated with + scalar flux weighting (or reduced to an equivalent representation) + and thus are angle-independent, or if the data was generated with angular + dependent fluxes and thus the data is angle-dependent. The options are + either "isotropic" or "angle". + + *Default*: "isotropic" + + :num_azimuthal: + This element provides the number of equal width angular bins that the + azimuthal angular domain is subdivided in the case of angle-dependent + cross sections (i.e., "angle" is passed to the ``representation`` element). + Note that these bins are equal in azimuthal angle widths, not equal in the + cosine of the azimuthal angle widths. + + *Default*: If ``representation`` is "angle", this must be provided. This + parameter is not used for other ``representation`` types. + + :num_polar: + This element provides the number of equal width angular bins that the + polar angular domain is subdivided in the case of angle-dependent + cross sections (i.e., "angle" is passed to the ``representation`` element). + Note that these bins are equal in polar angle widths, not equal in the + cosine of the polar angle widths. + + + *Default*: If ``representation`` is "angle", this must be provided. This + parameter is not used for other ``representation`` types. + + :scatt_type: + This element provides the representation of the angular distribution + associated with each group-to-group transfer probability. The options are + either "legendre", "histogram", or "tabular". + The "legendre" option means the angular distribution has been + expanded via Legendre polynomials of the order provided in the "order" + element. + The "histogram" option means the angular distribution is provided in + an equi-width histogram format with a number of bins as provided in the + "order" element. This is useful when the angular distribution was + obtained from a Monte Carlo tally and thus is natively in the histogram + format. + The "tabular" option means the angular distribution is provided in an + equi-spaced point-wise representation. + + *Default*: "legendre" + + :order: + This element provides either the Legendre order, number of bins, or number + of points used to describe the angular distribution associated with each + group-to-group transfer probability. The specific meaning of this bin + depends upon the value of ``scatt_type`` as discussed above. + + *Default*: None, this element must be provided. + + :tabular_legendre: + This optional element is used to set how the Legendre scattering kernel, if + provided via the ``scatt_type`` element above, is represented and thus used + during the scattering process. Specifically, the options are to either + convert the Legendre expansion to a tabular representation or leave it as + a set of Legendre coefficients. Converting to a tabular representation will + cost memory but is likely to decrease runtime compared to leaving as a + set of Legendre coefficients. This element has the following + attributes/sub-elements: + + :enable: + This attribute/sub-element denotes whether or not the conversion to the + tabular format should be performed or not. A value of "true" means + the conversion should be performed, "false" means it should not. + + *Default*: "true" + + :num_points: + If the conversion is to take place the number of tabular points is + required. This attribute/sub-element allows the user to set the desired + number of points. + + *Default*: 33 + + The following attributes/sub-elements are the cross section values to + be used during the transport process. + + :total: + This element requires the group-wise total cross section ordered by + increasing group index (i.e., fast to thermal). If ``representation`` is + "isotropic", then the length of this list should equal the number of + groups described in the ``groups`` element. If ``representation`` is + "angle", then the length of this list should equal the number of groups + times the number of azimuthal angles times the number of polar angles, + with the inner-dimension being groups, intermediate-dimension being + azimuthal angles and outer-dimension being the polar angles. + + *Default*: If not provided, it will be determined by summing the + absorption and scattering cross sections. + + :absorption: + This element requires the group-wise absorption cross section ordered by + increasing group index (i.e., fast to thermal). If ``representation`` is + "isotropic", then the length of this list should equal the number of + groups described in the ``groups`` element. If ``representation`` is + "angle", then the length of this list should equal the number of groups + times the number of azimuthal angles times the number of polar angles, + with the inner-dimension being groups, intermediate-dimension being + azimuthal angles and outer-dimension being the polar angles. + + *Default*: None, this must be provided. + + :scatter: + This element requires the scattering moment matrices presented with the + columns representing incoming group and rows representing the outgoing + group. That is, down-scatter will be above the diagonal of the resultant + matrix. This matrix is repeated for every Legendre order (in order of + increasing orders) if ``scatt_type`` is "legendre"; otherwise, this + matrix is repeated for every bin of the histogram or tabular + representation. Finally, if ``representation`` is "angle", the above + is repeated for every azimuthal angle and every polar angle, in that + order. + + *Default*: None, this must be provided. + + :multiplicity: + This element provides the ratio of neutrons produced in scattering + collisions to the neutrons which undergo scattering collisions; that is, + the multiplicity provides the code with a scaling factor to account for + neutrons being produced in (n,xn) reactions. This information is assumed + isotropic and therefore does not need to be repeated for every Legendre + moment or histogram/tabular bin. This matrix follows the same arrangement + as described for the ``scatter`` element, with the exception of the + data needed to provide the scattering type information. + + *Default*: Multiplicities of 1.0 are assumed (i.e., (n,xn) reactions are + neglected). + + The following fission-specific data are only needed should ``fissionable`` + be "true". + + :fission: + This element requires the group-wise fission cross section ordered by + increasing group index (i.e., fast to thermal). If ``representation`` is + "isotropic", then the length of this list should equal the number of + groups described in the ``groups`` element. If ``representation`` is + "angle", then the length of this list should equal the number of groups + times the number of azimuthal angles times the number of polar angles, + with the inner-dimension being groups, intermediate-dimension being + azimuthal angles and outer-dimension being the polar angles. + + *Default*: None, this is required only if fission tallies are + requested and the material is fissionable. + + :kappa_fission: + This element requires the group-wise kappa-fission cross section ordered by + increasing group index (i.e., fast to thermal). If ``representation`` is + "isotropic", then the length of this list should equal the number of + groups described in the ``groups`` element. If ``representation`` is + "angle", then the length of this list should equal the number of groups + times the number of azimuthal angles times the number of polar angles, + with the inner-dimension being groups, intermediate-dimension being + azimuthal angles and outer-dimension being the polar angles. + + *Default*: None, this is required only if kappa_fission tallies are + requested and the material is fissionable. + + :chi: + This element requires the group-wise fission spectra ordered by + increasing group index (i.e., fast to thermal). This element should be + used if making the common approximation that the fission spectra does + not depend on incoming energy. If the user does not wish to make this + approximation, then this should not be provided and this information + included in the ``nu_fission`` element instead. If ``representation`` is + "isotropic", then the length of this list should equal the number of + groups described in the ``groups`` element. If ``representation`` is + "angle", then the length of this list should equal the number of groups + times the number of azimuthal angles times the number of polar angles, + with the inner-dimension being groups, intermediate-dimension being + azimuthal angles and outer-dimension being the polar angles. + + *Default*: None, either this element is provided or ``nu_fission`` is + provided in fission matrix form, or the material is not fissionable. + + :nu_fission: + This element provides either the group-wise fission production cross + section vector (i.e., if ``chi`` is provided), or is the group-wise fission + production matrix. If providing the vector, it should be ordered the same + as the ``fission`` data. If providing the matrix, it should be ordered + the same as the ``multiplicity`` matrix. + + *Default*: None, either this element must be provided if the material + is fissionable. + diff --git a/docs/source/usersguide/output/particle_restart.rst b/docs/source/usersguide/output/particle_restart.rst index e0d89a515..70f00a930 100644 --- a/docs/source/usersguide/output/particle_restart.rst +++ b/docs/source/usersguide/output/particle_restart.rst @@ -46,7 +46,8 @@ The current revision of the particle restart file format is 1. **/energy** (*double*) - Energy of the particle in MeV. + Energy of the particle in MeV for continuous-energy mode, or the energy + group of the particle for multi-group mode. **/xyz** (*double[3]*) diff --git a/docs/source/usersguide/output/source.rst b/docs/source/usersguide/output/source.rst index 2981b0f66..53841a5eb 100644 --- a/docs/source/usersguide/output/source.rst +++ b/docs/source/usersguide/output/source.rst @@ -15,5 +15,6 @@ is that documented here. **/source_bank** (Compound type) Source bank information for each particle. The compound type has fields - ``wgt``, ``xyz``, ``uvw``, and ``E`` which represent the weight, position, - direction, and energy of the source particle, respectively. + ``wgt``, ``xyz``, ``uvw``, ``E``, and ``delayed_group``, which + represent the weight, position, direction, energy, energy group, and + delayed_group of the source particle, respectively. diff --git a/docs/source/usersguide/output/statepoint.rst b/docs/source/usersguide/output/statepoint.rst index 786b7e8fb..4a51877f1 100644 --- a/docs/source/usersguide/output/statepoint.rst +++ b/docs/source/usersguide/output/statepoint.rst @@ -4,7 +4,7 @@ State Point File Format ======================= -The current revision of the statepoint file format is 14. +The current revision of the statepoint file format is 15. **/filetype** (*char[]*) @@ -39,6 +39,12 @@ The current revision of the statepoint file format is 14. Pseudo-random number generator seed. +**/run_CE** (*int*) + + Flag to denote continuous-energy or multi-group mode. A value of 1 + indicates a continuous-energy run while a value of 0 indicates a + multi-group run. + **/run_mode** (*char[]*) Run mode used. A value of 1 indicates a fixed-source run and a value of 2 @@ -258,7 +264,7 @@ if run_mode == 'k-eigenvalue': Accumulated sum and sum-of-squares for each global tally. The compound type has fields named ``sum`` and ``sum_sq``. -**tallies_present** (*int*) +**/tallies_present** (*int*) Flag indicated if tallies are present in the file. @@ -267,5 +273,72 @@ if (run_mode == 'k-eigenvalue' and source_present > 0) **/source_bank** (Compound type) Source bank information for each particle. The compound type has fields - ``wgt``, ``xyz``, ``uvw``, and ``E`` which represent the weight, - position, direction, and energy of the source particle, respectively. + ``wgt``, ``xyz``, ``uvw``, ``E``, ``g``, and ``delayed_group``, which + represent the weight, position, direction, energy, energy group, and + delayed_group of the source particle, respectively. + +**/runtime/total initialization** (*double*) + + Time (in seconds on the master process) spent reading inputs, allocating + arrays, etc. + +**/runtime/reading cross sections** (*double*) + + Time (in seconds on the master process) spent loading cross section + libraries (this is a subset of initialization). + +**/runtime/simulation** (*double*) + + Time (in seconds on the master process) spent between initialization and + finalization. + +**/runtime/transport** (*double*) + + Time (in seconds on the master process) spent transporting particles. + +**/runtime/inactive batches** (*double*) + + Time (in seconds on the master process) spent in the inactive batches + (including non-transport activities like communcating sites). + +**/runtime/active batches** (*double*) + + Time (in seconds on the master process) spent in the active batches + (including non-transport activities like communicating sites). + +**/runtime/synchronizing fission bank** (*double*) + + Time (in seconds on the master process) spent sampling source particles + from fission sites and communicating them to other processes for load + balancing. + +**/runtime/sampling source sites** (*double*) + + Time (in seconds on the master process) spent sampling source particles + from fission sites. + +**/runtime/SEND-RECV source sites** (*double*) + + Time (in seconds on the master process) spent communicating source sites + between processes for load balancing. + +**/runtime/accumulating tallies** (*double*) + + Time (in seconds on the master process) spent communicating tally results + and evaluating their statistics. + +**/runtime/CMFD** (*double*) + + Time (in seconds on the master process) spent evaluating CMFD. + +**/runtime/CMFD building matrices** (*double*) + + Time (in seconds on the master process) spent buliding CMFD matrices. + +**/runtime/CMFD solving matrices** (*double*) + + Time (in seconds on the master process) spent solving CMFD matrices. + +**/runtime/total** (*double*) + + Total time spent (in seconds on the master process) in the program. diff --git a/docs/source/usersguide/output/summary.rst b/docs/source/usersguide/output/summary.rst index 3be0cfdfe..cb9f725e8 100644 --- a/docs/source/usersguide/output/summary.rst +++ b/docs/source/usersguide/output/summary.rst @@ -297,6 +297,13 @@ The current revision of the summary file format is 1. Filter offset (used for distribcell filter). +**/tallies/tally /filter /paths** (*char[][]*) + + The paths traversed through the CSG tree to reach each distribcell + instance (for 'distribcell' filters only). This consists of the integer + IDs for each universe, cell and lattice delimited by '->'. Each lattice + cell is specified by its (x,y) or (x,y,z) indices. + **/tallies/tally /filter /n_bins** (*int*) Number of bins for the j-th filter. diff --git a/docs/source/usersguide/processing.rst b/docs/source/usersguide/processing.rst index b18569ec6..059659dbc 100644 --- a/docs/source/usersguide/processing.rst +++ b/docs/source/usersguide/processing.rst @@ -196,10 +196,10 @@ Data Extraction A great deal of information is available in statepoint files (See :ref:`usersguide_statepoint`), all of which is accessible through the Python -API. The ``openmc.statepoint`` module (see :ref:`pythonapi_statepoint`) provides -a class to load statepoints and access data as requested; it is used in many of -the provided plotting utilities, OpenMC's regression test suite, and can be used -in user-created scripts to carry out manipulations of the data. +API. The :class:`openmc.StatePoint` class can load statepoints and access data +as requested; it is used in many of the provided plotting utilities, OpenMC's +regression test suite, and can be used in user-created scripts to carry out +manipulations of the data. An :ref:`example IPython notebook ` demonstrates how to extract data from a statepoint using the Python API. diff --git a/examples/python/basic/build-xml.py b/examples/python/basic/build-xml.py index 97591c992..fbe683661 100644 --- a/examples/python/basic/build-xml.py +++ b/examples/python/basic/build-xml.py @@ -1,6 +1,5 @@ import openmc -from openmc.source import Source -from openmc.stats import Box + ############################################################################### # Simulation Input File Parameters @@ -94,7 +93,12 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box([-4, -4, -4], [4, 4, 4])) + +# Create an initial uniform spatial source distribution over fissionable zones +bounds = [-4., -4., -4., 4., 4., 4.] +uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.export_to_xml() @@ -109,29 +113,20 @@ energyout_filter = openmc.Filter(type='energyout', bins=[0., 20.]) # Instantiate the first Tally first_tally = openmc.Tally(tally_id=1, name='first tally') -first_tally.add_filter(cell_filter) -scores = ['total', 'scatter', 'nu-scatter', \ +first_tally.filters = [cell_filter] +scores = ['total', 'scatter', 'nu-scatter', 'absorption', 'fission', 'nu-fission'] -for score in scores: - first_tally.add_score(score) +first_tally.scores = scores # Instantiate the second Tally second_tally = openmc.Tally(tally_id=2, name='second tally') -second_tally.add_filter(cell_filter) -second_tally.add_filter(energy_filter) -scores = ['total', 'scatter', 'nu-scatter', \ - 'absorption', 'fission', 'nu-fission'] -for score in scores: - second_tally.add_score(score) +second_tally.filters = [cell_filter, energy_filter] +second_tally.scores = scores # Instantiate the third Tally third_tally = openmc.Tally(tally_id=3, name='third tally') -third_tally.add_filter(cell_filter) -third_tally.add_filter(energy_filter) -third_tally.add_filter(energyout_filter) -scores = ['scatter', 'nu-scatter', 'nu-fission'] -for score in scores: - third_tally.add_score(score) +third_tally.filters = [cell_filter, energy_filter, energyout_filter] +third_tally.scores = ['scatter', 'nu-scatter', 'nu-fission'] # Instantiate a TalliesFile, register all Tallies, and export to XML tallies_file = openmc.TalliesFile() diff --git a/examples/python/boxes/build-xml.py b/examples/python/boxes/build-xml.py index 2ae3ee612..ea3e81d17 100644 --- a/examples/python/boxes/build-xml.py +++ b/examples/python/boxes/build-xml.py @@ -1,8 +1,5 @@ import numpy as np - import openmc -from openmc.source import Source -from openmc.stats import Box ############################################################################### # Simulation Input File Parameters @@ -119,7 +116,11 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box(*outer_cube.bounding_box)) + +# Create an initial uniform spatial source distribution over fissionable zones +uniform_dist = openmc.stats.Box(*outer_cube.bounding_box, only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.export_to_xml() ############################################################################### diff --git a/examples/python/lattice/hexagonal/build-xml.py b/examples/python/lattice/hexagonal/build-xml.py index 1125e8ce0..7f92e6602 100644 --- a/examples/python/lattice/hexagonal/build-xml.py +++ b/examples/python/lattice/hexagonal/build-xml.py @@ -1,6 +1,4 @@ import openmc -from openmc.source import Source -from openmc.stats import Box ############################################################################### # Simulation Input File Parameters @@ -126,8 +124,12 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box( - [-1, -1, -1], [1, 1, 1])) + +# Create an initial uniform spatial source distribution over fissionable zones +bounds = [-1, -1, -1, 1, 1, 1] +uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.keff_trigger = {'type' : 'std_dev', 'threshold' : 5E-4} settings_file.trigger_active = True settings_file.trigger_max_batches = 100 @@ -166,8 +168,8 @@ plot_file.export_to_xml() # Instantiate a distribcell Tally tally = openmc.Tally(tally_id=1) -tally.add_filter(openmc.Filter(type='distribcell', bins=[cell2.id])) -tally.add_score('total') +tally.filters = [openmc.Filter(type='distribcell', bins=[cell2.id])] +tally.scores = ['total'] # Instantiate a TalliesFile, register Tally/Mesh, and export to XML tallies_file = openmc.TalliesFile() diff --git a/examples/python/lattice/nested/build-xml.py b/examples/python/lattice/nested/build-xml.py index 389af8e9b..f54f06453 100644 --- a/examples/python/lattice/nested/build-xml.py +++ b/examples/python/lattice/nested/build-xml.py @@ -1,6 +1,4 @@ import openmc -from openmc.source import Source -from openmc.stats import Box ############################################################################### # Simulation Input File Parameters @@ -137,8 +135,12 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box( - [-1, -1, -1], [1, 1, 1])) + +# Create an initial uniform spatial source distribution over fissionable zones +bounds = [-1, -1, -1, 1, 1, 1] +uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.export_to_xml() @@ -175,8 +177,8 @@ mesh_filter.mesh = mesh # Instantiate the Tally tally = openmc.Tally(tally_id=1) -tally.add_filter(mesh_filter) -tally.add_score('total') +tally.filters = [mesh_filter] +tally.scores = ['total'] # Instantiate a TalliesFile, register Tally/Mesh, and export to XML tallies_file = openmc.TalliesFile() diff --git a/examples/python/lattice/simple/build-xml.py b/examples/python/lattice/simple/build-xml.py index e648c3d5b..f633fa96f 100644 --- a/examples/python/lattice/simple/build-xml.py +++ b/examples/python/lattice/simple/build-xml.py @@ -1,6 +1,4 @@ import openmc -from openmc.source import Source -from openmc.stats import Box ############################################################################### # Simulation Input File Parameters @@ -127,8 +125,12 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box( - [-1, -1, -1], [1, 1, 1])) + +# Create an initial uniform spatial source distribution over fissionable zones +bounds = [-1, -1, -1, 1, 1, 1] +uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.trigger_active = True settings_file.trigger_max_batches = 100 settings_file.export_to_xml() @@ -167,13 +169,13 @@ mesh_filter.mesh = mesh # Instantiate tally Trigger trigger = openmc.Trigger(trigger_type='rel_err', threshold=1E-2) -trigger.add_score('all') +trigger.scores = ['all'] # Instantiate the Tally tally = openmc.Tally(tally_id=1) -tally.add_filter(mesh_filter) -tally.add_score('total') -tally.add_trigger(trigger) +tally.filters = [mesh_filter] +tally.scores = ['total'] +tally.triggers = [trigger] # Instantiate a TalliesFile, register Tally/Mesh, and export to XML tallies_file = openmc.TalliesFile() diff --git a/examples/python/pincell/build-xml.py b/examples/python/pincell/build-xml.py index ca71b04e5..2e72d82ab 100644 --- a/examples/python/pincell/build-xml.py +++ b/examples/python/pincell/build-xml.py @@ -1,6 +1,4 @@ import openmc -from openmc.source import Source -from openmc.stats import Box ############################################################################### # Simulation Input File Parameters @@ -170,8 +168,12 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box( - [-0.62992, -0.62992, -1], [0.62992, 0.62992, 1])) + +# Create an initial uniform spatial source distribution over fissionable zones +bounds = [-0.62992, -0.62992, -1, 0.62992, 0.62992, 1] +uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.entropy_lower_left = [-0.39218, -0.39218, -1.e50] settings_file.entropy_upper_right = [0.39218, 0.39218, 1.e50] settings_file.entropy_dimension = [10, 10, 1] @@ -196,11 +198,8 @@ mesh_filter.mesh = mesh # Instantiate the Tally tally = openmc.Tally(tally_id=1, name='tally 1') -tally.add_filter(energy_filter) -tally.add_filter(mesh_filter) -tally.add_score('flux') -tally.add_score('fission') -tally.add_score('nu-fission') +tally.filters = [energy_filter, mesh_filter] +tally.scores = ['flux', 'fission', 'nu-fission'] # Instantiate a TalliesFile, register all Tallies, and export to XML tallies_file = openmc.TalliesFile() diff --git a/examples/python/pincell_multigroup/build-xml.py b/examples/python/pincell_multigroup/build-xml.py new file mode 100644 index 000000000..60026c089 --- /dev/null +++ b/examples/python/pincell_multigroup/build-xml.py @@ -0,0 +1,184 @@ +import numpy as np +import openmc +import openmc.mgxs + +############################################################################### +# Simulation Input File Parameters +############################################################################### + +# OpenMC simulation parameters +batches = 100 +inactive = 10 +particles = 1000 + +############################################################################### +# Exporting to OpenMC mg_cross_sections.xml File +############################################################################### + +# Instantiate the energy group data +groups = openmc.mgxs.EnergyGroups(group_edges=[1E-11, 0.0635E-6, 10.0E-6, + 1.0E-4, 1.0E-3, 0.5, 1.0, 20.0]) + +# Instantiate the 7-group (C5G7) cross section data +uo2_xsdata = openmc.XSdata('UO2.300K', groups) +uo2_xsdata.order = 0 +uo2_xsdata.total = np.array([0.1779492, 0.3298048, 0.4803882, 0.5543674, + 0.3118013, 0.3951678, 0.5644058]) +uo2_xsdata.absorption = np.array([8.0248E-03, 3.7174E-03, 2.6769E-02, 9.6236E-02, + 3.0020E-02, 1.1126E-01, 2.8278E-01]) +scatter = [[[0.1275370, 0.0423780, 0.0000094, 0.0000000, 0.0000000, 0.0000000, 0.0000000], + [0.0000000, 0.3244560, 0.0016314, 0.0000000, 0.0000000, 0.0000000, 0.0000000], + [0.0000000, 0.0000000, 0.4509400, 0.0026792, 0.0000000, 0.0000000, 0.0000000], + [0.0000000, 0.0000000, 0.0000000, 0.4525650, 0.0055664, 0.0000000, 0.0000000], + [0.0000000, 0.0000000, 0.0000000, 0.0001253, 0.2714010, 0.0102550, 0.0000000], + [0.0000000, 0.0000000, 0.0000000, 0.0000000, 0.0012968, 0.2658020, 0.0168090], + [0.0000000, 0.0000000, 0.0000000, 0.0000000, 0.0000000, 0.0085458, 0.2730800]]] +uo2_xsdata.scatter = np.array(scatter[:][:]) +uo2_xsdata.fission = np.array([7.21206E-03, 8.19301E-04, 6.45320E-03, + 1.85648E-02, 1.78084E-02, 8.30348E-02, + 2.16004E-01]) +uo2_xsdata.nu_fission = np.array([2.005998E-02, 2.027303E-03, 1.570599E-02, + 4.518301E-02, 4.334208E-02, 2.020901E-01, + 5.257105E-01]) +uo2_xsdata.chi = np.array([5.8791E-01, 4.1176E-01, 3.3906E-04, 1.1761E-07, + 0.0000E+00, 0.0000E+00, 0.0000E+00]) + +h2o_xsdata = openmc.XSdata('LWTR.300K', groups) +h2o_xsdata.order = 0 +h2o_xsdata.total = np.array([0.15920605, 0.412969593, 0.59030986, 0.58435, + 0.718, 1.2544497, 2.650379]) +h2o_xsdata.absorption = np.array([6.0105E-04, 1.5793E-05, 3.3716E-04, + 1.9406E-03, 5.7416E-03, 1.5001E-02, + 3.7239E-02]) +scatter = [[[0.0444777, 0.1134000, 0.0007235, 0.0000037, 0.0000001, 0.0000000, 0.0000000], + [0.0000000, 0.2823340, 0.1299400, 0.0006234, 0.0000480, 0.0000074, 0.0000010], + [0.0000000, 0.0000000, 0.3452560, 0.2245700, 0.0169990, 0.0026443, 0.0005034], + [0.0000000, 0.0000000, 0.0000000, 0.0910284, 0.4155100, 0.0637320, 0.0121390], + [0.0000000, 0.0000000, 0.0000000, 0.0000714, 0.1391380, 0.5118200, 0.0612290], + [0.0000000, 0.0000000, 0.0000000, 0.0000000, 0.0022157, 0.6999130, 0.5373200], + [0.0000000, 0.0000000, 0.0000000, 0.0000000, 0.0000000, 0.1324400, 2.4807000]]] +h2o_xsdata.scatter = np.array(scatter) + +mg_cross_sections_file = openmc.MGXSLibraryFile(groups) +mg_cross_sections_file.add_xsdatas([uo2_xsdata,h2o_xsdata]) +mg_cross_sections_file.export_to_xml() + + +############################################################################### +# Exporting to OpenMC materials.xml File +############################################################################### + +# Instantiate some Macroscopic Data +uo2_data = openmc.Macroscopic('UO2', '300K') +h2o_data = openmc.Macroscopic('LWTR', '300K') + +# Instantiate some Materials and register the appropriate Macroscopic objects +uo2 = openmc.Material(material_id=1, name='UO2 fuel') +uo2.set_density('macro', 1.0) +uo2.add_macroscopic(uo2_data) + +water = openmc.Material(material_id=2, name='Water') +water.set_density('macro', 1.0) +water.add_macroscopic(h2o_data) + +# Instantiate a MaterialsFile, register all Materials, and export to XML +materials_file = openmc.MaterialsFile() +materials_file.default_xs = '300K' +materials_file.add_materials([uo2, water]) +materials_file.export_to_xml() + + +############################################################################### +# Exporting to OpenMC geometry.xml File +############################################################################### + +# Instantiate ZCylinder surfaces +fuel_or = openmc.ZCylinder(surface_id=1, x0=0, y0=0, R=0.54, name='Fuel OR') +left = openmc.XPlane(surface_id=4, x0=-0.63, name='left') +right = openmc.XPlane(surface_id=5, x0=0.63, name='right') +bottom = openmc.YPlane(surface_id=6, y0=-0.63, name='bottom') +top = openmc.YPlane(surface_id=7, y0=0.63, name='top') + +left.boundary_type = 'reflective' +right.boundary_type = 'reflective' +top.boundary_type = 'reflective' +bottom.boundary_type = 'reflective' + +# Instantiate Cells +fuel = openmc.Cell(cell_id=1, name='cell 1') +moderator = openmc.Cell(cell_id=2, name='cell 2') + +# Use surface half-spaces to define regions +fuel.region = -fuel_or +moderator.region = +fuel_or & +left & -right & +bottom & -top + +# Register Materials with Cells +fuel.fill = uo2 +moderator.fill = water + +# Instantiate Universe +root = openmc.Universe(universe_id=0, name='root universe') + +# Register Cells with Universe +root.add_cells([fuel, moderator]) + +# Instantiate a Geometry and register the root Universe +geometry = openmc.Geometry() +geometry.root_universe = root + +# Instantiate a GeometryFile, register Geometry, and export to XML +geometry_file = openmc.GeometryFile() +geometry_file.geometry = geometry +geometry_file.export_to_xml() + + +############################################################################### +# Exporting to OpenMC settings.xml File +############################################################################### + +# Instantiate a SettingsFile, set all runtime parameters, and export to XML +settings_file = openmc.SettingsFile() +settings_file.energy_mode = "multi-group" +settings_file.cross_sections = "./mg_cross_sections.xml" +settings_file.batches = batches +settings_file.inactive = inactive +settings_file.particles = particles + +# Create an initial uniform spatial source distribution over fissionable zones +bounds = [-0.63, -0.63, -1, 0.63, 0.63, 1] +uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:]) +settings_file.source = openmc.source.Source(space=uniform_dist) + +settings_file.export_to_xml() + +############################################################################### +# Exporting to OpenMC tallies.xml File +############################################################################### + +# Instantiate a tally mesh +mesh = openmc.Mesh(mesh_id=1) +mesh.type = 'regular' +mesh.dimension = [100, 100, 1] +mesh.lower_left = [-0.63, -0.63, -1.e50] +mesh.upper_right = [0.63, 0.63, 1.e50] + +# Instantiate some tally Filters +energy_filter = openmc.Filter(type='energy', + bins=[1E-11, 0.0635E-6, 10.0E-6, 1.0E-4, 1.0E-3, + 0.5, 1.0, 20.0]) +mesh_filter = openmc.Filter() +mesh_filter.mesh = mesh + +# Instantiate the Tally +tally = openmc.Tally(tally_id=1, name='tally 1') +tally.add_filter(energy_filter) +tally.add_filter(mesh_filter) +tally.add_score('flux') +tally.add_score('fission') +tally.add_score('nu-fission') + +# Instantiate a TalliesFile, register all Tallies, and export to XML +tallies_file = openmc.TalliesFile() +tallies_file.add_mesh(mesh) +tallies_file.add_tally(tally) +tallies_file.export_to_xml() diff --git a/examples/python/reflective/build-xml.py b/examples/python/reflective/build-xml.py index 7e4fd30be..01a5c7815 100644 --- a/examples/python/reflective/build-xml.py +++ b/examples/python/reflective/build-xml.py @@ -1,8 +1,5 @@ import numpy as np - import openmc -from openmc.stats import Box -from openmc.source import Source ############################################################################### # Simulation Input File Parameters @@ -86,5 +83,10 @@ settings_file = openmc.SettingsFile() settings_file.batches = batches settings_file.inactive = inactive settings_file.particles = particles -settings_file.source = Source(space=Box(*cell.region.bounding_box)) + +# Create an initial uniform spatial source distribution over fissionable zones +uniform_dist = openmc.stats.Box(*cell.region.bounding_box, + only_fissionable=True) +settings_file.source = openmc.source.Source(space=uniform_dist) + settings_file.export_to_xml() diff --git a/examples/xml/pincell_multigroup/geometry.xml b/examples/xml/pincell_multigroup/geometry.xml new file mode 100644 index 000000000..94c70cb34 --- /dev/null +++ b/examples/xml/pincell_multigroup/geometry.xml @@ -0,0 +1,16 @@ + + + + + + + + + + + + + + + + diff --git a/examples/xml/pincell_multigroup/materials.xml b/examples/xml/pincell_multigroup/materials.xml new file mode 100644 index 000000000..696116654 --- /dev/null +++ b/examples/xml/pincell_multigroup/materials.xml @@ -0,0 +1,54 @@ + + + + 300K + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + diff --git a/examples/xml/pincell_multigroup/mg_cross_sections.xml b/examples/xml/pincell_multigroup/mg_cross_sections.xml new file mode 100644 index 000000000..3c671a192 --- /dev/null +++ b/examples/xml/pincell_multigroup/mg_cross_sections.xml @@ -0,0 +1,383 @@ + + + + 7 + + 1E-11 0.0635E-6 10.0E-6 1.0E-4 1.0E-3 0.5 1.0 20.0 + + + + + + UO2.300K + UO2.300K + 2.53E-8 + 0 + true + + isotropic + + + + 8.0248E-03 3.7174E-03 2.6769E-02 9.6236E-02 3.0020E-02 1.1126E-01 2.8278E-01 + + + + 2.005998E-02 2.027303E-03 1.570599E-02 4.518301E-02 4.334208E-02 2.020901E-01 5.257105E-01 + + + + 5.8791E-01 4.1176E-01 3.3906E-04 1.1761E-07 0.0000E+00 0.0000E+00 0.0000E+00 + + + 7.21206E-03 8.19301E-04 6.45320E-03 1.85648E-02 1.78084E-02 8.30348E-02 2.16004E-01 + + + + + + 1.0 1.0 1.0 1.0 1.0 1.0 1.0 + + + + + + 0.1275370 0.0423780 0.0000094 0.0000000 0.0000000 0.0000000 0.0000000 + 0.0000000 0.3244560 0.0016314 0.0000000 0.0000000 0.0000000 0.0000000 + 0.0000000 0.0000000 0.4509400 0.0026792 0.0000000 0.0000000 0.0000000 + 0.0000000 0.0000000 0.0000000 0.4525650 0.0055664 0.0000000 0.0000000 + 0.0000000 0.0000000 0.0000000 0.0001253 0.2714010 0.0102550 0.0000000 + 0.0000000 0.0000000 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3.16774000E-01 2.38760000E-01 + 0.00000000E00 0.00000000E00 0.00000000E00 0.00000000E00 0.00000000E00 4.97930000E-02 1.09910000E00 + + + + 1.26032048E-01 2.93160367E-01 2.84250824E-01 2.81025244E-01 3.34460185E-01 5.65640735E-01 1.17213908E00 + + + + + + + GT.300K + GT.300K + 2.53E-8 + 0 + false + + + + 5.11320000E-04 7.58010000E-05 3.15720000E-04 1.15820000E-03 3.39750000E-03 9.18780000E-03 2.32420000E-02 + + + + + + 6.61659000E-02 5.90700000E-02 2.83340000E-04 1.46220000E-06 2.06420000E-08 0.00000000E+00 0.00000000E+00 + 0.00000000E+00 2.40377000E-01 5.24350000E-02 2.49900000E-04 1.92390000E-05 2.98750000E-06 4.21400000E-07 + 0.00000000E+00 0.00000000E+00 1.83297000E-01 9.23970000E-02 6.94460000E-03 1.08030000E-03 2.05670000E-04 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 7.88511000E-02 1.70140000E-01 2.58810000E-02 4.92970000E-03 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 3.73330000E-05 9.97372000E-02 2.06790000E-01 2.44780000E-02 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 0.00000000E+00 9.17260000E-04 3.16765000E-01 2.38770000E-01 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 0.00000000E+00 0.00000000E+00 4.97920000E-02 1.09912000E+00 + + + + 1.26032043E-01 2.93160349E-01 2.84240290E-01 2.80960000E-01 3.34440033E-01 5.65640060E-01 1.17215400E+00 + + + + + + LWTR.300K + LWTR.300K + 2.53E-8 + 0 + false + + + + 6.0105E-04 1.5793E-05 3.3716E-04 1.9406E-03 5.7416E-03 1.5001E-02 3.7239E-02 + + + + + + 0.0444777 0.1134000 0.0007235 0.0000037 0.0000001 0.0000000 0.0000000 + 0.0000000 0.2823340 0.1299400 0.0006234 0.0000480 0.0000074 0.0000010 + 0.0000000 0.0000000 0.3452560 0.2245700 0.0169990 0.0026443 0.0005034 + 0.0000000 0.0000000 0.0000000 0.0910284 0.4155100 0.0637320 0.0121390 + 0.0000000 0.0000000 0.0000000 0.0000714 0.1391380 0.5118200 0.0612290 + 0.0000000 0.0000000 0.0000000 0.0000000 0.0022157 0.6999130 0.5373200 + 0.0000000 0.0000000 0.0000000 0.0000000 0.0000000 0.1324400 2.4807000 + + + + 0.15920605 0.41296959299999997 0.59030986 0.5843499999999999 0.7180000000000001 1.2544497000000001 2.650379 + + + + + + + CR.300K + CR.300K + 2.53E-8 + 0 + false + + + + 1.70490000E-03 8.36224000E-03 8.37901000E-02 3.97797000E-01 6.98763000E-01 9.29508000E-01 1.17836000E+00 + + + + + + 1.70563000E-01 4.44012000E-02 9.83670000E-05 1.27786000E-07 0.00000000E+00 0.00000000E+00 0.00000000E+00 + 0.00000000E+00 4.71050000E-01 6.85480000E-04 3.91395000E-10 0.00000000E+00 0.00000000E+00 0.00000000E+00 + 0.00000000E+00 0.00000000E+00 8.01859000E-01 7.20132000E-04 0.00000000E+00 0.00000000E+00 0.00000000E+00 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 5.70752000E-01 1.46015000E-03 0.00000000E+00 0.00000000E+00 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 6.55562000E-05 2.07838000E-01 3.81486000E-03 3.69760000E-09 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 0.00000000E+00 1.02427000E-03 2.02465000E-01 4.75290000E-03 + 0.00000000E+00 0.00000000E+00 0.00000000E+00 0.00000000E+00 0.00000000E+00 3.53043000E-03 6.58597000E-01 + + + + 2.16767595E-01 4.80097720E-01 8.86369232E-01 9.70009150E-01 9.10481420E-01 1.13775017E+00 1.84048743E+00 + + + diff --git a/examples/xml/pincell_multigroup/plots.xml b/examples/xml/pincell_multigroup/plots.xml new file mode 100644 index 000000000..cbb8e532c --- /dev/null +++ b/examples/xml/pincell_multigroup/plots.xml @@ -0,0 +1,28 @@ + + + + + 1 + mat + material + 0 0 0 + 1.26 1.26 + slice + 1000 1000 + + + + + + + + 2 + cell + cell + 0 0 0 + 1.26 1.26 + slice + 1000 1000 + + + diff --git a/examples/xml/pincell_multigroup/settings.xml b/examples/xml/pincell_multigroup/settings.xml new file mode 100644 index 000000000..dfd2fac81 --- /dev/null +++ b/examples/xml/pincell_multigroup/settings.xml @@ -0,0 +1,40 @@ + + + + multi-group + + + + 100 + 10 + 1000 + + + + + + + -0.63 -0.63 -1E50 + 0.63 0.63 1E50 + + + + + + true + true + true + + + false + + ./mg_cross_sections.xml + + diff --git a/examples/xml/pincell_multigroup/tallies.xml b/examples/xml/pincell_multigroup/tallies.xml new file mode 100644 index 000000000..df65b461d --- /dev/null +++ b/examples/xml/pincell_multigroup/tallies.xml @@ -0,0 +1,13 @@ + + + + 100 100 1 + -0.63 -0.63 -1e+50 + 0.63 0.63 1e+50 + + + + + flux fission nu-fission + + diff --git a/openmc/__init__.py b/openmc/__init__.py index ee3db59ae..02fd51dc7 100644 --- a/openmc/__init__.py +++ b/openmc/__init__.py @@ -1,11 +1,15 @@ +from openmc.cell import * +from openmc.lattice import * from openmc.element import * from openmc.geometry import * from openmc.nuclide import * +from openmc.macroscopic import * from openmc.material import * from openmc.plots import * from openmc.settings import * from openmc.surface import * from openmc.universe import * +from openmc.mgxs_library import * from openmc.mesh import * from openmc.filter import * from openmc.trigger import * @@ -15,6 +19,9 @@ from openmc.cmfd import * from openmc.executor import * from openmc.statepoint import * from openmc.summary import * +from openmc.region import * +from openmc.source import * +from openmc.particle_restart import * try: from openmc.opencg_compatible import * diff --git a/openmc/arithmetic.py b/openmc/arithmetic.py index 8574c4873..5869cad80 100644 --- a/openmc/arithmetic.py +++ b/openmc/arithmetic.py @@ -1,5 +1,7 @@ import sys +import copy from numbers import Integral +from collections import Iterable import numpy as np @@ -14,7 +16,7 @@ if sys.version_info[0] >= 3: _TALLY_ARITHMETIC_OPS = ['+', '-', '*', '/', '^'] # Acceptable tally aggregation operations -_TALLY_AGGREGATE_OPS = ['sum', 'mean'] +_TALLY_AGGREGATE_OPS = ['sum', 'avg'] class CrossScore(object): @@ -186,6 +188,23 @@ class CrossNuclide(object): return existing def __repr__(self): + return self.name + + + @property + def left_nuclide(self): + return self._left_nuclide + + @property + def right_nuclide(self): + return self._right_nuclide + + @property + def binary_op(self): + return self._binary_op + + @property + def name(self): string = '' @@ -207,18 +226,6 @@ class CrossNuclide(object): return string - @property - def left_nuclide(self): - return self._left_nuclide - - @property - def right_nuclide(self): - return self._right_nuclide - - @property - def binary_op(self): - return self._binary_op - @left_nuclide.setter def left_nuclide(self, left_nuclide): cv.check_type('left_nuclide', left_nuclide, @@ -430,7 +437,7 @@ class CrossFilter(object): filter_index = left_index * self.right_filter.num_bins + right_index return filter_index - def get_pandas_dataframe(self, datasize, summary=None): + def get_pandas_dataframe(self, data_size, summary=None): """Builds a Pandas DataFrame for the CrossFilter's bins. This method constructs a Pandas DataFrame object for the CrossFilter @@ -445,7 +452,7 @@ class CrossFilter(object): Parameters ---------- - datasize : Integral + data_size : Integral The total number of bins in the tally corresponding to this filter summary : None or Summary An optional Summary object to be used to construct columns for @@ -472,19 +479,18 @@ class CrossFilter(object): # If left and right filters are identical, do not combine bins if self.left_filter == self.right_filter: - df = self.left_filter.get_pandas_dataframe(datasize, summary) + df = self.left_filter.get_pandas_dataframe(data_size, summary) # If left and right filters are different, combine their bins else: - left_df = self.left_filter.get_pandas_dataframe(datasize, summary) - right_df = self.right_filter.get_pandas_dataframe(datasize, summary) + left_df = self.left_filter.get_pandas_dataframe(data_size, summary) + right_df = self.right_filter.get_pandas_dataframe(data_size, summary) left_df = left_df.astype(str) right_df = right_df.astype(str) df = '(' + left_df + ' ' + self.binary_op + ' ' + right_df + ')' return df - class AggregateScore(object): """A special-purpose tally score used to encapsulate an aggregate of a subset or all of tally's scores for tally aggregation. @@ -494,7 +500,7 @@ class AggregateScore(object): scores : Iterable of str or CrossScore The scores included in the aggregation aggregate_op : str - The tally aggregation operator (e.g., 'sum', 'mean', etc.) used + The tally aggregation operator (e.g., 'sum', 'avg', etc.) used to aggregate across a tally's scores with this AggregateScore Attributes @@ -502,7 +508,7 @@ class AggregateScore(object): scores : Iterable of str or CrossScore The scores included in the aggregation aggregate_op : str - The tally aggregation operator (e.g., 'sum', 'mean', etc.) used + The tally aggregation operator (e.g., 'sum', 'avg', etc.) used to aggregate across a tally's scores with this AggregateScore """ @@ -556,10 +562,16 @@ class AggregateScore(object): def aggregate_op(self): return self._aggregate_op + @property + def name(self): + + # Append each score in the aggregate to the string + string = '(' + ', '.join(self.scores) + ')' + return string + @scores.setter def scores(self, scores): - cv.check_iterable_type('scores', scores, - (basestring, CrossScore, AggregateScore)) + cv.check_iterable_type('scores', scores, basestring) self._scores = scores @aggregate_op.setter @@ -578,7 +590,7 @@ class AggregateNuclide(object): nuclides : Iterable of str or Nuclide or CrossNuclide The nuclides included in the aggregation aggregate_op : str - The tally aggregation operator (e.g., 'sum', 'mean', etc.) used + The tally aggregation operator (e.g., 'sum', 'avg', etc.) used to aggregate across a tally's nuclides with this AggregateNuclide Attributes @@ -586,7 +598,7 @@ class AggregateNuclide(object): nuclides : Iterable of str or Nuclide or CrossNuclide The nuclides included in the aggregation aggregate_op : str - The tally aggregation operator (e.g., 'sum', 'mean', etc.) used + The tally aggregation operator (e.g., 'sum', 'avg', etc.) used to aggregate across a tally's nuclides with this AggregateNuclide """ @@ -644,10 +656,19 @@ class AggregateNuclide(object): def aggregate_op(self): return self._aggregate_op + @property + def name(self): + + # Append each nuclide in the aggregate to the string + names = [nuclide.name if isinstance(nuclide, Nuclide) else str(nuclide) + for nuclide in self.nuclides] + string = '(' + ', '.join(map(str, names)) + ')' + return string + @nuclides.setter def nuclides(self, nuclides): cv.check_iterable_type('nuclides', nuclides, - (basestring, Nuclide, CrossNuclide, AggregateNuclide)) + (basestring, Nuclide, CrossNuclide)) self._nuclides = nuclides @aggregate_op.setter @@ -668,7 +689,7 @@ class AggregateFilter(object): bins : Iterable of tuple The filter bins included in the aggregation aggregate_op : str - The tally aggregation operator (e.g., 'sum', 'mean', etc.) used + The tally aggregation operator (e.g., 'sum', 'avg', etc.) used to aggregate across a tally filter's bins with this AggregateFilter Attributes @@ -678,7 +699,7 @@ class AggregateFilter(object): aggregate_filter : filter The filter included in the aggregation aggregate_op : str - The tally aggregation operator (e.g., 'sum', 'mean', etc.) used + The tally aggregation operator (e.g., 'sum', 'avg', etc.) used to aggregate across a tally filter's bins with this AggregateFilter bins : Iterable of tuple The filter bins included in the aggregation @@ -715,6 +736,21 @@ class AggregateFilter(object): def __ne__(self, other): return not self == other + def __gt__(self, other): + if self.type != other.type: + if self.aggregate_filter.type in _FILTER_TYPES and \ + other.aggregate_filter.type in _FILTER_TYPES: + delta = _FILTER_TYPES.index(self.aggregate_filter.type) - \ + _FILTER_TYPES.index(other.aggregate_filter.type) + return delta > 0 + else: + return False + else: + return False + + def __lt__(self, other): + return not self > other + def __repr__(self): string = 'AggregateFilter\n' string += '{0: <16}{1}{2}\n'.format('\tType', '=\t', self.type) @@ -759,7 +795,7 @@ class AggregateFilter(object): @property def num_bins(self): - return 1 if self.aggregate_filter else 0 + return len(self.bins) if self.aggregate_filter else 0 @property def stride(self): @@ -776,14 +812,13 @@ class AggregateFilter(object): @aggregate_filter.setter def aggregate_filter(self, aggregate_filter): - cv.check_type('aggregate_filter', aggregate_filter, - (Filter, CrossFilter, AggregateFilter)) + cv.check_type('aggregate_filter', aggregate_filter, (Filter, CrossFilter)) self._aggregate_filter = aggregate_filter @bins.setter def bins(self, bins): - cv.check_iterable_type('bins', bins, (Integral, tuple)) - self._bins = bins + cv.check_iterable_type('bins', bins, Iterable) + self._bins = list(map(tuple, bins)) @aggregate_op.setter def aggregate_op(self, aggregate_op): @@ -823,15 +858,14 @@ class AggregateFilter(object): """ - if filter_bin not in self.bins and \ - filter_bin != self._aggregate_filter.bins: + if filter_bin not in self.bins: msg = 'Unable to get the bin index for AggregateFilter since ' \ '"{0}" is not one of the bins'.format(filter_bin) raise ValueError(msg) else: - return 0 + return self.bins.index(filter_bin) - def get_pandas_dataframe(self, datasize, summary=None): + def get_pandas_dataframe(self, data_size, summary=None): """Builds a Pandas DataFrame for the AggregateFilter's bins. This method constructs a Pandas DataFrame object for the AggregateFilter @@ -840,7 +874,7 @@ class AggregateFilter(object): Parameters ---------- - datasize : Integral + data_size : Integral The total number of bins in the tally corresponding to this filter summary : None or Summary An optional Summary object to be used to construct columns for @@ -868,14 +902,80 @@ class AggregateFilter(object): import pandas as pd - # Construct a sring representing the filter aggregation - aggregate_bin = '{0}('.format(self.aggregate_op) - aggregate_bin += ', '.join(map(str, self.bins)) + ')' + # Create NumPy array of the bin tuples for repeating / tiling + filter_bins = np.empty(self.num_bins, dtype=tuple) + for i, bin in enumerate(self.bins): + filter_bins[i] = bin - # Construct NumPy array of bin repeated for each element in dataframe - aggregate_bin_array = np.array([aggregate_bin]) - aggregate_bin_array = np.repeat(aggregate_bin_array, datasize) + # Repeat and tile bins as needed for DataFrame + filter_bins = np.repeat(filter_bins, self.stride) + tile_factor = data_size / len(filter_bins) + filter_bins = np.tile(filter_bins, tile_factor) - # Construct Pandas DataFrame for the AggregateFilter - df = pd.DataFrame({self.type: aggregate_bin_array}) + # Create DataFrame with aggregated bins + df = pd.DataFrame({self.type: filter_bins}) return df + + def can_merge(self, other): + """Determine if AggregateFilter can be merged with another. + + Parameters + ---------- + other : AggregateFilter + Filter to compare with + + Returns + ------- + bool + Whether the filter can be merged + + """ + + if not isinstance(other, AggregateFilter): + return False + + # Filters must be of the same type + elif self.type != other.type: + return False + + # None of the bins in this filter should match in the other filter + for bin in self.bins: + if bin in other.bins: + return False + + # If all conditional checks passed then filters are mergeable + return True + + def merge(self, other): + """Merge this aggregatefilter with another. + + Parameters + ---------- + other : AggregateFilter + Filter to merge with + + Returns + ------- + merged_filter : AggregateFilter + Filter resulting from the merge + + """ + + if not self.can_merge(other): + msg = 'Unable to merge "{0}" with "{1}" ' \ + 'filters'.format(self.type, other.type) + raise ValueError(msg) + + # Create deep copy of filter to return as merged filter + merged_filter = copy.deepcopy(self) + + # Merge unique filter bins + merged_bins = self.bins + other.bins + + # Sort energy bin edges + if 'energy' in self.type: + merged_bins = sorted(merged_bins) + + # Assign merged bins to merged filter + merged_filter.bins = list(merged_bins) + return merged_filter diff --git a/openmc/cell.py b/openmc/cell.py new file mode 100644 index 000000000..2554df2d2 --- /dev/null +++ b/openmc/cell.py @@ -0,0 +1,478 @@ +from collections import OrderedDict, Iterable +from numbers import Real, Integral +from xml.etree import ElementTree as ET +import sys +import warnings + +import openmc +import openmc.checkvalue as cv +from openmc.surface import Halfspace +from openmc.region import Region, Intersection, Complement + +if sys.version_info[0] >= 3: + basestring = str + + +# A static variable for auto-generated Cell IDs +AUTO_CELL_ID = 10000 + + +def reset_auto_cell_id(): + global AUTO_CELL_ID + AUTO_CELL_ID = 10000 + + +class Cell(object): + """A region of space defined as the intersection of half-space created by + quadric surfaces. + + Parameters + ---------- + cell_id : int, optional + Unique identifier for the cell. If not specified, an identifier will + automatically be assigned. + name : str, optional + Name of the cell. If not specified, the name is the empty string. + + Attributes + ---------- + id : int + Unique identifier for the cell + name : str + Name of the cell + fill : openmc.Material or openmc.Universe or openmc.Lattice or 'void' or iterable of openmc.Material + Indicates what the region of space is filled with + region : openmc.Region + Region of space that is assigned to the cell. + rotation : numpy.ndarray + If the cell is filled with a universe, this array specifies the angles + in degrees about the x, y, and z axes that the filled universe should be + rotated. + temperature : float or iterable of float + Temperature of the cell in Kelvin. Multiple temperatures can be given + to give each distributed cell instance a unique temperature. + translation : numpy.ndarray + If the cell is filled with a universe, this array specifies a vector + that is used to translate (shift) the universe. + offsets : ndarray + Array of offsets used for distributed cell searches + distribcell_index : int + Index of this cell in distribcell arrays + + """ + + def __init__(self, cell_id=None, name=''): + # Initialize Cell class attributes + self.id = cell_id + self.name = name + self._fill = None + self._type = None + self._region = None + self._temperature = None + self._rotation = None + self._translation = None + self._offsets = None + self._distribcell_index = None + + def __eq__(self, other): + if not isinstance(other, Cell): + return False + elif self.id != other.id: + return False + elif self.name != other.name: + return False + elif self.fill != other.fill: + return False + elif self.region != other.region: + return False + elif self.rotation != other.rotation: + return False + elif self.temperature != other.temperature: + return False + elif self.translation != other.translation: + return False + else: + return True + + def __ne__(self, other): + return not self == other + + def __hash__(self): + return hash(repr(self)) + + def __repr__(self): + string = 'Cell\n' + string += '{0: <16}{1}{2}\n'.format('\tID', '=\t', self._id) + string += '{0: <16}{1}{2}\n'.format('\tName', '=\t', self._name) + + if isinstance(self._fill, openmc.Material): + string += '{0: <16}{1}{2}\n'.format('\tMaterial', '=\t', + self._fill._id) + elif isinstance(self._fill, Iterable): + string += '{0: <16}{1}'.format('\tMaterial', '=\t') + string += '[' + string += ', '.join(['void' if m == 'void' else str(m.id) + for m in self.fill]) + string += ']\n' + elif isinstance(self._fill, (openmc.Universe, openmc.Lattice)): + string += '{0: <16}{1}{2}\n'.format('\tFill', '=\t', + self._fill._id) + else: + string += '{0: <16}{1}{2}\n'.format('\tFill', '=\t', self._fill) + + string += '{0: <16}{1}{2}\n'.format('\tRegion', '=\t', self._region) + + string += '{0: <16}{1}{2}\n'.format('\tRotation', '=\t', + self._rotation) + if self.fill_type == 'material': + string += '\t{0: <15}=\t{1}\n'.format('Temperature', + self.temperature) + string += '{0: <16}{1}{2}\n'.format('\tTranslation', '=\t', + self._translation) + string += '{0: <16}{1}{2}\n'.format('\tOffset', '=\t', self._offsets) + string += '{0: <16}{1}{2}\n'.format('\tDistribcell index', '=\t', + self._distribcell_index) + + return string + + @property + def id(self): + return self._id + + @property + def name(self): + return self._name + + @property + def fill(self): + return self._fill + + @property + def fill_type(self): + if isinstance(self.fill, openmc.Material): + return 'material' + elif isinstance(self.fill, openmc.Universe): + return 'universe' + elif isinstance(self.fill, openmc.Lattice): + return 'lattice' + else: + return None + + @property + def region(self): + return self._region + + @property + def rotation(self): + return self._rotation + + @property + def temperature(self): + return self._temperature + + @property + def translation(self): + return self._translation + + @property + def offsets(self): + return self._offsets + + @property + def distribcell_index(self): + return self._distribcell_index + + @id.setter + def id(self, cell_id): + if cell_id is None: + global AUTO_CELL_ID + self._id = AUTO_CELL_ID + AUTO_CELL_ID += 1 + else: + cv.check_type('cell ID', cell_id, Integral) + cv.check_greater_than('cell ID', cell_id, 0, equality=True) + self._id = cell_id + + @name.setter + def name(self, name): + if name is not None: + cv.check_type('cell name', name, basestring) + self._name = name + else: + self._name = '' + + @fill.setter + def fill(self, fill): + if isinstance(fill, basestring): + if fill.strip().lower() == 'void': + self._type = 'void' + else: + msg = 'Unable to set Cell ID="{0}" to use a non-Material or ' \ + 'Universe fill "{1}"'.format(self._id, fill) + raise ValueError(msg) + + elif isinstance(fill, openmc.Material): + self._type = 'normal' + + elif isinstance(fill, Iterable): + cv.check_type('cell.fill', fill, Iterable, + (openmc.Material, basestring)) + self._type = 'normal' + + elif isinstance(fill, openmc.Universe): + self._type = 'fill' + + elif isinstance(fill, openmc.Lattice): + self._type = 'lattice' + + else: + msg = 'Unable to set Cell ID="{0}" to use a non-Material or ' \ + 'Universe fill "{1}"'.format(self._id, fill) + raise ValueError(msg) + + self._fill = fill + + @rotation.setter + def rotation(self, rotation): + cv.check_type('cell rotation', rotation, Iterable, Real) + cv.check_length('cell rotation', rotation, 3) + self._rotation = rotation + + @translation.setter + def translation(self, translation): + cv.check_type('cell translation', translation, Iterable, Real) + cv.check_length('cell translation', translation, 3) + self._translation = translation + + @temperature.setter + def temperature(self, temperature): + cv.check_type('cell temperature', temperature, (Iterable, Real)) + if isinstance(temperature, Iterable): + cv.check_type('cell temperature', temperature, Iterable, Real) + for T in temperature: + cv.check_greater_than('cell temperature', T, 0.0, True) + else: + cv.check_greater_than('cell temperature', temperature, 0.0, True) + self._temperature = temperature + + @offsets.setter + def offsets(self, offsets): + cv.check_type('cell offsets', offsets, Iterable) + self._offsets = offsets + + @region.setter + def region(self, region): + cv.check_type('cell region', region, Region) + self._region = region + + @distribcell_index.setter + def distribcell_index(self, ind): + cv.check_type('distribcell index', ind, Integral) + self._distribcell_index = ind + + def add_surface(self, surface, halfspace): + """Add a half-space to the list of half-spaces whose intersection defines the + cell. + + .. deprecated:: 0.7.1 + Use the :attr:`Cell.region` property to directly specify a Region + expression. + + Parameters + ---------- + surface : openmc.Surface + Quadric surface dividing space + halfspace : {-1, 1} + Indicate whether the negative or positive half-space is to be used + + """ + + warnings.warn("Cell.add_surface(...) has been deprecated and may be " + "removed in a future version. The region for a Cell " + "should be defined using the region property directly.", + DeprecationWarning) + + if not isinstance(surface, openmc.Surface): + msg = 'Unable to add Surface "{0}" to Cell ID="{1}" since it is ' \ + 'not a Surface object'.format(surface, self._id) + raise ValueError(msg) + + if halfspace not in [-1, +1]: + msg = 'Unable to add Surface "{0}" to Cell ID="{1}" with halfspace ' \ + '"{2}" since it is not +/-1'.format(surface, self._id, halfspace) + raise ValueError(msg) + + # If no region has been assigned, simply use the half-space. Otherwise, + # take the intersection of the current region and the half-space + # specified + region = +surface if halfspace == 1 else -surface + if self.region is None: + self.region = region + else: + if isinstance(self.region, Intersection): + self.region.nodes.append(region) + else: + self.region = Intersection(self.region, region) + + def get_cell_instance(self, path, distribcell_index): + + # If the Cell is filled by a Material + if self._type == 'normal' or self._type == 'void': + offset = 0 + + # If the Cell is filled by a Universe + elif self._type == 'fill': + offset = self.offsets[distribcell_index-1] + offset += self.fill.get_cell_instance(path, distribcell_index) + + # If the Cell is filled by a Lattice + else: + offset = self.fill.get_cell_instance(path, distribcell_index) + + return offset + + def get_all_nuclides(self): + """Return all nuclides contained in the cell + + Returns + ------- + nuclides : dict + Dictionary whose keys are nuclide names and values are 2-tuples of + (nuclide, density) + + """ + + nuclides = OrderedDict() + + if self._type != 'void': + nuclides.update(self._fill.get_all_nuclides()) + + return nuclides + + def get_all_cells(self): + """Return all cells that are contained within this one if it is filled with a + universe or lattice + + Returns + ------- + cells : dict + Dictionary whose keys are cell IDs and values are :class:`Cell` + instances + + """ + + cells = OrderedDict() + + if self._type == 'fill' or self._type == 'lattice': + cells.update(self._fill.get_all_cells()) + + return cells + + def get_all_materials(self): + """Return all materials that are contained within the cell + + Returns + ------- + materials : dict + Dictionary whose keys are material IDs and values are + :class:`Material` instances + + """ + + materials = OrderedDict() + if self.fill_type == 'material': + materials[self.fill.id] = self.fill + + # Append all Cells in each Cell in the Universe to the dictionary + cells = self.get_all_cells() + for cell_id, cell in cells.items(): + materials.update(cell.get_all_materials()) + + return materials + + def get_all_universes(self): + """Return all universes that are contained within this one if any of + its cells are filled with a universe or lattice. + + Returns + ------- + universes : dict + Dictionary whose keys are universe IDs and values are + :class:`Universe` instances + + """ + + universes = OrderedDict() + + if self._type == 'fill': + universes[self._fill._id] = self._fill + universes.update(self._fill.get_all_universes()) + elif self._type == 'lattice': + universes.update(self._fill.get_all_universes()) + + return universes + + def create_xml_subelement(self, xml_element): + element = ET.Element("cell") + element.set("id", str(self.id)) + + if len(self._name) > 0: + element.set("name", str(self.name)) + + if isinstance(self.fill, basestring): + element.set("material", "void") + + elif isinstance(self.fill, openmc.Material): + element.set("material", str(self.fill.id)) + + elif isinstance(self.fill, Iterable): + element.set("material", ' '.join([m if m == 'void' else str(m.id) + for m in self.fill])) + + elif isinstance(self.fill, (openmc.Universe, openmc.Lattice)): + element.set("fill", str(self.fill.id)) + self.fill.create_xml_subelement(xml_element) + + else: + element.set("fill", str(self.fill)) + self.fill.create_xml_subelement(xml_element) + + if self.region is not None: + # Set the region attribute with the region specification + element.set("region", str(self.region)) + + # Only surfaces that appear in a region are added to the geometry + # file, so the appropriate check is performed here. First we create + # a function which is called recursively to navigate through the CSG + # tree. When it reaches a leaf (a Halfspace), it creates a + # element for the corresponding surface if none has been created + # thus far. + def create_surface_elements(node, element): + if isinstance(node, Halfspace): + path = './surface[@id=\'{0}\']'.format(node.surface.id) + if xml_element.find(path) is None: + surface_subelement = node.surface.create_xml_subelement() + xml_element.append(surface_subelement) + elif isinstance(node, Complement): + create_surface_elements(node.node, element) + else: + for subnode in node.nodes: + create_surface_elements(subnode, element) + + # Call the recursive function from the top node + create_surface_elements(self.region, xml_element) + + if self.temperature is not None: + if isinstance(self.temperature, Iterable): + element.set("temperature", ' '.join( + str(t) for t in self.temperature)) + else: + element.set("temperature", str(self.temperature)) + + if self.translation is not None: + element.set("translation", ' '.join(map(str, self.translation))) + + if self.rotation is not None: + element.set("rotation", ' '.join(map(str, self.rotation))) + + return element diff --git a/openmc/checkvalue.py b/openmc/checkvalue.py index 787052f5d..53f4b8368 100644 --- a/openmc/checkvalue.py +++ b/openmc/checkvalue.py @@ -41,25 +41,36 @@ def check_type(name, value, expected_type, expected_iter_type=None): Description of value being checked value : object Object to check type of - expected_type : type + expected_type : type or Iterable of type type to check object against - expected_iter_type : type or None, optional + expected_iter_type : type or Iterable of type or None, optional Expected type of each element in value, assuming it is iterable. If None, no check will be performed. """ if not _isinstance(value, expected_type): - msg = 'Unable to set "{0}" to "{1}" which is not of type "{2}"'.format( - name, value, expected_type.__name__) + if isinstance(expected_type, Iterable): + msg = 'Unable to set "{0}" to "{1}" which is not one of the ' \ + 'following types: "{2}"'.format(name, value, ', '.join( + [t.__name__ for t in expected_type])) + else: + msg = 'Unable to set "{0}" to "{1}" which is not of type "{2}"'.format( + name, value, expected_type.__name__) raise ValueError(msg) if expected_iter_type: for item in value: if not _isinstance(item, expected_iter_type): - msg = 'Unable to set "{0}" to "{1}" since each item must be ' \ - 'of type "{2}"'.format(name, value, - expected_iter_type.__name__) + if isinstance(expected_iter_type, Iterable): + msg = 'Unable to set "{0}" to "{1}" since each item must be ' \ + 'one of the following types: "{2}"'.format( + name, value, ', '.join([t.__name__ for t in + expected_iter_type])) + else: + msg = 'Unable to set "{0}" to "{1}" since each item must be ' \ + 'of type "{2}"'.format(name, value, + expected_iter_type.__name__) raise ValueError(msg) @@ -127,7 +138,7 @@ def check_iterable_type(name, value, expected_type, min_depth=1, max_depth=1): # But first, have we exceeded the max depth? if len(tree) > max_depth: msg = 'Error setting {0}: Found an iterable at {1}, items '\ - 'in that iterable excceed the maximum depth of {2}' \ + 'in that iterable exceed the maximum depth of {2}' \ .format(name, ind_str, max_depth) raise ValueError(msg) @@ -245,3 +256,50 @@ def check_greater_than(name, value, minimum, equality=False): msg = 'Unable to set "{0}" to "{1}" since it is less than ' \ 'or equal to "{2}"'.format(name, value, minimum) raise ValueError(msg) + + +class CheckedList(list): + """A list for which each element is type-checked as it's added + + Parameters + ---------- + expected_type : type or Iterable of type + Type(s) which each element should be + name : str + Name of data being checked + items : Iterable, optional + Items to initialize the list with + + """ + + def __init__(self, expected_type, name, items=[]): + self.expected_type = expected_type + self.name = name + for item in items: + self.append(item) + + def append(self, item): + """Append item to list + + Parameters + ---------- + item : object + Item to append + + """ + check_type(self.name, item, self.expected_type) + super(CheckedList, self).append(item) + + def insert(self, index, item): + """Insert item before index + + Parameters + ---------- + index : int + Index in list + item : object + Item to insert + + """ + check_type(self.name, item, self.expected_type) + super(CheckedList, self).insert(index, item) diff --git a/openmc/cmfd.py b/openmc/cmfd.py index c247719c9..b9977a288 100644 --- a/openmc/cmfd.py +++ b/openmc/cmfd.py @@ -69,7 +69,7 @@ class CMFDMesh(object): to any tallies far away from fission source neutron regions. A ``2`` must be used to identify any fission source region. -""" + """ def __init__(self): self._lower_left = None @@ -219,7 +219,7 @@ class CMFDFile(object): inner tolerance for Gauss-Seidel iterations when performing CMFD. ktol : float Tolerance on the eigenvalue when performing CMFD power iteration - cmfd_mesh : CMFDMesh + cmfd_mesh : openmc.CMFDMesh Structured mesh to be used for acceleration norm : float Normalization factor applied to the CMFD fission source distribution diff --git a/openmc/element.py b/openmc/element.py index 9f04abfda..219aafbdf 100644 --- a/openmc/element.py +++ b/openmc/element.py @@ -24,7 +24,7 @@ class Element(object): Chemical symbol of the element, e.g. Pu xs : str Cross section identifier, e.g. 71c - scattering : 'data' or 'iso-in-lab' or None + scattering : {'data', 'iso-in-lab', None} The type of angular scattering distribution to use """ @@ -57,6 +57,15 @@ class Element(object): def __ne__(self, other): return not self == other + def __gt__(self, other): + return repr(self) > repr(other) + + def __lt__(self, other): + return not self > other + + def __hash__(self): + return hash(repr(self)) + def __hash__(self): return hash(repr(self)) diff --git a/openmc/executor.py b/openmc/executor.py index 58cb91246..214517d6e 100644 --- a/openmc/executor.py +++ b/openmc/executor.py @@ -27,7 +27,8 @@ class Executor(object): # Launch a subprocess to run OpenMC p = subprocess.Popen(command, shell=True, cwd=self._working_directory, - stdout=subprocess.PIPE) + stdout=subprocess.PIPE, + universal_newlines=True) # Capture and re-print OpenMC output in real-time while True: diff --git a/openmc/filter.py b/openmc/filter.py index 54814a6b6..249bdcc02 100644 --- a/openmc/filter.py +++ b/openmc/filter.py @@ -40,11 +40,14 @@ class Filter(object): The bins for the filter num_bins : Integral The number of filter bins - mesh : Mesh or None + mesh : openmc.Mesh or None A Mesh object for 'mesh' type filters. stride : Integral The number of filter, nuclide and score bins within each of this filter's bins. + distribcell_paths : list of str + The paths traversed through the CSG tree to reach each distribcell + instance (for 'distribcell' filters only) """ @@ -56,6 +59,7 @@ class Filter(object): self._bins = None self._mesh = None self._stride = None + self._distribcell_paths = None if type is not None: self.type = type @@ -77,6 +81,25 @@ class Filter(object): def __ne__(self, other): return not self == other + def __gt__(self, other): + if self.type != other.type: + if self.type in _FILTER_TYPES and other.type in _FILTER_TYPES: + delta = _FILTER_TYPES.index(self.type) - \ + _FILTER_TYPES.index(other.type) + return delta > 0 + else: + return False + else: + # Compare largest/smallest energy bin edges in energy filters + # This logic is used when merging tallies with energy filters + if 'energy' in self.type and 'energy' in other.type: + return self.bins[0] >= other.bins[-1] + else: + return max(self.bins) > max(other.bins) + + def __lt__(self, other): + return not self > other + def __hash__(self): return hash(repr(self)) @@ -91,6 +114,7 @@ class Filter(object): clone._num_bins = self.num_bins clone._mesh = copy.deepcopy(self.mesh, memo) clone._stride = self.stride + clone._distribcell_paths = copy.deepcopy(self.distribcell_paths) memo[id(self)] = clone @@ -133,6 +157,10 @@ class Filter(object): def stride(self): return self._stride + @property + def distribcell_paths(self): + return self._distribcell_paths + @type.setter def type(self, type): if type is None: @@ -227,12 +255,17 @@ class Filter(object): self._stride = stride + @distribcell_paths.setter + def distribcell_paths(self, distribcell_paths): + cv.check_iterable_type('distribcell_paths', distribcell_paths, str) + self._distribcell_paths = distribcell_paths + def can_merge(self, other): """Determine if filter can be merged with another. Parameters ---------- - other : Filter + other : openmc.Filter Filter to compare with Returns @@ -246,20 +279,28 @@ class Filter(object): return False # Filters must be of the same type - elif self.type != other.type: + if self.type != other.type: return False # Distribcell filters cannot have more than one bin - elif self.type == 'distribcell': + if self.type == 'distribcell': return False # Mesh filters cannot have more than one bin elif self.type == 'mesh': return False - # Different energy bins are not mergeable + # Different energy bins structures must be mutually exclusive and + # share only one shared bin edge at the minimum or maximum energy elif 'energy' in self.type: - return False + # This low energy edge coincides with other's high energy edge + if self.bins[0] == other.bins[-1]: + return True + # This high energy edge coincides with other's low energy edge + elif self.bins[-1] == other.bins[0]: + return True + else: + return False else: return True @@ -269,12 +310,12 @@ class Filter(object): Parameters ---------- - other : Filter + other : openmc.Filter Filter to merge with Returns ------- - merged_filter : Filter + merged_filter : openmc.Filter Filter resulting from the merge """ @@ -288,9 +329,21 @@ class Filter(object): merged_filter = copy.deepcopy(self) # Merge unique filter bins - merged_bins = list(set(np.concatenate((self.bins, other.bins)))) - merged_filter.bins = merged_bins - merged_filter.num_bins = len(merged_bins) + merged_bins = np.concatenate((self.bins, other.bins)) + merged_bins = np.unique(merged_bins) + + # Sort energy bin edges + if 'energy' in self.type: + merged_bins = sorted(merged_bins) + + # Assign merged bins to merged filter + merged_filter.bins = list(merged_bins) + + # Count bins in the merged filter + if 'energy' in merged_filter.type: + merged_filter.num_bins = len(merged_bins) - 1 + else: + merged_filter.num_bins = len(merged_bins) return merged_filter @@ -302,7 +355,7 @@ class Filter(object): Parameters ---------- - other : Filter + other : openmc.Filter The filter to query as a subset of this filter Returns @@ -466,8 +519,8 @@ class Filter(object): """Builds a Pandas DataFrame for the Filter's bins. This method constructs a Pandas DataFrame object for the filter with - columns annotated by filter bin information. This is a helper method - for the Tally.get_pandas_dataframe(...) method. + columns annotated by filter bin information. This is a helper method for + :meth:`Tally.get_pandas_dataframe`. This capability has been tested for Pandas >=0.13.1. However, it is recommended to use v0.16 or newer versions of Pandas since this method @@ -477,7 +530,7 @@ class Filter(object): ---------- data_size : Integral The total number of bins in the tally corresponding to this filter - summary : None or Summary + summary : None or openmc.Summary An optional Summary object to be used to construct columns for distribcell tally filters (default is None). The geometric information in the Summary object is embedded into a Multi-index @@ -502,9 +555,9 @@ class Filter(object): 2. separate columns for the cell IDs, universe IDs, and lattice IDs and x,y,z cell indices corresponding to each (with summary info). - For 'energy' and 'energyout' filters, the DataFrame include a single - column with each element comprising a string with the lower, upper - energy bounds for each filter bin. + For 'energy' and 'energyout' filters, the DataFrame includes one + column for the lower energy bound and one column for the upper + energy bound for each filter bin. For 'mesh' filters, the DataFrame includes three columns for the x,y,z mesh cell indices corresponding to each filter bin. @@ -521,14 +574,8 @@ class Filter(object): """ - # Attempt to import Pandas - try: - import pandas as pd - except ImportError: - msg = 'The Pandas Python package must be installed on your system' - raise ImportError(msg) - # Initialize Pandas DataFrame + import pandas as pd df = pd.DataFrame() # mesh filters @@ -599,18 +646,10 @@ class Filter(object): # offsets to OpenCG LocalCoords linked lists offsets_to_coords = {} - # Use OpenCG to compute LocalCoords linked list for - # each region and store in dictionary - for region in range(num_regions): + for offset, path in enumerate(self.distribcell_paths): + region = opencg_geometry.get_region_from_path(path) coords = opencg_geometry.find_region(region) - path = opencg.get_path(coords) - cell_id = path[-1] - - # If this region is in Cell corresponding to the - # distribcell filter bin, store it in dictionary - if cell_id == self.bins[0]: - offset = openmc_geometry.get_cell_instance(path) - offsets_to_coords[offset] = coords + offsets_to_coords[offset] = coords # Each distribcell offset is a DataFrame bin # Unravel the paths into DataFrame columns @@ -707,7 +746,6 @@ class Filter(object): filter_bins = np.repeat(filter_bins, self.stride) tile_factor = data_size / len(filter_bins) filter_bins = np.tile(filter_bins, tile_factor) - filter_bins = filter_bins df = pd.DataFrame({self.type : filter_bins}) # If OpenCG level info DataFrame was created, concatenate @@ -719,21 +757,30 @@ class Filter(object): # energy, energyout filters elif 'energy' in self.type: - bins = self.bins - num_bins = self.num_bins + # Extract the lower and upper energy bounds, then repeat and tile + # them as necessary to account for other filters. + lo_bins = np.repeat(self.bins[:-1], self.stride) + hi_bins = np.repeat(self.bins[1:], self.stride) + tile_factor = data_size / len(lo_bins) + lo_bins = np.tile(lo_bins, tile_factor) + hi_bins = np.tile(hi_bins, tile_factor) - # Create strings for - template = '({0:.1e} - {1:.1e})' - filter_bins = [] - for i in range(num_bins): - filter_bins.append(template.format(bins[i], bins[i+1])) + # Add the new energy columns to the DataFrame. + df.loc[:, self.type + ' low [MeV]'] = lo_bins + df.loc[:, self.type + ' high [MeV]'] = hi_bins - # Tile the energy bins into a DataFrame column - filter_bins = np.repeat(filter_bins, self.stride) - tile_factor = data_size / len(filter_bins) - filter_bins = np.tile(filter_bins, tile_factor) - filter_bins = filter_bins - df = pd.concat([df, pd.DataFrame({self.type + ' [MeV]' : filter_bins})]) + elif self.type in ('azimuthal', 'polar'): + # Extract the lower and upper angle bounds, then repeat and tile + # them as necessary to account for other filters. + lo_bins = np.repeat(self.bins[:-1], self.stride) + hi_bins = np.repeat(self.bins[1:], self.stride) + tile_factor = data_size / len(lo_bins) + lo_bins = np.tile(lo_bins, tile_factor) + hi_bins = np.tile(hi_bins, tile_factor) + + # Add the new angle columns to the DataFrame. + df.loc[:, self.type + ' low'] = lo_bins + df.loc[:, self.type + ' high'] = hi_bins # universe, material, surface, cell, and cellborn filters else: diff --git a/openmc/geometry.py b/openmc/geometry.py index 9788671f5..f5dfe97e4 100644 --- a/openmc/geometry.py +++ b/openmc/geometry.py @@ -17,7 +17,7 @@ class Geometry(object): Attributes ---------- - root_universe : openmc.universe.Universe + root_universe : openmc.Universe Root universe which contains all others """ @@ -63,13 +63,19 @@ class Geometry(object): """ + # Extract the cell id from the path + last_index = path.rfind('>') + cell_id = int(path[last_index+1:]) + # Find the distribcell index of the cell. cells = self.get_all_cells() - if path[-1] in cells: - distribcell_index = cells[path[-1]].distribcell_index + for cell in cells: + if cell.id == cell_id: + distribcell_index = cell.distribcell_index + break else: raise RuntimeError('Could not find cell {} specified in a \ - distribcell filter'.format(path[-1])) + distribcell filter'.format(cell_id)) # Return memoize'd offset if possible if (path, distribcell_index) in self._offsets: @@ -89,31 +95,48 @@ class Geometry(object): Returns ------- - list of openmc.universe.Cell + list of openmc.Cell Cells in the geometry """ - return self._root_universe.get_all_cells() + all_cells = self._root_universe.get_all_cells() + cells = set() + + for cell in all_cells.values(): + if cell._type == 'normal': + cells.add(cell) + + cells = list(cells) + cells.sort(key=lambda x: x.id) + return cells def get_all_universes(self): """Return all universes defined Returns ------- - list of openmc.universe.Universe + list of openmc.Universe Universes in the geometry """ - return self._root_universe.get_all_universes() + all_universes = self._root_universe.get_all_universes() + universes = set() + + for universe in all_universes.values(): + universes.add(universe) + + universes = list(universes) + universes.sort(key=lambda x: x.id) + return universes def get_all_nuclides(self): """Return all nuclides assigned to a material in the geometry Returns ------- - list of openmc.nuclide.Nuclide + list of openmc.Nuclide Nuclides in the geometry """ @@ -131,7 +154,7 @@ class Geometry(object): Returns ------- - list of openmc.material.Material + list of openmc.Material Materials in the geometry """ @@ -150,10 +173,19 @@ class Geometry(object): return materials def get_all_material_cells(self): + """Return all cells filled by a material + + Returns + ------- + list of openmc.Cell + Cells filled by Materials in the geometry + + """ + all_cells = self.get_all_cells() material_cells = set() - for cell_id, cell in all_cells.items(): + for cell in all_cells: if cell._type == 'normal': material_cells.add(cell) @@ -166,7 +198,7 @@ class Geometry(object): Returns ------- - list of openmc.universe.Universe + list of openmc.Universe Universes with non-fill cells """ @@ -174,9 +206,9 @@ class Geometry(object): all_universes = self.get_all_universes() material_universes = set() - for universe_id, universe in all_universes.items(): - cells = universe._cells - for cell_id, cell in cells.items(): + for universe in all_universes: + cells = universe.cells + for cell in cells: if cell._type == 'normal': material_universes.add(universe) @@ -184,6 +216,227 @@ class Geometry(object): material_universes.sort(key=lambda x: x.id) return material_universes + def get_all_lattices(self): + """Return all lattices defined + + Returns + ------- + list of openmc.Lattice + Lattices in the geometry + + """ + + cells = self.get_all_cells() + lattices = set() + + for cell in cells: + if isinstance(cell.fill, openmc.Lattice): + lattices.add(cell.fill) + + lattices = list(lattices) + lattices.sort(key=lambda x: x.id) + return lattices + + def get_materials_by_name(self, name, case_sensitive=False, matching=False): + """Return a list of materials with matching names. + + Parameters + ---------- + name : str + The name to match + case_sensitive : bool + Whether to distinguish upper and lower case letters in each + material's name (default is True) + matching : bool + Whether the names must match completely (default is True) + + Returns + ------- + list of openmc.Material + Materials matching the queried name + + """ + + if not case_sensitive: + name = name.lower() + + all_materials = self.get_all_materials() + materials = set() + + for material in all_materials: + material_name = material.name + if not case_sensitive: + material_name = material_name.lower() + + if material_name == name: + materials.add(material) + elif not matching and name in material_name: + materials.add(material) + + materials = list(materials) + materials.sort(key=lambda x: x.id) + return materials + + def get_cells_by_name(self, name, case_sensitive=False, matching=False): + """Return a list of cells with matching names. + + Parameters + ---------- + name : str + The name to search match + case_sensitive : bool + Whether to distinguish upper and lower case letters in each + cell's name (default is True) + matching : bool + Whether the names must match completely (default is True) + + Returns + ------- + list of openmc.Cell + Cells matching the queried name + + """ + + if not case_sensitive: + name = name.lower() + + all_cells = self.get_all_cells() + cells = set() + + for cell in all_cells: + cell_name = cell.name + if not case_sensitive: + cell_name = cell_name.lower() + + if cell_name == name: + cells.add(cell) + elif not matching and name in cell_name: + cells.add(cell) + + cells = list(cells) + cells.sort(key=lambda x: x.id) + return cells + + def get_cells_by_fill_name(self, name, case_sensitive=False, matching=False): + """Return a list of cells with fills with matching names. + + Parameters + ---------- + name : str + The name to match + case_sensitive : bool + Whether to distinguish upper and lower case letters in each + cell's name (default is True) + matching : bool + Whether the names must match completely (default is True) + + Returns + ------- + list of openmc.Cell + Cells with fills matching the queried name + + """ + + if not case_sensitive: + name = name.lower() + + all_cells = self.get_all_cells() + cells = set() + + for cell in all_cells: + cell_fill_name = cell.fill.name + if not case_sensitive: + cell_fill_name = cell_fill_name.lower() + + if cell_fill_name == name: + cells.add(cell) + elif not matching and name in cell_fill_name: + cells.add(cell) + + cells = list(cells) + cells.sort(key=lambda x: x.id) + return cells + + def get_universes_by_name(self, name, case_sensitive=False, matching=False): + """Return a list of universes with matching names. + + Parameters + ---------- + name : str + The name to match + case_sensitive : bool + Whether to distinguish upper and lower case letters in each + universe's name (default is True) + matching : bool + Whether the names must match completely (default is True) + + Returns + ------- + list of openmc.Universe + Universes matching the queried name + + """ + + if not case_sensitive: + name = name.lower() + + all_universes = self.get_all_universes() + universes = set() + + for universe in all_universes: + universe_name = universe.name + if not case_sensitive: + universe_name = universe_name.lower() + + if universe_name == name: + universes.add(universe) + elif not matching and name in universe_name: + universes.add(universe) + + universes = list(universes) + universes.sort(key=lambda x: x.id) + return universes + + def get_lattices_by_name(self, name, case_sensitive=False, matching=False): + """Return a list of lattices with matching names. + + Parameters + ---------- + name : str + The name to match + case_sensitive : bool + Whether to distinguish upper and lower case letters in each + lattice's name (default is True) + matching : bool + Whether the names must match completely (default is True) + + Returns + ------- + list of openmc.Lattice + Lattices matching the queried name + + """ + + if not case_sensitive: + name = name.lower() + + all_lattices = self.get_all_lattices() + lattices = set() + + for lattice in all_lattices: + lattice_name = lattice.name + if not case_sensitive: + lattice_name = lattice_name.lower() + + if lattice_name == name: + lattices.add(lattice) + elif not matching and name in lattice_name: + lattices.add(lattice) + + lattices = list(lattices) + lattices.sort(key=lambda x: x.id) + return lattices + class GeometryFile(object): """Geometry file used for an OpenMC simulation. Corresponds directly to the @@ -191,7 +444,7 @@ class GeometryFile(object): Attributes ---------- - geometry : Geometry + geometry : openmc.Geometry The geometry to be used """ diff --git a/openmc/lattice.py b/openmc/lattice.py new file mode 100644 index 000000000..7e78abf06 --- /dev/null +++ b/openmc/lattice.py @@ -0,0 +1,871 @@ +import abc +from collections import OrderedDict, Iterable +from numbers import Real, Integral +from xml.etree import ElementTree as ET +import sys + +import numpy as np + +import openmc.checkvalue as cv +from openmc.universe import Universe, AUTO_UNIVERSE_ID + +if sys.version_info[0] >= 3: + basestring = str + + +class Lattice(object): + """A repeating structure wherein each element is a universe. + + Parameters + ---------- + lattice_id : int, optional + Unique identifier for the lattice. If not specified, an identifier will + automatically be assigned. + name : str, optional + Name of the lattice. If not specified, the name is the empty string. + + Attributes + ---------- + id : int + Unique identifier for the lattice + name : str + Name of the lattice + pitch : float + Pitch of the lattice in cm + outer : int + The unique identifier of a universe to fill all space outside the + lattice + universes : numpy.ndarray of openmc.Universe + An array of universes filling each element of the lattice + + """ + + # This is an abstract class which cannot be instantiated + __metaclass__ = abc.ABCMeta + + def __init__(self, lattice_id=None, name=''): + # Initialize Lattice class attributes + self.id = lattice_id + self.name = name + self._pitch = None + self._outer = None + self._universes = None + + def __eq__(self, other): + if not isinstance(other, Lattice): + return False + elif self.id != other.id: + return False + elif self.name != other.name: + return False + elif self.pitch != other.pitch: + return False + elif self.outer != other.outer: + return False + elif self.universes != other.universes: + return False + else: + return True + + def __ne__(self, other): + return not self == other + + @property + def id(self): + return self._id + + @property + def name(self): + return self._name + + @property + def pitch(self): + return self._pitch + + @property + def outer(self): + return self._outer + + @property + def universes(self): + return self._universes + + @id.setter + def id(self, lattice_id): + if lattice_id is None: + global AUTO_UNIVERSE_ID + self._id = AUTO_UNIVERSE_ID + AUTO_UNIVERSE_ID += 1 + else: + cv.check_type('lattice ID', lattice_id, Integral) + cv.check_greater_than('lattice ID', lattice_id, 0, equality=True) + self._id = lattice_id + + @name.setter + def name(self, name): + if name is not None: + cv.check_type('lattice name', name, basestring) + self._name = name + else: + self._name = '' + + @outer.setter + def outer(self, outer): + cv.check_type('outer universe', outer, Universe) + self._outer = outer + + @universes.setter + def universes(self, universes): + cv.check_iterable_type('lattice universes', universes, Universe, + min_depth=2, max_depth=3) + self._universes = np.asarray(universes) + + def get_unique_universes(self): + """Determine all unique universes in the lattice + + Returns + ------- + universes : collections.OrderedDict + Dictionary whose keys are universe IDs and values are + :class:`Universe` instances + + """ + + univs = OrderedDict() + for k in range(len(self._universes)): + for j in range(len(self._universes[k])): + if isinstance(self._universes[k][j], Universe): + u = self._universes[k][j] + univs[u._id] = u + else: + for i in range(len(self._universes[k][j])): + u = self._universes[k][j][i] + assert isinstance(u, Universe) + univs[u._id] = u + + if self.outer is not None: + univs[self.outer._id] = self.outer + + return univs + + def get_all_nuclides(self): + """Return all nuclides contained in the lattice + + Returns + ------- + nuclides : collections.OrderedDict + Dictionary whose keys are nuclide names and values are 2-tuples of + (nuclide, density) + + """ + + nuclides = OrderedDict() + + # Get all unique Universes contained in each of the lattice cells + unique_universes = self.get_unique_universes() + + # Append all Universes containing each cell to the dictionary + for universe_id, universe in unique_universes.items(): + nuclides.update(universe.get_all_nuclides()) + + return nuclides + + def get_all_cells(self): + """Return all cells that are contained within the lattice + + Returns + ------- + cells : collections.OrderedDict + Dictionary whose keys are cell IDs and values are :class:`Cell` + instances + + """ + + cells = OrderedDict() + unique_universes = self.get_unique_universes() + + for universe_id, universe in unique_universes.items(): + cells.update(universe.get_all_cells()) + + return cells + + def get_all_materials(self): + """Return all materials that are contained within the lattice + + Returns + ------- + materials : collections.OrderedDict + Dictionary whose keys are material IDs and values are + :class:`Material` instances + + """ + + materials = OrderedDict() + + # Append all Cells in each Cell in the Universe to the dictionary + cells = self.get_all_cells() + for cell_id, cell in cells.items(): + materials.update(cell.get_all_materials()) + + return materials + + def get_all_universes(self): + """Return all universes that are contained within the lattice + + Returns + ------- + universes : collections.OrderedDict + Dictionary whose keys are universe IDs and values are + :class:`Universe` instances + + """ + + # Initialize a dictionary of all Universes contained by the Lattice + # in each nested Universe level + all_universes = OrderedDict() + + # Get all unique Universes contained in each of the lattice cells + unique_universes = self.get_unique_universes() + + # Add the unique Universes filling each Lattice cell + all_universes.update(unique_universes) + + # Append all Universes containing each cell to the dictionary + for universe_id, universe in unique_universes.items(): + all_universes.update(universe.get_all_universes()) + + return all_universes + + +class RectLattice(Lattice): + """A lattice consisting of rectangular prisms. + + Parameters + ---------- + lattice_id : int, optional + Unique identifier for the lattice. If not specified, an identifier will + automatically be assigned. + name : str, optional + Name of the lattice. If not specified, the name is the empty string. + + Attributes + ---------- + id : int + Unique identifier for the lattice + name : str + Name of the lattice + dimension : Iterable of int + An array of two or three integers representing the number of lattice + cells in the x- and y- (and z-) directions, respectively. + lower_left : Iterable of float + The coordinates of the lower-left corner of the lattice. If the lattice + is two-dimensional, only the x- and y-coordinates are specified. + + """ + + def __init__(self, lattice_id=None, name=''): + super(RectLattice, self).__init__(lattice_id, name) + + # Initialize Lattice class attributes + self._dimension = None + self._lower_left = None + self._offsets = None + + def __eq__(self, other): + if not isinstance(other, RectLattice): + return False + elif not super(RectLattice, self).__eq__(other): + return False + elif self.dimension != other.dimension: + return False + elif self.lower_left != other.lower_left: + return False + else: + return True + + def __ne__(self, other): + return not self == other + + def __hash__(self): + return hash(repr(self)) + + def __repr__(self): + string = 'RectLattice\n' + string += '{0: <16}{1}{2}\n'.format('\tID', '=\t', self._id) + string += '{0: <16}{1}{2}\n'.format('\tName', '=\t', self._name) + string += '{0: <16}{1}{2}\n'.format('\tDimension', '=\t', + self._dimension) + string += '{0: <16}{1}{2}\n'.format('\tLower Left', '=\t', + self._lower_left) + string += '{0: <16}{1}{2}\n'.format('\tPitch', '=\t', self._pitch) + + if self._outer is not None: + string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', + self._outer._id) + else: + string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', + self._outer) + + string += '{0: <16}\n'.format('\tUniverses') + + # Lattice nested Universe IDs - column major for Fortran + for i, universe in enumerate(np.ravel(self._universes)): + string += '{0} '.format(universe._id) + + # Add a newline character every time we reach end of row of cells + if (i+1) % self._dimension[-1] == 0: + string += '\n' + + string = string.rstrip('\n') + + if self._offsets is not None: + string += '{0: <16}\n'.format('\tOffsets') + + # Lattice cell offsets + for i, offset in enumerate(np.ravel(self._offsets)): + string += '{0} '.format(offset) + + # Add a newline character when we reach end of row of cells + if (i+1) % self._dimension[-1] == 0: + string += '\n' + + string = string.rstrip('\n') + + return string + + @property + def dimension(self): + return self._dimension + + @property + def lower_left(self): + return self._lower_left + + @property + def offsets(self): + return self._offsets + + @dimension.setter + def dimension(self, dimension): + cv.check_type('lattice dimension', dimension, Iterable, Integral) + cv.check_length('lattice dimension', dimension, 2, 3) + for dim in dimension: + cv.check_greater_than('lattice dimension', dim, 0) + self._dimension = dimension + + @lower_left.setter + def lower_left(self, lower_left): + cv.check_type('lattice lower left corner', lower_left, Iterable, Real) + cv.check_length('lattice lower left corner', lower_left, 2, 3) + self._lower_left = lower_left + + @offsets.setter + def offsets(self, offsets): + cv.check_type('lattice offsets', offsets, Iterable) + self._offsets = offsets + + @Lattice.pitch.setter + def pitch(self, pitch): + cv.check_type('lattice pitch', pitch, Iterable, Real) + cv.check_length('lattice pitch', pitch, 2, 3) + for dim in pitch: + cv.check_greater_than('lattice pitch', dim, 0.0) + self._pitch = pitch + + def get_cell_instance(self, path, distribcell_index): + + # Extract the lattice element from the path + next_index = path.index('-') + lat_id_indices = path[:next_index] + path = path[next_index+2:] + + # Extract the lattice cell indices from the path + i1 = lat_id_indices.index('(') + i2 = lat_id_indices.index(')') + i = lat_id_indices[i1+1:i2] + lat_x = int(i.split(',')[0]) - 1 + lat_y = int(i.split(',')[1]) - 1 + lat_z = int(i.split(',')[2]) - 1 + + # For 2D Lattices + if len(self._dimension) == 2: + offset = self._offsets[lat_z, lat_y, lat_x, distribcell_index-1] + offset += self._universes[lat_x][lat_y].get_cell_instance(path, + distribcell_index) + + # For 3D Lattices + else: + offset = self._offsets[lat_z, lat_y, lat_x, distribcell_index-1] + offset += self._universes[lat_z][lat_y][lat_x].get_cell_instance( + path, distribcell_index) + + return offset + + def create_xml_subelement(self, xml_element): + + # Determine if XML element already contains subelement for this Lattice + path = './lattice[@id=\'{0}\']'.format(self._id) + test = xml_element.find(path) + + # If the element does contain the Lattice subelement, then return + if test is not None: + return + + lattice_subelement = ET.Element("lattice") + lattice_subelement.set("id", str(self._id)) + + if len(self._name) > 0: + lattice_subelement.set("name", str(self._name)) + + # Export the Lattice cell pitch + pitch = ET.SubElement(lattice_subelement, "pitch") + pitch.text = ' '.join(map(str, self._pitch)) + + # Export the Lattice outer Universe (if specified) + if self._outer is not None: + outer = ET.SubElement(lattice_subelement, "outer") + outer.text = '{0}'.format(self._outer._id) + self._outer.create_xml_subelement(xml_element) + + # Export Lattice cell dimensions + dimension = ET.SubElement(lattice_subelement, "dimension") + dimension.text = ' '.join(map(str, self._dimension)) + + # Export Lattice lower left + lower_left = ET.SubElement(lattice_subelement, "lower_left") + lower_left.text = ' '.join(map(str, self._lower_left)) + + # Export the Lattice nested Universe IDs - column major for Fortran + universe_ids = '\n' + + # 3D Lattices + if len(self._dimension) == 3: + for z in range(self._dimension[2]): + for y in range(self._dimension[1]): + for x in range(self._dimension[0]): + universe = self._universes[z][y][x] + + # Append Universe ID to the Lattice XML subelement + universe_ids += '{0} '.format(universe._id) + + # Create XML subelement for this Universe + universe.create_xml_subelement(xml_element) + + # Add newline character when we reach end of row of cells + universe_ids += '\n' + + # Add newline character when we reach end of row of cells + universe_ids += '\n' + + # 2D Lattices + else: + for y in range(self._dimension[1]): + for x in range(self._dimension[0]): + universe = self._universes[y][x] + + # Append Universe ID to Lattice XML subelement + universe_ids += '{0} '.format(universe._id) + + # Create XML subelement for this Universe + universe.create_xml_subelement(xml_element) + + # Add newline character when we reach end of row of cells + universe_ids += '\n' + + # Remove trailing newline character from Universe IDs string + universe_ids = universe_ids.rstrip('\n') + + universes = ET.SubElement(lattice_subelement, "universes") + universes.text = universe_ids + + # Append the XML subelement for this Lattice to the XML element + xml_element.append(lattice_subelement) + + +class HexLattice(Lattice): + """A lattice consisting of hexagonal prisms. + + Parameters + ---------- + lattice_id : int, optional + Unique identifier for the lattice. If not specified, an identifier will + automatically be assigned. + name : str, optional + Name of the lattice. If not specified, the name is the empty string. + + Attributes + ---------- + id : int + Unique identifier for the lattice + name : str + Name of the lattice + num_rings : int + Number of radial ring positions in the xy-plane + num_axial : int + Number of positions along the z-axis. + center : Iterable of float + Coordinates of the center of the lattice. If the lattice does not have + axial sections then only the x- and y-coordinates are specified + + """ + + def __init__(self, lattice_id=None, name=''): + super(HexLattice, self).__init__(lattice_id, name) + + # Initialize Lattice class attributes + self._num_rings = None + self._num_axial = None + self._center = None + + def __eq__(self, other): + if not isinstance(other, HexLattice): + return False + elif not super(HexLattice, self).__eq__(other): + return False + elif self.num_rings != other.num_rings: + return False + elif self.num_axial != other.num_axial: + return False + elif self.center != other.center: + return False + else: + return True + + def __ne__(self, other): + return not self == other + + def __hash__(self): + return hash(repr(self)) + + def __repr__(self): + string = 'HexLattice\n' + string += '{0: <16}{1}{2}\n'.format('\tID', '=\t', self._id) + string += '{0: <16}{1}{2}\n'.format('\tName', '=\t', self._name) + string += '{0: <16}{1}{2}\n'.format('\t# Rings', '=\t', self._num_rings) + string += '{0: <16}{1}{2}\n'.format('\t# Axial', '=\t', self._num_axial) + string += '{0: <16}{1}{2}\n'.format('\tCenter', '=\t', + self._center) + string += '{0: <16}{1}{2}\n'.format('\tPitch', '=\t', self._pitch) + + if self._outer is not None: + string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', + self._outer._id) + else: + string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', + self._outer) + + string += '{0: <16}\n'.format('\tUniverses') + + if self._num_axial is not None: + slices = [self._repr_axial_slice(x) for x in self._universes] + string += '\n'.join(slices) + + else: + string += self._repr_axial_slice(self._universes) + + return string + + @property + def num_rings(self): + return self._num_rings + + @property + def num_axial(self): + return self._num_axial + + @property + def center(self): + return self._center + + @num_rings.setter + def num_rings(self, num_rings): + cv.check_type('number of rings', num_rings, Integral) + cv.check_greater_than('number of rings', num_rings, 0) + self._num_rings = num_rings + + @num_axial.setter + def num_axial(self, num_axial): + cv.check_type('number of axial', num_axial, Integral) + cv.check_greater_than('number of axial', num_axial, 0) + self._num_axial = num_axial + + @center.setter + def center(self, center): + cv.check_type('lattice center', center, Iterable, Real) + cv.check_length('lattice center', center, 2, 3) + self._center = center + + @Lattice.pitch.setter + def pitch(self, pitch): + cv.check_type('lattice pitch', pitch, Iterable, Real) + cv.check_length('lattice pitch', pitch, 1, 2) + for dim in pitch: + cv.check_greater_than('lattice pitch', dim, 0) + self._pitch = pitch + + @Lattice.universes.setter + def universes(self, universes): + # Call Lattice.universes parent class setter property + Lattice.universes.fset(self, universes) + + # NOTE: This routine assumes that the user creates a "ragged" list of + # lists, where each sub-list corresponds to one ring of Universes. + # The sub-lists are ordered from outermost ring to innermost ring. + # The Universes within each sub-list are ordered from the "top" in a + # clockwise fashion. + + # Check to see if the given universes look like a 2D or a 3D array. + if isinstance(self._universes[0][0], Universe): + n_dims = 2 + + elif isinstance(self._universes[0][0][0], Universe): + n_dims = 3 + + else: + msg = 'HexLattice ID={0:d} does not appear to be either 2D or ' \ + '3D. Make sure set_universes was given a two-deep or ' \ + 'three-deep iterable of universes.'.format(self._id) + raise RuntimeError(msg) + + # Set the number of axial positions. + if n_dims == 3: + self.num_axial = len(self._universes) + else: + self._num_axial = None + + # Set the number of rings and make sure this number is consistent for + # all axial positions. + if n_dims == 3: + self.num_rings = len(self._universes) + for rings in self._universes: + if len(rings) != self._num_rings: + msg = 'HexLattice ID={0:d} has an inconsistent number of ' \ + 'rings per axial positon'.format(self._id) + raise ValueError(msg) + + else: + self.num_rings = len(self._universes) + + # Make sure there are the correct number of elements in each ring. + if n_dims == 3: + for axial_slice in self._universes: + # Check the center ring. + if len(axial_slice[-1]) != 1: + msg = 'HexLattice ID={0:d} has the wrong number of ' \ + 'elements in the innermost ring. Only 1 element is ' \ + 'allowed in the innermost ring.'.format(self._id) + raise ValueError(msg) + + # Check the outer rings. + for r in range(self._num_rings-1): + if len(axial_slice[r]) != 6*(self._num_rings - 1 - r): + msg = 'HexLattice ID={0:d} has the wrong number of ' \ + 'elements in ring number {1:d} (counting from the '\ + 'outermost ring). This ring should have {2:d} ' \ + 'elements.'.format(self._id, r, + 6*(self._num_rings - 1 - r)) + raise ValueError(msg) + + else: + axial_slice = self._universes + # Check the center ring. + if len(axial_slice[-1]) != 1: + msg = 'HexLattice ID={0:d} has the wrong number of ' \ + 'elements in the innermost ring. Only 1 element is ' \ + 'allowed in the innermost ring.'.format(self._id) + raise ValueError(msg) + + # Check the outer rings. + for r in range(self._num_rings-1): + if len(axial_slice[r]) != 6*(self._num_rings - 1 - r): + msg = 'HexLattice ID={0:d} has the wrong number of ' \ + 'elements in ring number {1:d} (counting from the '\ + 'outermost ring). This ring should have {2:d} ' \ + 'elements.'.format(self._id, r, + 6*(self._num_rings - 1 - r)) + raise ValueError(msg) + + def create_xml_subelement(self, xml_element): + # Determine if XML element already contains subelement for this Lattice + path = './hex_lattice[@id=\'{0}\']'.format(self._id) + test = xml_element.find(path) + + # If the element does contain the Lattice subelement, then return + if test is not None: + return + + lattice_subelement = ET.Element("hex_lattice") + lattice_subelement.set("id", str(self._id)) + + if len(self._name) > 0: + lattice_subelement.set("name", str(self._name)) + + # Export the Lattice cell pitch + pitch = ET.SubElement(lattice_subelement, "pitch") + pitch.text = ' '.join(map(str, self._pitch)) + + # Export the Lattice outer Universe (if specified) + if self._outer is not None: + outer = ET.SubElement(lattice_subelement, "outer") + outer.text = '{0}'.format(self._outer._id) + self._outer.create_xml_subelement(xml_element) + + lattice_subelement.set("n_rings", str(self._num_rings)) + + if self._num_axial is not None: + lattice_subelement.set("n_axial", str(self._num_axial)) + + # Export Lattice cell center + dimension = ET.SubElement(lattice_subelement, "center") + dimension.text = ' '.join(map(str, self._center)) + + # Export the Lattice nested Universe IDs. + + # 3D Lattices + if self._num_axial is not None: + slices = [] + for z in range(self._num_axial): + # Initialize the center universe. + universe = self._universes[z][-1][0] + universe.create_xml_subelement(xml_element) + + # Initialize the remaining universes. + for r in range(self._num_rings-1): + for theta in range(6*(self._num_rings - 1 - r)): + universe = self._universes[z][r][theta] + universe.create_xml_subelement(xml_element) + + # Get a string representation of the universe IDs. + slices.append(self._repr_axial_slice(self._universes[z])) + + # Collapse the list of axial slices into a single string. + universe_ids = '\n'.join(slices) + + # 2D Lattices + else: + # Initialize the center universe. + universe = self._universes[-1][0] + universe.create_xml_subelement(xml_element) + + # Initialize the remaining universes. + for r in range(self._num_rings - 1): + for theta in range(6*(self._num_rings - 1 - r)): + universe = self._universes[r][theta] + universe.create_xml_subelement(xml_element) + + # Get a string representation of the universe IDs. + universe_ids = self._repr_axial_slice(self._universes) + + universes = ET.SubElement(lattice_subelement, "universes") + universes.text = '\n' + universe_ids + + # Append the XML subelement for this Lattice to the XML element + xml_element.append(lattice_subelement) + + def _repr_axial_slice(self, universes): + """Return string representation for the given 2D group of universes. + + The 'universes' argument should be a list of lists of universes where + each sub-list represents a single ring. The first list should be the + outer ring. + """ + + # Find the largest universe ID and count the number of digits so we can + # properly pad the output string later. + largest_id = max([max([univ._id for univ in ring]) + for ring in universes]) + n_digits = len(str(largest_id)) + pad = ' '*n_digits + id_form = '{: ^' + str(n_digits) + 'd}' + + # Initialize the list for each row. + rows = [[] for i in range(1 + 4 * (self._num_rings-1))] + middle = 2 * (self._num_rings - 1) + + # Start with the degenerate first ring. + universe = universes[-1][0] + rows[middle] = [id_form.format(universe._id)] + + # Add universes one ring at a time. + for r in range(1, self._num_rings): + # r_prime increments down while r increments up. + r_prime = self._num_rings - 1 - r + theta = 0 + y = middle + 2*r + + # Climb down the top-right. + for i in range(r): + # Add the universe. + universe = universes[r_prime][theta] + rows[y].append(id_form.format(universe._id)) + + # Translate the indices. + y -= 1 + theta += 1 + + # Climb down the right. + for i in range(r): + # Add the universe. + universe = universes[r_prime][theta] + rows[y].append(id_form.format(universe._id)) + + # Translate the indices. + y -= 2 + theta += 1 + + # Climb down the bottom-right. + for i in range(r): + # Add the universe. + universe = universes[r_prime][theta] + rows[y].append(id_form.format(universe._id)) + + # Translate the indices. + y -= 1 + theta += 1 + + # Climb up the bottom-left. + for i in range(r): + # Add the universe. + universe = universes[r_prime][theta] + rows[y].insert(0, id_form.format(universe._id)) + + # Translate the indices. + y += 1 + theta += 1 + + # Climb up the left. + for i in range(r): + # Add the universe. + universe = universes[r_prime][theta] + rows[y].insert(0, id_form.format(universe._id)) + + # Translate the indices. + y += 2 + theta += 1 + + # Climb up the top-left. + for i in range(r): + # Add the universe. + universe = universes[r_prime][theta] + rows[y].insert(0, id_form.format(universe._id)) + + # Translate the indices. + y += 1 + theta += 1 + + # Flip the rows and join each row into a single string. + rows = [pad.join(x) for x in rows[::-1]] + + # Pad the beginning of the rows so they line up properly. + for y in range(self._num_rings - 1): + rows[y] = (self._num_rings - 1 - y)*pad + rows[y] + rows[-1 - y] = (self._num_rings - 1 - y)*pad + rows[-1 - y] + + for y in range(self._num_rings % 2, self._num_rings, 2): + rows[middle + y] = pad + rows[middle + y] + if y != 0: + rows[middle - y] = pad + rows[middle - y] + + # Join the rows together and return the string. + universe_ids = '\n'.join(rows) + return universe_ids diff --git a/openmc/macroscopic.py b/openmc/macroscopic.py new file mode 100644 index 000000000..9f67a50ba --- /dev/null +++ b/openmc/macroscopic.py @@ -0,0 +1,85 @@ +from numbers import Integral +import sys + +from openmc.checkvalue import check_type + +if sys.version_info[0] >= 3: + basestring = str + + +class Macroscopic(object): + """A Macroscopic object that can be used in a material. + + Parameters + ---------- + name : str + Name of the macroscopic data, e.g. UO2 + xs : str + Cross section identifier, e.g. 71c + + Attributes + ---------- + name : str + Name of the nuclide, e.g. UO2 + xs : str + Cross section identifier, e.g. 71c + + """ + + def __init__(self, name='', xs=None): + # Initialize class attributes + self._name = '' + self._xs = None + + # Set the Material class attributes + self.name = name + + if xs is not None: + self.xs = xs + + def __eq__(self, other): + if isinstance(other, Macroscopic): + if self._name != other._name: + return False + elif self._xs != other._xs: + return False + else: + return True + elif isinstance(other, basestring) and other == self.name: + return True + else: + return False + + def __ne__(self, other): + return not self == other + + def __hash__(self): + return hash((self._name, self._xs)) + + def __repr__(self): + string = 'Nuclide - {0}\n'.format(self._name) + string += '{0: <16}{1}{2}\n'.format('\tXS', '=\t', self._xs) + return string + + @property + def name(self): + return self._name + + @property + def xs(self): + return self._xs + + @name.setter + def name(self, name): + check_type('name', name, basestring) + self._name = name + + @xs.setter + def xs(self, xs): + check_type('cross-section identifier', xs, basestring) + self._xs = xs + + def __repr__(self): + string = 'Macroscopic - {0}\n'.format(self._name) + string += '{0: <16}{1}{2}\n'.format('\tXS', '=\t', self.xs) + return string diff --git a/openmc/material.py b/openmc/material.py index 542078c7c..2c04a9ecf 100644 --- a/openmc/material.py +++ b/openmc/material.py @@ -22,14 +22,15 @@ def reset_auto_material_id(): # Units for density supported by OpenMC -DENSITY_UNITS = ['g/cm3', 'g/cc', 'kg/cm3', 'atom/b-cm', 'atom/cm3', 'sum'] +DENSITY_UNITS = ['g/cm3', 'g/cc', 'kg/cm3', 'atom/b-cm', 'atom/cm3', 'sum', + 'macro'] # Constant for density when not needed NO_DENSITY = 99999. class Material(object): - """A material composed of a collection of nuclides/elements that can be + """A material composed of a collection of nuclides/elements that can be assigned to a region of space. Parameters @@ -49,7 +50,8 @@ class Material(object): Density of the material (units defined separately) density_units : str Units used for `density`. Can be one of 'g/cm3', 'g/cc', 'kg/cm3', - 'atom/b-cm', 'atom/cm3', or 'sum'. + 'atom/b-cm', 'atom/cm3', 'sum', or 'macro'. The 'macro' unit only + applies in the case of a multi-group calculation. """ @@ -65,6 +67,10 @@ class Material(object): # Values - tuple (nuclide, percent, percent type) self._nuclides = OrderedDict() + # The single instance of Macroscopic data present in this material + # (only one is allowed, hence this is different than _nuclides, etc) + self._macroscopic = None + # An ordered dictionary of Elements (order affects OpenMC results) # Keys - Element names # Values - tuple (element, percent, percent type) @@ -128,6 +134,10 @@ class Material(object): string += '{0: <16}'.format('\t{0}'.format(nuclide)) string += '=\t{0: <12} [{1}]\n'.format(percent, percent_type) + if self._macroscopic is not None: + string += '{0: <16}\n'.format('\tMacroscopic Data') + string += '{0: <16}'.format('\t{0}'.format(self._macroscopic)) + string += '{0: <16}\n'.format('\tElements') for element in self._elements: @@ -149,6 +159,7 @@ class Material(object): clone._density = self._density clone._density_units = self._density_units clone._nuclides = deepcopy(self._nuclides, memo) + clone._macroscopic = self._macroscopic clone._elements = deepcopy(self._elements, memo) clone._sab = deepcopy(self._sab, memo) clone._convert_to_distrib_comps = self._convert_to_distrib_comps @@ -259,7 +270,7 @@ class Material(object): Parameters ---------- - nuclide : str or openmc.nuclide.Nuclide + nuclide : str or openmc.Nuclide Nuclide to add percent : float Atom or weight percent @@ -268,6 +279,11 @@ class Material(object): """ + if self._macroscopic is not None: + msg = 'Unable to add a Nuclide to Material ID="{0}" as a ' \ + 'macroscopic data-set has already been added'.format(self._id) + raise ValueError(msg) + if not isinstance(nuclide, (openmc.Nuclide, str)): msg = 'Unable to add a Nuclide to Material ID="{0}" with a ' \ 'non-Nuclide value "{1}"'.format(self._id, nuclide) @@ -297,7 +313,7 @@ class Material(object): Parameters ---------- - nuclide : openmc.nuclide.Nuclide + nuclide : openmc.Nuclide Nuclide to remove """ @@ -311,12 +327,70 @@ class Material(object): if nuclide._name in self._nuclides: del self._nuclides[nuclide._name] + def add_macroscopic(self, macroscopic): + """Add a macroscopic to the material + + Parameters + ---------- + macroscopic : str or openmc.Macroscopic + Macroscopic to add + + """ + + # Ensure no nuclides, elements, or sab are added since these would be + # incompatible with macroscopics + if self._nuclides or self._elements or self._sab: + msg = 'Unable to add a Macroscopic data set to Material ID="{0}" ' \ + 'with a macroscopic value "{1}" as an incompatible data ' \ + 'member (i.e., nuclide, element, or S(a,b) table) ' \ + 'has already been added'.format(self._id, macroscopic) + raise ValueError(msg) + + if not isinstance(macroscopic, (openmc.Macroscopic, basestring)): + msg = 'Unable to add a Macroscopic to Material ID="{0}" with a ' \ + 'non-Macroscopic value "{1}"'.format(self._id, macroscopic) + raise ValueError(msg) + + if isinstance(macroscopic, openmc.Macroscopic): + # Copy this Macroscopic to separate it from the Macroscopic in + # other Materials + macroscopic = deepcopy(macroscopic) + else: + macroscopic = openmc.Macroscopic(macroscopic) + + if self._macroscopic is None: + self._macroscopic = macroscopic + else: + msg = 'Unable to add a Macroscopic to Material ID="{0}", ' \ + 'Only One Macroscopic allowed per ' \ + 'Material!'.format(self._id, macroscopic) + raise ValueError(msg) + + def remove_macroscopic(self, macroscopic): + """Remove a macroscopic from the material + + Parameters + ---------- + macroscopic : openmc.Macroscopic + Macroscopic to remove + + """ + + if not isinstance(macroscopic, openmc.Macroscopic): + msg = 'Unable to remove a Macroscopic "{0}" in Material ID="{1}" ' \ + 'since it is not a Macroscopic'.format(self._id, macroscopic) + raise ValueError(msg) + + # If the Material contains the Macroscopic, delete it + if macroscopic._name == self._macroscopic.name: + self._macroscopic = None + def add_element(self, element, percent, percent_type='ao'): """Add a natural element to the material Parameters ---------- - element : openmc.element.Element + element : openmc.Element Element to add percent : float Atom or weight percent @@ -325,6 +399,11 @@ class Material(object): """ + if self._macroscopic is not None: + msg = 'Unable to add an Element to Material ID="{0}" as a ' \ + 'macroscopic data-set has already been added'.format(self._id) + raise ValueError(msg) + if not isinstance(element, openmc.Element): msg = 'Unable to add an Element to Material ID="{0}" with a ' \ 'non-Element value "{1}"'.format(self._id, element) @@ -350,7 +429,7 @@ class Material(object): Parameters ---------- - element : openmc.element.Element + element : openmc.Element Element to remove """ @@ -371,6 +450,11 @@ class Material(object): """ + if self._macroscopic is not None: + msg = 'Unable to add an S(a,b) table to Material ID="{0}" as a ' \ + 'macroscopic data-set has already been added'.format(self._id) + raise ValueError(msg) + if not isinstance(name, basestring): msg = 'Unable to add an S(a,b) table to Material ID="{0}" with a ' \ 'non-string table name "{1}"'.format(self._id, name) @@ -427,6 +511,15 @@ class Material(object): return xml_element + def _get_macroscopic_xml(self, macroscopic): + xml_element = ET.Element("macroscopic") + xml_element.set("name", macroscopic._name) + + if macroscopic.xs is not None: + xml_element.set("xs", macroscopic.xs) + + return xml_element + def _get_element_xml(self, element, distrib=False): xml_element = ET.Element("element") xml_element.set("name", str(element[0]._name)) @@ -482,14 +575,19 @@ class Material(object): subelement.set("units", self._density_units) if not self._convert_to_distrib_comps: - # Create nuclide XML subelements - subelements = self._get_nuclides_xml(self._nuclides) - for subelement in subelements: - element.append(subelement) + if self._macroscopic is None: + # Create nuclide XML subelements + subelements = self._get_nuclides_xml(self._nuclides) + for subelement in subelements: + element.append(subelement) - # Create element XML subelements - subelements = self._get_elements_xml(self._elements) - for subelement in subelements: + # Create element XML subelements + subelements = self._get_elements_xml(self._elements) + for subelement in subelements: + element.append(subelement) + else: + # Create macroscopic XML subelements + subelement = self._get_macroscopic_xml(self._macroscopic) element.append(subelement) else: @@ -516,15 +614,21 @@ class Material(object): subsubelement = ET.SubElement(subelement, "otf_file_path") subsubelement.text = self._distrib_otf_file - # Create nuclide XML subelements - subelements = self.get_nuclides_xml(self._nuclides, distrib=True) - for subelement_nuc in subelements: - subelement.append(subelement_nuc) + if self._macroscopic is None: + # Create nuclide XML subelements + subelements = self.get_nuclides_xml(self._nuclides, distrib=True) + for subelement_nuc in subelements: + subelement.append(subelement_nuc) - # Create element XML subelements - subelements = self._get_elements_xml(self._elements, distrib=True) - for subelement_ele in subelements: - subelement.append(subelement_ele) + # Create element XML subelements + subelements = self._get_elements_xml(self._elements, distrib=True) + for subsubelement in subelements: + subelement.append(subsubelement) + else: + # Create macroscopic XML subelements + subsubelement = self._get_macroscopic_xml(self._macroscopic, + distrib=True) + subelement.append(subsubelement) if len(self._sab) > 0: for sab in self._sab: @@ -567,7 +671,7 @@ class MaterialsFile(object): Parameters ---------- - material : Material + material : openmc.Material Material to add """ @@ -584,7 +688,7 @@ class MaterialsFile(object): Parameters ---------- - materials : tuple or list of Material + materials : tuple or list of openmc.Material Materials to add """ @@ -602,7 +706,7 @@ class MaterialsFile(object): Parameters ---------- - material : Material + material : openmc.Material Material to remove """ @@ -619,9 +723,8 @@ class MaterialsFile(object): material.make_isotropic_in_lab() def _create_material_subelements(self): - subelement = ET.SubElement(self._materials_file, "default_xs") - if self._default_xs is not None: + subelement = ET.SubElement(self._materials_file, "default_xs") subelement.text = self._default_xs for material in self._materials: diff --git a/openmc/mgxs/groups.py b/openmc/mgxs/groups.py index 3436c0e03..068977d88 100644 --- a/openmc/mgxs/groups.py +++ b/openmc/mgxs/groups.py @@ -24,7 +24,7 @@ class EnergyGroups(object): ---------- group_edges : Iterable of Real The energy group boundaries [MeV] - num_group : Integral + num_groups : int The number of energy groups """ @@ -54,10 +54,12 @@ class EnergyGroups(object): def __eq__(self, other): if not isinstance(other, EnergyGroups): return False - elif self.group_edges != other.group_edges: + elif self.num_groups != other.num_groups: return False - else: + elif np.allclose(self.group_edges, other.group_edges): return True + else: + return False def __ne__(self, other): return not self == other @@ -84,7 +86,7 @@ class EnergyGroups(object): Parameters ---------- - energy : Real + energy : float The energy of interest in MeV Returns @@ -113,7 +115,7 @@ class EnergyGroups(object): Parameters ---------- - group : Integral + group : int The energy group index, starting at 1 for the highest energies Returns @@ -151,7 +153,7 @@ class EnergyGroups(object): Returns ------- - ndarray + numpy.ndarray The ndarray array indices for each energy group of interest Raises @@ -198,7 +200,7 @@ class EnergyGroups(object): Returns ------- - EnergyGroups + openmc.mgxs.EnergyGroups A coarsened version of this EnergyGroups object. Raises @@ -236,3 +238,64 @@ class EnergyGroups(object): condensed_groups.group_edges = group_edges return condensed_groups + + def can_merge(self, other): + """Determine if energy groups can be merged with another. + + Parameters + ---------- + other : openmc.mgxs.EnergyGroups + EnergyGroups to compare with + + Returns + ------- + bool + Whether the energy groups can be merged + + """ + + if not isinstance(other, EnergyGroups): + return False + + # If the energy group structures match then groups are mergeable + if self == other: + return True + + # This low energy edge coincides with other's high energy edge + if self.group_edges[0] == other.group_edges[-1]: + return True + # This high energy edge coincides with other's low energy edge + elif self.group_edges[-1] == other.group_edges[0]: + return True + else: + return False + + def merge(self, other): + """Merge this energy groups with another. + + Parameters + ---------- + other : openmc.mgxs.EnergyGroups + EnergyGroups to merge with + + Returns + ------- + merged_groups : openmc.mgxs.EnergyGroups + EnergyGroups resulting from the merge + + """ + + if not self.can_merge(other): + raise ValueError('Unable to merge energy groups') + + # Create deep copy to return as merged energy groups + merged_groups = copy.deepcopy(self) + + # Merge unique filter bins + merged_edges = np.concatenate((self.group_edges, other.group_edges)) + merged_edges = np.unique(merged_edges) + merged_edges = sorted(merged_edges) + + # Assign merged edges to merged groups + merged_groups.group_edges = list(merged_edges) + return merged_groups diff --git a/openmc/mgxs/library.py b/openmc/mgxs/library.py index e87b4bdae..4de4bb48a 100644 --- a/openmc/mgxs/library.py +++ b/openmc/mgxs/library.py @@ -53,22 +53,22 @@ class Library(object): The types of cross sections in the library (e.g., ['total', 'scatter']) domain_type : {'material', 'cell', 'distribcell', 'universe'} Domain type for spatial homogenization - domains : Iterable of Material, Cell or Universe + domains : Iterable of openmc.Material, openmc.Cell or openmc.Universe The spatial domain(s) for which MGXS in the Library are computed - correction : 'P0' or None + correction : {'P0', None} Apply the P0 correction to scattering matrices if set to 'P0' - energy_groups : EnergyGroups + energy_groups : openmc.mgxs.EnergyGroups Energy group structure for energy condensation - tally_trigger : Trigger + tally_trigger : openmc.Trigger An (optional) tally precision trigger given to each tally used to compute the cross section - all_mgxs : OrderedDict + all_mgxs : collections.OrderedDict MGXS objects keyed by domain ID and cross section type sp_filename : str The filename of the statepoint with tally data used to the compute cross sections keff : Real or None - The combined keff from the statepoint file with tally data used to + The combined keff from the statepoint file with tally data used to compute cross sections (for eigenvalue calculations only) name : str, optional Name of the multi-group cross section library. Used as a label to @@ -116,11 +116,11 @@ class Library(object): clone._by_nuclide = self.by_nuclide clone._mgxs_types = self.mgxs_types clone._domain_type = self.domain_type - clone._domains = self.domains + clone._domains = copy.deepcopy(self.domains) clone._correction = self.correction clone._energy_groups = copy.deepcopy(self.energy_groups, memo) clone._tally_trigger = copy.deepcopy(self.tally_trigger, memo) - clone._all_mgxs = self.all_mgxs + clone._all_mgxs = copy.deepcopy(self.all_mgxs) clone._sp_filename = self._sp_filename clone._keff = self._keff clone._sparse = self.sparse @@ -308,7 +308,7 @@ class Library(object): """ cv.check_type('sparse', sparse, bool) - + # Sparsify or densify each MGXS in the Library for domain in self.domains: for mgxs_type in self.mgxs_types: @@ -350,7 +350,7 @@ class Library(object): def add_to_tallies_file(self, tallies_file, merge=True): """Add all tallies from all MGXS objects to a tallies file. - NOTE: This assumes that build_library() has been called + NOTE: This assumes that :meth:`Library.build_library` has been called Parameters ---------- @@ -426,7 +426,7 @@ class Library(object): ---------- domain : Material or Cell or Universe or Integral The material, cell, or universe object of interest (or its ID) - mgxs_type : {'total', 'transport', 'absorption', 'capture', 'fission', 'nu-fission', 'scatter', 'nu-scatter', 'scatter matrix', 'nu-scatter matrix', 'chi'} + mgxs_type : {'total', 'transport', 'absorption', 'capture', 'fission', 'nu-fission', 'kappa-fission', 'scatter', 'nu-scatter', 'scatter matrix', 'nu-scatter matrix', 'chi'} The type of multi-group cross section object to return Returns @@ -457,7 +457,7 @@ class Library(object): break else: msg = 'Unable to find MGXS for {0} "{1}" in ' \ - 'library'.format(self.domain_type, domain) + 'library'.format(self.domain_type, domain_id) raise ValueError(msg) else: domain_id = domain.id @@ -537,7 +537,7 @@ class Library(object): Returns ------- - Library + openmc.mgxs.Library A new multi-group cross section library averaged across subdomains Raises diff --git a/openmc/mgxs/mgxs.py b/openmc/mgxs/mgxs.py index f24127458..0c3612e9f 100644 --- a/openmc/mgxs/mgxs.py +++ b/openmc/mgxs/mgxs.py @@ -25,6 +25,7 @@ MGXS_TYPES = ['total', 'capture', 'fission', 'nu-fission', + 'kappa-fission', 'scatter', 'nu-scatter', 'scatter matrix', @@ -58,11 +59,11 @@ class MGXS(object): Parameters ---------- - domain : Material or Cell or Universe + domain : openmc.Material or openmc.Cell or openmc.Universe The domain for spatial homogenization domain_type : {'material', 'cell', 'distribcell', 'universe'} The domain type for spatial homogenization - energy_groups : EnergyGroups + energy_groups : openmc.mgxs.EnergyGroups The energy group structure for energy condensation by_nuclide : bool If true, computes cross sections for each nuclide in domain @@ -82,34 +83,38 @@ class MGXS(object): Domain for spatial homogenization domain_type : {'material', 'cell', 'distribcell', 'universe'} Domain type for spatial homogenization - energy_groups : EnergyGroups + energy_groups : openmc.mgxs.EnergyGroups Energy group structure for energy condensation - tally_trigger : Trigger + tally_trigger : openmc.Trigger An (optional) tally precision trigger given to each tally used to compute the cross section - tallies : OrderedDict + tallies : collections.OrderedDict OpenMC tallies needed to compute the multi-group cross section - rxn_rate_tally : Tally + rxn_rate_tally : openmc.Tally Derived tally for the reaction rate tally used in the numerator to compute the multi-group cross section. This attribute is None unless the multi-group cross section has been computed. - xs_tally : Tally + xs_tally : openmc.Tally Derived tally for the multi-group cross section. This attribute is None unless the multi-group cross section has been computed. - num_subdomains : Integral + num_subdomains : int The number of subdomains is unity for 'material', 'cell' and 'universe' domain types. When the This is equal to the number of cell instances for 'distribcell' domain types (it is equal to unity prior to loading tally data from a statepoint file). - num_nuclides : Integral + num_nuclides : int The number of nuclides for which the multi-group cross section is being tracked. This is unity if the by_nuclide attribute is False. - nuclides : list of str or 'sum' - A list of nuclide string names (e.g., 'U-238', 'O-16') when by_nuclide - is True and 'sum' when by_nuclide is False. + nuclides : Iterable of str or 'sum' + The optional user-specified nuclides for which to compute cross + sections (e.g., 'U-238', 'O-16'). If by_nuclide is True but nuclides + are not specified by the user, all nuclides in the spatial domain + are included. This attribute is 'sum' if by_nuclide is false. sparse : bool Whether or not the MGXS' tallies use SciPy's LIL sparse matrix format for compressed data storage + derived : bool + Whether or not the MGXS is merged from one or more other MGXS """ @@ -122,6 +127,7 @@ class MGXS(object): self._name = '' self._rxn_type = None self._by_nuclide = None + self._nuclides = None self._domain = None self._domain_type = None self._energy_groups = None @@ -130,6 +136,7 @@ class MGXS(object): self._rxn_rate_tally = None self._xs_tally = None self._sparse = False + self._derived = False self.name = name self.by_nuclide = by_nuclide @@ -150,6 +157,7 @@ class MGXS(object): clone._name = self.name clone._rxn_type = self.rxn_type clone._by_nuclide = self.by_nuclide + clone._nuclides = copy.deepcopy(self._nuclides) clone._domain = self.domain clone._domain_type = self.domain_type clone._energy_groups = copy.deepcopy(self.energy_groups, memo) @@ -157,6 +165,7 @@ class MGXS(object): clone._rxn_rate_tally = copy.deepcopy(self._rxn_rate_tally, memo) clone._xs_tally = copy.deepcopy(self._xs_tally, memo) clone._sparse = self.sparse + clone._derived = self.derived clone._tallies = OrderedDict() for tally_type, tally in self.tallies.items(): @@ -231,8 +240,7 @@ class MGXS(object): @property def num_subdomains(self): - tally = list(self.tallies.values())[0] - domain_filter = tally.find_filter(self.domain_type) + domain_filter = self.xs_tally.find_filter(self.domain_type) return domain_filter.num_bins @property @@ -249,6 +257,10 @@ class MGXS(object): else: return 'sum' + @property + def derived(self): + return self._derived + @name.setter def name(self, name): cv.check_type('name', name, basestring) @@ -259,6 +271,11 @@ class MGXS(object): cv.check_type('by_nuclide', by_nuclide, bool) self._by_nuclide = by_nuclide + @nuclides.setter + def nuclides(self, nuclides): + cv.check_iterable_type('nuclides', nuclides, basestring) + self._nuclides = nuclides + @domain.setter def domain(self, domain): cv.check_type('domain', domain, tuple(_DOMAINS)) @@ -315,13 +332,13 @@ class MGXS(object): Parameters ---------- - mgxs_type : {'total', 'transport', 'absorption', 'capture', 'fission', 'nu-fission', 'scatter', 'nu-scatter', 'scatter matrix', 'nu-scatter matrix', 'chi'} + mgxs_type : {'total', 'transport', 'absorption', 'capture', 'fission', 'nu-fission', 'kappa-fission', 'scatter', 'nu-scatter', 'scatter matrix', 'nu-scatter matrix', 'chi'} The type of multi-group cross section object to return - domain : Material or Cell or Universe + domain : openmc.Material or openmc.Cell or openmc.Universe The domain for spatial homogenization domain_type : {'material', 'cell', 'distribcell', 'universe'} The domain type for spatial homogenization - energy_groups : EnergyGroups + energy_groups : openmc.mgxs.EnergyGroups The energy group structure for energy condensation by_nuclide : bool If true, computes cross sections for each nuclide in domain. @@ -332,7 +349,7 @@ class MGXS(object): Returns ------- - MGXS + openmc.mgxs.MGXS A subclass of the abstract MGXS class for the multi-group cross section type requested by the user @@ -352,6 +369,8 @@ class MGXS(object): mgxs = FissionXS(domain, domain_type, energy_groups) elif mgxs_type == 'nu-fission': mgxs = NuFissionXS(domain, domain_type, energy_groups) + elif mgxs_type == 'kappa-fission': + mgxs = KappaFissionXS(domain, domain_type, energy_groups) elif mgxs_type == 'scatter': mgxs = ScatterXS(domain, domain_type, energy_groups) elif mgxs_type == 'nu-scatter': @@ -386,8 +405,14 @@ class MGXS(object): if self.domain is None: raise ValueError('Unable to get all nuclides without a domain') - nuclides = self.domain.get_all_nuclides() - return nuclides.keys() + # If the user defined nuclides, return them + if self._nuclides: + return self._nuclides + + # Otherwise, return all nuclides in the spatial domain + else: + nuclides = self.domain.get_all_nuclides() + return nuclides.keys() def get_nuclide_density(self, nuclide): """Get the atomic number density in units of atoms/b-cm for a nuclide @@ -400,7 +425,7 @@ class MGXS(object): Returns ------- - Real + float The atomic number density (atom/b-cm) for the nuclide of interest Raises @@ -439,7 +464,7 @@ class MGXS(object): Returns ------- - ndarray of Real + numpy.ndarray of float An array of the atomic number densities (atom/b-cm) for each of the nuclides in the spatial domain @@ -487,11 +512,11 @@ class MGXS(object): ---------- scores : Iterable of str Scores for each tally - all_filters : Iterable of tuple of Filter + all_filters : Iterable of tuple of openmc.Filter Tuples of non-spatial domain filters for each tally keys : Iterable of str Key string used to store each tally in the tallies dictionary - estimator : {'analog' or 'tracklength'} + estimator : {'analog', 'tracklength'} Type of estimator to use for each tally """ @@ -510,27 +535,27 @@ class MGXS(object): # Create each Tally needed to compute the multi group cross section for score, key, filters in zip(scores, keys, all_filters): self.tallies[key] = openmc.Tally(name=self.name) - self.tallies[key].add_score(score) + self.tallies[key].scores = [score] self.tallies[key].estimator = estimator - self.tallies[key].add_filter(domain_filter) + self.tallies[key].filters = [domain_filter] # If a tally trigger was specified, add it to each tally if self.tally_trigger: trigger_clone = copy.deepcopy(self.tally_trigger) - trigger_clone.add_score(score) - self.tallies[key].add_trigger(trigger_clone) + trigger_clone.scores = [score] + self.tallies[key].triggers.append(trigger_clone) # Add all non-domain specific Filters (e.g., 'energy') to the Tally for add_filter in filters: - self.tallies[key].add_filter(add_filter) + self.tallies[key].filters.append(add_filter) # If this is a by-nuclide cross-section, add all nuclides to Tally if self.by_nuclide and score != 'flux': - all_nuclides = self.domain.get_all_nuclides() + all_nuclides = self.get_all_nuclides() for nuclide in all_nuclides: - self.tallies[key].add_nuclide(nuclide) + self.tallies[key].nuclides.append(nuclide) else: - self.tallies[key].add_nuclide('total') + self.tallies[key].nuclides.append('total') def _compute_xs(self): """Performs generic cleanup after a subclass' uses tally arithmetic to @@ -550,9 +575,9 @@ class MGXS(object): # If computing xs for each nuclide, replace CrossNuclides with originals if self.by_nuclide: self.xs_tally._nuclides = [] - nuclides = self.domain.get_all_nuclides() + nuclides = self.get_all_nuclides() for nuclide in nuclides: - self.xs_tally.add_nuclide(openmc.Nuclide(nuclide)) + self.xs_tally.nuclides.append(openmc.Nuclide(nuclide)) # Remove NaNs which may have resulted from divide-by-zero operations self.xs_tally._mean = np.nan_to_num(self.xs_tally.mean) @@ -659,7 +684,7 @@ class MGXS(object): Returns ------- - ndarray + numpy.ndarray A NumPy array of the multi-group cross section indexed in the order each group, subdomain and nuclide is listed in the parameters. @@ -679,7 +704,7 @@ class MGXS(object): # Construct a collection of the domain filter bins if not isinstance(subdomains, basestring): - cv.check_iterable_type('subdomains', subdomains, Integral) + cv.check_iterable_type('subdomains', subdomains, Integral, max_depth=2) for subdomain in subdomains: filters.append(self.domain_type) filter_bins.append((subdomain,)) @@ -734,10 +759,9 @@ class MGXS(object): # Reverse energies to align with increasing energy groups xs = xs[:, ::-1, :] - # Eliminate trivial dimensions - xs = np.squeeze(xs) - xs = np.atleast_1d(xs) - + # Eliminate trivial dimensions + xs = np.squeeze(xs) + xs = np.atleast_1d(xs) return xs def get_condensed_xs(self, coarse_groups): @@ -831,7 +855,7 @@ class MGXS(object): Returns ------- - MGXS + openmc.mgxs.MGXS A new MGXS averaged across the subdomains of interest Raises @@ -852,19 +876,181 @@ class MGXS(object): # Clone this MGXS to initialize the subdomain-averaged version avg_xs = copy.deepcopy(self) - avg_xs._rxn_rate_tally = None - avg_xs._xs_tally = None - # Average each of the tallies across subdomains - for tally_type, tally in avg_xs.tallies.items(): - tally_avg = tally.summation(filter_type=self.domain_type, - filter_bins=subdomains) - avg_xs.tallies[tally_type] = tally_avg + if self.derived: + avg_xs._rxn_rate_tally = avg_xs.rxn_rate_tally.average( + filter_type=self.domain_type, filter_bins=subdomains) + else: + avg_xs._rxn_rate_tally = None + avg_xs._xs_tally = None - avg_xs._domain_type = 'sum({0})'.format(self.domain_type) + # Average each of the tallies across subdomains + for tally_type, tally in avg_xs.tallies.items(): + tally_avg = tally.average(filter_type=self.domain_type, + filter_bins=subdomains) + avg_xs.tallies[tally_type] = tally_avg + + avg_xs._domain_type = 'avg({0})'.format(self.domain_type) avg_xs.sparse = self.sparse return avg_xs + def get_slice(self, nuclides=[], groups=[]): + """Build a sliced MGXS for the specified nuclides and energy groups. + + This method constructs a new MGXS to encapsulate a subset of the data + represented by this MGXS. The subset of data to include in the tally + slice is determined by the nuclides and energy groups specified in + the input parameters. + + Parameters + ---------- + nuclides : list of str + A list of nuclide name strings + (e.g., ['U-235', 'U-238']; default is []) + groups : list of int + A list of energy group indices starting at 1 for the high energies + (e.g., [1, 2, 3]; default is []) + + Returns + ------- + openmc.mgxs.MGXS + A new tally which encapsulates the subset of data requested for the + nuclide(s) and/or energy group(s) requested in the parameters. + + """ + + cv.check_iterable_type('nuclides', nuclides, basestring) + cv.check_iterable_type('energy_groups', groups, Integral) + + # Build lists of filters and filter bins to slice + if len(groups) == 0: + filters = [] + filter_bins = [] + else: + filter_bins = [] + for group in groups: + group_bounds = self.energy_groups.get_group_bounds(group) + filter_bins.append(group_bounds) + filter_bins = [tuple(filter_bins)] + filters = ['energy'] + + # Clone this MGXS to initialize the sliced version + slice_xs = copy.deepcopy(self) + slice_xs._rxn_rate_tally = None + slice_xs._xs_tally = None + + # Slice each of the tallies across nuclides and energy groups + for tally_type, tally in slice_xs.tallies.items(): + slice_nuclides = [nuc for nuc in nuclides if nuc in tally.nuclides] + if len(groups) != 0 and tally.contains_filter('energy'): + tally_slice = tally.get_slice(filters=filters, + filter_bins=filter_bins, nuclides=slice_nuclides) + else: + tally_slice = tally.get_slice(nuclides=slice_nuclides) + slice_xs.tallies[tally_type] = tally_slice + + # Assign sliced energy group structure to sliced MGXS + if groups: + new_group_edges = [] + for group in groups: + group_edges = self.energy_groups.get_group_bounds(group) + new_group_edges.extend(group_edges) + new_group_edges = np.unique(new_group_edges) + slice_xs.energy_groups.group_edges = sorted(new_group_edges) + + # Assign sliced nuclides to sliced MGXS + if nuclides: + slice_xs.nuclides = nuclides + + slice_xs.sparse = self.sparse + return slice_xs + + def can_merge(self, other): + """Determine if another MGXS can be merged with this one + + If results have been loaded from a statepoint, then MGXS are only + mergeable along one and only one of enegy groups or nuclides. + + Parameters + ---------- + other : openmc.mgxs.MGXS + MGXS to check for merging + + """ + + if not isinstance(other, type(self)): + return False + + # Compare reaction type, energy groups, nuclides, domain type + if self.rxn_type != other.rxn_type: + return False + elif not self.energy_groups.can_merge(other.energy_groups): + return False + elif self.by_nuclide != other.by_nuclide: + return False + elif self.domain_type != other.domain_type: + return False + elif 'distribcell' not in self.domain_type and self.domain != other.domain: + return False + elif not self.xs_tally.can_merge(other.xs_tally): + return False + elif not self.rxn_rate_tally.can_merge(other.rxn_rate_tally): + return False + + # If all conditionals pass then MGXS are mergeable + return True + + def merge(self, other): + """Merge another MGXS with this one + + MGXS are only mergeable if their energy groups and nuclides are either + identical or mutually exclusive. If results have been loaded from a + statepoint, then MGXS are only mergeable along one and only one of + energy groups or nuclides. + + Parameters + ---------- + other : openmc.mgxs.MGXS + MGXS to merge with this one + + Returns + ------- + merged_mgxs : openmc.mgxs.MGXS + Merged MGXS + + """ + + if not self.can_merge(other): + raise ValueError('Unable to merge MGXS') + + # Create deep copy of tally to return as merged tally + merged_mgxs = copy.deepcopy(self) + merged_mgxs._derived = True + + # Merge energy groups + if self.energy_groups != other.energy_groups: + merged_groups = self.energy_groups.merge(other.energy_groups) + merged_mgxs.energy_groups = merged_groups + + # Merge nuclides + if self.nuclides != other.nuclides: + + # The nuclides must be mutually exclusive + for nuclide in self.nuclides: + if nuclide in other.nuclides: + msg = 'Unable to merge MGXS with shared nuclides' + raise ValueError(msg) + + # Concatenate lists of nuclides for the merged MGXS + merged_mgxs.nuclides = self.nuclides + other.nuclides + + # Null base tallies but merge reaction rate and cross section tallies + merged_mgxs._tallies = OrderedDict() + merged_mgxs._rxn_rate_tally = self.rxn_rate_tally.merge(other.rxn_rate_tally) + merged_mgxs._xs_tally = self.xs_tally.merge(other.xs_tally) + + return merged_mgxs + def print_xs(self, subdomains='all', nuclides='all', xs_type='macro'): """Print a string representation for the multi-group cross section. @@ -1019,6 +1205,9 @@ class MGXS(object): cv.check_iterable_type('subdomains', subdomains, Integral) elif self.domain_type == 'distribcell': subdomains = np.arange(self.num_subdomains, dtype=np.int) + elif self.domain_type == 'avg(distribcell)': + domain_filter = self.xs_tally.find_filter('avg(distribcell)') + subdomains = domain_filter.bins else: subdomains = [self.domain.id] @@ -1160,7 +1349,7 @@ class MGXS(object): xs_type='macro', summary=None): """Build a Pandas DataFrame for the MGXS data. - This method leverages the Tally.get_pandas_dataframe(...) method, but + This method leverages :meth:`openmc.Tally.get_pandas_dataframe`, but renames the columns with terminology appropriate for cross section data. Parameters @@ -1177,7 +1366,7 @@ class MGXS(object): xs_type: {'macro', 'micro'} Return macro or micro cross section in units of cm^-1 or barns. Defaults to 'macro'. - summary : None or Summary + summary : None or openmc.Summary An optional Summary object to be used to construct columns for distribcell tally filters (default is None). The geometric information in the Summary object is embedded into a multi-index @@ -1232,28 +1421,34 @@ class MGXS(object): # Override energy groups bounds with indices all_groups = np.arange(self.num_groups, 0, -1, dtype=np.int) all_groups = np.repeat(all_groups, self.num_nuclides) - if 'energy [MeV]' in df and 'energyout [MeV]' in df: - df.rename(columns={'energy [MeV]': 'group in'}, inplace=True) + if 'energy low [MeV]' in df and 'energyout low [MeV]' in df: + df.rename(columns={'energy low [MeV]': 'group in'}, + inplace=True) in_groups = np.tile(all_groups, self.num_subdomains) - in_groups = np.repeat(in_groups, self.num_groups) + in_groups = np.repeat(in_groups, df.shape[0] / in_groups.size) df['group in'] = in_groups + del df['energy high [MeV]'] - df.rename(columns={'energyout [MeV]': 'group out'}, inplace=True) - out_groups = \ - np.tile(all_groups, self.num_subdomains * self.num_groups) + df.rename(columns={'energyout low [MeV]': 'group out'}, + inplace=True) + out_groups = np.tile(all_groups, df.shape[0] / all_groups.size) df['group out'] = out_groups + del df['energyout high [MeV]'] columns = ['group in', 'group out'] - elif 'energyout [MeV]' in df: - df.rename(columns={'energyout [MeV]': 'group out'}, inplace=True) + elif 'energyout low [MeV]' in df: + df.rename(columns={'energyout low [MeV]': 'group out'}, + inplace=True) in_groups = np.tile(all_groups, self.num_subdomains) df['group out'] = in_groups + del df['energyout high [MeV]'] columns = ['group out'] - elif 'energy [MeV]' in df: - df.rename(columns={'energy [MeV]': 'group in'}, inplace=True) + elif 'energy low [MeV]' in df: + df.rename(columns={'energy low [MeV]': 'group in'}, inplace=True) in_groups = np.tile(all_groups, self.num_subdomains) df['group in'] = in_groups + del df['energy high [MeV]'] columns = ['group in'] # Select out those groups the user requested @@ -1275,8 +1470,7 @@ class MGXS(object): # Sort the dataframe by domain type id (e.g., distribcell id) and # energy groups such that data is from fast to thermal - df.sort([self.domain_type] + columns, inplace=True) - + df.sort_values(by=[self.domain_type] + columns, inplace=True) return df @@ -1319,7 +1513,7 @@ class TotalXS(MGXS): @property def rxn_rate_tally(self): - if self._rxn_rate_tally is None: + if self._rxn_rate_tally is None : self._rxn_rate_tally = self.tallies['total'] self._rxn_rate_tally.sparse = self.sparse return self._rxn_rate_tally @@ -1477,96 +1671,80 @@ class CaptureXS(MGXS): self._rxn_rate_tally.sparse = self.sparse return self._rxn_rate_tally +class FissionXSBase(MGXS): + """A fission production multi-group cross section base class + for NuFission and KappaFission + """ -class FissionXS(MGXS): + # This is an abstract class which cannot be instantiated + __metaclass__ = abc.ABCMeta + + def __init__(self, rxn_type, domain=None, domain_type=None, + groups=None, by_nuclide=False, name=''): + super(FissionXSBase, self).__init__(domain, domain_type, + groups, by_nuclide, name) + self._rxn_type = rxn_type + + @property + def tallies(self): + """Construct the OpenMC tallies needed to compute this cross section. + + This method constructs two tracklength tallies to compute the 'flux' + and 'rxn_type' reaction rates in the spatial domain and energy + groups of interest. + + """ + + # Instantiate tallies if they do not exist + if self._tallies is None: + + # Create a list of scores for each Tally to be created + scores = ['flux', self._rxn_type] + estimator = 'tracklength' + keys = scores + + # Create the non-domain specific Filters for the Tallies + group_edges = self.energy_groups.group_edges + energy_filter = openmc.Filter('energy', group_edges) + filters = [[energy_filter], [energy_filter]] + + # Initialize the Tallies + self._create_tallies(scores, filters, keys, estimator) + + return self._tallies + + @property + def rxn_rate_tally(self): + if self._rxn_rate_tally is None: + self._rxn_rate_tally = self.tallies[self._rxn_type] + self._rxn_rate_tally.sparse = self.sparse + return self._rxn_rate_tally + + +class FissionXS(FissionXSBase): """A fission multi-group cross section.""" def __init__(self, domain=None, domain_type=None, groups=None, by_nuclide=False, name=''): - super(FissionXS, self).__init__(domain, domain_type, + super(FissionXS, self).__init__('fission', domain, domain_type, groups, by_nuclide, name) - self._rxn_type = 'fission' - - @property - def tallies(self): - """Construct the OpenMC tallies needed to compute this cross section. - - This method constructs two tracklength tallies to compute the 'flux' - and 'fission' reaction rates in the spatial domain and energy - groups of interest. - - """ - - # Instantiate tallies if they do not exist - if self._tallies is None: - - # Create a list of scores for each Tally to be created - scores = ['flux', 'fission'] - estimator = 'tracklength' - keys = scores - - # Create the non-domain specific Filters for the Tallies - group_edges = self.energy_groups.group_edges - energy_filter = openmc.Filter('energy', group_edges) - filters = [[energy_filter], [energy_filter]] - - # Initialize the Tallies - self._create_tallies(scores, filters, keys, estimator) - - return self._tallies - - @property - def rxn_rate_tally(self): - if self._rxn_rate_tally is None: - self._rxn_rate_tally = self.tallies['fission'] - self._rxn_rate_tally.sparse = self.sparse - return self._rxn_rate_tally -class NuFissionXS(MGXS): +class NuFissionXS(FissionXSBase): """A fission production multi-group cross section.""" def __init__(self, domain=None, domain_type=None, groups=None, by_nuclide=False, name=''): - super(NuFissionXS, self).__init__(domain, domain_type, + super(NuFissionXS, self).__init__('nu-fission', domain, domain_type, groups, by_nuclide, name) - self._rxn_type = 'nu-fission' - @property - def tallies(self): - """Construct the OpenMC tallies needed to compute this cross section. - - This method constructs two tracklength tallies to compute the 'flux' - and 'nu-fission' reaction rates in the spatial domain and energy - groups of interest. - - """ - - # Instantiate tallies if they do not exist - if self._tallies is None: - - # Create a list of scores for each Tally to be created - scores = ['flux', 'nu-fission'] - estimator = 'tracklength' - keys = scores - - # Create the non-domain specific Filters for the Tallies - group_edges = self.energy_groups.group_edges - energy_filter = openmc.Filter('energy', group_edges) - filters = [[energy_filter], [energy_filter]] - - # Initialize the Tallies - self._create_tallies(scores, filters, keys, estimator) - - return self._tallies - - @property - def rxn_rate_tally(self): - if self._rxn_rate_tally is None: - self._rxn_rate_tally = self.tallies['nu-fission'] - self._rxn_rate_tally.sparse = self.sparse - return self._rxn_rate_tally +class KappaFissionXS(FissionXSBase): + """A recoverable fission energy production rate multi-group cross section.""" + def __init__(self, domain=None, domain_type=None, + groups=None, by_nuclide=False, name=''): + super(KappaFissionXS, self).__init__('kappa-fission', domain, domain_type, + groups, by_nuclide, name) class ScatterXS(MGXS): """A scatter multi-group cross section.""" @@ -1741,6 +1919,58 @@ class ScatterMatrixXS(MGXS): cv.check_value('correction', correction, ('P0', None)) self._correction = correction + def get_slice(self, nuclides=[], in_groups=[], out_groups=[]): + """Build a sliced ScatterMatrix for the specified nuclides and + energy groups. + + This method constructs a new MGXS to encapsulate a subset of the data + represented by this MGXS. The subset of data to include in the tally + slice is determined by the nuclides and energy groups specified in + the input parameters. + + Parameters + ---------- + nuclides : list of str + A list of nuclide name strings + (e.g., ['U-235', 'U-238']; default is []) + in_groups : list of int + A list of incoming energy group indices starting at 1 for the high + energies (e.g., [1, 2, 3]; default is []) + out_groups : list of int + A list of outgoing energy group indices starting at 1 for the high + energies (e.g., [1, 2, 3]; default is []) + + Returns + ------- + openmc.mgxs.MGXS + A new tally which encapsulates the subset of data requested for the + nuclide(s) and/or energy group(s) requested in the parameters. + + """ + + # Call super class method and null out derived tallies + slice_xs = super(ScatterMatrixXS, self).get_slice(nuclides, in_groups) + slice_xs._rxn_rate_tally = None + slice_xs._xs_tally = None + + # Slice outgoing energy groups if needed + if len(out_groups) != 0: + filter_bins = [] + for group in out_groups: + group_bounds = self.energy_groups.get_group_bounds(group) + filter_bins.append(group_bounds) + filter_bins = [tuple(filter_bins)] + + # Slice each of the tallies across energyout groups + for tally_type, tally in slice_xs.tallies.items(): + if tally.contains_filter('energyout'): + tally_slice = tally.get_slice(filters=['energyout'], + filter_bins=filter_bins) + slice_xs.tallies[tally_type] = tally_slice + + slice_xs.sparse = self.sparse + return slice_xs + def get_xs(self, in_groups='all', out_groups='all', subdomains='all', nuclides='all', xs_type='macro', order_groups='increasing', value='mean'): @@ -1795,7 +2025,7 @@ class ScatterMatrixXS(MGXS): # Construct a collection of the domain filter bins if not isinstance(subdomains, basestring): - cv.check_iterable_type('subdomains', subdomains, Integral) + cv.check_iterable_type('subdomains', subdomains, Integral, max_depth=2) for subdomain in subdomains: filters.append(self.domain_type) filter_bins.append((subdomain,)) @@ -2080,10 +2310,117 @@ class Chi(MGXS): super(Chi, self)._compute_xs() # Add the coarse energy filter back to the nu-fission tally - nu_fission_in.add_filter(energy_filter) + nu_fission_in.filters.append(energy_filter) return self._xs_tally + def get_slice(self, nuclides=[], groups=[]): + """Build a sliced Chi for the specified nuclides and energy groups. + + This method constructs a new MGXS to encapsulate a subset of the data + represented by this MGXS. The subset of data to include in the tally + slice is determined by the nuclides and energy groups specified in + the input parameters. + + Parameters + ---------- + nuclides : list of str + A list of nuclide name strings + (e.g., ['U-235', 'U-238']; default is []) + groups : list of Integral + A list of energy group indices starting at 1 for the high energies + (e.g., [1, 2, 3]; default is []) + + Returns + ------- + MGXS + A new tally which encapsulates the subset of data requested for the + nuclide(s) and/or energy group(s) requested in the parameters. + + """ + + # Temporarily remove energy filter from nu-fission-in since its + # group structure will work in super MGXS.get_slice(...) method + nu_fission_in = self.tallies['nu-fission-in'] + energy_filter = nu_fission_in.find_filter('energy') + nu_fission_in.remove_filter(energy_filter) + + # Call super class method and null out derived tallies + slice_xs = super(Chi, self).get_slice(nuclides, groups) + slice_xs._rxn_rate_tally = None + slice_xs._xs_tally = None + + # Slice energy groups if needed + if len(groups) != 0: + filter_bins = [] + for group in groups: + group_bounds = self.energy_groups.get_group_bounds(group) + filter_bins.append(group_bounds) + filter_bins = [tuple(filter_bins)] + + # Slice nu-fission-out tally along energyout filter + nu_fission_out = slice_xs.tallies['nu-fission-out'] + tally_slice = nu_fission_out.get_slice(filters=['energyout'], + filter_bins=filter_bins) + slice_xs._tallies['nu-fission-out'] = tally_slice + + # Add energy filter back to nu-fission-in tallies + self.tallies['nu-fission-in'].add_filter(energy_filter) + slice_xs._tallies['nu-fission-in'].add_filter(energy_filter) + + slice_xs.sparse = self.sparse + return slice_xs + + def merge(self, other): + """Merge another Chi with this one + + If results have been loaded from a statepoint, then Chi are only + mergeable along one and only one of energy groups or nuclides. + + Parameters + ---------- + other : openmc.mgxs.MGXS + MGXS to merge with this one + + Returns + ------- + merged_mgxs : openmc.mgxs.MGXS + Merged MGXS + """ + + if not self.can_merge(other): + raise ValueError('Unable to merge Chi') + + # Create deep copy of tally to return as merged tally + merged_mgxs = copy.deepcopy(self) + merged_mgxs._derived = True + merged_mgxs._rxn_rate_tally = None + merged_mgxs._xs_tally = None + + # Merge energy groups + if self.energy_groups != other.energy_groups: + merged_groups = self.energy_groups.merge(other.energy_groups) + merged_mgxs.energy_groups = merged_groups + + # Merge nuclides + if self.nuclides != other.nuclides: + + # The nuclides must be mutually exclusive + for nuclide in self.nuclides: + if nuclide in other.nuclides: + msg = 'Unable to merge Chi with shared nuclides' + raise ValueError(msg) + + # Concatenate lists of nuclides for the merged MGXS + merged_mgxs.nuclides = self.nuclides + other.nuclides + + # Merge tallies + for tally_key in self.tallies: + merged_tally = self.tallies[tally_key].merge(other.tallies[tally_key]) + merged_mgxs.tallies[tally_key] = merged_tally + + return merged_mgxs + def get_xs(self, groups='all', subdomains='all', nuclides='all', xs_type='macro', order_groups='increasing', value='mean'): """Returns an array of the fission spectrum. @@ -2115,7 +2452,7 @@ class Chi(MGXS): Returns ------- - ndarray + numpy.ndarray A NumPy array of the multi-group cross section indexed in the order each group, subdomain and nuclide is listed in the parameters. @@ -2135,7 +2472,7 @@ class Chi(MGXS): # Construct a collection of the domain filter bins if not isinstance(subdomains, basestring): - cv.check_iterable_type('subdomains', subdomains, Integral) + cv.check_iterable_type('subdomains', subdomains, Integral, max_depth=2) for subdomain in subdomains: filters.append(self.domain_type) filter_bins.append((subdomain,)) @@ -2172,7 +2509,7 @@ class Chi(MGXS): xs_tally = nu_fission_out / nu_fission_in # Add the coarse energy filter back to the nu-fission tally - nu_fission_in.add_filter(energy_filter) + nu_fission_in.filters.append(energy_filter) xs = xs_tally.get_values(filters=filters, filter_bins=filter_bins, value=value) @@ -2223,7 +2560,7 @@ class Chi(MGXS): xs_type='macro', summary=None): """Build a Pandas DataFrame for the MGXS data. - This method leverages the Tally.get_pandas_dataframe(...) method, but + This method leverages :meth:`openmc.Tally.get_pandas_dataframe`, but renames the columns with terminology appropriate for cross section data. Parameters @@ -2240,7 +2577,7 @@ class Chi(MGXS): xs_type: {'macro', 'micro'} Return macro or micro cross section in units of cm^-1 or barns. Defaults to 'macro'. - summary : None or Summary + summary : None or openmc.Summary An optional Summary object to be used to construct columns for distribcell tally filters (default is None). The geometric information in the Summary object is embedded into a multi-index diff --git a/openmc/mgxs_library.py b/openmc/mgxs_library.py new file mode 100644 index 000000000..c0b04fed1 --- /dev/null +++ b/openmc/mgxs_library.py @@ -0,0 +1,797 @@ +from collections import Iterable +from numbers import Real, Integral +from xml.etree import ElementTree as ET +import warnings +import sys +if sys.version_info[0] >= 3: + basestring = str + +import numpy as np + +import openmc +from openmc.mgxs import EnergyGroups +from openmc.checkvalue import check_type, check_value, check_greater_than, \ + check_iterable_type +from openmc.clean_xml import * + +# Supported incoming particle MGXS angular treatment representations +_REPRESENTATIONS = ['isotropic', 'angle'] + + +def ndarray_to_string(arr): + """Converts a numpy ndarray in to a join with spaces between entries + similar to ' '.join(map(str,arr)) but applied to all sub-dimensions. + + Parameters + ---------- + arr : numpy.ndarray + Array to combine in to a string + + Returns + ------- + text : str + String representation of array in arr + + """ + + shape = arr.shape + ndim = arr.ndim + tab = ' ' + indent = '\n' + tab + tab + text = indent + + if ndim == 1: + text += tab + for i in range(shape[0]): + text += '{:.7E} '.format(arr[i]) + text += indent + elif ndim == 2: + for i in range(shape[0]): + text += tab + for j in range(shape[1]): + text += '{:.7E} '.format(arr[i, j]) + text += indent + elif ndim == 3: + for i in range(shape[0]): + for j in range(shape[1]): + text += tab + for k in range(shape[2]): + text += '{:.7E} '.format(arr[i, j, k]) + text += indent + elif ndim == 4: + for i in range(shape[0]): + for j in range(shape[1]): + for k in range(shape[2]): + text += tab + for l in range(shape[3]): + text += '{:.7E} '.format(arr[i, j, k, l]) + text += indent + elif ndim == 5: + for i in range(shape[0]): + for j in range(shape[1]): + for k in range(shape[2]): + for l in range(shape[3]): + text += tab + for m in range(shape[4]): + text += '{:.7E} '.format(arr[i, j, k, l, m]) + text += indent + + return text + + +class XSdata(object): + """A multi-group cross section data set providing all the + multi-group data necessary for a multi-group OpenMC calculation. + + Parameters + ---------- + name : str, optional + Name of the mgxs data set. + energy_groups : openmc.mgxs.EnergyGroups + Energygroup structure + representation : {'isotropic', 'angle'}, optional + Method used in generating the MGXS (isotropic or angle-dependent flux + weighting). Defaults to 'isotropic' + + Attributes + ---------- + name : str + Unique identifier for the xsdata object + alias : str + Separate unique identifier for the xsdata object + kT : float + Temperature (in units of MeV). + energy_groups : openmc.mgxs.EnergyGroups + Energy group structure + fissionable : bool + Whether or not this is a fissionable data set. + scatt_type : {'legendre', 'histogram', or 'tabular'} + Angular distribution representation (legendre, histogram, or tabular) + order : int + Either the Legendre order, number of bins, or number of points used to + describe the angular distribution associated with each group-to-group + transfer probability. + tabular_legendre : dict + Set how to treat the Legendre scattering kernel (tabular or leave in + Legendre polynomial form). Dict contains two keys: 'enable' and + 'num_points'. 'enable' is a boolean and 'num_points' is the + number of points to use, if 'enable' is True. + num_azimuthal : int + Number of equal width angular bins that the azimuthal angular domain is + subdivided into. This only applies when ``representation`` is "angle". + num_polar : int + Number of equal width angular bins that the polar angular domain is + subdivided into. This only applies when ``representation`` is "angle". + total : numpy.ndarray + Group-wise total cross section ordered by increasing group index (i.e., + fast to thermal). If ``representation`` is "isotropic", then the length + of this list should equal the number of groups described in the + ``groups`` element. If ``representation`` is "angle", then the length + of this list should equal the number of groups times the number of + azimuthal angles times the number of polar angles, with the + inner-dimension being groups, intermediate-dimension being azimuthal + angles and outer-dimension being the polar angles. + absorption : numpy.ndarray + Group-wise absorption cross section ordered by increasing group index + (i.e., fast to thermal). If ``representation`` is "isotropic", then the + length of this list should equal the number of groups described in the + ``groups`` attribute. If ``representation`` is "angle", then the length + of this list should equal the number of groups times the number of + azimuthal angles times the number of polar angles, with the + inner-dimension being groups, intermediate-dimension being azimuthal + angles and outer-dimension being the polar angles. + scatter : numpy.ndarray + Scattering moment matrices presented with the columns representing + incoming group and rows representing the outgoing group. That is, + down-scatter will be above the diagonal of the resultant matrix. This + matrix is repeated for every Legendre order (in order of increasing + orders) if ``scatt_type`` is "legendre"; otherwise, this matrix is + repeated for every bin of the histogram or tabular representation. + Finally, if ``representation`` is "angle", the above is repeated for + every azimuthal angle and every polar angle, in that order. + multiplicity : numpy.ndarray + Ratio of neutrons produced in scattering collisions to the neutrons + which undergo scattering collisions; that is, the multiplicity provides + the code with a scaling factor to account for neutrons being produced in + (n,xn) reactions. This information is assumed isotropic and therefore + does not need to be repeated for every Legendre moment or + histogram/tabular bin. This matrix follows the same arrangement as + described for the ``scatter`` attribute, with the exception of the data + needed to provide the scattering type information. + fission : numpy.ndarray + Group-wise fission cross section ordered by increasing group index + (i.e., fast to thermal). If ``representation`` is "isotropic", then the + length of this list should equal the number of groups described in the + ``groups`` attribute. If ``representation`` is "angle", then the length + of this list should equal the number of groups times the number of + azimuthal angles times the number of polar angles, with the + inner-dimension being groups, intermediate-dimension being azimuthal + angles and outer-dimension being the polar angles. + k_fission : numpy.ndarray + Group-wise kappa-fission cross section ordered by increasing group index + (i.e., fast to thermal). If ``representation`` is "isotropic", then the + length of this list should equal the number of groups described in the + ``groups`` attribute. If ``representation`` is "angle", then the length + of this list should equal the number of groups times the number of + azimuthal angles times the number of polar angles, with the + inner-dimension being groups, intermediate-dimension being azimuthal + angles and outer-dimension being the polar angles. + chi : numpy.ndarray + Group-wise fission spectra ordered by increasing group index (i.e., fast + to thermal). This attribute should be used if making the common + approximation that the fission spectra does not depend on incoming + energy. If the user does not wish to make this approximation, then this + should not be provided and this information included in the + ``nu_fission`` element instead. If ``representation`` is "isotropic", + then the length of this list should equal the number of groups described + in the ``groups`` element. If ``representation`` is "angle", then the + length of this list should equal the number of groups times the number + of azimuthal angles times the number of polar angles, with the + inner-dimension being groups, intermediate-dimension being azimuthal + angles and outer-dimension being the polar angles. + nu_fission : numpy.ndarray + Group-wise fission production cross section vector (i.e., if ``chi`` is + provided), or is the group-wise fission production matrix. If providing + the vector, it should be ordered the same as the ``fission`` data. If + providing the matrix, it should be ordered the same as the + ``multiplicity`` matrix. + + """ + def __init__(self, name, energy_groups, representation="isotropic"): + # Initialize class attributes + self._name = name + self._energy_groups = energy_groups + self._representation = representation + self._alias = None + self._kT = None + self._fissionable = False + self._scatt_type = 'legendre' + self._order = None + self._tabular_legendre = None + self._num_polar = None + self._num_azimuthal = None + self._total = None + self._absorption = None + self._scatter = None + self._multiplicity = None + self._fission = None + self._nu_fission = None + self._k_fission = None + self._chi = None + self._use_chi = None + + @property + def name(self): + return self._name + + @property + def energy_groups(self): + return self._energy_groups + + @property + def representation(self): + return self._representation + + @property + def alias(self): + return self._alias + + @property + def kT(self): + return self._kT + + @property + def scatt_type(self): + return self._scatt_type + + @property + def order(self): + return self._order + + @property + def tabular_legendre(self): + return self._tabular_legendre + + @property + def num_polar(self): + return self._num_polar + + @property + def num_azimuthal(self): + return self._num_azimuthal + + @property + def total(self): + return self._total + + @property + def absorption(self): + return self._absorption + + @property + def scatter(self): + return self._scatter + + @property + def multiplicity(self): + return self._multiplicity + + @property + def fission(self): + return self._fission + + @property + def nu_fission(self): + return self._nu_fission + + @property + def k_fission(self): + return self._k_fission + + @property + def chi(self): + return self._chi + + @property + def num_orders(self): + if (self._order is not None) and (self._scatt_type is not None): + if self._scatt_type is 'legendre': + return self._order + 1 + else: + return self._order + + @name.setter + def name(self, name): + check_type('name for XSdata', name, basestring) + self._name = name + + @energy_groups.setter + def energy_groups(self, energy_groups): + # Check validity of energy_groups + check_type("energy_groups", energy_groups, EnergyGroups) + + # Check that there is one or more groups + if ((energy_groups.num_groups is None) or + (energy_groups.num_groups < 1)): + + msg = 'energy_groups object incorrectly initialized.' + raise ValueError(msg) + + self._energy_groups = energy_groups + + @representation.setter + def representation(self, representation): + # Check it is of valid type. + check_value('representation', representation, _REPRESENTATIONS) + self._representation = representation + + @alias.setter + def alias(self, alias): + if alias is not None: + check_type('alias', alias, basestring) + self._alias = alias + else: + self._alias = self._name + + @kT.setter + def kT(self, kT): + # Check validity of type and that the kT value is >= 0 + check_type("kT", kT, Real) + check_greater_than("kT", kT, 0.0, equality=True) + self._kT = kT + + @scatt_type.setter + def scatt_type(self, scatt_type): + # check to see it is of a valid type and value + check_value("scatt_type", scatt_type, ['legendre', 'histogram', + 'tabular']) + self._scatt_type = scatt_type + + @order.setter + def order(self, order): + # Check type and value + check_type("order", order, Integral) + check_greater_than("order", order, 0, equality=True) + self._order = order + + @tabular_legendre.setter + def tabular_legendre(self, tabular_legendre): + # Check to make sure this is a dict and it has our keys with the + # right values. + check_type("tabular_legendre", tabular_legendre, dict) + if 'enable' in tabular_legendre: + enable = tabular_legendre['enable'] + check_type('enable', enable, bool) + else: + msg = "enable must be provided in tabular_legendre" + raise ValueError(msg) + if 'num_points' in tabular_legendre: + num_points = tabular_legendre['num_points'] + check_value('num_points', num_points, Integral) + check_greater_than('num_points', num_points, 0) + else: + if not enable: + num_points = 1 + else: + num_points = 33 + self._tabular_legendre = {'enable': enable, 'num_points': num_points} + + @num_polar.setter + def num_polar(self, num_polar): + # Make sure we have positive ints + check_value("num_polar", num_polar, Integral) + check_greater_than("num_polar", num_polar, 0) + self._num_polar = num_polar + + @num_azimuthal.setter + def num_azimuthal(self, num_azimuthal): + check_value("num_azimuthal", num_azimuthal, Integral) + check_greater_than("num_azimuthal", num_azimuthal, 0) + self._num_azimuthal = num_azimuthal + + @total.setter + def total(self, total): + if self._representation is 'isotropic': + shape = (self._energy_groups.num_groups,) + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups) + # check we have a numpy list + check_type("total", total, np.ndarray, expected_iter_type=Real) + if total.shape == shape: + self._total = np.copy(total) + else: + msg = 'Shape of provided total "{0}" does not match shape ' \ + 'required, "{1}"'.format(total.shape, shape) + raise ValueError(msg) + + @absorption.setter + def absorption(self, absorption): + if self._representation is 'isotropic': + shape = (self._energy_groups.num_groups,) + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups) + # check we have a numpy list + check_type("absorption", absorption, np.ndarray, expected_iter_type=Real) + if absorption.shape == shape: + self._absorption = np.copy(absorption) + else: + msg = 'Shape of provided absorption "{0}" does not match shape ' \ + 'required, "{1}"'.format(absorption.shape, shape) + raise ValueError(msg) + + @fission.setter + def fission(self, fission): + if self._representation is 'isotropic': + shape = (self._energy_groups.num_groups,) + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups) + # check we have a numpy list + check_type("fission", fission, np.ndarray, expected_iter_type=Real) + if fission.shape == shape: + self._fission = np.copy(fission) + if np.sum(self._fission) > 0.0: + self._fissionable = True + else: + msg = 'Shape of provided fission "{0}" does not match shape ' \ + 'required, "{1}"'.format(fission.shape, shape) + raise ValueError(msg) + + @k_fission.setter + def k_fission(self, k_fission): + if self._representation is 'isotropic': + shape = (self._energy_groups.num_groups,) + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups) + # check we have a numpy list + check_type("k_fission", k_fission, np.ndarray, expected_iter_type=Real) + if k_fission.shape == shape: + self._k_fission = np.copy(k_fission) + if np.sum(self._k_fission) > 0.0: + self._fissionable = True + else: + msg = 'Shape of provided k_fission "{0}" does not match shape ' \ + 'required, "{1}"'.format(k_fission.shape, shape) + raise ValueError(msg) + + @chi.setter + def chi(self, chi): + if not self._use_chi: + msg = 'Providing chi when nu_fission already provided as matrix!' + raise ValueError(msg) + if self._representation is 'isotropic': + shape = (self._energy_groups.num_groups,) + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups) + # check we have a numpy list + check_type("chi", chi, np.ndarray, expected_iter_type=Real) + if chi.shape == shape: + self._chi = np.copy(chi) + else: + msg = 'Shape of provided chi "{0}" does not match shape ' \ + 'required, "{1}"'.format(chi.shape, shape) + raise ValueError(msg) + if self._use_chi is not None: + self._use_chi = True + + @scatter.setter + def scatter(self, scatter): + if self._representation is 'isotropic': + shape = (self.num_orders, self._energy_groups.num_groups, + self._energy_groups.num_groups) + max_depth = 3 + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, self.num_orders, + self._energy_groups.num_groups, + self._energy_groups.num_groups) + max_depth = 5 + # check we have a numpy list + check_iterable_type("scatter", scatter, expected_type=Real, + max_depth=max_depth) + if scatter.shape == shape: + self._scatter = np.copy(scatter) + else: + msg = 'Shape of provided scatter "{0}" does not match shape ' \ + 'required, "{1}"'.format(scatter.shape, shape) + raise ValueError(msg) + + @multiplicity.setter + def multiplicity(self, multiplicity): + if self._representation is 'isotropic': + shape = (self._energy_groups.num_groups, + self._energy_groups.num_groups) + max_depth = 2 + elif self._representation is 'angle': + shape = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups, + self._energy_groups.num_groups) + max_depth = 4 + # check we have a numpy list + check_iterable_type("multiplicity", multiplicity, expected_type=Real, + max_depth=max_depth) + if multiplicity.shape == shape: + self._multiplicity = np.copy(multiplicity) + else: + msg = 'Shape of provided multiplicity "{0}" does not match shape ' \ + 'required, "{1}"'.format(multiplicity.shape, shape) + raise ValueError(msg) + + @nu_fission.setter + def nu_fission(self, nu_fission): + # nu_fission can be given as a vector or a matrix + # Vector is used when chi also exists. + # Matrix is used when chi does not exist. + # We have to check that the correct form is given, but only if + # chi already has been set. If not, we just check that this is OK + # and set the use_chi flag. + + # First lets set our dimensions here since they get used repeatedly + # throughout this code. + if self._representation is 'isotropic': + shape_vec = (self._energy_groups.num_groups,) + shape_mat = (self._energy_groups.num_groups, + self._energy_groups.num_groups) + elif self._representation is 'angle': + shape_vec = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups) + shape_mat = (self._num_polar, self._num_azimuthal, + self._energy_groups.num_groups, + self._energy_groups.num_groups) + + # Begin by checking the case when chi has already been given and thus + # the rules for filling in nu_fission are set. + if self._use_chi is not None: + if self._use_chi: + shape = shape_vec + else: + shape = shape_mat + if nu_fission.shape != shape: + msg = "Invalid Shape of Nu_fission!" + raise ValueError(msg) + else: + # Get shape of nu_fission so we can figure if we need chi or not + if nu_fission.shape == shape_vec: + self._use_chi = True + shape = shape_vec + elif nu_fission.shape == shape_mat: + self._use_chi = False + shape = shape_mat + else: + msg = "Invalid Shape of Nu_fission!" + raise ValueError(msg) + + # check we have a numpy list + check_type("nu_fission", nu_fission, np.ndarray, expected_iter_type=Real) + self._nu_fission = np.copy(nu_fission) + if np.sum(self._nu_fission) > 0.0: + self._fissionable = True + + def _get_xsdata_xml(self): + element = ET.Element("xsdata") + element.set("name", self._name) + + if self._alias is not None: + subelement = ET.SubElement(element, 'alias') + subelement.text = self.alias + + if self._kT is not None: + subelement = ET.SubElement(element, 'kT') + subelement.text = str(self._kT) + + if self._fissionable is not None: + subelement = ET.SubElement(element, 'fissionable') + subelement.text = str(self._fissionable) + + if self._representation is not None: + subelement = ET.SubElement(element, 'representation') + subelement.text = self._representation + + if self._representation == 'angle': + if self._num_azimuthal is not None: + subelement = ET.SubElement(element, 'num_azimuthal') + subelement.text = str(self._num_azimuthal) + if self._num_polar is not None: + subelement = ET.SubElement(element, 'num_polar') + subelement.text = str(self._num_polar) + + if self._scatt_type is not None: + subelement = ET.SubElement(element, 'scatt_type') + subelement.text = self._scatt_type + + if self._order is not None: + subelement = ET.SubElement(element, 'order') + subelement.text = str(self._order) + + if self._tabular_legendre is not None: + subelement = ET.SubElement(element, 'tabular_legendre') + subelement.set('enable', str(self._tabular_legendre['enable'])) + subelement.set('num_points', str(self._tabular_legendre['num_points'])) + + if self._total is not None: + subelement = ET.SubElement(element, 'total') + subelement.text = ndarray_to_string(self._total) + + if self._absorption is not None: + subelement = ET.SubElement(element, 'absorption') + subelement.text = ndarray_to_string(self._absorption) + + if self._scatter is not None: + subelement = ET.SubElement(element, 'scatter') + subelement.text = ndarray_to_string(self._scatter) + + if self._multiplicity is not None: + subelement = ET.SubElement(element, 'multiplicity') + subelement.text = ndarray_to_string(self._multiplicity) + + if self._fissionable: + if self._fission is not None: + subelement = ET.SubElement(element, 'fission') + subelement.text = ndarray_to_string(self._fission) + + if self._k_fission is not None: + subelement = ET.SubElement(element, 'k_fission') + subelement.text = ndarray_to_string(self._k_fission) + + if self._nu_fission is not None: + subelement = ET.SubElement(element, 'nu_fission') + subelement.text = ndarray_to_string(self._nu_fission) + + if self._chi is not None: + subelement = ET.SubElement(element, 'chi') + subelement.text = ndarray_to_string(self._chi) + + return element + + +class MGXSLibraryFile(object): + """Multi-Group Cross Sections file used for an OpenMC simulation. + Corresponds directly to the MG version of the cross_sections.xml input file. + + Attributes + ---------- + energy_groups : openmc.mgxs.EnergyGroups + Energy group structure. + inverse_velocities : Iterable of Real + Inverse of velocities, units of sec/cm + xsdatas : Iterable of openmc.XSdata + Iterable of multi-Group cross section data objects + """ + + def __init__(self, energy_groups): + # Initialize MGXSLibraryFile class attributes + self._xsdatas = [] + self._energy_groups = energy_groups + self._inverse_velocities = None + self._cross_sections_file = ET.Element("cross_sections") + + @property + def inverse_velocities(self): + return self._inverse_velocities + + @property + def energy_groups(self): + return self._energy_groups + + @inverse_velocities.setter + def inverse_velocities(self, inverse_velocities): + cv.check_type('inverse_velocities', inverse_velocities, Iterable, Real) + cv.check_greater_than('number of inverse_velocities', + len(inverse_velocities), 0.0) + self._inverse_velocities = np.array(inverse_velocities) + + @energy_groups.setter + def energy_groups(self, energy_groups): + check_type("energy groups", energy_groups, EnergyGroups) + self._energy_groups = energy_groups + + def add_xsdata(self, xsdata): + """Add an XSdata entry to the file. + + Parameters + ---------- + xsdata : openmc.XSdata + MGXS information to add + + """ + + # Check the type + if not isinstance(xsdata, XSdata): + msg = 'Unable to add a non-XSdata "{0}" to the ' \ + 'MGXSLibraryFile'.format(xsdata) + raise ValueError(msg) + + # Make sure energy groups match. + if xsdata.energy_groups != self._energy_groups: + msg = 'Energy groups of XSdata do not match that of MGXSLibraryFile!' + raise ValueError(msg) + + self._xsdatas.append(xsdata) + + def add_xsdatas(self, xsdatas): + """Add multiple xsdatas to the file. + + Parameters + ---------- + xsdatas : tuple or list of openmc.XSdata + XSdatas to add + + """ + + if not isinstance(xsdatas, Iterable): + msg = 'Unable to create OpenMC xsdatas.xml file from "{0}" which ' \ + 'is not iterable'.format(xsdatas) + raise ValueError(msg) + + for xsdata in xsdatas: + self.add_xsdata(xsdata) + + def remove_xsdata(self, xsdata): + """Remove a xsdata from the file + + Parameters + ---------- + xsdata : openmc.XSdata + XSdata to remove + + """ + + if not isinstance(xsdata, XSdata): + msg = 'Unable to remove a non-XSdata "{0}" from the ' \ + 'XSdatasFile'.format(xsdata) + raise ValueError(msg) + + self._xsdatas.remove(xsdata) + + def _create_groups_subelement(self): + if self._energy_groups is not None: + element = ET.SubElement(self._cross_sections_file, "groups") + element.text = str(self._energy_groups.num_groups) + + def _create_group_structure_subelement(self): + if self._energy_groups is not None: + element = ET.SubElement(self._cross_sections_file, + "group_structure") + element.text = ' '.join(map(str, self._energy_groups.group_edges)) + + def _create_inverse_velocities_subelement(self): + if self._inverse_velocities is not None: + element = ET.SubElement(self._cross_sections_file, + "inverse_velocities") + element.text = ' '.join(map(str, self._inverse_velocities)) + + def _create_xsdata_subelements(self): + for xsdata in self._xsdatas: + xml_element = xsdata._get_xsdata_xml() + self._cross_sections_file.append(xml_element) + + def export_to_xml(self, filename='mg_cross_sections.xml'): + """Create an mg_cross_sections.xml file that can be used for a + simulation. + + Parameters + ---------- + filename : str, optional + filename of file, default is mg_cross_sections.xml + + """ + + # Reset xml element tree + self._cross_sections_file.clear() + + self._create_groups_subelement() + self._create_group_structure_subelement() + self._create_inverse_velocities_subelement() + self._create_xsdata_subelements() + + # Clean the indentation in the file to be user-readable + sort_xml_elements(self._cross_sections_file) + clean_xml_indentation(self._cross_sections_file) + + # Write the XML Tree to the xsdatas.xml file + tree = ET.ElementTree(self._cross_sections_file) + tree.write(filename, xml_declaration=True, + encoding='utf-8', method="xml") diff --git a/openmc/nuclide.py b/openmc/nuclide.py index 01fb2aa45..8e97f1a1c 100644 --- a/openmc/nuclide.py +++ b/openmc/nuclide.py @@ -60,6 +60,12 @@ class Nuclide(object): def __ne__(self, other): return not self == other + def __gt__(self, other): + return repr(self) > repr(other) + + def __lt__(self, other): + return not self > other + def __hash__(self): return hash(repr(self)) diff --git a/openmc/opencg_compatible.py b/openmc/opencg_compatible.py index 0bda48c16..d690c2c6a 100644 --- a/openmc/opencg_compatible.py +++ b/openmc/opencg_compatible.py @@ -11,6 +11,7 @@ except ImportError: import openmc from openmc.region import Intersection from openmc.surface import Halfspace +import openmc.checkvalue as cv # A dictionary of all OpenMC Materials created @@ -79,10 +80,7 @@ def get_opencg_material(openmc_material): """ - if not isinstance(openmc_material, openmc.Material): - msg = 'Unable to create an OpenCG Material from "{0}" ' \ - 'which is not an OpenMC Material'.format(openmc_material) - raise ValueError(msg) + cv.check_type('openmc_material', openmc_material, openmc.Material) global OPENCG_MATERIALS material_id = openmc_material.id @@ -119,10 +117,7 @@ def get_openmc_material(opencg_material): """ - if not isinstance(opencg_material, opencg.Material): - msg = 'Unable to create an OpenMC Material from "{0}" ' \ - 'which is not an OpenCG Material'.format(opencg_material) - raise ValueError(msg) + cv.check_type('opencg_material', opencg_material, opencg.Material) global OPENMC_MATERIALS material_id = opencg_material.id @@ -165,10 +160,7 @@ def is_opencg_surface_compatible(opencg_surface): """ - if not isinstance(opencg_surface, opencg.Surface): - msg = 'Unable to check if OpenCG Surface is compatible' \ - 'since "{0}" is not a Surface'.format(opencg_surface) - raise ValueError(msg) + cv.check_type('opencg_surface', opencg_surface, opencg.Surface) if opencg_surface.type in ['x-squareprism', 'y-squareprism', 'z-squareprism']: @@ -192,10 +184,7 @@ def get_opencg_surface(openmc_surface): """ - if not isinstance(openmc_surface, openmc.Surface): - msg = 'Unable to create an OpenCG Surface from "{0}" ' \ - 'which is not an OpenMC Surface'.format(openmc_surface) - raise ValueError(msg) + cv.check_type('openmc_surface', openmc_surface, openmc.Surface) global OPENCG_SURFACES surface_id = openmc_surface.id @@ -278,10 +267,7 @@ def get_openmc_surface(opencg_surface): """ - if not isinstance(opencg_surface, opencg.Surface): - msg = 'Unable to create an OpenMC Surface from "{0}" which ' \ - 'is not an OpenCG Surface'.format(opencg_surface) - raise ValueError(msg) + cv.check_type('opencg_surface', opencg_surface, opencg.Surface) global openmc_surface surface_id = opencg_surface.id @@ -369,10 +355,7 @@ def get_compatible_opencg_surfaces(opencg_surface): """ - if not isinstance(opencg_surface, opencg.Surface): - msg = 'Unable to create an OpenMC Surface from "{0}" which ' \ - 'is not an OpenCG Surface'.format(opencg_surface) - raise ValueError(msg) + cv.check_type('opencg_surface', opencg_surface, opencg.Surface) global OPENMC_SURFACES surface_id = opencg_surface.id @@ -451,10 +434,7 @@ def get_opencg_cell(openmc_cell): """ - if not isinstance(openmc_cell, openmc.Cell): - msg = 'Unable to create an OpenCG Cell from "{0}" which ' \ - 'is not an OpenMC Cell'.format(openmc_cell) - raise ValueError(msg) + cv.check_type('openmc_cell', openmc_cell, openmc.Cell) global OPENCG_CELLS cell_id = openmc_cell.id @@ -469,9 +449,9 @@ def get_opencg_cell(openmc_cell): fill = openmc_cell.fill - if (openmc_cell.fill_type == 'material'): + if openmc_cell.fill_type == 'material': opencg_cell.fill = get_opencg_material(fill) - elif (openmc_cell.fill_type == 'universe'): + elif openmc_cell.fill_type == 'universe': opencg_cell.fill = get_opencg_universe(fill) else: opencg_cell.fill = get_opencg_lattice(fill) @@ -533,20 +513,10 @@ def get_compatible_opencg_cells(opencg_cell, opencg_surface, halfspace): OpenMC """ - if not isinstance(opencg_cell, opencg.Cell): - msg = 'Unable to create compatible OpenMC Cell from "{0}" which ' \ - 'is not an OpenCG Cell'.format(opencg_cell) - raise ValueError(msg) - elif not isinstance(opencg_surface, opencg.Surface): - msg = 'Unable to create compatible OpenMC Cell since "{0}" is ' \ - 'not an OpenCG Surface'.format(opencg_surface) - raise ValueError(msg) - - elif halfspace not in [-1, +1]: - msg = 'Unable to create compatible Cell since "{0}"' \ - 'is not a +/-1 halfspace'.format(halfspace) - raise ValueError(msg) + cv.check_type('opencg_cell', opencg_cell, opencg.Cell) + cv.check_type('opencg_surface', opencg_surface, opencg.Surface) + cv.check_value('halfspace', halfspace, (-1, +1)) # Initialize an empty list for the new compatible cells compatible_cells = [] @@ -575,7 +545,7 @@ def get_compatible_opencg_cells(opencg_cell, opencg_surface, halfspace): num_clones = 8 for clone_id in range(num_clones): - # Create a cloned OpenCG Cell with Surfaces compatible with OpenMC + # Create cloned OpenCG Cell with Surfaces compatible with OpenMC clone = opencg_cell.clone() compatible_cells.append(clone) @@ -641,10 +611,7 @@ def make_opencg_cells_compatible(opencg_universe): """ - if not isinstance(opencg_universe, opencg.Universe): - msg = 'Unable to make compatible OpenCG Cells for "{0}" which ' \ - 'is not an OpenCG Universe'.format(opencg_universe) - raise ValueError(msg) + cv.check_type('opencg_universe', opencg_universe, opencg.Universe) # Check all OpenCG Cells in this Universe for compatibility with OpenMC opencg_cells = opencg_universe.cells @@ -700,10 +667,7 @@ def get_openmc_cell(opencg_cell): """ - if not isinstance(opencg_cell, opencg.Cell): - msg = 'Unable to create an OpenMC Cell from "{0}" which ' \ - 'is not an OpenCG Cell'.format(opencg_cell) - raise ValueError(msg) + cv.check_type('opencg_cell', opencg_cell, opencg.Cell) global OPENMC_CELLS cell_id = opencg_cell.id @@ -718,9 +682,9 @@ def get_openmc_cell(opencg_cell): fill = opencg_cell.fill - if (opencg_cell.type == 'universe'): + if opencg_cell.type == 'universe': openmc_cell.fill = get_openmc_universe(fill) - elif (opencg_cell.type == 'lattice'): + elif opencg_cell.type == 'lattice': openmc_cell.fill = get_openmc_lattice(fill) else: openmc_cell.fill = get_openmc_material(fill) @@ -764,10 +728,7 @@ def get_opencg_universe(openmc_universe): """ - if not isinstance(openmc_universe, openmc.Universe): - msg = 'Unable to create an OpenCG Universe from "{0}" which ' \ - 'is not an OpenMC Universe'.format(openmc_universe) - raise ValueError(msg) + cv.check_type('openmc_universe', openmc_universe, openmc.Universe) global OPENCG_UNIVERSES universe_id = openmc_universe.id @@ -811,10 +772,7 @@ def get_openmc_universe(opencg_universe): """ - if not isinstance(opencg_universe, opencg.Universe): - msg = 'Unable to create an OpenMC Universe from "{0}" which ' \ - 'is not an OpenCG Universe'.format(opencg_universe) - raise ValueError(msg) + cv.check_type('opencg_universe', opencg_universe, opencg.Universe) global OPENMC_UNIVERSES universe_id = opencg_universe.id @@ -861,10 +819,7 @@ def get_opencg_lattice(openmc_lattice): """ - if not isinstance(openmc_lattice, openmc.Lattice): - msg = 'Unable to create an OpenCG Lattice from "{0}" which ' \ - 'is not an OpenMC Lattice'.format(openmc_lattice) - raise ValueError(msg) + cv.check_type('openmc_lattice', openmc_lattice, openmc.Lattice) global OPENCG_LATTICES lattice_id = openmc_lattice.id @@ -958,10 +913,7 @@ def get_openmc_lattice(opencg_lattice): """ - if not isinstance(opencg_lattice, opencg.Lattice): - msg = 'Unable to create an OpenMC Lattice from "{0}" which ' \ - 'is not an OpenCG Lattice'.format(opencg_lattice) - raise ValueError(msg) + cv.check_type('opencg_lattice', opencg_lattice, opencg.Lattice) global OPENMC_LATTICES lattice_id = opencg_lattice.id @@ -1032,10 +984,7 @@ def get_opencg_geometry(openmc_geometry): """ - if not isinstance(openmc_geometry, openmc.Geometry): - msg = 'Unable to get OpenCG geometry from "{0}" which is ' \ - 'not an OpenMC Geometry object'.format(openmc_geometry) - raise ValueError(msg) + cv.check_type('openmc_geometry', openmc_geometry, openmc.Geometry) # Clear dictionaries and auto-generated IDs OPENMC_SURFACES.clear() @@ -1053,6 +1002,7 @@ def get_opencg_geometry(openmc_geometry): opencg_geometry = opencg.Geometry() opencg_geometry.root_universe = opencg_root_universe opencg_geometry.initialize_cell_offsets() + opencg_geometry.assign_auto_ids() return opencg_geometry @@ -1072,10 +1022,7 @@ def get_openmc_geometry(opencg_geometry): """ - if not isinstance(opencg_geometry, opencg.Geometry): - msg = 'Unable to get OpenMC geometry from "{0}" which is ' \ - 'not an OpenCG Geometry object'.format(opencg_geometry) - raise ValueError(msg) + cv.check_type('opencg_geometry', opencg_geometry, opencg.Geometry) # Deep copy the goemetry since it may be modified to make all Surfaces # compatible with OpenMC's specifications diff --git a/openmc/plots.py b/openmc/plots.py index 636ca225c..6e78995f4 100644 --- a/openmc/plots.py +++ b/openmc/plots.py @@ -275,7 +275,7 @@ class Plot(object): The random number seed used to generate the color scheme """ - + cv.check_type('geometry', geometry, openmc.Geometry) cv.check_type('seed', seed, Integral) cv.check_greater_than('seed', seed, 1, equality=True) @@ -417,7 +417,7 @@ class PlotsFile(object): Parameters ---------- - plot : Plot + plot : openmc.Plot Plot to add """ @@ -433,7 +433,7 @@ class PlotsFile(object): Parameters ---------- - plot : Plot + plot : openmc.Plot Plot to remove """ diff --git a/openmc/region.py b/openmc/region.py index 7589184aa..a2edbeedd 100644 --- a/openmc/region.py +++ b/openmc/region.py @@ -9,10 +9,11 @@ from openmc.checkvalue import check_type class Region(object): """Region of space that can be assigned to a cell. - Region is an abstract base class that is inherited by Halfspace, - Intersection, Union, and Complement. Each of those respective classes are - typically not instantiated directly but rather are created through operators - of the Surface and Region classes. + Region is an abstract base class that is inherited by + :class:`openmc.Halfspace`, :class:`openmc.Intersection`, + :class:`openmc.Union`, and :class:`openmc.Complement`. Each of those + respective classes are typically not instantiated directly but rather are + created through operators of the Surface and Region classes. """ @@ -201,11 +202,11 @@ class Intersection(Region): """Intersection of two or more regions. Instances of Intersection are generally created via the __and__ operator - applied to two instances of Region. This is illustrated in the following - example: + applied to two instances of :class:`openmc.Region`. This is illustrated in + the following example: - >>> equator = openmc.surface.ZPlane(z0=0.0) - >>> earth = openmc.surface.Sphere(R=637.1e6) + >>> equator = openmc.ZPlane(z0=0.0) + >>> earth = openmc.Sphere(R=637.1e6) >>> northern_hemisphere = -earth & +equator >>> southern_hemisphere = -earth & -equator >>> type(northern_hemisphere) @@ -213,12 +214,12 @@ class Intersection(Region): Parameters ---------- - *nodes + \*nodes Regions to take the intersection of Attributes ---------- - nodes : tuple of Region + nodes : tuple of openmc.Region Regions to take the intersection of bounding_box : tuple of numpy.array Lower-left and upper-right coordinates of an axis-aligned bounding box @@ -255,21 +256,22 @@ class Union(Region): """Union of two or more regions. Instances of Union are generally created via the __or__ operator applied to - two instances of Region. This is illustrated in the following example: + two instances of :class:`openmc.Region`. This is illustrated in the + following example: - >>> s1 = openmc.surface.ZPlane(z0=0.0) - >>> s2 = openmc.surface.Sphere(R=637.1e6) + >>> s1 = openmc.ZPlane(z0=0.0) + >>> s2 = openmc.Sphere(R=637.1e6) >>> type(-s2 | +s1) Parameters ---------- - *nodes + \*nodes Regions to take the union of Attributes ---------- - nodes : tuple of Region + nodes : tuple of openmc.Region Regions to take the union of bounding_box : tuple of numpy.array Lower-left and upper-right coordinates of an axis-aligned bounding box @@ -305,13 +307,13 @@ class Union(Region): class Complement(Region): """Complement of a region. - The Complement of an existing Region can be created by using the __invert__ - operator as the following example demonstrates: + The Complement of an existing :class:`openmc.Region` can be created by using + the __invert__ operator as the following example demonstrates: - >>> xl = openmc.surface.XPlane(x0=-10.0) - >>> xr = openmc.surface.XPlane(x0=10.0) - >>> yl = openmc.surface.YPlane(y0=-10.0) - >>> yr = openmc.surface.YPlane(y0=10.0) + >>> xl = openmc.XPlane(x0=-10.0) + >>> xr = openmc.XPlane(x0=10.0) + >>> yl = openmc.YPlane(y0=-10.0) + >>> yr = openmc.YPlane(y0=10.0) >>> inside_box = +xl & -xr & +yl & -yl >>> outside_box = ~inside_box >>> type(outside_box) @@ -319,12 +321,12 @@ class Complement(Region): Parameters ---------- - node : Region + node : openmc.Region Region to take the complement of Attributes ---------- - node : Region + node : openmc.Region Regions to take the complement of bounding_box : tuple of numpy.array Lower-left and upper-right coordinates of an axis-aligned bounding box diff --git a/openmc/settings.py b/openmc/settings.py index ec386c2f8..c01f2afd7 100644 --- a/openmc/settings.py +++ b/openmc/settings.py @@ -9,6 +9,7 @@ import numpy as np from openmc.clean_xml import * from openmc.checkvalue import (check_type, check_length, check_value, check_greater_than, check_less_than) +from openmc import Nuclide from openmc.source import Source if sys.version_info[0] >= 3: @@ -37,7 +38,7 @@ class SettingsFile(object): type are 'variance', 'std_dev', and 'rel_err'. The threshold value should be a float indicating the variance, standard deviation, or relative error used. - source : Iterable of openmc.source.Source + source : Iterable of openmc.Source Distribution of source sites in space, angle, and energy output : dict Dictionary indicating what files to output. Valid keys are 'summary', @@ -70,15 +71,20 @@ class SettingsFile(object): cross_sections : str Indicates the path to an XML cross section listing file (usually named cross_sections.xml). If it is not set, the :envvar:`CROSS_SECTIONS` - environment variable will be used to find the path to the XML cross - section listing. + environment variable will be used for continuous-energy calculations + and :envvar:`MG_CROSS_SECTIONS` will be used for multi-group + calculations to find the path to the XML cross section file. multipole_library : str Indicates the path to a directory containing a windowed multipole - cross section library. If it is not set, the :envvar:`MULTIPOLE_LIBRARY' - environment variable will be used. A multipole library is optional. - energy_grid : str - Set the method used to search energy grids. Acceptable values are - 'nuclide', 'logarithm', and 'material-union'. + cross section library. If it is not set, the + :envvar:`OPENMC_MULTIPOLE_LIBRARY' environment variable will be used. A + multipole library is optional. + energy_grid : {'nuclide', 'logarithm', 'material-union'} + Set the method used to search energy grids. + energy_mode : {'continuous-energy', 'multi-group'} + Set whether the calculation should be continuous-energy or multi-group. + max_order : int + Maximum scattering order to apply globally when in multi-group mode. ptables : bool Determine whether probability tables are used. run_cmfd : bool @@ -128,6 +134,8 @@ class SettingsFile(object): use_windowed_multipole : bool Whether or not windowed multipole can be used to evaluate resolved resonance cross sections. + resonance_scattering : ResonanceScattering or iterable of ResonanceScattering + The elastic scattering model to use for resonant isotopes """ @@ -141,6 +149,10 @@ class SettingsFile(object): self._particles = None self._keff_trigger = None + # Energy mode subelement + self._energy_mode = None + self._max_order = None + # Source subelement self._source = None @@ -206,6 +218,8 @@ class SettingsFile(object): self._source_element = None self._multipole_active = None + self._resonance_scattering = None + @property def run_mode(self): return self._run_mode @@ -230,6 +244,14 @@ class SettingsFile(object): def keff_trigger(self): return self._keff_trigger + @property + def energy_mode(self): + return self._energy_mode + + @property + def max_order(self): + return self._max_order + @property def source(self): return self._source @@ -394,9 +416,13 @@ class SettingsFile(object): def use_windowed_multipole(self): return self._multipole_active + @property + def resonance_scattering(self): + return self._resonance_scattering + @run_mode.setter def run_mode(self, run_mode): - if 'run_mode' not in ['eigenvalue', 'fixed source']: + if run_mode not in ['eigenvalue', 'fixed source']: msg = 'Unable to set run mode to "{0}". Only "eigenvalue" ' \ 'and "fixed source" are supported."'.format(run_mode) raise ValueError(msg) @@ -455,6 +481,18 @@ class SettingsFile(object): self._keff_trigger = keff_trigger + @energy_mode.setter + def energy_mode(self, energy_mode): + check_value('energy mode', energy_mode, + ['continuous-energy', 'multi-group']) + self._energy_mode = energy_mode + + @max_order.setter + def max_order(self, max_order): + check_type('maximum scattering order', max_order, Integral) + check_greater_than('maximum scattering order', max_order, 0, True) + self._max_order = max_order + @source.setter def source(self, source): if isinstance(source, Source): @@ -763,6 +801,16 @@ class SettingsFile(object): check_type('use_windowed_multipole', active, bool) self._multipole_active = active + @resonance_scattering.setter + def resonance_scattering(self, res): + if isinstance(res, Iterable): + check_type('resonance_scattering', res, Iterable, + ResonanceScattering) + self._resonance_scattering = res + else: + check_type('resonance_scattering', res, ResonanceScattering) + self._resonance_scattering = [res] + def _create_run_mode_subelement(self): if self.run_mode == 'eigenvalue': @@ -809,6 +857,16 @@ class SettingsFile(object): subelement = ET.SubElement(element, key) subelement.text = str(self._keff_trigger[key]).lower() + def _create_energy_mode_subelement(self): + if self._energy_mode is not None: + element = ET.SubElement(self._settings_file, "energy_mode") + element.text = str(self._energy_mode) + + def _create_max_order_subelement(self): + if self._max_order is not None: + element = ET.SubElement(self._settings_file, "max_order") + element.text = str(self._max_order) + def _create_source_subelement(self): if self.source is not None: for source in self.source: @@ -1002,7 +1060,7 @@ class SettingsFile(object): element = ET.SubElement(self._settings_file, "uniform_fs") subelement = ET.SubElement(element, "dimension") - subelement.text = str(self._ufs_dimension) + subelement.text = ' '.join(map(str, self._ufs_dimension)) subelement = ET.SubElement(element, "lower_left") subelement.text = ' '.join(map(str, self._ufs_lower_left)) @@ -1043,6 +1101,17 @@ class SettingsFile(object): "use_windowed_multipole") element.text = str(self._multipole_active) + def _create_resonance_scattering_element(self): + if self.resonance_scattering is None: return + + element = ET.SubElement(self._settings_file, "resonance_scattering") + + for r in self.resonance_scattering: + if r.nuclide.name != r.nuclide_0K.name: + raise ValueError("The nuclide and nuclide_0K attributes of " + "a ResonantScattering object must have identical names.") + r.create_xml_subelement(element) + def export_to_xml(self): """Create a settings.xml file that can be used for a simulation. @@ -1064,6 +1133,8 @@ class SettingsFile(object): self._create_cross_sections_subelement() self._create_multipole_library_subelement() self._create_energy_grid_subelement() + self._create_energy_mode_subelement() + self._create_max_order_subelement() self._create_ptables_subelement() self._create_run_cmfd_subelement() self._create_seed_subelement() @@ -1079,6 +1150,7 @@ class SettingsFile(object): self._create_ufs_subelement() self._create_dd_subelement() self._create_use_multipole_subelement() + self._create_resonance_scattering_element() # Clean the indentation in the file to be user-readable clean_xml_indentation(self._settings_file) @@ -1087,3 +1159,104 @@ class SettingsFile(object): tree = ET.ElementTree(self._settings_file) tree.write("settings.xml", xml_declaration=True, encoding='utf-8', method="xml") + + +class ResonanceScattering(object): + """Specification of the elastic scattering model for resonant isotopes + + Attributes + ---------- + nuclide : openmc.Nuclide + The nuclide affected by this resonance scattering treatment. + nuclide_0K : openmc.Nuclide + This should be the same isotope as the nuclide attribute above, but it + should have an xs attribute that identifies 0 Kelvin data. + method : str + The method used to sample outgoing scattering energies. Valid options + are 'ARES', 'CXS' (constant cross section), 'DBRC' (Doppler broadening + rejection correction), and 'WCM' (weight correction method). + E_min : float + The minimum energy above which the specified method is applied. By + default, CXS will be used below E_min. + E_max : float + The maximum energy below which the specified method is applied. By + default, the asymptotic target-at-rest model is applied above E_max. + + """ + + def __init__(self): + self._nuclide = None + self._nuclide_0K = None + self._method = None + self._E_min = None + self._E_max = None + + @property + def nuclide(self): + return self._nuclide + + @property + def nuclide_0K(self): + return self._nuclide_0K + + @property + def method(self): + return self._method + + @property + def E_min(self): + return self._E_min + + @property + def E_max(self): + return self._E_max + + @nuclide.setter + def nuclide(self, nuc): + check_type('nuclide', nuc, Nuclide) + if nuc.zaid == None: raise ValueError("The nuclide must have an " + "explicitly defined zaid attribute.") + self._nuclide = nuc + + @nuclide_0K.setter + def nuclide_0K(self, nuc): + check_type('nuclide_0K', nuc, Nuclide) + if nuc.zaid == None: raise ValueError("The nuclide_0K must have an " + "explicitly defined zaid attribute.") + self._nuclide_0K = nuc + + @method.setter + def method(self, m): + check_value('method', m, ('ARES', 'CXS', 'DBRC', 'WCM')) + self._method = m + + @E_min.setter + def E_min(self, E): + check_type('E_min', E, Real) + check_greater_than('E_min', E, 0, True) + self._E_min = E + + @E_max.setter + def E_max(self, E): + check_type('E_max', E, Real) + check_greater_than('E_max', E, 0, True) + self._E_max = E + + def create_xml_subelement(self, xml_element): + scatterer = ET.SubElement(xml_element, "scatterer") + subelement = ET.SubElement(scatterer, 'nuclide') + subelement.text = self.nuclide.name + if self.method is not None: + subelement = ET.SubElement(scatterer, 'method') + subelement.text = self.method + subelement = ET.SubElement(scatterer, 'xs_label') + subelement.text = str(self.nuclide.zaid) + '.' + str(self.nuclide.xs) + subelement = ET.SubElement(scatterer, 'xs_label_0K') + subelement.text = str(self.nuclide_0K.zaid) + '.' \ + + str(self.nuclide_0K.xs) + if self.E_min is not None: + subelement = ET.SubElement(scatterer, 'E_min') + subelement.text = str(self.E_min) + if self.E_max is not None: + subelement = ET.SubElement(scatterer, 'E_max') + subelement.text = str(self.E_max) diff --git a/openmc/statepoint.py b/openmc/statepoint.py index a1f19ecd8..e11b1c096 100644 --- a/openmc/statepoint.py +++ b/openmc/statepoint.py @@ -18,59 +18,62 @@ class StatePoint(object): ---------- cmfd_on : bool Indicate whether CMFD is active - cmfd_balance : ndarray + cmfd_balance : numpy.ndarray Residual neutron balance for each batch cmfd_dominance Dominance ratio for each batch - cmfd_entropy : ndarray + cmfd_entropy : numpy.ndarray Shannon entropy of CMFD fission source for each batch - cmfd_indices : ndarray + cmfd_indices : numpy.ndarray Number of CMFD mesh cells and energy groups. The first three indices correspond to the x-, y-, and z- spatial directions and the fourth index is the number of energy groups. - cmfd_srccmp : ndarray + cmfd_srccmp : numpy.ndarray Root-mean-square difference between OpenMC and CMFD fission source for each batch - cmfd_src : ndarray + cmfd_src : numpy.ndarray CMFD fission source distribution over all mesh cells and energy groups. - current_batch : Integral + current_batch : int Number of batches simulated date_and_time : str Date and time when simulation began - entropy : ndarray + entropy : numpy.ndarray Shannon entropy of fission source at each batch gen_per_batch : Integral Number of fission generations per batch - global_tallies : ndarray of compound datatype + global_tallies : numpy.ndarray of compound datatype Global tallies for k-effective estimates and leakage. The compound datatype has fields 'name', 'sum', 'sum_sq', 'mean', and 'std_dev'. k_combined : list Combined estimator for k-effective and its uncertainty - k_col_abs : Real + k_col_abs : float Cross-product of collision and absorption estimates of k-effective - k_col_tra : Real + k_col_tra : float Cross-product of collision and tracklength estimates of k-effective - k_abs_tra : Real + k_abs_tra : float Cross-product of absorption and tracklength estimates of k-effective - k_generation : ndarray + k_generation : numpy.ndarray Estimate of k-effective for each batch/generation meshes : dict Dictionary whose keys are mesh IDs and whose values are Mesh objects - n_batches : Integral + n_batches : int Number of batches - n_inactive : Integral + n_inactive : int Number of inactive batches - n_particles : Integral + n_particles : int Number of particles per generation - n_realizations : Integral + n_realizations : int Number of tally realizations path : str Working directory for simulation run_mode : str Simulation run mode, e.g. 'k-eigenvalue' - seed : Integral + runtime : dict + Dictionary whose keys are strings describing various runtime metrics + and whose values are time values in seconds. + seed : int Pseudorandom number generator seed - source : ndarray of compound datatype + source : numpy.ndarray of compound datatype Array of source sites. The compound datatype has fields 'wgt', 'xyz', 'uvw', and 'E' corresponding to the weight, position, direction, and energy of the source site. @@ -88,7 +91,7 @@ class StatePoint(object): TallyDerivative objects version: tuple of Integral Version of OpenMC - summary : None or openmc.summary.Summary + summary : None or openmc.Summary A summary object if the statepoint has been linked with a summary file """ @@ -104,13 +107,14 @@ class StatePoint(object): raise IOError('{} is not a statepoint file.'.format(filename)) except AttributeError: raise IOError('Could not read statepoint file. This most likely ' - 'means the statepoint file was produced by a different ' - 'version of OpenMC than the one you are using.') - if self._f['revision'].value != 14: + 'means the statepoint file was produced by a ' + 'different version of OpenMC than the one you are ' + 'using.') + if self._f['revision'].value != 15: raise IOError('Statepoint file has a file revision of {} ' 'which is not consistent with the revision this ' 'version of OpenMC expects ({}).'.format( - self._f['revision'].value, 14)) + self._f['revision'].value, 15)) # Set flags for what data has been read self._meshes_read = False @@ -315,6 +319,11 @@ class StatePoint(object): def run_mode(self): return self._f['run_mode'].value.decode() + @property + def runtime(self): + return {name: dataset.value + for name, dataset in self._f['runtime'].items()} + @property def seed(self): return self._f['seed'].value @@ -399,7 +408,7 @@ class StatePoint(object): new_filter.mesh = self.meshes[key] # Add Filter to the Tally - tally.add_filter(new_filter) + tally.filters.append(new_filter) # Read Nuclide bins nuclide_names = \ @@ -408,7 +417,7 @@ class StatePoint(object): # Add all Nuclides to the Tally for name in nuclide_names: nuclide = openmc.Nuclide(name.decode().strip()) - tally.add_nuclide(nuclide) + tally.nuclides.append(nuclide) scores = self._f['{0}{1}/score_bins'.format( base, tally_key)].value @@ -435,7 +444,7 @@ class StatePoint(object): pattern = r'-n$|-pn$|-yn$' score = re.sub(pattern, '-' + moments[j].decode(), score) - tally.add_score(score) + tally.scores.append(score) # Add Tally to the global dictionary of all Tallies tally.sparse = self.sparse @@ -542,7 +551,7 @@ class StatePoint(object): Returns ------- - tally : Tally + tally : openmc.Tally A tally matching the specified criteria Raises @@ -639,7 +648,7 @@ class StatePoint(object): Parameters ---------- - summary : Summary + summary : openmc.Summary A Summary object. Raises @@ -656,11 +665,13 @@ class StatePoint(object): raise ValueError(msg) for tally_id, tally in self.tallies.items(): - # Get the Tally name from the summary file - tally.name = summary.tallies[tally_id].name + summary_tally = summary.tallies[tally_id] + tally.name = summary_tally.name tally.with_summary = True for tally_filter in tally.filters: + summary_filter = summary_tally.find_filter(tally_filter.type) + if tally_filter.type == 'surface': surface_ids = [] for bin in tally_filter.bins: @@ -673,6 +684,10 @@ class StatePoint(object): distribcell_ids.append(summary.cells[bin].id) tally_filter.bins = distribcell_ids + if tally_filter.type == 'distribcell': + tally_filter.distribcell_paths = \ + summary_filter.distribcell_paths + if tally_filter.type == 'universe': universe_ids = [] for bin in tally_filter.bins: diff --git a/openmc/stats/multivariate.py b/openmc/stats/multivariate.py index 29258ee8d..4ce34a071 100644 --- a/openmc/stats/multivariate.py +++ b/openmc/stats/multivariate.py @@ -22,12 +22,12 @@ class UnitSphere(object): Parameters ---------- - reference_uvw : Iterable of Real + reference_uvw : Iterable of float Direction from which polar angle is measured Attributes ---------- - reference_uvw : Iterable of Real + reference_uvw : Iterable of float Direction from which polar angle is measured """ @@ -62,19 +62,19 @@ class PolarAzimuthal(UnitSphere): Parameters ---------- - mu : Univariate + mu : openmc.stats.Univariate Distribution of the cosine of the polar angle - phi : Univariate + phi : openmc.stats.Univariate Distribution of the azimuthal angle in radians - reference_uvw : Iterable of Real + reference_uvw : Iterable of float Direction from which polar angle is measured. Defaults to the positive z-direction. Attributes ---------- - mu : Univariate + mu : openmc.stats.Univariate Distribution of the cosine of the polar angle - phi : Univariate + phi : openmc.stats.Univariate Distribution of the azimuthal angle in radians """ @@ -142,7 +142,7 @@ class Monodirectional(UnitSphere): Parameters ---------- - reference_uvw : Iterable of Real + reference_uvw : Iterable of float Direction from which polar angle is measured. Defaults to the positive x-direction. @@ -186,20 +186,20 @@ class CartesianIndependent(Spatial): Parameters ---------- - x : Univariate + x : openmc.stats.Univariate Distribution of x-coordinates - y : Univariate + y : openmc.stats.Univariate Distribution of y-coordinates - z : Univariate + z : openmc.stats.Univariate Distribution of z-coordinates Attributes ---------- - x : Univariate + x : openmc.stats.Univariate Distribution of x-coordinates - y : Univariate + y : openmc.stats.Univariate Distribution of y-coordinates - z : Univariate + z : openmc.stats.Univariate Distribution of z-coordinates """ @@ -252,9 +252,9 @@ class Box(Spatial): Parameters ---------- - lower_left : Iterable of Real + lower_left : Iterable of float Lower-left coordinates of cuboid - upper_right : Iterable of Real + upper_right : Iterable of float Upper-right coordinates of cuboid only_fissionable : bool, optional Whether spatial sites should only be accepted if they occur in @@ -262,9 +262,9 @@ class Box(Spatial): Attributes ---------- - lower_left : Iterable of Real + lower_left : Iterable of float Lower-left coordinates of cuboid - upper_right : Iterable of Real + upper_right : Iterable of float Upper-right coordinates of cuboid only_fissionable : bool, optional Whether spatial sites should only be accepted if they occur in @@ -328,12 +328,12 @@ class Point(Spatial): Parameters ---------- - xyz : Iterable of Real + xyz : Iterable of float Cartesian coordinates of location Attributes ---------- - xyz : Iterable of Real + xyz : Iterable of float Cartesian coordinates of location """ diff --git a/openmc/stats/univariate.py b/openmc/stats/univariate.py index 04e70bd00..0deeb600c 100644 --- a/openmc/stats/univariate.py +++ b/openmc/stats/univariate.py @@ -37,16 +37,16 @@ class Discrete(Univariate): Parameters ---------- - x : Iterable of Real + x : Iterable of float Values of the random variable - p : Iterable of Real + p : Iterable of float Discrete probability for each value Attributes ---------- - x : Iterable of Real + x : Iterable of float Values of the random variable - p : Iterable of Real + p : Iterable of float Discrete probability for each value """ @@ -243,9 +243,9 @@ class Tabular(Univariate): Parameters ---------- - x : Iterable of Real + x : Iterable of float Tabulated values of the random variable - p : Iterable of Real + p : Iterable of float Tabulated probabilities interpolation : {'histogram', 'linear-linear'}, optional Indicate whether the density function is constant between tabulated @@ -253,9 +253,9 @@ class Tabular(Univariate): Attributes ---------- - x : Iterable of Real + x : Iterable of float Tabulated values of the random variable - p : Iterable of Real + p : Iterable of float Tabulated probabilities interpolation : {'histogram', 'linear-linear'}, optional Indicate whether the density function is constant between tabulated diff --git a/openmc/summary.py b/openmc/summary.py index 614a02206..fbe3f90c8 100644 --- a/openmc/summary.py +++ b/openmc/summary.py @@ -60,6 +60,9 @@ class Summary(object): # Read date and time self.date_and_time = self._f['date_and_time'][...] + # Read if continuous-energy or multi-group + self.run_CE = (self._f['run_CE'].value == 1) + self.n_batches = self._f['n_batches'].value self.n_particles = self._f['n_particles'].value self.n_active = self._f['n_active'].value @@ -279,7 +282,7 @@ class Summary(object): # Get the distribcell index ind = self._f['geometry/cells'][key]['distribcell_index'].value if ind != 0: - cell.distribcell_index = ind + cell.distribcell_index = ind # Add the Cell to the global dictionary of all Cells self.cells[index] = cell @@ -542,7 +545,7 @@ class Summary(object): # If this is a moment, use generic moment order pattern = r'-n$|-pn$|-yn$' score = re.sub(pattern, '-' + moments[j].decode(), score) - tally.add_score(score) + tally.scores.append(score) # Read filter metadata num_filters = self._f['{0}/n_filters'.format(subbase)].value @@ -562,8 +565,14 @@ class Summary(object): new_filter = openmc.Filter(filter_type, bins) new_filter.num_bins = num_bins + # Read in distribcell paths + if filter_type == 'distribcell': + paths = self._f['{0}/paths'.format(subsubbase)][...] + paths = [str(path.decode()) for path in paths] + new_filter.distribcell_paths = paths + # Add Filter to the Tally - tally.add_filter(new_filter) + tally.filters.append(new_filter) # Add Tally to the global dictionary of all Tallies self.tallies[tally_id] = tally @@ -578,7 +587,7 @@ class Summary(object): Returns ------- - material : openmc.material.Material + material : openmc.Material Material with given id """ @@ -599,7 +608,7 @@ class Summary(object): Returns ------- - surface : openmc.surface.Surface + surface : openmc.Surface Surface with given id """ @@ -620,7 +629,7 @@ class Summary(object): Returns ------- - cell : openmc.universe.Cell + cell : openmc.Cell Cell with given id """ @@ -641,7 +650,7 @@ class Summary(object): Returns ------- - universe : openmc.universe.Universe + universe : openmc.Universe Universe with given id """ @@ -662,7 +671,7 @@ class Summary(object): Returns ------- - lattice : openmc.universe.Lattice + lattice : openmc.Lattice Lattice with given id """ diff --git a/openmc/surface.py b/openmc/surface.py index 8dc45209b..5c8b20856 100644 --- a/openmc/surface.py +++ b/openmc/surface.py @@ -153,10 +153,10 @@ class Surface(object): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -278,8 +278,7 @@ class Plane(Surface): class XPlane(Plane): - """A plane perpendicular to the x axis, i.e. a surface of the form :math:`x - - x_0 = 0` + """A plane perpendicular to the x axis of the form :math:`x - x_0 = 0` Parameters ---------- @@ -338,10 +337,10 @@ class XPlane(Plane): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -356,8 +355,7 @@ class XPlane(Plane): class YPlane(Plane): - """A plane perpendicular to the y axis, i.e. a surface of the form :math:`y - - y_0 = 0` + """A plane perpendicular to the y axis of the form :math:`y - y_0 = 0` Parameters ---------- @@ -416,10 +414,10 @@ class YPlane(Plane): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -434,8 +432,7 @@ class YPlane(Plane): class ZPlane(Plane): - """A plane perpendicular to the z axis, i.e. a surface of the form :math:`z - - z_0 = 0` + """A plane perpendicular to the z axis of the form :math:`z - z_0 = 0` Parameters ---------- @@ -494,10 +491,10 @@ class ZPlane(Plane): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -641,10 +638,10 @@ class XCylinder(Cylinder): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -740,10 +737,10 @@ class YCylinder(Cylinder): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -839,10 +836,10 @@ class ZCylinder(Cylinder): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -967,10 +964,10 @@ class Sphere(Surface): Returns ------- - numpy.array + numpy.ndarray Lower-left coordinates of the axis-aligned bounding box for the desired half-space - numpy.array + numpy.ndarray Upper-right coordinates of the axis-aligned bounding box for the desired half-space @@ -1383,7 +1380,7 @@ class Halfspace(Region): can be created from an existing Surface through the __neg__ and __pos__ operators, as the following example demonstrates: - >>> sphere = openmc.surface.Sphere(surface_id=1, R=10.0) + >>> sphere = openmc.Sphere(surface_id=1, R=10.0) >>> inside_sphere = -sphere >>> outside_sphere = +sphere >>> type(inside_sphere) @@ -1391,18 +1388,18 @@ class Halfspace(Region): Parameters ---------- - surface : Surface + surface : openmc.Surface Surface which divides Euclidean space. side : {'+', '-'} Indicates whether the positive or negative half-space is used. Attributes ---------- - surface : Surface + surface : openmc.Surface Surface which divides Euclidean space. side : {'+', '-'} Indicates whether the positive or negative half-space is used. - bounding_box : tuple of numpy.array + bounding_box : tuple of numpy.ndarray Lower-left and upper-right coordinates of an axis-aligned bounding box """ diff --git a/openmc/tallies.py b/openmc/tallies.py index ae9493b16..3d37da65b 100644 --- a/openmc/tallies.py +++ b/openmc/tallies.py @@ -1,13 +1,15 @@ from __future__ import division -from collections import Iterable, defaultdict +from collections import Iterable, MutableSequence, defaultdict import copy +from functools import partial import os import pickle import itertools from numbers import Integral, Real -from xml.etree import ElementTree as ET import sys +import warnings +from xml.etree import ElementTree as ET import numpy as np @@ -17,10 +19,10 @@ from openmc.filter import _FILTER_TYPES import openmc.checkvalue as cv from openmc.clean_xml import * - if sys.version_info[0] >= 3: basestring = str + # "Static" variable for auto-generated Tally IDs AUTO_TALLY_ID = 10000 @@ -31,6 +33,12 @@ AUTO_TALLY_ID = 10000 # specified axis. _PRODUCT_TYPES = ['tensor', 'entrywise'] +# The following indicate acceptable types when setting Tally.scores, +# Tally.nuclides, and Tally.filters +_SCORE_CLASSES = (basestring, CrossScore, AggregateScore) +_NUCLIDE_CLASSES = (basestring, Nuclide, CrossNuclide, AggregateNuclide) +_FILTER_CLASSES = (Filter, CrossFilter, AggregateFilter) + def reset_auto_tally_id(): global AUTO_TALLY_ID @@ -43,7 +51,7 @@ class Tally(object): Parameters ---------- - tally_id : Integral, optional + tally_id : int, optional Unique identifier for the tally. If none is specified, an identifier will automatically be assigned name : str, optional @@ -51,43 +59,43 @@ class Tally(object): Attributes ---------- - id : Integral + id : int Unique identifier for the tally name : str Name of the tally - filters : list of openmc.filter.Filter + filters : list of openmc.Filter List of specified filters for the tally - nuclides : list of openmc.nuclide.Nuclide + nuclides : list of openmc.Nuclide List of nuclides to score results for scores : list of str List of defined scores, e.g. 'flux', 'fission', etc. estimator : {'analog', 'tracklength', 'collision'} Type of estimator for the tally - triggers : list of openmc.trigger.Trigger + triggers : list of openmc.Trigger List of tally triggers - num_scores : Integral + num_scores : int Total number of scores, accounting for the fact that a single user-specified score, e.g. scatter-P3 or flux-Y2,2, might have multiple bins - num_filter_bins : Integral + num_filter_bins : int Total number of filter bins accounting for all filters - num_bins : Integral + num_bins : int Total number of bins for the tally - shape : 3-tuple of Integral - The shape of the tally data array ordered as the number of filter bins, + shape : 3-tuple of int + The shape of the tally data array ordered as the number of filter bins, nuclide bins and score bins - num_realizations : Integral + num_realizations : int Total number of realizations with_summary : bool Whether or not a Summary has been linked - sum : ndarray + sum : numpy.ndarray An array containing the sum of each independent realization for each bin - sum_sq : ndarray + sum_sq : numpy.ndarray An array containing the sum of each independent realization squared for each bin - mean : ndarray + mean : numpy.ndarray An array containing the sample mean for each bin - std_dev : ndarray + std_dev : numpy.ndarray An array containing the sample standard deviation for each bin derived : bool Whether or not the tally is derived from one or more other tallies @@ -103,11 +111,11 @@ class Tally(object): # Initialize Tally class attributes self.id = tally_id self.name = name - self._filters = [] - self._nuclides = [] - self._scores = [] + self._filters = cv.CheckedList(_FILTER_CLASSES, 'tally filters') + self._nuclides = cv.CheckedList(_NUCLIDE_CLASSES, 'tally nuclides') + self._scores = cv.CheckedList(_SCORE_CLASSES, 'tally scores') self._estimator = None - self._triggers = [] + self._triggers = cv.CheckedList(Trigger, 'tally triggers') self._derivative = None self._num_realizations = 0 @@ -148,19 +156,19 @@ class Tally(object): clone._filters = [] for self_filter in self.filters: - clone.add_filter(copy.deepcopy(self_filter, memo)) + clone.filters.append(copy.deepcopy(self_filter, memo)) clone._nuclides = [] for nuclide in self.nuclides: - clone.add_nuclide(copy.deepcopy(nuclide, memo)) + clone.nuclides.append(copy.deepcopy(nuclide, memo)) clone._scores = [] for score in self.scores: - clone.add_score(score) + clone.scores.append(score) clone._triggers = [] for trigger in self.triggers: - clone.add_trigger(trigger) + clone.triggers.append(trigger) memo[id(self)] = clone @@ -313,7 +321,7 @@ class Tally(object): @property def sum(self): - if not self._sp_filename: + if not self._sp_filename or self.derived: return None if not self._results_read: @@ -438,23 +446,30 @@ class Tally(object): ['analog', 'tracklength', 'collision']) self._estimator = estimator + @triggers.setter + def triggers(self, triggers): + cv.check_type('tally triggers', triggers, MutableSequence) + self._triggers = cv.CheckedList(Trigger, 'tally triggers', triggers) + def add_trigger(self, trigger): """Add a tally trigger to the tally + .. deprecated:: 0.8 + Use the Tally.triggers property directly, i.e., + Tally.triggers.append(...) + Parameters ---------- - trigger : openmc.trigger.Trigger + trigger : openmc.Trigger Trigger to add """ - if not isinstance(trigger, Trigger): - msg = 'Unable to add a tally trigger for Tally ID="{0}" to ' \ - 'since "{1}" is not a Trigger'.format(self.id, trigger) - raise ValueError(msg) - - if trigger not in self.triggers: - self.triggers.append(trigger) + warnings.warn('Tally.add_trigger(...) has been deprecated and may be ' + 'removed in a future version. Tally triggers should be ' + 'defined using the triggers property directly.', + DeprecationWarning) + self.triggers.append(trigger) @id.setter def id(self, tally_id): @@ -481,9 +496,60 @@ class Tally(object): cv.check_type('tally derivative', deriv, TallyDerivative) self._derivative = deriv + @filters.setter + def filters(self, filters): + cv.check_type('tally filters', filters, MutableSequence) + + # If the filter is already in the Tally, raise an error + for i, f in enumerate(filters[:-1]): + if f in filters[i+1:]: + msg = 'Unable to add a duplicate filter "{0}" to Tally ID="{1}" ' \ + 'since duplicate filters are not supported in the OpenMC ' \ + 'Python API'.format(f, self.id) + raise ValueError(msg) + + self._filters = cv.CheckedList(_FILTER_CLASSES, 'tally filters', filters) + + @nuclides.setter + def nuclides(self, nuclides): + cv.check_type('tally nuclides', nuclides, MutableSequence) + + # If the nuclide is already in the Tally, raise an error + for i, nuclide in enumerate(nuclides[:-1]): + if nuclide in nuclides[i+1:]: + msg = 'Unable to add a duplicate nuclide "{0}" to Tally ID="{1}" ' \ + 'since duplicate nuclides are not supported in the OpenMC ' \ + 'Python API'.format(nuclide, self.id) + raise ValueError(msg) + + self._nuclides = cv.CheckedList(_NUCLIDE_CLASSES, 'tally nuclides', + nuclides) + + @scores.setter + def scores(self, scores): + cv.check_type('tally scores', scores, MutableSequence) + + for i, score in enumerate(scores[:-1]): + # If the score is already in the Tally, raise an error + if score in scores[i+1:]: + msg = 'Unable to add a duplicate score "{0}" to Tally ID="{1}" ' \ + 'since duplicate scores are not supported in the OpenMC ' \ + 'Python API'.format(score, self.id) + raise ValueError(msg) + + # If score is a string, strip whitespace + if isinstance(score, basestring): + scores[i] = score.strip() + + self._scores = cv.CheckedList(_SCORE_CLASSES, 'tally scores', scores) + def add_filter(self, new_filter): """Add a filter to the tally + .. deprecated:: 0.8 + Use the Tally.filters property directly, i.e., + Tally.filters.append(...) + Parameters ---------- new_filter : Filter, CrossFilter or AggregateFilter @@ -496,23 +562,19 @@ class Tally(object): """ - if not isinstance(new_filter, (Filter, CrossFilter, AggregateFilter)): - msg = 'Unable to add Filter "{0}" to Tally ID="{1}" since it is ' \ - 'not a Filter object'.format(new_filter, self.id) - raise ValueError(msg) - - # If the filter is already in the Tally, raise an error - if new_filter in self.filters: - msg = 'Unable to add a duplicate filter "{0}" to Tally ID="{1}" ' \ - 'since duplicate filters are not supported in the OpenMC ' \ - 'Python API'.format(new_filter, self.id) - raise ValueError(msg) - - self._filters.append(new_filter) + warnings.warn('Tally.add_filter(...) has been deprecated and may be ' + 'removed in a future version. Tally filters should be ' + 'defined using the filters property directly.', + DeprecationWarning) + self.filters.append(new_filter) def add_nuclide(self, nuclide): """Specify that scores for a particular nuclide should be accumulated + .. deprecated:: 0.8 + Use the Tally.nuclides property directly, i.e., + Tally.nuclides.append(...) + Parameters ---------- nuclide : str, Nuclide, CrossNuclide or AggregateNuclide @@ -525,24 +587,19 @@ class Tally(object): """ - if not isinstance(nuclide, (basestring, Nuclide, - CrossNuclide, AggregateNuclide)): - msg = 'Unable to add nuclide "{0}" to Tally ID="{1}" since it is ' \ - 'not a Nuclide object'.format(nuclide) - raise ValueError(msg) - - # If the nuclide is already in the Tally, raise an error - if nuclide in self.nuclides: - msg = 'Unable to add a duplicate nuclide "{0}" to Tally ID="{1}" ' \ - 'since duplicate nuclides are not supported in the OpenMC ' \ - 'Python API'.format(nuclide, self.id) - raise ValueError(msg) - - self._nuclides.append(nuclide) + warnings.warn('Tally.add_nuclide(...) has been deprecated and may be ' + 'removed in a future version. Tally nuclides should be ' + 'defined using the nuclides property directly.', + DeprecationWarning) + self.nuclides.append(nuclide) def add_score(self, score): """Specify a quantity to be scored + .. deprecated:: 0.8 + Use the Tally.scores property directly, i.e., + Tally.scores.append(...) + Parameters ---------- score : str, CrossScore or AggregateScore @@ -554,24 +611,11 @@ class Tally(object): """ - if not isinstance(score, (basestring, CrossScore, AggregateScore)): - msg = 'Unable to add score "{0}" to Tally ID="{1}" since it is ' \ - 'not a string'.format(score, self.id) - raise ValueError(msg) - - # If the score is already in the Tally, raise an error - if score in self.scores: - msg = 'Unable to add a duplicate score "{0}" to Tally ID="{1}" ' \ - 'since duplicate scores are not supported in the OpenMC ' \ - 'Python API'.format(score, self.id) - raise ValueError(msg) - - # Normal score strings - if isinstance(score, basestring): - self._scores.append(score.strip()) - # CrossScores and AggrgateScore - else: - self._scores.append(score) + warnings.warn('Tally.add_score(...) has been deprecated and may be ' + 'removed in a future version. Tally scores should be ' + 'defined using the scores property directly.', + DeprecationWarning) + self.scores.append(score) @num_realizations.setter def num_realizations(self, num_realizations): @@ -666,7 +710,7 @@ class Tally(object): Parameters ---------- - old_filter : openmc.filter.Filter + old_filter : openmc.Filter Filter to remove """ @@ -683,7 +727,7 @@ class Tally(object): Parameters ---------- - nuclide : openmc.nuclide.Nuclide + nuclide : openmc.Nuclide Nuclide to remove """ @@ -695,84 +739,205 @@ class Tally(object): self._nuclides.remove(nuclide) - def can_merge(self, tally): - """Determine if another tally can be merged with this one + def _can_merge_filters(self, other): + """Determine if another tally's filters can be merged with this one's + + The types of filters between the two tallies must match identically. + The bins in all of the filters must match identically, or be mergeable + in only one filter. This is a helper method for the can_merge(...) + and merge(...) methods. Parameters ---------- - tally : Tally - Tally to check for merging + other : openmc.Tally + Tally to check for mergeable filters """ - if not isinstance(tally, Tally): + # Two tallys must have the same number of filters + if len(self.filters) != len(other.filters): return False - # Must have same estimator - if self.estimator != tally.estimator: - return False - - # Must have same nuclides - if len(self.nuclides) != len(tally.nuclides): - return False - - for nuclide in self.nuclides: - if nuclide not in tally.nuclides: - return False - - # Must have same or mergeable filters - if len(self.filters) != len(tally.filters): - return False - - # Check if only one tally contains a delayed group filter - tally1_dg = False - for filter1 in self.filters: - if filter1.type == 'delayedgroup': - tally1_dg = True - - tally2_dg = False - for filter2 in tally.filters: - if filter2.type == 'delayedgroup': - tally2_dg = True - # Return False if only one tally has a delayed group filter - if (tally1_dg or tally2_dg) and not (tally1_dg and tally2_dg): + tally1_dg = self.contains_filter('delayedgroup') + tally2_dg = other.contains_filter('delayedgroup') + if sum([tally1_dg, tally2_dg]) == 1: return False # Look to see if all filters are the same, or one or more can be merged for filter1 in self.filters: + merge_filters = False mergeable_filter = False - for filter2 in tally.filters: - if filter1 == filter2 or filter1.can_merge(filter2): + for filter2 in other.filters: + + # If filters match, they are mergeable + if filter1 == filter2: mergeable_filter = True break + # If filters are first mergeable filters encountered + elif filter1.can_merge(filter2) and not merge_filters: + merge_filters = True + mergeable_filter = True + break + + # If filters are the second mergeable filters encountered + elif filter1.can_merge(filter2) and merge_filters: + return False + # If no mergeable filter was found, the tallies are not mergeable if not mergeable_filter: return False - # Tallies are mergeable if all conditional checks passed + # Tally filters are mergeable if all conditional checks passed return True - def merge(self, tally): - """Merge another tally with this one + def _can_merge_nuclides(self, other): + """Determine if another tally's nuclides can be merged with this one's + + The nuclides between the two tallies must be mutually exclusive or + identically matching. This is a helper method for the can_merge(...) + and merge(...) methods. Parameters ---------- - tally : Tally + other : openmc.Tally + Tally to check for mergeable nuclides + + """ + + no_nuclides_match = True + all_nuclides_match = True + + # Search for each of this tally's nuclides in the other tally + for nuclide in self.nuclides: + if nuclide not in other.nuclides: + all_nuclides_match = False + else: + no_nuclides_match = False + + # Search for each of the other tally's nuclides in this tally + for nuclide in other.nuclides: + if nuclide not in self.nuclides: + all_nuclides_match = False + else: + no_nuclides_match = False + + # Either all nuclides should match, or none should + if no_nuclides_match or all_nuclides_match: + return True + else: + return False + + def _can_merge_scores(self, other): + """Determine if another tally's scores can be merged with this one's + + The scores between the two tallies must be mutually exclusive or + identically matching. This is a helper method for the can_merge(...) + and merge(...) methods. + + Parameters + ---------- + other : openmc.Tally + Tally to check for mergeable scores + + """ + + no_scores_match = True + all_scores_match = True + + # Search for each of this tally's scores in the other tally + for score in self.scores: + if score not in other.scores: + all_scores_match = False + else: + no_scores_match = False + + # Search for each of the other tally's scores in this tally + for score in other.scores: + if score not in self.scores: + all_scores_match = False + else: + no_scores_match = False + + # Nuclides cannot be specified on 'flux' scores + if 'flux' in self.scores or 'flux' in other.scores: + if self.nuclides != other.nuclides: + return False + + # Either all scores should match, or none should + if no_scores_match or all_scores_match: + return True + else: + return False + + def can_merge(self, other): + """Determine if another tally can be merged with this one + + If results have been loaded from a statepoint, then tallies are only + mergeable along one and only one of filter bins, nuclides or scores. + + Parameters + ---------- + other : openmc.Tally + Tally to check for merging + + """ + + if not isinstance(other, Tally): + return False + + # Must have same estimator + if self.estimator != other.estimator: + return False + + equal_filters = sorted(self.filters) == sorted(other.filters) + equal_nuclides = sorted(self.nuclides) == sorted(other.nuclides) + equal_scores = sorted(self.scores) == sorted(other.scores) + equality = [equal_filters, equal_nuclides, equal_scores] + + # If all filters, nuclides and scores match then tallies are mergeable + if equal_filters and equal_nuclides and equal_scores: + return True + + # Variables to indicate matching filter bins, nuclides and scores + merge_filters = self._can_merge_filters(other) + merge_nuclides = self._can_merge_nuclides(other) + merge_scores = self._can_merge_scores(other) + mergeability = [merge_filters, merge_nuclides, merge_scores] + + if not all(mergeability): + return False + + # If the tally results have been read from the statepoint, we can only + # at least two of filters, nuclides and scores must match + elif self._results_read and sum(equality) < 2: + return False + else: + return True + + def merge(self, other): + """Merge another tally with this one + + If results have been loaded from a statepoint, then tallies are only + mergeable along one and only one of filter bins, nuclides or scores. + + Parameters + ---------- + other : openmc.Tally Tally to merge with this one Returns ------- - merged_tally : Tally + merged_tally : openmc.Tally Merged tallies """ - if not self.can_merge(tally): - msg = 'Unable to merge tally ID="{0}" with ' + \ - '"{1}"'.format(tally.id, self.id) + if not self.can_merge(other): + msg = 'Unable to merge tally ID="{0}" with ' \ + '"{1}"'.format(other.id, self.id) raise ValueError(msg) # Create deep copy of tally to return as merged tally @@ -781,22 +946,126 @@ class Tally(object): # Differentiate Tally with a new auto-generated Tally ID merged_tally.id = None - # Merge filters - for i, filter1 in enumerate(merged_tally.filters): - for filter2 in tally.filters: - if filter1 != filter2 and filter1.can_merge(filter2): - merged_filter = filter1.merge(filter2) - merged_tally.filters[i] = merged_filter - break + # If the two tallies are equal, simply return copy + if self == other: + return merged_tally - # Add unique scores from second tally to merged tally - for score in tally.scores: - if score not in merged_tally.scores: - merged_tally.add_score(score) + # Create deep copy of other tally to use for array concatenation + other_copy = copy.deepcopy(other) - # Add triggers from second tally to merged tally - for trigger in tally.triggers: - merged_tally.add_trigger(trigger) + # Identify if filters, nuclides and scores are mergeable and/or equal + merge_filters = self._can_merge_filters(other) + merge_nuclides = self._can_merge_nuclides(other) + merge_scores = self._can_merge_scores(other) + equal_filters = sorted(self.filters) == sorted(other.filters) + equal_nuclides = sorted(self.nuclides) == sorted(other.nuclides) + equal_scores = sorted(self.scores) == sorted(other.scores) + + # If two tallies can be merged along a filter's bins + if merge_filters and not equal_filters: + + # Search for mergeable filters + for i, filter1 in enumerate(self.filters): + for j, filter2 in enumerate(other.filters): + if filter1 != filter2 and filter1.can_merge(filter2): + other_copy._swap_filters(other_copy.filters[i], filter2) + merged_tally.filters[i] = filter1.merge(filter2) + join_right = filter1 < filter2 + merge_axis = i + break + + # If two tallies can be merged along nuclide bins + if merge_nuclides and not equal_nuclides: + merge_axis = self.num_filters + join_right = True + + # Add unique nuclides from other tally to merged tally + for nuclide in other.nuclides: + if nuclide not in merged_tally.nuclides: + merged_tally.nuclides.append(nuclide) + + # If two tallies can be merged along score bins + if merge_scores and not equal_scores: + merge_axis = self.num_filters + 1 + join_right = True + + # Add unique scores from other tally to merged tally + for score in other.scores: + if score not in merged_tally.scores: + merged_tally.scores.append(score) + + # Add triggers from other tally to merged tally + for trigger in other.triggers: + merged_tally.triggers.append(trigger) + + # If results have not been read, then return tally for input generation + if self._results_read is None: + return merged_tally + # Otherwise, this is a derived tally which needs merged results arrays + else: + self._derived = True + + # Update filter strides in merged tally + merged_tally._update_filter_strides() + + # Concatenate sum arrays if present in both tallies + if self.sum is not None and other_copy.sum is not None: + self_sum = self.get_reshaped_data(value='sum') + other_sum = other_copy.get_reshaped_data(value='sum') + + if join_right: + merged_sum = \ + np.concatenate((self_sum, other_sum), axis=merge_axis) + else: + merged_sum = \ + np.concatenate((other_sum, self_sum), axis=merge_axis) + + merged_tally._sum = np.reshape(merged_sum, merged_tally.shape) + + # Concatenate sum_sq arrays if present in both tallies + if self.sum_sq is not None and other.sum_sq is not None: + self_sum_sq = self.get_reshaped_data(value='sum_sq') + other_sum_sq = other_copy.get_reshaped_data(value='sum_sq') + + if join_right: + merged_sum_sq = \ + np.concatenate((self_sum_sq, other_sum_sq), axis=merge_axis) + else: + merged_sum_sq = \ + np.concatenate((other_sum_sq, self_sum_sq), axis=merge_axis) + + merged_tally._sum_sq = np.reshape(merged_sum_sq, merged_tally.shape) + + # Concatenate mean arrays if present in both tallies + if self.mean is not None and other.mean is not None: + self_mean = self.get_reshaped_data(value='mean') + other_mean = other_copy.get_reshaped_data(value='mean') + + if join_right: + merged_mean = \ + np.concatenate((self_mean, other_mean), axis=merge_axis) + else: + merged_mean = \ + np.concatenate((other_mean, self_mean), axis=merge_axis) + + merged_tally._mean = np.reshape(merged_mean, merged_tally.shape) + + # Concatenate std. dev. arrays if present in both tallies + if self.std_dev is not None and other.std_dev is not None: + self_std_dev = self.get_reshaped_data(value='std_dev') + other_std_dev = other_copy.get_reshaped_data(value='std_dev') + + if join_right: + merged_std_dev = \ + np.concatenate((self_std_dev, other_std_dev), axis=merge_axis) + else: + merged_std_dev = \ + np.concatenate((other_std_dev, self_std_dev), axis=merge_axis) + + merged_tally._std_dev = np.reshape(merged_std_dev, merged_tally.shape) + + # Sparsify merged tally if both tallies are sparse + merged_tally.sparse = self.sparse and other.sparse return merged_tally @@ -873,6 +1142,32 @@ class Tally(object): return element + def contains_filter(self, filter_type): + """Looks for a filter in the tally that matches a specified type + + Parameters + ---------- + filter_type : str + Type of the filter, e.g. 'mesh' + + Returns + ------- + filter_found : bool + True if the tally contains a filter of the requested type; + otherwise false + + """ + + filter_found = False + + # Look through all of this Tally's Filters for the type requested + for test_filter in self.filters: + if test_filter.type == filter_type: + filter_found = True + break + + return filter_found + def find_filter(self, filter_type): """Return a filter in the tally that matches a specified type @@ -883,7 +1178,7 @@ class Tally(object): Returns ------- - filter_found : openmc.filter.Filter + filter_found : openmc.Filter Filter from this tally with matching type, or None if no matching Filter is found @@ -917,7 +1212,7 @@ class Tally(object): ---------- filter_type : str The type of Filter (e.g., 'cell', 'energy', etc.) - filter_bin : Integral or tuple + filter_bin : int or tuple The bin is an integer ID for 'material', 'surface', 'cell', 'cellborn', and 'universe' Filters. The bin is an integer for the cell instance ID for 'distribcell' Filters. The bin is a 2-tuple of @@ -1043,7 +1338,7 @@ class Tally(object): Returns ------- - ndarray + numpy.ndarray A NumPy array of the filter indices """ @@ -1125,7 +1420,7 @@ class Tally(object): Returns ------- - ndarray + numpy.ndarray A NumPy array of the nuclide indices """ @@ -1159,7 +1454,7 @@ class Tally(object): Returns ------- - ndarray + numpy.ndarray A NumPy array of the score indices """ @@ -1221,7 +1516,7 @@ class Tally(object): Returns ------- - float or ndarray + float or numpy.ndarray A scalar or NumPy array of the Tally data indexed in the order each filter, nuclide and score is listed in the parameters. @@ -1271,7 +1566,8 @@ class Tally(object): return data def get_pandas_dataframe(self, filters=True, nuclides=True, - scores=True, derivative=True, summary=None): + scores=True, derivative=True, summary=None, + float_format='{:.2e}'): """Build a Pandas DataFrame for the Tally data. This method constructs a Pandas DataFrame object for the Tally data @@ -1291,12 +1587,15 @@ class Tally(object): Include columns with score bin information (default is True). derivative : bool Include columns with differential tally info (default is True). - summary : None or Summary + summary : None or openmc.Summary An optional Summary object to be used to construct columns for distribcell tally filters (default is None). The geometric information in the Summary object is embedded into a Multi-index column with a geometric "path" to each distribcell intance. NOTE: This option requires the OpenCG Python package. + float_format : str + All floats in the DataFrame will be formatted using the given + format string before printing. Returns ------- @@ -1327,14 +1626,8 @@ class Tally(object): 'Summary info'.format(self.id) raise KeyError(msg) - # Attempt to import Pandas - try: - import pandas as pd - except ImportError: - msg = 'The Pandas Python package must be installed on your system' - raise ImportError(msg) - # Initialize a pandas dataframe for the tally data + import pandas as pd df = pd.DataFrame() # Find the total length of the tally data array @@ -1351,23 +1644,36 @@ class Tally(object): # Include DataFrame column for nuclides if user requested it if nuclides: nuclides = [] + column_name = 'nuclide' for nuclide in self.nuclides: - # Write Nuclide name if Summary info was linked with StatePoint if isinstance(nuclide, Nuclide): nuclides.append(nuclide.name) + elif isinstance(nuclide, AggregateNuclide): + nuclides.append(nuclide.name) + column_name = '{0}(nuclide)'.format(nuclide.aggregate_op) else: nuclides.append(nuclide) # Tile the nuclide bins into a DataFrame column nuclides = np.repeat(nuclides, len(self.scores)) tile_factor = data_size / len(nuclides) - df['nuclide'] = np.tile(nuclides, int(tile_factor)) + df[column_name] = np.tile(nuclides, int(tile_factor)) # Include column for scores if user requested it if scores: + scores = [] + column_name = 'score' + + for score in self.scores: + if isinstance(score, (basestring, CrossScore)): + scores.append(score) + elif isinstance(score, AggregateScore): + scores.append(score.name) + column_name = '{0}(score)'.format(score.aggregate_op) + tile_factor = data_size / len(self.scores) - df['score'] = np.tile(self.scores, int(tile_factor)) + df[column_name] = np.tile(scores, int(tile_factor)) # Include columns for derivatives if user requested it if derivative and (self.derivative is not None): @@ -1404,6 +1710,10 @@ class Tally(object): # Create and set a MultiIndex for the DataFrame's columns df.columns = pd.MultiIndex.from_tuples(columns) + # Modify the df.to_string method so that it prints formatted strings. + # Credit to http://stackoverflow.com/users/3657742/chrisb for this trick + df.to_string = partial(df.to_string, float_format=float_format.format) + return df def get_reshaped_data(self, value='mean'): @@ -1411,8 +1721,8 @@ class Tally(object): The tally data in OpenMC is stored as a 3D array with the dimensions corresponding to filters, nuclides and scores. As a result, tally data - can be opaque for a user to directly index (i.e., without use of the - Tally.get_values(...) method) since one must know how to properly use + can be opaque for a user to directly index (i.e., without use of + :meth:`openmc.Tally.get_values`) since one must know how to properly use the number of bins and strides for each filter to index into the first (filter) dimension. @@ -1432,7 +1742,7 @@ class Tally(object): Returns ------- - ndarray + numpy.ndarray The tally data array indexed by filters, nuclides and scores. """ @@ -1610,7 +1920,7 @@ class Tally(object): Parameters ---------- - other : Tally + other : openmc.Tally The tally on the right hand side of the hybrid product binary_op : {'+', '-', '*', '/', '^'} The binary operation in the hybrid product @@ -1632,7 +1942,7 @@ class Tally(object): Returns ------- - Tally + openmc.Tally A new Tally that is the hybrid product with this one. Raises @@ -1752,33 +2062,33 @@ class Tally(object): # Add filters to the new tally if filter_product == 'entrywise': for self_filter in self_copy.filters: - new_tally.add_filter(self_filter) + new_tally.filters.append(self_filter) else: all_filters = [self_copy.filters, other_copy.filters] for self_filter, other_filter in itertools.product(*all_filters): new_filter = CrossFilter(self_filter, other_filter, binary_op) - new_tally.add_filter(new_filter) + new_tally.filters.append(new_filter) # Add nuclides to the new tally if nuclide_product == 'entrywise': for self_nuclide in self_copy.nuclides: - new_tally.add_nuclide(self_nuclide) + new_tally.nuclides.append(self_nuclide) else: all_nuclides = [self_copy.nuclides, other_copy.nuclides] for self_nuclide, other_nuclide in itertools.product(*all_nuclides): new_nuclide = \ CrossNuclide(self_nuclide, other_nuclide, binary_op) - new_tally.add_nuclide(new_nuclide) + new_tally.nuclides.append(new_nuclide) # Add scores to the new tally if score_product == 'entrywise': for self_score in self_copy.scores: - new_tally.add_score(self_score) + new_tally.scores.append(self_score) else: all_scores = [self_copy.scores, other_copy.scores] for self_score, other_score in itertools.product(*all_scores): new_score = CrossScore(self_score, other_score, binary_op) - new_tally.add_score(new_score) + new_tally.scores.append(new_score) # Update the new tally's filter strides new_tally._update_filter_strides() @@ -1810,7 +2120,7 @@ class Tally(object): Parameters ---------- - other : Tally + other : openmc.Tally The tally to outer product with this tally filter_product : {'entrywise'} The type of product to be performed between filter data. Currently, @@ -1841,14 +2151,14 @@ class Tally(object): filter_copy = copy.deepcopy(other_filter) other._mean = np.repeat(other.mean, filter_copy.num_bins, axis=0) other._std_dev = np.repeat(other.std_dev, filter_copy.num_bins, axis=0) - other.add_filter(filter_copy) + other.filters.append(filter_copy) # Add filters present in other but not in self to self for self_filter in self_missing_filters: filter_copy = copy.deepcopy(self_filter) self._mean = np.repeat(self.mean, filter_copy.num_bins, axis=0) self._std_dev = np.repeat(self.std_dev, filter_copy.num_bins, axis=0) - self.add_filter(filter_copy) + self.filters.append(filter_copy) # Align other filters with self filters for i, self_filter in enumerate(self.filters): @@ -1871,7 +2181,7 @@ class Tally(object): np.tile(other.std_dev, (1, self.num_nuclides, 1)) # Add nuclides to each tally such that each tally contains the complete - # set of nuclides necessary to perform an entrywise product. New + # set of nuclides necessary to perform an entrywise product. New # nuclides added to a tally will have all their scores set to zero. else: @@ -1887,7 +2197,7 @@ class Tally(object): np.insert(other.mean, other.num_nuclides, 0, axis=1) other._std_dev = \ np.insert(other.std_dev, other.num_nuclides, 0, axis=1) - other.add_nuclide(nuclide) + other.nuclides.append(nuclide) # Add nuclides present in other but not in self to self for nuclide in self_missing_nuclides: @@ -1895,7 +2205,7 @@ class Tally(object): np.insert(self.mean, self.num_nuclides, 0, axis=1) self._std_dev = \ np.insert(self.std_dev, self.num_nuclides, 0, axis=1) - self.add_nuclide(nuclide) + self.nuclides.append(nuclide) # Align other nuclides with self nuclides for i, nuclide in enumerate(self.nuclides): @@ -1928,13 +2238,13 @@ class Tally(object): for score in other_missing_scores: other._mean = np.insert(other.mean, other.num_scores, 0, axis=2) other._std_dev = np.insert(other.std_dev, other.num_scores, 0, axis=2) - other.add_score(score) + other.scores.append(score) # Add scores present in other but not in self to self for score in self_missing_scores: self._mean = np.insert(self.mean, self.num_scores, 0, axis=2) self._std_dev = np.insert(self.std_dev, self.num_scores, 0, axis=2) - self.add_score(score) + self.scores.append(score) # Align other scores with self scores for i, score in enumerate(self.scores): @@ -1980,19 +2290,12 @@ class Tally(object): """ - # Check that results have been read - if not self.derived and self.sum is None: - msg = 'Unable to use tally arithmetic with Tally ID="{0}" ' \ - 'since it does not contain any results.'.format(self.id) - raise ValueError(msg) - - cv.check_type('filter1', filter1, Filter) - cv.check_type('filter2', filter2, Filter) + cv.check_type('filter1', filter1, (Filter, CrossFilter, AggregateFilter)) + cv.check_type('filter2', filter2, (Filter, CrossFilter, AggregateFilter)) # Check that the filters exist in the tally and are not the same if filter1 == filter2: - msg = 'Unable to swap a filter with itself' - raise ValueError(msg) + return elif filter1 not in self.filters: msg = 'Unable to swap "{0}" filter1 in Tally ID="{1}" since it ' \ 'does not contain such a filter'.format(filter1.type, self.id) @@ -2199,12 +2502,12 @@ class Tally(object): Parameters ---------- - other : Tally or Real + other : openmc.Tally or float The tally or scalar value to add to this tally Returns ------- - Tally + openmc.Tally A new derived tally which is the sum of this tally and the other tally or scalar value in the addition. @@ -2239,12 +2542,9 @@ class Tally(object): new_tally.with_summary = self.with_summary new_tally.num_realization = self.num_realizations - for self_filter in self.filters: - new_tally.add_filter(self_filter) - for nuclide in self.nuclides: - new_tally.add_nuclide(nuclide) - for score in self.scores: - new_tally.add_score(score) + new_tally.filters = copy.deepcopy(self.filters) + new_tally.nuclides = copy.deepcopy(self.nuclides) + new_tally.scores = copy.deepcopy(self.scores) # If this tally operand is sparse, sparsify the new tally new_tally.sparse = self.sparse @@ -2274,12 +2574,12 @@ class Tally(object): Parameters ---------- - other : Tally or Real + other : openmc.Tally or float The tally or scalar value to subtract from this tally Returns ------- - Tally + openmc.Tally A new derived tally which is the difference of this tally and the other tally or scalar value in the subtraction. @@ -2313,12 +2613,9 @@ class Tally(object): new_tally.with_summary = self.with_summary new_tally.num_realization = self.num_realizations - for self_filter in self.filters: - new_tally.add_filter(self_filter) - for nuclide in self.nuclides: - new_tally.add_nuclide(nuclide) - for score in self.scores: - new_tally.add_score(score) + new_tally.filters = copy.deepcopy(self.filters) + new_tally.nuclides = copy.deepcopy(self.nuclides) + new_tally.scores = copy.deepcopy(self.scores) # If this tally operand is sparse, sparsify the new tally new_tally.sparse = self.sparse @@ -2349,12 +2646,12 @@ class Tally(object): Parameters ---------- - other : Tally or Real + other : openmc.Tally or float The tally or scalar value to multiply with this tally Returns ------- - Tally + openmc.Tally A new derived tally which is the product of this tally and the other tally or scalar value in the multiplication. @@ -2388,12 +2685,9 @@ class Tally(object): new_tally.with_summary = self.with_summary new_tally.num_realization = self.num_realizations - for self_filter in self.filters: - new_tally.add_filter(self_filter) - for nuclide in self.nuclides: - new_tally.add_nuclide(nuclide) - for score in self.scores: - new_tally.add_score(score) + new_tally.filters = copy.deepcopy(self.filters) + new_tally.nuclides = copy.deepcopy(self.nuclides) + new_tally.scores = copy.deepcopy(self.scores) # If this tally operand is sparse, sparsify the new tally new_tally.sparse = self.sparse @@ -2424,12 +2718,12 @@ class Tally(object): Parameters ---------- - other : Tally or Real + other : openmc.Tally or float The tally or scalar value to divide this tally by Returns ------- - Tally + openmc.Tally A new derived tally which is the dividend of this tally and the other tally or scalar value in the division. @@ -2463,12 +2757,9 @@ class Tally(object): new_tally.with_summary = self.with_summary new_tally.num_realization = self.num_realizations - for self_filter in self.filters: - new_tally.add_filter(self_filter) - for nuclide in self.nuclides: - new_tally.add_nuclide(nuclide) - for score in self.scores: - new_tally.add_score(score) + new_tally.filters = copy.deepcopy(self.filters) + new_tally.nuclides = copy.deepcopy(self.nuclides) + new_tally.scores = copy.deepcopy(self.scores) # If this tally operand is sparse, sparsify the new tally new_tally.sparse = self.sparse @@ -2502,12 +2793,12 @@ class Tally(object): Parameters ---------- - power : Tally or Real + power : openmc.Tally or float The tally or scalar value exponent Returns ------- - Tally + openmc.Tally A new derived tally which is this tally raised to the power of the other tally or scalar value in the exponentiation. @@ -2542,12 +2833,9 @@ class Tally(object): new_tally.with_summary = self.with_summary new_tally.num_realization = self.num_realizations - for self_filter in self.filters: - new_tally.add_filter(self_filter) - for nuclide in self.nuclides: - new_tally.add_nuclide(nuclide) - for score in self.scores: - new_tally.add_score(score) + new_tally.filters = copy.deepcopy(self.filters) + new_tally.nuclides = copy.deepcopy(self.nuclides) + new_tally.scores = copy.deepcopy(self.scores) # If original tally was sparse, sparsify the exponentiated tally new_tally.sparse = self.sparse @@ -2566,12 +2854,12 @@ class Tally(object): Parameters ---------- - other : Integer or Real + other : float The scalar value to add to this tally Returns ------- - Tally + openmc.Tally A new derived tally of this tally added with the scalar value. """ @@ -2585,12 +2873,12 @@ class Tally(object): Parameters ---------- - other : Integer or Real + other : float The scalar value to subtract this tally from Returns ------- - Tally + openmc.Tally A new derived tally of this tally subtracted from the scalar value. """ @@ -2604,12 +2892,12 @@ class Tally(object): Parameters ---------- - other : Integer or Real + other : float The scalar value to multiply with this tally Returns ------- - Tally + openmc.Tally A new derived tally of this tally multiplied by the scalar value. """ @@ -2623,12 +2911,12 @@ class Tally(object): Parameters ---------- - other : Integer or Real + other : float The scalar value to divide by this tally Returns ------- - Tally + openmc.Tally A new derived tally of the scalar value divided by this tally. """ @@ -2640,7 +2928,7 @@ class Tally(object): Returns ------- - Tally + openmc.Tally A new derived tally which is the absolute value of this tally. """ @@ -2654,7 +2942,7 @@ class Tally(object): Returns ------- - Tally + openmc.Tally A new derived tally which is the negated value of this tally. """ @@ -2696,7 +2984,7 @@ class Tally(object): Returns ------- - Tally + openmc.Tally A new tally which encapsulates the subset of data requested in the order each filter, nuclide and score is listed in the parameters. @@ -2713,7 +3001,13 @@ class Tally(object): 'since it does not contain any results.'.format(self.id) raise ValueError(msg) + # Create deep copy of tally to return as sliced tally new_tally = copy.deepcopy(self) + new_tally._derived = True + + # Differentiate Tally with a new auto-generated Tally ID + new_tally.id = None + new_tally.sparse = False if not self.derived and self.sum is not None: @@ -2798,7 +3092,7 @@ class Tally(object): def summation(self, scores=[], filter_type=None, filter_bins=[], nuclides=[], remove_filter=False): """Vectorized sum of tally data across scores, filter bins and/or - nuclides using tally addition. + nuclides using tally aggregation. This method constructs a new tally to encapsulate the sum of the data represented by the summation of the data in this tally. The tally data @@ -2813,7 +3107,7 @@ class Tally(object): filter_type : str A filter type string (e.g., 'cell', 'energy') corresponding to the filter bins to sum across - filter_bins : Iterable of Integral or tuple + filter_bins : Iterable of int or tuple A list of the filter bins corresponding to the filter_type parameter Each bin in the list is the integer ID for 'material', 'surface', 'cell', 'cellborn', and 'universe' Filters. Each bin is an integer @@ -2831,7 +3125,7 @@ class Tally(object): Returns ------- - Tally + openmc.Tally A new tally which encapsulates the sum of data requested. """ @@ -2840,7 +3134,7 @@ class Tally(object): tally_sum._derived = True tally_sum._estimator = self.estimator tally_sum._num_realizations = self.num_realizations - tally_sum.with_batch_statistics = self.with_batch_statistics + tally_sum._with_batch_statistics = self.with_batch_statistics tally_sum._with_summary = self.with_summary tally_sum._sp_filename = self._sp_filename tally_sum._results_read = self._results_read @@ -2881,12 +3175,12 @@ class Tally(object): # Add AggregateFilter to the tally sum if not remove_filter: filter_sum = \ - AggregateFilter(self_filter, filter_bins, 'sum') - tally_sum.add_filter(filter_sum) + AggregateFilter(self_filter, [tuple(filter_bins)], 'sum') + tally_sum.filters.append(filter_sum) # Add a copy of each filter not summed across to the tally sum else: - tally_sum.add_filter(copy.deepcopy(self_filter)) + tally_sum.filters.append(copy.deepcopy(self_filter)) # Add a copy of this tally's filters to the tally sum else: @@ -2904,7 +3198,7 @@ class Tally(object): # Add AggregateNuclide to the tally sum nuclide_sum = AggregateNuclide(nuclides, 'sum') - tally_sum.add_nuclide(nuclide_sum) + tally_sum.nuclides.append(nuclide_sum) # Add a copy of this tally's nuclides to the tally sum else: @@ -2922,7 +3216,7 @@ class Tally(object): # Add AggregateScore to the tally sum score_sum = AggregateScore(scores, 'sum') - tally_sum.add_score(score_sum) + tally_sum.scores.append(score_sum) # Add a copy of this tally's scores to the tally sum else: @@ -2943,6 +3237,157 @@ class Tally(object): tally_sum.sparse = self.sparse return tally_sum + def average(self, scores=[], filter_type=None, + filter_bins=[], nuclides=[], remove_filter=False): + """Vectorized average of tally data across scores, filter bins and/or + nuclides using tally aggregation. + + This method constructs a new tally to encapsulate the average of the + data represented by the average of the data in this tally. The tally + data average is determined by the scores, filter bins and nuclides + specified in the input parameters. + + Parameters + ---------- + scores : list of str + A list of one or more score strings to average across + (e.g., ['absorption', 'nu-fission']; default is []) + filter_type : str + A filter type string (e.g., 'cell', 'energy') corresponding to the + filter bins to average across + filter_bins : Iterable of int or tuple + A list of the filter bins corresponding to the filter_type parameter + Each bin in the list is the integer ID for 'material', 'surface', + 'cell', 'cellborn', and 'universe' Filters. Each bin is an integer + for the cell instance ID for 'distribcell' Filters. Each bin is a + 2-tuple of floats for 'energy' and 'energyout' filters corresponding + to the energy boundaries of the bin of interest. Each bin is an + (x,y,z) 3-tuple for 'mesh' filters corresponding to the mesh cell of + interest. + nuclides : list of str + A list of nuclide name strings to average across + (e.g., ['U-235', 'U-238']; default is []) + remove_filter : bool + If a filter is being averaged over, this bool indicates whether to + remove that filter in the returned tally. Default is False. + + Returns + ------- + openmc.Tally + A new tally which encapsulates the average of data requested. + """ + + # Create new derived Tally for average + tally_avg = Tally() + tally_avg._derived = True + tally_avg._estimator = self.estimator + tally_avg._num_realizations = self.num_realizations + tally_avg._with_batch_statistics = self.with_batch_statistics + tally_avg._with_summary = self.with_summary + tally_avg._sp_filename = self._sp_filename + tally_avg._results_read = self._results_read + + # Get tally data arrays reshaped with one dimension per filter + mean = self.get_reshaped_data(value='mean') + std_dev = self.get_reshaped_data(value='std_dev') + + # Average across any filter bins specified by the user + if filter_type in _FILTER_TYPES: + find_filter = self.find_filter(filter_type) + + # If user did not specify filter bins, average across all bins + if len(filter_bins) == 0: + bin_indices = np.arange(find_filter.num_bins) + + if filter_type == 'distribcell': + filter_bins = np.arange(find_filter.num_bins) + else: + num_bins = find_filter.num_bins + filter_bins = \ + [(find_filter.get_bin(i)) for i in range(num_bins)] + + # Only average across bins specified by the user + else: + bin_indices = \ + [find_filter.get_bin_index(bin) for bin in filter_bins] + + # Average across the bins in the user-specified filter + for i, self_filter in enumerate(self.filters): + if self_filter.type == filter_type: + mean = np.take(mean, indices=bin_indices, axis=i) + std_dev = np.take(std_dev, indices=bin_indices, axis=i) + mean = np.mean(mean, axis=i, keepdims=True) + std_dev = np.mean(std_dev**2, axis=i, keepdims=True) + std_dev /= len(bin_indices) + std_dev = np.sqrt(std_dev) + + # Add AggregateFilter to the tally avg + if not remove_filter: + filter_sum = \ + AggregateFilter(self_filter, [tuple(filter_bins)], 'avg') + tally_avg.filters.append(filter_sum) + + # Add a copy of each filter not averaged across to the tally avg + else: + tally_avg.filters.append(copy.deepcopy(self_filter)) + + # Add a copy of this tally's filters to the tally avg + else: + tally_avg._filters = copy.deepcopy(self.filters) + + # Sum across any nuclides specified by the user + if len(nuclides) != 0: + nuclide_bins = [self.get_nuclide_index(nuclide) for nuclide in nuclides] + axis_index = self.num_filters + mean = np.take(mean, indices=nuclide_bins, axis=axis_index) + std_dev = np.take(std_dev, indices=nuclide_bins, axis=axis_index) + mean = np.mean(mean, axis=axis_index, keepdims=True) + std_dev = np.mean(std_dev**2, axis=axis_index, keepdims=True) + std_dev /= len(nuclide_bins) + std_dev = np.sqrt(std_dev) + + # Add AggregateNuclide to the tally avg + nuclide_avg = AggregateNuclide(nuclides, 'avg') + tally_avg.nuclides.append(nuclide_avg) + + # Add a copy of this tally's nuclides to the tally avg + else: + tally_avg._nuclides = copy.deepcopy(self.nuclides) + + # Sum across any scores specified by the user + if len(scores) != 0: + score_bins = [self.get_score_index(score) for score in scores] + axis_index = self.num_filters + 1 + mean = np.take(mean, indices=score_bins, axis=axis_index) + std_dev = np.take(std_dev, indices=score_bins, axis=axis_index) + mean = np.sum(mean, axis=axis_index, keepdims=True) + std_dev = np.sum(std_dev**2, axis=axis_index, keepdims=True) + std_dev /= len(score_bins) + std_dev = np.sqrt(std_dev) + + # Add AggregateScore to the tally avg + score_sum = AggregateScore(scores, 'avg') + tally_avg.scores.append(score_sum) + + # Add a copy of this tally's scores to the tally avg + else: + tally_avg._scores = copy.deepcopy(self.scores) + + # Update the tally avg's filter strides + tally_avg._update_filter_strides() + + # Reshape condensed data arrays with one dimension for all filters + mean = np.reshape(mean, tally_avg.shape) + std_dev = np.reshape(std_dev, tally_avg.shape) + + # Assign tally avg's data with the new arrays + tally_avg._mean = mean + tally_avg._std_dev = std_dev + + # If original tally was sparse, sparsify the tally average + tally_avg.sparse = self.sparse + return tally_avg + def diagonalize_filter(self, new_filter): """Diagonalize the tally data array along a new axis of filter bins. @@ -2961,7 +3406,7 @@ class Tally(object): Returns ------- - Tally + openmc.Tally A new derived Tally with data diagaonalized along the new filter. """ @@ -2975,7 +3420,7 @@ class Tally(object): # Add the new filter to a copy of this Tally new_tally = copy.deepcopy(self) - new_tally.add_filter(new_filter) + new_tally.filters.append(new_filter) # Determine "base" indices along the new "diagonal", and the factor # by which the "base" indices should be repeated to account for all @@ -3037,9 +3482,8 @@ class TalliesFile(object): Parameters ---------- - tally : Tally + tally : openmc.Tally Tally to add to file - merge : bool Indicate whether the tally should be merged with an existing tally, if possible. Defaults to False. @@ -3076,7 +3520,7 @@ class TalliesFile(object): Parameters ---------- - tally : Tally + tally : openmc.Tally Tally to remove """ @@ -3112,7 +3556,7 @@ class TalliesFile(object): Parameters ---------- - mesh : openmc.mesh.Mesh + mesh : openmc.Mesh Mesh to add to the file """ @@ -3128,7 +3572,7 @@ class TalliesFile(object): Parameters ---------- - mesh : openmc.mesh.Mesh + mesh : openmc.Mesh Mesh to remove from the file """ diff --git a/openmc/trigger.py b/openmc/trigger.py index bcac8c31c..b8383bd27 100644 --- a/openmc/trigger.py +++ b/openmc/trigger.py @@ -1,8 +1,10 @@ from numbers import Real from xml.etree import ElementTree as ET import sys +import warnings +from collections import Iterable -from openmc.checkvalue import check_type, check_value +import openmc.checkvalue as cv if sys.version_info[0] >= 3: basestring = str @@ -46,9 +48,7 @@ class Trigger(object): clone._trigger_type = self._trigger_type clone._threshold = self._threshold - clone._scores = [] - for score in self._scores: - clone.add_score(score) + clone.scores = self.scores memo[id(self)] = clone @@ -88,15 +88,26 @@ class Trigger(object): @trigger_type.setter def trigger_type(self, trigger_type): - check_value('tally trigger type', trigger_type, + cv.check_value('tally trigger type', trigger_type, ['variance', 'std_dev', 'rel_err']) self._trigger_type = trigger_type @threshold.setter def threshold(self, threshold): - check_type('tally trigger threshold', threshold, Real) + cv.check_type('tally trigger threshold', threshold, Real) self._threshold = threshold + @scores.setter + def scores(self, scores): + cv.check_type('trigger scores', scores, Iterable, basestring) + + # Set scores making sure not to have duplicates + self._scores = [] + for score in scores: + if score not in self._scores: + self._scores.append(score) + + def add_score(self, score): """Add a score to the list of scores to be checked against the trigger. @@ -107,16 +118,11 @@ class Trigger(object): """ - if not isinstance(score, basestring): - msg = 'Unable to add score "{0}" to tally trigger since ' \ - 'it is not a string'.format(score) - raise ValueError(msg) - - # If the score is already in the Tally, don't add it again - if score in self._scores: - return - else: - self._scores.append(score) + warnings.warn('Trigger.add_score(...) has been deprecated and may be ' + 'removed in a future version. Tally trigger scores should ' + 'be defined using the scores property directly.', + DeprecationWarning) + self.scores.append(score) def get_trigger_xml(self, element): """Return XML representation of the trigger diff --git a/openmc/universe.py b/openmc/universe.py index edc4619dd..eb6d13233 100644 --- a/openmc/universe.py +++ b/openmc/universe.py @@ -1,6 +1,5 @@ -import abc from collections import OrderedDict, Iterable -from numbers import Real, Integral +from numbers import Integral from xml.etree import ElementTree as ET import sys import warnings @@ -9,484 +8,15 @@ import numpy as np import openmc import openmc.checkvalue as cv -from openmc.surface import Halfspace -from openmc.region import Region, Intersection, Complement if sys.version_info[0] >= 3: basestring = str -# DeprecationWarning filter for the Cell.add_surface(...) method -warnings.simplefilter('always', DeprecationWarning) - -# A static variable for auto-generated Cell IDs -AUTO_CELL_ID = 10000 - # A dictionary for storing IDs of cell elements that have already been written, # used to optimize the writing process WRITTEN_IDS = {} - -def reset_auto_cell_id(): - global AUTO_CELL_ID - AUTO_CELL_ID = 10000 - - -class Cell(object): - """A region of space defined as the intersection of half-space created by - quadric surfaces. - - Parameters - ---------- - cell_id : int, optional - Unique identifier for the cell. If not specified, an identifier will - automatically be assigned. - name : str, optional - Name of the cell. If not specified, the name is the empty string. - - Attributes - ---------- - id : int - Unique identifier for the cell - name : str - Name of the cell - fill : Material or Universe or Lattice or 'void' or iterable of Material - Indicates what the region of space is filled with. Multiple materials - can be given to give each distributed cell instance a unique material. - region : openmc.region.Region - Region of space that is assigned to the cell. - temperature : float or iterable of float - Temperature of the cell in Kelvin. Multiple temperatures can be given - to give each distributed cell instance a unique temperature. - rotation : ndarray - If the cell is filled with a universe, this array specifies the angles - in degrees about the x, y, and z axes that the filled universe should be - rotated. - translation : ndarray - If the cell is filled with a universe, this array specifies a vector - that is used to translate (shift) the universe. - offsets : ndarray - Array of offsets used for distributed cell searches - distribcell_index : int - Index of this cell in distribcell arrays - - """ - - def __init__(self, cell_id=None, name=''): - # Initialize Cell class attributes - self.id = cell_id - self.name = name - self._fill = None - self._type = None - self._region = None - self._temperature = None - self._rotation = None - self._translation = None - self._offsets = None - self._distribcell_index = None - - def __eq__(self, other): - if not isinstance(other, Cell): - return False - elif self.id != other.id: - return False - elif self.name != other.name: - return False - elif self.fill != other.fill: - return False - elif self.region != other.region: - return False - elif self.temperature != other.temperature: - return False - elif self.rotation != other.rotation: - return False - elif self.translation != other.translation: - return False - else: - return True - - def __ne__(self, other): - return not self == other - - def __hash__(self): - return hash(repr(self)) - - def __repr__(self): - string = 'Cell\n' - string += '{0: <16}{1}{2}\n'.format('\tID', '=\t', self._id) - string += '{0: <16}{1}{2}\n'.format('\tName', '=\t', self._name) - - if isinstance(self._fill, openmc.Material): - string += '{0: <16}{1}{2}\n'.format('\tMaterial', '=\t', - self._fill._id) - elif isinstance(self._fill, Iterable): - string += '{0: <16}{1}'.format('\tMaterial', '=\t') - string += '[' - string += ', '.join(['void' if m == 'void' else str(m.id) - for m in self.fill]) - string += ']\n' - elif isinstance(self._fill, (Universe, Lattice)): - string += '{0: <16}{1}{2}\n'.format('\tFill', '=\t', - self._fill._id) - else: - string += '{0: <16}{1}{2}\n'.format('\tFill', '=\t', self._fill) - - string += '{0: <16}{1}{2}\n'.format('\tRegion', '=\t', self._region) - - if self.fill_type == 'material': - string += '\t{0: <15}=\t{1}\n'.format('Temperature', - self.temperature) - - string += '{0: <16}{1}{2}\n'.format('\tRotation', '=\t', - self._rotation) - string += '{0: <16}{1}{2}\n'.format('\tTranslation', '=\t', - self._translation) - string += '{0: <16}{1}{2}\n'.format('\tOffset', '=\t', self._offsets) - string += '{0: <16}{1}{2}\n'.format('\tDistribcell index', '=\t', - self._distribcell_index) - - return string - - @property - def id(self): - return self._id - - @property - def name(self): - return self._name - - @property - def fill(self): - return self._fill - - @property - def fill_type(self): - if isinstance(self.fill, (openmc.Material, Iterable)): - return 'material' - elif isinstance(self.fill, openmc.Universe): - return 'universe' - elif isinstance(self.fill, openmc.Lattice): - return 'lattice' - else: - return None - - @property - def region(self): - return self._region - - @property - def temperature(self): - return self._temperature - - @property - def rotation(self): - return self._rotation - - @property - def translation(self): - return self._translation - - @property - def offsets(self): - return self._offsets - - @property - def distribcell_index(self): - return self._distribcell_index - - @id.setter - def id(self, cell_id): - if cell_id is None: - global AUTO_CELL_ID - self._id = AUTO_CELL_ID - AUTO_CELL_ID += 1 - else: - cv.check_type('cell ID', cell_id, Integral) - cv.check_greater_than('cell ID', cell_id, 0, equality=True) - self._id = cell_id - - @name.setter - def name(self, name): - if name is not None: - cv.check_type('cell name', name, basestring) - self._name = name - else: - self._name = '' - - @fill.setter - def fill(self, fill): - if isinstance(fill, basestring): - if fill.strip().lower() == 'void': - self._type = 'void' - else: - msg = 'Unable to set Cell ID="{0}" to use a non-Material or ' \ - 'Universe fill "{1}"'.format(self._id, fill) - raise ValueError(msg) - - elif isinstance(fill, openmc.Material): - self._type = 'normal' - - elif isinstance(fill, Iterable): - cv.check_type('cell.fill', fill, Iterable, - (openmc.Material, basestring)) - self._type = 'normal' - - elif isinstance(fill, Universe): - self._type = 'fill' - - elif isinstance(fill, Lattice): - self._type = 'lattice' - - else: - msg = 'Unable to set Cell ID="{0}" to use a non-Material or ' \ - 'Universe fill "{1}"'.format(self._id, fill) - raise ValueError(msg) - - self._fill = fill - - @rotation.setter - def rotation(self, rotation): - cv.check_type('cell rotation', rotation, Iterable, Real) - cv.check_length('cell rotation', rotation, 3) - self._rotation = rotation - - @translation.setter - def translation(self, translation): - cv.check_type('cell translation', translation, Iterable, Real) - cv.check_length('cell translation', translation, 3) - self._translation = translation - - @offsets.setter - def offsets(self, offsets): - cv.check_type('cell offsets', offsets, Iterable) - self._offsets = offsets - - @region.setter - def region(self, region): - cv.check_type('cell region', region, Region) - self._region = region - - @temperature.setter - def temperature(self, temperature): - cv.check_type('cell temperature', temperature, (Iterable, Real)) - if isinstance(temperature, Iterable): - cv.check_type('cell temperature', temperature, Iterable, Real) - for T in temperature: - cv.check_greater_than('cell temperature', T, 0.0, True) - else: - cv.check_greater_than('cell temperature', temperature, 0.0, True) - self._temperature = temperature - - @distribcell_index.setter - def distribcell_index(self, ind): - cv.check_type('distribcell index', ind, Integral) - self._distribcell_index = ind - - def add_surface(self, surface, halfspace): - """Add a half-space to the list of half-spaces whose intersection defines the - cell. - - Parameters - ---------- - surface : openmc.surface.Surface - Quadric surface dividing space - halfspace : {-1, 1} - Indicate whether the negative or positive half-space is to be used - - """ - - warnings.warn("Cell.add_surface(...) has been deprecated and may be " - "removed in a future version. The region for a Cell " - "should be defined using the region property directly.", - DeprecationWarning) - - if not isinstance(surface, openmc.Surface): - msg = 'Unable to add Surface "{0}" to Cell ID="{1}" since it is ' \ - 'not a Surface object'.format(surface, self._id) - raise ValueError(msg) - - if halfspace not in [-1, +1]: - msg = 'Unable to add Surface "{0}" to Cell ID="{1}" with halfspace ' \ - '"{2}" since it is not +/-1'.format(surface, self._id, halfspace) - raise ValueError(msg) - - # If no region has been assigned, simply use the half-space. Otherwise, - # take the intersection of the current region and the half-space - # specified - region = +surface if halfspace == 1 else -surface - if self.region is None: - self.region = region - else: - if isinstance(self.region, Intersection): - self.region.nodes.append(region) - else: - self.region = Intersection(self.region, region) - - def get_cell_instance(self, path, distribcell_index): - # Get the current element and remove it from the list - cell_id = path[0] - path = path[1:] - - # If the Cell is filled by a Material - if self._type == 'normal' or self._type == 'void': - offset = 0 - - # If the Cell is filled by a Universe - elif self._type == 'fill': - offset = self.offsets[distribcell_index-1] - offset += self.fill.get_cell_instance(path, distribcell_index) - - # If the Cell is filled by a Lattice - else: - offset = self.fill.get_cell_instance(path, distribcell_index) - - return offset - - def get_all_nuclides(self): - """Return all nuclides contained in the cell - - Returns - ------- - nuclides : dict - Dictionary whose keys are nuclide names and values are 2-tuples of - (nuclide, density) - - """ - - nuclides = OrderedDict() - - if self._type != 'void': - nuclides.update(self._fill.get_all_nuclides()) - - return nuclides - - def get_all_cells(self): - """Return all cells that are contained within this one if it is filled with a - universe or lattice - - Returns - ------- - cells : dict - Dictionary whose keys are cell IDs and values are Cell instances - - """ - - cells = OrderedDict() - - if self._type == 'fill' or self._type == 'lattice': - cells.update(self._fill.get_all_cells()) - - return cells - - def get_all_materials(self): - """Return all materials that are contained within the cell - - Returns - ------- - materials : dict - Dictionary whose keys are material IDs and values are Material instances - - """ - - materials = OrderedDict() - if self.fill_type == 'material': - materials[self.fill.id] = self.fill - - # Append all Cells in each Cell in the Universe to the dictionary - cells = self.get_all_cells() - for cell_id, cell in cells.items(): - materials.update(cell.get_all_materials()) - - return materials - - def get_all_universes(self): - """Return all universes that are contained within this one if any of - its cells are filled with a universe or lattice. - - Returns - ------- - universes : dict - Dictionary whose keys are universe IDs and values are Universe - instances - - """ - - universes = OrderedDict() - - if self._type == 'fill': - universes[self._fill._id] = self._fill - universes.update(self._fill.get_all_universes()) - elif self._type == 'lattice': - universes.update(self._fill.get_all_universes()) - - return universes - - def create_xml_subelement(self, xml_element): - element = ET.Element("cell") - element.set("id", str(self.id)) - - if len(self._name) > 0: - element.set("name", str(self.name)) - - if isinstance(self.fill, basestring): - element.set("material", "void") - - elif isinstance(self.fill, openmc.Material): - element.set("material", str(self.fill.id)) - - elif isinstance(self.fill, Iterable): - element.set("material", ' '.join([m if m == 'void' else str(m.id) - for m in self.fill])) - - elif isinstance(self.fill, (Universe, Lattice)): - element.set("fill", str(self.fill.id)) - self.fill.create_xml_subelement(xml_element) - - else: - element.set("fill", str(self.fill)) - self.fill.create_xml_subelement(xml_element) - - if self.region is not None: - # Set the region attribute with the region specification - element.set("region", str(self.region)) - - # Only surfaces that appear in a region are added to the geometry - # file, so the appropriate check is performed here. First we create - # a function which is called recursively to navigate through the CSG - # tree. When it reaches a leaf (a Halfspace), it creates a - # element for the corresponding surface if none has been created - # thus far. - def create_surface_elements(node, element): - if isinstance(node, Halfspace): - path = './surface[@id=\'{0}\']'.format(node.surface.id) - if xml_element.find(path) is None: - surface_subelement = node.surface.create_xml_subelement() - xml_element.append(surface_subelement) - elif isinstance(node, Complement): - create_surface_elements(node.node, element) - else: - for subnode in node.nodes: - create_surface_elements(subnode, element) - - # Call the recursive function from the top node - create_surface_elements(self.region, xml_element) - - if self.temperature is not None: - if isinstance(self.temperature, Iterable): - element.set("temperature", ' '.join( - [str(t) for t in self.temperature])) - else: - element.set("temperature", str(self.temperature)) - - if self.translation is not None: - element.set("translation", ' '.join(map(str, self.translation))) - - if self.rotation is not None: - element.set("rotation", ' '.join(map(str, self.rotation))) - - return element - - # A static variable for auto-generated Lattice (Universe) IDs AUTO_UNIVERSE_ID = 10000 @@ -513,8 +43,9 @@ class Universe(object): Unique identifier of the universe name : str Name of the universe - cells : dict - Dictionary whose keys are cell IDs and values are Cell instances + cells : collections.OrderedDict + Dictionary whose keys are cell IDs and values are :class:`Cell` + instances """ @@ -596,12 +127,12 @@ class Universe(object): Parameters ---------- - cell : Cell + cell : openmc.Cell Cell to add """ - if not isinstance(cell, Cell): + if not isinstance(cell, openmc.Cell): msg = 'Unable to add a Cell to Universe ID="{0}" since "{1}" is not ' \ 'a Cell'.format(self._id, cell) raise ValueError(msg) @@ -616,7 +147,7 @@ class Universe(object): Parameters ---------- - cells : array-like of Cell + cells : Iterable of openmc.Cell Cells to add """ @@ -634,12 +165,12 @@ class Universe(object): Parameters ---------- - cell : Cell + cell : openmc.Cell Cell to remove """ - if not isinstance(cell, Cell): + if not isinstance(cell, openmc.Cell): msg = 'Unable to remove a Cell from Universe ID="{0}" since "{1}" is ' \ 'not a Cell'.format(self._id, cell) raise ValueError(msg) @@ -654,11 +185,19 @@ class Universe(object): self._cells.clear() def get_cell_instance(self, path, distribcell_index): - # Get the current element and remove it from the list - path = path[1:] - # Get the Cell ID - cell_id = path[0] + # Pop off the root Universe ID from the path + next_index = path.index('-') + path = path[next_index+2:] + + # Extract the Cell ID from the path + if '-' in path: + next_index = path.index('-') + cell_id = int(path[:next_index]) + path = path[next_index+2:] + else: + cell_id = int(path) + path = '' # Make a recursive call to the Cell within this Universe offset = self.cells[cell_id].get_cell_instance(path, distribcell_index) @@ -671,7 +210,7 @@ class Universe(object): Returns ------- - nuclides : dict + nuclides : collections.OrderedDict Dictionary whose keys are nuclide names and values are 2-tuples of (nuclide, density) @@ -690,8 +229,9 @@ class Universe(object): Returns ------- - cells : dict - Dictionary whose keys are cell IDs and values are Cell instances + cells : collections.OrderedDict + Dictionary whose keys are cell IDs and values are :class:`Cell` + instances """ @@ -711,8 +251,9 @@ class Universe(object): Returns ------- - materials : dict - Dictionary whose keys are material IDs and values are Material instances + materials : Collections.OrderedDict + Dictionary whose keys are material IDs and values are + :class:`Material` instances """ @@ -730,9 +271,9 @@ class Universe(object): Returns ------- - universes : dict - Dictionary whose keys are universe IDs and values are Universe - instances + universes : collections.OrderedDict + Dictionary whose keys are universe IDs and values are + :class:`Universe` instances """ @@ -762,849 +303,3 @@ class Universe(object): # Append the Universe ID to the subelement and add to Element cell_subelement.set("universe", str(self._id)) xml_element.append(cell_subelement) - - -class Lattice(object): - """A repeating structure wherein each element is a universe. - - Parameters - ---------- - lattice_id : int, optional - Unique identifier for the lattice. If not specified, an identifier will - automatically be assigned. - name : str, optional - Name of the lattice. If not specified, the name is the empty string. - - Attributes - ---------- - id : int - Unique identifier for the lattice - name : str - Name of the lattice - pitch : float - Pitch of the lattice in cm - outer : int - The unique identifier of a universe to fill all space outside the - lattice - universes : ndarray of Universe - An array of universes filling each element of the lattice - - """ - - # This is an abstract class which cannot be instantiated - __metaclass__ = abc.ABCMeta - - def __init__(self, lattice_id=None, name=''): - # Initialize Lattice class attributes - self.id = lattice_id - self.name = name - self._pitch = None - self._outer = None - self._universes = None - - def __eq__(self, other): - if not isinstance(other, Lattice): - return False - elif self.id != other.id: - return False - elif self.name != other.name: - return False - elif self.pitch != other.pitch: - return False - elif self.outer != other.outer: - return False - elif self.universes != other.universes: - return False - else: - return True - - def __ne__(self, other): - return not self == other - - @property - def id(self): - return self._id - - @property - def name(self): - return self._name - - @property - def pitch(self): - return self._pitch - - @property - def outer(self): - return self._outer - - @property - def universes(self): - return self._universes - - @id.setter - def id(self, lattice_id): - if lattice_id is None: - global AUTO_UNIVERSE_ID - self._id = AUTO_UNIVERSE_ID - AUTO_UNIVERSE_ID += 1 - else: - cv.check_type('lattice ID', lattice_id, Integral) - cv.check_greater_than('lattice ID', lattice_id, 0, equality=True) - self._id = lattice_id - - @name.setter - def name(self, name): - if name is not None: - cv.check_type('lattice name', name, basestring) - self._name = name - else: - self._name = '' - - @outer.setter - def outer(self, outer): - cv.check_type('outer universe', outer, Universe) - self._outer = outer - - @universes.setter - def universes(self, universes): - cv.check_iterable_type('lattice universes', universes, Universe, - min_depth=2, max_depth=3) - self._universes = np.asarray(universes) - - def get_unique_universes(self): - """Determine all unique universes in the lattice - - Returns - ------- - universes : dict - Dictionary whose keys are universe IDs and values are Universe - instances - - """ - - univs = OrderedDict() - for k in range(len(self._universes)): - for j in range(len(self._universes[k])): - if isinstance(self._universes[k][j], Universe): - u = self._universes[k][j] - univs[u._id] = u - else: - for i in range(len(self._universes[k][j])): - u = self._universes[k][j][i] - assert isinstance(u, Universe) - univs[u._id] = u - - if self.outer is not None: - univs[self.outer._id] = self.outer - - return univs - - def get_all_nuclides(self): - """Return all nuclides contained in the lattice - - Returns - ------- - nuclides : dict - Dictionary whose keys are nuclide names and values are 2-tuples of - (nuclide, density) - - """ - - nuclides = OrderedDict() - - # Get all unique Universes contained in each of the lattice cells - unique_universes = self.get_unique_universes() - - # Append all Universes containing each cell to the dictionary - for universe_id, universe in unique_universes.items(): - nuclides.update(universe.get_all_nuclides()) - - return nuclides - - def get_all_cells(self): - """Return all cells that are contained within the lattice - - Returns - ------- - cells : dict - Dictionary whose keys are cell IDs and values are Cell instances - - """ - - cells = OrderedDict() - unique_universes = self.get_unique_universes() - - for universe_id, universe in unique_universes.items(): - cells.update(universe.get_all_cells()) - - return cells - - def get_all_materials(self): - """Return all materials that are contained within the lattice - - Returns - ------- - materials : dict - Dictionary whose keys are material IDs and values are Material instances - - """ - - materials = OrderedDict() - - # Append all Cells in each Cell in the Universe to the dictionary - cells = self.get_all_cells() - for cell_id, cell in cells.items(): - materials.update(cell.get_all_materials()) - - return materials - - def get_all_universes(self): - """Return all universes that are contained within the lattice - - Returns - ------- - universes : dict - Dictionary whose keys are universe IDs and values are Universe - instances - - """ - - # Initialize a dictionary of all Universes contained by the Lattice - # in each nested Universe level - all_universes = OrderedDict() - - # Get all unique Universes contained in each of the lattice cells - unique_universes = self.get_unique_universes() - - # Add the unique Universes filling each Lattice cell - all_universes.update(unique_universes) - - # Append all Universes containing each cell to the dictionary - for universe_id, universe in unique_universes.items(): - all_universes.update(universe.get_all_universes()) - - return all_universes - - -class RectLattice(Lattice): - """A lattice consisting of rectangular prisms. - - Parameters - ---------- - lattice_id : int, optional - Unique identifier for the lattice. If not specified, an identifier will - automatically be assigned. - name : str, optional - Name of the lattice. If not specified, the name is the empty string. - - Attributes - ---------- - id : int - Unique identifier for the lattice - name : str - Name of the lattice - dimension : array-like of int - An array of two or three integers representing the number of lattice - cells in the x- and y- (and z-) directions, respectively. - lower_left : array-like of float - The coordinates of the lower-left corner of the lattice. If the lattice - is two-dimensional, only the x- and y-coordinates are specified. - - """ - - def __init__(self, lattice_id=None, name=''): - super(RectLattice, self).__init__(lattice_id, name) - - # Initialize Lattice class attributes - self._dimension = None - self._lower_left = None - self._offsets = None - - def __eq__(self, other): - if not isinstance(other, RectLattice): - return False - elif not super(RectLattice, self).__eq__(other): - return False - elif self.dimension != other.dimension: - return False - elif self.lower_left != other.lower_left: - return False - else: - return True - - def __ne__(self, other): - return not self == other - - def __hash__(self): - return hash(repr(self)) - - def __repr__(self): - string = 'RectLattice\n' - string += '{0: <16}{1}{2}\n'.format('\tID', '=\t', self._id) - string += '{0: <16}{1}{2}\n'.format('\tName', '=\t', self._name) - string += '{0: <16}{1}{2}\n'.format('\tDimension', '=\t', - self._dimension) - string += '{0: <16}{1}{2}\n'.format('\tLower Left', '=\t', - self._lower_left) - string += '{0: <16}{1}{2}\n'.format('\tPitch', '=\t', self._pitch) - - if self._outer is not None: - string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', - self._outer._id) - else: - string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', - self._outer) - - string += '{0: <16}\n'.format('\tUniverses') - - # Lattice nested Universe IDs - column major for Fortran - for i, universe in enumerate(np.ravel(self._universes)): - string += '{0} '.format(universe._id) - - # Add a newline character every time we reach end of row of cells - if (i+1) % self._dimension[-1] == 0: - string += '\n' - - string = string.rstrip('\n') - - if self._offsets is not None: - string += '{0: <16}\n'.format('\tOffsets') - - # Lattice cell offsets - for i, offset in enumerate(np.ravel(self._offsets)): - string += '{0} '.format(offset) - - # Add a newline character when we reach end of row of cells - if (i+1) % self._dimension[-1] == 0: - string += '\n' - - string = string.rstrip('\n') - - return string - - @property - def dimension(self): - return self._dimension - - @property - def lower_left(self): - return self._lower_left - - @property - def offsets(self): - return self._offsets - - @dimension.setter - def dimension(self, dimension): - cv.check_type('lattice dimension', dimension, Iterable, Integral) - cv.check_length('lattice dimension', dimension, 2, 3) - for dim in dimension: - cv.check_greater_than('lattice dimension', dim, 0) - self._dimension = dimension - - @lower_left.setter - def lower_left(self, lower_left): - cv.check_type('lattice lower left corner', lower_left, Iterable, Real) - cv.check_length('lattice lower left corner', lower_left, 2, 3) - self._lower_left = lower_left - - @offsets.setter - def offsets(self, offsets): - cv.check_type('lattice offsets', offsets, Iterable) - self._offsets = offsets - - @Lattice.pitch.setter - def pitch(self, pitch): - cv.check_type('lattice pitch', pitch, Iterable, Real) - cv.check_length('lattice pitch', pitch, 2, 3) - for dim in pitch: - cv.check_greater_than('lattice pitch', dim, 0.0) - self._pitch = pitch - - def get_cell_instance(self, path, distribcell_index): - # Get the current element and remove it from the list - i = path[0] - path = path[1:] - - # For 2D Lattices - if len(self._dimension) == 2: - offset = self._offsets[i[3]-1, i[2]-1, i[1]-1, distribcell_index-1] - offset += self._universes[i[1]-1][i[2]-1].get_cell_instance(path, - distribcell_index) - - # For 3D Lattices - else: - offset = self._offsets[i[3]-1, i[2]-1, i[1]-1, distribcell_index-1] - offset += self._universes[i[3]-1][i[2]-1][i[1]-1].get_cell_instance( - path, distribcell_index) - - return offset - - def create_xml_subelement(self, xml_element): - - # Determine if XML element already contains subelement for this Lattice - path = './lattice[@id=\'{0}\']'.format(self._id) - test = xml_element.find(path) - - # If the element does contain the Lattice subelement, then return - if test is not None: - return - - lattice_subelement = ET.Element("lattice") - lattice_subelement.set("id", str(self._id)) - - if len(self._name) > 0: - lattice_subelement.set("name", str(self._name)) - - # Export the Lattice cell pitch - pitch = ET.SubElement(lattice_subelement, "pitch") - pitch.text = ' '.join(map(str, self._pitch)) - - # Export the Lattice outer Universe (if specified) - if self._outer is not None: - outer = ET.SubElement(lattice_subelement, "outer") - outer.text = '{0}'.format(self._outer._id) - self._outer.create_xml_subelement(xml_element) - - # Export Lattice cell dimensions - dimension = ET.SubElement(lattice_subelement, "dimension") - dimension.text = ' '.join(map(str, self._dimension)) - - # Export Lattice lower left - lower_left = ET.SubElement(lattice_subelement, "lower_left") - lower_left.text = ' '.join(map(str, self._lower_left)) - - # Export the Lattice nested Universe IDs - column major for Fortran - universe_ids = '\n' - - # 3D Lattices - if len(self._dimension) == 3: - for z in range(self._dimension[2]): - for y in range(self._dimension[1]): - for x in range(self._dimension[0]): - universe = self._universes[z][y][x] - - # Append Universe ID to the Lattice XML subelement - universe_ids += '{0} '.format(universe._id) - - # Create XML subelement for this Universe - universe.create_xml_subelement(xml_element) - - # Add newline character when we reach end of row of cells - universe_ids += '\n' - - # Add newline character when we reach end of row of cells - universe_ids += '\n' - - # 2D Lattices - else: - for y in range(self._dimension[1]): - for x in range(self._dimension[0]): - universe = self._universes[y][x] - - # Append Universe ID to Lattice XML subelement - universe_ids += '{0} '.format(universe._id) - - # Create XML subelement for this Universe - universe.create_xml_subelement(xml_element) - - # Add newline character when we reach end of row of cells - universe_ids += '\n' - - # Remove trailing newline character from Universe IDs string - universe_ids = universe_ids.rstrip('\n') - - universes = ET.SubElement(lattice_subelement, "universes") - universes.text = universe_ids - - # Append the XML subelement for this Lattice to the XML element - xml_element.append(lattice_subelement) - - -class HexLattice(Lattice): - """A lattice consisting of hexagonal prisms. - - Parameters - ---------- - lattice_id : int, optional - Unique identifier for the lattice. If not specified, an identifier will - automatically be assigned. - name : str, optional - Name of the lattice. If not specified, the name is the empty string. - - Attributes - ---------- - id : int - Unique identifier for the lattice - name : str - Name of the lattice - num_rings : int - Number of radial ring positions in the xy-plane - num_axial : int - Number of positions along the z-axis. - center : array-like of float - Coordinates of the center of the lattice. If the lattice does not have - axial sections then only the x- and y-coordinates are specified - - """ - - def __init__(self, lattice_id=None, name=''): - super(HexLattice, self).__init__(lattice_id, name) - - # Initialize Lattice class attributes - self._num_rings = None - self._num_axial = None - self._center = None - - def __eq__(self, other): - if not isinstance(other, HexLattice): - return False - elif not super(HexLattice, self).__eq__(other): - return False - elif self.num_rings != other.num_rings: - return False - elif self.num_axial != other.num_axial: - return False - elif self.center != other.center: - return False - else: - return True - - def __ne__(self, other): - return not self == other - - def __hash__(self): - return hash(repr(self)) - - def __repr__(self): - string = 'HexLattice\n' - string += '{0: <16}{1}{2}\n'.format('\tID', '=\t', self._id) - string += '{0: <16}{1}{2}\n'.format('\tName', '=\t', self._name) - string += '{0: <16}{1}{2}\n'.format('\t# Rings', '=\t', self._num_rings) - string += '{0: <16}{1}{2}\n'.format('\t# Axial', '=\t', self._num_axial) - string += '{0: <16}{1}{2}\n'.format('\tCenter', '=\t', - self._center) - string += '{0: <16}{1}{2}\n'.format('\tPitch', '=\t', self._pitch) - - if self._outer is not None: - string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', - self._outer._id) - else: - string += '{0: <16}{1}{2}\n'.format('\tOuter', '=\t', - self._outer) - - string += '{0: <16}\n'.format('\tUniverses') - - if self._num_axial is not None: - slices = [self._repr_axial_slice(x) for x in self._universes] - string += '\n'.join(slices) - - else: - string += self._repr_axial_slice(self._universes) - - return string - - @property - def num_rings(self): - return self._num_rings - - @property - def num_axial(self): - return self._num_axial - - @property - def center(self): - return self._center - - @num_rings.setter - def num_rings(self, num_rings): - cv.check_type('number of rings', num_rings, Integral) - cv.check_greater_than('number of rings', num_rings, 0) - self._num_rings = num_rings - - @num_axial.setter - def num_axial(self, num_axial): - cv.check_type('number of axial', num_axial, Integral) - cv.check_greater_than('number of axial', num_axial, 0) - self._num_axial = num_axial - - @center.setter - def center(self, center): - cv.check_type('lattice center', center, Iterable, Real) - cv.check_length('lattice center', center, 2, 3) - self._center = center - - @Lattice.pitch.setter - def pitch(self, pitch): - cv.check_type('lattice pitch', pitch, Iterable, Real) - cv.check_length('lattice pitch', pitch, 1, 2) - for dim in pitch: - cv.check_greater_than('lattice pitch', dim, 0) - self._pitch = pitch - - @Lattice.universes.setter - def universes(self, universes): - # Call Lattice.universes parent class setter property - Lattice.universes.fset(self, universes) - - # NOTE: This routine assumes that the user creates a "ragged" list of - # lists, where each sub-list corresponds to one ring of Universes. - # The sub-lists are ordered from outermost ring to innermost ring. - # The Universes within each sub-list are ordered from the "top" in a - # clockwise fashion. - - # Check to see if the given universes look like a 2D or a 3D array. - if isinstance(self._universes[0][0], Universe): - n_dims = 2 - - elif isinstance(self._universes[0][0][0], Universe): - n_dims = 3 - - else: - msg = 'HexLattice ID={0:d} does not appear to be either 2D or ' \ - '3D. Make sure set_universes was given a two-deep or ' \ - 'three-deep iterable of universes.'.format(self._id) - raise RuntimeError(msg) - - # Set the number of axial positions. - if n_dims == 3: - self.num_axial = len(self._universes) - else: - self._num_axial = None - - # Set the number of rings and make sure this number is consistent for - # all axial positions. - if n_dims == 3: - self.num_rings = len(self._universes) - for rings in self._universes: - if len(rings) != self._num_rings: - msg = 'HexLattice ID={0:d} has an inconsistent number of ' \ - 'rings per axial positon'.format(self._id) - raise ValueError(msg) - - else: - self.num_rings = len(self._universes) - - # Make sure there are the correct number of elements in each ring. - if n_dims == 3: - for axial_slice in self._universes: - # Check the center ring. - if len(axial_slice[-1]) != 1: - msg = 'HexLattice ID={0:d} has the wrong number of ' \ - 'elements in the innermost ring. Only 1 element is ' \ - 'allowed in the innermost ring.'.format(self._id) - raise ValueError(msg) - - # Check the outer rings. - for r in range(self._num_rings-1): - if len(axial_slice[r]) != 6*(self._num_rings - 1 - r): - msg = 'HexLattice ID={0:d} has the wrong number of ' \ - 'elements in ring number {1:d} (counting from the '\ - 'outermost ring). This ring should have {2:d} ' \ - 'elements.'.format(self._id, r, - 6*(self._num_rings - 1 - r)) - raise ValueError(msg) - - else: - axial_slice = self._universes - # Check the center ring. - if len(axial_slice[-1]) != 1: - msg = 'HexLattice ID={0:d} has the wrong number of ' \ - 'elements in the innermost ring. Only 1 element is ' \ - 'allowed in the innermost ring.'.format(self._id) - raise ValueError(msg) - - # Check the outer rings. - for r in range(self._num_rings-1): - if len(axial_slice[r]) != 6*(self._num_rings - 1 - r): - msg = 'HexLattice ID={0:d} has the wrong number of ' \ - 'elements in ring number {1:d} (counting from the '\ - 'outermost ring). This ring should have {2:d} ' \ - 'elements.'.format(self._id, r, - 6*(self._num_rings - 1 - r)) - raise ValueError(msg) - - def create_xml_subelement(self, xml_element): - # Determine if XML element already contains subelement for this Lattice - path = './hex_lattice[@id=\'{0}\']'.format(self._id) - test = xml_element.find(path) - - # If the element does contain the Lattice subelement, then return - if test is not None: - return - - lattice_subelement = ET.Element("hex_lattice") - lattice_subelement.set("id", str(self._id)) - - if len(self._name) > 0: - lattice_subelement.set("name", str(self._name)) - - # Export the Lattice cell pitch - pitch = ET.SubElement(lattice_subelement, "pitch") - pitch.text = ' '.join(map(str, self._pitch)) - - # Export the Lattice outer Universe (if specified) - if self._outer is not None: - outer = ET.SubElement(lattice_subelement, "outer") - outer.text = '{0}'.format(self._outer._id) - self._outer.create_xml_subelement(xml_element) - - lattice_subelement.set("n_rings", str(self._num_rings)) - - if self._num_axial is not None: - lattice_subelement.set("n_axial", str(self._num_axial)) - - # Export Lattice cell center - dimension = ET.SubElement(lattice_subelement, "center") - dimension.text = ' '.join(map(str, self._center)) - - # Export the Lattice nested Universe IDs. - - # 3D Lattices - if self._num_axial is not None: - slices = [] - for z in range(self._num_axial): - # Initialize the center universe. - universe = self._universes[z][-1][0] - universe.create_xml_subelement(xml_element) - - # Initialize the remaining universes. - for r in range(self._num_rings-1): - for theta in range(6*(self._num_rings - 1 - r)): - universe = self._universes[z][r][theta] - universe.create_xml_subelement(xml_element) - - # Get a string representation of the universe IDs. - slices.append(self._repr_axial_slice(self._universes[z])) - - # Collapse the list of axial slices into a single string. - universe_ids = '\n'.join(slices) - - # 2D Lattices - else: - # Initialize the center universe. - universe = self._universes[-1][0] - universe.create_xml_subelement(xml_element) - - # Initialize the remaining universes. - for r in range(self._num_rings - 1): - for theta in range(6*(self._num_rings - 1 - r)): - universe = self._universes[r][theta] - universe.create_xml_subelement(xml_element) - - # Get a string representation of the universe IDs. - universe_ids = self._repr_axial_slice(self._universes) - - universes = ET.SubElement(lattice_subelement, "universes") - universes.text = '\n' + universe_ids - - # Append the XML subelement for this Lattice to the XML element - xml_element.append(lattice_subelement) - - def _repr_axial_slice(self, universes): - """Return string representation for the given 2D group of universes. - - The 'universes' argument should be a list of lists of universes where - each sub-list represents a single ring. The first list should be the - outer ring. - """ - - # Find the largest universe ID and count the number of digits so we can - # properly pad the output string later. - largest_id = max([max([univ._id for univ in ring]) - for ring in universes]) - n_digits = len(str(largest_id)) - pad = ' '*n_digits - id_form = '{: ^' + str(n_digits) + 'd}' - - # Initialize the list for each row. - rows = [ [] for i in range(1 + 4 * (self._num_rings-1)) ] - middle = 2 * (self._num_rings - 1) - - # Start with the degenerate first ring. - universe = universes[-1][0] - rows[middle] = [id_form.format(universe._id)] - - # Add universes one ring at a time. - for r in range(1, self._num_rings): - # r_prime increments down while r increments up. - r_prime = self._num_rings - 1 - r - theta = 0 - y = middle + 2*r - - # Climb down the top-right. - for i in range(r): - # Add the universe. - universe = universes[r_prime][theta] - rows[y].append(id_form.format(universe._id)) - - # Translate the indices. - y -= 1 - theta += 1 - - # Climb down the right. - for i in range(r): - # Add the universe. - universe = universes[r_prime][theta] - rows[y].append(id_form.format(universe._id)) - - # Translate the indices. - y -= 2 - theta += 1 - - # Climb down the bottom-right. - for i in range(r): - # Add the universe. - universe = universes[r_prime][theta] - rows[y].append(id_form.format(universe._id)) - - # Translate the indices. - y -= 1 - theta += 1 - - # Climb up the bottom-left. - for i in range(r): - # Add the universe. - universe = universes[r_prime][theta] - rows[y].insert(0, id_form.format(universe._id)) - - # Translate the indices. - y += 1 - theta += 1 - - # Climb up the left. - for i in range(r): - # Add the universe. - universe = universes[r_prime][theta] - rows[y].insert(0, id_form.format(universe._id)) - - # Translate the indices. - y += 2 - theta += 1 - - # Climb up the top-left. - for i in range(r): - # Add the universe. - universe = universes[r_prime][theta] - rows[y].insert(0, id_form.format(universe._id)) - - # Translate the indices. - y += 1 - theta += 1 - - # Flip the rows and join each row into a single string. - rows = [pad.join(x) for x in rows[::-1]] - - # Pad the beginning of the rows so they line up properly. - for y in range(self._num_rings - 1): - rows[y] = (self._num_rings - 1 - y)*pad + rows[y] - rows[-1 - y] = (self._num_rings - 1 - y)*pad + rows[-1 - y] - - for y in range(self._num_rings % 2, self._num_rings, 2): - rows[middle + y] = pad + rows[middle + y] - if y != 0: - rows[middle - y] = pad + rows[middle - y] - - # Join the rows together and return the string. - universe_ids = '\n'.join(rows) - return universe_ids diff --git a/setup.py b/setup.py index 87fdff68c..e66b0b7a0 100644 --- a/setup.py +++ b/setup.py @@ -36,7 +36,7 @@ if have_setuptools: # Optional dependencies 'extras_require': { - 'pandas': ['pandas'], + 'pandas': ['pandas>=0.17.0'], 'sparse' : ['scipy'], 'vtk': ['vtk', 'silomesh'], 'validate': ['lxml'] diff --git a/src/ace.F90 b/src/ace.F90 index f84b82030..b401caca8 100644 --- a/src/ace.F90 +++ b/src/ace.F90 @@ -1,23 +1,25 @@ module ace - use ace_header, only: Nuclide, Reaction, SAlphaBeta, XsListing + use angleenergy_header, only: AngleEnergy use constants use distribution_univariate, only: Uniform, Equiprobable, Tabular use endf, only: is_fission, is_disappearance + use endf_header, only: Constant1D, Tabulated1D, Polynomial use energy_distribution, only: TabularEquiprobable, LevelInelastic, & - ContinuousTabular, MaxwellEnergy, Evaporation, WattEnergy, NBodyPhaseSpace + ContinuousTabular, MaxwellEnergy, Evaporation, WattEnergy use error, only: fatal_error, warning - use fission, only: nu_total use global use list_header, only: ListInt use material_header, only: Material use multipole, only: multipole_read - use multipole_header, only: max_L, max_poles, max_poly + use nuclide_header use output, only: write_message + use product_header, only: ReactionProduct + use sab_header use set_header, only: SetChar - use secondary_header, only: AngleEnergy use secondary_correlated, only: CorrelatedAngleEnergy use secondary_kalbach, only: KalbachMann + use secondary_nbody, only: NBodyPhaseSpace use secondary_uncorrelated, only: UncorrelatedAngleEnergy use string, only: to_str, to_lower @@ -35,11 +37,11 @@ module ace contains !=============================================================================== -! READ_XS reads all the cross sections for the problem and stores them in +! READ_ACE_XS reads all the cross sections for the problem and stores them in ! nuclides and sab_tables arrays !=============================================================================== - subroutine read_xs() + subroutine read_ace_xs() integer :: i ! index in materials array integer :: j ! index over nuclides in material @@ -53,8 +55,9 @@ contains integer :: temp_table ! temporary value for sorting character(12) :: name ! name of isotope, e.g. 92235.03c character(12) :: alias ! alias of nuclide, e.g. U-235.03c + logical :: mp_found ! if windowed multipole libraries were found type(Material), pointer :: mat - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc type(SAlphaBeta), pointer :: sab type(SetChar) :: already_read @@ -228,15 +231,30 @@ contains ! Show which nuclide results in lowest energy for neutron transport do i = 1, n_nuclides_total - if (nuclides(i)%energy(nuclides(i)%n_grid) == energy_max_neutron) then + if (nuclides(i) % energy(nuclides(i) % n_grid) == energy_max_neutron) then call write_message("Maximum neutron transport energy: " // & trim(to_str(energy_max_neutron)) // " MeV for " // & - trim(adjustl(nuclides(i)%name)), 6) + trim(adjustl(nuclides(i) % name)), 6) exit end if end do - end subroutine read_xs + ! If the user wants multipole, make sure we found a multipole library. + if (multipole_active) then + mp_found = .false. + do i = 1, n_nuclides_total + if (nuclides(i) % mp_present) then + mp_found = .true. + exit + end if + end do + if (.not. mp_found) call warning("Windowed multipole functionality is & + &turned on, but no multipole libraries were found. Set the & + & element in settings.xml or the & + &OPENMC_MULTIPOLE_LIBRARY environment variable.") + end if + + end subroutine read_ace_xs !=============================================================================== ! READ_ACE_TABLE reads a single cross section table in either ASCII or binary @@ -268,9 +286,9 @@ contains character(10) :: mat ! material identifier character(70) :: comment ! comment for ACE table character(MAX_FILE_LEN) :: filename ! path to ACE cross section library - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc type(SAlphaBeta), pointer :: sab - type(XsListing), pointer :: listing + type(XsListing), pointer :: listing ! determine path, record length, and location of table listing => xs_listings(i_listing) @@ -371,7 +389,7 @@ contains nuc % name = name nuc % awr = awr nuc % kT = kT - nuc % zaid = NXS(2) + nuc % zaid = listing % zaid end if ! read all blocks @@ -381,8 +399,8 @@ contains if (data_0K) then continue else - call read_nu_data(nuc) call read_reactions(nuc) + call read_nu_data(nuc) call read_energy_dist(nuc) call read_angular_dist(nuc) call read_unr_res(nuc) @@ -426,12 +444,12 @@ contains subroutine read_multipole_data(i_table) - integer, intent(in) :: i_table ! index in nuclides/sab_tables + integer, intent(in) :: i_table ! index in nuclides/sab_tables - logical :: file_exists ! does multipole library exist? - character(7) :: readable ! is multipole library readable? - character(6) :: zaid_string ! String of the ZAID - character(MAX_FILE_LEN+9) :: filename ! path to multipole xs library + logical :: file_exists ! Does multipole library exist? + character(7) :: readable ! Is multipole library readable? + character(6) :: zaid_string ! String of the ZAID + character(MAX_FILE_LEN+9) :: filename ! Path to multipole xs library ! For the time being, and I know this is a bit hacky, we just assume ! that the file will be zaid.h5. @@ -459,19 +477,6 @@ contains call multipole_read(filename, nuc % multipole, i_table) nuc % mp_present = .true. - ! Update the maximum number of poles, l indices, and polynomial order - if (nuc % multipole % max_w > max_poles) then - max_poles = nuc % multipole % max_w - end if - - if (nuc % multipole % num_l > max_L) then - max_L = nuc % multipole % num_l - end if - - if (nuc % multipole % fit_order + 1 > max_poly) then - max_poly = nuc % multipole % fit_order + 1 - end if - ! Recreate nu-fission tables if (nuc % fissionable) then call generate_nu_fission(nuc) @@ -487,8 +492,8 @@ contains !=============================================================================== subroutine read_esz(nuc, data_0K) - type(Nuclide), intent(inout) :: nuc - logical, intent(in) :: data_0K ! are we reading 0K data? + type(NuclideCE), intent(inout) :: nuc + logical, intent(in) :: data_0K ! are we reading 0K data? integer :: NE ! number of energy points for total and elastic cross sections integer :: i ! index in 0K elastic xs array for this nuclide @@ -575,200 +580,211 @@ contains !=============================================================================== subroutine read_nu_data(nuc) - type(Nuclide), intent(inout) :: nuc + type(NuclideCE), intent(inout) :: nuc - integer :: i ! loop index - integer :: JXS2 ! location for fission nu data - integer :: JXS24 ! location for delayed neutron data + integer :: i, j ! loop index + integer :: idx ! index in XSS integer :: KNU ! location for nu data integer :: LNU ! type of nu data (polynomial or tabular) - integer :: NC ! number of polynomial coefficients integer :: NR ! number of interpolation regions integer :: NE ! number of energies integer :: NPCR ! number of delayed neutron precursor groups - integer :: LED ! location of energy distribution locators - integer :: LDIS ! location of all energy distributions integer :: LOCC ! location of energy distributions for given MT integer :: LAW integer :: IDAT - integer :: lc ! locator - integer :: length ! length of data to allocate + real(8) :: total_group_probability + type(Tabulated1D) :: yield_delayed + type(Tabulated1D) :: group_probability - JXS2 = JXS(2) - JXS24 = JXS(24) - - if (JXS2 == 0) then - ! ======================================================================= - ! NO PROMPT/TOTAL NU DATA - nuc % nu_t_type = NU_NONE - nuc % nu_p_type = NU_NONE - - elseif (XSS(JXS2) > 0) then - ! ======================================================================= - ! PROMPT OR TOTAL NU DATA - KNU = JXS2 - LNU = int(XSS(KNU)) - if (LNU == 1) then - ! Polynomial data - nuc % nu_t_type = NU_POLYNOMIAL - nuc % nu_p_type = NU_NONE - - ! allocate determine how many coefficients for polynomial - NC = int(XSS(KNU+1)) - length = NC + 1 - elseif (LNU == 2) then - ! Tabular data - nuc % nu_t_type = NU_TABULAR - nuc % nu_p_type = NU_NONE - - ! determine number of interpolation regions and number of energies - NR = int(XSS(KNU+1)) - NE = int(XSS(KNU+2+2*NR)) - length = 2 + 2*NR + 2*NE - end if - - ! allocate space for nu data storage - allocate(nuc % nu_t_data(length)) - - ! read data -- for polynomial, this is the number of coefficients and the - ! coefficients themselves, and for tabular, this is interpolation data - ! and tabular E/nu - XSS_index = KNU + 1 - nuc % nu_t_data = get_real(length) - - elseif (XSS(JXS2) < 0) then - ! ======================================================================= - ! PROMPT AND TOTAL NU DATA -- read prompt data first - KNU = JXS2 + 1 - LNU = int(XSS(KNU)) - if (LNU == 1) then - ! Polynomial data - nuc % nu_p_type = NU_POLYNOMIAL - - ! allocate determine how many coefficients for polynomial - NC = int(XSS(KNU+1)) - length = NC + 1 - elseif (LNU == 2) then - ! Tabular data - nuc % nu_p_type = NU_TABULAR - - ! determine number of interpolation regions and number of energies - NR = int(XSS(KNU+1)) - NE = int(XSS(KNU+2+2*NR)) - length = 2 + 2*NR + 2*NE - end if - - ! allocate space for nu data storage - allocate(nuc % nu_p_data(length)) - - ! read data - XSS_index = KNU + 1 - nuc % nu_p_data = get_real(length) - - ! Now read total nu data - KNU = JXS2 + int(abs(XSS(JXS2))) + 1 - LNU = int(XSS(KNU)) - if (LNU == 1) then - ! Polynomial data - nuc % nu_t_type = NU_POLYNOMIAL - - ! allocate determine how many coefficients for polynomial - NC = int(XSS(KNU+1)) - length = NC + 1 - elseif (LNU == 2) then - ! Tabular data - nuc % nu_t_type = NU_TABULAR - - ! determine number of interpolation regions and number of energies - NR = int(XSS(KNU+1)) - NE = int(XSS(KNU+2+2*NR)) - length = 2 + 2*NR + 2*NE - end if - - ! allocate space for nu data storage - allocate(nuc % nu_t_data(length)) - - ! read data - XSS_index = KNU + 1 - nuc % nu_t_data = get_real(length) + if (JXS(2) == 0) then + ! Nuclide is not fissionable + return end if - if (JXS24 > 0) then - ! ======================================================================= - ! DELAYED NU DATA - - nuc % nu_d_type = NU_TABULAR - KNU = JXS24 - - ! determine size of tabular delayed nu data - NR = int(XSS(KNU+1)) - NE = int(XSS(KNU+2+2*NR)) - length = 2 + 2*NR + 2*NE - - ! allocate space for delayed nu data - allocate(nuc % nu_d_data(length)) - - ! read delayed nu data - XSS_index = KNU + 1 - nuc % nu_d_data = get_real(length) - - ! ======================================================================= - ! DELAYED NEUTRON ENERGY DISTRIBUTION - - ! Allocate space for secondary energy distribution + ! Determine number of delayed neutron precursors + if (JXS(24) > 0) then NPCR = NXS(8) + else + NPCR = 0 + end if + nuc % n_precursor = NPCR - ! Check to make sure nuclide does not have more than the maximum number - ! of delayed groups - if (NPCR > MAX_DELAYED_GROUPS) then - call fatal_error("Encountered nuclide with " // trim(to_str(NPCR)) & - // " delayed groups while the maximum number of delayed groups & - &set in constants.F90 is " // trim(to_str(MAX_DELAYED_GROUPS))) + ! Check to make sure nuclide does not have more than the maximum number + ! of delayed groups + if (NPCR > MAX_DELAYED_GROUPS) then + call fatal_error("Encountered nuclide with " // trim(to_str(NPCR)) & + // " delayed groups while the maximum number of delayed groups is " & + // trim(to_str(MAX_DELAYED_GROUPS))) + end if + + associate (rx => nuc % reactions(nuc % index_fission(1))) + ! Allocate space for prompt/delayed neutron products + allocate(rx % products(1 + NPCR)) + rx % products(:) % particle = NEUTRON + + if (XSS(JXS(2)) > 0) then + ! ======================================================================= + ! PROMPT OR TOTAL NU DATA + + ! If delayed data is present, then prompt data must be present. Otherwise + ! the product represents 'total' neutron emission + if (JXS(24) > 0) then + rx % products(1) % emission_mode = EMISSION_PROMPT + else + rx % products(1) % emission_mode = EMISSION_TOTAL + end if + + KNU = JXS(2) + LNU = nint(XSS(KNU)) + if (LNU == 1) then + ! Polynomial data + allocate(Polynomial :: rx % products(1) % yield) + + ! determine order of polynomial and read coefficients + select type (yield => rx % products(1) % yield) + type is (Polynomial) + call yield % from_ace(XSS, KNU + 1) + end select + + elseif (LNU == 2) then + ! Tabulated data + allocate(Tabulated1D :: rx % products(1) % yield) + + select type(yield => rx % products(1) % yield) + type is (Tabulated1D) + call yield % from_ace(XSS, KNU + 1) + end select + + end if + + elseif (XSS(JXS(2)) < 0) then + ! ======================================================================= + ! PROMPT AND TOTAL NU DATA + + rx % products(1) % emission_mode = EMISSION_PROMPT + + KNU = JXS(2) + 1 + LNU = nint(XSS(KNU)) + if (LNU == 1) then + ! Polynomial data + allocate(Polynomial :: rx % products(1) % yield) + + ! determine order of polynomial and read coefficients + select type (yield => rx % products(1) % yield) + type is (Polynomial) + call yield % from_ace(XSS, KNU + 1) + end select + + elseif (LNU == 2) then + ! Tabulated data + allocate(Tabulated1D :: rx % products(1) % yield) + + select type(yield => rx % products(1) % yield) + type is (Tabulated1D) + call yield % from_ace(XSS, KNU + 1) + end select + end if + + KNU = JXS(2) + nint(abs(XSS(JXS(2)))) + 1 + LNU = nint(XSS(KNU)) + if (LNU == 1) then + ! Polynomial data + allocate(Polynomial :: nuc % total_nu) + + ! determine order of polynomial and read coefficients + select type (yield => nuc % total_nu) + type is (Polynomial) + call yield % from_ace(XSS, KNU + 1) + end select + + elseif (LNU == 2) then + ! Tabulated data + allocate(Tabulated1D :: nuc % total_nu) + + select type(yield => nuc % total_nu) + type is (Tabulated1D) + call yield % from_ace(XSS, KNU + 1) + end select + end if end if - nuc % n_precursor = NPCR - allocate(nuc % nu_d_edist(NPCR)) + if (JXS(24) > 0) then + ! ======================================================================= + ! DELAYED NU DATA - LED = JXS(26) - LDIS = JXS(27) + ! Read total yield of delayed neutrons + call yield_delayed % from_ace(XSS, JXS(24) + 1) - ! Loop over all delayed neutron precursor groups - do i = 1, NPCR - ! find location of energy distribution data - LOCC = nint(XSS(LED + i - 1)) + idx = JXS(25) + total_group_probability = ZERO + do i = 1, NPCR + ! Set emission mode and decay rate + rx % products(1 + i) % emission_mode = EMISSION_DELAYED + rx % products(1 + i) % decay_rate = XSS(idx) - ! Determine law and location of data - LAW = nint(XSS(LDIS + LOCC)) - IDAT = nint(XSS(LDIS + LOCC + 1)) + ! Read probability for this precursor group + call group_probability % from_ace(XSS, idx + 1) - ! read energy distribution data - call get_energy_dist(nuc%nu_d_edist(i)%obj, LAW, LDIS, IDAT, & - ZERO, ZERO) + ! Set yield based on product of group probability and delayed yield + if (all(group_probability % y == group_probability % y(1))) then + allocate(Tabulated1D :: rx % products(1 + i) % yield) + select type (yield => rx % products(1 + i) % yield) + type is (Tabulated1D) + yield = yield_delayed + yield % y(:) = yield % y(:) * group_probability % y(1) + total_group_probability = total_group_probability + group_probability % y(1) + end select + else + call fatal_error("Delayed neutron with energy-dependent group & + &probability not implemented") + end if + + ! Advance position + NR = nint(XSS(idx + 1)) + NE = nint(XSS(idx + 2 + 2*NR)) + idx = idx + 3 + 2*(NR + NE) + + ! ======================================================================= + ! DELAYED NEUTRON ENERGY DISTRIBUTION + + ! Read energy distribution + LOCC = nint(XSS(JXS(26) + i - 1)) + + ! Determine law and location of data + LAW = nint(XSS(JXS(27) + LOCC)) + IDAT = nint(XSS(JXS(27) + LOCC + 1)) + + ! read energy distribution data + associate(p => rx % products(1 + i)) + allocate(p % applicability(1)) + allocate(p % distribution(1)) + call get_energy_dist(p % distribution(1) % obj, LAW, JXS(27), IDAT, & + ZERO, ZERO) + + select type (aedist => p % distribution(1) % obj) + type is (UncorrelatedAngleEnergy) + aedist % fission = .true. + end select + end associate + end do + + ! Renormalize delayed neutron yields to reflect fact that in ACE file, the + ! sum of the group probabilities is not exactly one + do i = 1, NPCR + select type (yield => rx % products(1 + i) % yield) + type is (Tabulated1D) + yield % y(:) = yield % y(:) / total_group_probability + end select + end do + end if + + ! Assign products to other fission reactions + do i = 2, nuc % n_fission + j = nuc % index_fission(i) + allocate(nuc % reactions(j) % products(1 + NPCR)) + nuc % reactions(j) % products(:) = rx % products(:) end do - - ! ======================================================================= - ! DELAYED NEUTRON PRECUSOR YIELDS AND CONSTANTS - - ! determine length of all precursor constants/yields/interp data - length = 0 - lc = JXS(25) - do i = 1, NPCR - NR = int(XSS(lc + length + 1)) - NE = int(XSS(lc + length + 2 + 2*NR)) - length = length + 3 + 2*NR + 2*NE - end do - - ! allocate space for precusor data - allocate(nuc % nu_d_precursor_data(length)) - - ! read delayed neutron precursor data - XSS_index = lc - nuc % nu_d_precursor_data = get_real(length) - - else - nuc % nu_d_type = NU_NONE - nuc % n_precursor = 0 - end if + end associate end subroutine read_nu_data @@ -779,7 +795,7 @@ contains !=============================================================================== subroutine read_reactions(nuc) - type(Nuclide), intent(inout) :: nuc + type(NuclideCE), intent(inout) :: nuc integer :: i ! loop indices integer :: i_fission ! index in nuc % index_fission @@ -792,7 +808,7 @@ contains integer :: LOCA ! location of cross-section for given MT integer :: IE ! reaction's starting index on energy grid integer :: NE ! number of energies - integer :: NR ! number of interpolation regions + real(8) :: y type(ListInt) :: MTs LMT = JXS(3) @@ -811,13 +827,19 @@ contains ! sigma array is not allocated or stored for elastic scattering since it is ! already stored in nuc % elastic associate (rxn => nuc % reactions(1)) - rxn%MT = 2 - rxn%Q_value = ZERO - rxn%multiplicity = 1 - rxn%threshold = 1 - rxn%scatter_in_cm = .true. - allocate(rxn%secondary%distribution(1)) - allocate(UncorrelatedAngleEnergy :: rxn%secondary%distribution(1)%obj) + rxn % MT = 2 + rxn % Q_value = ZERO + allocate(rxn % products(1)) + rxn % products(1) % particle = NEUTRON + allocate(Constant1D :: rxn % products(1) % yield) + select type(yield => rxn % products(1) % yield) + type is (Constant1D) + yield % y = 1 + end select + rxn % threshold = 1 + rxn % scatter_in_cm = .true. + allocate(rxn % products(1) % distribution(1)) + allocate(UncorrelatedAngleEnergy :: rxn % products(1) % distribution(1) % obj) end associate ! Add contribution of elastic scattering to total cross section @@ -833,45 +855,35 @@ contains do i = 1, NMT associate (rxn => nuc % reactions(i+1)) ! read MT number, Q-value, and neutrons produced - rxn % MT = int(XSS(LMT + i - 1)) - rxn % Q_value = XSS(JXS4 + i - 1) - rxn % multiplicity = abs(nint(XSS(JXS5 + i - 1))) + rxn % MT = int(XSS(LMT + i - 1)) + rxn % Q_value = XSS(JXS4 + i - 1) rxn % scatter_in_cm = (nint(XSS(JXS5 + i - 1)) < 0) - ! Read energy-dependent multiplicities - if (rxn % multiplicity > 100) then - ! Set flag and allocate space for Tab1 to store yield - rxn % multiplicity_with_E = .true. - allocate(rxn % multiplicity_E) + if (.not. is_fission(rxn % MT)) then + allocate(rxn % products(1)) + rxn % products(1) % particle = NEUTRON - XSS_index = JXS(11) + rxn % multiplicity - 101 - NR = nint(XSS(XSS_index)) - rxn % multiplicity_E % n_regions = NR + y = abs(nint(XSS(JXS5 + i - 1))) + if (y > 100) then + ! Read energy-dependent multiplicities - ! allocate space for ENDF interpolation parameters - if (NR > 0) then - allocate(rxn % multiplicity_E % nbt(NR)) - allocate(rxn % multiplicity_E % int(NR)) + ! Set flag and allocate space for Tabulated1D to store yield + allocate(Tabulated1D :: rxn % products(1) % yield) + + ! Read yield function + select type (yield => rxn % products(1) % yield) + type is (Tabulated1D) + XSS_index = JXS(11) + int(y) - 101 + call yield % from_ace(XSS, XSS_index) + end select + else + ! Integral yield + allocate(Constant1D :: rxn % products(1) % yield) + select type (yield => rxn % products(1) % yield) + type is (Constant1D) + yield % y = y + end select end if - - ! read ENDF interpolation parameters - XSS_index = XSS_index + 1 - if (NR > 0) then - rxn % multiplicity_E % nbt = get_int(NR) - rxn % multiplicity_E % int = get_int(NR) - end if - - ! allocate space for yield data - XSS_index = XSS_index + 2*NR - NE = nint(XSS(XSS_index)) - rxn % multiplicity_E % n_pairs = NE - allocate(rxn % multiplicity_E % x(NE)) - allocate(rxn % multiplicity_E % y(NE)) - - ! read yield data - XSS_index = XSS_index + 1 - rxn % multiplicity_E % x = get_real(NE) - rxn % multiplicity_E % y = get_real(NE) end if ! read starting energy index @@ -959,7 +971,7 @@ contains !=============================================================================== subroutine read_angular_dist(nuc) - type(Nuclide), intent(inout) :: nuc + type(NuclideCE), intent(inout) :: nuc integer :: LOCB ! location of angular distribution for given MT integer :: NE ! number of incoming energies @@ -988,42 +1000,42 @@ contains ! "one" angular distribution, it is repeated as many times as there are ! energy distributions for this reaction since the ! UncorrelatedAngleEnergy type holds one angle and energy distribution. - do k = 1, size(rxn%secondary%distribution) - select type (aedist => rxn%secondary%distribution(k)%obj) + do k = 1, size(rxn % products(1) % distribution) + select type (aedist => rxn % products(1) % distribution(k) % obj) type is (UncorrelatedAngleEnergy) ! allocate space for incoming energies and locations NE = int(XSS(JXS(9) + LOCB - 1)) - allocate(aedist%angle%energy(NE)) - allocate(aedist%angle%distribution(NE)) + allocate(aedist % angle % energy(NE)) + allocate(aedist % angle % distribution(NE)) allocate(LC(NE)) ! read incoming energy grid and location of nucs XSS_index = JXS(9) + LOCB - aedist%angle%energy(:) = get_real(NE) + aedist % angle % energy(:) = get_real(NE) LC(:) = get_int(NE) ! determine dize of data block do j = 1, NE if (LC(j) == 0) then ! isotropic - allocate(Uniform :: aedist%angle%distribution(j)%obj) - select type (adist => aedist%angle%distribution(j)%obj) + allocate(Uniform :: aedist % angle % distribution(j) % obj) + select type (adist => aedist % angle % distribution(j) % obj) type is (Uniform) - adist%a = -ONE - adist%b = ONE + adist % a = -ONE + adist % b = ONE end select elseif (LC(j) > 0) then ! 32 equiprobable bins - allocate(Equiprobable :: aedist%angle%distribution(j)%obj) - select type (adist => aedist%angle%distribution(j)%obj) + allocate(Equiprobable :: aedist % angle % distribution(j) % obj) + select type (adist => aedist % angle % distribution(j) % obj) type is (Equiprobable) - allocate(adist%x(33)) + allocate(adist % x(33)) end select elseif (LC(j) < 0) then ! tabular distribution - allocate(Tabular :: aedist%angle%distribution(j)%obj) + allocate(Tabular :: aedist % angle % distribution(j) % obj) end if end do @@ -1032,9 +1044,9 @@ contains ! on-the-fly do j = 1, NE XSS_index = JXS(9) + abs(LC(j)) - 1 - select type(adist => aedist%angle%distribution(j)%obj) + select type(adist => aedist % angle % distribution(j) % obj) type is (Equiprobable) - adist%x(:) = get_real(33) + adist % x(:) = get_real(33) type is (Tabular) ! determine interpolation and number of points interp = nint(XSS(XSS_index)) @@ -1042,10 +1054,10 @@ contains ! Get probability density data XSS_index = XSS_index + 2 - allocate(adist%x(NP), adist%p(NP), adist%c(NP)) - adist%x(:) = get_real(NP) - adist%p(:) = get_real(NP) - adist%c(:) = get_real(NP) + allocate(adist % x(NP), adist % p(NP), adist % c(NP)) + adist % x(:) = get_real(NP) + adist % p(:) = get_real(NP) + adist % c(:) = get_real(NP) end select end do deallocate(LC) @@ -1063,7 +1075,7 @@ contains !=============================================================================== subroutine read_energy_dist(nuc) - type(Nuclide), intent(inout) :: nuc + type(NuclideCE), intent(inout) :: nuc integer :: i ! loop index integer :: n @@ -1082,9 +1094,9 @@ contains end do ! Allocate space for distributions and probability of validity - associate (secondary => nuc%reactions(i + 1)%secondary) - allocate(secondary%applicability(n)) - allocate(secondary%distribution(n)) + associate (p => nuc % reactions(i + 1) % products(1)) + allocate(p % applicability(n)) + allocate(p % distribution(n)) LNW = nint(XSS(JXS(10) + i - 1)) n = 0 @@ -1096,11 +1108,11 @@ contains IDAT = nint(XSS(JXS(11) + LNW + 1)) ! Read probability of law validity - call secondary%applicability(n)%from_ace(XSS, JXS(11) + LNW + 2) + call p % applicability(n) % from_ace(XSS, JXS(11) + LNW + 2) ! Read energy law data - call get_energy_dist(secondary%distribution(n)%obj, LAW, & - JXS(11), IDAT, nuc%awr, nuc%reactions(i + 1)%Q_value) + call get_energy_dist(p % distribution(n) % obj, LAW, & + JXS(11), IDAT, nuc % awr, nuc % reactions(i + 1) % Q_value) ! <<<<<<<<<<<<<<<<<<<<<<<<<<<< REMOVE THIS <<<<<<<<<<<<<<<<<<<<<<<<<<< ! Before the secondary distribution refactor, when the angle/energy @@ -1109,11 +1121,11 @@ contains ! distribution even when no angle distribution exists in the ACE file ! (isotropic is assumed). To preserve the RNG stream, we explicitly ! mark fission reactions so that we avoid the angle sampling. - if (any(nuc%reactions(i + 1)%MT == & + if (any(nuc % reactions(i + 1) % MT == & [N_FISSION, N_F, N_NF, N_2NF, N_3NF])) then - select type (aedist => secondary%distribution(n)%obj) + select type (aedist => p % distribution(n) % obj) type is (UncorrelatedAngleEnergy) - aedist%fission = .true. + aedist % fission = .true. end select end if ! <<<<<<<<<<<<<<<<<<<<<<<<<<<< REMOVE THIS <<<<<<<<<<<<<<<<<<<<<<<<<<< @@ -1154,6 +1166,8 @@ contains allocate(KalbachMann :: aedist) elseif (law == 61) then allocate(CorrelatedAngleEnergy :: aedist) + elseif (law == 66) then + allocate(NBodyPhaseSpace :: aedist) else allocate(UncorrelatedAngleEnergy :: aedist) end if @@ -1165,8 +1179,8 @@ contains select case (law) case (1) - allocate(TabularEquiprobable :: aedist%energy) - select type (edist => aedist%energy) + allocate(TabularEquiprobable :: aedist % energy) + select type (edist => aedist % energy) type is (TabularEquiprobable) NR = nint(XSS(XSS_index)) NE = nint(XSS(XSS_index + 1 + 2*NR)) @@ -1174,33 +1188,33 @@ contains call fatal_error("Multiple interpolation regions not yet supported & &for tabular equiprobable energy distributions.") end if - edist%n_region = NR + edist % n_region = NR ! Read incoming energies for which outgoing energies are tabulated - allocate(edist%energy_in(NE)) + allocate(edist % energy_in(NE)) XSS_index = XSS_index + 2 + 2*NR - edist%energy_in(:) = get_real(NE) + edist % energy_in(:) = get_real(NE) ! Read outgoing energy tables NP = nint(XSS(XSS_index)) - allocate(edist%energy_out(NP, NE)) + allocate(edist % energy_out(NP, NE)) XSS_index = XSS_index + 1 do i = 1, NE - edist%energy_out(:, i) = get_real(NP) + edist % energy_out(:, i) = get_real(NP) end do end select case (3) - allocate(LevelInelastic :: aedist%energy) - select type (edist => aedist%energy) + allocate(LevelInelastic :: aedist % energy) + select type (edist => aedist % energy) type is (LevelInelastic) - edist%threshold = XSS(XSS_index) - edist%mass_ratio = XSS(XSS_index + 1) + edist % threshold = XSS(XSS_index) + edist % mass_ratio = XSS(XSS_index + 1) end select case (4) - allocate(ContinuousTabular :: aedist%energy) - select type (edist => aedist%energy) + allocate(ContinuousTabular :: aedist % energy) + select type (edist => aedist % energy) type is (ContinuousTabular) NR = nint(XSS(XSS_index)) XSS_index = XSS_index + 1 @@ -1208,94 +1222,84 @@ contains call fatal_error("Multiple interpolation regions not yet supported & &for continuous tabular energy distributions.") end if - edist%n_region = NR + edist % n_region = NR ! Read breakpoints and interpolation parameters if (NR > 0) then - allocate(edist%breakpoints(NR)) - allocate(edist%interpolation(NR)) - edist%breakpoints(:) = get_int(NR) - edist%interpolation(:) = get_int(NR) + allocate(edist % breakpoints(NR)) + allocate(edist % interpolation(NR)) + edist % breakpoints(:) = get_int(NR) + edist % interpolation(:) = get_int(NR) end if ! Read incoming energies for which outgoing energies are tabulated and ! locators NE = nint(XSS(XSS_index)) XSS_index = XSS_index + 1 - allocate(edist%energy_in(NE)) + allocate(edist % energy(NE)) allocate(L(NE)) - edist%energy_in(:) = get_real(NE) + edist % energy(:) = get_real(NE) L(:) = get_int(NE) ! Read outgoing energy tables - allocate(edist%energy_out(NE)) + allocate(edist % distribution(NE)) do i = 1, NE ! Determine interpolation and number of discrete points XSS_index = LDIS + L(i) - 1 interp = nint(XSS(XSS_index)) - edist%energy_out(i)%interpolation = mod(interp, 10) - edist%energy_out(i)%n_discrete = (interp - & - edist%energy_out(i)%interpolation)/10 + edist % distribution(i) % interpolation = mod(interp, 10) + edist % distribution(i) % n_discrete = (interp - & + edist % distribution(i) % interpolation)/10 ! check for discrete lines present - if (edist%energy_out(i)%n_discrete > 0) then + if (edist % distribution(i) % n_discrete > 0) then call fatal_error("Discrete lines in continuous tabular & &distribution not yet supported") end if ! Determine number of points and allocate space NP = nint(XSS(XSS_index + 1)) - allocate(edist%energy_out(i)%e_out(NP)) - allocate(edist%energy_out(i)%p(NP)) - allocate(edist%energy_out(i)%c(NP)) + allocate(edist % distribution(i) % e_out(NP)) + allocate(edist % distribution(i) % p(NP)) + allocate(edist % distribution(i) % c(NP)) ! Read tabular PDF for outgoing energy XSS_index = XSS_index + 2 - edist%energy_out(i)%e_out(:) = get_real(NP) - edist%energy_out(i)%p(:) = get_real(NP) - edist%energy_out(i)%c(:) = get_real(NP) + edist % distribution(i) % e_out(:) = get_real(NP) + edist % distribution(i) % p(:) = get_real(NP) + edist % distribution(i) % c(:) = get_real(NP) end do deallocate(L) end select case (7) - allocate(MaxwellEnergy :: aedist%energy) - select type (edist => aedist%energy) + allocate(MaxwellEnergy :: aedist % energy) + select type (edist => aedist % energy) type is (MaxwellEnergy) - call edist%theta%from_ace(XSS, XSS_index) - edist%u = XSS(XSS_index + 2 + 2*edist%theta%n_regions + & - 2*edist%theta%n_pairs) + call edist % theta % from_ace(XSS, XSS_index) + edist % u = XSS(XSS_index + 2 + 2*edist % theta % n_regions + & + 2*edist % theta % n_pairs) end select case (9) - allocate(Evaporation :: aedist%energy) - select type(edist => aedist%energy) + allocate(Evaporation :: aedist % energy) + select type(edist => aedist % energy) type is (Evaporation) - call edist%theta%from_ace(XSS, XSS_index) - edist%u = XSS(XSS_index + 2 + 2*edist%theta%n_regions + & - 2*edist%theta%n_pairs) + call edist % theta % from_ace(XSS, XSS_index) + edist % u = XSS(XSS_index + 2 + 2*edist % theta % n_regions + & + 2*edist % theta % n_pairs) end select case (11) - allocate(WattEnergy :: aedist%energy) - select type(edist => aedist%energy) + allocate(WattEnergy :: aedist % energy) + select type(edist => aedist % energy) type is (WattEnergy) - call edist%a%from_ace(XSS, XSS_index) - XSS_index = XSS_index + 2 + 2*edist%a%n_regions + 2*edist%a%n_pairs - call edist%b%from_ace(XSS, XSS_index) - XSS_index = XSS_index + 2 + 2*edist%b%n_regions + 2*edist%b%n_pairs - edist%u = XSS(XSS_index) - end select - - case (66) - allocate(NBodyPhaseSpace :: aedist%energy) - select type(edist => aedist%energy) - type is (NBodyPhaseSpace) - edist%n_bodies = int(XSS(XSS_index)) - edist%mass_ratio = XSS(XSS_index + 1) - edist%A = awr - edist%Q = Q_value + call edist % a % from_ace(XSS, XSS_index) + XSS_index = XSS_index + 2 + 2*edist % a % n_regions + 2*edist % a % n_pairs + call edist % b % from_ace(XSS, XSS_index) + XSS_index = XSS_index + 2 + 2*edist % b % n_regions + 2*edist % b % n_pairs + edist % u = XSS(XSS_index) end select end select @@ -1310,45 +1314,45 @@ contains call fatal_error("Multiple interpolation regions not yet supported & &for Kalbach-Mann energy distributions.") end if - aedist%n_region = NR + aedist % n_region = NR ! Read incoming energies for which outgoing energies are tabulated and locators - allocate(aedist%energy_in(NE)) + allocate(aedist % energy(NE)) allocate(L(NE)) XSS_index = XSS_index + 2 + 2*NR - aedist%energy_in(:) = get_real(NE) + aedist % energy(:) = get_real(NE) L(:) = get_int(NE) ! Read outgoing energy tables - allocate(aedist%table(NE)) + allocate(aedist % distribution(NE)) do i = 1, NE ! Determine interpolation and number of discrete points XSS_index = LDIS + L(i) - 1 interp = nint(XSS(XSS_index)) - aedist%table(i)%interpolation = mod(interp, 10) - aedist%table(i)%n_discrete = (interp - aedist%table(i)%interpolation)/10 + aedist % distribution(i) % interpolation = mod(interp, 10) + aedist % distribution(i) % n_discrete = (interp - aedist % distribution(i) % interpolation)/10 ! check for discrete lines present - if (aedist%table(i)%n_discrete > 0) then + if (aedist % distribution(i) % n_discrete > 0) then call fatal_error("Discrete lines in Kalbach-Mann distribution not & &yet supported") end if ! Determine number of points and allocate space NP = nint(XSS(XSS_index + 1)) - allocate(aedist%table(i)%e_out(NP)) - allocate(aedist%table(i)%p(NP)) - allocate(aedist%table(i)%c(NP)) - allocate(aedist%table(i)%r(NP)) - allocate(aedist%table(i)%a(NP)) + allocate(aedist % distribution(i) % e_out(NP)) + allocate(aedist % distribution(i) % p(NP)) + allocate(aedist % distribution(i) % c(NP)) + allocate(aedist % distribution(i) % r(NP)) + allocate(aedist % distribution(i) % a(NP)) ! Read tabular PDF for outgoing energy XSS_index = XSS_index + 2 - aedist%table(i)%e_out(:) = get_real(NP) - aedist%table(i)%p(:) = get_real(NP) - aedist%table(i)%c(:) = get_real(NP) - aedist%table(i)%r(:) = get_real(NP) - aedist%table(i)%a(:) = get_real(NP) + aedist % distribution(i) % e_out(:) = get_real(NP) + aedist % distribution(i) % p(:) = get_real(NP) + aedist % distribution(i) % c(:) = get_real(NP) + aedist % distribution(i) % r(:) = get_real(NP) + aedist % distribution(i) % a(:) = get_real(NP) end do deallocate(L) @@ -1363,67 +1367,67 @@ contains call fatal_error("Multiple interpolation regions not yet supported & &for correlated angle-energy distributions.") end if - aedist%n_region = NR + aedist % n_region = NR ! Read incoming energies for which outgoing energies are tabulated and ! locators - allocate(aedist%energy_in(NE)) + allocate(aedist % energy(NE)) allocate(L(NE)) XSS_index = XSS_index + 2 + 2*NR - aedist%energy_in(:) = get_real(NE) + aedist % energy(:) = get_real(NE) L(:) = get_int(NE) ! Read outgoing energy tables - allocate(aedist%table(NE)) + allocate(aedist % distribution(NE)) do i = 1, NE ! Determine interpolation and number of discrete points XSS_index = LDIS + L(i) - 1 interp = nint(XSS(XSS_index)) - aedist%table(i)%interpolation = mod(interp, 10) - aedist%table(i)%n_discrete = (interp - aedist%table(i)%interpolation)/10 + aedist % distribution(i) % interpolation = mod(interp, 10) + aedist % distribution(i) % n_discrete = (interp - aedist % distribution(i) % interpolation)/10 ! check for discrete lines present - if (aedist%table(i)%n_discrete > 0) then + if (aedist % distribution(i) % n_discrete > 0) then call fatal_error("Discrete lines in correlated angle-energy & &distribution not yet supported") end if ! Determine number of points and allocate space NP = nint(XSS(XSS_index + 1)) - allocate(aedist%table(i)%e_out(NP)) - allocate(aedist%table(i)%p(NP)) - allocate(aedist%table(i)%c(NP)) + allocate(aedist % distribution(i) % e_out(NP)) + allocate(aedist % distribution(i) % p(NP)) + allocate(aedist % distribution(i) % c(NP)) allocate(LC(NP)) ! Read tabular PDF for outgoing energy XSS_index = XSS_index + 2 - aedist%table(i)%e_out(:) = get_real(NP) - aedist%table(i)%p(:) = get_real(NP) - aedist%table(i)%c(:) = get_real(NP) + aedist % distribution(i) % e_out(:) = get_real(NP) + aedist % distribution(i) % p(:) = get_real(NP) + aedist % distribution(i) % c(:) = get_real(NP) LC(:) = get_int(NP) ! allocate angular distributions for each incoming/outgoing energy - allocate(aedist%table(i)%angle(NP)) + allocate(aedist % distribution(i) % angle(NP)) do j = 1, NP if (LC(j) == 0) then ! isotropic - allocate(Uniform :: aedist%table(i)%angle(j)%obj) - select type (adist => aedist%table(i)%angle(j)%obj) + allocate(Uniform :: aedist % distribution(i) % angle(j) % obj) + select type (adist => aedist % distribution(i) % angle(j) % obj) type is (Uniform) - adist%a = -ONE - adist%b = ONE + adist % a = -ONE + adist % b = ONE end select elseif (LC(j) > 0) then ! tabular distribution - allocate(Tabular :: aedist%table(i)%angle(j)%obj) + allocate(Tabular :: aedist % distribution(i) % angle(j) % obj) end if end do ! read angular distributions do j = 1, NP XSS_index = LDIS + abs(LC(j)) - 1 - select type(adist => aedist%table(i)%angle(j)%obj) + select type(adist => aedist % distribution(i) % angle(j) % obj) type is (Tabular) ! determine interpolation and number of points interp = nint(XSS(XSS_index)) @@ -1431,10 +1435,10 @@ contains ! Get probability density data XSS_index = XSS_index + 2 - allocate(adist%x(NP), adist%p(NP), adist%c(NP)) - adist%x(:) = get_real(NP) - adist%p(:) = get_real(NP) - adist%c(:) = get_real(NP) + allocate(adist % x(NP), adist % p(NP), adist % c(NP)) + adist % x(:) = get_real(NP) + adist % p(:) = get_real(NP) + adist % c(:) = get_real(NP) end select end do deallocate(LC) @@ -1442,6 +1446,15 @@ contains end do deallocate(L) + + type is (NBodyPhaseSpace) + ! ======================================================================== + ! N-BODY PHASE SPACE DISTRIBUTION + + aedist % n_bodies = int(XSS(XSS_index)) + aedist % mass_ratio = XSS(XSS_index + 1) + aedist % A = awr + aedist % Q = Q_value end select end subroutine get_energy_dist @@ -1451,7 +1464,7 @@ contains !=============================================================================== subroutine read_unr_res(nuc) - type(Nuclide), intent(inout) :: nuc + type(NuclideCE), intent(inout) :: nuc integer :: JXS23 ! location of URR data integer :: lc ! locator @@ -1531,7 +1544,6 @@ contains end if end subroutine read_unr_res - !=============================================================================== ! GENERATE_NU_FISSION precalculates the microscopic nu-fission cross section for ! a given nuclide. This is done so that the nu_total function does not need to @@ -1539,23 +1551,14 @@ contains !=============================================================================== subroutine generate_nu_fission(nuc) - type(Nuclide), intent(inout) :: nuc + type(NuclideCE), intent(inout) :: nuc integer :: i ! index on nuclide energy grid - real(8) :: E ! energy - real(8) :: nu ! # of neutrons per fission - do i = 1, nuc % n_grid - ! determine energy - E = nuc % energy(i) - - ! determine total nu at given energy - nu = nu_total(nuc, E) - - ! determine nu-fission microscopic cross section - nuc % nu_fission(i) = nu * nuc % fission(i) + do i = 1, size(nuc % energy) + nuc % nu_fission(i) = nuc % nu(nuc % energy(i), EMISSION_TOTAL) * & + nuc % fission(i) end do - end subroutine generate_nu_fission !=============================================================================== @@ -1732,26 +1735,4 @@ contains end function get_real -!=============================================================================== -! SAME_NUCLIDE_LIST creates a linked list for each nuclide containing the -! indices in the nuclides array of all other instances of that nuclide. For -! example, the same nuclide may exist at multiple temperatures resulting -! in multiple entries in the nuclides array for a single zaid number. -!=============================================================================== - - subroutine same_nuclide_list() - - integer :: i ! index in nuclides array - integer :: j ! index in nuclides array - - do i = 1, n_nuclides_total - do j = 1, n_nuclides_total - if (nuclides(i) % zaid == nuclides(j) % zaid) then - call nuclides(i) % nuc_list % push_back(j) - end if - end do - end do - - end subroutine same_nuclide_list - end module ace diff --git a/src/ace_header.F90 b/src/ace_header.F90 deleted file mode 100644 index 1dfa06872..000000000 --- a/src/ace_header.F90 +++ /dev/null @@ -1,298 +0,0 @@ -module ace_header - - use constants, only: MAX_FILE_LEN, ZERO - use dict_header, only: DictIntInt - use endf_header, only: Tab1 - use multipole_header, only: MultipoleArray - use secondary_header, only: SecondaryDistribution, AngleEnergyContainer - use stl_vector, only: VectorInt - - implicit none - -!=============================================================================== -! REACTION contains the cross-section and secondary energy and angle -! distributions for a single reaction in a continuous-energy ACE-format table -!=============================================================================== - - type Reaction - integer :: MT ! ENDF MT value - real(8) :: Q_value ! Reaction Q value - integer :: multiplicity ! Number of secondary particles released - type(Tab1), pointer :: multiplicity_E => null() ! Energy-dependent neutron yield - integer :: threshold ! Energy grid index of threshold - logical :: scatter_in_cm ! scattering system in center-of-mass? - logical :: multiplicity_with_E = .false. ! Flag to indicate E-dependent multiplicity - real(8), allocatable :: sigma(:) ! Cross section values - type(SecondaryDistribution) :: secondary - - ! Type-Bound procedures - contains - procedure :: clear => reaction_clear ! Deallocates Reaction - end type Reaction - -!=============================================================================== -! URRDATA contains probability tables for the unresolved resonance range. -!=============================================================================== - - type UrrData - integer :: n_energy ! # of incident neutron energies - integer :: n_prob ! # of probabilities - integer :: interp ! inteprolation (2=lin-lin, 5=log-log) - integer :: inelastic_flag ! inelastic competition flag - integer :: absorption_flag ! other absorption flag - logical :: multiply_smooth ! multiply by smooth cross section? - real(8), allocatable :: energy(:) ! incident energies - real(8), allocatable :: prob(:,:,:) ! actual probabibility tables - end type UrrData - -!=============================================================================== -! NUCLIDE contains all the data for an ACE-format continuous-energy cross -! section. The ACE format (A Compact ENDF format) is used in MCNP and several -! other Monte Carlo codes. -!=============================================================================== - - type Nuclide - character(10) :: name ! name of nuclide, e.g. 92235.03c - integer :: zaid ! Z and A identifier, e.g. 92235 - integer :: listing ! index in xs_listings - real(8) :: awr ! weight of nucleus in neutron masses - real(8) :: kT ! temperature in MeV (k*T) - - ! Linked list of indices in nuclides array of instances of this same nuclide - type(VectorInt) :: nuc_list - - ! Energy grid information - integer :: n_grid ! # of nuclide grid points - integer, allocatable :: grid_index(:) ! log grid mapping indices - real(8), allocatable :: energy(:) ! energy values corresponding to xs - - ! Microscopic cross sections - real(8), allocatable :: total(:) ! total cross section - real(8), allocatable :: elastic(:) ! elastic scattering - real(8), allocatable :: fission(:) ! fission - real(8), allocatable :: nu_fission(:) ! neutron production - real(8), allocatable :: absorption(:) ! absorption (MT > 100) - real(8), allocatable :: heating(:) ! heating - - ! Resonance scattering info - logical :: resonant = .false. ! resonant scatterer? - character(10) :: name_0K = '' ! name of 0K nuclide, e.g. 92235.00c - character(16) :: scheme ! target velocity sampling scheme - integer :: n_grid_0K ! number of 0K energy grid points - real(8), allocatable :: energy_0K(:) ! energy grid for 0K xs - real(8), allocatable :: elastic_0K(:) ! Microscopic elastic cross section - real(8), allocatable :: xs_cdf(:) ! CDF of v_rel times cross section - real(8) :: E_min ! lower cutoff energy for res scattering - real(8) :: E_max ! upper cutoff energy for res scattering - - ! Fission information - logical :: fissionable ! nuclide is fissionable? - logical :: has_partial_fission ! nuclide has partial fission reactions? - integer :: n_fission ! # of fission reactions - integer, allocatable :: index_fission(:) ! indices in reactions - - ! Total fission neutron emission - integer :: nu_t_type - real(8), allocatable :: nu_t_data(:) - - ! Prompt fission neutron emission - integer :: nu_p_type - real(8), allocatable :: nu_p_data(:) - - ! Delayed fission neutron emission - integer :: nu_d_type - integer :: n_precursor ! # of delayed neutron precursors - real(8), allocatable :: nu_d_data(:) - real(8), allocatable :: nu_d_precursor_data(:) - type(AngleEnergyContainer), allocatable :: nu_d_edist(:) - - ! Unresolved resonance data - logical :: urr_present - integer :: urr_inelastic - type(UrrData), pointer :: urr_data => null() - - ! Multipole data - logical :: mp_present = .false. - type(MultipoleArray), pointer :: multipole => null() - - ! Reactions - integer :: n_reaction ! # of reactions - type(Reaction), allocatable :: reactions(:) - type(DictIntInt) :: reaction_index ! map MT values to index in reactions - ! array; used at tally-time - - ! Type-Bound procedures - contains - procedure :: clear => nuclide_clear ! Deallocates Nuclide - end type Nuclide - -!=============================================================================== -! NUCLIDE0K temporarily contains all 0K cross section data and other parameters -! needed to treat resonance scattering before transferring them to NUCLIDE -!=============================================================================== - - type Nuclide0K - character(10) :: nuclide ! name of nuclide, e.g. U-238 - character(16) :: scheme = 'ares' ! target velocity sampling scheme - character(10) :: name ! name of nuclide, e.g. 92235.03c - character(10) :: name_0K ! name of 0K nuclide, e.g. 92235.00c - real(8) :: E_min = 0.01e-6_8 ! lower cutoff energy for res scattering - real(8) :: E_max = 1000.0e-6_8 ! upper cutoff energy for res scattering - end type Nuclide0K - -!=============================================================================== -! DISTENERGYSAB contains the secondary energy/angle distributions for inelastic -! thermal scattering collisions which utilize a continuous secondary energy -! representation. -!=============================================================================== - - type DistEnergySab - integer :: n_e_out - real(8), allocatable :: e_out(:) - real(8), allocatable :: e_out_pdf(:) - real(8), allocatable :: e_out_cdf(:) - real(8), allocatable :: mu(:,:) - end type DistEnergySab - -!=============================================================================== -! SALPHABETA contains S(a,b) data for thermal neutron scattering, typically off -! of light isotopes such as water, graphite, Be, etc -!=============================================================================== - - type SAlphaBeta - character(10) :: name ! name of table, e.g. lwtr.10t - real(8) :: awr ! weight of nucleus in neutron masses - real(8) :: kT ! temperature in MeV (k*T) - integer :: n_zaid ! Number of valid zaids - integer, allocatable :: zaid(:) ! List of valid Z and A identifiers, e.g. 6012 - - ! threshold for S(a,b) treatment (usually ~4 eV) - real(8) :: threshold_inelastic - real(8) :: threshold_elastic = ZERO - - ! Inelastic scattering data - integer :: n_inelastic_e_in ! # of incoming E for inelastic - integer :: n_inelastic_e_out ! # of outgoing E for inelastic - integer :: n_inelastic_mu ! # of outgoing angles for inelastic - integer :: secondary_mode ! secondary mode (equal/skewed/continuous) - real(8), allocatable :: inelastic_e_in(:) - real(8), allocatable :: inelastic_sigma(:) - ! The following are used only if secondary_mode is 0 or 1 - real(8), allocatable :: inelastic_e_out(:,:) - real(8), allocatable :: inelastic_mu(:,:,:) - ! The following is used only if secondary_mode is 3 - ! The different implementation is necessary because the continuous - ! representation has a variable number of outgoing energy points for each - ! incoming energy - type(DistEnergySab), allocatable :: inelastic_data(:) ! One for each Ein - - ! Elastic scattering data - integer :: elastic_mode ! elastic mode (discrete/exact) - integer :: n_elastic_e_in ! # of incoming E for elastic - integer :: n_elastic_mu ! # of outgoing angles for elastic - real(8), allocatable :: elastic_e_in(:) - real(8), allocatable :: elastic_P(:) - real(8), allocatable :: elastic_mu(:,:) - end type SAlphaBeta - -!=============================================================================== -! XSLISTING contains data read from a cross_sections.xml file -!=============================================================================== - - type XsListing - character(12) :: name ! table name, e.g. 92235.70c - character(12) :: alias ! table alias, e.g. U-235.70c - integer :: type ! type of table (cont-E neutron, S(A,b), etc) - integer :: zaid ! ZAID identifier = 1000*Z + A - integer :: filetype ! ASCII or BINARY - integer :: location ! location of table within library - integer :: recl ! record length for library - integer :: entries ! number of entries per record - real(8) :: awr ! atomic weight ratio (# of neutron masses) - real(8) :: kT ! Boltzmann constant * temperature (MeV) - logical :: metastable ! is this nuclide metastable? - character(MAX_FILE_LEN) :: path ! path to library containing table - end type XsListing - -!=============================================================================== -! NUCLIDEMICROXS contains cached microscopic cross sections for a -! particular nuclide at the current energy -!=============================================================================== - - type NuclideMicroXS - integer :: index_grid ! index on nuclide energy grid - integer :: index_temp ! temperature index for nuclide - real(8) :: last_E = ZERO ! last evaluated energy - real(8) :: interp_factor ! interpolation factor on nuc. energy grid - real(8) :: total ! microscropic total xs - real(8) :: elastic ! microscopic elastic scattering xs - real(8) :: absorption ! microscopic absorption xs - real(8) :: fission ! microscopic fission xs - real(8) :: nu_fission ! microscopic production xs - - ! Information for S(a,b) use - integer :: index_sab ! index in sab_tables (zero means no table) - integer :: last_index_sab = 0 ! index in sab_tables last used by this nuclide - real(8) :: elastic_sab ! microscopic elastic scattering on S(a,b) table - - ! Information for URR probability table use - logical :: use_ptable ! in URR range with probability tables? - real(8) :: last_prn - - ! Information for Doppler broadening - real(8) :: last_sqrtkT = ZERO ! last temperature in sqrt(Boltzmann constant * temperature (MeV)) - end type NuclideMicroXS - -!=============================================================================== -! MATERIALMACROXS contains cached macroscopic cross sections for the material a -! particle is traveling through -!=============================================================================== - - type MaterialMacroXS - real(8) :: total ! macroscopic total xs - real(8) :: elastic ! macroscopic elastic scattering xs - real(8) :: absorption ! macroscopic absorption xs - real(8) :: fission ! macroscopic fission xs - real(8) :: nu_fission ! macroscopic production xs - end type MaterialMacroXS - - contains - -!=============================================================================== -! REACTION_CLEAR resets and deallocates data in Reaction. -!=============================================================================== - - subroutine reaction_clear(this) - class(Reaction), intent(inout) :: this ! The Reaction object to clear - - if (associated(this % multiplicity_E)) deallocate(this % multiplicity_E) - end subroutine reaction_clear - -!=============================================================================== -! NUCLIDE_CLEAR resets and deallocates data in Nuclide. -!=============================================================================== - - subroutine nuclide_clear(this) - class(Nuclide), intent(inout) :: this - - integer :: i ! Loop counter - - if (associated(this % urr_data)) deallocate(this % urr_data) - - if (this % mp_present) then - deallocate(this % multipole) - end if - - if (allocated(this % reactions)) then - do i = 1, size(this % reactions) - call this % reactions(i) % clear() - end do - end if - - call this % reaction_index % clear() - - if (associated(this % multipole)) deallocate(this % multipole) - - end subroutine nuclide_clear - -end module ace_header diff --git a/src/angleenergy_header.F90 b/src/angleenergy_header.F90 new file mode 100644 index 000000000..483bad856 --- /dev/null +++ b/src/angleenergy_header.F90 @@ -0,0 +1,29 @@ +module angleenergy_header + +!=============================================================================== +! ANGLEENERGY (abstract) defines a correlated or uncorrelated angle-energy +! distribution that is a function of incoming energy. Each derived type must +! implement a sample() subroutine that returns an outgoing energy and scattering +! cosine given an incoming energy. +!=============================================================================== + + type, abstract :: AngleEnergy + contains + procedure(angleenergy_sample_), deferred :: sample + end type AngleEnergy + + abstract interface + subroutine angleenergy_sample_(this, E_in, E_out, mu) + import AngleEnergy + class(AngleEnergy), intent(in) :: this + real(8), intent(in) :: E_in + real(8), intent(out) :: E_out + real(8), intent(out) :: mu + end subroutine angleenergy_sample_ + end interface + + type :: AngleEnergyContainer + class(AngleEnergy), allocatable :: obj + end type AngleEnergyContainer + +end module angleenergy_header diff --git a/src/bank_header.F90 b/src/bank_header.F90 index 0cb49af35..97fb1f11f 100644 --- a/src/bank_header.F90 +++ b/src/bank_header.F90 @@ -14,7 +14,7 @@ module bank_header real(C_DOUBLE) :: wgt ! weight of bank site real(C_DOUBLE) :: xyz(3) ! location of bank particle real(C_DOUBLE) :: uvw(3) ! diretional cosines - real(C_DOUBLE) :: E ! energy + real(C_DOUBLE) :: E ! energy / energy group if in MG mode. integer(C_INT) :: delayed_group ! delayed group end type Bank diff --git a/src/cmfd_data.F90 b/src/cmfd_data.F90 index 19fe39572..347351e31 100644 --- a/src/cmfd_data.F90 +++ b/src/cmfd_data.F90 @@ -49,13 +49,13 @@ contains subroutine compute_xs() - use constants, only: FILTER_MESH, FILTER_ENERGYIN, FILTER_ENERGYOUT, & - FILTER_SURFACE, IN_RIGHT, OUT_RIGHT, IN_FRONT, & - OUT_FRONT, IN_TOP, OUT_TOP, CMFD_NOACCEL, ZERO, & - ONE, TINY_BIT + use constants, only: FILTER_MESH, FILTER_ENERGYIN, FILTER_ENERGYOUT, & + FILTER_SURFACE, IN_RIGHT, OUT_RIGHT, IN_FRONT, & + OUT_FRONT, IN_TOP, OUT_TOP, CMFD_NOACCEL, ZERO, & + ONE, TINY_BIT use error, only: fatal_error use global, only: cmfd, n_cmfd_tallies, cmfd_tallies, meshes,& - matching_bins + matching_bins use mesh, only: mesh_indices_to_bin use mesh_header, only: RegularMesh use string, only: to_str @@ -625,10 +625,10 @@ contains subroutine compute_dhat() - use constants, only: CMFD_NOACCEL, ZERO - use global, only: cmfd, cmfd_coremap, dhat_reset - use output, only: write_message - use string, only: to_str + use constants, only: CMFD_NOACCEL, ZERO + use global, only: cmfd, cmfd_coremap, dhat_reset + use output, only: write_message + use string, only: to_str integer :: nx ! maximum number of cells in x direction integer :: ny ! maximum number of cells in y direction diff --git a/src/cmfd_execute.F90 b/src/cmfd_execute.F90 index 4dfe99d77..b7d0cc387 100644 --- a/src/cmfd_execute.F90 +++ b/src/cmfd_execute.F90 @@ -89,9 +89,9 @@ contains subroutine calc_fission_source() - use constants, only: CMFD_NOACCEL, ZERO, TWO - use global, only: cmfd, cmfd_coremap, master, entropy_on, current_batch - use string, only: to_str + use constants, only: CMFD_NOACCEL, ZERO, TWO + use global, only: cmfd, cmfd_coremap, master, entropy_on, current_batch + use string, only: to_str #ifdef MPI use global, only: mpi_err diff --git a/src/cmfd_input.F90 b/src/cmfd_input.F90 index dac74c9c3..f69c09fe1 100644 --- a/src/cmfd_input.F90 +++ b/src/cmfd_input.F90 @@ -45,14 +45,14 @@ contains subroutine read_cmfd_xml() use constants, only: ZERO, ONE - use error, only: fatal_error, warning + use error, only: fatal_error, warning use global - use output, only: write_message - use string, only: to_lower + use output, only: write_message + use string, only: to_lower use xml_interface use, intrinsic :: ISO_FORTRAN_ENV - integer :: i + integer :: i, g integer :: ng integer :: n_params integer, allocatable :: iarray(:) @@ -70,7 +70,7 @@ contains inquire(FILE=filename, EXIST=file_exists) if (.not. file_exists) then ! CMFD is optional unless it is in on from settings - if (cmfd_on) then + if (cmfd_run) then call fatal_error("No CMFD XML file, '" // trim(filename) // "' does not& & exist!") end if @@ -102,6 +102,23 @@ contains if(.not.allocated(cmfd%egrid)) allocate(cmfd%egrid(ng)) call get_node_array(node_mesh, "energy", cmfd%egrid) cmfd % indices(4) = ng - 1 ! sets energy group dimension + ! If using MG mode, check to see if these egrid points at least match + ! the MG Data breakpoints + if (.not. run_CE) then + do i = 1, ng + found = .false. + do g = 1, energy_groups + 1 + if (cmfd % egrid(i) == energy_bins(g)) then + found = .true. + exit + end if + end do + if (.not. found) then + call fatal_error("CMFD energy mesh boundaries must align with& + & boundaries of multi-group data!") + end if + end do + end if else if(.not.allocated(cmfd % egrid)) allocate(cmfd % egrid(2)) cmfd % egrid = [ ZERO, 20.0_8 ] diff --git a/src/constants.F90 b/src/constants.F90 index bdd8c041d..0998a87c1 100644 --- a/src/constants.F90 +++ b/src/constants.F90 @@ -11,10 +11,10 @@ module constants integer, parameter :: VERSION_RELEASE = 1 ! Revision numbers for binary files - integer, parameter :: REVISION_STATEPOINT = 14 + integer, parameter :: REVISION_STATEPOINT = 15 integer, parameter :: REVISION_PARTICLE_RESTART = 1 integer, parameter :: REVISION_TRACK = 1 - integer, parameter :: REVISION_SUMMARY = 2 + integer, parameter :: REVISION_SUMMARY = 3 ! ============================================================================ ! ADJUSTABLE PARAMETERS @@ -163,9 +163,14 @@ module constants ! Angular distribution type integer, parameter :: & - ANGLE_ISOTROPIC = 1, & ! Isotropic angular distribution - ANGLE_32_EQUI = 2, & ! 32 equiprobable bins - ANGLE_TABULAR = 3 ! Tabular angular distribution + ANGLE_ISOTROPIC = 1, & ! Isotropic angular distribution (CE) + ANGLE_32_EQUI = 2, & ! 32 equiprobable bins (CE) + ANGLE_TABULAR = 3, & ! Tabular angular distribution (CE or MG) + ANGLE_LEGENDRE = 4, & ! Legendre angular distribution (MG) + ANGLE_HISTOGRAM = 5 ! Histogram angular distribution (MG) + + ! Number of mu bins to use when converting Legendres to tabular type + integer, parameter :: DEFAULT_NMU = 33 ! Secondary energy mode for S(a,b) inelastic scattering integer, parameter :: & @@ -209,12 +214,23 @@ module constants ACE_THERMAL = 2, & ! thermal S(a,b) scattering data ACE_DOSIMETRY = 3 ! dosimetry cross sections + ! MGXS Table Types + integer, parameter :: & + MGXS_ISOTROPIC = 1, & ! Isotropically Weighted Data + MGXS_ANGLE = 2 ! Data by Angular Bins + ! Fission neutron emission (nu) type integer, parameter :: & NU_NONE = 0, & ! No nu values (non-fissionable) NU_POLYNOMIAL = 1, & ! Nu values given by polynomial NU_TABULAR = 2 ! Nu values given by tabular distribution + ! Secondary particle emission type + integer, parameter :: & + EMISSION_PROMPT = 1, & ! Prompt emission of secondary particle + EMISSION_DELAYED = 2, & ! Delayed emission of secondary particle + EMISSION_TOTAL = 3 ! Yield represents total emission (prompt + delayed) + ! Cross section filetypes integer, parameter :: & ASCII = 1, & ! ASCII cross section file @@ -363,10 +379,11 @@ module constants ! ============================================================================ ! RANDOM NUMBER STREAM CONSTANTS - integer, parameter :: N_STREAMS = 3 - integer, parameter :: STREAM_TRACKING = 1 - integer, parameter :: STREAM_TALLIES = 2 - integer, parameter :: STREAM_SOURCE = 3 + integer, parameter :: N_STREAMS = 4 + integer, parameter :: STREAM_TRACKING = 1 + integer, parameter :: STREAM_TALLIES = 2 + integer, parameter :: STREAM_SOURCE = 3 + integer, parameter :: STREAM_URR_PTABLE = 4 ! ============================================================================ ! MISCELLANEOUS CONSTANTS diff --git a/src/cross_section.F90 b/src/cross_section.F90 index 0a61373e2..8d1eb6898 100644 --- a/src/cross_section.F90 +++ b/src/cross_section.F90 @@ -1,31 +1,23 @@ module cross_section - use ace_header, only: Nuclide, SAlphaBeta, Reaction, UrrData use constants use energy_grid, only: grid_method, log_spacing use error, only: fatal_error - use fission, only: nu_total use global use list_header, only: ListElemInt use material_header, only: Material - use math, only: w, w_derivative, broaden_n_polynomials + use math, only: faddeeva, w_derivative, broaden_wmp_polynomials use multipole_header, only: FORM_RM, FORM_MLBW, MP_EA, RM_RT, RM_RA, RM_RF, & - MLBW_RT, MLBW_RX, MLBW_RA, MLBW_RF, FIT_T, FIT_A, FIT_F, & - MultipoleArray, max_poly, max_L, max_poles + MLBW_RT, MLBW_RX, MLBW_RA, MLBW_RF, FIT_T, FIT_A,& + FIT_F, MultipoleArray + use nuclide_header use particle_header, only: Particle - use random_lcg, only: prn + use random_lcg, only: prn, future_prn, prn_set_stream + use sab_header, only: SAlphaBeta use search, only: binary_search implicit none - ! Allocatable arrays for multipole that are allocated once for speed purposes - complex(8), allocatable :: sigT_factor(:) - real(8), allocatable :: twophi(:) - real(8), allocatable :: broadened_polynomials(:) - logical :: mp_already_alloc = .false. - -!$omp threadprivate(sigT_factor, twophi, broadened_polynomials, mp_already_alloc) - contains !=============================================================================== @@ -164,8 +156,8 @@ contains integer :: i_high ! upper logarithmic mapping index real(8) :: f ! interp factor on nuclide energy grid real(8) :: sigT, sigA, sigF ! Intermediate multipole variables - type(Nuclide), pointer :: nuc - type(Material), pointer :: mat + type(NuclideCE), pointer :: nuc + type(Material), pointer :: mat ! Set pointer to nuclide and material nuc => nuclides(i_nuclide) @@ -185,7 +177,7 @@ contains if (nuc % fissionable) then micro_xs(i_nuclide) % fission = sigF - micro_xs(i_nuclide) % nu_fission = sigF * nu_total(nuc, E) + micro_xs(i_nuclide) % nu_fission = sigF * nuc % nu(E, EMISSION_TOTAL) else micro_xs(i_nuclide) % fission = ZERO micro_xs(i_nuclide) % nu_fission = ZERO @@ -403,154 +395,136 @@ contains integer, intent(in) :: i_nuclide ! index into nuclides array real(8), intent(in) :: E ! energy - integer :: i ! loop index integer :: i_energy ! index for energy integer :: i_low ! band index at lower bounding energy integer :: i_up ! band index at upper bounding energy - integer :: same_nuc_idx ! index of same nuclide real(8) :: f ! interpolation factor real(8) :: r ! pseudo-random number real(8) :: elastic ! elastic cross section real(8) :: capture ! (n,gamma) cross section real(8) :: fission ! fission cross section real(8) :: inelastic ! inelastic cross section - logical :: same_nuc ! do we know the xs for this nuclide at this energy? - type(UrrData), pointer :: urr - type(Nuclide), pointer :: nuc micro_xs(i_nuclide) % use_ptable = .true. - ! get pointer to probability table - nuc => nuclides(i_nuclide) - urr => nuc % urr_data + associate (nuc => nuclides(i_nuclide), urr => nuclides(i_nuclide) % urr_data) + ! determine energy table + i_energy = 1 + do + if (E < urr % energy(i_energy + 1)) exit + i_energy = i_energy + 1 + end do - ! determine energy table - i_energy = 1 - do - if (E < urr % energy(i_energy + 1)) exit - i_energy = i_energy + 1 - end do + ! determine interpolation factor on table + f = (E - urr % energy(i_energy)) / & + (urr % energy(i_energy + 1) - urr % energy(i_energy)) - ! determine interpolation factor on table - f = (E - urr % energy(i_energy)) / & - (urr % energy(i_energy + 1) - urr % energy(i_energy)) + ! sample probability table using the cumulative distribution - ! sample probability table using the cumulative distribution + ! Random numbers for xs calculation are sampled from a separated stream. + ! This guarantees the randomness and, at the same time, makes sure we reuse + ! random number for the same nuclide at different temperatures, therefore + ! preserving correlation of temperature in probability tables. + call prn_set_stream(STREAM_URR_PTABLE) + r = future_prn(int(nuc_zaid_dict % get_key(nuc % zaid), 8)) + call prn_set_stream(STREAM_TRACKING) - ! if we're dealing with a nuclide that we've previously encountered at - ! this energy but a different temperature, use the original random number to - ! preserve correlation of temperature in probability tables - same_nuc = .false. - do i = 1, nuc % nuc_list % size() - if (E /= ZERO .and. E == micro_xs(nuc % nuc_list % data(i)) % last_E) then - same_nuc = .true. - same_nuc_idx = i - exit - end if - end do + i_low = 1 + do + if (urr % prob(i_energy, URR_CUM_PROB, i_low) > r) exit + i_low = i_low + 1 + end do + i_up = 1 + do + if (urr % prob(i_energy + 1, URR_CUM_PROB, i_up) > r) exit + i_up = i_up + 1 + end do - if (same_nuc) then - r = micro_xs(nuc % nuc_list % data(same_nuc_idx)) % last_prn - else - r = prn() - micro_xs(i_nuclide) % last_prn = r - end if + ! determine elastic, fission, and capture cross sections from probability + ! table + if (urr % interp == LINEAR_LINEAR) then + elastic = (ONE - f) * urr % prob(i_energy, URR_ELASTIC, i_low) + & + f * urr % prob(i_energy + 1, URR_ELASTIC, i_up) + fission = (ONE - f) * urr % prob(i_energy, URR_FISSION, i_low) + & + f * urr % prob(i_energy + 1, URR_FISSION, i_up) + capture = (ONE - f) * urr % prob(i_energy, URR_N_GAMMA, i_low) + & + f * urr % prob(i_energy + 1, URR_N_GAMMA, i_up) + elseif (urr % interp == LOG_LOG) then + ! Get logarithmic interpolation factor + f = log(E / urr % energy(i_energy)) / & + log(urr % energy(i_energy + 1) / urr % energy(i_energy)) - i_low = 1 - do - if (urr % prob(i_energy, URR_CUM_PROB, i_low) > r) exit - i_low = i_low + 1 - end do - i_up = 1 - do - if (urr % prob(i_energy + 1, URR_CUM_PROB, i_up) > r) exit - i_up = i_up + 1 - end do - - ! determine elastic, fission, and capture cross sections from probability - ! table - if (urr % interp == LINEAR_LINEAR) then - elastic = (ONE - f) * urr % prob(i_energy, URR_ELASTIC, i_low) + & - f * urr % prob(i_energy + 1, URR_ELASTIC, i_up) - fission = (ONE - f) * urr % prob(i_energy, URR_FISSION, i_low) + & - f * urr % prob(i_energy + 1, URR_FISSION, i_up) - capture = (ONE - f) * urr % prob(i_energy, URR_N_GAMMA, i_low) + & - f * urr % prob(i_energy + 1, URR_N_GAMMA, i_up) - elseif (urr % interp == LOG_LOG) then - ! Get logarithmic interpolation factor - f = log(E / urr % energy(i_energy)) / & - log(urr % energy(i_energy + 1) / urr % energy(i_energy)) - - ! Calculate elastic cross section/factor - elastic = ZERO - if (urr % prob(i_energy, URR_ELASTIC, i_low) > ZERO .and. & - urr % prob(i_energy + 1, URR_ELASTIC, i_up) > ZERO) then - elastic = exp((ONE - f) * log(urr % prob(i_energy, URR_ELASTIC, & - i_low)) + f * log(urr % prob(i_energy + 1, URR_ELASTIC, & - i_up))) - end if - - ! Calculate fission cross section/factor - fission = ZERO - if (urr % prob(i_energy, URR_FISSION, i_low) > ZERO .and. & - urr % prob(i_energy + 1, URR_FISSION, i_up) > ZERO) then - fission = exp((ONE - f) * log(urr % prob(i_energy, URR_FISSION, & - i_low)) + f * log(urr % prob(i_energy + 1, URR_FISSION, & - i_up))) - end if - - ! Calculate capture cross section/factor - capture = ZERO - if (urr % prob(i_energy, URR_N_GAMMA, i_low) > ZERO .and. & - urr % prob(i_energy + 1, URR_N_GAMMA, i_up) > ZERO) then - capture = exp((ONE - f) * log(urr % prob(i_energy, URR_N_GAMMA, & - i_low)) + f * log(urr % prob(i_energy + 1, URR_N_GAMMA, & - i_up))) - end if - end if - - ! Determine treatment of inelastic scattering - inelastic = ZERO - if (urr % inelastic_flag > 0) then - ! Get index on energy grid and interpolation factor - i_energy = micro_xs(i_nuclide) % index_grid - f = micro_xs(i_nuclide) % interp_factor - - ! Determine inelastic scattering cross section - associate (rxn => nuc % reactions(nuc % urr_inelastic)) - if (i_energy >= rxn % threshold) then - inelastic = (ONE - f) * rxn % sigma(i_energy - rxn%threshold + 1) + & - f * rxn % sigma(i_energy - rxn%threshold + 2) + ! Calculate elastic cross section/factor + elastic = ZERO + if (urr % prob(i_energy, URR_ELASTIC, i_low) > ZERO .and. & + urr % prob(i_energy + 1, URR_ELASTIC, i_up) > ZERO) then + elastic = exp((ONE - f) * log(urr % prob(i_energy, URR_ELASTIC, & + i_low)) + f * log(urr % prob(i_energy + 1, URR_ELASTIC, & + i_up))) end if - end associate - end if - ! Multiply by smooth cross-section if needed - if (urr % multiply_smooth) then - elastic = elastic * micro_xs(i_nuclide) % elastic - capture = capture * (micro_xs(i_nuclide) % absorption - & - micro_xs(i_nuclide) % fission) - fission = fission * micro_xs(i_nuclide) % fission - end if + ! Calculate fission cross section/factor + fission = ZERO + if (urr % prob(i_energy, URR_FISSION, i_low) > ZERO .and. & + urr % prob(i_energy + 1, URR_FISSION, i_up) > ZERO) then + fission = exp((ONE - f) * log(urr % prob(i_energy, URR_FISSION, & + i_low)) + f * log(urr % prob(i_energy + 1, URR_FISSION, & + i_up))) + end if - ! Check for negative values - if (elastic < ZERO) elastic = ZERO - if (fission < ZERO) fission = ZERO - if (capture < ZERO) capture = ZERO + ! Calculate capture cross section/factor + capture = ZERO + if (urr % prob(i_energy, URR_N_GAMMA, i_low) > ZERO .and. & + urr % prob(i_energy + 1, URR_N_GAMMA, i_up) > ZERO) then + capture = exp((ONE - f) * log(urr % prob(i_energy, URR_N_GAMMA, & + i_low)) + f * log(urr % prob(i_energy + 1, URR_N_GAMMA, & + i_up))) + end if + end if - ! Set elastic, absorption, fission, and total cross sections. Note that the - ! total cross section is calculated as sum of partials rather than using the - ! table-provided value - micro_xs(i_nuclide) % elastic = elastic - micro_xs(i_nuclide) % absorption = capture + fission - micro_xs(i_nuclide) % fission = fission - micro_xs(i_nuclide) % total = elastic + inelastic + capture + fission + ! Determine treatment of inelastic scattering + inelastic = ZERO + if (urr % inelastic_flag > 0) then + ! Get index on energy grid and interpolation factor + i_energy = micro_xs(i_nuclide) % index_grid + f = micro_xs(i_nuclide) % interp_factor - ! Determine nu-fission cross section - if (nuc % fissionable) then - micro_xs(i_nuclide) % nu_fission = nu_total(nuc, E) * & - micro_xs(i_nuclide) % fission - end if + ! Determine inelastic scattering cross section + associate (rxn => nuc % reactions(nuc % urr_inelastic)) + if (i_energy >= rxn % threshold) then + inelastic = (ONE - f) * rxn % sigma(i_energy - rxn%threshold + 1) + & + f * rxn % sigma(i_energy - rxn%threshold + 2) + end if + end associate + end if + + ! Multiply by smooth cross-section if needed + if (urr % multiply_smooth) then + elastic = elastic * micro_xs(i_nuclide) % elastic + capture = capture * (micro_xs(i_nuclide) % absorption - & + micro_xs(i_nuclide) % fission) + fission = fission * micro_xs(i_nuclide) % fission + end if + + ! Check for negative values + if (elastic < ZERO) elastic = ZERO + if (fission < ZERO) fission = ZERO + if (capture < ZERO) capture = ZERO + + ! Set elastic, absorption, fission, and total cross sections. Note that the + ! total cross section is calculated as sum of partials rather than using the + ! table-provided value + micro_xs(i_nuclide) % elastic = elastic + micro_xs(i_nuclide) % absorption = capture + fission + micro_xs(i_nuclide) % fission = fission + micro_xs(i_nuclide) % total = elastic + inelastic + capture + fission + + ! Determine nu-fission cross section + if (nuc % fissionable) then + micro_xs(i_nuclide) % nu_fission = nuc % nu(E, EMISSION_TOTAL) * & + micro_xs(i_nuclide) % fission + end if + end associate end subroutine calculate_urr_xs @@ -576,19 +550,6 @@ contains end function find_energy_index -!=============================================================================== -! MULTIPOLE_EVAL_ALLOCATE allocates fixed-length arrays that vary based on -! what nuclides are loaded into the problem -!=============================================================================== - - subroutine multipole_eval_allocate() - allocate(sigT_factor(max_L)) - allocate(twophi(max_L)) - allocate(broadened_polynomials(max_poly)) - - mp_already_alloc = .true. - end subroutine - !=============================================================================== ! MULTIPOLE_EVAL evaluates the windowed multipole equations for cross ! sections in the resolved resonance regions @@ -606,128 +567,121 @@ contains real(8), intent(out) :: sigT ! Total cross section real(8), intent(out) :: sigA ! Absorption cross section real(8), intent(out) :: sigF ! Fission cross section - complex(8) :: psi_ki ! The value of the psi-ki function for the asymptotic - ! form + complex(8) :: psi_chi ! The value of the psi-chi function for the + ! asymptotic form complex(8) :: c_temp ! complex temporary variable complex(8) :: w_val ! The faddeeva function evaluated at Z complex(8) :: Z ! sqrt(atomic weight ratio / kT) * (sqrt(E) - pole) + complex(8) :: sigT_factor(multipole % num_l) + real(8) :: broadened_polynomials(multipole % fit_order + 1) real(8) :: sqrtE ! sqrt(E), eV real(8) :: invE ! 1/E, eV - real(8) :: dopp ! sqrt(atomic weight ratio / kT) - real(8) :: dopp_ecoef ! sqrt(atomic weight ratio * pi / kT) / E + real(8) :: dopp ! sqrt(atomic weight ratio / kT) = 1 / (2 sqrt(xi)) real(8) :: temp ! real temporary value real(8) :: E ! energy, eV real(8) :: sqrtkT ! sqrt(kT (in eV)) - integer :: iP ! index of pole - integer :: iC ! index of curvefit - integer :: iW ! index of window + integer :: i_pole ! index of pole + integer :: i_poly ! index of curvefit + integer :: i_window ! index of window integer :: startw ! window start pointer (for poles) - integer :: startw_1 ! window start pointer - 1 - integer :: startw_endw ! window start pointer - window end pointer integer :: endw ! window end pointer - ! Convert to eV + ! ========================================================================== + ! Bookkeeping + + ! Convert to eV. E = Emev * 1.0e6_8 sqrtkT = sqrtkT_ * 1.0e3_8 + ! Define some frequently used variables. sqrtE = sqrt(E) - invE = ONE/E + invE = ONE / E + dopp = multipole % sqrtAWR / sqrtkT - if(.not. mp_already_alloc) then - call multipole_eval_allocate() - end if + ! Locate us. + i_window = floor((sqrtE - sqrt(multipole % start_E)) / multipole % spacing & + + ONE) + startw = multipole % w_start(i_window) + endw = multipole % w_end(i_window) - ! Locate us - iW = floor((sqrtE - sqrt(multipole % start_E))/multipole % spacing + ONE) - - startw = multipole % w_start(iW) - startw_1 = startw - 1 ! This is an index shift parameter. - endw = multipole % w_end(iW) - startw_endw = endw - startw + 1 - - ! Fill in factors + ! Fill in factors. if (startw <= endw) then - call fill_factors(multipole, sqrtE, sigT_factor, twophi, multipole % num_l) + call compute_sigT_factor(multipole, sqrtE, sigT_factor) end if - ! Generate some doppler broadening parameters - - ! dopp_ecoef is inverse of dopp, divided by E, multiplied by sqrt(pi). - dopp = multipole % sqrtAWR / sqrtKT - dopp_ecoef = dopp * invE * SQRT_PI - + ! Initialize the ouptut cross sections. sigT = ZERO sigA = ZERO sigF = ZERO - ! Evaluate linefit first - if(sqrtkT /= 0 .and. multipole % broaden_poly(iW) == 1) then ! Broaden the curvefit. - call broaden_n_polynomials(E, dopp, multipole % fit_order + 1, broadened_polynomials) + ! ========================================================================== + ! Add the contribution from the curvefit polynomial. - do iC = 1, multipole % fit_order+1 - sigT = sigT + multipole % curvefit(FIT_T, iC, iW)*broadened_polynomials(iC) - sigA = sigA + multipole % curvefit(FIT_A, iC, iW)*broadened_polynomials(iC) - if (multipole % fissionable) then - sigF = sigF + multipole % curvefit(FIT_F, iC, iW)*broadened_polynomials(iC) - end if + if (sqrtkT /= ZERO .and. multipole % broaden_poly(i_window) == 1) then + ! Broaden the curvefit. + call broaden_wmp_polynomials(E, dopp, multipole % fit_order + 1, & + broadened_polynomials) + do i_poly = 1, multipole % fit_order+1 + sigT = sigT + multipole % curvefit(FIT_T, i_poly, i_window) & + * broadened_polynomials(i_poly) + sigA = sigA + multipole % curvefit(FIT_A, i_poly, i_window) & + * broadened_polynomials(i_poly) + sigF = sigF + multipole % curvefit(FIT_F, i_poly, i_window) & + * broadened_polynomials(i_poly) end do else ! Evaluate as if it were a polynomial temp = invE - do iC = 1, multipole % fit_order+1 - - sigT = sigT + multipole % curvefit(FIT_T, iC, iW)*temp - sigA = sigA + multipole % curvefit(FIT_A, iC, iW)*temp - if (multipole % fissionable) then - sigF = sigF + multipole % curvefit(FIT_F, iC, iW)*temp - end if - + do i_poly = 1, multipole % fit_order+1 + sigT = sigT + multipole % curvefit(FIT_T, i_poly, i_window) * temp + sigA = sigA + multipole % curvefit(FIT_A, i_poly, i_window) * temp + sigF = sigF + multipole % curvefit(FIT_F, i_poly, i_window) * temp temp = temp * sqrtE end do end if - ! Then get the poles we want and broaden them. + ! ========================================================================== + ! Add the contribution from the poles in this window. if (sqrtkT == ZERO) then ! If at 0K, use asymptotic form. - do iP = startw, endw - psi_ki = -ONEI/(multipole % data(MP_EA, iP) - sqrtE) - c_temp = psi_ki/E + do i_pole = startw, endw + psi_chi = -ONEI / (multipole % data(MP_EA, i_pole) - sqrtE) + c_temp = psi_chi / E if (multipole % formalism == FORM_MLBW) then - sigT = sigT + real(multipole % data(MLBW_RT, iP) * c_temp * & - sigT_factor(multipole % l_value(iP))) & - + real(multipole % data(MLBW_RX, iP) * c_temp) - sigA = sigA + real(multipole % data(MLBW_RA, iP) * c_temp) - sigF = sigF + real(multipole % data(MLBW_RF, iP) * c_temp) + sigT = sigT + real(multipole % data(MLBW_RT, i_pole) * c_temp * & + sigT_factor(multipole % l_value(i_pole))) & + + real(multipole % data(MLBW_RX, i_pole) * c_temp) + sigA = sigA + real(multipole % data(MLBW_RA, i_pole) * c_temp) + sigF = sigF + real(multipole % data(MLBW_RF, i_pole) * c_temp) else if (multipole % formalism == FORM_RM) then - sigT = sigT + real(multipole % data(RM_RT, iP) * c_temp* & - sigT_factor(multipole % l_value(iP))) - sigA = sigA + real(multipole % data(RM_RA, iP) * c_temp) - sigF = sigF + real(multipole % data(RM_RF, iP) * c_temp) + sigT = sigT + real(multipole % data(RM_RT, i_pole) * c_temp * & + sigT_factor(multipole % l_value(i_pole))) + sigA = sigA + real(multipole % data(RM_RA, i_pole) * c_temp) + sigF = sigF + real(multipole % data(RM_RF, i_pole) * c_temp) end if end do else ! At temperature, use Faddeeva function-based form. - if(endw >= startw) then - do iP = startw, endw - Z = (sqrtE - multipole % data(MP_EA, iP)) * dopp - w_val = w(Z) * dopp_ecoef - + if (endw >= startw) then + do i_pole = startw, endw + Z = (sqrtE - multipole % data(MP_EA, i_pole)) * dopp + w_val = faddeeva(Z) * dopp * invE * SQRT_PI if (multipole % formalism == FORM_MLBW) then - sigT = sigT + real((multipole % data(MLBW_RT, iP) * & - sigT_factor(multipole%l_value(iP)) + & - multipole % data(MLBW_RX, iP)) * w_val) - sigA = sigA + real(multipole % data(MLBW_RA, iP) * w_val) - sigF = sigF + real(multipole % data(MLBW_RF, iP) * w_val) + sigT = sigT + real((multipole % data(MLBW_RT, i_pole) * & + sigT_factor(multipole % l_value(i_pole)) + & + multipole % data(MLBW_RX, i_pole)) * w_val) + sigA = sigA + real(multipole % data(MLBW_RA, i_pole) * w_val) + sigF = sigF + real(multipole % data(MLBW_RF, i_pole) * w_val) else if (multipole % formalism == FORM_RM) then - sigT = sigT + real(multipole % data(RM_RT, iP) * w_val * & - sigT_factor(multipole % l_value(iP))) - sigA = sigA + real(multipole % data(RM_RA, iP) * w_val) - sigF = sigF + real(multipole % data(RM_RF, iP) * w_val) + sigT = sigT + real(multipole % data(RM_RT, i_pole) * w_val * & + sigT_factor(multipole % l_value(i_pole))) + sigA = sigA + real(multipole % data(RM_RA, i_pole) * w_val) + sigF = sigF + real(multipole % data(RM_RF, i_pole) * w_val) end if end do end if end if - end subroutine + end subroutine multipole_eval !=============================================================================== ! MULTIPOLE_DERIV_EVAL evaluates the windowed multipole equations for the @@ -776,82 +730,72 @@ contains real(8), intent(out) :: sigT ! Total cross section real(8), intent(out) :: sigA ! Absorption cross section real(8), intent(out) :: sigF ! Fission cross section - complex(8) :: psi_ki ! The value of the psi-ki function for the asymptotic - ! form - complex(8) :: c_temp ! complex temporary variable complex(8) :: w_val ! The faddeeva function evaluated at Z complex(8) :: Z ! sqrt(atomic weight ratio / kT) * (sqrt(E) - pole) + complex(8) :: sigT_factor(multipole % num_l) real(8) :: sqrtE ! sqrt(E), eV real(8) :: invE ! 1/E, eV real(8) :: dopp ! sqrt(atomic weight ratio / kT) - real(8) :: dopp_ecoef ! sqrt(atomic weight ratio * pi / kT) / E - real(8) :: temp ! real temporary value real(8) :: E ! energy, eV real(8) :: sqrtkT ! sqrt(kT (in eV)) - integer :: iP ! index of pole - integer :: iC ! index of curvefit - integer :: iW ! index of window + integer :: i_pole ! index of pole + integer :: i_window ! index of window integer :: startw ! window start pointer (for poles) - integer :: startw_1 ! window start pointer - 1 - integer :: startw_endw ! window start pointer - window end pointer integer :: endw ! window end pointer real(8) :: T - ! Convert to eV + ! ========================================================================== + ! Bookkeeping + + ! Convert to eV. E = Emev * 1.0e6_8 sqrtkT = sqrtkT_ * 1.0e3_8 + ! Define some frequently used variables. + sqrtE = sqrt(E) + invE = ONE / E + dopp = multipole % sqrtAWR / sqrtkT T = sqrtkT_**2 / K_BOLTZMANN if (sqrtkT == ZERO) call fatal_error("Windowed multipole temperature & &derivatives are not implemented for 0 Kelvin cross sections.") - sqrtE = sqrt(E) - invE = ONE/E - - if(.not. mp_already_alloc) then - call multipole_eval_allocate() - end if - ! Locate us - iW = floor((sqrtE - sqrt(multipole % start_E))/multipole % spacing + ONE) + i_window = floor((sqrtE - sqrt(multipole % start_E)) / multipole % spacing & + + ONE) + startw = multipole % w_start(i_window) + endw = multipole % w_end(i_window) - startw = multipole % w_start(iW) - startw_1 = startw - 1 ! This is an index shift parameter. - endw = multipole % w_end(iW) - startw_endw = endw - startw + 1 - - ! Fill in factors + ! Fill in factors. if (startw <= endw) then - call fill_factors(multipole, sqrtE, sigT_factor, twophi, multipole % num_l) + call compute_sigT_factor(multipole, sqrtE, sigT_factor) end if - ! dopp_ecoef is inverse of dopp, divided by E, multiplied by sqrt(pi). - dopp = multipole % sqrtAWR / sqrtKT - dopp_ecoef = dopp * invE * SQRT_PI - + ! Initialize the ouptut cross sections. sigT = ZERO sigA = ZERO sigF = ZERO ! TODO Polynomials - if (endw >= startw) then - do iP = startw, endw - Z = (sqrtE - multipole % data(MP_EA, iP)) * dopp - w_val = -invE * SQRT_PI * HALF * w_derivative(Z, 2) + ! ========================================================================== + ! Add the contribution from the poles in this window. + if (endw >= startw) then + do i_pole = startw, endw + Z = (sqrtE - multipole % data(MP_EA, i_pole)) * dopp + w_val = -invE * SQRT_PI * HALF * w_derivative(Z, 2) if (multipole % formalism == FORM_MLBW) then - sigT = sigT + real((multipole % data(MLBW_RT, iP) * & - sigT_factor(multipole%l_value(iP)) + & - multipole % data(MLBW_RX, iP)) * w_val) - sigA = sigA + real(multipole % data(MLBW_RA, iP) * w_val) - sigF = sigF + real(multipole % data(MLBW_RF, iP) * w_val) + sigT = sigT + real((multipole % data(MLBW_RT, i_pole) * & + sigT_factor(multipole%l_value(i_pole)) + & + multipole % data(MLBW_RX, i_pole)) * w_val) + sigA = sigA + real(multipole % data(MLBW_RA, i_pole) * w_val) + sigF = sigF + real(multipole % data(MLBW_RF, i_pole) * w_val) else if (multipole % formalism == FORM_RM) then - sigT = sigT + real(multipole % data(RM_RT, iP) * w_val * & - sigT_factor(multipole % l_value(iP))) - sigA = sigA + real(multipole % data(RM_RA, iP) * w_val) - sigF = sigF + real(multipole % data(RM_RF, iP) * w_val) + sigT = sigT + real(multipole % data(RM_RT, i_pole) * w_val * & + sigT_factor(multipole % l_value(i_pole))) + sigA = sigA + real(multipole % data(RM_RA, i_pole) * w_val) + sigF = sigF + real(multipole % data(RM_RF, i_pole) * w_val) end if end do sigT = -HALF*multipole % sqrtAWR / sqrt(K_BOLTZMANN*1.0e6_8) * T**(-1.5)& @@ -864,22 +808,20 @@ contains end subroutine multipole_deriv_eval !=============================================================================== -! FILL_FACTORS calculates the value of phi, the hardsphere phase shift factor, -! and sigT_factor, a factor inside of the sigT equation not present in the -! sigA and sigF equations. +! COMPUTE_SIGT_FACTOR calculates the sigT_factor, a factor inside of the sigT +! equation not present in the sigA and sigF equations. !=============================================================================== - subroutine fill_factors(multipole, sqrtE, sigT_factor, twophi, max_L) - type(MultipoleArray), intent(in) :: multipole - real(8), intent(in) :: sqrtE - integer, intent(in) :: max_L - complex(8), intent(out) :: sigT_factor(max_L) - real(8), intent(out) :: twophi(max_L) + subroutine compute_sigT_factor(multipole, sqrtE, sigT_factor) + type(MultipoleArray), intent(in) :: multipole + real(8), intent(in) :: sqrtE + complex(8), intent(out) :: sigT_factor(multipole % num_l) integer :: iL + real(8) :: twophi(multipole % num_l) real(8) :: arg - do iL = 1, max_L + do iL = 1, multipole % num_l twophi(iL) = multipole % pseudo_k0RS(iL) * sqrtE if (iL == 2) then twophi(iL) = twophi(iL) - atan(twophi(iL)) @@ -887,14 +829,15 @@ contains arg = 3.0_8 * twophi(iL) / (3.0_8 - twophi(iL)**2) twophi(iL) = twophi(iL) - atan(arg) else if (iL == 4) then - arg = twophi(iL) * (15.0_8 - twophi(iL)**2) / (15.0_8 - 6.0_8 * twophi(iL)**2) + arg = twophi(iL) * (15.0_8 - twophi(iL)**2) & + / (15.0_8 - 6.0_8 * twophi(iL)**2) twophi(iL) = twophi(iL) - atan(arg) end if end do twophi = 2.0_8 * twophi - sigT_factor = cmplx(cos(twophi),-sin(twophi), KIND=8) - end subroutine + sigT_factor = cmplx(cos(twophi), -sin(twophi), KIND=8) + end subroutine compute_sigT_factor !=============================================================================== ! 0K_ELASTIC_XS determines the microscopic 0K elastic cross section @@ -902,9 +845,9 @@ contains !=============================================================================== pure function elastic_xs_0K(E, nuc) result(xs_out) - real(8), intent(in) :: E ! trial energy - type(Nuclide), intent(in) :: nuc ! target nuclide at temperature - real(8) :: xs_out ! 0K xs at trial energy + real(8), intent(in) :: E ! trial energy + type(NuclideCE), intent(in) :: nuc ! target nuclide at temperature + real(8) :: xs_out ! 0K xs at trial energy integer :: i_grid ! index on nuclide energy grid real(8) :: f ! interp factor on nuclide energy grid diff --git a/src/distribution_multivariate.F90 b/src/distribution_multivariate.F90 index c288c40c1..68b246df8 100644 --- a/src/distribution_multivariate.F90 +++ b/src/distribution_multivariate.F90 @@ -1,9 +1,9 @@ module distribution_multivariate - use constants, only: ONE, TWO, PI + use constants, only: ONE, TWO, PI use distribution_univariate, only: Distribution - use math, only: rotate_angle - use random_lcg, only: prn + use random_lcg, only: prn + use math, only: rotate_angle implicit none @@ -16,15 +16,15 @@ module distribution_multivariate type, abstract :: UnitSphereDistribution real(8) :: reference_uvw(3) contains - procedure(iSample), deferred :: sample + procedure(unitsphere_distribution_sample_), deferred :: sample end type UnitSphereDistribution abstract interface - function iSample(this) result(uvw) + function unitsphere_distribution_sample_(this) result(uvw) import UnitSphereDistribution class(UnitSphereDistribution), intent(in) :: this real(8) :: uvw(3) - end function iSample + end function unitsphere_distribution_sample_ end interface !=============================================================================== @@ -58,15 +58,15 @@ module distribution_multivariate type, abstract :: SpatialDistribution contains - procedure(iSampleSpatial), deferred :: sample + procedure(spatial_distribution_sample_), deferred :: sample end type SpatialDistribution abstract interface - function iSampleSpatial(this) result(xyz) + function spatial_distribution_sample_(this) result(xyz) import SpatialDistribution class(SpatialDistribution), intent(in) :: this real(8) :: xyz(3) - end function iSampleSpatial + end function spatial_distribution_sample_ end interface type, extends(SpatialDistribution) :: CartesianIndependent diff --git a/src/distribution_univariate.F90 b/src/distribution_univariate.F90 index f596536d0..6c053e594 100644 --- a/src/distribution_univariate.F90 +++ b/src/distribution_univariate.F90 @@ -1,11 +1,11 @@ module distribution_univariate - use constants, only: ZERO, ONE, HALF, HISTOGRAM, LINEAR_LINEAR, & + use constants, only: ZERO, ONE, HALF, HISTOGRAM, LINEAR_LINEAR, & MAX_LINE_LEN, MAX_WORD_LEN - use error, only: fatal_error - use math, only: maxwell_spectrum, watt_spectrum + use error, only: fatal_error use random_lcg, only: prn - use string, only: to_lower + use math, only: maxwell_spectrum, watt_spectrum + use string, only: to_lower use xml_interface implicit none @@ -16,7 +16,7 @@ module distribution_univariate type, abstract :: Distribution contains - procedure(iSample), deferred :: sample + procedure(distribution_sample_), deferred :: sample end type Distribution type DistributionContainer @@ -24,11 +24,11 @@ module distribution_univariate end type DistributionContainer abstract interface - function iSample(this) result(x) + function distribution_sample_(this) result(x) import Distribution class(Distribution), intent(in) :: this real(8) :: x - end function iSample + end function distribution_sample_ end interface !=============================================================================== diff --git a/src/eigenvalue.F90 b/src/eigenvalue.F90 index 403347caa..9befbe3c3 100644 --- a/src/eigenvalue.F90 +++ b/src/eigenvalue.F90 @@ -4,16 +4,15 @@ module eigenvalue use message_passing #endif - use constants, only: ZERO - use error, only: fatal_error, warning + use constants, only: ZERO + use error, only: fatal_error, warning use global - use math, only: t_percentile - use mesh, only: count_bank_sites - use mesh_header, only: RegularMesh - use particle_header, only: Particle - use random_lcg, only: prn, set_particle_seed, prn_skip - use search, only: binary_search - use string, only: to_str + use math, only: t_percentile + use mesh, only: count_bank_sites + use mesh_header, only: RegularMesh + use random_lcg, only: prn, set_particle_seed, advance_prn_seed + use search, only: binary_search + use string, only: to_str implicit none @@ -100,7 +99,7 @@ contains call set_particle_seed(int((current_batch - 1)*gen_per_batch + & current_gen,8)) - call prn_skip(start) + call advance_prn_seed(start) ! Determine how many fission sites we need to sample from the source bank ! and the probability for selecting a site. diff --git a/src/endf_header.F90 b/src/endf_header.F90 index 7388ea2f5..e9a073f4e 100644 --- a/src/endf_header.F90 +++ b/src/endf_header.F90 @@ -1,12 +1,51 @@ module endf_header - implicit none + use constants, only: ZERO, HISTOGRAM, LINEAR_LINEAR, LINEAR_LOG, & + LOG_LINEAR, LOG_LOG + use search, only: binary_search + +implicit none + + type, abstract :: Function1D + contains + procedure(function1d_evaluate_), deferred :: evaluate + end type Function1D + + abstract interface + pure function function1d_evaluate_(this, x) result(y) + import Function1D + class(Function1D), intent(in) :: this + real(8), intent(in) :: x + real(8) :: y + end function function1d_evaluate_ + end interface !=============================================================================== -! TAB1 represents a one-dimensional interpolable function +! CONSTANT1D represents a constant one-dimensional function !=============================================================================== - type Tab1 + type, extends(Function1D) :: Constant1D + real(8) :: y + contains + procedure :: evaluate => constant1d_evaluate + end type Constant1D + +!=============================================================================== +! POLYNOMIAL represents a one-dimensional function expressed as a polynomial +!=============================================================================== + + type, extends(Function1D) :: Polynomial + real(8), allocatable :: coef(:) ! coefficients + contains + procedure :: evaluate => polynomial_evaluate + procedure :: from_ace => polynomial_from_ace + end type Polynomial + +!=============================================================================== +! TABULATED1D represents a one-dimensional interpolable function +!=============================================================================== + + type, extends(Function1D) :: Tabulated1D integer :: n_regions = 0 ! # of interpolation regions integer, allocatable :: nbt(:) ! values separating interpolation regions integer, allocatable :: int(:) ! interpolation scheme @@ -14,18 +53,78 @@ module endf_header real(8), allocatable :: x(:) ! values of abscissa real(8), allocatable :: y(:) ! values of ordinate contains - procedure :: from_ace - end type Tab1 + procedure :: from_ace => tabulated1d_from_ace + procedure :: evaluate => tabulated1d_evaluate + end type Tabulated1D contains - subroutine from_ace(this, xss, idx) - class(Tab1), intent(inout) :: this +!=============================================================================== +! Constant1D implementation +!=============================================================================== + + pure function constant1d_evaluate(this, x) result(y) + class(Constant1D), intent(in) :: this + real(8), intent(in) :: x + real(8) :: y + + y = this % y + end function constant1d_evaluate + +!=============================================================================== +! Polynomial implementation +!=============================================================================== + + subroutine polynomial_from_ace(this, xss, idx) + class(Polynomial), intent(inout) :: this + real(8), intent(in) :: xss(:) + integer, intent(in) :: idx + + integer :: nc ! number of coefficients (order - 1) + + ! Clear space + if (allocated(this % coef)) deallocate(this % coef) + + ! Determine number of coefficients + nc = nint(xss(idx)) + + ! Allocate space for and read coefficients + allocate(this % coef(nc)) + this % coef(:) = xss(idx + 1 : idx + nc) + end subroutine polynomial_from_ace + + pure function polynomial_evaluate(this, x) result(y) + class(Polynomial), intent(in) :: this + real(8), intent(in) :: x + real(8) :: y + + integer :: i + + ! Use Horner's rule to evaluate polynomial. Note that coefficients are + ! ordered in increasing powers of x. + y = ZERO + do i = size(this % coef), 1, -1 + y = y*x + this % coef(i) + end do + end function polynomial_evaluate + +!=============================================================================== +! Tabulated1D implementation +!=============================================================================== + + subroutine tabulated1d_from_ace(this, xss, idx) + class(Tabulated1D), intent(inout) :: this real(8), intent(in) :: xss(:) integer, intent(in) :: idx integer :: nr, ne + ! Clear space + if (allocated(this % nbt)) deallocate(this % nbt) + if (allocated(this % int)) deallocate(this % int) + if (allocated(this % x)) deallocate(this % x) + if (allocated(this % y)) deallocate(this % y) + ! Determine number of regions nr = nint(xss(idx)) this%n_regions = nr @@ -47,6 +146,81 @@ contains allocate(this%y(ne)) this%x(:) = xss(idx + 2*nr + 2 : idx + 2*nr + 1 + ne) this%y(:) = xss(idx + 2*nr + 2 + ne : idx + 2*nr + 1 + 2*ne) - end subroutine from_ace + end subroutine tabulated1d_from_ace + + pure function tabulated1d_evaluate(this, x) result(y) + class(Tabulated1D), intent(in) :: this + real(8), intent(in) :: x ! x value to find y at + real(8) :: y ! y(x) + + integer :: i ! bin in which to interpolate + integer :: j ! index for interpolation region + integer :: n_regions ! number of interpolation regions + integer :: n_pairs ! number of tabulated values + integer :: interp ! ENDF interpolation scheme + real(8) :: r ! interpolation factor + real(8) :: x0, x1 ! bounding x values + real(8) :: y0, y1 ! bounding y values + + ! determine number of interpolation regions and pairs + n_regions = this % n_regions + n_pairs = this % n_pairs + + ! find which bin the abscissa is in -- if the abscissa is outside the + ! tabulated range, the first or last point is chosen, i.e. no interpolation + ! is done outside the energy range + if (x < this % x(1)) then + y = this % y(1) + return + elseif (x > this % x(n_pairs)) then + y = this % y(n_pairs) + return + else + i = binary_search(this % x, n_pairs, x) + end if + + ! determine interpolation scheme + if (n_regions == 0) then + interp = LINEAR_LINEAR + elseif (n_regions == 1) then + interp = this % int(1) + elseif (n_regions > 1) then + do j = 1, n_regions + if (i < this % nbt(j)) then + interp = this % int(j) + exit + end if + end do + end if + + ! handle special case of histogram interpolation + if (interp == HISTOGRAM) then + y = this % y(i) + return + end if + + ! determine bounding values + x0 = this % x(i) + x1 = this % x(i + 1) + y0 = this % y(i) + y1 = this % y(i + 1) + + ! determine interpolation factor and interpolated value + select case (interp) + case (LINEAR_LINEAR) + r = (x - x0)/(x1 - x0) + y = y0 + r*(y1 - y0) + case (LINEAR_LOG) + r = log(x/x0)/log(x1/x0) + y = y0 + r*(y1 - y0) + case (LOG_LINEAR) + r = (x - x0)/(x1 - x0) + y = y0*exp(r*log(y1/y0)) + case (LOG_LOG) + r = log(x/x0)/log(x1/x0) + y = y0*exp(r*log(y1/y0)) + end select + + end function tabulated1d_evaluate end module endf_header diff --git a/src/energy_distribution.F90 b/src/energy_distribution.F90 index db3dcc441..3a42bb73d 100644 --- a/src/energy_distribution.F90 +++ b/src/energy_distribution.F90 @@ -1,11 +1,10 @@ module energy_distribution - use constants, only: ZERO, ONE, TWO, PI, HISTOGRAM, LINEAR_LINEAR - use endf_header, only: Tab1 - use interpolation, only: interpolate_tab1 - use math, only: maxwell_spectrum, watt_spectrum - use random_lcg, only: prn - use search, only: binary_search + use constants, only: ZERO, ONE, TWO, PI, HISTOGRAM, LINEAR_LINEAR + use endf_header, only: Tabulated1D + use math, only: maxwell_spectrum, watt_spectrum + use random_lcg, only: prn + use search, only: binary_search !=============================================================================== ! ENERGYDISTRIBUTION (abstract) defines an energy distribution that is a @@ -16,16 +15,16 @@ module energy_distribution type, abstract :: EnergyDistribution contains - procedure(iSampleEnergy), deferred :: sample + procedure(energy_distribution_sample_), deferred :: sample end type EnergyDistribution abstract interface - function iSampleEnergy(this, E_in) result(E_out) + function energy_distribution_sample_(this, E_in) result(E_out) import EnergyDistribution class(EnergyDistribution), intent(in) :: this real(8), intent(in) :: E_in real(8) :: E_out - end function iSampleEnergy + end function energy_distribution_sample_ end interface type :: EnergyDistributionContainer @@ -83,8 +82,8 @@ module energy_distribution integer :: n_region integer, allocatable :: breakpoints(:) integer, allocatable :: interpolation(:) - real(8), allocatable :: energy_in(:) - type(CTTable), allocatable :: energy_out(:) + real(8), allocatable :: energy(:) + type(CTTable), allocatable :: distribution(:) contains procedure :: sample => continuous_sample end type ContinuousTabular @@ -95,7 +94,7 @@ module energy_distribution !=============================================================================== type, extends(EnergyDistribution) :: MaxwellEnergy - type(Tab1) :: theta ! incoming-energy-dependent parameter + type(Tabulated1D) :: theta ! incoming-energy-dependent parameter real(8) :: u ! restriction energy contains procedure :: sample => maxwellenergy_sample @@ -107,7 +106,7 @@ module energy_distribution !=============================================================================== type, extends(EnergyDistribution) :: Evaporation - type(Tab1) :: theta + type(Tabulated1D) :: theta real(8) :: u contains procedure :: sample => evaporation_sample @@ -119,28 +118,13 @@ module energy_distribution !=============================================================================== type, extends(EnergyDistribution) :: WattEnergy - type(Tab1) :: a - type(Tab1) :: b + type(Tabulated1D) :: a + type(Tabulated1D) :: b real(8) :: u contains procedure :: sample => watt_sample end type WattEnergy -!=============================================================================== -! NBODYPHASESPACE gives the energy distribution for particles emitted from -! neutron and charged-particle reactions. This corresponds to ACE law 66 and -! ENDF File 6, LAW=6. -!=============================================================================== - - type, extends(EnergyDistribution) :: NBodyPhaseSpace - integer :: n_bodies - real(8) :: mass_ratio - real(8) :: A - real(8) :: Q - contains - procedure :: sample => nbody_sample - end type NBodyPhaseSpace - contains function equiprobable_sample(this, E_in) result(E_out) @@ -202,6 +186,7 @@ contains end if end function equiprobable_sample + function level_inelastic_sample(this, E_in) result(E_out) class(LevelInelastic), intent(in) :: this real(8), intent(in) :: E_in @@ -210,6 +195,7 @@ contains E_out = this%mass_ratio*(E_in - this%threshold) end function level_inelastic_sample + function continuous_sample(this, E_in) result(E_out) class(ContinuousTabular), intent(in) :: this real(8), intent(in) :: E_in ! incoming energy @@ -238,17 +224,17 @@ contains ! Find energy bin and calculate interpolation factor -- if the energy is ! outside the range of the tabulated energies, choose the first or last bins - n_energy_in = size(this%energy_in) - if (E_in < this%energy_in(1)) then + n_energy_in = size(this%energy) + if (E_in < this%energy(1)) then i = 1 r = ZERO - elseif (E_in > this%energy_in(n_energy_in)) then + elseif (E_in > this%energy(n_energy_in)) then i = n_energy_in - 1 r = ONE else - i = binary_search(this%energy_in, n_energy_in, E_in) - r = (E_in - this%energy_in(i)) / & - (this%energy_in(i+1) - this%energy_in(i)) + i = binary_search(this%energy, n_energy_in, E_in) + r = (E_in - this%energy(i)) / & + (this%energy(i+1) - this%energy(i)) end if ! Sample between the ith and (i+1)th bin @@ -263,23 +249,23 @@ contains end if ! Interpolation for energy E1 and EK - n_energy_out = size(this%energy_out(i)%e_out) - E_i_1 = this%energy_out(i)%e_out(1) - E_i_K = this%energy_out(i)%e_out(n_energy_out) + n_energy_out = size(this%distribution(i)%e_out) + E_i_1 = this%distribution(i)%e_out(1) + E_i_K = this%distribution(i)%e_out(n_energy_out) - n_energy_out = size(this%energy_out(i+1)%e_out) - E_i1_1 = this%energy_out(i+1)%e_out(1) - E_i1_K = this%energy_out(i+1)%e_out(n_energy_out) + n_energy_out = size(this%distribution(i+1)%e_out) + E_i1_1 = this%distribution(i+1)%e_out(1) + E_i1_K = this%distribution(i+1)%e_out(n_energy_out) E_1 = E_i_1 + r*(E_i1_1 - E_i_1) E_K = E_i_K + r*(E_i1_K - E_i_K) ! Determine outgoing energy bin - n_energy_out = size(this%energy_out(l)%e_out) + n_energy_out = size(this%distribution(l)%e_out) r1 = prn() - c_k = this%energy_out(l)%c(1) + c_k = this%distribution(l)%c(1) do k = 1, n_energy_out - 1 - c_k1 = this%energy_out(l)%c(k+1) + c_k1 = this%distribution(l)%c(k+1) if (r1 < c_k1) exit c_k = c_k1 end do @@ -287,9 +273,9 @@ contains ! Check to make sure k is <= NP - 1 k = min(k, n_energy_out - 1) - E_l_k = this%energy_out(l)%e_out(k) - p_l_k = this%energy_out(l)%p(k) - if (this%energy_out(l)%interpolation == HISTOGRAM) then + E_l_k = this%distribution(l)%e_out(k) + p_l_k = this%distribution(l)%p(k) + if (this%distribution(l)%interpolation == HISTOGRAM) then ! Histogram interpolation if (p_l_k > ZERO) then E_out = E_l_k + (r1 - c_k)/p_l_k @@ -297,10 +283,10 @@ contains E_out = E_l_k end if - elseif (this%energy_out(l)%interpolation == LINEAR_LINEAR) then + elseif (this%distribution(l)%interpolation == LINEAR_LINEAR) then ! Linear-linear interpolation - E_l_k1 = this%energy_out(l)%e_out(k+1) - p_l_k1 = this%energy_out(l)%p(k+1) + E_l_k1 = this%distribution(l)%e_out(k+1) + p_l_k1 = this%distribution(l)%p(k+1) frac = (p_l_k1 - p_l_k)/(E_l_k1 - E_l_k) if (frac == ZERO) then @@ -321,6 +307,7 @@ contains end if end function continuous_sample + function maxwellenergy_sample(this, E_in) result(E_out) class(MaxwellEnergy), intent(in) :: this real(8), intent(in) :: E_in ! incoming energy @@ -329,7 +316,7 @@ contains real(8) :: theta ! Maxwell distribution parameter ! Get temperature corresponding to incoming energy - theta = interpolate_tab1(this%theta, E_in) + theta = this % theta % evaluate(E_in) do ! Sample maxwell fission spectrum @@ -349,9 +336,9 @@ contains real(8) :: x, y, v ! Get temperature corresponding to incoming energy - theta = interpolate_tab1(this%theta, E_in) + theta = this % theta % evaluate(E_in) - y = (E_in - this%U)/theta + y = (E_in - this%u)/theta v = 1 - exp(-y) ! Sample outgoing energy based on evaporation spectrum probability @@ -372,10 +359,10 @@ contains real(8) :: a, b ! Watt spectrum parameters ! Determine Watt parameter 'a' from tabulated function - a = interpolate_tab1(this%a, E_in) + a = this % a % evaluate(E_in) ! Determine Watt parameter 'b' from tabulated function - b = interpolate_tab1(this%b, E_in) + b = this % b % evaluate(E_in) do ! Sample energy-dependent Watt fission spectrum @@ -386,44 +373,4 @@ contains end do end function watt_sample - function nbody_sample(this, E_in) result(E_out) - class(NBodyPhaseSpace), intent(in) :: this - real(8), intent(in) :: E_in ! incoming energy - real(8) :: E_out ! sampled outgoing energy - - real(8) :: Ap ! total mass of particles in neutron masses - real(8) :: E_max ! maximum possible COM energy - real(8) :: x, y, v - real(8) :: r1, r2, r3, r4, r5, r6 - - ! Determine E_max parameter - Ap = this%mass_ratio - E_max = (Ap - ONE)/Ap * (this%A/(this%A + ONE)*E_in + this%Q) - - ! x is essentially a Maxwellian distribution - x = maxwell_spectrum(ONE) - - select case (this%n_bodies) - case (3) - y = maxwell_spectrum(ONE) - case (4) - r1 = prn() - r2 = prn() - r3 = prn() - y = -log(r1*r2*r3) - case (5) - r1 = prn() - r2 = prn() - r3 = prn() - r4 = prn() - r5 = prn() - r6 = prn() - y = -log(r1*r2*r3*r4) - log(r5) * cos(PI/TWO*r6)**2 - end select - - ! Now determine v and E_out - v = x/(x+y) - E_out = E_max * v - end function nbody_sample - end module energy_distribution diff --git a/src/energy_grid.F90 b/src/energy_grid.F90 index 66419f83c..248462f70 100644 --- a/src/energy_grid.F90 +++ b/src/energy_grid.F90 @@ -27,7 +27,7 @@ contains integer :: i ! index in nuclides array integer :: j ! index in materials array type(ListReal) :: list - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc type(Material), pointer :: mat call write_message("Creating unionized energy grid...", 5) @@ -70,7 +70,7 @@ contains real(8) :: E_max ! Maximum energy in MeV real(8) :: E_min ! Minimum energy in MeV real(8), allocatable :: umesh(:) ! Equally log-spaced energy grid - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc ! Set minimum/maximum energies E_max = energy_max_neutron @@ -179,7 +179,7 @@ contains integer :: index_e ! index on union energy grid real(8) :: union_energy ! energy on union grid real(8) :: energy ! energy on nuclide grid - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc type(Material), pointer :: mat do k = 1, n_materials diff --git a/src/fission.F90 b/src/fission.F90 deleted file mode 100644 index a005d9f5b..000000000 --- a/src/fission.F90 +++ /dev/null @@ -1,161 +0,0 @@ -module fission - - use ace_header, only: Nuclide - use constants - use error, only: fatal_error - use interpolation, only: interpolate_tab1 - use search, only: binary_search - - implicit none - -contains - -!=============================================================================== -! NU_TOTAL calculates the total number of neutrons emitted per fission for a -! given nuclide and incoming neutron energy -!=============================================================================== - - pure function nu_total(nuc, E) result(nu) - type(Nuclide), intent(in) :: nuc ! nuclide from which to find nu - real(8), intent(in) :: E ! energy of incoming neutron - real(8) :: nu ! number of total neutrons emitted per fission - - integer :: i ! loop index - integer :: NC ! number of polynomial coefficients - real(8) :: c ! polynomial coefficient - - if (nuc % nu_t_type == NU_NONE) then - nu = ERROR_REAL - elseif (nuc % nu_t_type == NU_POLYNOMIAL) then - ! determine number of coefficients - NC = int(nuc % nu_t_data(1)) - - ! sum up polynomial in energy - nu = ZERO - do i = 0, NC - 1 - c = nuc % nu_t_data(i+2) - nu = nu + c * E**i - end do - elseif (nuc % nu_t_type == NU_TABULAR) then - ! use ENDF interpolation laws to determine nu - nu = interpolate_tab1(nuc % nu_t_data, E) - end if - - end function nu_total - -!=============================================================================== -! NU_PROMPT calculates the total number of prompt neutrons emitted per fission -! for a given nuclide and incoming neutron energy -!=============================================================================== - - pure function nu_prompt(nuc, E) result(nu) - type(Nuclide), intent(in) :: nuc ! nuclide from which to find nu - real(8), intent(in) :: E ! energy of incoming neutron - real(8) :: nu ! number of prompt neutrons emitted per fission - - integer :: i ! loop index - integer :: NC ! number of polynomial coefficients - real(8) :: c ! polynomial coefficient - - if (nuc % nu_p_type == NU_NONE) then - ! since no prompt or delayed data is present, this means all neutron - ! emission is prompt -- WARNING: This currently returns zero. The calling - ! routine needs to know this situation is occurring since we don't want - ! to call nu_total unnecessarily if it has already been called. - nu = ZERO - elseif (nuc % nu_p_type == NU_POLYNOMIAL) then - ! determine number of coefficients - NC = int(nuc % nu_p_data(1)) - - ! sum up polynomial in energy - nu = ZERO - do i = 0, NC - 1 - c = nuc % nu_p_data(i+2) - nu = nu + c * E**i - end do - elseif (nuc % nu_p_type == NU_TABULAR) then - ! use ENDF interpolation laws to determine nu - nu = interpolate_tab1(nuc % nu_p_data, E) - end if - - end function nu_prompt - -!=============================================================================== -! NU_DELAYED calculates the total number of delayed neutrons emitted per fission -! for a given nuclide and incoming neutron energy -!=============================================================================== - - pure function nu_delayed(nuc, E) result(nu) - type(Nuclide), intent(in) :: nuc ! nuclide from which to find nu - real(8), intent(in) :: E ! energy of incoming neutron - real(8) :: nu ! number of delayed neutrons emitted per fission - - if (nuc % nu_d_type == NU_NONE) then - ! since no prompt or delayed data is present, this means all neutron - ! emission is prompt -- WARNING: This currently returns zero. The calling - ! routine needs to know this situation is occurring since we don't want - ! to call nu_delayed unnecessarily if it has already been called. - nu = ZERO - elseif (nuc % nu_d_type == NU_TABULAR) then - ! use ENDF interpolation laws to determine nu - nu = interpolate_tab1(nuc % nu_d_data, E) - end if - - end function nu_delayed - -!=============================================================================== -! YIELD_DELAYED calculates the fractional yield of delayed neutrons emitted for -! a given nuclide and incoming neutron energy in a given delayed group. -!=============================================================================== - - pure function yield_delayed(nuc, E, g) result(yield) - type(Nuclide), intent(in) :: nuc ! nuclide from which to find nu - real(8), intent(in) :: E ! energy of incoming neutron - real(8) :: yield ! delayed neutron precursor yield - integer, intent(in) :: g ! the delayed neutron precursor group - integer :: d ! precursor group - integer :: lc ! index before start of energies/nu values - integer :: NR ! number of interpolation regions - integer :: NE ! number of energies tabulated - - yield = ZERO - - if (g > nuc % n_precursor .or. g < 1) then - ! if the precursor group is outside the range of precursor groups for - ! the input nuclide, return ZERO. - yield = ZERO - else if (nuc % nu_d_type == NU_NONE) then - ! since no prompt or delayed data is present, this means all neutron - ! emission is prompt -- WARNING: This currently returns zero. The calling - ! routine needs to know this situation is occurring since we don't want - ! to call yield_delayed unnecessarily if it has already been called. - yield = ZERO - else if (nuc % nu_d_type == NU_TABULAR) then - - lc = 1 - - ! loop over delayed groups and determine the yield for the desired group - do d = 1, nuc % n_precursor - - ! determine number of interpolation regions and energies - NR = int(nuc % nu_d_precursor_data(lc + 1)) - NE = int(nuc % nu_d_precursor_data(lc + 2 + 2*NR)) - - ! check if this is the desired group - if (d == g) then - - ! determine delayed neutron precursor yield for group g - yield = interpolate_tab1(nuc % nu_d_precursor_data( & - lc+1:lc+2+2*NR+2*NE), E) - - exit - end if - - ! advance pointer - lc = lc + 2 + 2*NR + 2*NE + 1 - end do - end if - - end function yield_delayed - -end module fission diff --git a/src/geometry_header.F90 b/src/geometry_header.F90 index 0756e23dc..e4f220e3d 100644 --- a/src/geometry_header.F90 +++ b/src/geometry_header.F90 @@ -31,12 +31,10 @@ module geometry_header integer :: outer ! universe to tile outside the lat logical :: is_3d ! Lattice has cells on z axis integer, allocatable :: offset(:,:,:,:) ! Distribcell offsets - - contains - - procedure(are_valid_indices_), deferred :: are_valid_indices - procedure(get_indices_), deferred :: get_indices - procedure(get_local_xyz_), deferred :: get_local_xyz + contains + procedure(lattice_are_valid_indices_), deferred :: are_valid_indices + procedure(lattice_get_indices_), deferred :: get_indices + procedure(lattice_get_local_xyz_), deferred :: get_local_xyz end type Lattice abstract interface @@ -45,33 +43,33 @@ module geometry_header ! ARE_VALID_INDICES returns .true. if the given lattice indices fit within the ! bounds of the lattice. Returns false otherwise. - function are_valid_indices_(this, i_xyz) result(is_valid) + function lattice_are_valid_indices_(this, i_xyz) result(is_valid) import Lattice class(Lattice), intent(in) :: this integer, intent(in) :: i_xyz(3) logical :: is_valid - end function are_valid_indices_ + end function lattice_are_valid_indices_ !=============================================================================== ! GET_INDICES returns the indices in a lattice for the given global xyz. - function get_indices_(this, global_xyz) result(i_xyz) + function lattice_get_indices_(this, global_xyz) result(i_xyz) import Lattice class(Lattice), intent(in) :: this real(8), intent(in) :: global_xyz(3) integer :: i_xyz(3) - end function get_indices_ + end function lattice_get_indices_ !=============================================================================== ! GET_LOCAL_XYZ returns the translated local version of the given global xyz. - function get_local_xyz_(this, global_xyz, i_xyz) result(local_xyz) + function lattice_get_local_xyz_(this, global_xyz, i_xyz) result(local_xyz) import Lattice class(Lattice), intent(in) :: this real(8), intent(in) :: global_xyz(3) integer, intent(in) :: i_xyz(3) real(8) :: local_xyz(3) - end function get_local_xyz_ + end function lattice_get_local_xyz_ end interface !=============================================================================== diff --git a/src/global.F90 b/src/global.F90 index b36689ca9..bfd993bc5 100644 --- a/src/global.F90 +++ b/src/global.F90 @@ -1,15 +1,16 @@ module global - use ace_header, only: Nuclide, SAlphaBeta, xsListing, NuclideMicroXS, & - MaterialMacroXS, Nuclide0K use bank_header, only: Bank use cmfd_header use constants use dict_header, only: DictCharInt, DictIntInt use geometry_header, only: Cell, Universe, Lattice, LatticeContainer + use macroxs_header, only: MacroXSContainer use material_header, only: Material use mesh_header, only: RegularMesh + use nuclide_header use plot_header, only: ObjectPlot + use sab_header, only: SAlphaBeta use set_header, only: SetInt use surface_header, only: SurfaceContainer use source_header, only: SourceDistribution @@ -59,42 +60,82 @@ module global integer :: n_lost_particles ! ============================================================================ - ! CROSS SECTION RELATED VARIABLES + ! ENERGY TREATMENT RELATED VARIABLES + logical :: run_CE = .true. ! Run in CE mode? + + ! ============================================================================ + ! CROSS SECTION RELATED VARIABLES NEEDED REGARDLESS OF CE OR MG ! Cross section arrays - type(Nuclide), allocatable, target :: nuclides(:) ! Nuclide cross-sections - type(SAlphaBeta), allocatable, target :: sab_tables(:) ! S(a,b) tables type(XsListing), allocatable, target :: xs_listings(:) ! cross_sections.xml listings + integer :: n_nuclides_total ! Number of nuclide cross section tables + integer :: n_listings ! Number of listings in cross_sections.xml + ! Cross section caches type(NuclideMicroXS), allocatable :: micro_xs(:) ! Cache for each nuclide type(MaterialMacroXS) :: material_xs ! Cache for current material - integer :: n_nuclides_total ! Number of nuclide cross section tables + ! Dictionaries to look up cross sections and listings + type(DictCharInt) :: nuclide_dict + type(DictCharInt) :: xs_listing_dict + + ! Default xs identifier (e.g. 70c or 300K) + character(5):: default_xs + + ! ============================================================================ + ! CONTINUOUS-ENERGY CROSS SECTION RELATED VARIABLES + + ! Cross section arrays + type(NuclideCE), allocatable, target :: nuclides(:) ! Nuclide cross-sections + type(SAlphaBeta), allocatable, target :: sab_tables(:) ! S(a,b) tables + integer :: n_sab_tables ! Number of S(a,b) thermal scattering tables - integer :: n_listings ! Number of listings in cross_sections.xml ! Minimum/maximum energies real(8) :: energy_min_neutron = ZERO real(8) :: energy_max_neutron = INFINITY ! Dictionaries to look up cross sections and listings - type(DictCharInt) :: nuclide_dict type(DictCharInt) :: sab_dict - type(DictCharInt) :: xs_listing_dict ! Unreoslved resonance probablity tables logical :: urr_ptables_on = .true. - ! Default xs identifier (e.g. 70c) - character(3):: default_xs - ! What to assume for expanding natural elements integer :: default_expand = ENDF_BVII1 ! Whether or not windowed multipole cross sections should be used. logical :: multipole_active = .false. + ! Total amount of nuclide ZAID and dictionary of nuclide ZAID and index + integer(8) :: n_nuc_zaid_total + type(DictIntInt) :: nuc_zaid_dict + + ! ============================================================================ + ! MULTI-GROUP CROSS SECTION RELATED VARIABLES + + ! Cross section arrays + type(NuclideMGContainer), allocatable, target :: nuclides_MG(:) + + ! Cross section caches + type(MacroXSContainer), target, allocatable :: macro_xs(:) + + ! Number of energy groups + integer :: energy_groups + + ! Energy group structure + real(8), allocatable :: energy_bins(:) + + ! Midpoint of the energy group structure + real(8), allocatable :: energy_bin_avg(:) + + ! Inverse velocities of the energy groups (provided or estimated) + real(8), allocatable :: inverse_velocities(:) + + ! Maximum Data Order + integer :: max_order + ! ============================================================================ ! TALLY-RELATED VARIABLES @@ -399,7 +440,7 @@ module global type(SetInt) :: sourcepoint_batch ! Various output options - logical :: output_summary = .false. + logical :: output_summary = .true. logical :: output_xs = .false. logical :: output_tallies = .true. @@ -453,6 +494,14 @@ contains deallocate(nuclides_0K) end if + if (allocated(nuclides_MG)) then + deallocate(nuclides_MG) + end if + + if (allocated(macro_xs)) then + deallocate(macro_xs) + end if + if (allocated(sab_tables)) deallocate(sab_tables) if (allocated(xs_listings)) deallocate(xs_listings) if (allocated(micro_xs)) deallocate(micro_xs) diff --git a/src/initialize.F90 b/src/initialize.F90 index 4b412fb29..e3fe3e25d 100644 --- a/src/initialize.F90 +++ b/src/initialize.F90 @@ -1,30 +1,31 @@ module initialize - use ace, only: read_xs, same_nuclide_list - use bank_header, only: Bank + use ace, only: read_ace_xs + use bank_header, only: Bank use constants - use dict_header, only: DictIntInt, ElemKeyValueII - use set_header, only: SetInt - use energy_grid, only: logarithmic_grid, grid_method, unionized_grid - use error, only: fatal_error, warning - use geometry, only: neighbor_lists, count_instance, calc_offsets, & - maximum_levels - use geometry_header, only: Cell, Universe, Lattice, RectLattice, HexLattice,& - &BASE_UNIVERSE + use dict_header, only: DictIntInt, ElemKeyValueII + use set_header, only: SetInt + use energy_grid, only: logarithmic_grid, grid_method, unionized_grid + use error, only: fatal_error, warning + use geometry, only: neighbor_lists, count_instance, calc_offsets, & + maximum_levels + use geometry_header, only: Cell, Universe, Lattice, RectLattice, HexLattice,& + &BASE_UNIVERSE use global - use hdf5_interface, only: file_open, read_dataset, file_close, hdf5_bank_t,& - hdf5_tallyresult_t, hdf5_integer8_t - use input_xml, only: read_input_xml, read_cross_sections_xml, & - cells_in_univ_dict, read_plots_xml - use material_header, only: Material - use output, only: title, header, print_version, write_message, & - print_usage, write_xs_summary, print_plot - use random_lcg, only: initialize_prng - use state_point, only: load_state_point - use string, only: to_str, str_to_int, starts_with, ends_with - use summary, only: write_summary - use tally_header, only: TallyObject, TallyResult, TallyFilter - use tally_initialize, only: configure_tallies + use hdf5_interface, only: file_open, read_dataset, file_close, hdf5_bank_t,& + hdf5_tallyresult_t, hdf5_integer8_t + use input_xml, only: read_input_xml, cells_in_univ_dict, read_plots_xml + use material_header, only: Material + use mgxs_data, only: read_mgxs, create_macro_xs + use output, only: title, header, print_version, write_message, & + print_usage, write_xs_summary, print_plot + use random_lcg, only: initialize_prng + use state_point, only: load_state_point + use string, only: to_str, starts_with, ends_with, str_to_int + use summary, only: write_summary + use tally_header, only: TallyObject, TallyResult, TallyFilter + use tally_initialize,only: configure_tallies + use tally, only: init_tally_routines #ifdef MPI use message_passing @@ -114,30 +115,40 @@ contains ! Read ACE-format cross sections call time_read_xs%start() - call read_xs() + if (run_CE) then + call read_ace_xs() + else + call read_mgxs() + end if call time_read_xs%stop() - ! Create linked lists for multiple instances of the same nuclide - call same_nuclide_list() + ! Construct information needed for nuclear data + if (run_CE) then + ! Set undefined cell temperatures to match the material data. + call lookup_material_temperatures() - ! Set undefined cell temperatures to match the material data. - call lookup_material_temperatures() - - ! Construct unionized or log energy grid for cross-sections - select case (grid_method) - case (GRID_NUCLIDE) - continue - case (GRID_MAT_UNION) - call time_unionize%start() - call unionized_grid() - call time_unionize%stop() - case (GRID_LOGARITHM) - call logarithmic_grid() - end select + ! Construct unionized or log energy grid for cross-sections + select case (grid_method) + case (GRID_NUCLIDE) + continue + case (GRID_MAT_UNION) + call time_unionize%start() + call unionized_grid() + call time_unionize%stop() + case (GRID_LOGARITHM) + call logarithmic_grid() + end select + else + ! Create material macroscopic data for MGXS + call create_macro_xs() + end if ! Allocate and setup tally stride, matching_bins, and tally maps call configure_tallies() + ! Set up tally procedure pointers + call init_tally_routines() + ! Determine how much work each processor should do call calculate_work() @@ -1176,7 +1187,7 @@ contains do k = 2, mat % n_nuclides ! Warn the user if the nuclides don't have identical temperatues. if (nuclides(mat % nuclide(k)) % kT /= min_temp & - .and. .not. warning_given) then + .and. .not. warning_given .and. multipole_active) then call warning("OpenMC cannot & &identify the temperature of at least one cell. For the & &purposes of multipole cross section evaluations, all cells & diff --git a/src/input_xml.F90 b/src/input_xml.F90 index b922b194e..e7d666b4f 100644 --- a/src/input_xml.F90 +++ b/src/input_xml.F90 @@ -17,8 +17,8 @@ module input_xml use random_lcg, only: prn, seed use surface_header use stl_vector, only: VectorInt - use string, only: to_lower, to_str, str_to_int, str_to_real, & - starts_with, ends_with, tokenize + use string, only: str_to_int, str_to_real, tokenize, & + to_lower, to_str, starts_with, ends_with use tally_header, only: TallyObject, TallyFilter use tally_initialize, only: add_tallies use xml_interface @@ -39,7 +39,13 @@ contains subroutine read_input_xml() call read_settings_xml() - if (run_mode /= MODE_PLOTTING) call read_cross_sections_xml() + if (run_mode /= MODE_PLOTTING) then + if (run_CE) then + call read_ce_cross_sections_xml() + else + call read_mg_cross_sections_xml() + end if + end if call read_geometry_xml() call read_materials_xml() call read_tallies_xml() @@ -103,6 +109,17 @@ contains ! Parse settings.xml file call open_xmldoc(doc, filename) + ! Find if a multi-group or continuous-energy simulation is desired + if (check_for_node(doc, "energy_mode")) then + call get_node_value(doc, "energy_mode", temp_str) + temp_str = trim(to_lower(temp_str)) + if (temp_str == "mg" .or. temp_str == "multi-group") then + run_CE = .false. + else if (temp_str == "ce" .or. temp_str == "continuous-energy") then + run_CE = .true. + end if + end if + ! Find cross_sections.xml file -- the first place to look is the ! settings.xml file. If no file is found there, then we check the ! CROSS_SECTIONS environment variable @@ -111,16 +128,37 @@ contains run_mode /= MODE_PLOTTING) then ! No cross_sections.xml file specified in settings.xml, check ! environment variable - call get_environment_variable("CROSS_SECTIONS", env_variable) - if (len_trim(env_variable) == 0) then - call fatal_error("No cross_sections.xml file was specified in & - &settings.xml or in the CROSS_SECTIONS environment variable. & - &OpenMC needs a cross_sections.xml file to identify where to & - &find ACE cross section libraries. Please consult the user's & - &guide at http://mit-crpg.github.io/openmc for information on & - &how to set up ACE cross section libraries.") - else + if (run_CE) then + call get_environment_variable("OPENMC_CROSS_SECTIONS", env_variable) + if (len_trim(env_variable) == 0) then + call get_environment_variable("CROSS_SECTIONS", env_variable) + if (len_trim(env_variable) == 0) then + call fatal_error("No cross_sections.xml file was specified in & + &settings.xml or in the OPENMC_CROSS_SECTIONS environment & + &variable. OpenMC needs such a file to identify where to & + &find ACE cross section libraries. Please consult the & + &user's guide at http://mit-crpg.github.io/openmc for & + &information on how to set up ACE cross section libraries.") + else + call warning("The CROSS_SECTIONS environment variable is & + &deprecated. Please update your environment to use & + &OPENMC_CROSS_SECTIONS instead.") + end if + end if path_cross_sections = trim(env_variable) + else + call get_environment_variable("OPENMC_MG_CROSS_SECTIONS", & + env_variable) + if (len_trim(env_variable) == 0) then + call fatal_error("No cross_sections.xml file was specified in & + &settings.xml or in the OPENMC_MG_CROSS_SECTIONS environment & + &variable. OpenMC needs such a file to identify where to & + &find the cross section libraries. Please consult the user's & + &guide at http://mit-crpg.github.io/openmc for information on & + &how to set up the cross section libraries.") + else + path_cross_sections = trim(env_variable) + end if end if else call get_node_value(doc, "cross_sections", path_cross_sections) @@ -129,11 +167,10 @@ contains ! Find the windowed multipole library if (run_mode /= MODE_PLOTTING) then - if (.not. check_for_node(doc, "multipole_library") .and. & - run_mode /= MODE_PLOTTING) then + if (.not. check_for_node(doc, "multipole_library")) then ! No library location specified in settings.xml, check ! environment variable - call get_environment_variable("MULTIPOLE_LIBRARY", env_variable) + call get_environment_variable("OPENMC_MULTIPOLE_LIBRARY", env_variable) path_multipole = trim(env_variable) else call get_node_value(doc, "multipole_library", path_multipole) @@ -142,6 +179,19 @@ contains path_multipole = trim(path_multipole) // "/" end if + if (.not. run_CE) then + ! Scattering Treatments + if (check_for_node(doc, "max_order")) then + call get_node_value(doc, "max_order", max_order) + else + ! Set to default of largest int, which means to use whatever is + ! contained in library + max_order = huge(0) + end if + else + max_order = 0 + end if + ! Set output directory if a path has been specified on the ! element if (check_for_node(doc, "output_path")) then @@ -188,8 +238,8 @@ contains end if ! Make sure that either eigenvalue or fixed source was specified - if (.not.check_for_node(doc, "eigenvalue") .and. & - .not.check_for_node(doc, "fixed_source")) then + if (.not. check_for_node(doc, "eigenvalue") .and. & + .not. check_for_node(doc, "fixed_source")) then call fatal_error(" or not specified.") end if @@ -202,7 +252,7 @@ contains call get_node_ptr(doc, "eigenvalue", node_mode) ! Check number of particles - if (.not.check_for_node(node_mode, "particles")) then + if (.not. check_for_node(node_mode, "particles")) then call fatal_error("Need to specify number of particles per generation.") end if @@ -272,7 +322,7 @@ contains call get_node_ptr(doc, "fixed_source", node_mode) ! Check number of particles - if (.not.check_for_node(node_mode, "particles")) then + if (.not. check_for_node(node_mode, "particles")) then call fatal_error("Need to specify number of particles per batch.") end if @@ -920,8 +970,8 @@ contains if (check_for_node(node_output, "summary")) then call get_node_value(node_output, "summary", temp_str) temp_str = to_lower(temp_str) - if (trim(temp_str) == 'true' .or. & - trim(temp_str) == '1') output_summary = .true. + if (trim(temp_str) == 'false' .or. & + trim(temp_str) == '0') output_summary = .false. end if ! Check for cross sections option @@ -968,7 +1018,7 @@ contains ! check to make sure a nuclide is specified if (.not. check_for_node(node_scatterer, "nuclide")) then call fatal_error("No nuclide specified for scatterer " & - &// trim(to_str(i)) // " in settings.xml file!") + // trim(to_str(i)) // " in settings.xml file!") end if call get_node_value(node_scatterer, "nuclide", & nuclides_0K(i) % nuclide) @@ -982,7 +1032,7 @@ contains if (.not. check_for_node(node_scatterer, "xs_label")) then call fatal_error("Must specify the temperature dependent name of & &scatterer " // trim(to_str(i)) & - &// " given in cross_sections.xml") + // " given in cross_sections.xml") end if call get_node_value(node_scatterer, "xs_label", & nuclides_0K(i) % name) @@ -990,7 +1040,7 @@ contains ! check to make sure 0K xs name for which method is applied is given if (.not. check_for_node(node_scatterer, "xs_label_0K")) then call fatal_error("Must specify the 0K name of scatterer " & - &// trim(to_str(i)) // " given in cross_sections.xml") + // trim(to_str(i)) // " given in cross_sections.xml") end if call get_node_value(node_scatterer, "xs_label_0K", & nuclides_0K(i) % name_0K) @@ -1050,7 +1100,7 @@ contains default_expand = JENDL_40 case default call fatal_error("Unknown natural element expansion option: " & - &// trim(temp_str)) + // trim(temp_str)) end select end if @@ -1058,9 +1108,9 @@ contains if (check_for_node(doc, "use_windowed_multipole")) then call get_node_value(doc, "use_windowed_multipole", temp_str) select case (to_lower(temp_str)) - case ('true', 't', '1', 'y') + case ('true', '1') multipole_active = .true. - case ('false', 'f', '0', 'n') + case ('false', '0') multipole_active = .false. case default call fatal_error("Unrecognized value for in & @@ -1181,7 +1231,7 @@ contains ! Check to make sure 'id' hasn't been used if (cell_dict % has_key(c % id)) then call fatal_error("Two or more cells use the same unique ID: " & - &// to_str(c % id)) + // to_str(c % id)) end if ! Read material @@ -1283,7 +1333,7 @@ contains n = get_arraysize_double(node_cell, "rotation") if (n /= 3) then call fatal_error("Incorrect number of rotation parameters on cell " & - &// to_str(c % id)) + // to_str(c % id)) end if ! Copy rotation angles in x,y,z directions @@ -1311,7 +1361,7 @@ contains ! another universe if (c % fill == NONE) then call fatal_error("Cannot apply a translation to cell " & - &// trim(to_str(c % id)) // " because it is not filled with & + // trim(to_str(c % id)) // " because it is not filled with & &another universe") end if @@ -1330,7 +1380,11 @@ contains ! Read cell temperatures. If the temperature is not specified, set it to ! ERROR_REAL for now. During initialization we'll replace ERROR_REAL with ! the temperature from the material data. - if (check_for_node(node_cell, "temperature")) then + if (.not. run_CE) then + ! Cell temperatures are not used for MG mode. + allocate(c % sqrtkT(1)) + c % sqrtkT(1) = ZERO + else if (check_for_node(node_cell, "temperature")) then n = get_arraysize_double(node_cell, "temperature") if (n > 0) then ! Make sure this is a "normal" cell. @@ -1461,7 +1515,7 @@ contains ! Check to make sure 'id' hasn't been used if (surface_dict % has_key(s%id)) then call fatal_error("Two or more surfaces use the same unique ID: " & - &// to_str(s%id)) + // to_str(s%id)) end if ! Copy surface name @@ -1476,10 +1530,10 @@ contains n = get_arraysize_double(node_surf, "coeffs") if (n < coeffs_reqd) then call fatal_error("Not enough coefficients specified for surface: " & - &// trim(to_str(s%id))) + // trim(to_str(s%id))) elseif (n > coeffs_reqd) then call fatal_error("Too many coefficients specified for surface: " & - &// trim(to_str(s%id))) + // trim(to_str(s%id))) end if allocate(coeffs(n)) @@ -1605,7 +1659,7 @@ contains ! Check to make sure 'id' hasn't been used if (lattice_dict % has_key(lat % id)) then call fatal_error("Two or more lattices use the same unique ID: " & - &// to_str(lat % id)) + // to_str(lat % id)) end if ! Copy lattice name @@ -1733,7 +1787,7 @@ contains ! Check to make sure 'id' hasn't been used if (lattice_dict % has_key(lat % id)) then call fatal_error("Two or more lattices use the same unique ID: " & - &// to_str(lat % id)) + // to_str(lat % id)) end if ! Copy lattice name @@ -1905,21 +1959,23 @@ contains subroutine read_materials_xml() - integer :: i ! loop index for materials - integer :: j ! loop index for nuclides - integer :: k ! loop index for elements - integer :: n ! number of nuclides - integer :: n_sab ! number of sab tables for a material - integer :: n_nuc_ele ! number of nuclides in an element - integer :: index_list ! index in xs_listings array - integer :: index_nuclide ! index in nuclides - integer :: index_sab ! index in sab_tables - real(8) :: val ! value entered for density - real(8) :: temp_dble ! temporary double prec. real - logical :: file_exists ! does materials.xml exist? - logical :: sum_density ! density is taken to be sum of nuclide densities - character(12) :: name ! name of isotope, e.g. 92235.03c - character(12) :: alias ! alias of nuclide, e.g. U-235.03c + integer :: i ! loop index for materials + integer :: j ! loop index for nuclides + integer :: k ! loop index for elements + integer :: n ! number of nuclides + integer :: n_sab ! number of sab tables for a material + integer :: n_nuc_ele ! number of nuclides in an element + integer :: index_list ! index in xs_listings array + integer :: index_nuclide ! index in nuclides + integer :: index_nuc_zaid ! index in nuclide ZAID + integer :: index_sab ! index in sab_tables + real(8) :: val ! value entered for density + real(8) :: temp_dble ! temporary double prec. real + logical :: file_exists ! does materials.xml exist? + logical :: sum_density ! density is taken to be sum of nuclide densities + integer :: zaid ! ZAID of nuclide + character(12) :: name ! name of isotope, e.g. 92235.03c + character(12) :: alias ! alias of nuclide, e.g. U-235.03c character(MAX_WORD_LEN) :: units ! units on density character(MAX_LINE_LEN) :: filename ! absolute path to materials.xml character(MAX_LINE_LEN) :: temp_str ! temporary string when reading @@ -1935,6 +1991,7 @@ contains type(Node), pointer :: node_sab => null() type(NodeList), pointer :: node_mat_list => null() type(NodeList), pointer :: node_nuc_list => null() + type(NodeList), pointer :: node_macro_list => null() type(NodeList), pointer :: node_ele_list => null() type(NodeList), pointer :: node_sab_list => null() @@ -1968,6 +2025,7 @@ contains ! Initialize count for number of nuclides/S(a,b) tables index_nuclide = 0 + index_nuc_zaid = 0 index_sab = 0 do i = 1, n_materials @@ -1986,12 +2044,13 @@ contains ! Check to make sure 'id' hasn't been used if (material_dict % has_key(mat % id)) then call fatal_error("Two or more materials use the same unique ID: " & - &// to_str(mat % id)) + // to_str(mat % id)) end if ! Copy material name if (check_for_node(node_mat, "name")) then call get_node_value(node_mat, "name", mat % name) + mat % name = to_lower(mat % name) end if if (run_mode == MODE_PLOTTING) then @@ -2008,7 +2067,7 @@ contains call get_node_ptr(node_mat, "density", node_dens) else call fatal_error("Must specify density element in material " & - &// trim(to_str(mat % id))) + // trim(to_str(mat % id))) end if ! Initialize value to zero @@ -2024,6 +2083,19 @@ contains sum_density = .true. + else if (units == 'macro') then + if (check_for_node(node_dens, "value")) then + ! Copy value + call get_node_value(node_dens, "value", val) + else + val = ONE + end if + + ! Set density + mat % density = val + + sum_density = .false. + else ! Copy value call get_node_value(node_dens, "value", val) @@ -2032,7 +2104,7 @@ contains sum_density = .false. if (val <= ZERO) then call fatal_error("Need to specify a positive density on material " & - &// trim(to_str(mat % id)) // ".") + // trim(to_str(mat % id)) // ".") end if ! Adjust material density based on specified units @@ -2047,7 +2119,7 @@ contains mat % density = 1.0e-24_8 * val case default call fatal_error("Unkwown units '" // trim(units) & - &// "' specified on material " // trim(to_str(mat % id))) + // "' specified on material " // trim(to_str(mat % id))) end select end if @@ -2056,80 +2128,141 @@ contains ! Check to ensure material has at least one nuclide if (.not. check_for_node(node_mat, "nuclide") .and. & - .not. check_for_node(node_mat, "element")) then - call fatal_error("No nuclides or natural elements specified on & - &material " // trim(to_str(mat % id))) + .not. check_for_node(node_mat, "element") .and. & + .not. check_for_node(node_mat, "macroscopic")) then + call fatal_error("No macroscopic data, nuclides or natural elements & + &specified on material " // trim(to_str(mat % id))) end if - ! Get pointer list of XML - call get_node_list(node_mat, "nuclide", node_nuc_list) + ! Create list of macroscopic x/s based on those specified, just treat + ! them as nuclides. This is all really a facade so the user thinks they + ! are entering in macroscopic data but the code treats them the same + ! as nuclides internally. + ! Get pointer list of XML + call get_node_list(node_mat, "macroscopic", node_macro_list) + if (run_CE .and. (get_list_size(node_macro_list) > 0)) then + call fatal_error("Macroscopic can not be used in continuous-energy& + & mode!") + else if (get_list_size(node_macro_list) > 1) then + call fatal_error("Only one macroscopic object permitted per material, " & + // trim(to_str(mat % id))) + else if (get_list_size(node_macro_list) == 1) then - ! Create list of nuclides based on those specified plus natural elements - INDIVIDUAL_NUCLIDES: do j = 1, get_list_size(node_nuc_list) - ! Combine nuclide identifier and cross section and copy into names - call get_list_item(node_nuc_list, j, node_nuc) + call get_list_item(node_macro_list, 1, node_nuc) ! Check for empty name on nuclide - if (.not.check_for_node(node_nuc, "name")) then - call fatal_error("No name specified on nuclide in material " & - &// trim(to_str(mat % id))) + if (.not. check_for_node(node_nuc, "name")) then + call fatal_error("No name specified on macroscopic data in material " & + // trim(to_str(mat % id))) end if ! Check for cross section - if (.not.check_for_node(node_nuc, "xs")) then + if (.not. check_for_node(node_nuc, "xs")) then if (default_xs == '') then - call fatal_error("No cross section specified for nuclide in & - &material " // trim(to_str(mat % id))) + call fatal_error("No cross section specified for macroscopic data & + & in material " // trim(to_str(mat % id))) else - name = trim(default_xs) + name = to_lower(trim(default_xs)) end if end if - ! Check enforced isotropic lab scattering - if (check_for_node(node_nuc, "scattering")) then - call get_node_value(node_nuc, "scattering", temp_str) - if (adjustl(to_lower(temp_str)) == "iso-in-lab") then - call list_iso_lab % append(1) - else if (adjustl(to_lower(temp_str)) == "data") then - call list_iso_lab % append(0) - else - call fatal_error("Scattering must be isotropic in lab or follow& - & the ACE file data") - end if - else - call list_iso_lab % append(0) - end if - ! store full name call get_node_value(node_nuc, "name", temp_str) if (check_for_node(node_nuc, "xs")) & call get_node_value(node_nuc, "xs", name) name = trim(temp_str) // "." // trim(name) + name = to_lower(name) ! save name and density to list call list_names % append(name) ! Check if no atom/weight percents were specified or if both atom and ! weight percents were specified - if (.not.check_for_node(node_nuc, "ao") .and. & - .not.check_for_node(node_nuc, "wo")) then - call fatal_error("No atom or weight percent specified for nuclide " & - &// trim(name)) - elseif (check_for_node(node_nuc, "ao") .and. & - check_for_node(node_nuc, "wo")) then - call fatal_error("Cannot specify both atom and weight percents for a & - &nuclide: " // trim(name)) - end if - - ! Copy atom/weight percents - if (check_for_node(node_nuc, "ao")) then - call get_node_value(node_nuc, "ao", temp_dble) - call list_density % append(temp_dble) + if (units == 'macro') then + call list_density % append(ONE) else - call get_node_value(node_nuc, "wo", temp_dble) - call list_density % append(-temp_dble) + call fatal_error("Units can only be macro for macroscopic data " & + // trim(name)) end if - end do INDIVIDUAL_NUCLIDES + else + + ! Get pointer list of XML + call get_node_list(node_mat, "nuclide", node_nuc_list) + + ! Create list of nuclides based on those specified plus natural elements + INDIVIDUAL_NUCLIDES: do j = 1, get_list_size(node_nuc_list) + ! Combine nuclide identifier and cross section and copy into names + call get_list_item(node_nuc_list, j, node_nuc) + + ! Check for empty name on nuclide + if (.not. check_for_node(node_nuc, "name")) then + call fatal_error("No name specified on nuclide in material " & + // trim(to_str(mat % id))) + end if + + ! Check for cross section + if (.not. check_for_node(node_nuc, "xs")) then + if (default_xs == '') then + call fatal_error("No cross section specified for nuclide in & + &material " // trim(to_str(mat % id))) + else + name = to_lower(trim(default_xs)) + end if + end if + + ! Check enforced isotropic lab scattering + if (run_CE) then + if (check_for_node(node_nuc, "scattering")) then + call get_node_value(node_nuc, "scattering", temp_str) + if (adjustl(to_lower(temp_str)) == "iso-in-lab") then + call list_iso_lab % append(1) + else if (adjustl(to_lower(temp_str)) == "data") then + call list_iso_lab % append(0) + else + call fatal_error("Scattering must be isotropic in lab or follow& + & the ACE file data") + end if + else + call list_iso_lab % append(0) + end if + end if + + ! store full name + call get_node_value(node_nuc, "name", temp_str) + if (check_for_node(node_nuc, "xs")) & + call get_node_value(node_nuc, "xs", name) + name = trim(temp_str) // "." // trim(name) + name = to_lower(name) + + ! save name and density to list + call list_names % append(name) + + ! Check if no atom/weight percents were specified or if both atom and + ! weight percents were specified + if (units == 'macro') then + call list_density % append(ONE) + else + if (.not. check_for_node(node_nuc, "ao") .and. & + .not. check_for_node(node_nuc, "wo")) then + call fatal_error("No atom or weight percent specified for nuclide " & + // trim(name)) + elseif (check_for_node(node_nuc, "ao") .and. & + check_for_node(node_nuc, "wo")) then + call fatal_error("Cannot specify both atom and weight percents for a & + &nuclide: " // trim(name)) + end if + + ! Copy atom/weight percents + if (check_for_node(node_nuc, "ao")) then + call get_node_value(node_nuc, "ao", temp_dble) + call list_density % append(temp_dble) + else + call get_node_value(node_nuc, "wo", temp_dble) + call list_density % append(-temp_dble) + end if + end if + end do INDIVIDUAL_NUCLIDES + end if ! ======================================================================= ! READ AND PARSE TAGS @@ -2141,9 +2274,9 @@ contains call get_list_item(node_ele_list, j, node_ele) ! Check for empty name on natural element - if (.not.check_for_node(node_ele, "name")) then + if (.not. check_for_node(node_ele, "name")) then call fatal_error("No name specified on nuclide in material " & - &// trim(to_str(mat % id))) + // trim(to_str(mat % id))) end if call get_node_value(node_ele, "name", name) @@ -2155,16 +2288,16 @@ contains call fatal_error("No cross section specified for nuclide in & &material " // trim(to_str(mat % id))) else - temp_str = trim(default_xs) + temp_str = to_lower(trim(default_xs)) end if end if ! Check if no atom/weight percents were specified or if both atom and ! weight percents were specified - if (.not.check_for_node(node_ele, "ao") .and. & - .not.check_for_node(node_ele, "wo")) then + if (.not. check_for_node(node_ele, "ao") .and. & + .not. check_for_node(node_ele, "wo")) then call fatal_error("No atom or weight percent specified for element " & - &// trim(name)) + // trim(name)) elseif (check_for_node(node_ele, "ao") .and. & check_for_node(node_ele, "wo")) then call fatal_error("Cannot specify both atom and weight percents for & @@ -2188,23 +2321,25 @@ contains n_nuc_ele = list_names % size() - n_nuc_ele ! Check enforced isotropic lab scattering - if (check_for_node(node_ele, "scattering")) then - call get_node_value(node_ele, "scattering", temp_str) - else - temp_str = "data" - end if - - ! Set ace or iso-in-lab scattering for each nuclide in element - do k = 1, n_nuc_ele - if (adjustl(to_lower(temp_str)) == "iso-in-lab") then - call list_iso_lab % append(1) - else if (adjustl(to_lower(temp_str)) == "data") then - call list_iso_lab % append(0) + if (run_CE) then + if (check_for_node(node_ele, "scattering")) then + call get_node_value(node_ele, "scattering", temp_str) else - call fatal_error("Scattering must be isotropic in lab or follow& - & the ACE file data") + temp_str = "data" end if - end do + + ! Set ace or iso-in-lab scattering for each nuclide in element + do k = 1, n_nuc_ele + if (adjustl(to_lower(temp_str)) == "iso-in-lab") then + call list_iso_lab % append(1) + else if (adjustl(to_lower(temp_str)) == "data") then + call list_iso_lab % append(0) + else + call fatal_error("Scattering must be isotropic in lab or follow& + & the ACE file data") + end if + end do + end if end do NATURAL_ELEMENTS @@ -2224,20 +2359,23 @@ contains name = trim(list_names % get_item(j)) if (.not. xs_listing_dict % has_key(to_lower(name))) then call fatal_error("Could not find nuclide " // trim(name) & - &// " in cross_sections.xml file!") + // " in cross_sections data file!") end if - ! Check to make sure cross-section is continuous energy neutron table - n = len_trim(name) - if (name(n:n) /= 'c') then - call fatal_error("Cross-section table " // trim(name) & - &// " is not a continuous-energy neutron table.") + if (run_CE) then + ! Check to make sure cross-section is continuous energy neutron table + n = len_trim(name) + if (name(n:n) /= 'c') then + call fatal_error("Cross-section table " // trim(name) & + // " is not a continuous-energy neutron table.") + end if end if ! Find xs_listing and set the name/alias according to the listing index_list = xs_listing_dict % get_key(to_lower(name)) name = xs_listings(index_list) % name alias = xs_listings(index_list) % alias + zaid = xs_listings(index_list) % zaid ! If this nuclide hasn't been encountered yet, we need to add its name ! and alias to the nuclide_dict @@ -2251,6 +2389,12 @@ contains mat % nuclide(j) = nuclide_dict % get_key(to_lower(name)) end if + ! Construct dict of nuclide zaid + if (.not. nuc_zaid_dict % has_key(zaid)) then + index_nuc_zaid = index_nuc_zaid + 1 + call nuc_zaid_dict % add_key(zaid, index_nuc_zaid) + end if + ! Copy name and atom/weight percent mat % names(j) = name mat % atom_density(j) = list_density % get_item(j) @@ -2269,7 +2413,7 @@ contains if (.not. (all(mat % atom_density >= ZERO) .or. & all(mat % atom_density <= ZERO))) then call fatal_error("Cannot mix atom and weight percents in material " & - &// to_str(mat % id)) + // to_str(mat % id)) end if ! Determine density if it is a sum value @@ -2282,59 +2426,60 @@ contains ! ======================================================================= ! READ AND PARSE TAG FOR S(a,b) DATA + if (run_CE) then + ! Get pointer list to XML + call get_node_list(node_mat, "sab", node_sab_list) - ! Get pointer list to XML - call get_node_list(node_mat, "sab", node_sab_list) + n_sab = get_list_size(node_sab_list) + if (n_sab > 0) then + ! Set number of S(a,b) tables + mat % n_sab = n_sab - n_sab = get_list_size(node_sab_list) - if (n_sab > 0) then - ! Set number of S(a,b) tables - mat % n_sab = n_sab + ! Allocate names and indices for nuclides and tables + allocate(mat % sab_names(n_sab)) + allocate(mat % i_sab_nuclides(n_sab)) + allocate(mat % i_sab_tables(n_sab)) - ! Allocate names and indices for nuclides and tables - allocate(mat % sab_names(n_sab)) - allocate(mat % i_sab_nuclides(n_sab)) - allocate(mat % i_sab_tables(n_sab)) + ! Initialize i_sab_nuclides + mat % i_sab_nuclides = NONE - ! Initialize i_sab_nuclides - mat % i_sab_nuclides = NONE + do j = 1, n_sab + ! Get pointer to S(a,b) table + call get_list_item(node_sab_list, j, node_sab) - do j = 1, n_sab - ! Get pointer to S(a,b) table - call get_list_item(node_sab_list, j, node_sab) + ! Determine name of S(a,b) table + if (.not. check_for_node(node_sab, "name") .or. & + .not. check_for_node(node_sab, "xs")) then + call fatal_error("Need to specify and for S(a,b) & + &table.") + end if + call get_node_value(node_sab, "name", name) + call get_node_value(node_sab, "xs", temp_str) + name = trim(name) // "." // trim(temp_str) + mat % sab_names(j) = name - ! Determine name of S(a,b) table - if (.not.check_for_node(node_sab, "name") .or. & - .not.check_for_node(node_sab, "xs")) then - call fatal_error("Need to specify and for S(a,b) & - &table.") - end if - call get_node_value(node_sab, "name", name) - call get_node_value(node_sab, "xs", temp_str) - name = trim(name) // "." // trim(temp_str) - mat % sab_names(j) = name + ! Check that this nuclide is listed in the cross_sections.xml file + if (.not. xs_listing_dict % has_key(to_lower(name))) then + call fatal_error("Could not find S(a,b) table " // trim(name) & + // " in cross_sections.xml file!") + end if - ! Check that this nuclide is listed in the cross_sections.xml file - if (.not. xs_listing_dict % has_key(to_lower(name))) then - call fatal_error("Could not find S(a,b) table " // trim(name) & - &// " in cross_sections.xml file!") - end if + ! Find index in xs_listing and set the name and alias according to the + ! listing + index_list = xs_listing_dict % get_key(to_lower(name)) + name = xs_listings(index_list) % name - ! Find index in xs_listing and set the name and alias according to the - ! listing - index_list = xs_listing_dict % get_key(to_lower(name)) - name = xs_listings(index_list) % name - - ! If this S(a,b) table hasn't been encountered yet, we need to add its - ! name and alias to the sab_dict - if (.not. sab_dict % has_key(to_lower(name))) then - index_sab = index_sab + 1 - mat % i_sab_tables(j) = index_sab - call sab_dict % add_key(to_lower(name), index_sab) - else - mat % i_sab_tables(j) = sab_dict % get_key(to_lower(name)) - end if - end do + ! If this S(a,b) table hasn't been encountered yet, we need to add its + ! name and alias to the sab_dict + if (.not. sab_dict % has_key(to_lower(name))) then + index_sab = index_sab + 1 + mat % i_sab_tables(j) = index_sab + call sab_dict % add_key(to_lower(name), index_sab) + else + mat % i_sab_tables(j) = sab_dict % get_key(to_lower(name)) + end if + end do + end if end if ! Add material to dictionary @@ -2344,6 +2489,7 @@ contains ! Set total number of nuclides and S(a,b) tables n_nuclides_total = index_nuclide n_sab_tables = index_sab + n_nuc_zaid_total = index_nuc_zaid ! Close materials XML file call close_xmldoc(doc) @@ -2485,7 +2631,7 @@ contains ! Check to make sure 'id' hasn't been used if (mesh_dict % has_key(m % id)) then call fatal_error("Two or more meshes use the same unique ID: " & - &// to_str(m % id)) + // to_str(m % id)) end if ! Read mesh type @@ -2541,8 +2687,8 @@ contains end if ! Make sure either upper-right or width was specified - if (.not.check_for_node(node_mesh, "upper_right") .and. & - .not.check_for_node(node_mesh, "width")) then + if (.not. check_for_node(node_mesh, "upper_right") .and. & + .not. check_for_node(node_mesh, "width")) then call fatal_error("Must specify either and on a & &tally mesh.") end if @@ -2709,7 +2855,7 @@ contains ! Check to make sure 'id' hasn't been used if (tally_dict % has_key(t % id)) then call fatal_error("Two or more tallies use the same unique ID: " & - &// to_str(t % id)) + // to_str(t % id)) end if ! Copy tally name @@ -2750,7 +2896,7 @@ contains end if else call fatal_error("Bins not set in filter on tally " & - &// trim(to_str(t % id))) + // trim(to_str(t % id))) end if ! Determine type of filter @@ -2842,7 +2988,7 @@ contains m => meshes(i_mesh) else call fatal_error("Could not find mesh " // trim(to_str(id)) & - &// " specified on tally " // trim(to_str(t % id))) + // " specified on tally " // trim(to_str(t % id))) end if ! Determine number of bins -- this is assuming that the tally is @@ -2865,6 +3011,14 @@ contains allocate(t % filters(j) % real_bins(n_words)) call get_node_array(node_filt, "bins", t % filters(j) % real_bins) + if (.not. run_CE) then + if (n_words /= energy_groups + 1) then + t % energy_matches_groups = .false. + else if (all(t % filters(j) % real_bins == energy_bins)) then + t % energy_matches_groups = .false. + end if + end if + case ('energyout') ! Set type of filter t % filters(j) % type = FILTER_ENERGYOUT @@ -2876,10 +3030,27 @@ contains allocate(t % filters(j) % real_bins(n_words)) call get_node_array(node_filt, "bins", t % filters(j) % real_bins) + if (.not. run_CE) then + if (n_words /= energy_groups + 1) then + t % energy_matches_groups = .false. + else if (all(t % filters(j) % real_bins == energy_bins)) then + t % energy_matches_groups = .false. + end if + end if + ! Set to analog estimator t % estimator = ESTIMATOR_ANALOG case ('delayedgroup') + ! Check to see if running in MG mode, because if so, the current + ! system isnt set up yet to support delayed group data and thus + ! these tallies + if (.not. run_CE) then + call fatal_error("delayedgroup filter on tally " & + // trim(to_str(t % id)) // " not yet supported& + & for multi-group mode.") + end if + ! Set type of filter t % filters(j) % type = FILTER_DELAYEDGROUP @@ -3001,8 +3172,8 @@ contains case default ! Specified tally filter is invalid, raise error call fatal_error("Unknown filter type '" & - &// trim(temp_str) // "' on tally " & - &// trim(to_str(t % id)) // ".") + // trim(temp_str) // "' on tally " & + // trim(to_str(t % id)) // ".") end select @@ -3080,7 +3251,7 @@ contains ! Append default_xs specifier to nuclide if needed if ((default_xs /= '') .and. (.not. ends_with(sarray(j), 'c'))) then - word = trim(word) // "." // default_xs + word = trim(word) // "." // trim(default_xs) end if ! Search through nuclides @@ -3167,12 +3338,12 @@ contains ! maximum order. ! The above scheme will essentially take the absolute value if (master) call warning("Invalid scattering order of " & - &// trim(to_str(n_order)) // " requested. Setting to the & + // trim(to_str(n_order)) // " requested. Setting to the & &maximum permissible value, " & - &// trim(to_str(MAX_ANG_ORDER))) + // trim(to_str(MAX_ANG_ORDER))) n_order = MAX_ANG_ORDER sarray(j) = trim(MOMENT_STRS(imomstr)) & - &// trim(to_str(MAX_ANG_ORDER)) + // trim(to_str(MAX_ANG_ORDER)) end if ! Find total number of bins for this case if (imomstr >= YN_LOC) then @@ -3234,9 +3405,9 @@ contains ! maximum order. ! The above scheme will essentially take the absolute value if (master) call warning("Invalid scattering order of " & - &// trim(to_str(n_order)) // " requested. Setting to & + // trim(to_str(n_order)) // " requested. Setting to & &the maximum permissible value, " & - &// trim(to_str(MAX_ANG_ORDER))) + // trim(to_str(MAX_ANG_ORDER))) n_order = MAX_ANG_ORDER end if score_name = trim(MOMENT_N_STRS(imomstr)) // "n" @@ -3419,6 +3590,12 @@ contains ! Set tally estimator to analog t % estimator = ESTIMATOR_ANALOG end if + + ! Disallow for MG mode since data not present + if (.not. run_CE) then + call fatal_error("Cannot tally delayed nu-fission rate in & + &multi-group mode") + end if case ('kappa-fission') t % score_bins(j) = SCORE_KAPPA_FISSION case ('inverse-velocity') @@ -3564,16 +3741,24 @@ contains t % score_bins(j) = MT else call fatal_error("Invalid MT on : " & - &// trim(sarray(l))) + // trim(sarray(l))) end if else ! Specified score was not an integer call fatal_error("Unknown scoring function: " & - &// trim(sarray(l))) + // trim(sarray(l))) end if end select + + ! Do a check at the end (instead of for every case) to make sure + ! the tallies are compatible with MG mode where we have less detailed + ! nuclear data + if (.not. run_CE .and. t % score_bins(j) > 0) then + call fatal_error("Cannot tally " // trim(score_name) // & + " reaction rate in multi-group mode") + end if end do t % n_score_bins = n_scores @@ -3609,7 +3794,7 @@ contains end do else call fatal_error("No specified on tally " & - &// trim(to_str(t % id)) // ".") + // trim(to_str(t % id)) // ".") end if ! Check for a tally derivative. @@ -3893,7 +4078,7 @@ contains inquire(FILE=filename, EXIST=file_exists) if (.not. file_exists) then call fatal_error("Plots XML file '" // trim(filename) & - &// "' does not exist!") + // "' does not exist!") end if ! Display output message @@ -3925,7 +4110,7 @@ contains ! Check to make sure 'id' hasn't been used if (plot_dict % has_key(pl % id)) then call fatal_error("Two or more plots use the same unique ID: " & - &// to_str(pl % id)) + // to_str(pl % id)) end if ! Copy plot type @@ -3940,7 +4125,7 @@ contains pl % type = PLOT_TYPE_VOXEL case default call fatal_error("Unsupported plot type '" // trim(temp_str) & - &// "' in plot " // trim(to_str(pl % id))) + // "' in plot " // trim(to_str(pl % id))) end select ! Set output file path @@ -3960,14 +4145,14 @@ contains call get_node_array(node_plot, "pixels", pl % pixels(1:2)) else call fatal_error(" must be length 2 in slice plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if else if (pl % type == PLOT_TYPE_VOXEL) then if (get_arraysize_integer(node_plot, "pixels") == 3) then call get_node_array(node_plot, "pixels", pl % pixels(1:3)) else call fatal_error(" must be length 3 in voxel plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if end if @@ -3975,13 +4160,13 @@ contains if (check_for_node(node_plot, "background")) then if (pl % type == PLOT_TYPE_VOXEL) then if (master) call warning("Background color ignored in voxel plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if if (get_arraysize_integer(node_plot, "background") == 3) then call get_node_array(node_plot, "background", pl % not_found % rgb) else call fatal_error("Bad background RGB in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if else pl % not_found % rgb = (/ 255, 255, 255 /) @@ -4002,7 +4187,7 @@ contains pl % basis = PLOT_BASIS_YZ case default call fatal_error("Unsupported plot basis '" // trim(temp_str) & - &// "' in plot " // trim(to_str(pl % id))) + // "' in plot " // trim(to_str(pl % id))) end select end if @@ -4011,7 +4196,7 @@ contains call get_node_array(node_plot, "origin", pl % origin) else call fatal_error("Origin must be length 3 in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if ! Copy plotting width @@ -4020,14 +4205,14 @@ contains call get_node_array(node_plot, "width", pl % width(1:2)) else call fatal_error(" must be length 2 in slice plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if else if (pl % type == PLOT_TYPE_VOXEL) then if (get_arraysize_double(node_plot, "width") == 3) then call get_node_array(node_plot, "width", pl % width(1:3)) else call fatal_error(" must be length 3 in voxel plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if end if @@ -4037,7 +4222,7 @@ contains if (pl % level < 0) then call fatal_error("Bad universe level in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if else pl % level = PLOT_LEVEL_LOWEST @@ -4071,7 +4256,7 @@ contains case default call fatal_error("Unsupported plot color type '" // trim(temp_str) & - &// "' in plot " // trim(to_str(pl % id))) + // "' in plot " // trim(to_str(pl % id))) end select ! Get the number of nodes and get a list of them @@ -4094,7 +4279,7 @@ contains ! Check and make sure 3 values are specified for RGB if (get_arraysize_double(node_col, "rgb") /= 3) then call fatal_error("Bad RGB in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if ! Ensure that there is an id for this color specification @@ -4113,7 +4298,7 @@ contains call get_node_array(node_col, "rgb", pl % colors(col_id) % rgb) else call fatal_error("Could not find cell " // trim(to_str(col_id)) & - &// " specified in plot " // trim(to_str(pl % id))) + // " specified in plot " // trim(to_str(pl % id))) end if else if (pl % color_by == PLOT_COLOR_MATS) then @@ -4123,8 +4308,8 @@ contains call get_node_array(node_col, "rgb", pl % colors(col_id) % rgb) else call fatal_error("Could not find material " & - &// trim(to_str(col_id)) // " specified in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(col_id)) // " specified in plot " & + // trim(to_str(pl % id))) end if end if @@ -4138,7 +4323,7 @@ contains if (pl % type == PLOT_TYPE_VOXEL) then call warning("Meshlines ignored in voxel plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if select case(n_meshlines) @@ -4172,7 +4357,7 @@ contains ! Check and make sure 3 values are specified for RGB if (get_arraysize_double(node_meshlines, "color") /= 3) then call fatal_error("Bad RGB for meshlines color in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if call get_node_array(node_meshlines, "color", & @@ -4189,7 +4374,7 @@ contains if (.not. associated(ufs_mesh)) then call fatal_error("No UFS mesh for meshlines on plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if pl % meshlines_mesh => ufs_mesh @@ -4210,7 +4395,7 @@ contains if (.not. associated(entropy_mesh)) then call fatal_error("No entropy mesh for meshlines on plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if if (.not. allocated(entropy_mesh % dimension)) then @@ -4239,18 +4424,18 @@ contains end if else call fatal_error("Could not find mesh " & - &// trim(to_str(meshid)) // " specified in meshlines for & + // trim(to_str(meshid)) // " specified in meshlines for & &plot " // trim(to_str(pl % id))) end if case default call fatal_error("Invalid type for meshlines on plot " & - &// trim(to_str(pl % id)) // ": " // trim(meshtype)) + // trim(to_str(pl % id)) // ": " // trim(meshtype)) end select case default call fatal_error("Mutliple meshlines specified in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end select end if @@ -4262,13 +4447,13 @@ contains if (pl % type == PLOT_TYPE_VOXEL) then if (master) call warning("Mask ignored in voxel plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if select case(n_masks) case default call fatal_error("Mutliple masks specified in plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) case (1) ! Get pointer to mask @@ -4279,7 +4464,7 @@ contains n_comp = get_arraysize_integer(node_mask, "components") if (n_comp == 0) then call fatal_error("Missing in mask of plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if allocate(iarray(n_comp)) call get_node_array(node_mask, "components", iarray) @@ -4295,7 +4480,7 @@ contains iarray(j) = cell_dict % get_key(col_id) else call fatal_error("Could not find cell " & - &// trim(to_str(col_id)) // " specified in the mask in & + // trim(to_str(col_id)) // " specified in the mask in & &plot " // trim(to_str(pl % id))) end if @@ -4305,7 +4490,7 @@ contains iarray(j) = material_dict % get_key(col_id) else call fatal_error("Could not find material " & - &// trim(to_str(col_id)) // " specified in the mask in & + // trim(to_str(col_id)) // " specified in the mask in & &plot " // trim(to_str(pl % id))) end if @@ -4319,7 +4504,7 @@ contains call get_node_array(node_mask, "background", pl % colors(j) % rgb) else call fatal_error("Missing in mask of plot " & - &// trim(to_str(pl % id))) + // trim(to_str(pl % id))) end if end if end do @@ -4341,11 +4526,11 @@ contains end subroutine read_plots_xml !=============================================================================== -! READ_CROSS_SECTIONS_XML reads information from a cross_sections.xml file. This -! file contains a listing of the ACE cross sections that may be used. +! READ_*_CROSS_SECTIONS_XML reads information from a cross_sections.xml file. This +! file contains a listing of the CE and MG cross sections that may be used. !=============================================================================== - subroutine read_cross_sections_xml() + subroutine read_ce_cross_sections_xml() integer :: i ! loop index integer :: filetype ! default file type @@ -4364,7 +4549,7 @@ contains if (.not. file_exists) then ! Could not find cross_sections.xml file call fatal_error("Cross sections XML file '" & - &// trim(path_cross_sections) // "' does not exist!") + // trim(path_cross_sections) // "' does not exist!") end if call write_message("Reading cross sections XML file...", 5) @@ -4394,7 +4579,7 @@ contains filetype = ASCII else call fatal_error("Unknown filetype in cross_sections.xml: " & - &// trim(temp_str)) + // trim(temp_str)) end if ! copy default record length and entries for binary files @@ -4458,7 +4643,7 @@ contains end if ! determine metastable state - if (.not.check_for_node(node_ace, "metastable")) then + if (.not. check_for_node(node_ace, "metastable")) then listing % metastable = .false. else listing % metastable = .true. @@ -4492,15 +4677,129 @@ contains do i = 1, n_res_scatterers_total if (.not. xs_listing_dict % has_key(trim(nuclides_0K(i) % name_0K))) then call fatal_error("Could not find nuclide " & - &// trim(nuclides_0K(i) % name_0K) & - &// " in cross_sections.xml file!") + // trim(nuclides_0K(i) % name_0K) & + // " in cross_sections.xml file!") end if end do ! Close cross sections XML file call close_xmldoc(doc) - end subroutine read_cross_sections_xml + end subroutine read_ce_cross_sections_xml + + subroutine read_mg_cross_sections_xml() + + integer :: i ! loop index + logical :: file_exists ! does cross_sections.xml exist? + type(XsListing), pointer :: listing => null() + type(Node), pointer :: doc => null() + type(Node), pointer :: node_xsdata => null() + type(NodeList), pointer :: node_xsdata_list => null() + + ! Check if cross_sections.xml exists + inquire(FILE=path_cross_sections, EXIST=file_exists) + if (.not. file_exists) then + ! Could not find cross_sections.xml file + call fatal_error("Cross sections XML file '" & + // trim(path_cross_sections) // "' does not exist!") + end if + + call write_message("Reading cross sections XML file...", 5) + + ! Parse cross_sections.xml file + call open_xmldoc(doc, path_cross_sections) + + if (check_for_node(doc, "groups")) then + ! Get neutron group count + call get_node_value(doc, "groups", energy_groups) + else + call fatal_error("groups element must exist!") + end if + + allocate(energy_bins(energy_groups + 1)) + if (check_for_node(doc, "group_structure")) then + ! Get neutron group structure + call get_node_array(doc, "group_structure", energy_bins) + else + call fatal_error("group_structures element must exist!") + end if + + allocate(energy_bin_avg(energy_groups)) + do i = 1, energy_groups + energy_bin_avg(i) = HALF * (energy_bins(i) + energy_bins(i + 1)) + end do + + allocate(inverse_velocities(energy_groups)) + if (check_for_node(doc, "inverse_velocities")) then + ! Get inverse velocities + call get_node_array(doc, "inverse_velocities", inverse_velocities) + else + ! If not given, estimate them by using average energy in group which is + ! assumed to be the midpoint + do i = 1, energy_groups + inverse_velocities(i) = & + (sqrt(TWO * energy_bin_avg(i) / (MASS_NEUTRON_MEV)) * & + C_LIGHT * 100.0_8) + end do + end if + + ! Get node list of all + call get_node_list(doc, "xsdata", node_xsdata_list) + n_listings = get_list_size(node_xsdata_list) + + ! Allocate xs_listings array + if (n_listings == 0) then + call fatal_error("At least one element must be present in & + &cross_sections.xml file!") + else + allocate(xs_listings(n_listings)) + end if + + do i = 1, n_listings + listing => xs_listings(i) + + ! Get pointer to xsdata table XML node + call get_list_item(node_xsdata_list, i, node_xsdata) + + ! copy a number of attributes + call get_node_value(node_xsdata, "name", listing % name) + listing % name = to_lower(listing % name) + listing % alias = listing % name + if (check_for_node(node_xsdata, "alias")) & + call get_node_value(node_xsdata, "alias", listing % alias) + listing % alias = to_lower(listing % alias) + if (check_for_node(node_xsdata, "zaid")) then + call get_node_value(node_xsdata, "zaid", listing % zaid) + else + listing % zaid = -1 + end if + if (check_for_node(node_xsdata, "awr")) then + call get_node_value(node_xsdata, "awr", listing % awr) + else + ! Set to a default of 1; this allows a macroscopic library to still + ! be used with materials with atom/b-cm units for testing purposes + listing % awr = ONE + end if + if (check_for_node(node_xsdata, "kT")) then + call get_node_value(node_xsdata, "kT", listing % kT) + else + listing % kT = 293.6_8 * K_BOLTZMANN + end if + + ! determine type of cross section + if (ends_with(listing % name, 'c')) then + listing % type = NEUTRON + end if + + ! create dictionary entry for both name and alias + call xs_listing_dict % add_key(to_lower(listing % name), i) + call xs_listing_dict % add_key(to_lower(listing % alias), i) + end do + + ! Close cross sections XML file + call close_xmldoc(doc) + + end subroutine read_mg_cross_sections_xml !=============================================================================== ! EXPAND_NATURAL_ELEMENT converts natural elements specified using an diff --git a/src/interpolation.F90 b/src/interpolation.F90 deleted file mode 100644 index 5f8787067..000000000 --- a/src/interpolation.F90 +++ /dev/null @@ -1,205 +0,0 @@ -module interpolation - - use constants - use endf_header, only: Tab1 - use search, only: binary_search - use string, only: to_str - - implicit none - - interface interpolate_tab1 - module procedure interpolate_tab1_array, interpolate_tab1_object - end interface interpolate_tab1 - -contains - -!=============================================================================== -! INTERPOLATE_TAB1_ARRAY interpolates a function between two points based on -! particular interpolation scheme. The data needs to be organized as a ENDF TAB1 -! type function containing the interpolation regions, break points, and -! tabulated x's and y's. -!=============================================================================== - - pure function interpolate_tab1_array(data, x, loc_start) result(y) - - real(8), intent(in) :: data(:) ! array of data - real(8), intent(in) :: x ! x value to find y at - integer, intent(in), optional :: loc_start ! starting location in data - real(8) :: y ! y(x) - - integer :: i ! bin in which to interpolate - integer :: j ! index for interpolation region - integer :: loc_0 ! starting location - integer :: n_regions ! number of interpolation regions - integer :: n_points ! number of tabulated values - integer :: interp ! ENDF interpolation scheme - integer :: loc_breakpoints ! location of breakpoints in data - integer :: loc_interp ! location of interpolation schemes in data - integer :: loc_x ! location of x's in data - integer :: loc_y ! location of y's in data - real(8) :: r ! interpolation factor - real(8) :: x0, x1 ! bounding x values - real(8) :: y0, y1 ! bounding y values - - ! determine starting location - if (present(loc_start)) then - loc_0 = loc_start - 1 - else - loc_0 = 0 - end if - - ! determine number of interpolation regions - n_regions = int(data(loc_0 + 1)) - - ! set locations for breakpoints and interpolation schemes - loc_breakpoints = loc_0 + 1 - loc_interp = loc_breakpoints + n_regions - - ! determine number of tabulated values - n_points = int(data(loc_interp + n_regions + 1)) - - ! set locations for x's and y's - loc_x = loc_interp + n_regions + 1 - loc_y = loc_x + n_points - - ! find which bin the abscissa is in -- if the abscissa is outside the - ! tabulated range, the first or last point is chosen, i.e. no interpolation - ! is done outside the energy range - if (x < data(loc_x + 1)) then - y = data(loc_y + 1) - return - elseif (x > data(loc_x + n_points)) then - y = data(loc_y + n_points) - return - else - i = binary_search(data(loc_x + 1:loc_x + n_points), n_points, x) - end if - - ! determine interpolation scheme - if (n_regions == 0) then - interp = LINEAR_LINEAR - elseif (n_regions == 1) then - interp = int(data(loc_interp + 1)) - elseif (n_regions > 1) then - do j = 1, n_regions - if (i < data(loc_breakpoints + j)) then - interp = int(data(loc_interp + j)) - exit - end if - end do - end if - - ! handle special case of histogram interpolation - if (interp == HISTOGRAM) then - y = data(loc_y + i) - return - end if - - ! determine bounding values - x0 = data(loc_x + i) - x1 = data(loc_x + i + 1) - y0 = data(loc_y + i) - y1 = data(loc_y + i + 1) - - ! determine interpolation factor and interpolated value - select case (interp) - case (LINEAR_LINEAR) - r = (x - x0)/(x1 - x0) - y = y0 + r*(y1 - y0) - case (LINEAR_LOG) - r = log(x/x0)/log(x1/x0) - y = y0 + r*(y1 - y0) - case (LOG_LINEAR) - r = (x - x0)/(x1 - x0) - y = y0*exp(r*log(y1/y0)) - case (LOG_LOG) - r = log(x/x0)/log(x1/x0) - y = y0*exp(r*log(y1/y0)) - end select - - end function interpolate_tab1_array - -!=============================================================================== -! INTERPOLATE_TAB1_OBJECT interpolates a function between two points based on -! particular interpolation scheme. The data needs to be organized as a ENDF TAB1 -! type function containing the interpolation regions, break points, and -! tabulated x's and y's. -!=============================================================================== - - pure function interpolate_tab1_object(obj, x) result(y) - - type(Tab1), intent(in) :: obj ! ENDF Tab1 interpolable function - real(8), intent(in) :: x ! x value to find y at - real(8) :: y ! y(x) - - integer :: i ! bin in which to interpolate - integer :: j ! index for interpolation region - integer :: n_regions ! number of interpolation regions - integer :: n_pairs ! number of tabulated values - integer :: interp ! ENDF interpolation scheme - real(8) :: r ! interpolation factor - real(8) :: x0, x1 ! bounding x values - real(8) :: y0, y1 ! bounding y values - - ! determine number of interpolation regions and pairs - n_regions = obj % n_regions - n_pairs = obj % n_pairs - - ! find which bin the abscissa is in -- if the abscissa is outside the - ! tabulated range, the first or last point is chosen, i.e. no interpolation - ! is done outside the energy range - if (x < obj % x(1)) then - y = obj % y(1) - return - elseif (x > obj % x(n_pairs)) then - y = obj % y(n_pairs) - return - else - i = binary_search(obj % x, n_pairs, x) - end if - - ! determine interpolation scheme - if (n_regions == 0) then - interp = LINEAR_LINEAR - elseif (n_regions == 1) then - interp = obj % int(1) - elseif (n_regions > 1) then - do j = 1, n_regions - if (i < obj % nbt(j)) then - interp = obj % int(j) - exit - end if - end do - end if - - ! handle special case of histogram interpolation - if (interp == HISTOGRAM) then - y = obj % y(i) - return - end if - - ! determine bounding values - x0 = obj % x(i) - x1 = obj % x(i + 1) - y0 = obj % y(i) - y1 = obj % y(i + 1) - - ! determine interpolation factor and interpolated value - select case (interp) - case (LINEAR_LINEAR) - r = (x - x0)/(x1 - x0) - y = y0 + r*(y1 - y0) - case (LINEAR_LOG) - r = log(x/x0)/log(x1/x0) - y = y0 + r*(y1 - y0) - case (LOG_LINEAR) - r = (x - x0)/(x1 - x0) - y = y0*exp(r*log(y1/y0)) - case (LOG_LOG) - r = log(x/x0)/log(x1/x0) - y = y0*exp(r*log(y1/y0)) - end select - - end function interpolate_tab1_object - -end module interpolation diff --git a/src/macroxs_header.F90 b/src/macroxs_header.F90 new file mode 100644 index 000000000..2a1234510 --- /dev/null +++ b/src/macroxs_header.F90 @@ -0,0 +1,860 @@ +module macroxs_header + + use constants, only: MAX_FILE_LEN, ZERO, ONE, TWO, PI + use list_header, only: ListInt + use material_header, only: material + use math, only: calc_pn, calc_rn, expand_harmonic, find_angle + use nuclide_header + use random_lcg, only: prn + use scattdata_header + + implicit none + +!=============================================================================== +! MACROXS_* contains cached macroscopic cross sections for the material a +! particle is traveling through +!=============================================================================== + + type, abstract :: MacroXS + ! Data Order + integer :: order + + contains + procedure(macroxs_init_), deferred :: init ! initializes object + procedure(macroxs_get_xs_), deferred :: get_xs ! Return xs + ! Sample the outgoing energy from a fission event + procedure(macroxs_sample_fission_), deferred :: sample_fission_energy + ! Sample the outgoing energy and angle from a scatter event + procedure(macroxs_sample_scatter_), deferred :: sample_scatter + ! Calculate the material specific MGXS data from the nuclides + procedure(macroxs_calculate_xs_), deferred :: calculate_xs + end type MacroXS + + abstract interface + subroutine macroxs_init_(this, mat, nuclides, groups, get_kfiss, get_fiss, & + max_order, scatt_type, legendre_mu_points, & + error_code, error_text) + import MacroXS, Material, NuclideMGContainer, MAX_LINE_LEN + class(MacroXS), intent(inout) :: this ! The MacroXS to initialize + type(Material), pointer, intent(in) :: mat ! base material + type(NuclideMGContainer), intent(in) :: nuclides(:) ! List of nuclides to harvest from + integer, intent(in) :: groups ! Number of E groups + logical, intent(in) :: get_kfiss ! Should we get kfiss data? + logical, intent(in) :: get_fiss ! Should we get fiss data? + integer, intent(in) :: max_order ! Maximum requested order + integer, intent(in) :: scatt_type ! Legendre or Tabular Scatt? + integer, intent(in) :: legendre_mu_points ! Treat as Leg or Tabular? + integer, intent(inout) :: error_code ! Code signifying error + character(MAX_LINE_LEN), intent(inout) :: error_text ! Error message to print + end subroutine macroxs_init_ + + function macroxs_get_xs_(this, g, xstype, gout, uvw) result(xs) + import MacroXS + class(MacroXS), intent(in) :: this ! The MacroXS to initialize + integer, intent(in) :: g ! Incoming Energy group + character(*) , intent(in) :: xstype ! Cross Section Type + integer, optional, intent(in) :: gout ! Outgoing Energy group + real(8), optional, intent(in) :: uvw(3) ! Requested Angle + real(8) :: xs ! Resultant xs + end function macroxs_get_xs_ + + function macroxs_sample_fission_(this, gin, uvw) result(gout) + import MacroXS + class(MacroXS), intent(in) :: this ! Data to work with + integer, intent(in) :: gin ! Incoming energy group + real(8), intent(in) :: uvw(3) ! Particle Direction + integer :: gout ! Sampled outgoing group + + end function macroxs_sample_fission_ + + subroutine macroxs_sample_scatter_(this, uvw, gin, gout, mu, wgt) + import MacroXS + class(MacroXS), intent(in) :: this + real(8), intent(in) :: uvw(3) ! Incoming neutron direction + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + end subroutine macroxs_sample_scatter_ + + subroutine macroxs_calculate_xs_(this, gin, uvw, xs) + import MacroXS, MaterialMacroXS + class(MacroXS), intent(in) :: this + integer, intent(in) :: gin ! Incoming neutron group + real(8), intent(in) :: uvw(3) ! Incoming neutron direction + type(MaterialMacroXS), intent(inout) :: xs + end subroutine macroxs_calculate_xs_ + end interface + + type, extends(MacroXS) :: MacroXSIso + ! Microscopic cross sections + real(8), allocatable :: total(:) ! total cross section + real(8), allocatable :: absorption(:) ! absorption cross section + class(ScattData), allocatable :: scatter ! scattering information + real(8), allocatable :: nu_fission(:) ! nu-fission + real(8), allocatable :: k_fission(:) ! kappa-fission + real(8), allocatable :: fission(:) ! fission x/s + real(8), allocatable :: scattxs(:) ! scattering xs + real(8), allocatable :: chi(:,:) ! fission spectra + + contains + procedure :: init => macroxsiso_init ! inits object + procedure :: get_xs => macroxsiso_get_xs ! Returns xs + procedure :: sample_fission_energy => macroxsiso_sample_fission_energy + procedure :: sample_scatter => macroxsiso_sample_scatter + procedure :: calculate_xs => macroxsiso_calculate_xs + end type MacroXSIso + + type, extends(MacroXS) :: MacroXSAngle + ! Macroscopic cross sections + real(8), allocatable :: total(:,:,:) ! total cross section + real(8), allocatable :: absorption(:,:,:) ! absorption cross section + type(ScattDataContainer), allocatable :: scatter(:,:) ! scattering information + real(8), allocatable :: nu_fission(:,:,:) ! nu-fission + real(8), allocatable :: k_fission(:,:,:) ! kappa-fission + real(8), allocatable :: fission(:,:,:) ! fission x/s + real(8), allocatable :: chi(:,:,:,:) ! fission spectra + real(8), allocatable :: scattxs(:,:,:) ! scattering xs + real(8), allocatable :: polar(:) ! polar angles + real(8), allocatable :: azimuthal(:) ! azimuthal angles + + contains + procedure :: init => macroxsangle_init ! inits object + procedure :: get_xs => macroxsangle_get_xs ! Returns xs + procedure :: sample_fission_energy => macroxsangle_sample_fission_energy + procedure :: sample_scatter => macroxsangle_sample_scatter + procedure :: calculate_xs => macroxsangle_calculate_xs + end type MacroXSAngle + +!=============================================================================== +! MACROXSCONTAINER pointer array for storing MacroXS objects. +!=============================================================================== + + type MacroXSContainer + class(MacroXS), allocatable :: obj + end type MacroXSContainer + +contains + +!=============================================================================== +! MACROXS*_INIT sets the MacroXS Data +!=============================================================================== + + subroutine macroxsiso_init(this, mat, nuclides, groups, get_kfiss, get_fiss, & + max_order, scatt_type, legendre_mu_points, error_code, error_text) + class(MacroXSIso), intent(inout) :: this ! The MacroXS to initialize + type(Material), pointer, intent(in) :: mat ! base material + type(NuclideMGContainer), intent(in) :: nuclides(:) ! List of nuclides to harvest from + integer, intent(in) :: groups ! Number of E groups + logical, intent(in) :: get_kfiss ! Should we get kfiss data? + logical, intent(in) :: get_fiss ! Should we get fiss data? + integer, intent(in) :: max_order ! Maximum requested order + integer, intent(in) :: scatt_type ! How is data presented + integer, intent(in) :: legendre_mu_points ! Treat as Leg or Tabular? + integer, intent(inout) :: error_code ! Code signifying error + character(MAX_LINE_LEN), intent(inout) :: error_text ! Error message to print + + integer :: i ! loop index over nuclides + integer :: gin, gout ! group indices + real(8) :: atom_density ! atom density of a nuclide + integer :: imu + real(8) :: norm + integer :: mat_max_order, order, l + real(8), allocatable :: temp_mult(:,:) + real(8), allocatable :: temp_energy(:,:) + real(8), allocatable :: scatt_coeffs(:,:,:) + + ! Initialize error data + error_code = 0 + error_text = '' + + ! If we have tabular only data, then make sure all datasets have same size + if (scatt_type == ANGLE_HISTOGRAM) then + ! Check all scattering data of same size + order = nuclides(mat % nuclide(1)) % obj % order + do i = 2, mat % n_nuclides + if (order /= nuclides(mat % nuclide(i)) % obj % order) then + error_code = 1 + error_text = "All Histogram Scattering Entries Must Be Same Length!" + return + end if + end do + ! Ok, got our order, store it + this % order = order + + ! Allocate stuff for later + allocate(scatt_coeffs(order, groups, groups)) + scatt_coeffs = ZERO + allocate(ScattDataHistogram :: this % scatter) + + else if (scatt_type == ANGLE_TABULAR) then + ! Check all scattering data of same size + order = nuclides(mat % nuclide(1)) % obj % order + do i = 2, mat % n_nuclides + if (order /= nuclides(mat % nuclide(i)) % obj % order) then + error_code = 1 + error_text = "All Tabular Scattering Entries Must Be Same Length!" + return + end if + end do + ! Ok, got our order, store it + this % order = order + + ! Allocate stuff for later + allocate(scatt_coeffs(order, groups, groups)) + scatt_coeffs = ZERO + allocate(ScattDataTabular :: this % scatter) + + else if (scatt_type == ANGLE_LEGENDRE) then + ! Otherwise find the maximum scattering order + ! Need to determine the maximum scattering order of all data in this material + mat_max_order = 0 + do i = 1, mat % n_nuclides + if (nuclides(mat % nuclide(i)) % obj % order > mat_max_order) then + mat_max_order = nuclides(mat % nuclide(i)) % obj % order + end if + end do + + ! Now need to compare this material maximum scattering order with + ! the problem wide max scatt order and use whichever is lower + order = min(mat_max_order, max_order) + this % order = order + 1 + + ! Now we can allocate our scatt_coeffs object accordingly + allocate(scatt_coeffs(order + 1, groups, groups)) + scatt_coeffs = ZERO + if (legendre_mu_points == 1) then + allocate(ScattDataLegendre :: this % scatter) + else + allocate(ScattDataTabular :: this % scatter) + end if + end if + + ! Allocate and initialize data within macro_xs(i_mat) object + allocate(this % total(groups)) + this % total = ZERO + allocate(this % absorption(groups)) + this % absorption = ZERO + if (get_fiss) then + allocate(this % fission(groups)) + this % fission = ZERO + end if + if (get_kfiss) then + allocate(this % k_fission(groups)) + this % k_fission = ZERO + end if + allocate(this % nu_fission(groups)) + this % nu_fission = ZERO + allocate(this % chi(groups, groups)) + this % chi = ZERO + allocate(temp_energy(groups, groups)) + temp_energy = ZERO + allocate(temp_mult(groups, groups)) + temp_mult = ZERO + allocate(this % scattxs(groups)) + + ! Add contribution from each nuclide in material + do i = 1, mat % n_nuclides + ! Copy atom density of nuclide in material + atom_density = mat % atom_density(i) + + ! Perform our operations which depend upon the type + select type(nuc => nuclides(mat % nuclide(i)) % obj) + type is (NuclideIso) + + ! Add contributions to total, absorption, and fission data (if necessary) + this % total = this % total + atom_density * nuc % total + this % absorption = this % absorption + & + atom_density * nuc % absorption + if (nuc % fissionable) then + if (allocated(nuc % chi)) then + do gin = 1, groups + do gout = 1, groups + this % chi(gout,gin) = this % chi(gout,gin) + atom_density * & + nuc % chi(gout) * nuc % nu_fission(gin,1) + end do + end do + this % nu_fission = this % nu_fission + atom_density * & + nuc % nu_fission(:,1) + else + this % chi = this % chi + atom_density * nuc % nu_fission + do gin = 1, groups + this % nu_fission(gin) = this % nu_fission(gin) + atom_density * & + sum(nuc % nu_fission(:,gin)) + end do + end if + if (get_fiss) then + this % fission = this % fission + atom_density * nuc % fission + end if + if (get_kfiss) then + this % k_fission = this % k_fission + atom_density * nuc % k_fission + end if + end if + + ! Now time to do the scattering + do gin = 1, groups + do gout = 1, groups + if (scatt_type == ANGLE_HISTOGRAM .or. scatt_type == ANGLE_TABULAR) then + ! Transfer matrix + temp_energy(gout,gin) = temp_energy(gout,gin) + atom_density * & + sum(nuc % scatter(gout,gin,:)) + + ! Determine the angular distribution + do imu = 1, order + scatt_coeffs(imu, gout, gin) = scatt_coeffs(imu, gout, gin) + & + nuc % scatter(gout,gin,imu) * & + atom_density + end do + + else if (scatt_type == ANGLE_LEGENDRE) then + ! Transfer matrix + temp_energy(gout,gin) = temp_energy(gout,gin) + atom_density * & + nuc % scatter(gout,gin,1) + + ! Determine the angular distribution coefficients so we can later + ! expand do the complete distribution + do l = 1, min(nuc % order, order) + 1 + scatt_coeffs(l, gout, gin) = scatt_coeffs(l, gout, gin) + & + nuc % scatter(gout,gin,l) * & + atom_density + end do + + end if + + ! Multiplicity matrix + temp_mult(gout,gin) = temp_mult(gout,gin) + atom_density * & + nuc % mult(gout,gin) + end do + end do + type is (NuclideAngle) + error_code = 1 + error_text = "Invalid Passing of NuclideAngle to MacroXSIso Object" + return + end select + end do + + ! Store the scattering xs + if (scatt_type == ANGLE_HISTOGRAM .or. scatt_type == ANGLE_TABULAR) then + this % scattxs(:) = sum(sum(scatt_coeffs(:,:,:),dim=1),dim=1) + else if (scatt_type == ANGLE_LEGENDRE) then + this % scattxs(:) = sum(scatt_coeffs(1,:,:),dim=1) + end if + + ! Normalize the scatt_coeffs + do gin = 1, groups + do gout = 1, groups + if (scatt_type == ANGLE_HISTOGRAM .or. scatt_type == ANGLE_TABULAR) then + norm = sum(scatt_coeffs(:,gout,gin)) + else if (scatt_type == ANGLE_LEGENDRE) then + norm = scatt_coeffs(1,gout,gin) + end if + if (norm /= ZERO) then + scatt_coeffs(:, gout, gin) = scatt_coeffs(:, gout,gin) / norm + end if + end do + ! Now normalize temp_energy (outgoing scattering energy probabilities) + norm = sum(temp_energy(:,gin)) + if (norm > ZERO) then + temp_energy(:,gin) = temp_energy(:,gin) / norm + end if + end do + + if (scatt_type == ANGLE_LEGENDRE .and. legendre_mu_points /= 1) then + call this % scatter % init(legendre_mu_points, temp_energy, temp_mult, & + scatt_coeffs) + else + call this % scatter % init(this % order, temp_energy, temp_mult, & + scatt_coeffs) + end if + + ! Now normalize chi + if (mat % fissionable) then + do gin = 1, groups + ! Normalize Chi + norm = sum(this % chi(:,gin)) + if (norm > ZERO) then + this % chi(:,gin) = this % chi(:,gin) / norm + end if + end do + end if + + ! Deallocate temporaries for the next material + deallocate(scatt_coeffs, temp_energy, temp_mult) + + end subroutine macroxsiso_init + + subroutine macroxsangle_init(this, mat, nuclides, groups, get_kfiss, get_fiss, & + max_order, scatt_type, legendre_mu_points, error_code, error_text) + class(MacroXSAngle), intent(inout) :: this ! The MacroXS to initialize + type(Material), pointer, intent(in) :: mat ! base material + type(NuclideMGContainer), intent(in) :: nuclides(:) ! List of nuclides to harvest from + integer, intent(in) :: groups ! Number of E groups + logical, intent(in) :: get_kfiss ! Should we get kfiss data? + logical, intent(in) :: get_fiss ! Should we get fiss data? + integer, intent(in) :: max_order ! Maximum requested order + integer, intent(in) :: scatt_type ! Legendre or Tabular Scatt? + integer, intent(in) :: legendre_mu_points ! Treat as Leg or Tabular? + integer, intent(inout) :: error_code ! Code signifying error + character(MAX_LINE_LEN), intent(inout) :: error_text ! Error message to print + + integer :: i ! loop index over nuclides + integer :: gin, gout ! group indices + real(8) :: atom_density ! atom density of a nuclide + integer :: ipol, iazi, npol, nazi + integer :: imu + real(8) :: norm + integer :: mat_max_order, order, l + real(8), allocatable :: temp_mult(:,:,:,:) + real(8), allocatable :: temp_energy(:,:,:,:) + real(8), allocatable :: scatt_coeffs(:,:,:,:,:) + + ! Initialize error data + error_code = 0 + error_text = '' + + ! Get the number of each polar and azi angles and make sure all the + ! NuclideAngle types have the same number of these angles + npol = -1 + nazi = -1 + do i = 1, mat % n_nuclides + select type(nuc => nuclides(mat % nuclide(i)) % obj) + type is (NuclideAngle) + if (npol == -1) then + npol = nuc % n_pol + nazi = nuc % n_azi + allocate(this % polar(npol)) + this % polar = nuc % polar + allocate(this % azimuthal(nazi)) + this % azimuthal = nuc % azimuthal + else + if ((npol /= nuc % n_pol) .or. (nazi /= nuc % n_azi)) then + error_code = 1 + error_text = "All Angular Data Must Be Same Length!" + end if + end if + end select + end do + + ! If we have tabular only data, then make sure all datasets have same size + if (scatt_type == ANGLE_HISTOGRAM) then + ! Check all scattering data of same size + order = nuclides(mat % nuclide(1)) % obj % order + do i = 2, mat % n_nuclides + if (order /= nuclides(mat % nuclide(i)) % obj % order) then + error_code = 1 + error_text = "All Histogram Scattering Entries Must Be Same Length!" + return + end if + end do + ! Ok, got our order, store it + this % order = order + + ! Allocate stuff for later + allocate(scatt_coeffs(order, groups, groups, nazi, npol)) + scatt_coeffs = ZERO + allocate(this % scatter(nazi, npol)) + do ipol = 1, npol + do iazi = 1, nazi + allocate(ScattDataHistogram :: this % scatter(iazi, ipol) % obj) + end do + end do + + else if (scatt_type == ANGLE_TABULAR) then + ! Check all scattering data of same size + order = nuclides(mat % nuclide(1)) % obj % order + do i = 2, mat % n_nuclides + if (order /= nuclides(mat % nuclide(i)) % obj % order) then + error_code = 1 + error_text = "All Tabular Scattering Entries Must Be Same Length!" + return + end if + end do + ! Ok, got our order, store it + this % order = order + + ! Allocate stuff for later + allocate(scatt_coeffs(order, groups, groups, nazi, npol)) + scatt_coeffs = ZERO + allocate(this % scatter(nazi, npol)) + do ipol = 1, npol + do iazi = 1, nazi + allocate(ScattDataTabular :: this % scatter(iazi, ipol) % obj) + end do + end do + + else if (scatt_type == ANGLE_LEGENDRE) then + ! Otherwise find the maximum scattering order + ! Need to determine the maximum scattering order of all data in this material + mat_max_order = 0 + do i = 1, mat % n_nuclides + if (nuclides(mat % nuclide(i)) % obj % order > mat_max_order) then + mat_max_order = nuclides(mat % nuclide(i)) % obj % order + end if + end do + + ! Now need to compare this material maximum scattering order with + ! the problem wide max scatt order and use whichever is lower + order = min(mat_max_order, max_order) + this % order = order + 1 + + ! Now we can allocate our scatt_coeffs object accordingly + allocate(scatt_coeffs(order + 1, groups, groups, nazi, npol)) + scatt_coeffs = ZERO + allocate(this % scatter(nazi, npol)) + do ipol = 1, npol + do iazi = 1, nazi + if (legendre_mu_points == 1) then + allocate(ScattDataLegendre :: this % scatter(iazi, ipol) % obj) + else + allocate(ScattDataTabular :: this % scatter(iazi, ipol) % obj) + end if + end do + end do + end if + + ! Allocate and initialize data within macro_xs(i_mat) object + allocate(this % total(groups,nazi,npol)) + this % total = ZERO + allocate(this % absorption(groups,nazi,npol)) + this % absorption = ZERO + if (get_fiss) then + allocate(this % fission(groups,nazi,npol)) + this % fission = ZERO + end if + if (get_kfiss) then + allocate(this % k_fission(groups,nazi,npol)) + this % k_fission = ZERO + end if + allocate(this % nu_fission(groups,nazi,npol)) + this % nu_fission = ZERO + allocate(this % chi(groups, groups, nazi, npol)) + this % chi = ZERO + allocate(temp_energy(groups,groups,nazi,npol)) + temp_energy = ZERO + allocate(temp_mult(groups,groups,nazi,npol)) + temp_mult = ZERO + allocate(this % scattxs(groups,nazi,npol)) + + ! Add contribution from each nuclide in material + do i = 1, mat % n_nuclides + ! Copy atom density of nuclide in material + atom_density = mat % atom_density(i) + + ! Perform our operations which depend upon the type + select type(nuc => nuclides(mat % nuclide(i)) % obj) + type is (NuclideIso) + error_code = 1 + error_text = "Invalid Passing of NuclideIso to MacroXSAngle Object" + return + type is (NuclideAngle) + ! Add contributions to total, absorption, and fission data (if necessary) + this % total = this % total + atom_density * nuc % total + this % absorption = this % absorption + & + atom_density * nuc % absorption + if (nuc % fissionable) then + if (allocated(nuc % chi)) then + do gin = 1, groups + do gout = 1, groups + this % chi(gout,gin,:,:) = this % chi(gout,gin,:,:) + atom_density * & + nuc % chi(gout,:,:) * nuc % nu_fission(gin,1,:,:) + end do + end do + this % nu_fission = this % nu_fission + atom_density * & + nuc % nu_fission(:,1,:,:) + else + this % chi = this % chi + atom_density * nuc % nu_fission + do gin = 1, groups + this % nu_fission(gin,:,:) = this % nu_fission(gin,:,:) + atom_density * & + sum(nuc % nu_fission(:,gin,:,:),dim=1) + end do + end if + if (get_fiss) then + this % fission = this % fission + atom_density * nuc % fission + end if + if (get_kfiss) then + this % k_fission = this % k_fission + atom_density * nuc % k_fission + end if + end if + + ! Now time to do the scattering + do gin = 1, groups + do gout = 1, groups + if (scatt_type == ANGLE_HISTOGRAM .or. scatt_type == ANGLE_TABULAR) then + ! Transfer matrix + temp_energy(gout,gin,:,:) = temp_energy(gout,gin,:,:) + atom_density * & + sum(nuc % scatter(gout,gin,:,:,:),dim=1) + + ! Determine the angular distribution + do imu = 1, order + scatt_coeffs(imu,gout,gin,:,:) = scatt_coeffs(imu,gout,gin,:,:) + & + nuc % scatter(gout,gin,imu,:,:) * & + atom_density + end do + else if (scatt_type == ANGLE_LEGENDRE) then + ! Transfer matrix + temp_energy(gout,gin,:,:) = temp_energy(gout,gin,:,:) + atom_density * & + nuc % scatter(gout,gin,1,:,:) + + ! Determine the angular distribution coefficients so we can later + ! expand do the complete distribution + do l = 1, min(nuc % order, order) + 1 + scatt_coeffs(l, gout, gin,:,:) = scatt_coeffs(l, gout, gin,:,:) + & + nuc % scatter(gout,gin,l,:,:) * & + atom_density + end do + end if + + ! Multiplicity matrix + temp_mult(gout,gin,:,:) = temp_mult(gout,gin,:,:) + atom_density * & + nuc % mult(gout,gin,:,:) + end do + end do + end select + end do + + ! Store the scattering xs + if (scatt_type == ANGLE_HISTOGRAM .or. scatt_type == ANGLE_TABULAR) then + this % scattxs(:,:,:) = sum(sum(scatt_coeffs(:,:,:,:,:),dim=1),dim=1) + else if (scatt_type == ANGLE_LEGENDRE) then + this % scattxs(:,:,:) = sum(scatt_coeffs(1,:,:,:,:),dim=1) + end if + + ! Normalize the scatt_coeffs + do ipol = 1, npol + do iazi = 1, nazi + do gin = 1, groups + do gout = 1, groups + if (scatt_type == ANGLE_HISTOGRAM .or. scatt_type == ANGLE_TABULAR) then + norm = sum(scatt_coeffs(:,gout,gin,iazi,ipol)) + else if (scatt_type == ANGLE_LEGENDRE) then + norm = scatt_coeffs(1,gout,gin,iazi,ipol) + end if + if (norm /= ZERO) then + scatt_coeffs(:,gout,gin,iazi,ipol) = & + scatt_coeffs(:,gout,gin,iazi,ipol) / norm + end if + end do + ! Now normalize temp_energy (outgoing scattering energy probabilities) + norm = sum(temp_energy(:,gin,iazi,ipol)) + if (norm > ZERO) then + temp_energy(:,gin,iazi,ipol) = temp_energy(:,gin,iazi,ipol) / norm + end if + end do + + if (scatt_type == ANGLE_LEGENDRE .and. legendre_mu_points /= 1) then + call this % scatter(iazi, ipol) % obj % init(legendre_mu_points, & + temp_energy(:,:,iazi,ipol), temp_mult(:,:,iazi,ipol), & + scatt_coeffs(:,:,:,iazi,ipol)) + else + call this % scatter(iazi, ipol) % obj % init(this % order, & + temp_energy(:,:,iazi,ipol), temp_mult(:,:,iazi,ipol), & + scatt_coeffs(:,:,:,iazi,ipol)) + end if + + end do + end do + + ! Now go through and normalize chi + if (mat % fissionable) then + do ipol = 1, npol + do iazi = 1, nazi + do gin = 1, groups + ! Normalize Chi + norm = sum(this % chi(:,gin,iazi,ipol)) + if (norm > ZERO) then + this % chi(:,gin,iazi,ipol) = this % chi(:,gin,iazi,ipol) / norm + end if + end do + end do + end do + end if + + ! Deallocate temporaries for the next material + deallocate(scatt_coeffs, temp_energy, temp_mult) + + end subroutine macroxsangle_init + +!=============================================================================== +! MACROXS_*_GET_XS returns the requested data type +!=============================================================================== + + function macroxsiso_get_xs(this, g, xstype, gout, uvw) result(xs) + class(MacroXSIso), intent(in) :: this ! The MacroXS to initialize + integer, intent(in) :: g ! Incoming Energy group + character(*) , intent(in) :: xstype ! Type of xs requested + integer, optional, intent(in) :: gout ! Outgoing Energy group + real(8), optional, intent(in) :: uvw(3) ! Requested Angle + real(8) :: xs ! Requested x/s + + select case(xstype) + case('total') + xs = this % total(g) + case('absorption') + xs = this % absorption(g) + case('fission') + xs = this % fission(g) + case('k_fission') + xs = this % k_fission(g) + case('nu_fission') + xs = this % nu_fission(g) + case('scatter') + xs = this % scattxs(g) + case('mult') + if (present(gout)) then + xs = this % scatter % mult(gout,g) + else + xs = sum(this % scatter % mult(:,g)) + end if + end select + + end function macroxsiso_get_xs + + function macroxsangle_get_xs(this, g, xstype, gout,uvw) result(xs) + class(MacroXSAngle), intent(in) :: this ! The MacroXS to initialize + integer, intent(in) :: g ! Incoming Energy group + character(*) , intent(in) :: xstype ! Type of xs requested + integer, optional, intent(in) :: gout ! Outgoing Energy group + real(8), optional, intent(in) :: uvw(3) ! Requested Angle + real(8) :: xs ! Requested x/s + + integer :: iazi, ipol + + if (present(uvw)) then + call find_angle(this % polar, this % azimuthal, uvw, iazi, ipol) + select case(xstype) + case('total') + xs = this % total(g,iazi,ipol) + case('absorption') + xs = this % absorption(g,iazi,ipol) + case('fission') + xs = this % fission(g,iazi,ipol) + case('k_fission') + xs = this % k_fission(g,iazi,ipol) + case('nu_fission') + xs = this % nu_fission(g,iazi,ipol) + case('scatter') + xs = this % scattxs(g,iazi,ipol) + case('mult') + if (present(gout)) then + xs = this % scatter(iazi,ipol) % obj % mult(gout,g) + else + xs = sum(this % scatter(iazi,ipol) % obj % mult(:,g)) + end if + end select + end if + + end function macroxsangle_get_xs + +!=============================================================================== +! MACROXS_*_SAMPLE_FISSION_ENERGY samples the outgoing energy from a fission +! event +!=============================================================================== + + function macroxsiso_sample_fission_energy(this, gin, uvw) result(gout) + class(MacroXSIso), intent(in) :: this ! Data to work with + integer, intent(in) :: gin ! Incoming energy group + real(8), intent(in) :: uvw(3) ! Particle Direction + integer :: gout ! Sampled outgoing group + real(8) :: xi ! Our random number + real(8) :: prob ! Running probability + + xi = prn() + prob = ZERO + gout = 0 + + do while (prob < xi) + gout = gout + 1 + prob = prob + this % chi(gout,gin) + end do + + end function macroxsiso_sample_fission_energy + + function macroxsangle_sample_fission_energy(this, gin, uvw) result(gout) + class(MacroXSAngle), intent(in) :: this ! Data to work with + integer, intent(in) :: gin ! Incoming energy group + real(8), intent(in) :: uvw(3) ! Particle Direction + integer :: gout ! Sampled outgoing group + real(8) :: xi ! Our random number + real(8) :: prob ! Running probability + integer :: iazi, ipol + + call find_angle(this % polar, this % azimuthal, uvw, iazi, ipol) + + xi = prn() + prob = ZERO + gout = 0 + + do while (prob < xi) + gout = gout + 1 + prob = prob + this % chi(gout,gin,iazi,ipol) + end do + + end function macroxsangle_sample_fission_energy + +!=============================================================================== +! MACROXS*_SAMPLE_SCATTER Selects outgoing energy and angle after a scatter +! event +!=============================================================================== + + subroutine macroxsiso_sample_scatter(this, uvw, gin, gout, mu, wgt) + class(MacroXSIso), intent(in) :: this + real(8), intent(in) :: uvw(3) ! Incoming neutron direction + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + + call this % scatter % sample(gin, gout, mu, wgt) + + end subroutine macroxsiso_sample_scatter + + subroutine macroxsangle_sample_scatter(this, uvw, gin, gout, mu, wgt) + class(MacroXSAngle), intent(in) :: this + real(8), intent(in) :: uvw(3) ! Incoming neutron direction + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + + integer :: iazi, ipol ! Angular indices + + call find_angle(this % polar, this % azimuthal, uvw, iazi, ipol) + call this % scatter(iazi,ipol) % obj % sample(gin,gout,mu,wgt) + + end subroutine macroxsangle_sample_scatter + +!=============================================================================== +! MACROXS*_CALCULATE_XS determines the multi-group macroscopic cross sections +! for the material the particle is currently traveling through. +!=============================================================================== + + subroutine macroxsiso_calculate_xs(this, gin, uvw, xs) + class(MacroXSIso), intent(in) :: this + integer, intent(in) :: gin ! Incoming neutron group + real(8), intent(in) :: uvw(3) ! Incoming neutron direction + type(MaterialMacroXS), intent(inout) :: xs ! Resultant MacroXS Data + + xs % total = this % total(gin) + xs % elastic = this % scattxs(gin) + xs % absorption = this % absorption(gin) + xs % nu_fission = this % nu_fission(gin) + + end subroutine macroxsiso_calculate_xs + + subroutine macroxsangle_calculate_xs(this, gin, uvw, xs) + class(MacroXSAngle), intent(in) :: this + integer, intent(in) :: gin ! Incoming neutron group + real(8), intent(in) :: uvw(3) ! Incoming neutron direction + type(MaterialMacroXS), intent(inout) :: xs ! Resultant MacroXS Data + + integer :: iazi, ipol + + call find_angle(this % polar, this % azimuthal, uvw, iazi, ipol) + xs % total = this % total(gin, iazi, ipol) + xs % elastic = this % scattxs(gin, iazi, ipol) + xs % absorption = this % absorption(gin, iazi, ipol) + xs % nu_fission = this % nu_fission(gin, iazi, ipol) + + end subroutine macroxsangle_calculate_xs + +end module macroxs_header diff --git a/src/math.F90 b/src/math.F90 index f3247fb4a..dfaa903f4 100644 --- a/src/math.F90 +++ b/src/math.F90 @@ -573,6 +573,49 @@ contains end function calc_rn +!=============================================================================== +! EXPAND_HARMONIC expands a given series of real spherical harmonics +!=============================================================================== + + pure function expand_harmonic(data, order, uvw) result(val) + real(8), intent(in) :: data(:) + integer, intent(in) :: order + real(8), intent(in) :: uvw(3) + real(8) :: val + + integer :: l, lm_lo, lm_hi + + val = data(1) + lm_lo = 2 + lm_hi = 4 + do l = 1, order - 1 + val = val + sqrt(TWO * real(l,8) + ONE) * & + dot_product(calc_rn(l,uvw), data(lm_lo:lm_hi)) + lm_lo = lm_hi + 1 + lm_hi = lm_lo + 2 * (l + 1) + end do + + end function expand_harmonic + +!=============================================================================== +! EVALUATE_LEGENDRE Find the value of f(x) given a set of Legendre coefficients +! and the value of x +!=============================================================================== + + pure function evaluate_legendre(data, x) result(val) + real(8), intent(in) :: data(:) + real(8), intent(in) :: x + real(8) :: val + + integer :: l + + val = HALF * data(1) + do l = 1, size(data) - 1 + val = val + (real(l,8) + HALF) * data(l + 1) * calc_pn(l,x) + end do + + end function evaluate_legendre + !=============================================================================== ! ROTATE_ANGLE rotates direction cosines through a polar angle whose cosine is ! mu and through an azimuthal angle sampled uniformly. Note that this is done @@ -676,13 +719,14 @@ contains end function watt_spectrum !=============================================================================== -! W acts as a front end to the MIT Faddeeva function, Faddeeva_w. +! FADDEEVA the Faddeeva function, using Stephen Johnson's implementation !=============================================================================== - function w(z) result(wv) + function faddeeva(z) result(wv) complex(C_DOUBLE_COMPLEX), intent(in) :: z ! The point to evaluate Z at complex(8) :: wv ! The resulting w(z) value - real(C_DOUBLE) :: relerr ! Target relative error in inner loop of MIT Faddeeva + real(C_DOUBLE) :: relerr ! Target relative error in inner loop of MIT + ! Faddeeva ! Technically, the value we want is given by the equation: ! w(z) = I/Pi * Integrate[Exp[-t^2]/(z-t), {t, -Infinity, Infinity}] @@ -697,13 +741,16 @@ contains ! For imag(z) > 0, w_int(z) = w_fun(z) ! For imag(z) < 0, w_int(z) = -conjg(w_fun(conjg(z))) + ! Note that faddeeva_w will interpret zero as machine epsilon + relerr = ZERO if (aimag(z) > ZERO) then wv = faddeeva_w(z, relerr) else wv = -conjg(faddeeva_w(conjg(z), relerr)) end if - end function w + + end function faddeeva recursive function w_derivative(z, order) result(wv) complex(C_DOUBLE_COMPLEX), intent(in) :: z ! The point to evaluate Z at @@ -712,9 +759,9 @@ contains select case(order) case (0) - wv = w(z) + wv = faddeeva(z) case (1) - wv = -TWO * z * w(z) + TWO * ONEI / SQRT_PI + wv = -TWO * z * faddeeva(z) + TWO * ONEI / SQRT_PI case default wv = -TWO * z * w_derivative(z, order-1) & - TWO * (order-1) * w_derivative(z, order-2) @@ -722,20 +769,21 @@ contains end function w_derivative !=============================================================================== -! BROADEN_N_POLYNOMIALS doppler broadens polynomials of the form +! BROADEN_WMP_POLYNOMIALS Doppler broadens the windowed multipole curvefit. The +! curvefit is a polynomial of the form ! a/En + b/sqrt(En) + c + d sqrt(En) ... -! exactly and quickly. !=============================================================================== - subroutine broaden_n_polynomials(En, dopp, n, factors) + subroutine broaden_wmp_polynomials(En, dopp, n, factors) real(8), intent(in) :: En ! Energy to evaluate at - real(8), intent(in) :: dopp ! sqrt(atomic weight ratio / kT), kT given in eV. + real(8), intent(in) :: dopp ! sqrt(atomic weight ratio / kT), + ! kT given in eV. integer, intent(in) :: n ! number of components to polynomial real(8), intent(out):: factors(n) ! output leading coefficient integer :: i - real(8) :: sqrtE ! Sqrt(energy) + real(8) :: sqrtE ! sqrt(energy) real(8) :: beta ! sqrt(atomic weight ratio * E / kT) real(8) :: half_inv_dopp2 ! 0.5 / dopp**2 real(8) :: quarter_inv_dopp4 ! 0.25 / dopp**4 @@ -762,19 +810,46 @@ contains factors(1) = erfbeta / En factors(2) = ONE / sqrtE - factors(3) = factors(1) * (half_inv_dopp2 + En) + exp_m_beta2 / (beta * SQRT_PI) + factors(3) = factors(1) * (half_inv_dopp2 + En) & + + exp_m_beta2 / (beta * SQRT_PI) ! Perform recursive broadening of high order components do i = 1, n-3 if (i /= 1) then - factors(i+3) = -factors(i-1) * (i - ONE) * i * quarter_inv_dopp4 + & - factors(i+1) * (En + (ONE + TWO * i) * half_inv_dopp2) + factors(i+3) = -factors(i-1) * (i - ONE) * i * quarter_inv_dopp4 & + + factors(i+1) * (En + (ONE + TWO * i) * half_inv_dopp2) else ! Although it's mathematically identical, factors(0) will contain ! nothing, and we don't want to have to worry about memory. factors(i+3) = factors(i+1)*(En + (ONE + TWO * i) * half_inv_dopp2) end if end do - end subroutine broaden_n_polynomials + end subroutine broaden_wmp_polynomials + +!=============================================================================== +! find_angle finds the closest angle on the data grid and returns that index +!=============================================================================== + + pure subroutine find_angle(polar, azimuthal, uvw, i_azi, i_pol) + real(8), intent(in) :: polar(:) ! Polar angles [0,pi] + real(8), intent(in) :: azimuthal(:) ! Azi. angles [-pi,pi] + real(8), intent(in) :: uvw(3) ! Direction of motion + integer, intent(inout) :: i_pol ! Closest polar bin + integer, intent(inout) :: i_azi ! Closest azi bin + + real(8) :: my_pol, my_azi, dangle + + ! Convert uvw to polar and azi + + my_pol = acos(uvw(3)) + my_azi = atan2(uvw(2), uvw(1)) + + ! Search for equi-binned angles + dangle = PI / real(size(polar),8) + i_pol = floor(my_pol / dangle + ONE) + dangle = TWO * PI / real(size(azimuthal),8) + i_azi = floor((my_azi + PI) / dangle + ONE) + + end subroutine find_angle end module math diff --git a/src/mesh.F90 b/src/mesh.F90 index 905772eb0..4ec84345b 100644 --- a/src/mesh.F90 +++ b/src/mesh.F90 @@ -3,7 +3,6 @@ module mesh use constants use global use mesh_header - use particle_header, only: Particle use search, only: binary_search #ifdef MPI @@ -160,10 +159,10 @@ contains sites_outside) type(RegularMesh), pointer :: m ! mesh to count sites - type(Bank), intent(in) :: bank_array(:) ! fission or source bank - real(8), intent(out) :: cnt(:,:,:,:) ! weight of sites in each + type(Bank), intent(in) :: bank_array(:) ! fission or source bank + real(8), intent(out) :: cnt(:,:,:,:) ! weight of sites in each ! cell and energy group - real(8), intent(in), optional :: energies(:) ! energy grid to search + real(8), intent(in), optional :: energies(:) ! energy grid to search integer(8), intent(in), optional :: size_bank ! # of bank sites (on each proc) logical, intent(inout), optional :: sites_outside ! were there sites outside mesh? diff --git a/src/mgxs_data.F90 b/src/mgxs_data.F90 new file mode 100644 index 000000000..08941870c --- /dev/null +++ b/src/mgxs_data.F90 @@ -0,0 +1,224 @@ +module mgxs_data + +use constants + use error, only: fatal_error + use global + use macroxs_header + use material_header, only: Material + use nuclide_header + use output, only: write_message + use set_header, only: SetChar + use string, only: to_lower + use xml_interface + + implicit none + +contains + +!=============================================================================== +! READ_XS reads all the cross sections for the problem and stores them in +! nuclides and sab_tables arrays +!=============================================================================== + + subroutine read_mgxs() + + integer :: i ! index in materials array + integer :: j ! index over nuclides in material + integer :: i_listing ! index in xs_listings array + integer :: i_nuclide ! index in nuclides + character(12) :: name ! name of isotope, e.g. 92235.03c + character(12) :: alias ! alias of isotope, e.g. U-235.03c + integer :: representation ! Data representation + type(Material), pointer :: mat + type(SetChar) :: already_read + type(Node), pointer :: doc => null() + type(Node), pointer :: node_xsdata + type(NodeList), pointer :: node_xsdata_list => null() + logical :: file_exists + character(MAX_LINE_LEN) :: temp_str + logical :: get_kfiss, get_fiss + integer :: l + + ! Check if cross_sections.xml exists + inquire(FILE=path_cross_sections, EXIST=file_exists) + if (.not. file_exists) then + ! Could not find cross_sections.xml file + call fatal_error("Cross sections XML file '" & + &// trim(path_cross_sections) // "' does not exist!") + end if + + call write_message("Loading Cross Section Data...", 5) + + ! Parse cross_sections.xml file + call open_xmldoc(doc, path_cross_sections) + + ! Get node list of all + call get_node_list(doc, "xsdata", node_xsdata_list) + n_listings = get_list_size(node_xsdata_list) + + ! allocate arrays for ACE table storage and cross section cache + allocate(nuclides_MG(n_nuclides_total)) +!$omp parallel + allocate(micro_xs(n_nuclides_total)) +!$omp end parallel + + ! Find out if we need fission & kappa fission + ! (i.e., are there any SCORE_FISSION or SCORE_KAPPA_FISSION tallies?) + get_kfiss = .false. + get_fiss = .false. + do i = 1, n_tallies + do l = 1, tallies(i) % n_score_bins + if (tallies(i) % score_bins(l) == SCORE_KAPPA_FISSION) then + get_kfiss = .true. + end if + if (tallies(i) % score_bins(l) == SCORE_FISSION) then + get_fiss = .true. + end if + end do + if (get_kfiss .and. get_fiss) exit + end do + + ! ========================================================================== + ! READ ALL ACE CROSS SECTION TABLES + + ! Loop over all files + MATERIAL_LOOP: do i = 1, n_materials + mat => materials(i) + + NUCLIDE_LOOP: do j = 1, mat % n_nuclides + name = mat % names(j) + + if (.not. already_read % contains(name)) then + i_listing = xs_listing_dict % get_key(to_lower(name)) + i_nuclide = mat % nuclide(j) + name = xs_listings(i_listing) % name + alias = xs_listings(i_listing) % alias + + ! Get pointer to xsdata table XML node + call get_list_item(node_xsdata_list, i_listing, node_xsdata) + + call write_message("Loading " // trim(name) // " Data...", 5) + + ! First find out the data representation + if (check_for_node(node_xsdata, "representation")) then + call get_node_value(node_xsdata, "representation", temp_str) + temp_str = trim(to_lower(temp_str)) + if (temp_str == 'isotropic' .or. temp_str == 'iso') then + representation = MGXS_ISOTROPIC + else if (temp_str == 'angle') then + representation = MGXS_ANGLE + else + call fatal_error("Invalid Data Representation!") + end if + else + ! Default to isotropic representation + representation = MGXS_ISOTROPIC + end if + + ! Now allocate accordingly + select case(representation) + case(MGXS_ISOTROPIC) + allocate(NuclideIso :: nuclides_MG(i_nuclide) % obj) + case(MGXS_ANGLE) + allocate(NuclideAngle :: nuclides_MG(i_nuclide) % obj) + end select + + ! Now read in the data specific to the type we just declared + call nuclides_MG(i_nuclide) % obj % init(node_xsdata, energy_groups, & + get_kfiss, get_fiss) + + ! Keep track of what listing is associated with this nuclide + nuclides_MG(i_nuclide) % obj % listing = i_listing + + ! Add name and alias to dictionary + call already_read % add(name) + call already_read % add(alias) + end if + end do NUCLIDE_LOOP + end do MATERIAL_LOOP + + ! Avoid some valgrind leak errors + call already_read % clear() + + ! Loop around material + MATERIAL_LOOP3: do i = 1, n_materials + + ! Get material + mat => materials(i) + + ! Loop around nuclides in material + NUCLIDE_LOOP2: do j = 1, mat % n_nuclides + ! Is this fissionable? + if (nuclides_MG(mat % nuclide(j)) % obj % fissionable) then + mat % fissionable = .true. + end if + if (mat % fissionable) then + exit NUCLIDE_LOOP2 + end if + + end do NUCLIDE_LOOP2 + end do MATERIAL_LOOP3 + + end subroutine read_mgxs + +!=============================================================================== +! CREATE_MACRO_XS generates the macroscopic x/s from the microscopic input data +!=============================================================================== + + subroutine create_macro_xs() + integer :: i_mat ! index in materials array + integer :: i ! loop index over nuclides + integer :: l ! Loop over score bins + type(Material), pointer :: mat ! current material + logical :: get_kfiss, get_fiss + integer :: error_code + character(MAX_LINE_LEN) :: error_text + integer :: scatt_type + integer :: legendre_mu_points + + ! Find out if we need fission & kappa fission + ! (i.e., are there any SCORE_FISSION or SCORE_KAPPA_FISSION tallies?) + get_kfiss = .false. + get_fiss = .false. + do i = 1, n_tallies + do l = 1, tallies(i) % n_score_bins + if (tallies(i) % score_bins(l) == SCORE_KAPPA_FISSION) then + get_kfiss = .true. + end if + if (tallies(i) % score_bins(l) == SCORE_FISSION) then + get_fiss = .true. + end if + end do + if (get_kfiss .and. get_fiss) & + exit + end do + + allocate(macro_xs(n_materials)) + + do i_mat = 1, n_materials + mat => materials(i_mat) + + ! Check to see how our nuclides are represented + ! Force all to be the same type + ! Therefore type(nuclides(mat % nuclide(1)) % obj) dictates type(macroxs) + ! At the same time, we will find the scattering type, as that will dictate + ! how we allocate the scatter object within macroxs + legendre_mu_points = nuclides_MG(mat % nuclide(1)) % obj % legendre_mu_points + scatt_type = nuclides_MG(mat % nuclide(1)) % obj % scatt_type + select type(nuc => nuclides_MG(mat % nuclide(1)) % obj) + type is (NuclideIso) + allocate(MacroXSIso :: macro_xs(i_mat) % obj) + type is (NuclideAngle) + allocate(MacroXSAngle :: macro_xs(i_mat) % obj) + end select + + call macro_xs(i_mat) % obj % init(mat, nuclides_MG, energy_groups, & + get_kfiss, get_fiss, max_order, & + scatt_type, legendre_mu_points, & + error_code, error_text) + ! Handle any errors + if (error_code /= 0) call fatal_error(trim(error_text)) + end do + end subroutine create_macro_xs + +end module mgxs_data \ No newline at end of file diff --git a/src/multipole.F90 b/src/multipole.F90 index da57c96a2..cb83d85d1 100644 --- a/src/multipole.F90 +++ b/src/multipole.F90 @@ -4,8 +4,8 @@ module multipole use global use hdf5 use hdf5_interface - use multipole_header, only: MultipoleArray, FIT_T, FIT_A, FIT_F, max_L, & - max_poles, max_poly, MP_FISS, FORM_MLBW, FORM_RM + use multipole_header, only: MultipoleArray, FIT_T, FIT_A, FIT_F, & + MP_FISS, FORM_MLBW, FORM_RM implicit none @@ -32,7 +32,6 @@ contains integer :: i, j integer, allocatable :: MT(:) logical :: accumulated_fission - character(len=3) :: MT_string character(len=24) :: MT_n ! Takes the form '/nuclide/reactions/MT???' integer :: is_fissionable @@ -91,13 +90,13 @@ contains allocate(nuc % nu_fission(nuc % n_grid)) allocate(nuc % absorption(nuc % n_grid)) - nuc % total = ZERO - nuc % absorption = ZERO - nuc % fission = ZERO + nuc % total(:) = ZERO + nuc % absorption(:) = ZERO + nuc % fission(:) = ZERO ! Read in new energy axis (converting eV to MeV) call read_dataset(group_id, "energy_points", nuc % energy) - nuc % energy = nuc % energy / 1.0D6 + nuc % energy = nuc % energy / 1.0e6_8 ! Get count and list of MT tables call read_dataset(group_id, "MT_count", NMT) @@ -111,8 +110,7 @@ contains ! Loop over each MT entry and load it into a reaction. do i = 1, NMT - write(MT_string, '(I3.3)') MT(i) - MT_n = "/nuclide/reactions/MT" // MT_string + write(MT_n, '(A, I3.3)') '/nuclide/reactions/MT', MT(i) group_id = open_group(file_id, MT_n) @@ -120,11 +118,11 @@ contains select case (MT(i)) case(ELASTIC) call read_dataset(group_id, "MT_sigma", nuc % elastic) - nuc % total = nuc % total + nuc % elastic + nuc % total(:) = nuc % total + nuc % elastic case(N_FISSION) call read_dataset(group_id, "MT_sigma", nuc % fission) - nuc % total = nuc % total + nuc % fission - nuc % absorption = nuc % absorption + nuc % fission + nuc % total(:) = nuc % total + nuc % fission + nuc % absorption(:) = nuc % absorption + nuc % fission accumulated_fission = .true. case default ! Search through all of our secondary reactions @@ -136,36 +134,42 @@ contains ! fission cross section. if ( (MT(i) == N_F .or. MT(i) == N_NF .or. MT(i) == N_2NF & .or. MT(i) == N_3NF) .and. accumulated_fission) then - nuc % total = nuc % total - nuc % fission - nuc % absorption = nuc % absorption - nuc % fission - nuc % fission = 0.0_8 + nuc % total(:) = nuc % total - nuc % fission + nuc % absorption(:) = nuc % absorption - nuc % fission + nuc % fission(:) = ZERO accumulated_fission = .false. end if deallocate(nuc % reactions(j) % sigma) allocate(nuc % reactions(j) % sigma(nuc % n_grid)) - call read_dataset(group_id, "MT_sigma", nuc % reactions(j) % sigma) - call read_dataset(group_id, "Q_value", nuc % reactions(j) % Q_value) - call read_dataset(group_id, "threshold", nuc % reactions(j) % threshold) + call read_dataset(group_id, "MT_sigma", & + nuc % reactions(j) % sigma) + call read_dataset(group_id, "Q_value", & + nuc % reactions(j) % Q_value) + call read_dataset(group_id, "threshold", & + nuc % reactions(j) % threshold) nuc % reactions(j) % threshold = 1 ! TODO: reconsider implications. - nuc % reactions(j) % Q_value = nuc % reactions(j) % Q_value / 1.0D6 + nuc % reactions(j) % Q_value = nuc % reactions(j) % Q_value & + / 1.0e6_8 ! Accumulate total if (MT(i) /= N_LEVEL .and. MT(i) <= N_DA) then - nuc % total = nuc % total + nuc % reactions(j) % sigma + nuc % total(:) = nuc % total + nuc % reactions(j) % sigma end if ! Accumulate absorption if (MT(i) >= N_GAMMA .and. MT(i) <= N_DA) then - nuc % absorption = nuc % absorption + nuc % reactions(j) % sigma + nuc % absorption(:) = nuc % absorption & + + nuc % reactions(j) % sigma end if ! Accumulate fission (if needed) if ( (MT(i) == N_F .or. MT(i) == N_NF .or. MT(i) == N_2NF & .or. MT(i) == N_3NF) ) then - nuc % fission = nuc % fission + nuc % reactions(j) % sigma - nuc % absorption = nuc % absorption + nuc % reactions(j) % sigma + nuc % fission(:) = nuc % fission + nuc % reactions(j) % sigma + nuc % absorption(:) = nuc % absorption & + + nuc % reactions(j) % sigma end if end if end do diff --git a/src/multipole_header.F90 b/src/multipole_header.F90 index a3642b890..a21677a95 100644 --- a/src/multipole_header.F90 +++ b/src/multipole_header.F90 @@ -32,12 +32,6 @@ module multipole_header ! Value of 'true' when checking if nuclide is fissionable integer, parameter :: MP_FISS = 1 - ! These variables store the maximum value from every nuclide in order - ! to preallocate some arrays to improve performance. - integer :: max_poly ! Maximum number of polynomials we expect - integer :: max_poles ! Maximum number of poles in the problem for allocation - integer :: max_L ! Maximum L value for allocation - !=============================================================================== ! MULTIPOLE contains all the components needed for the windowed multipole ! temperature dependent cross section libraries for the resolved resonance diff --git a/src/nuclide_header.F90 b/src/nuclide_header.F90 new file mode 100644 index 000000000..ca128b6e1 --- /dev/null +++ b/src/nuclide_header.F90 @@ -0,0 +1,1179 @@ +module nuclide_header + + use, intrinsic :: ISO_FORTRAN_ENV + + use constants + use dict_header, only: DictIntInt + use endf, only: reaction_name, is_fission, is_disappearance + use endf_header, only: Function1D + use error, only: fatal_error, warning + use list_header, only: ListInt + use math, only: evaluate_legendre, find_angle + use multipole_header, only: MultipoleArray + use product_header, only: AngleEnergyContainer + use reaction_header, only: Reaction + use stl_vector, only: VectorInt + use string + use urr_header, only: UrrData + use xml_interface + + implicit none + +!=============================================================================== +! Nuclide contains the base nuclidic data for a nuclide, which does not depend +! upon how the nuclear data is represented (i.e., CE, or any variant of MG). +! The extended types, NuclideCE and NuclideMG deal with the rest +!=============================================================================== + + type, abstract :: Nuclide + character(12) :: name ! name of nuclide, e.g. 92235.03c + integer :: zaid ! Z and A identifier, e.g. 92235 + real(8) :: awr ! Atomic Weight Ratio + integer :: listing ! index in xs_listings + real(8) :: kT ! temperature in MeV (k*T) + + ! Fission information + logical :: fissionable ! nuclide is fissionable? + + contains + procedure(nuclide_print_), deferred :: print ! Writes nuclide info + end type Nuclide + + abstract interface + subroutine nuclide_print_(this, unit) + import Nuclide + class(Nuclide),intent(in) :: this + integer, optional, intent(in) :: unit + end subroutine nuclide_print_ + end interface + + type, extends(Nuclide) :: NuclideCE + ! Energy grid information + integer :: n_grid ! # of nuclide grid points + integer, allocatable :: grid_index(:) ! log grid mapping indices + real(8), allocatable :: energy(:) ! energy values corresponding to xs + + ! Microscopic cross sections + real(8), allocatable :: total(:) ! total cross section + real(8), allocatable :: elastic(:) ! elastic scattering + real(8), allocatable :: fission(:) ! fission + real(8), allocatable :: nu_fission(:) ! neutron production + real(8), allocatable :: absorption(:) ! absorption (MT > 100) + real(8), allocatable :: heating(:) ! heating + + ! Resonance scattering info + logical :: resonant = .false. ! resonant scatterer? + character(10) :: name_0K = '' ! name of 0K nuclide, e.g. 92235.00c + character(16) :: scheme ! target velocity sampling scheme + integer :: n_grid_0K ! number of 0K energy grid points + real(8), allocatable :: energy_0K(:) ! energy grid for 0K xs + real(8), allocatable :: elastic_0K(:) ! Microscopic elastic cross section + real(8), allocatable :: xs_cdf(:) ! CDF of v_rel times cross section + real(8) :: E_min ! lower cutoff energy for res scattering + real(8) :: E_max ! upper cutoff energy for res scattering + + ! Fission information + logical :: has_partial_fission = .false. ! nuclide has partial fission reactions? + integer :: n_fission ! # of fission reactions + integer :: n_precursor = 0 ! # of delayed neutron precursors + integer, allocatable :: index_fission(:) ! indices in reactions + class(Function1D), allocatable :: total_nu + + ! Unresolved resonance data + logical :: urr_present + integer :: urr_inelastic + type(UrrData), pointer :: urr_data => null() + + ! Multipole data + logical :: mp_present = .false. + type(MultipoleArray), pointer :: multipole => null() + + ! Reactions + integer :: n_reaction ! # of reactions + type(Reaction), allocatable :: reactions(:) + type(DictIntInt) :: reaction_index ! map MT values to index in reactions + ! array; used at tally-time + + contains + procedure :: clear => nuclidece_clear + procedure :: print => nuclidece_print + procedure :: nu => nuclidece_nu + end type NuclideCE + + type, abstract, extends(Nuclide) :: NuclideMG + ! Scattering Order Information + integer :: order ! Order of data (Scattering for NuclideIso, + ! Number of angles for all in NuclideAngle) + integer :: scatt_type ! either legendre, histogram, or tabular. + integer :: legendre_mu_points ! Number of tabular points to use to represent + ! Legendre distribs, -1 if sample with the + ! Legendres themselves + contains + procedure(nuclidemg_init_), deferred :: init ! Initialize the data + procedure(nuclidemg_get_xs_), deferred :: get_xs ! Get the requested xs + procedure(nuclidemg_calc_f_), deferred :: calc_f ! Calculates f, given mu + end type NuclideMG + + abstract interface + + subroutine nuclidemg_init_(this, node_xsdata, groups, get_kfiss, get_fiss) + import NuclideMG, Node + class(NuclideMG), intent(inout) :: this ! Working Object + type(Node), pointer, intent(in) :: node_xsdata ! Data from MGXS xml + integer, intent(in) :: groups ! Number of Energy groups + logical, intent(in) :: get_kfiss ! Need Kappa-Fission? + logical, intent(in) :: get_fiss ! Should we get fiss data? + end subroutine nuclidemg_init_ + + function nuclidemg_get_xs_(this, g, xstype, gout, uvw, mu, i_azi, i_pol) & + result(xs) + import NuclideMG + class(NuclideMG), intent(in) :: this + integer, intent(in) :: g ! Incoming Energy group + character(*), intent(in) :: xstype ! Cross Section Type + integer, optional, intent(in) :: gout ! Outgoing Group + real(8), optional, intent(in) :: uvw(3) ! Requested Angle + real(8), optional, intent(in) :: mu ! Change in angle + integer, optional, intent(in) :: i_azi ! Azimuthal Index + integer, optional, intent(in) :: i_pol ! Polar Index + real(8) :: xs ! Resultant xs + end function nuclidemg_get_xs_ + + pure function nuclidemg_calc_f_(this, gin, gout, mu, uvw, i_azi, i_pol) result(f) + import NuclideMG + class(NuclideMG), intent(in) :: this + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8), intent(in), optional :: uvw(3) ! Direction vector + integer, intent(in), optional :: i_azi ! Incoming Energy Group + integer, intent(in), optional :: i_pol ! Outgoing Energy Group + real(8) :: f ! Return value of f(mu) + + end function nuclidemg_calc_f_ + end interface + +!=============================================================================== +! NuclideIso contains the base MGXS data for a nuclide specifically for +! isotropically weighted MGXS +!=============================================================================== + + type, extends(NuclideMG) :: NuclideIso + + ! Microscopic cross sections + real(8), allocatable :: total(:) ! total cross section + real(8), allocatable :: absorption(:) ! absorption cross section + real(8), allocatable :: scatter(:,:,:) ! scattering information + real(8), allocatable :: nu_fission(:,:) ! fission matrix (Gout x Gin) + real(8), allocatable :: k_fission(:) ! kappa-fission + real(8), allocatable :: fission(:) ! neutron production + real(8), allocatable :: chi(:) ! Fission Spectra + real(8), allocatable :: mult(:,:) ! Scatter multiplicity (Gout x Gin) + + contains + procedure :: init => nuclideiso_init ! Initialize Nuclidic MGXS Data + procedure :: print => nuclideiso_print ! Writes nuclide info + procedure :: get_xs => nuclideiso_get_xs ! Gets Size of Data w/in Object + procedure :: calc_f => nuclideiso_calc_f ! Calcs f given mu + end type NuclideIso + +!=============================================================================== +! NuclideAngle contains the base MGXS data for a nuclide specifically for +! explicit angle-dependent weighted MGXS +!=============================================================================== + + type, extends(NuclideMG) :: NuclideAngle + + ! Microscopic cross sections. Dimensions are: (n_pol, n_azi, Nl, Ng, Ng) + real(8), allocatable :: total(:,:,:) ! total cross section + real(8), allocatable :: absorption(:,:,:) ! absorption cross section + real(8), allocatable :: scatter(:,:,:,:,:) ! scattering information + real(8), allocatable :: nu_fission(:,:,:,:) ! fission matrix (Gout x Gin) + real(8), allocatable :: k_fission(:,:,:) ! kappa-fission + real(8), allocatable :: fission(:,:,:) ! neutron production + real(8), allocatable :: chi(:,:,:) ! Fission Spectra + real(8), allocatable :: mult(:,:,:,:) ! Scatter multiplicity (Gout x Gin) + + ! In all cases, right-most indices are theta, phi + integer :: n_pol ! Number of polar angles + integer :: n_azi ! Number of azimuthal angles + real(8), allocatable :: polar(:) ! polar angles + real(8), allocatable :: azimuthal(:) ! azimuthal angles + + contains + procedure :: init => nuclideangle_init ! Initialize Nuclidic MGXS Data + procedure :: print => nuclideangle_print ! Gets Size of Data w/in Object + procedure :: get_xs => nuclideangle_get_xs ! Gets Size of Data w/in Object + procedure :: calc_f => nuclideangle_calc_f ! Calcs f given mu + end type NuclideAngle + +!=============================================================================== +! NUCLIDEMGCONTAINER pointer array for storing Nuclides +!=============================================================================== + + type NuclideMGContainer + class(NuclideMG), pointer :: obj + end type NuclideMGContainer + +!=============================================================================== +! NUCLIDE0K temporarily contains all 0K cross section data and other parameters +! needed to treat resonance scattering before transferring them to NuclideCE +!=============================================================================== + + type Nuclide0K + character(10) :: nuclide ! name of nuclide, e.g. U-238 + character(16) :: scheme = 'ares' ! target velocity sampling scheme + character(10) :: name ! name of nuclide, e.g. 92235.03c + character(10) :: name_0K ! name of 0K nuclide, e.g. 92235.00c + real(8) :: E_min = 0.01e-6_8 ! lower cutoff energy for res scattering + real(8) :: E_max = 1000.0e-6_8 ! upper cutoff energy for res scattering + end type Nuclide0K + +!=============================================================================== +! NUCLIDEMICROXS contains cached microscopic cross sections for a +! particular nuclide at the current energy +!=============================================================================== + + type NuclideMicroXS + integer :: index_grid ! index on nuclide energy grid + integer :: index_temp ! temperature index for nuclide + real(8) :: last_E = ZERO ! last evaluated energy + real(8) :: interp_factor ! interpolation factor on nuc. energy grid + real(8) :: total ! microscropic total xs + real(8) :: elastic ! microscopic elastic scattering xs + real(8) :: absorption ! microscopic absorption xs + real(8) :: fission ! microscopic fission xs + real(8) :: nu_fission ! microscopic production xs + + ! Information for S(a,b) use + integer :: index_sab ! index in sab_tables (zero means no table) + integer :: last_index_sab = 0 ! index in sab_tables last used by this nuclide + real(8) :: elastic_sab ! microscopic elastic scattering on S(a,b) table + + ! Information for URR probability table use + logical :: use_ptable ! in URR range with probability tables? + + ! Information for Doppler broadening + real(8) :: last_sqrtkT = ZERO ! Last temperature in sqrt(Boltzmann + ! constant * temperature (MeV)) + end type NuclideMicroXS + +!=============================================================================== +! MATERIALMACROXS contains cached macroscopic cross sections for the material a +! particle is traveling through +!=============================================================================== + + type MaterialMacroXS + real(8) :: total ! macroscopic total xs + real(8) :: elastic ! macroscopic elastic scattering xs + real(8) :: absorption ! macroscopic absorption xs + real(8) :: fission ! macroscopic fission xs + real(8) :: nu_fission ! macroscopic production xs + end type MaterialMacroXS + +!=============================================================================== +! XSLISTING contains data read from a CE or MG cross_sections.xml file +! (or equivalent) +!=============================================================================== + + type XsListing + character(12) :: name ! table name, e.g. 92235.70c + character(12) :: alias ! table alias, e.g. U-235.70c + integer :: type ! type of table (cont-E neutron, S(A,b), etc) + integer :: zaid ! ZAID identifier = 1000*Z + A + integer :: filetype ! ASCII or BINARY + integer :: location ! location of table within library + integer :: recl ! record length for library + integer :: entries ! number of entries per record + real(8) :: awr ! atomic weight ratio (# of neutron masses) + real(8) :: kT ! Boltzmann constant * temperature (MeV) + logical :: metastable ! is this nuclide metastable? + character(MAX_FILE_LEN) :: path ! path to library containing table + end type XsListing + + contains + +!=============================================================================== +! NUCLIDE_*_INIT reads in the data from the XML file, as already accessed +!=============================================================================== + + subroutine nuclidemg_init(this, node_xsdata) + class(NuclideMG), intent(inout) :: this ! Working Object + type(Node), pointer, intent(in) :: node_xsdata ! Data from MGXS xml + + type(Node), pointer :: node_legendre_mu + character(MAX_LINE_LEN) :: temp_str + logical :: enable_leg_mu + + ! Load the data + call get_node_value(node_xsdata, "name", this % name) + this % name = to_lower(this % name) + if (check_for_node(node_xsdata, "kT")) then + call get_node_value(node_xsdata, "kT", this % kT) + else + this % kT = ZERO + end if + if (check_for_node(node_xsdata, "zaid")) then + call get_node_value(node_xsdata, "zaid", this % zaid) + else + this % zaid = -1 + end if + if (check_for_node(node_xsdata, "scatt_type")) then + call get_node_value(node_xsdata, "scatt_type", temp_str) + temp_str = trim(to_lower(temp_str)) + if (temp_str == 'legendre') then + this % scatt_type = ANGLE_LEGENDRE + else if (temp_str == 'histogram') then + this % scatt_type = ANGLE_HISTOGRAM + else if (temp_str == 'tabular') then + this % scatt_type = ANGLE_TABULAR + else + call fatal_error("Invalid Scatt Type Option!") + end if + else + this % scatt_type = ANGLE_LEGENDRE + end if + + if (check_for_node(node_xsdata, "order")) then + call get_node_value(node_xsdata, "order", this % order) + else + call fatal_error("Order Must Be Provided!") + end if + + ! Get scattering treatment + if (check_for_node(node_xsdata, "tabular_legendre")) then + call get_node_ptr(node_xsdata, "tabular_legendre", node_legendre_mu) + if (check_for_node(node_legendre_mu, "enable")) then + call get_node_value(node_legendre_mu, "enable", temp_str) + temp_str = trim(to_lower(temp_str)) + if (temp_str == 'true' .or. temp_str == '1') then + enable_leg_mu = .true. + elseif (temp_str == 'false' .or. temp_str == '0') then + enable_leg_mu = .false. + this % legendre_mu_points = 1 + else + call fatal_error("Unrecognized tabular_legendre/enable: " // temp_str) + end if + else + enable_leg_mu = .true. + this % legendre_mu_points = 33 + end if + if (enable_leg_mu .and. & + check_for_node(node_legendre_mu, "num_points")) then + call get_node_value(node_legendre_mu, "num_points", & + this % legendre_mu_points) + if (this % legendre_mu_points <= 0) then + call fatal_error("num_points element must be positive and non-zero!") + end if + this % legendre_mu_points = -1 * this % legendre_mu_points + end if + else + this % legendre_mu_points = 1 + end if + + if (check_for_node(node_xsdata, "fissionable")) then + call get_node_value(node_xsdata, "fissionable", temp_str) + temp_str = to_lower(temp_str) + if (trim(temp_str) == 'true' .or. trim(temp_str) == '1') then + this % fissionable = .true. + else + this % fissionable = .false. + end if + else + call fatal_error("Fissionable element must be set!") + end if + + end subroutine nuclidemg_init + + subroutine nuclideiso_init(this, node_xsdata, groups, get_kfiss, get_fiss) + class(NuclideIso), intent(inout) :: this ! Working Object + type(Node), pointer, intent(in) :: node_xsdata ! Data from MGXS xml + integer, intent(in) :: groups ! Number of Energy groups + logical, intent(in) :: get_kfiss ! Need Kappa-Fission? + logical, intent(in) :: get_fiss ! Need fiss data? + + real(8), allocatable :: temp_arr(:) + integer :: arr_len + integer :: order_dim + + ! Call generic data gathering routine + call nuclidemg_init(this, node_xsdata) + + ! Load the more specific data + if (this % fissionable) then + + if (check_for_node(node_xsdata, "chi")) then + ! Get chi + allocate(this % chi(groups)) + call get_node_array(node_xsdata, "chi", this % chi) + + ! Get nu_fission (as a vector) + if (check_for_node(node_xsdata, "nu_fission")) then + allocate(temp_arr(groups * 1)) + call get_node_array(node_xsdata, "nu_fission", temp_arr) + allocate(this % nu_fission(groups, 1)) + this % nu_fission = reshape(temp_arr, (/groups, 1/)) + deallocate(temp_arr) + else + call fatal_error("If fissionable, must provide nu_fission!") + end if + + else + ! Get nu_fission (as a matrix) + if (check_for_node(node_xsdata, "nu_fission")) then + + allocate(temp_arr(groups*groups)) + call get_node_array(node_xsdata, "nu_fission", temp_arr) + allocate(this % nu_fission(groups, groups)) + this % nu_fission = reshape(temp_arr, (/groups, groups/)) + deallocate(temp_arr) + else + call fatal_error("If fissionable, must provide nu_fission!") + end if + end if + if (get_fiss) then + allocate(this % fission(groups)) + if (check_for_node(node_xsdata, "fission")) then + call get_node_array(node_xsdata, "fission", this % fission) + else + call fatal_error("Fission data missing, required due to fission& + & tallies in tallies.xml file!") + end if + end if + if (get_kfiss) then + allocate(this % k_fission(groups)) + if (check_for_node(node_xsdata, "kappa_fission")) then + call get_node_array(node_xsdata, "kappa_fission", this % k_fission) + else + call fatal_error("kappa_fission data missing, required due to & + &kappa-fission tallies in tallies.xml file!") + end if + end if + end if + + allocate(this % absorption(groups)) + if (check_for_node(node_xsdata, "absorption")) then + call get_node_array(node_xsdata, "absorption", this % absorption) + else + call fatal_error("Must provide absorption!") + end if + + if (this % scatt_type == ANGLE_LEGENDRE) then + order_dim = this % order + 1 + else if (this % scatt_type == ANGLE_HISTOGRAM) then + order_dim = this % order + else if (this % scatt_type == ANGLE_TABULAR) then + order_dim = this % order + end if + + allocate(this % scatter(groups, groups, order_dim)) + if (check_for_node(node_xsdata, "scatter")) then + allocate(temp_arr(groups * groups * order_dim)) + call get_node_array(node_xsdata, "scatter", temp_arr) + this % scatter = reshape(temp_arr, (/groups, groups, order_dim/)) + deallocate(temp_arr) + else + call fatal_error("Must provide scatter!") + return + end if + + + allocate(this % total(groups)) + if (check_for_node(node_xsdata, "total")) then + call get_node_array(node_xsdata, "total", this % total) + else + this % total = this % absorption + sum(this%scatter(:,:,1),dim=1) + end if + + ! Get Mult Data + allocate(this % mult(groups, groups)) + if (check_for_node(node_xsdata, "multiplicity")) then + arr_len = get_arraysize_double(node_xsdata, "multiplicity") + if (arr_len == groups * groups) then + allocate(temp_arr(arr_len)) + call get_node_array(node_xsdata, "multiplicity", temp_arr) + this % mult = reshape(temp_arr, (/groups, groups/)) + deallocate(temp_arr) + else + call fatal_error("Multiplicity length not same as number of groups& + & squared!") + return + end if + else + this % mult = ONE + end if + + end subroutine nuclideiso_init + + subroutine nuclideangle_init(this, node_xsdata, groups, get_kfiss, get_fiss) + class(NuclideAngle), intent(inout) :: this ! Working Object + type(Node), pointer, intent(in) :: node_xsdata ! Data from MGXS xml + integer, intent(in) :: groups ! Number of Energy groups + logical, intent(in) :: get_kfiss ! Need Kappa-Fission? + logical, intent(in) :: get_fiss ! Should we get fiss data? + + real(8), allocatable :: temp_arr(:) + integer :: arr_len + real(8) :: dangle + integer :: iangle + integer :: order_dim + + ! Call generic data gathering routine + call nuclidemg_init(this, node_xsdata) + + if (this % scatt_type == ANGLE_LEGENDRE) then + order_dim = this % order + 1 + else if (this % scatt_type == ANGLE_HISTOGRAM) then + order_dim = this % order + else if (this % scatt_type == ANGLE_TABULAR) then + order_dim = this % order + end if + + if (check_for_node(node_xsdata, "num_polar")) then + call get_node_value(node_xsdata, "num_polar", this % n_pol) + else + call fatal_error("num_polar Must Be Provided!") + end if + + if (check_for_node(node_xsdata, "num_azimuthal")) then + call get_node_value(node_xsdata, "num_azimuthal", this % n_azi) + else + call fatal_error("num_azimuthal Must Be Provided!") + end if + + ! Load angle data, if present (else equally spaced) + allocate(this % polar(this % n_pol)) + allocate(this % azimuthal(this % n_azi)) + if (check_for_node(node_xsdata, "polar")) then + call fatal_error("User-Specified polar angle bins not yet supported!") + ! When this feature is supported, this line will be activated + call get_node_array(node_xsdata, "polar", this % polar) + else + dangle = PI / real(this % n_pol,8) + do iangle = 1, this % n_pol + this % polar(iangle) = (real(iangle,8) - HALF) * dangle + end do + end if + if (check_for_node(node_xsdata, "azimuthal")) then + call fatal_error("User-Specified azimuthal angle bins not yet supported!") + ! When this feature is supported, this line will be activated + call get_node_array(node_xsdata, "azimuthal", this % azimuthal) + else + dangle = TWO * PI / real(this % n_azi,8) + do iangle = 1, this % n_azi + this % azimuthal(iangle) = -PI + (real(iangle,8) - HALF) * dangle + end do + end if + + ! Load the more specific data + if (this % fissionable) then + + if (check_for_node(node_xsdata, "chi")) then + ! Get chi + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "chi", temp_arr) + allocate(this % chi(groups, this % n_azi, this % n_pol)) + this % chi = reshape(temp_arr, (/groups, this % n_azi, this % n_pol/)) + deallocate(temp_arr) + + ! Get nu_fission (as a vector) + if (check_for_node(node_xsdata, "nu_fission")) then + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "nu_fission", temp_arr) + allocate(this % nu_fission(groups, 1, this % n_azi, this % n_pol)) + this % nu_fission = reshape(temp_arr, (/groups, 1, this % n_azi, & + this % n_pol/)) + deallocate(temp_arr) + else + call fatal_error("If fissionable, must provide nu_fission!") + end if + + else + ! Get nu_fission (as a matrix) + if (check_for_node(node_xsdata, "nu_fission")) then + + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "nu_fission", temp_arr) + allocate(this % nu_fission(groups, groups, this % n_azi, this % n_pol)) + this % nu_fission = reshape(temp_arr, (/groups, groups, & + this % n_azi, this % n_pol/)) + deallocate(temp_arr) + else + call fatal_error("If fissionable, must provide nu_fission!") + end if + end if + if (get_fiss) then + if (check_for_node(node_xsdata, "fission")) then + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "fission", temp_arr) + allocate(this % fission(groups, this % n_azi, this % n_pol)) + this % fission = reshape(temp_arr, (/groups, this % n_azi, this % n_pol/)) + deallocate(temp_arr) + else + call fatal_error("Fission data missing, required due to fission& + & tallies in tallies.xml file!") + end if + end if + if (get_kfiss) then + if (check_for_node(node_xsdata, "kappa_fission")) then + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "kappa_fission", temp_arr) + allocate(this % k_fission(groups, this % n_azi, this % n_pol)) + this % k_fission = reshape(temp_arr, (/groups, this % n_azi, this % n_pol/)) + deallocate(temp_arr) + else + call fatal_error("kappa_fission data missing, required due to & + &kappa-fission tallies in tallies.xml file!") + end if + end if + end if + + if (check_for_node(node_xsdata, "absorption")) then + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "absorption", temp_arr) + allocate(this % absorption(groups, this % n_azi, this % n_pol)) + this % absorption = reshape(temp_arr, (/groups, this % n_azi, this % n_pol/)) + deallocate(temp_arr) + else + call fatal_error("Must provide absorption!") + end if + + allocate(this % scatter(groups, groups, order_dim, this % n_azi, this % n_pol)) + if (check_for_node(node_xsdata, "scatter")) then + allocate(temp_arr(groups * groups * order_dim * this % n_azi * this%n_pol)) + call get_node_array(node_xsdata, "scatter", temp_arr) + this % scatter = reshape(temp_arr, (/groups, groups, order_dim, & + this%n_azi,this%n_pol/)) + deallocate(temp_arr) + else + call fatal_error("Must provide scatter!") + end if + + if (check_for_node(node_xsdata, "total")) then + allocate(temp_arr(groups * this % n_azi * this % n_pol)) + call get_node_array(node_xsdata, "total", temp_arr) + allocate(this % total(groups, this % n_azi, this % n_pol)) + this % total = reshape(temp_arr, (/groups, this % n_azi, this % n_pol/)) + deallocate(temp_arr) + else + this % total = this % absorption + sum(this%scatter(:,:,1,:,:),dim=1) + end if + + ! Get Mult Data + allocate(this % mult(groups, groups, this % n_azi, this % n_pol)) + if (check_for_node(node_xsdata, "multiplicity")) then + arr_len = get_arraysize_double(node_xsdata, "multiplicity") + if (arr_len == groups * groups * this % n_azi * this % n_pol) then + allocate(temp_arr(arr_len)) + call get_node_array(node_xsdata, "multiplicity", temp_arr) + this % mult = reshape(temp_arr, (/groups, groups, this % n_azi, this % n_pol/)) + deallocate(temp_arr) + else + call fatal_error("Multiplicity Length Does Not Match!") + end if + else + this % mult = ONE + end if + + end subroutine nuclideangle_init + +!=============================================================================== +! NUCLIDECE_CLEAR resets and deallocates data in Nuclide, NuclideIso +! or NuclideAngle +!=============================================================================== + + subroutine nuclidece_clear(this) + + class(NuclideCE), intent(inout) :: this ! The Nuclide object to clear + + if (associated(this % urr_data)) deallocate(this % urr_data) + + call this % reaction_index % clear() + + if (associated(this % multipole)) deallocate(this % multipole) + + end subroutine nuclidece_clear + + function nuclidece_nu(this, E, emission_mode, group) result(nu) + class(NuclideCE), intent(in) :: this + real(8), intent(in) :: E + integer, intent(in) :: emission_mode + integer, optional, intent(in) :: group + real(8) :: nu + + integer :: i + + if (.not. this % fissionable) then + nu = ZERO + return + end if + + select case (emission_mode) + case (EMISSION_PROMPT) + associate (product => this % reactions(this % index_fission(1)) % products(1)) + nu = product % yield % evaluate(E) + end associate + + case (EMISSION_DELAYED) + if (this % n_precursor > 0) then + if (present(group)) then + ! If delayed group specified, determine yield immediately + associate(p => this % reactions(this % index_fission(1)) % products(1 + group)) + nu = p % yield % evaluate(E) + end associate + + else + nu = ZERO + + associate (rx => this % reactions(this % index_fission(1))) + do i = 2, size(rx % products) + associate (product => rx % products(i)) + ! Skip any non-neutron products + if (product % particle /= NEUTRON) exit + + ! Evaluate yield + if (product % emission_mode == EMISSION_DELAYED) then + nu = nu + product % yield % evaluate(E) + end if + end associate + end do + end associate + end if + else + nu = ZERO + end if + + case (EMISSION_TOTAL) + if (allocated(this % total_nu)) then + nu = this % total_nu % evaluate(E) + else + associate (rx => this % reactions(this % index_fission(1))) + nu = rx % products(1) % yield % evaluate(E) + end associate + end if + end select + + end function nuclidece_nu + +!=============================================================================== +! NUCLIDE*_PRINT displays information about a continuous-energy neutron +! cross_section table and its reactions and secondary angle/energy distributions +!=============================================================================== + + subroutine nuclidece_print(this, unit) + class(NuclideCE), intent(in) :: this + integer, intent(in), optional :: unit + + integer :: i ! loop index over nuclides + integer :: unit_ ! unit to write to + integer :: size_xs ! memory used for cross-sections (bytes) + integer :: size_urr ! memory used for probability tables (bytes) + + ! set default unit for writing information + if (present(unit)) then + unit_ = unit + else + unit_ = OUTPUT_UNIT + end if + + ! Initialize totals + size_urr = 0 + size_xs = 0 + + ! Basic nuclide information + write(unit_,*) 'Nuclide ' // trim(this % name) + write(unit_,*) ' zaid = ' // trim(to_str(this % zaid)) + write(unit_,*) ' awr = ' // trim(to_str(this % awr)) + write(unit_,*) ' kT = ' // trim(to_str(this % kT)) + write(unit_,*) ' # of grid points = ' // trim(to_str(this % n_grid)) + write(unit_,*) ' Fissionable = ', this % fissionable + write(unit_,*) ' # of fission reactions = ' // trim(to_str(this % n_fission)) + write(unit_,*) ' # of reactions = ' // trim(to_str(this % n_reaction)) + + ! Information on each reaction + write(unit_,*) ' Reaction Q-value COM IE' + do i = 1, this % n_reaction + associate (rxn => this % reactions(i)) + write(unit_,'(3X,A11,1X,F8.3,3X,L1,3X,I6)') & + reaction_name(rxn % MT), rxn % Q_value, rxn % scatter_in_cm, & + rxn % threshold + + ! Accumulate data size + size_xs = size_xs + (this % n_grid - rxn%threshold + 1) * 8 + end associate + end do + + ! Add memory required for summary reactions (total, absorption, fission, + ! nu-fission) + size_xs = 8 * this % n_grid * 4 + + ! Write information about URR probability tables + size_urr = 0 + if (this % urr_present) then + associate(urr => this % urr_data) + write(unit_,*) ' Unresolved resonance probability table:' + write(unit_,*) ' # of energies = ' // trim(to_str(urr % n_energy)) + write(unit_,*) ' # of probabilities = ' // trim(to_str(urr % n_prob)) + write(unit_,*) ' Interpolation = ' // trim(to_str(urr % interp)) + write(unit_,*) ' Inelastic flag = ' // trim(to_str(urr % inelastic_flag)) + write(unit_,*) ' Absorption flag = ' // trim(to_str(urr % absorption_flag)) + write(unit_,*) ' Multiply by smooth? ', urr % multiply_smooth + write(unit_,*) ' Min energy = ', trim(to_str(urr % energy(1))) + write(unit_,*) ' Max energy = ', trim(to_str(urr % energy(urr % n_energy))) + + ! Calculate memory used by probability tables and add to total + size_urr = urr % n_energy * (urr % n_prob * 6 + 1) * 8 + end associate + end if + + ! Write memory used + write(unit_,*) ' Memory Requirements' + write(unit_,*) ' Cross sections = ' // trim(to_str(size_xs)) // ' bytes' + write(unit_,*) ' Probability Tables = ' // & + trim(to_str(size_urr)) // ' bytes' + + ! Blank line at end of nuclide + write(unit_,*) + end subroutine nuclidece_print + + subroutine nuclidemg_print(this, unit_) + class(NuclideMG), intent(in) :: this + integer, intent(in) :: unit_ + + character(MAX_LINE_LEN) :: temp_str + + ! Basic nuclide information + write(unit_,*) 'Nuclide ' // trim(this % name) + if (this % zaid > 0) then + ! Dont print if data was macroscopic and thus zaid & AWR would be nonsense + write(unit_,*) ' zaid = ' // trim(to_str(this % zaid)) + write(unit_,*) ' awr = ' // trim(to_str(this % awr)) + end if + write(unit_,*) ' kT = ' // trim(to_str(this % kT)) + if (this % scatt_type == ANGLE_LEGENDRE) then + temp_str = "Legendre" + write(unit_,*) ' Scattering Type = ' // trim(temp_str) + write(unit_,*) ' # of Scatter Moments = ' // & + trim(to_str(this % order)) + else if (this % scatt_type == ANGLE_HISTOGRAM) then + temp_str = "Histogram" + write(unit_,*) ' Scattering Type = ' // trim(temp_str) + write(unit_,*) ' # of Scatter Bins = ' // & + trim(to_str(this % order)) + else if (this % scatt_type == ANGLE_TABULAR) then + temp_str = "Tabular" + write(unit_,*) ' Scattering Type = ' // trim(temp_str) + write(unit_,*) ' # of Scatter Points = ' // trim(to_str(this % order)) + end if + write(unit_,*) ' Fissionable = ', this % fissionable + + end subroutine nuclidemg_print + + subroutine nuclideiso_print(this, unit) + + class(NuclideIso), intent(in) :: this + integer, optional, intent(in) :: unit + + integer :: unit_ ! unit to write to + integer :: size_total, size_scattmat, size_mgxs + + ! set default unit for writing information + if (present(unit)) then + unit_ = unit + else + unit_ = OUTPUT_UNIT + end if + + ! Write Basic Nuclide Information + call nuclidemg_print(this, unit_) + + ! Determine size of mgxs and scattering matrices + size_scattmat = (size(this % scatter) + size(this % mult)) * 8 + size_mgxs = size(this % total) + size(this % absorption) + & + size(this % nu_fission) + size(this % k_fission) + & + size(this % fission) + size(this % chi) + size_mgxs = size_mgxs * 8 + + ! Calculate total memory + size_total = size_scattmat + size_mgxs + + ! Write memory used + write(unit_,*) ' Memory Requirements' + write(unit_,*) ' Cross sections = ' // trim(to_str(size_mgxs)) // ' bytes' + write(unit_,*) ' Scattering Matrices = ' // & + trim(to_str(size_scattmat)) // ' bytes' + write(unit_,*) ' Total = ' // trim(to_str(size_total)) // ' bytes' + + ! Blank line at end of nuclide + write(unit_,*) + + end subroutine nuclideiso_print + + subroutine nuclideangle_print(this, unit) + + class(NuclideAngle), intent(in) :: this + integer, optional, intent(in) :: unit + + integer :: unit_ ! unit to write to + integer :: size_total, size_scattmat, size_mgxs + + ! set default unit for writing information + if (present(unit)) then + unit_ = unit + else + unit_ = OUTPUT_UNIT + end if + + ! Write Basic Nuclide Information + call nuclidemg_print(this, unit_) + write(unit_,*) ' # of Polar Angles = ' // trim(to_str(this % n_pol)) + write(unit_,*) ' # of Azimuthal Angles = ' // trim(to_str(this % n_azi)) + + ! Determine size of mgxs and scattering matrices + size_scattmat = (size(this % scatter) + size(this % mult)) * 8 + size_mgxs = size(this % total) + size(this % absorption) + & + size(this % nu_fission) + size(this % k_fission) + & + size(this % fission) + size(this % chi) + size_mgxs = size_mgxs * 8 + + ! Calculate total memory + size_total = size_scattmat + size_mgxs + + ! Write memory used + write(unit_,*) ' Memory Requirements' + write(unit_,*) ' Cross sections = ' // trim(to_str(size_mgxs)) // ' bytes' + write(unit_,*) ' Scattering Matrices = ' // & + trim(to_str(size_scattmat)) // ' bytes' + write(unit_,*) ' Total = ' // trim(to_str(size_total)) // ' bytes' + + ! Blank line at end of nuclide + write(unit_,*) + + + end subroutine nuclideangle_print + +!=============================================================================== +! NUCLIDE*_GET_XS Returns the requested data type +!=============================================================================== + + function nuclideiso_get_xs(this, g, xstype, gout, uvw, mu, i_azi, i_pol) & + result(xs) + class(NuclideIso), intent(in) :: this + integer, intent(in) :: g ! Incoming Energy group + character(*), intent(in) :: xstype ! Cross Section Type + integer, optional, intent(in) :: gout ! Outgoing Group + real(8), optional, intent(in) :: uvw(3) ! Requested Angle + real(8), optional, intent(in) :: mu ! Change in angle + integer, optional, intent(in) :: i_azi ! Azimuthal Index + integer, optional, intent(in) :: i_pol ! Polar Index + real(8) :: xs ! Resultant xs + + xs = ZERO + + if ((xstype == 'nu_fission' .or. xstype == 'fission' .or. xstype =='chi' & + .or. xstype =='k_fission') .and. (.not. this % fissionable)) then + return + end if + + if (present(gout)) then + select case(xstype) + case('mult') + xs = this % mult(gout,g) + case('nu_fission') + xs = this % nu_fission(gout,g) + case('f_mu', 'f_mu/mult') + xs = this % calc_f(g, gout, mu) + if (xstype == 'f_mu/mult') then + xs = xs / this % mult(gout,g) + end if + end select + else + select case(xstype) + case('total') + xs = this % total(g) + case('absorption') + xs = this % absorption(g) + case('fission') + xs = this % fission(g) + case('k_fission') + if (allocated(this % k_fission)) then + xs = this % k_fission(g) + end if + case('chi') + xs = this % chi(g) + case('scatter') + xs = this % total(g) - this % absorption(g) + end select + end if + end function nuclideiso_get_xs + + function nuclideangle_get_xs(this, g, xstype, gout, uvw, mu, i_azi, i_pol) & + result(xs) + class(NuclideAngle), intent(in) :: this + integer, intent(in) :: g ! Incoming Energy group + character(*), intent(in) :: xstype ! Cross Section Type + integer, optional, intent(in) :: gout ! Outgoing Group + real(8), optional, intent(in) :: mu ! Change in angle + real(8), optional, intent(in) :: uvw(3) ! Requested Angle + integer, optional, intent(in) :: i_azi ! Azimuthal Index + integer, optional, intent(in) :: i_pol ! Polar Index + real(8) :: xs ! Resultant xs + + integer :: i_azi_, i_pol_ + + xs = ZERO + + if ((xstype == 'nu_fission' .or. xstype == 'fission' .or. xstype =='chi' & + .or. xstype =='k_fission') .and. (.not. this % fissionable)) then + return + end if + + if (present(i_azi) .and. present(i_pol)) then + i_azi_ = i_azi + i_pol_ = i_pol + else + call find_angle(this % polar, this % azimuthal, uvw, i_azi_, i_pol_) + end if + + if (present(gout)) then + select case(xstype) + case('mult') + xs = this % mult(gout,g,i_azi_,i_pol_) + case('nu_fission') + xs = this % nu_fission(gout,g,i_azi_,i_pol_) + case('chi') + xs = this % chi(gout,i_azi_,i_pol_) + case('f_mu', 'f_mu/mult') + xs = this % calc_f(g, gout, mu, I_AZI=i_azi_, I_POL=i_pol_) + if (xstype == 'f_mu/mult') then + xs = xs / this % mult(gout,g,i_azi_,i_pol_) + end if + end select + else + select case(xstype) + case('total') + xs = this % total(g,i_azi_,i_pol_) + case('absorption') + xs = this % absorption(g,i_azi_,i_pol_) + case('fission') + xs = this % fission(g,i_azi_,i_pol_) + case('k_fission') + if (allocated(this % k_fission)) then + xs = this % k_fission(g,i_azi_,i_pol_) + end if + case('chi') + xs = this % chi(g,i_azi_,i_pol_) + case('scatter') + xs = this % total(g,i_azi_,i_pol_) - this % absorption(g,i_azi_,i_pol_) + end select + end if + + end function nuclideangle_get_xs + +!=============================================================================== +! NUCLIDE*_CALC_F Finds the value of f(mu), the scattering angle probability, +! given mu +!=============================================================================== + + pure function nuclideiso_calc_f(this, gin, gout, mu, uvw, i_azi, i_pol) & + result(f) + class(NuclideIso), intent(in) :: this + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8), intent(in), optional :: uvw(3) ! Direction vector + integer, intent(in), optional :: i_azi ! Incoming Energy Group + integer, intent(in), optional :: i_pol ! Outgoing Energy Group + real(8) :: f ! Return value of f(mu) + + real(8) :: dmu, r + integer :: imu + + if (this % scatt_type == ANGLE_LEGENDRE) then + f = evaluate_legendre(this % scatter(gout,gin,:), mu) + else if (this % scatt_type == ANGLE_TABULAR) then + dmu = TWO / real(this % order - 1,8) + ! Find mu bin algebraically, knowing that the spacing is equal + f = (mu + ONE) / dmu + ONE + imu = floor(f) + ! But save the amount that mu is past the previous index + ! so we can use interpolation later. + f = f - real(imu,8) + ! Adjust so interpolation works on the last bin if necessary + if (imu == size(this % scatter, dim=3)) then + imu = imu - 1 + end if + + ! Now intepolate to find f(mu) + r = f / dmu + f = (ONE - r) * this % scatter(gout,gin,imu) + & + r * this % scatter(gout,gin,imu+1) + else ! (ANGLE_HISTOGRAM) + dmu = TWO / real(this % order,8) + ! Find mu bin algebraically, knowing that the spacing is equal + imu = floor((mu + ONE) / dmu + ONE) + ! Adjust so interpolation works on the last bin if necessary + if (imu == size(this % scatter, dim=3)) then + imu = imu - 1 + end if + f = this % scatter(gout, gin, imu) + + end if + + end function nuclideiso_calc_f + + pure function nuclideangle_calc_f(this, gin, gout, mu, uvw, i_azi, & + i_pol) result(f) + class(NuclideAngle), intent(in) :: this + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8), intent(in), optional :: uvw(3) ! Direction vector + integer, intent(in), optional :: i_azi ! Incoming Energy Group + integer, intent(in), optional :: i_pol ! Outgoing Energy Group + real(8) :: f ! Return value of f(mu) + + real(8) :: dmu, r + integer :: imu + integer :: i_azi_, i_pol_ + if (present(i_azi) .and. present(i_pol)) then + i_azi_ = i_azi + i_pol_ = i_pol + else if (present(uvw)) then + call find_angle(this % polar, this % azimuthal, uvw, i_azi_, i_pol_) + end if + + if (this % scatt_type == ANGLE_LEGENDRE) then + f = evaluate_legendre(this % scatter(gout,gin,:,i_azi_,i_pol_), mu) + else if (this % scatt_type == ANGLE_TABULAR) then + dmu = TWO / real(this % order - 1,8) + ! Find mu bin algebraically, knowing that the spacing is equal + f = (mu + ONE) / dmu + ONE + imu = floor(f) + ! But save the amount that mu is past the previous index + ! so we can use interpolation later. + f = f - real(imu,8) + ! Adjust so interpolation works on the last bin if necessary + if (imu == size(this % scatter, dim=3)) then + imu = imu - 1 + end if + + ! Now intepolate to find f(mu) + r = f / dmu + f = (ONE - r) * this % scatter(gout,gin,imu,i_azi_,i_pol_) + & + r * this % scatter(gout,gin,imu+1,i_azi_,i_pol_) + else ! (ANGLE_HISTOGRAM) + dmu = TWO / real(this % order,8) + ! Find mu bin algebraically, knowing that the spacing is equal + imu = floor((mu + ONE) / dmu + ONE) + ! Adjust so interpolation works on the last bin if necessary + if (imu == size(this % scatter, dim=3)) then + imu = imu - 1 + end if + f = this % scatter(gout, gin, imu,i_azi_,i_pol_) + + end if + + end function nuclideangle_calc_f + +end module nuclide_header diff --git a/src/output.F90 b/src/output.F90 index fb4375b54..5e427aa6d 100644 --- a/src/output.F90 +++ b/src/output.F90 @@ -2,7 +2,6 @@ module output use, intrinsic :: ISO_FORTRAN_ENV - use ace_header, only: Nuclide, Reaction, UrrData use constants use endf, only: reaction_name use error, only: fatal_error, warning @@ -12,8 +11,10 @@ module output use math, only: t_percentile use mesh_header, only: RegularMesh use mesh, only: mesh_indices_to_bin, bin_to_mesh_indices + use nuclide_header use particle_header, only: LocalCoord, Particle use plot_header + use sab_header, only: SAlphaBeta use string, only: to_upper, to_str use tally_header, only: TallyObject @@ -100,9 +101,9 @@ contains !=============================================================================== subroutine header(msg, unit, level) - character(*), intent(in) :: msg ! header message - integer, intent(in), optional :: unit ! unit to write to - integer, intent(in), optional :: level ! specified header level + character(*), intent(in) :: msg ! header message + integer, intent(in), optional :: unit ! unit to write to + integer, intent(in), optional :: level ! specified header level integer :: n ! number of = signs on left integer :: m ! number of = signs on right @@ -305,175 +306,16 @@ contains ! Display weight, energy, grid index, and interpolation factor write(ou,*) ' Weight = ' // to_str(p % wgt) - write(ou,*) ' Energy = ' // to_str(p % E) + if (run_CE) then + write(ou,*) ' Energy = ' // to_str(p % E) + else + write(ou,*) ' Energy Group = ' // to_str(p % g) + end if write(ou,*) ' Delayed Group = ' // to_str(p % delayed_group) write(ou,*) end subroutine print_particle -!=============================================================================== -! PRINT_NUCLIDE displays information about a continuous-energy neutron -! cross_section table and its reactions and secondary angle/energy distributions -!=============================================================================== - - subroutine print_nuclide(nuc, unit) - type(Nuclide), intent(in) :: nuc - integer, intent(in), optional :: unit - - integer :: i ! loop index over nuclides - integer :: unit_ ! unit to write to - integer :: size_xs ! memory used for cross-sections (bytes) - integer :: size_urr ! memory used for probability tables (bytes) - type(UrrData), pointer :: urr - - ! set default unit for writing information - if (present(unit)) then - unit_ = unit - else - unit_ = OUTPUT_UNIT - end if - - ! Initialize totals - size_urr = 0 - size_xs = 0 - - ! Basic nuclide information - write(unit_,*) 'Nuclide ' // trim(nuc % name) - write(unit_,*) ' zaid = ' // trim(to_str(nuc % zaid)) - write(unit_,*) ' awr = ' // trim(to_str(nuc % awr)) - write(unit_,*) ' kT = ' // trim(to_str(nuc % kT)) - write(unit_,*) ' # of grid points = ' // trim(to_str(nuc % n_grid)) - write(unit_,*) ' Fissionable = ', nuc % fissionable - write(unit_,*) ' # of fission reactions = ' // trim(to_str(nuc % n_fission)) - write(unit_,*) ' # of reactions = ' // trim(to_str(nuc % n_reaction)) - - ! Information on each reaction - write(unit_,*) ' Reaction Q-value COM IE' - do i = 1, nuc % n_reaction - associate (rxn => nuc % reactions(i)) - write(unit_,'(3X,A11,1X,F8.3,3X,L1,3X,I6)') & - reaction_name(rxn % MT), rxn % Q_value, rxn % scatter_in_cm, & - rxn % threshold - - ! Accumulate data size - size_xs = size_xs + (nuc % n_grid - rxn%threshold + 1) * 8 - end associate - end do - - ! Add memory required for summary reactions (total, absorption, fission, - ! nu-fission) - size_xs = 8 * nuc % n_grid * 4 - - ! Write information about URR probability tables - size_urr = 0 - if (nuc % urr_present) then - urr => nuc % urr_data - write(unit_,*) ' Unresolved resonance probability table:' - write(unit_,*) ' # of energies = ' // trim(to_str(urr % n_energy)) - write(unit_,*) ' # of probabilities = ' // trim(to_str(urr % n_prob)) - write(unit_,*) ' Interpolation = ' // trim(to_str(urr % interp)) - write(unit_,*) ' Inelastic flag = ' // trim(to_str(urr % inelastic_flag)) - write(unit_,*) ' Absorption flag = ' // trim(to_str(urr % absorption_flag)) - write(unit_,*) ' Multiply by smooth? ', urr % multiply_smooth - write(unit_,*) ' Min energy = ', trim(to_str(urr % energy(1))) - write(unit_,*) ' Max energy = ', trim(to_str(urr % energy(urr % n_energy))) - - ! Calculate memory used by probability tables and add to total - size_urr = urr % n_energy * (urr % n_prob * 6 + 1) * 8 - end if - - ! Write memory used - write(unit_,*) ' Memory Requirements' - write(unit_,*) ' Cross sections = ' // trim(to_str(size_xs)) // ' bytes' - write(unit_,*) ' Probability Tables = ' // & - trim(to_str(size_urr)) // ' bytes' - - ! Blank line at end of nuclide - write(unit_,*) - - end subroutine print_nuclide - -!=============================================================================== -! PRINT_SAB_TABLE displays information about a S(a,b) table containing data -! describing thermal scattering from bound materials such as hydrogen in water. -!=============================================================================== - - subroutine print_sab_table(sab, unit) - type(SAlphaBeta), intent(in) :: sab - integer, intent(in), optional :: unit - - integer :: size_sab ! memory used by S(a,b) table - integer :: unit_ ! unit to write to - integer :: i ! Loop counter for parsing through sab % zaid - integer :: char_count ! Counter for the number of characters on a line - - ! set default unit for writing information - if (present(unit)) then - unit_ = unit - else - unit_ = OUTPUT_UNIT - end if - - ! Basic S(a,b) table information - write(unit_,*) 'S(a,b) Table ' // trim(sab % name) - write(unit_,'(A)',advance="no") ' zaids = ' - ! Initialize the counter based on the above string - char_count = 11 - do i = 1, sab % n_zaid - ! Deal with a line thats too long - if (char_count >= 73) then ! 73 = 80 - (5 ZAID chars + 1 space + 1 comma) - ! End the line - write(unit_,*) "" - ! Add 11 leading blanks - write(unit_,'(A)', advance="no") " " - ! reset the counter to 11 - char_count = 11 - end if - if (i < sab % n_zaid) then - ! Include a comma - write(unit_,'(A)',advance="no") trim(to_str(sab % zaid(i))) // ", " - char_count = char_count + len(trim(to_str(sab % zaid(i)))) + 2 - else - ! Don't include a comma, since we are all done - write(unit_,'(A)',advance="no") trim(to_str(sab % zaid(i))) - end if - - end do - write(unit_,*) "" ! Move to next line - write(unit_,*) ' awr = ' // trim(to_str(sab % awr)) - write(unit_,*) ' kT = ' // trim(to_str(sab % kT)) - - ! Inelastic data - write(unit_,*) ' # of Incoming Energies (Inelastic) = ' // & - trim(to_str(sab % n_inelastic_e_in)) - write(unit_,*) ' # of Outgoing Energies (Inelastic) = ' // & - trim(to_str(sab % n_inelastic_e_out)) - write(unit_,*) ' # of Outgoing Angles (Inelastic) = ' // & - trim(to_str(sab % n_inelastic_mu)) - write(unit_,*) ' Threshold for Inelastic = ' // & - trim(to_str(sab % threshold_inelastic)) - - ! Elastic data - if (sab % n_elastic_e_in > 0) then - write(unit_,*) ' # of Incoming Energies (Elastic) = ' // & - trim(to_str(sab % n_elastic_e_in)) - write(unit_,*) ' # of Outgoing Angles (Elastic) = ' // & - trim(to_str(sab % n_elastic_mu)) - write(unit_,*) ' Threshold for Elastic = ' // & - trim(to_str(sab % threshold_elastic)) - end if - - ! Determine memory used by S(a,b) table and write out - size_sab = 8 * (sab % n_inelastic_e_in * (2 + sab % n_inelastic_e_out * & - (1 + sab % n_inelastic_mu)) + sab % n_elastic_e_in * & - (2 + sab % n_elastic_mu)) - write(unit_,*) ' Memory Used = ' // trim(to_str(size_sab)) // ' bytes' - - ! Blank line at end - write(unit_,*) - - end subroutine print_sab_table - !=============================================================================== ! WRITE_XS_SUMMARY writes information about each nuclide and S(a,b) table to a ! file called cross_sections.out. This file shows the list of reactions as well @@ -486,8 +328,6 @@ contains integer :: i ! loop index integer :: unit_xs ! cross_sections.out file unit character(MAX_FILE_LEN) :: path ! path of summary file - type(Nuclide), pointer :: nuc - type(SAlphaBeta), pointer :: sab ! Create filename for log file path = trim(path_output) // "cross_sections.out" @@ -498,21 +338,22 @@ contains ! Write header call header("CROSS SECTION TABLES", unit=unit_xs) - NUCLIDE_LOOP: do i = 1, n_nuclides_total - ! Get pointer to nuclide - nuc => nuclides(i) + if (run_CE) then + NUCLIDE_LOOP: do i = 1, n_nuclides_total + ! Print information about nuclide + call nuclides(i) % print(unit=unit_xs) + end do NUCLIDE_LOOP - ! Print information about nuclide - call print_nuclide(nuc, unit=unit_xs) - end do NUCLIDE_LOOP - - SAB_TABLES_LOOP: do i = 1, n_sab_tables - ! Get pointer to S(a,b) table - sab => sab_tables(i) - - ! Print information about S(a,b) table - call print_sab_table(sab, unit=unit_xs) - end do SAB_TABLES_LOOP + SAB_TABLES_LOOP: do i = 1, n_sab_tables + ! Print information about S(a,b) table + call sab_tables(i) % print(unit=unit_xs) + end do SAB_TABLES_LOOP + else + NuclideMG_LOOP: do i = 1, n_nuclides_total + ! Print information about nuclide + call nuclides_mg(i) % obj % print(unit=unit_xs) + end do NuclideMG_LOOP + end if ! Close cross section summary file close(unit_xs) @@ -1334,7 +1175,7 @@ contains function get_label(t, i_filter) result(label) type(TallyObject), intent(in) :: t ! tally object integer, intent(in) :: i_filter ! index in filters array - character(100) :: label ! user-specified identifier + character(MAX_LINE_LEN) :: label ! user-specified identifier integer :: i ! index in cells/surfaces/etc array integer :: bin diff --git a/src/particle_header.F90 b/src/particle_header.F90 index fb02bc6a5..141f70c8b 100644 --- a/src/particle_header.F90 +++ b/src/particle_header.F90 @@ -47,9 +47,14 @@ module particle_header integer :: n_coord ! number of current coordinates type(LocalCoord) :: coord(MAX_COORD) ! coordinates for all levels + ! Energy Data + real(8) :: E ! post-collision energy + real(8) :: last_E ! pre-collision energy + integer :: g ! post-collision energy group (MG only) + integer :: last_g ! pre-collision energy group (MG only) + ! Other physical data real(8) :: wgt ! particle weight - real(8) :: E ! energy real(8) :: mu ! angle of scatter logical :: alive ! is particle alive? @@ -57,7 +62,6 @@ module particle_header real(8) :: last_xyz(3) ! previous coordinates real(8) :: last_uvw(3) ! previous direction coordinates real(8) :: last_wgt ! pre-collision particle weight - real(8) :: last_E ! pre-collision energy real(8) :: absorb_wgt ! weight absorbed for survival biasing ! What event last took place @@ -132,6 +136,7 @@ contains this % fission = .false. this % delayed_group = 0 this % n_delayed_bank(:) = 0 + this % g = 1 ! Set up base level coordinates this % coord(1) % universe = BASE_UNIVERSE @@ -178,9 +183,11 @@ contains ! fission, or simply as a secondary particle. !=============================================================================== - subroutine initialize_from_source(this, src) - class(Particle), intent(inout) :: this - type(Bank), intent(in) :: src + subroutine initialize_from_source(this, src, run_CE, energy_bin_avg) + class(Particle), intent(inout) :: this + type(Bank), intent(in) :: src + logical, intent(in) :: run_CE + real(8), allocatable, intent(in) :: energy_bin_avg(:) ! set defaults call this % initialize() @@ -192,8 +199,14 @@ contains this % coord(1) % uvw = src % uvw this % last_xyz = src % xyz this % last_uvw = src % uvw - this % E = src % E - this % last_E = src % E + if (run_CE) then + this % E = src % E + else + this % g = int(src % E) + this % last_g = int(src % E) + this % E = energy_bin_avg(this % g) + end if + this % last_E = src % E end subroutine initialize_from_source @@ -202,12 +215,13 @@ contains ! the secondary bank and increments the number of sites in the secondary bank. !=============================================================================== - subroutine create_secondary(this, uvw, type) + subroutine create_secondary(this, uvw, type, run_CE) class(Particle), intent(inout) :: this real(8), intent(in) :: uvw(3) integer, intent(in) :: type + logical, intent(in) :: run_CE - integer :: n + integer(8) :: n ! Check to make sure that the hard-limit on secondary particles is not ! exceeded. @@ -219,8 +233,11 @@ contains this % secondary_bank(n) % wgt = this % wgt this % secondary_bank(n) % xyz(:) = this % coord(1) % xyz this % secondary_bank(n) % uvw(:) = uvw - this % secondary_bank(n) % E = this % E this % n_secondary = n + this % secondary_bank(this % n_secondary) % E = this % E + if (.not. run_CE) then + this % secondary_bank(this % n_secondary) % E = real(this % g, 8) + end if end subroutine create_secondary diff --git a/src/particle_restart.F90 b/src/particle_restart.F90 index 2e0523d48..9d49a4f97 100644 --- a/src/particle_restart.F90 +++ b/src/particle_restart.F90 @@ -97,6 +97,7 @@ contains call read_dataset(file_id, 'id', p%id) call read_dataset(file_id, 'weight', p%wgt) call read_dataset(file_id, 'energy', p%E) + call read_dataset(file_id, 'energy_group', p%g) call read_dataset(file_id, 'xyz', p%coord(1)%xyz) call read_dataset(file_id, 'uvw', p%coord(1)%uvw) @@ -105,6 +106,7 @@ contains p%last_xyz = p%coord(1)%xyz p%last_uvw = p%coord(1)%uvw p%last_E = p%E + p%last_g = p%g ! Close hdf5 file call file_close(file_id) diff --git a/src/particle_restart_write.F90 b/src/particle_restart_write.F90 index edd779df0..d983b3db8 100644 --- a/src/particle_restart_write.F90 +++ b/src/particle_restart_write.F90 @@ -1,10 +1,10 @@ module particle_restart_write - use bank_header, only: Bank + use bank_header, only: Bank use global use hdf5_interface - use particle_header, only: Particle - use string, only: to_str + use particle_header, only: Particle + use string, only: to_str use hdf5 diff --git a/src/physics.F90 b/src/physics.F90 index da2682ebf..d6c4c45b0 100644 --- a/src/physics.F90 +++ b/src/physics.F90 @@ -1,23 +1,23 @@ module physics - use ace_header, only: Nuclide, Reaction use constants use cross_section, only: elastic_xs_0K use endf, only: reaction_name use error, only: fatal_error, warning - use fission, only: nu_total, nu_delayed use global - use interpolation, only: interpolate_tab1 use material_header, only: Material - use math, only: rotate_angle, maxwell_spectrum, watt_spectrum + use math use mesh, only: get_mesh_indices + use nuclide_header use output, only: write_message use particle_header, only: Particle use particle_restart_write, only: write_particle_restart - use random_lcg, only: prn + use physics_common + use random_lcg, only: prn, advance_prn_seed, prn_set_stream + use reaction_header, only: Reaction use search, only: binary_search - use string, only: to_str use secondary_uncorrelated, only: UncorrelatedAngleEnergy + use string, only: to_str implicit none @@ -56,6 +56,13 @@ contains if (master) call warning("Killing neutron with extremely low energy") end if + ! Advance URR seed stream 'N' times after energy changes + if (p % E /= p % last_E) then + call prn_set_stream(STREAM_URR_PTABLE) + call advance_prn_seed(n_nuc_zaid_total) + call prn_set_stream(STREAM_TRACKING) + endif + end subroutine collision !=============================================================================== @@ -73,7 +80,7 @@ contains integer :: i_nuclide ! index in nuclides array integer :: i_nuc_mat ! index in material's nuclides array integer :: i_reaction ! index in nuc % reactions array - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc call sample_nuclide(p, 'total ', i_nuclide, i_nuc_mat) @@ -196,7 +203,7 @@ contains real(8) :: f real(8) :: prob real(8) :: cutoff - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc ! Get pointer to nuclide nuc => nuclides(i_nuclide) @@ -242,7 +249,6 @@ contains !=============================================================================== subroutine absorption(p, i_nuclide) - type(Particle), intent(inout) :: p integer, intent(in) :: i_nuclide @@ -278,33 +284,11 @@ contains end subroutine absorption -!=============================================================================== -! RUSSIAN_ROULETTE -!=============================================================================== - - subroutine russian_roulette(p) - - type(Particle), intent(inout) :: p - - if (p % wgt < weight_cutoff) then - if (prn() < p % wgt / weight_survive) then - p % wgt = weight_survive - p % last_wgt = p % wgt - else - p % wgt = ZERO - p % last_wgt = ZERO - p % alive = .false. - end if - end if - - end subroutine russian_roulette - !=============================================================================== ! SCATTER !=============================================================================== subroutine scatter(p, i_nuclide, i_nuc_mat) - type(Particle), intent(inout) :: p integer, intent(in) :: i_nuclide integer, intent(in) :: i_nuc_mat @@ -317,7 +301,7 @@ contains real(8) :: uvw_new(3) ! outgoing uvw for iso-in-lab scattering real(8) :: uvw_old(3) ! incoming uvw for iso-in-lab scattering real(8) :: phi ! azimuthal angle for iso-in-lab scattering - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc ! copy incoming direction uvw_old(:) = p % coord(1) % uvw @@ -432,7 +416,7 @@ contains real(8) :: v_cm(3) ! velocity of center-of-mass real(8) :: v_t(3) ! velocity of target nucleus real(8) :: uvw_cm(3) ! directional cosines in center-of-mass - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc ! get pointer to nuclide nuc => nuclides(i_nuclide) @@ -461,9 +445,9 @@ contains vel = sqrt(dot_product(v_n, v_n)) ! Sample scattering angle - select type (dist => rxn%secondary%distribution(1)%obj) + select type (dist => rxn % products(1) % distribution(1) % obj) type is (UncorrelatedAngleEnergy) - mu_cm = dist%angle%sample(E) + mu_cm = dist % angle % sample(E) end select ! Determine direction cosines in CM @@ -501,7 +485,6 @@ contains !=============================================================================== subroutine sab_scatter(i_nuclide, i_sab, E, uvw, mu) - integer, intent(in) :: i_nuclide ! index in micro_xs integer, intent(in) :: i_sab ! index in sab_tables real(8), intent(inout) :: E ! incoming/outgoing energy @@ -759,7 +742,7 @@ contains !=============================================================================== subroutine sample_target_velocity(nuc, v_target, E, uvw, v_neut, wgt, xs_eff) - type(Nuclide), intent(in) :: nuc ! target nuclide at temperature T + type(NuclideCE), intent(in) :: nuc ! target nuclide at temperature T real(8), intent(out) :: v_target(3) ! target velocity real(8), intent(in) :: v_neut(3) ! neutron velocity real(8), intent(in) :: E ! particle energy @@ -1004,10 +987,10 @@ contains !=============================================================================== subroutine sample_cxs_target_velocity(nuc, v_target, E, uvw) - type(Nuclide), intent(in) :: nuc ! target nuclide at temperature - real(8), intent(out) :: v_target(3) - real(8), intent(in) :: E - real(8), intent(in) :: uvw(3) + type(NuclideCE), intent(in) :: nuc ! target nuclide at temperature + real(8), intent(out) :: v_target(3) + real(8), intent(in) :: E + real(8), intent(in) :: uvw(3) real(8) :: kT ! equilibrium temperature of target in MeV real(8) :: awr ! target/neutron mass ratio @@ -1088,11 +1071,9 @@ contains integer :: nu ! actual number of neutrons produced integer :: ijk(3) ! indices in ufs mesh real(8) :: nu_t ! total nu - real(8) :: mu ! fission neutron angular cosine - real(8) :: phi ! fission neutron azimuthal angle real(8) :: weight ! weight adjustment for ufs method logical :: in_mesh ! source site in ufs mesh? - type(Nuclide), pointer :: nuc + type(NuclideCE), pointer :: nuc ! Get pointers nuc => nuclides(i_nuclide) @@ -1160,25 +1141,12 @@ contains ! Set weight of fission bank site bank_array(i) % wgt = ONE/weight - ! Sample cosine of angle -- fission neutrons are always emitted - ! isotropically. Sometimes in ACE data, fission reactions actually have - ! an angular distribution listed, but for those that do, it's simply just - ! a uniform distribution in mu - mu = TWO * prn() - ONE + ! Sample delayed group and angle/energy for fission reaction + call sample_fission_neutron(nuc, nuc % reactions(i_reaction), & + p % E, bank_array(i)) - ! Sample azimuthal angle uniformly in [0,2*pi) - phi = TWO*PI*prn() - bank_array(i) % uvw(1) = mu - bank_array(i) % uvw(2) = sqrt(ONE - mu*mu) * cos(phi) - bank_array(i) % uvw(3) = sqrt(ONE - mu*mu) * sin(phi) - - ! Sample secondary energy distribution for fission reaction and set energy - ! in fission bank - bank_array(i) % E = sample_fission_energy(nuc, & - nuc % reactions(i_reaction), p) - - ! Set the delayed group of the neutron - bank_array(i) % delayed_group = p % delayed_group + ! Set delayed group on particle too + p % delayed_group = bank_array(i) % delayed_group ! Increment the number of neutrons born delayed if (p % delayed_group > 0) then @@ -1197,35 +1165,41 @@ contains end subroutine create_fission_sites !=============================================================================== -! SAMPLE_FISSION_ENERGY +! SAMPLE_FISSION_NEUTRON !=============================================================================== - function sample_fission_energy(nuc, rxn, p) result(E_out) + subroutine sample_fission_neutron(nuc, rxn, E_in, site) + type(NuclideCE), intent(in) :: nuc + type(Reaction), intent(in) :: rxn + real(8), intent(in) :: E_in + type(Bank), intent(inout) :: site - type(Nuclide), intent(in) :: nuc - type(Reaction), intent(in) :: rxn - type(Particle), intent(inout) :: p ! Particle causing fission - real(8) :: E_out ! outgoing energy of fission neutron - - integer :: j ! index on nu energy grid / precursor group - integer :: lc ! index before start of energies/nu values - integer :: NR ! number of interpolation regions - integer :: NE ! number of energies tabulated - integer :: n_sample ! number of times resampling + integer :: group ! index on nu energy grid / precursor group + integer :: n_sample ! number of resamples real(8) :: nu_t ! total nu real(8) :: nu_d ! delayed nu real(8) :: beta ! delayed neutron fraction real(8) :: xi ! random number real(8) :: yield ! delayed neutron precursor yield real(8) :: prob ! cumulative probability + real(8) :: mu ! cosine of scattering angle + real(8) :: phi ! azimuthal angle - ! Determine total nu - nu_t = nu_total(nuc, p % E) + ! Sample cosine of angle -- fission neutrons are always emitted + ! isotropically. Sometimes in ACE data, fission reactions actually have + ! an angular distribution listed, but for those that do, it's simply just + ! a uniform distribution in mu + mu = TWO * prn() - ONE - ! Determine delayed nu - nu_d = nu_delayed(nuc, p % E) + ! Sample azimuthal angle uniformly in [0,2*pi) + phi = TWO*PI*prn() + site % uvw(1) = mu + site % uvw(2) = sqrt(ONE - mu*mu) * cos(phi) + site % uvw(3) = sqrt(ONE - mu*mu) * sin(phi) - ! Determine delayed neutron fraction + ! Determine total nu, delayed nu, and delayed neutron fraction + nu_t = nuc % nu(E_in, EMISSION_TOTAL) + nu_d = nuc % nu(E_in, EMISSION_DELAYED) beta = nu_d / nu_t if (prn() < beta) then @@ -1233,51 +1207,41 @@ contains ! DELAYED NEUTRON SAMPLED ! sampled delayed precursor group - xi = prn() - lc = 1 + xi = prn()*nu_d prob = ZERO - do j = 1, nuc % n_precursor - ! determine number of interpolation regions and energies - NR = int(nuc % nu_d_precursor_data(lc + 1)) - NE = int(nuc % nu_d_precursor_data(lc + 2 + 2*NR)) + do group = 1, nuc % n_precursor ! determine delayed neutron precursor yield for group j - yield = interpolate_tab1(nuc % nu_d_precursor_data( & - lc+1:lc+2+2*NR+2*NE), p % E) + yield = rxn % products(1 + group) % yield % evaluate(E_in) ! Check if this group is sampled prob = prob + yield if (xi < prob) exit - - ! advance pointer - lc = lc + 2 + 2*NR + 2*NE + 1 end do ! if the sum of the probabilities is slightly less than one and the ! random number is greater, j will be greater than nuc % ! n_precursor -- check for this condition - j = min(j, nuc % n_precursor) + group = min(group, nuc % n_precursor) ! set the delayed group for the particle born from fission - p % delayed_group = j + site % delayed_group = group - ! sample from energy distribution n_sample = 0 do - select type (aedist => nuc%nu_d_edist(j)%obj) - type is (UncorrelatedAngleEnergy) - E_out = aedist%energy%sample(p%E) - end select + ! sample from energy/angle distribution -- note that mu has already been + ! sampled above and doesn't need to be resampled + call rxn % products(1 + group) % sample(E_in, site % E, mu) ! resample if energy is greater than maximum neutron energy - if (E_out < energy_max_neutron) exit + if (site % E < energy_max_neutron) exit ! check for large number of resamples n_sample = n_sample + 1 if (n_sample == MAX_SAMPLE) then ! call write_particle_restart(p) call fatal_error("Resampled energy distribution maximum number of " & - &// "times for nuclide " // nuc % name) + // "times for nuclide " // nuc % name) end if end do @@ -1286,28 +1250,27 @@ contains ! PROMPT NEUTRON SAMPLED ! set the delayed group for the particle born from fission to 0 - p % delayed_group = 0 + site % delayed_group = 0 ! sample from prompt neutron energy distribution n_sample = 0 do - call rxn%secondary%sample(p%E, E_out, prob) + call rxn % products(1) % sample(E_in, site % E, mu) ! resample if energy is greater than maximum neutron energy - if (E_out < energy_max_neutron) exit + if (site % E < energy_max_neutron) exit ! check for large number of resamples n_sample = n_sample + 1 if (n_sample == MAX_SAMPLE) then ! call write_particle_restart(p) call fatal_error("Resampled energy distribution maximum number of " & - &// "times for nuclide " // nuc % name) + // "times for nuclide " // nuc % name) end if end do - end if - end function sample_fission_energy + end subroutine sample_fission_neutron !=============================================================================== ! INELASTIC_SCATTER handles all reactions with a single secondary neutron (other @@ -1315,9 +1278,9 @@ contains !=============================================================================== subroutine inelastic_scatter(nuc, rxn, p) - type(Nuclide), intent(in) :: nuc - type(Reaction), intent(in) :: rxn - type(Particle), intent(inout) :: p + type(NuclideCE), intent(in) :: nuc + type(Reaction), intent(in) :: rxn + type(Particle), intent(inout) :: p integer :: i ! loop index real(8) :: E ! energy in lab (incoming/outgoing) @@ -1331,7 +1294,7 @@ contains E_in = p % E ! sample outgoing energy and scattering cosine - call rxn%secondary%sample(E_in, E, mu) + call rxn % products(1) % sample(E_in, E, mu) ! if scattering system is in center-of-mass, transfer cosine of scattering ! angle and outgoing energy from CM to LAB @@ -1359,14 +1322,16 @@ contains ! change direction of particle p % coord(1) % uvw = rotate_angle(p % coord(1) % uvw, mu) - ! change weight of particle based on yield - if (rxn % multiplicity_with_E) then - yield = interpolate_tab1(rxn % multiplicity_E, E_in) - p % wgt = yield * p % wgt - else - do i = 1, rxn % multiplicity - 1 - call p % create_secondary(p % coord(1) % uvw, NEUTRON) + ! evaluate yield + yield = rxn % products(1) % yield % evaluate(E_in) + if (mod(yield, ONE) == ZERO) then + ! If yield is integral, create exactly that many secondary particles + do i = 1, nint(yield) - 1 + call p % create_secondary(p % coord(1) % uvw, NEUTRON, run_CE=.true.) end do + else + ! Otherwise, change weight of particle based on yield + p % wgt = yield * p % wgt end if end subroutine inelastic_scatter diff --git a/src/physics_common.F90 b/src/physics_common.F90 new file mode 100644 index 000000000..98d240c07 --- /dev/null +++ b/src/physics_common.F90 @@ -0,0 +1,33 @@ +module physics_common + + use constants + use global, only: weight_cutoff, weight_survive + use particle_header, only: Particle + use random_lcg, only: prn + + implicit none + +contains + +!=============================================================================== +! RUSSIAN_ROULETTE +!=============================================================================== + + subroutine russian_roulette(p) + + type(Particle), intent(inout) :: p + + if (p % wgt < weight_cutoff) then + if (prn() < p % wgt / weight_survive) then + p % wgt = weight_survive + p % last_wgt = p % wgt + else + p % wgt = ZERO + p % last_wgt = ZERO + p % alive = .false. + end if + end if + + end subroutine russian_roulette + +end module physics_common diff --git a/src/physics_mg.F90 b/src/physics_mg.F90 new file mode 100644 index 000000000..6a58540c1 --- /dev/null +++ b/src/physics_mg.F90 @@ -0,0 +1,271 @@ +module physics_mg + ! This module contains the multi-group specific physics routines so as to not + ! hinder performance of the CE versions with multiple if-thens. + + use constants + use error, only: fatal_error, warning + use global + use macroxs_header, only: MacroXS, MacroXSContainer + use material_header, only: Material + use math, only: rotate_angle + use mesh, only: get_mesh_indices + use output, only: write_message + use particle_header, only: Particle + use particle_restart_write, only: write_particle_restart + use physics_common + use random_lcg, only: prn + use scattdata_header + use string, only: to_str + + implicit none + +contains + +!=============================================================================== +! COLLISION_MG samples a nuclide and reaction and then calls the appropriate +! routine for that reaction +!=============================================================================== + + subroutine collision_mg(p) + + type(Particle), intent(inout) :: p + + ! Store pre-collision particle properties + p % last_wgt = p % wgt + p % last_g = p % g + p % last_E = p % E + p % last_uvw = p % coord(1) % uvw + + ! Add to collision counter for particle + p % n_collision = p % n_collision + 1 + + ! Sample nuclide/reaction for the material the particle is in + call sample_reaction(p) + + ! Display information about collision + if (verbosity >= 10 .or. trace) then + call write_message(" " // "Energy Group = " // trim(to_str(p % g))) + end if + + end subroutine collision_mg + +!=============================================================================== +! SAMPLE_REACTION samples a nuclide based on the macroscopic cross sections for +! each nuclide within a material and then samples a reaction for that nuclide +! and calls the appropriate routine to process the physics. Note that there is +! special logic when suvival biasing is turned on since fission and +! disappearance are treated implicitly. +!=============================================================================== + + subroutine sample_reaction(p) + + type(Particle), intent(inout) :: p + + type(Material), pointer :: mat + + mat => materials(p % material) + + ! Create fission bank sites. Note that while a fission reaction is sampled, + ! it never actually "happens", i.e. the weight of the particle does not + ! change when sampling fission sites. The following block handles all + ! absorption (including fission) + + if (mat % fissionable) then + if (run_mode == MODE_EIGENVALUE) then + call create_fission_sites(p, fission_bank, n_bank) + elseif (run_mode == MODE_FIXEDSOURCE) then + call create_fission_sites(p, p % secondary_bank, p % n_secondary) + end if + end if + ! If survival biasing is being used, the following subroutine adjusts the + ! weight of the particle. Otherwise, it checks to see if absorption occurs + + if (material_xs % absorption > ZERO) then + call absorption(p) + else + p % absorb_wgt = ZERO + end if + if (.not. p % alive) return + + ! Sample a scattering reaction and determine the secondary energy of the + ! exiting neutron + call scatter(p) + + ! Play russian roulette if survival biasing is turned on + if (survival_biasing) then + call russian_roulette(p) + if (.not. p % alive) return + end if + + end subroutine sample_reaction + +!=============================================================================== +! ABSORPTION +!=============================================================================== + + subroutine absorption(p) + + type(Particle), intent(inout) :: p + + if (survival_biasing) then + ! Determine weight absorbed in survival biasing + p % absorb_wgt = (p % wgt * & + material_xs % absorption / material_xs % total) + + ! Adjust weight of particle by probability of absorption + p % wgt = p % wgt - p % absorb_wgt + p % last_wgt = p % wgt + + ! Score implicit absorption estimate of keff +!$omp atomic + global_tallies(K_ABSORPTION) % value = & + global_tallies(K_ABSORPTION) % value + p % absorb_wgt * & + material_xs % nu_fission / material_xs % absorption + else + ! See if disappearance reaction happens + if (material_xs % absorption > prn() * material_xs % total) then + ! Score absorption estimate of keff +!$omp atomic + global_tallies(K_ABSORPTION) % value = & + global_tallies(K_ABSORPTION) % value + p % wgt * & + material_xs % nu_fission / material_xs % absorption + + p % alive = .false. + p % event = EVENT_ABSORB + end if + end if + + end subroutine absorption + +!=============================================================================== +! SCATTER +!=============================================================================== + + subroutine scatter(p) + + type(Particle), intent(inout) :: p + + call macro_xs(p % material) % obj % sample_scatter(p % coord(1) % uvw, & + p % last_g, p % g, & + p % mu, p % wgt) + + ! Update energy value for downstream compatability (in tallying) + p % E = energy_bin_avg(p % g) + + ! Convert change in angle (mu) to new direction + p % coord(1) % uvw = rotate_angle(p % coord(1) % uvw, p % mu) + + ! Set event component + p % event = EVENT_SCATTER + + end subroutine scatter + +!=============================================================================== +! CREATE_FISSION_SITES determines the average total, prompt, and delayed +! neutrons produced from fission and creates appropriate bank sites. +!=============================================================================== + + subroutine create_fission_sites(p, bank_array, size_bank) + type(Particle), intent(inout) :: p + type(Bank), intent(inout) :: bank_array(:) + integer(8), intent(inout) :: size_bank + + integer :: i ! loop index + integer :: nu ! actual number of neutrons produced + integer :: ijk(3) ! indices in ufs mesh + real(8) :: nu_t ! total nu + real(8) :: mu ! fission neutron angular cosine + real(8) :: phi ! fission neutron azimuthal angle + real(8) :: weight ! weight adjustment for ufs method + logical :: in_mesh ! source site in ufs mesh? + class(MacroXS), pointer :: xs + + ! Get Pointers + xs => macro_xs(p % material) % obj + + ! TODO: Heat generation from fission + + ! If uniform fission source weighting is turned on, we increase of decrease + ! the expected number of fission sites produced + + if (ufs) then + ! Determine indices on ufs mesh for current location + call get_mesh_indices(ufs_mesh, p % coord(1) % xyz, ijk, in_mesh) + if (.not. in_mesh) then + call write_particle_restart(p) + call fatal_error("Source site outside UFS mesh!") + end if + + if (source_frac(1,ijk(1),ijk(2),ijk(3)) /= ZERO) then + weight = ufs_mesh % volume_frac / source_frac(1,ijk(1),ijk(2),ijk(3)) + else + weight = ONE + end if + else + weight = ONE + end if + + ! Determine expected number of neutrons produced + nu_t = p % wgt / keff * weight * & + material_xs % nu_fission / material_xs % total + ! Sample number of neutrons produced + if (prn() > nu_t - int(nu_t)) then + nu = int(nu_t) + else + nu = int(nu_t) + 1 + end if + + ! Check for bank size getting hit. For fixed source calculations, this is a + ! fatal error. For eigenvalue calculations, it just means that k-effective + ! was too high for a single batch. + if (size_bank + nu > size(bank_array)) then + if (run_mode == MODE_FIXEDSOURCE) then + call fatal_error("Secondary particle bank size limit reached. If you & + &are running a subcritical multiplication problem, k-effective & + &may be too close to one.") + else + if (master) call warning("Maximum number of sites in fission bank & + &reached. This can result in irreproducible results using different & + &numbers of processes/threads.") + end if + end if + + ! Bank source neutrons + if (nu == 0 .or. size_bank == size(bank_array)) return + + p % fission = .true. ! Fission neutrons will be banked + do i = int(size_bank,4) + 1, int(min(size_bank + nu, int(size(bank_array),8)),4) + ! Bank source neutrons by copying particle data + bank_array(i) % xyz = p % coord(1) % xyz + + ! Set weight of fission bank site + bank_array(i) % wgt = ONE/weight + + ! Sample cosine of angle -- fission neutrons are always emitted + ! isotropically. Sometimes in ACE data, fission reactions actually have + ! an angular distribution listed, but for those that do, it's simply just + ! a uniform distribution in mu + mu = TWO * prn() - ONE + + ! Sample azimuthal angle uniformly in [0,2*pi) + phi = TWO*PI*prn() + bank_array(i) % uvw(1) = mu + bank_array(i) % uvw(2) = sqrt(ONE - mu*mu) * cos(phi) + bank_array(i) % uvw(3) = sqrt(ONE - mu*mu) * sin(phi) + + ! Sample secondary energy distribution for fission reaction and set energy + ! in fission bank + bank_array(i) % E = & + real(xs % sample_fission_energy(p % g, fission_bank(i) % uvw), 8) + end do + + ! increment number of bank sites + size_bank = min(size_bank + nu, int(size(bank_array),8)) + + ! Store total weight banked for analog fission tallies + p % n_bank = nu + p % wgt_bank = nu/weight + + end subroutine create_fission_sites + +end module physics_mg diff --git a/src/plot.F90 b/src/plot.F90 index 75d0bc944..796cce6af 100644 --- a/src/plot.F90 +++ b/src/plot.F90 @@ -9,7 +9,7 @@ module plot use mesh, only: get_mesh_indices use mesh_header, only: RegularMesh use output, only: write_message - use particle_header, only: Particle, LocalCoord + use particle_header, only: LocalCoord, Particle use plot_header use ppmlib, only: Image, init_image, allocate_image, & deallocate_image, set_pixel @@ -56,7 +56,7 @@ contains subroutine position_rgb(p, pl, rgb, id) - type(Particle), intent(inout) :: p + type(Particle), intent(inout) :: p type(ObjectPlot), pointer, intent(in) :: pl integer, intent(out) :: rgb(3) integer, intent(out) :: id @@ -364,7 +364,7 @@ contains real(8) :: ll(3) ! lower left starting point for each sweep direction type(Particle) :: p type(ProgressBar) :: progress - type(c_ptr) :: f_ptr + type(c_ptr) :: f_ptr ! compute voxel widths in each direction vox = pl % width/dble(pl % pixels) diff --git a/src/product_header.F90 b/src/product_header.F90 new file mode 100644 index 000000000..e20c173b4 --- /dev/null +++ b/src/product_header.F90 @@ -0,0 +1,62 @@ +module product_header + + use angleenergy_header, only: AngleEnergyContainer + use constants, only: ZERO, MAX_WORD_LEN, EMISSION_PROMPT, EMISSION_DELAYED, & + EMISSION_TOTAL, NEUTRON, PHOTON + use endf_header, only: Tabulated1D, Function1D, Constant1D, Polynomial + use random_lcg, only: prn + +!=============================================================================== +! REACTIONPRODUCT stores a data for a reaction product including its yield and +! angle-energy distributions, each of which has a given probability of occurring +! for a given incoming energy. In general, most products only have one +! angle-energy distribution, but for some cases (e.g., (n,2n) in certain +! nuclides) multiple distinct distributions exist. +!=============================================================================== + + type :: ReactionProduct + integer :: particle + integer :: emission_mode ! prompt, delayed, or total emission + real(8) :: decay_rate ! Decay rate for delayed neutron precursors + class(Function1D), pointer :: yield => null() ! Energy-dependent neutron yield + type(Tabulated1D), allocatable :: applicability(:) + type(AngleEnergyContainer), allocatable :: distribution(:) + contains + procedure :: sample => reactionproduct_sample + end type ReactionProduct + +contains + + subroutine reactionproduct_sample(this, E_in, E_out, mu) + class(ReactionProduct), intent(in) :: this + real(8), intent(in) :: E_in ! incoming energy + real(8), intent(out) :: E_out ! sampled outgoing energy + real(8), intent(out) :: mu ! sampled scattering cosine + + integer :: i ! loop counter + integer :: n ! number of angle-energy distributions + real(8) :: prob ! cumulative probability + real(8) :: c ! sampled cumulative probability + + n = size(this%applicability) + if (n > 1) then + prob = ZERO + c = prn() + do i = 1, n + ! Determine probability that i-th energy distribution is sampled + prob = prob + this % applicability(i) % evaluate(E_in) + + ! If i-th distribution is sampled, sample energy from the distribution + if (c <= prob) then + call this%distribution(i)%obj%sample(E_in, E_out, mu) + exit + end if + end do + else + ! If only one distribution is present, go ahead and sample it + call this%distribution(1)%obj%sample(E_in, E_out, mu) + end if + + end subroutine reactionproduct_sample + +end module product_header diff --git a/src/random_lcg.F90 b/src/random_lcg.F90 index 8f50477c5..08f1034ab 100644 --- a/src/random_lcg.F90 +++ b/src/random_lcg.F90 @@ -24,9 +24,10 @@ module random_lcg !$omp threadprivate(prn_seed, stream) public :: prn + public :: future_prn public :: initialize_prng public :: set_particle_seed - public :: prn_skip + public :: advance_prn_seed public :: prn_set_stream public :: STREAM_TRACKING, STREAM_TALLIES @@ -52,6 +53,21 @@ contains end function prn +!=============================================================================== +! FUTURE_PRN generates a pseudo-random number which is 'n' times ahead from the +! current seed. +!=============================================================================== + + function future_prn(n) result(pseudo_rn) + + integer(8), intent(in) :: n ! number of prns to skip + + real(8) :: pseudo_rn + + pseudo_rn = future_seed(n, prn_seed(stream)) * prn_norm + + end function future_prn + !=============================================================================== ! INITIALIZE_PRNG sets up the random number generator, determining the seed and ! values for g, c, and m. @@ -90,31 +106,32 @@ contains integer :: i do i = 1, N_STREAMS - prn_seed(i) = prn_skip_ahead(id*prn_stride, prn_seed0 + i - 1) + prn_seed(i) = future_seed(id*prn_stride, prn_seed0 + i - 1) end do end subroutine set_particle_seed !=============================================================================== -! PRN_SKIP advances the random number seed 'n' times from the current seed +! ADVANCE_PRN_SEED advances the random number seed 'n' times from the current +! seed. !=============================================================================== - subroutine prn_skip(n) + subroutine advance_prn_seed(n) integer(8), intent(in) :: n ! number of seeds to skip - prn_seed(stream) = prn_skip_ahead(n, prn_seed(stream)) + prn_seed(stream) = future_seed(n, prn_seed(stream)) - end subroutine prn_skip + end subroutine advance_prn_seed !=============================================================================== -! PRN_SKIP_AHEAD advances the random number seed 'skip' times. This is usually +! FUTURE_SEED advances the random number seed 'skip' times. This is usually ! used to skip a fixed number of random numbers (the stride) so that a given ! particle always has the same starting seed regardless of how many processors ! are used !=============================================================================== - function prn_skip_ahead(n, seed) result(new_seed) + function future_seed(n, seed) result(new_seed) integer(8), intent(in) :: n ! number of seeds to skip integer(8), intent(in) :: seed ! original seed @@ -166,7 +183,7 @@ contains ! With G and C, we can now find the new seed new_seed = iand(g_new*seed + c_new, prn_mask) - end function prn_skip_ahead + end function future_seed !=============================================================================== ! PRN_SET_STREAM changes the random number stream. If random numbers are needed diff --git a/src/reaction_header.F90 b/src/reaction_header.F90 new file mode 100644 index 000000000..160ad6323 --- /dev/null +++ b/src/reaction_header.F90 @@ -0,0 +1,21 @@ +module reaction_header + + use product_header, only: ReactionProduct + + implicit none + +!=============================================================================== +! REACTION contains the cross-section and secondary energy and angle +! distributions for a single reaction in a continuous-energy ACE-format table +!=============================================================================== + + type Reaction + integer :: MT ! ENDF MT value + real(8) :: Q_value ! Reaction Q value + integer :: threshold ! Energy grid index of threshold + logical :: scatter_in_cm ! scattering system in center-of-mass? + real(8), allocatable :: sigma(:) ! Cross section values + type(ReactionProduct), allocatable :: products(:) + end type Reaction + +end module reaction_header diff --git a/src/relaxng/materials.rnc b/src/relaxng/materials.rnc index da68ebf9e..21b36c07e 100644 --- a/src/relaxng/materials.rnc +++ b/src/relaxng/materials.rnc @@ -11,10 +11,10 @@ element materials { } & element nuclide { - (element name { xsd:string { maxLength = "7" } } | + (element name { xsd:string { maxLength = "7" } } | attribute name { xsd:string { maxLength = "7" } }) & - (element xs { xsd:string { maxLength = "3" } } | - attribute xs { xsd:string { maxLength = "3" } })? & + (element xs { xsd:string { maxLength = "5" } } | + attribute xs { xsd:string { maxLength = "5" } })? & (element scattering { ( "data" | "iso-in-lab" ) } | attribute scattering { ( "data" | "iso-in-lab" ) })? & ( @@ -23,11 +23,18 @@ element materials { ) }* & + element macroscopic { + (element name { xsd:string } | + attribute name { xsd:string }) & + (element xs { xsd:string { maxLength = "5" } } | + attribute xs { xsd:string { maxLength = "5" } }) + }* & + element element { - (element name { xsd:string { maxLength = "2" } } | + (element name { xsd:string { maxLength = "2" } } | attribute name { xsd:string { maxLength = "2" } }) & - (element xs { xsd:string { maxLength = "3" } } | - attribute xs { xsd:string { maxLength = "3" } })? & + (element xs { xsd:string { maxLength = "5" } } | + attribute xs { xsd:string { maxLength = "5" } })? & (element scattering { ( "data" | "iso-in-lab" ) } | attribute scattering { ( "data" | "iso-in-lab" ) })? & ( @@ -37,12 +44,12 @@ element materials { }* & element sab { - (element name { xsd:string { maxLength = "7" } } | + (element name { xsd:string { maxLength = "7" } } | attribute name { xsd:string { maxLength = "7" } }) & - (element xs { xsd:string { maxLength = "3" } } | - attribute xs { xsd:string { maxLength = "3" } })? + (element xs { xsd:string { maxLength = "5" } } | + attribute xs { xsd:string { maxLength = "5" } })? }* }+ & - element default_xs { xsd:string { maxLength = "3" } }? + element default_xs { xsd:string { maxLength = "5" } }? } diff --git a/src/relaxng/materials.rng b/src/relaxng/materials.rng index 7aba5f738..6a4bc3964 100644 --- a/src/relaxng/materials.rng +++ b/src/relaxng/materials.rng @@ -118,6 +118,36 @@ + + + + + + + 7 + + + + + 7 + + + + + + + 3 + + + + + 3 + + + + + + diff --git a/src/relaxng/mg_cross_sections.rnc b/src/relaxng/mg_cross_sections.rnc new file mode 100644 index 000000000..b2aaec4d4 --- /dev/null +++ b/src/relaxng/mg_cross_sections.rnc @@ -0,0 +1,61 @@ +element cross_sections { + + element groups { xsd:int } & + + element group_structure { list { xsd:double+ } } & + + element inverse_velocities { list { xsd:double+ } }? & + + element xsdata { + (element name { xsd:string { maxLength = "15" } } | + attribute name { xsd:string { maxLength = "15" } }) & + (element alias { xsd:string { maxLength = "15" } } | + attribute alias { xsd:string { maxLength = "15" } })? & + (element kT { xsd:double } | attribute kT { xsd:double })? & + (element fissionable { ( "true" | "false" ) } | + attribute fissionable { ( "true" | "false" ) }) & + (element representation { ( "isotropic" | "angle" ) } | + attribute representation { ( "isotropic" | "angle" ) })? & + (element num_azimuthal { xsd:positiveInteger } | + attribute num_azimuthal { xsd:positiveInteger })? & + (element num_polar { xsd:positiveInteger } | + attribute num_polar { xsd:positiveInteger })? & + (element scatt_type { ( "legendre" | "histogram" | "tabular" ) } | + attribute scatt_type { ( "legendre" | "histogram" | "tabular" ) })? & + (element order { xsd:positiveInteger } | + attribute order { xsd:positiveInteger }) & + element tabular_legendre { + (element enable { ( "true" | "false" ) } | + attribute enable { ( "true" | "false" ) })? & + (element num_points { xsd:positiveInteger } | + attribute num_points { xsd:positiveInteger })? + }? & + + (element total { list { xsd:double+ } } | + attribute total { list { xsd:double+ } })? & + + (element absorption { list { xsd:double+ } } | + attribute absorption { list { xsd:double+ } }) & + + (element scatter { list { xsd:double+ } } | + attribute scatter { list { xsd:double+ } }) & + + (element fission { list { xsd:double+ } } | + attribute fission { list { xsd:double+ } })? & + + (element fission { list { xsd:double+ } } | + attribute fission { list { xsd:double+ } })? & + + (element k_fission { list { xsd:double+ } } | + attribute k_fission { list { xsd:double+ } })? & + + (element chi { list { xsd:double+ } } | + attribute chi { list { xsd:double+ } })? & + + (element nu_fission { list { xsd:double+ } } | + attribute nu_fission { list { xsd:double+ } })? + + }* + + +} \ No newline at end of file diff --git a/src/relaxng/mg_cross_sections.rng b/src/relaxng/mg_cross_sections.rng new file mode 100644 index 000000000..b293cddbe --- /dev/null +++ b/src/relaxng/mg_cross_sections.rng @@ -0,0 +1,314 @@ + + + + + + + + + + + + + + + + + + + + + + + + + + + + + 15 + + + + + 15 + + + + + + + + 15 + + + + + 15 + + + + + + + + + + + + + + + + + + true + false + + + + + true + false + + + + + + + + isotropic + angle + + + + + isotropic + angle + + + + + + + + + + + + + + + + + + + + + + + + + + + + + legendre + histogram + tabular + + + + + legendre + histogram + tabular + + + + + + + + + + + + + + + + + + + + true + false + + + + + true + false + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + diff --git a/src/relaxng/settings.rnc b/src/relaxng/settings.rnc index c4fc79ad2..46950c63f 100644 --- a/src/relaxng/settings.rnc +++ b/src/relaxng/settings.rnc @@ -36,6 +36,8 @@ element settings { element energy_grid { ( "nuclide" | "log" | "logarithm" | "logarithmic" | "material-union" | "union" ) }? & + element energy_mode { ( "continuous-energy" | "ce" | "CE" | "multi-group" | "mg" | "MG" ) }? & + element entropy { (element dimension { list { xsd:int+ } } | attribute dimension { list { xsd:int+ } })? & @@ -47,6 +49,8 @@ element settings { element log_grid_bins { xsd:positiveInteger }? & + element max_order { xsd:nonNegativeInteger }? & + element natural_elements { xsd:string { maxLength = "20" } }? & element no_reduce { xsd:boolean }? & diff --git a/src/relaxng/settings.rng b/src/relaxng/settings.rng index 15c37cc6e..0b50f7969 100644 --- a/src/relaxng/settings.rng +++ b/src/relaxng/settings.rng @@ -140,6 +140,18 @@ + + + + continuous-energy + ce + CE + multi-group + mg + MG + + + @@ -201,6 +213,11 @@ + + + + + diff --git a/src/sab_header.F90 b/src/sab_header.F90 new file mode 100644 index 000000000..695f735c0 --- /dev/null +++ b/src/sab_header.F90 @@ -0,0 +1,150 @@ +module sab_header + + use, intrinsic :: ISO_FORTRAN_ENV + + use constants + use string, only: to_str + + implicit none + +!=============================================================================== +! DISTENERGYSAB contains the secondary energy/angle distributions for inelastic +! thermal scattering collisions which utilize a continuous secondary energy +! representation. +!=============================================================================== + + type DistEnergySab + integer :: n_e_out + real(8), allocatable :: e_out(:) + real(8), allocatable :: e_out_pdf(:) + real(8), allocatable :: e_out_cdf(:) + real(8), allocatable :: mu(:,:) + end type DistEnergySab + +!=============================================================================== +! SALPHABETA contains S(a,b) data for thermal neutron scattering, typically off +! of light isotopes such as water, graphite, Be, etc +!=============================================================================== + + type SAlphaBeta + character(10) :: name ! name of table, e.g. lwtr.10t + real(8) :: awr ! weight of nucleus in neutron masses + real(8) :: kT ! temperature in MeV (k*T) + integer :: n_zaid ! Number of valid zaids + integer, allocatable :: zaid(:) ! List of valid Z and A identifiers, e.g. 6012 + + ! threshold for S(a,b) treatment (usually ~4 eV) + real(8) :: threshold_inelastic + real(8) :: threshold_elastic = ZERO + + ! Inelastic scattering data + integer :: n_inelastic_e_in ! # of incoming E for inelastic + integer :: n_inelastic_e_out ! # of outgoing E for inelastic + integer :: n_inelastic_mu ! # of outgoing angles for inelastic + integer :: secondary_mode ! secondary mode (equal/skewed/continuous) + real(8), allocatable :: inelastic_e_in(:) + real(8), allocatable :: inelastic_sigma(:) + ! The following are used only if secondary_mode is 0 or 1 + real(8), allocatable :: inelastic_e_out(:,:) + real(8), allocatable :: inelastic_mu(:,:,:) + ! The following is used only if secondary_mode is 3 + ! The different implementation is necessary because the continuous + ! representation has a variable number of outgoing energy points for each + ! incoming energy + type(DistEnergySab), allocatable :: inelastic_data(:) ! One for each Ein + + ! Elastic scattering data + integer :: elastic_mode ! elastic mode (discrete/exact) + integer :: n_elastic_e_in ! # of incoming E for elastic + integer :: n_elastic_mu ! # of outgoing angles for elastic + real(8), allocatable :: elastic_e_in(:) + real(8), allocatable :: elastic_P(:) + real(8), allocatable :: elastic_mu(:,:) + contains + procedure :: print => print_sab_table + end type SAlphaBeta + + contains + +!=============================================================================== +! PRINT_SAB_TABLE displays information about a S(a,b) table containing data +! describing thermal scattering from bound materials such as hydrogen in water. +!=============================================================================== + + subroutine print_sab_table(this, unit) + class(SAlphaBeta), intent(in) :: this + integer, intent(in), optional :: unit + + integer :: size_sab ! memory used by S(a,b) table + integer :: unit_ ! unit to write to + integer :: i ! Loop counter for parsing through this % zaid + integer :: char_count ! Counter for the number of characters on a line + + ! set default unit for writing information + if (present(unit)) then + unit_ = unit + else + unit_ = OUTPUT_UNIT + end if + + ! Basic S(a,b) table information + write(unit_,*) 'S(a,b) Table ' // trim(this % name) + write(unit_,'(A)',advance="no") ' zaids = ' + ! Initialize the counter based on the above string + char_count = 11 + do i = 1, this % n_zaid + ! Deal with a line thats too long + if (char_count >= 73) then ! 73 = 80 - (5 ZAID chars + 1 space + 1 comma) + ! End the line + write(unit_,*) "" + ! Add 11 leading blanks + write(unit_,'(A)', advance="no") " " + ! reset the counter to 11 + char_count = 11 + end if + if (i < this % n_zaid) then + ! Include a comma + write(unit_,'(A)',advance="no") trim(to_str(this % zaid(i))) // ", " + char_count = char_count + len(trim(to_str(this % zaid(i)))) + 2 + else + ! Don't include a comma, since we are all done + write(unit_,'(A)',advance="no") trim(to_str(this % zaid(i))) + end if + + end do + write(unit_,*) "" ! Move to next line + write(unit_,*) ' awr = ' // trim(to_str(this % awr)) + write(unit_,*) ' kT = ' // trim(to_str(this % kT)) + + ! Inelastic data + write(unit_,*) ' # of Incoming Energies (Inelastic) = ' // & + trim(to_str(this % n_inelastic_e_in)) + write(unit_,*) ' # of Outgoing Energies (Inelastic) = ' // & + trim(to_str(this % n_inelastic_e_out)) + write(unit_,*) ' # of Outgoing Angles (Inelastic) = ' // & + trim(to_str(this % n_inelastic_mu)) + write(unit_,*) ' Threshold for Inelastic = ' // & + trim(to_str(this % threshold_inelastic)) + + ! Elastic data + if (this % n_elastic_e_in > 0) then + write(unit_,*) ' # of Incoming Energies (Elastic) = ' // & + trim(to_str(this % n_elastic_e_in)) + write(unit_,*) ' # of Outgoing Angles (Elastic) = ' // & + trim(to_str(this % n_elastic_mu)) + write(unit_,*) ' Threshold for Elastic = ' // & + trim(to_str(this % threshold_elastic)) + end if + + ! Determine memory used by S(a,b) table and write out + size_sab = 8 * (this % n_inelastic_e_in * (2 + this % n_inelastic_e_out * & + (1 + this % n_inelastic_mu)) + this % n_elastic_e_in * & + (2 + this % n_elastic_mu)) + write(unit_,*) ' Memory Used = ' // trim(to_str(size_sab)) // ' bytes' + + ! Blank line at end + write(unit_,*) + + end subroutine print_sab_table + +end module sab_header diff --git a/src/scattdata_header.F90 b/src/scattdata_header.F90 new file mode 100644 index 000000000..f8fddbc6b --- /dev/null +++ b/src/scattdata_header.F90 @@ -0,0 +1,489 @@ +module scattdata_header + + use constants + use error, only: fatal_error + use math + use random_lcg, only: prn + use search, only: binary_search + + implicit none + +!=============================================================================== +! SCATTDATA contains all the data to describe the scattering energy and +! angular distribution +!=============================================================================== + + type, abstract :: ScattData + ! p0 matrix on its own for sampling energy + real(8), allocatable :: energy(:,:) ! (Gout x Gin) + real(8), allocatable :: mult(:,:) ! (Gout x Gin) + real(8), allocatable :: data(:,:,:) ! (Order/Nmu x Gout x Gin) + + contains + procedure(scattdata_init_), deferred :: init ! Initializes ScattData + procedure(scattdata_calc_f_), deferred :: calc_f ! Calculates f, given mu + procedure(scattdata_sample_), deferred :: sample ! sample the scatter event + end type ScattData + + abstract interface + subroutine scattdata_init_(this, order, energy, mult, coeffs) + import ScattData + class(ScattData), intent(inout) :: this ! Object to work on + integer, intent(in) :: order ! Data Order + real(8), intent(in) :: energy(:,:) ! Energy Transfer Matrix + real(8), intent(in) :: mult(:,:) ! Scatter Prod'n Matrix + real(8), intent(in) :: coeffs(:,:,:) ! Coefficients to use + end subroutine scattdata_init_ + + pure function scattdata_calc_f_(this, gin, gout, mu) result(f) + import ScattData + class(ScattData), intent(in) :: this ! The ScattData to evaluate + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8) :: f ! Return value of f(mu) + + end function scattdata_calc_f_ + + subroutine scattdata_sample_(this, gin, gout, mu, wgt) + import ScattData + class(ScattData), intent(in) :: this ! Scattering Object to Use + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + end subroutine scattdata_sample_ + end interface + + type, extends(ScattData) :: ScattDataLegendre + ! Maximal value for rejection sampling from rectangle + real(8), allocatable :: max_val(:,:) + contains + procedure :: init => scattdatalegendre_init + procedure :: calc_f => scattdatalegendre_calc_f + procedure :: sample => scattdatalegendre_sample + end type ScattDataLegendre + + type, extends(ScattData) :: ScattDataHistogram + real(8), allocatable :: mu(:) ! Mu bins + real(8) :: dmu ! Mu spacing + contains + procedure :: init => scattdatahistogram_init + procedure :: calc_f => scattdatahistogram_calc_f + procedure :: sample => scattdatahistogram_sample + end type ScattDataHistogram + + type, extends(ScattData) :: ScattDataTabular + real(8), allocatable :: mu(:) ! Mu bins + real(8) :: dmu ! Mu spacing + real(8), allocatable :: fmu(:,:,:) ! PDF of f(mu) + contains + procedure :: init => scattdatatabular_init + procedure :: calc_f => scattdatatabular_calc_f + procedure :: sample => scattdatatabular_sample + end type ScattDataTabular + +!=============================================================================== +! SCATTDATACONTAINER allocatable array for storing ScattData Objects (for angle) +!=============================================================================== + + type ScattDataContainer + class(ScattData), allocatable :: obj + end type ScattDataContainer + +contains + +!=============================================================================== +! SCATTDATA_INIT builds the scattdata object +!=============================================================================== + + subroutine scattdata_init(this, order, energy, mult) + class(ScattData), intent(inout) :: this ! Object to work on + integer, intent(in) :: order ! Data Order + real(8), intent(in) :: energy(:,:) ! Energy Transfer Matrix + real(8), intent(in) :: mult(:,:) ! Scatter Prod'n Matrix + + integer :: groups + + groups = size(energy, dim=1) + + allocate(this % energy(groups, groups)) + this % energy = energy + allocate(this % mult(groups, groups)) + this % mult = mult + allocate(this % data(order, groups, groups)) + this % data = ZERO + + end subroutine scattdata_init + + subroutine scattdatalegendre_init(this, order, energy, mult, coeffs) + class(ScattDataLegendre), intent(inout) :: this ! Object to work on + integer, intent(in) :: order ! Data Order + real(8), intent(in) :: energy(:,:) ! Energy Transfer Matrix + real(8), intent(in) :: mult(:,:) ! Scatter Prod'n Matrix + real(8), intent(in) :: coeffs(:,:,:) ! Coefficients to use + + real(8) :: dmu, mu, f + integer :: imu, Nmu, gout, gin, groups + + call scattdata_init(this, order, energy, mult) + + this % data = coeffs + + groups = size(this % energy,dim=1) + + allocate(this % max_val(groups, groups)) + this % max_val = ZERO + ! Step through the polynomial with fixed number of points to identify + ! the maximal value. + Nmu = 1001 + dmu = TWO / real(Nmu,8) + do imu = 1, Nmu + ! Update mu. Do first and last seperate to avoid float errors + if (imu == 1) then + mu = -ONE + else if (imu == Nmu) then + mu = ONE + end if + mu = -ONE + real(imu - 1,8) * dmu + do gin = 1, groups + do gout = 1, groups + ! Calculate probability + f = this % calc_f(gin,gout,mu) + ! If this is a new max, store it. + if (f > this % max_val(gout,gin)) this % max_val(gout,gin) = f + end do + end do + end do + + ! Finally, since we may not have caught the exact max, add 10% margin + this % max_val = this % max_val * 1.1_8 + + end subroutine scattdatalegendre_init + + subroutine scattdatahistogram_init(this, order, energy, mult, coeffs) + class(ScattDataHistogram), intent(inout) :: this ! Object to work on + integer, intent(in) :: order ! Data Order + real(8), intent(in) :: energy(:,:) ! Energy Transfer Matrix + real(8), intent(in) :: mult(:,:) ! Scatter Prod'n Matrix + real(8), intent(in) :: coeffs(:,:,:) ! Coefficients to use + + integer :: imu, gin, gout, groups + real(8) :: norm + + groups = size(energy,dim=1) + + call scattdata_init(this, order, energy, mult) + + allocate(this % mu(order)) + this % dmu = TWO / real(order,8) + this % mu(1) = -ONE + do imu = 2, order + this % mu(imu) = -ONE + real(imu - 1,8) * this % dmu + end do + + ! Best to integrate this histogram so we can avoid rejection sampling + do gin = 1, groups + do gout = 1, groups + if (energy(gout,gin) > ZERO) then + ! Integrate the histogram + this % data(1,gout,gin) = this % dmu * coeffs(1,gout,gin) + do imu = 2, order + this % data(imu,gout,gin) = this % dmu * coeffs(imu,gout,gin) + & + this % data(imu-1,gout,gin) + end do + ! Now make sure integral norms to zero + norm = this % data(order,gout,gin) + if (norm > ZERO) then + this % data(:,gout,gin) = this % data(:,gout,gin) / norm + end if + end if + end do + end do + + end subroutine scattdatahistogram_init + + subroutine scattdatatabular_init(this, order, energy, mult, coeffs) + class(ScattDataTabular), intent(inout) :: this ! Object to work on + integer, intent(in) :: order ! Data Order + real(8), intent(in) :: energy(:,:) ! Energy Transfer Matrix + real(8), intent(in) :: mult(:,:) ! Scatter Prod'n Matrix + real(8), intent(in) :: coeffs(:,:,:) ! Coefficients to use + + integer :: imu, gin, gout, groups + real(8) :: norm + logical :: legendre_flag + integer :: this_order + + if (order < 0) then + legendre_flag = .true. + this_order = -1 * order + else + legendre_flag = .false. + this_order = order + end if + + groups = size(energy,dim=1) + + call scattdata_init(this, this_order, energy, mult) + + allocate(this % mu(this_order)) + this % dmu = TWO / real(this_order - 1) + do imu = 1, this_order - 1 + this % mu(imu) = -ONE + real(imu - 1) * this % dmu + end do + this % mu(this_order) = ONE + + ! Best to integrate this histogram so we can avoid rejection sampling + allocate(this % fmu(this_order,groups,groups)) + do gin = 1, groups + do gout = 1, groups + if (energy(gout,gin) > ZERO) then + if (legendre_flag) then + ! Coeffs are legendre coeffs. Need to build f(mu) then integrate + ! and store the integral in this % data + ! Ensure the coeffs are normalized + norm = ONE / coeffs(1,gout,gin) + do imu = 1, this_order + this % fmu(imu,gout,gin) = evaluate_legendre(norm * coeffs(:,gout,gin), this % mu(imu)) + ! Force positivity + if (this % fmu(imu,gout,gin) < ZERO) then + this % fmu(imu,gout,gin) = ZERO + end if + end do + else + ! Coeffs contain f(mu), put in f(mu) to save duplicate. + this % fmu(:,gout,gin) = this % data(:,gout,gin) + end if + + ! Re-normalize fmu for numerical integration issues and in case + ! the negative fix-up introduced un-normalized data + norm = ZERO + do imu = 2, this_order + norm = norm + HALF * this % dmu * (this % fmu(imu-1,gout,gin) + this % fmu(imu,gout,gin)) + end do + if (norm > ZERO) then + this % fmu(:,gout,gin) = this % fmu(:,gout,gin) / norm + end if + + ! Now create CDF from fmu with trapezoidal rule + this % data(1,gout,gin) = ZERO + do imu = 2, this_order - 1 + this % data(imu,gout,gin) = this % data(imu-1,gout,gin) + & + HALF * this % dmu * (this % fmu(imu-1,gout,gin) + this % fmu(imu,gout,gin)) + end do + this % data(this_order,gout,gin) = ONE + end if + end do + end do + + end subroutine scattdatatabular_init + +!=============================================================================== +! SCATTDATA_*_CALC_F Calculates the value of f given mu (and gin,gout pair) +!=============================================================================== + + pure function scattdatalegendre_calc_f(this, gin, gout, mu) result(f) + class(ScattDataLegendre), intent(in) :: this ! The ScattData to evaluate + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8) :: f ! Return value of f(mu) + + ! Plug mu in to the legendre expansion and go from there + f = evaluate_legendre(this % data(:, gout, gin), mu) + + end function scattdatalegendre_calc_f + + pure function scattdatahistogram_calc_f(this, gin, gout, mu) result(f) + class(ScattDataHistogram), intent(in) :: this ! The ScattData to evaluate + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8) :: f ! Return value of f(mu) + + integer :: imu + + ! Find mu bin + imu = floor((mu + ONE)/ this % dmu + ONE) + ! Adjust so interpolation works on the last bin if necessary + if (imu == size(this % data, dim=1)) then + imu = imu - 1 + end if + + ! Use histogram interpolation to find f(mu) + f = this % data(imu, gout, gin) + + end function scattdatahistogram_calc_f + + pure function scattdatatabular_calc_f(this, gin, gout, mu) result(f) + class(ScattDataTabular), intent(in) :: this ! The ScattData to evaluate + integer, intent(in) :: gin ! Incoming Energy Group + integer, intent(in) :: gout ! Outgoing Energy Group + real(8), intent(in) :: mu ! Angle of interest + real(8) :: f ! Return value of f(mu) + + integer :: imu + real(8) :: r + + ! Find mu bin + imu = floor((mu + ONE)/ this % dmu + ONE) + ! Adjust so interpolation works on the last bin if necessary + if (imu == size(this % data, dim=1)) then + imu = imu - 1 + end if + + ! ! Now interpolate to find f(mu) + r = (mu - this % mu(imu)) / (this % mu(imu + 1) - this % mu(imu)) + f = (ONE - r) * this % data(imu, gout, gin) + & + r * this % data(imu + 1, gout, gin) + + end function scattdatatabular_calc_f + +!=============================================================================== +! SCATTDATA*_SCATTER Samples the outgoing energy and change in angle. +!=============================================================================== + + subroutine scattdatalegendre_sample(this, gin, gout, mu, wgt) + class(ScattDataLegendre), intent(in) :: this ! Scattering object to use + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + + real(8) :: xi ! Our random number + real(8) :: prob ! Running probability + real(8) :: u, f, M + integer :: samples + + xi = prn() + prob = ZERO + gout = 0 + + do while (prob < xi) + gout = gout + 1 + prob = prob + this % energy(gout,gin) + end do + + ! Now we can sample mu using the legendre representation of the thisering + ! kernel in data(1:this % order) + + ! Do with rejection sampling + ! Set maximal value + M = this % max_val(gout,gin) + samples = 0 + do + mu = TWO * prn() - ONE + f = this % calc_f(gin,gout,mu) + if (f > ZERO) then + u = prn() * M + if (u <= f) then + exit + end if + end if + samples = samples + 1 + if (samples > MAX_SAMPLE) then + call fatal_error("Maximum number of Legendre expansion samples reached!") + end if + end do + + wgt = wgt * this % mult(gout,gin) + + end subroutine scattdatalegendre_sample + + subroutine scattdatahistogram_sample(this, gin, gout, mu, wgt) + class(ScattDataHistogram), intent(in) :: this ! Scattering object to use + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + + real(8) :: xi ! Our random number + real(8) :: prob ! Running probability + integer :: imu + + xi = prn() + prob = ZERO + gout = 0 + + do while (prob < xi) + gout = gout + 1 + prob = prob + this % energy(gout,gin) + end do + + xi = prn() + if (xi < this % data(1,gout,gin)) then + imu = 1 + else + imu = binary_search(this % data(:,gout,gin), & + size(this % data(:,gout,gin)), xi) + end if + + ! Randomly select a mu in this bin. + mu = prn() * this % dmu + this % mu(imu) + + wgt = wgt * this % mult(gout,gin) + + end subroutine scattdatahistogram_sample + + subroutine scattdatatabular_sample(this, gin, gout, mu, wgt) + class(ScattDataTabular), intent(in) :: this ! Scattering object to use + integer, intent(in) :: gin ! Incoming neutron group + integer, intent(out) :: gout ! Sampled outgoin group + real(8), intent(out) :: mu ! Sampled change in angle + real(8), intent(inout) :: wgt ! Particle weight + + real(8) :: xi ! Our random number + real(8) :: prob ! Running probability + real(8) :: mu0, frac, mu1 + real(8) :: c_k, c_k1, p0, p1 + integer :: k, NP + + xi = prn() + prob = ZERO + gout = 0 + + do while (prob < xi) + gout = gout + 1 + prob = prob + this % energy(gout,gin) + end do + + ! determine outgoing cosine bin + NP = size(this % data(:,gout,gin)) + xi = prn() + + c_k = this % data(1,gout,gin) + do k = 1, NP - 1 + c_k1 = this % data(k+1,gout,gin) + if (xi < c_k1) exit + c_k = c_k1 + end do + + ! check to make sure k is <= NP - 1 + k = min(k, NP - 1) + + p0 = this % fmu(k,gout,gin) + mu0 = this % mu(k) + ! Linear-linear interpolation to find mu value w/in bin. + p1 = this % fmu(k+1,gout,gin) + mu1 = this % mu(k+1) + + frac = (p1 - p0)/(mu1 - mu0) + + if (frac == ZERO) then + mu = mu0 + (xi - c_k)/p0 + else + mu = mu0 + (sqrt(max(ZERO, p0*p0 + TWO*frac*(xi - c_k))) - p0)/frac + end if + + if (mu <= -ONE) then + mu = -ONE + else if (mu >= ONE) then + mu = ONE + end if + + wgt = wgt * this % mult(gout,gin) + + end subroutine scattdatatabular_sample + +end module scattdata_header diff --git a/src/secondary_correlated.F90 b/src/secondary_correlated.F90 index c0289d55e..b556d02dc 100644 --- a/src/secondary_correlated.F90 +++ b/src/secondary_correlated.F90 @@ -1,8 +1,8 @@ module secondary_correlated + use angleenergy_header, only: AngleEnergy use constants, only: ZERO, ONE, TWO, HISTOGRAM, LINEAR_LINEAR use distribution_univariate, only: DistributionContainer - use secondary_header, only: AngleEnergy use random_lcg, only: prn use search, only: binary_search @@ -24,8 +24,8 @@ module secondary_correlated integer :: n_region ! number of interpolation regions integer, allocatable :: breakpoints(:) ! breakpoints of interpolation regions integer, allocatable :: interpolation(:) ! interpolation region codes - real(8), allocatable :: energy_in(:) ! incoming energies - type(AngleEnergyTable), allocatable :: table(:) ! outgoing E/mu distributions + real(8), allocatable :: energy(:) ! incoming energies + type(AngleEnergyTable), allocatable :: distribution(:) ! outgoing E/mu distributions contains procedure :: sample => correlated_sample end type CorrelatedAngleEnergy @@ -61,17 +61,17 @@ contains ! find energy bin and calculate interpolation factor -- if the energy is ! outside the range of the tabulated energies, choose the first or last bins - n_energy_in = size(this%energy_in) - if (E_in < this%energy_in(1)) then + n_energy_in = size(this%energy) + if (E_in < this%energy(1)) then i = 1 r = ZERO - elseif (E_in > this%energy_in(n_energy_in)) then + elseif (E_in > this%energy(n_energy_in)) then i = n_energy_in - 1 r = ONE else - i = binary_search(this%energy_in, n_energy_in, E_in) - r = (E_in - this%energy_in(i)) / & - (this%energy_in(i+1) - this%energy_in(i)) + i = binary_search(this%energy, n_energy_in, E_in) + r = (E_in - this%energy(i)) / & + (this%energy(i+1) - this%energy(i)) end if ! Sample between the ith and (i+1)th bin @@ -82,23 +82,23 @@ contains end if ! interpolation for energy E1 and EK - n_energy_out = size(this%table(i)%e_out) - E_i_1 = this%table(i)%e_out(1) - E_i_K = this%table(i)%e_out(n_energy_out) + n_energy_out = size(this%distribution(i)%e_out) + E_i_1 = this%distribution(i)%e_out(1) + E_i_K = this%distribution(i)%e_out(n_energy_out) - n_energy_out = size(this%table(i+1)%e_out) - E_i1_1 = this%table(i+1)%e_out(1) - E_i1_K = this%table(i+1)%e_out(n_energy_out) + n_energy_out = size(this%distribution(i+1)%e_out) + E_i1_1 = this%distribution(i+1)%e_out(1) + E_i1_K = this%distribution(i+1)%e_out(n_energy_out) E_1 = E_i_1 + r*(E_i1_1 - E_i_1) E_K = E_i_K + r*(E_i1_K - E_i_K) ! determine outgoing energy bin - n_energy_out = size(this%table(l)%e_out) + n_energy_out = size(this%distribution(l)%e_out) r1 = prn() - c_k = this%table(l)%c(1) + c_k = this%distribution(l)%c(1) do k = 1, n_energy_out - 1 - c_k1 = this%table(l)%c(k+1) + c_k1 = this%distribution(l)%c(k+1) if (r1 < c_k1) exit c_k = c_k1 end do @@ -106,9 +106,9 @@ contains ! check to make sure k is <= NP - 1 k = min(k, n_energy_out - 1) - E_l_k = this%table(l)%e_out(k) - p_l_k = this%table(l)%p(k) - if (this%table(l)%interpolation == HISTOGRAM) then + E_l_k = this%distribution(l)%e_out(k) + p_l_k = this%distribution(l)%p(k) + if (this%distribution(l)%interpolation == HISTOGRAM) then ! Histogram interpolation if (p_l_k > ZERO) then E_out = E_l_k + (r1 - c_k)/p_l_k @@ -116,10 +116,10 @@ contains E_out = E_l_k end if - elseif (this%table(l)%interpolation == LINEAR_LINEAR) then + elseif (this%distribution(l)%interpolation == LINEAR_LINEAR) then ! Linear-linear interpolation - E_l_k1 = this%table(l)%e_out(k+1) - p_l_k1 = this%table(l)%p(k+1) + E_l_k1 = this%distribution(l)%e_out(k+1) + p_l_k1 = this%distribution(l)%p(k+1) frac = (p_l_k1 - p_l_k)/(E_l_k1 - E_l_k) if (frac == ZERO) then @@ -139,9 +139,9 @@ contains ! Find correlated angular distribution for closest outgoing energy bin if (r1 - c_k < c_k1 - r1) then - mu = this%table(l)%angle(k)%obj%sample() + mu = this%distribution(l)%angle(k)%obj%sample() else - mu = this%table(l)%angle(k + 1)%obj%sample() + mu = this%distribution(l)%angle(k + 1)%obj%sample() end if end subroutine correlated_sample diff --git a/src/secondary_header.F90 b/src/secondary_header.F90 deleted file mode 100644 index d85807412..000000000 --- a/src/secondary_header.F90 +++ /dev/null @@ -1,78 +0,0 @@ -module secondary_header - - use endf_header, only: Tab1 - use interpolation, only: interpolate_tab1 - use random_lcg, only: prn - -!=============================================================================== -! ANGLEENERGY (abstract) defines a correlated or uncorrelated angle-energy -! distribution that is a function of incoming energy. Each derived type must -! implement a sample() subroutine that returns an outgoing energy and scattering -! cosine given an incoming energy. -!=============================================================================== - - type, abstract :: AngleEnergy - contains - procedure(iSampleAngleEnergy), deferred :: sample - end type AngleEnergy - - abstract interface - subroutine iSampleAngleEnergy(this, E_in, E_out, mu) - import AngleEnergy - class(AngleEnergy), intent(in) :: this - real(8), intent(in) :: E_in - real(8), intent(out) :: E_out - real(8), intent(out) :: mu - end subroutine iSampleAngleEnergy - end interface - - type :: AngleEnergyContainer - class(AngleEnergy), allocatable :: obj - end type AngleEnergyContainer - -!=============================================================================== -! SECONDARYDISTRIBUTION stores multiple angle-energy distributions, each of -! which has a given probability of occurring for a given incoming energy. In -! general, most secondary distributions only have one angle-energy distribution, -! but for some cases (e.g., (n,2n) in certain nuclides) multiple distinct -! distributions exist. -!=============================================================================== - - type :: SecondaryDistribution - type(Tab1), allocatable :: applicability(:) - type(AngleEnergyContainer), allocatable :: distribution(:) - contains - procedure :: sample => secondary_sample - end type SecondaryDistribution - -contains - - subroutine secondary_sample(this, E_in, E_out, mu) - class(SecondaryDistribution), intent(in) :: this - real(8), intent(in) :: E_in ! incoming energy - real(8), intent(out) :: E_out ! sampled outgoing energy - real(8), intent(out) :: mu ! sampled scattering cosine - - integer :: n ! number of angle-energy distributions - real(8) :: p_valid ! probability that given distribution is valid - - n = size(this%applicability) - if (n > 1) then - do i = 1, n - ! Determine probability that i-th energy distribution is sampled - p_valid = interpolate_tab1(this%applicability(i), E_in) - - ! If i-th distribution is sampled, sample energy from the distribution - if (prn() <= p_valid) then - call this%distribution(i)%obj%sample(E_in, E_out, mu) - exit - end if - end do - else - ! If only one distribution is present, go ahead and sample it - call this%distribution(1)%obj%sample(E_in, E_out, mu) - end if - - end subroutine secondary_sample - -end module secondary_header diff --git a/src/secondary_kalbach.F90 b/src/secondary_kalbach.F90 index 5e6949206..668917d62 100644 --- a/src/secondary_kalbach.F90 +++ b/src/secondary_kalbach.F90 @@ -1,7 +1,7 @@ module secondary_kalbach + use angleenergy_header, only: AngleEnergy use constants, only: ZERO, ONE, TWO, HISTOGRAM, LINEAR_LINEAR - use secondary_header, only: AngleEnergy use random_lcg, only: prn use search, only: binary_search @@ -25,8 +25,8 @@ module secondary_kalbach integer :: n_region ! number of interpolation regions integer, allocatable :: breakpoints(:) ! breakpoints of interpolation regions integer, allocatable :: interpolation(:) ! interpolation region codes - real(8), allocatable :: energy_in(:) ! incoming energies - type(KalbachMannTable), allocatable :: table(:) ! outgoing E/mu parameters + real(8), allocatable :: energy(:) ! incoming energies + type(KalbachMannTable), allocatable :: distribution(:) ! outgoing E/mu parameters contains procedure :: sample => kalbachmann_sample end type KalbachMann @@ -64,17 +64,17 @@ contains ! find energy bin and calculate interpolation factor -- if the energy is ! outside the range of the tabulated energies, choose the first or last bins - n_energy_in = size(this%energy_in) - if (E_in < this%energy_in(1)) then + n_energy_in = size(this%energy) + if (E_in < this%energy(1)) then i = 1 r = ZERO - elseif (E_in > this%energy_in(n_energy_in)) then + elseif (E_in > this%energy(n_energy_in)) then i = n_energy_in - 1 r = ONE else - i = binary_search(this%energy_in, n_energy_in, E_in) - r = (E_in - this%energy_in(i)) / & - (this%energy_in(i+1) - this%energy_in(i)) + i = binary_search(this%energy, n_energy_in, E_in) + r = (E_in - this%energy(i)) / & + (this%energy(i+1) - this%energy(i)) end if ! Sample between the ith and (i+1)th bin @@ -85,23 +85,23 @@ contains end if ! interpolation for energy E1 and EK - n_energy_out = size(this%table(i)%e_out) - E_i_1 = this%table(i)%e_out(1) - E_i_K = this%table(i)%e_out(n_energy_out) + n_energy_out = size(this%distribution(i)%e_out) + E_i_1 = this%distribution(i)%e_out(1) + E_i_K = this%distribution(i)%e_out(n_energy_out) - n_energy_out = size(this%table(i+1)%e_out) - E_i1_1 = this%table(i+1)%e_out(1) - E_i1_K = this%table(i+1)%e_out(n_energy_out) + n_energy_out = size(this%distribution(i+1)%e_out) + E_i1_1 = this%distribution(i+1)%e_out(1) + E_i1_K = this%distribution(i+1)%e_out(n_energy_out) E_1 = E_i_1 + r*(E_i1_1 - E_i_1) E_K = E_i_K + r*(E_i1_K - E_i_K) ! determine outgoing energy bin - n_energy_out = size(this%table(l)%e_out) + n_energy_out = size(this%distribution(l)%e_out) r1 = prn() - c_k = this%table(l)%c(1) + c_k = this%distribution(l)%c(1) do k = 1, n_energy_out - 1 - c_k1 = this%table(l)%c(k+1) + c_k1 = this%distribution(l)%c(k+1) if (r1 < c_k1) exit c_k = c_k1 end do @@ -109,9 +109,9 @@ contains ! check to make sure k is <= NP - 1 k = min(k, n_energy_out - 1) - E_l_k = this%table(l)%e_out(k) - p_l_k = this%table(l)%p(k) - if (this%table(l)%interpolation == HISTOGRAM) then + E_l_k = this%distribution(l)%e_out(k) + p_l_k = this%distribution(l)%p(k) + if (this%distribution(l)%interpolation == HISTOGRAM) then ! Histogram interpolation if (p_l_k > ZERO) then E_out = E_l_k + (r1 - c_k)/p_l_k @@ -120,13 +120,13 @@ contains end if ! Determine Kalbach-Mann parameters - km_r = this%table(l)%r(k) - km_a = this%table(l)%a(k) + km_r = this%distribution(l)%r(k) + km_a = this%distribution(l)%a(k) - elseif (this%table(l)%interpolation == LINEAR_LINEAR) then + elseif (this%distribution(l)%interpolation == LINEAR_LINEAR) then ! Linear-linear interpolation - E_l_k1 = this%table(l)%e_out(k+1) - p_l_k1 = this%table(l)%p(k+1) + E_l_k1 = this%distribution(l)%e_out(k+1) + p_l_k1 = this%distribution(l)%p(k+1) frac = (p_l_k1 - p_l_k)/(E_l_k1 - E_l_k) if (frac == ZERO) then @@ -137,10 +137,10 @@ contains end if ! Determine Kalbach-Mann parameters - km_r = this%table(l)%r(k) + (E_out - E_l_k)/(E_l_k1 - E_l_k) * & - (this%table(l)%r(k+1) - this%table(l)%r(k)) - km_a = this%table(l)%a(k) + (E_out - E_l_k)/(E_l_k1 - E_l_k) * & - (this%table(l)%a(k+1) - this%table(l)%a(k)) + km_r = this%distribution(l)%r(k) + (E_out - E_l_k)/(E_l_k1 - E_l_k) * & + (this%distribution(l)%r(k+1) - this%distribution(l)%r(k)) + km_a = this%distribution(l)%a(k) + (E_out - E_l_k)/(E_l_k1 - E_l_k) * & + (this%distribution(l)%a(k+1) - this%distribution(l)%a(k)) end if ! Now interpolate between incident energy bins i and i + 1 diff --git a/src/secondary_nbody.F90 b/src/secondary_nbody.F90 new file mode 100644 index 000000000..71cae6fa2 --- /dev/null +++ b/src/secondary_nbody.F90 @@ -0,0 +1,70 @@ +module secondary_nbody + + use angleenergy_header, only: AngleEnergy + use constants, only: ONE, TWO, PI + use math, only: maxwell_spectrum + use random_lcg, only: prn + +!=============================================================================== +! NBODYPHASESPACE gives the energy distribution for particles emitted from +! neutron and charged-particle reactions. This corresponds to ACE law 66 and +! ENDF File 6, LAW=6. +!=============================================================================== + + type, extends(AngleEnergy) :: NBodyPhaseSpace + integer :: n_bodies + real(8) :: mass_ratio + real(8) :: A + real(8) :: Q + contains + procedure :: sample => nbody_sample + end type NBodyPhaseSpace + +contains + + subroutine nbody_sample(this, E_in, E_out, mu) + class(NBodyPhaseSpace), intent(in) :: this + real(8), intent(in) :: E_in ! incoming energy + real(8), intent(out) :: E_out ! sampled outgoing energy + real(8), intent(out) :: mu ! sampled outgoing energy + + real(8) :: Ap ! total mass of particles in neutron masses + real(8) :: E_max ! maximum possible COM energy + real(8) :: x, y, v + real(8) :: r1, r2, r3, r4, r5, r6 + + ! By definition, the distribution of the angle is isotropic for an N-body + ! phase space distribution + mu = TWO*prn() - ONE + + ! Determine E_max parameter + Ap = this%mass_ratio + E_max = (Ap - ONE)/Ap * (this%A/(this%A + ONE)*E_in + this%Q) + + ! x is essentially a Maxwellian distribution + x = maxwell_spectrum(ONE) + + select case (this%n_bodies) + case (3) + y = maxwell_spectrum(ONE) + case (4) + r1 = prn() + r2 = prn() + r3 = prn() + y = -log(r1*r2*r3) + case (5) + r1 = prn() + r2 = prn() + r3 = prn() + r4 = prn() + r5 = prn() + r6 = prn() + y = -log(r1*r2*r3*r4) - log(r5) * cos(PI/TWO*r6)**2 + end select + + ! Now determine v and E_out + v = x/(x+y) + E_out = E_max * v + end subroutine nbody_sample + +end module secondary_nbody diff --git a/src/secondary_uncorrelated.F90 b/src/secondary_uncorrelated.F90 index 22a56aa12..7bc8fa13d 100644 --- a/src/secondary_uncorrelated.F90 +++ b/src/secondary_uncorrelated.F90 @@ -1,9 +1,9 @@ module secondary_uncorrelated use angle_distribution, only: AngleDistribution + use angleenergy_header, only: AngleEnergy use constants, only: ONE, TWO use energy_distribution, only: EnergyDistribution - use secondary_header, only: AngleEnergy use random_lcg, only: prn !=============================================================================== diff --git a/src/simulation.F90 b/src/simulation.F90 index 6e2d7957c..7741338de 100644 --- a/src/simulation.F90 +++ b/src/simulation.F90 @@ -4,26 +4,26 @@ module simulation use mpi #endif - use cmfd_execute, only: cmfd_init_batch, execute_cmfd - use constants, only: ZERO - use eigenvalue, only: count_source_for_ufs, calculate_average_keff, & - calculate_combined_keff, calculate_generation_keff, & - shannon_entropy, synchronize_bank, keff_generation + use cmfd_execute, only: cmfd_init_batch, execute_cmfd + use constants, only: ZERO + use eigenvalue, only: count_source_for_ufs, calculate_average_keff, & + calculate_combined_keff, calculate_generation_keff, & + shannon_entropy, synchronize_bank, keff_generation #ifdef _OPENMP - use eigenvalue, only: join_bank_from_threads + use eigenvalue, only: join_bank_from_threads #endif use global - use output, only: write_message, header, print_columns, & - print_batch_keff, print_generation + use output, only: write_message, header, print_columns, & + print_batch_keff, print_generation use particle_header, only: Particle - use random_lcg, only: set_particle_seed - use source, only: initialize_source - use state_point, only: write_state_point, write_source_point - use string, only: to_str - use tally, only: synchronize_tallies, setup_active_usertallies, & - reset_result - use trigger, only: check_triggers - use tracking, only: transport + use random_lcg, only: set_particle_seed + use source, only: initialize_source + use state_point, only: write_state_point, write_source_point + use string, only: to_str + use tally, only: synchronize_tallies, setup_active_usertallies, & + reset_result + use trigger, only: check_triggers + use tracking, only: transport implicit none private @@ -131,7 +131,8 @@ contains integer :: i ! set defaults - call p % initialize_from_source(source_bank(index_source)) + call p % initialize_from_source(source_bank(index_source), run_CE, & + energy_bin_avg) ! set identifier for particle p % id = work_index(rank) + index_source diff --git a/src/source.F90 b/src/source.F90 index d1bead380..ad565c95c 100644 --- a/src/source.F90 +++ b/src/source.F90 @@ -9,12 +9,13 @@ module source use geometry_header, only: BASE_UNIVERSE use global use hdf5_interface, only: file_create, file_open, file_close, read_dataset - use math, only: maxwell_spectrum, watt_spectrum use output, only: write_message use particle_header, only: Particle use random_lcg, only: prn, set_particle_seed, prn_set_stream - use state_point, only: read_source_bank, write_source_bank + use search, only: binary_search use string, only: to_str + use math + use state_point, only: read_source_bank, write_source_bank #ifdef MPI use message_passing @@ -109,7 +110,7 @@ contains integer, save :: num_resamples = 0 ! Number of resamples encountered ! Set weight to one by default - site%wgt = ONE + site % wgt = ONE ! Set the random number generator to the source stream. call prn_set_stream(STREAM_SOURCE) @@ -117,10 +118,10 @@ contains ! Sample from among multiple source distributions n_source = size(external_source) if (n_source > 1) then - r(1) = prn()*sum(external_source(:)%strength) + r(1) = prn()*sum(external_source(:) % strength) c = ZERO do i = 1, n_source - c = c + external_source(i)%strength + c = c + external_source(i) % strength if (r(1) < c) exit end do else @@ -131,14 +132,14 @@ contains found = .false. do while (.not.found) ! Set particle defaults - call p%initialize() + call p % initialize() ! Sample spatial distribution - site%xyz(:) = external_source(i)%space%sample() + site % xyz(:) = external_source(i) % space % sample() ! Fill p with needed data - p%coord(1)%xyz(:) = site%xyz - p%coord(1)%uvw(:) = [ ONE, ZERO, ZERO ] + p % coord(1) % xyz(:) = site % xyz + p % coord(1) % uvw(:) = [ ONE, ZERO, ZERO ] ! Now search to see if location exists in geometry call find_cell(p, found) @@ -151,27 +152,27 @@ contains end if ! Check if spatial site is in fissionable material - select type (space => external_source(i)%space) + select type (space => external_source(i) % space) type is (SpatialBox) - if (space%only_fissionable) then - if (p%material == MATERIAL_VOID) then + if (space % only_fissionable) then + if (p % material == MATERIAL_VOID) then found = .false. - elseif (.not. materials(p%material)%fissionable) then + elseif (.not. materials(p % material) % fissionable) then found = .false. end if end if end select end do - call p%clear() + call p % clear() ! Sample angle - site%uvw(:) = external_source(i)%angle%sample() + site % uvw(:) = external_source(i) % angle % sample() ! Check for monoenergetic source above maximum neutron energy - select type (energy => external_source(i)%energy) + select type (energy => external_source(i) % energy) type is (Discrete) - if (any(energy%x >= energy_max_neutron)) then + if (any(energy % x >= energy_max_neutron)) then call fatal_error("Source energy above range of energies of at least & &one cross section table") end if @@ -179,14 +180,26 @@ contains do ! Sample energy spectrum - site%E = external_source(i)%energy%sample() + site % E = external_source(i) % energy % sample() ! resample if energy is greater than maximum neutron energy - if (site%E < energy_max_neutron) exit + if (site % E < energy_max_neutron) exit end do ! Set delayed group - site%delayed_group = 0 + site % delayed_group = 0 + + ! If running in MG, convert site % E to group + if (.not. run_CE) then + if (site % E <= energy_bins(1)) then + site % E = real(1, 8) + else if (site % E > energy_bins(energy_groups + 1)) then + site % E = real(energy_groups, 8) + else + site % E = real(binary_search(energy_bins, energy_groups + 1, & + site % E), 8) + end if + end if ! Set the random number generator back to the tracking stream. call prn_set_stream(STREAM_TRACKING) diff --git a/src/state_point.F90 b/src/state_point.F90 index ee7873034..d4fb2c21d 100644 --- a/src/state_point.F90 +++ b/src/state_point.F90 @@ -18,7 +18,7 @@ module state_point use global use hdf5_interface use output, only: write_message, time_stamp - use string, only: to_str, zero_padded, count_digits + use string, only: to_str, count_digits, zero_padded use tally_header, only: TallyObject use mesh_header, only: RegularMesh use dict_header, only: ElemKeyValueII, ElemKeyValueCI @@ -49,10 +49,9 @@ contains integer, allocatable :: id_array(:) integer, allocatable :: key_array(:) integer(HID_T) :: file_id - integer(HID_T) :: cmfd_group - integer(HID_T) :: tallies_group, tally_group - integer(HID_T) :: meshes_group, mesh_group - integer(HID_T) :: filter_group, derivs_group, deriv_group + integer(HID_T) :: cmfd_group, tallies_group, tally_group, meshes_group, & + mesh_group, filter_group, derivs_group, deriv_group, & + runtime_group character(20), allocatable :: str_array(:) character(MAX_FILE_LEN) :: filename type(RegularMesh), pointer :: meshp @@ -93,6 +92,11 @@ contains call write_dataset(file_id, "seed", seed) ! Write run information + if (run_CE) then + call write_dataset(file_id, "run_CE", 1) + else + call write_dataset(file_id, "run_CE", 0) + end if select case(run_mode) case (MODE_FIXEDSOURCE) call write_dataset(file_id, "run_mode", "fixed source") @@ -128,13 +132,13 @@ contains call write_dataset(file_id, "cmfd_on", 1) cmfd_group = create_group(file_id, "cmfd") - call write_dataset(cmfd_group, "indices", cmfd%indices) - call write_dataset(cmfd_group, "k_cmfd", cmfd%k_cmfd) - call write_dataset(cmfd_group, "cmfd_src", cmfd%cmfd_src) - call write_dataset(cmfd_group, "cmfd_entropy", cmfd%entropy) - call write_dataset(cmfd_group, "cmfd_balance", cmfd%balance) - call write_dataset(cmfd_group, "cmfd_dominance", cmfd%dom) - call write_dataset(cmfd_group, "cmfd_srccmp", cmfd%src_cmp) + call write_dataset(cmfd_group, "indices", cmfd % indices) + call write_dataset(cmfd_group, "k_cmfd", cmfd % k_cmfd) + call write_dataset(cmfd_group, "cmfd_src", cmfd % cmfd_src) + call write_dataset(cmfd_group, "cmfd_entropy", cmfd % entropy) + call write_dataset(cmfd_group, "cmfd_balance", cmfd % balance) + call write_dataset(cmfd_group, "cmfd_dominance", cmfd % dom) + call write_dataset(cmfd_group, "cmfd_srccmp", cmfd % src_cmp) call close_group(cmfd_group) else call write_dataset(file_id, "cmfd_on", 0) @@ -150,18 +154,18 @@ contains if (n_meshes > 0) then ! Print list of mesh IDs - current => mesh_dict%keys() + current => mesh_dict % keys() allocate(id_array(n_meshes)) allocate(key_array(n_meshes)) i = 1 do while (associated(current)) - key_array(i) = current%key - id_array(i) = current%value + key_array(i) = current % key + id_array(i) = current % value ! Move to next mesh - next => current%next + next => current % next deallocate(current) current => next i = i + 1 @@ -175,16 +179,17 @@ contains ! Write information for meshes MESH_LOOP: do i = 1, n_meshes meshp => meshes(id_array(i)) - mesh_group = create_group(meshes_group, "mesh " // trim(to_str(meshp%id))) + mesh_group = create_group(meshes_group, "mesh " & + // trim(to_str(meshp % id))) - select case (meshp%type) + select case (meshp % type) case (MESH_REGULAR) call write_dataset(mesh_group, "type", "regular") end select - call write_dataset(mesh_group, "dimension", meshp%dimension) - call write_dataset(mesh_group, "lower_left", meshp%lower_left) - call write_dataset(mesh_group, "upper_right", meshp%upper_right) - call write_dataset(mesh_group, "width", meshp%width) + call write_dataset(mesh_group, "dimension", meshp % dimension) + call write_dataset(mesh_group, "lower_left", meshp % lower_left) + call write_dataset(mesh_group, "upper_right", meshp % upper_right) + call write_dataset(mesh_group, "width", meshp % width) call close_group(mesh_group) end do MESH_LOOP @@ -239,7 +244,7 @@ contains ! Write all tally information except results do i = 1, n_tallies tally => tallies(i) - key_array(i) = tally%id + key_array(i) = tally % id id_array(i) = i end do @@ -254,9 +259,9 @@ contains ! Get pointer to tally tally => tallies(i) tally_group = create_group(tallies_group, "tally " // & - trim(to_str(tally%id))) + trim(to_str(tally % id))) - select case(tally%estimator) + select case(tally % estimator) case (ESTIMATOR_ANALOG) call write_dataset(tally_group, "estimator", "analog") case (ESTIMATOR_TRACKLENGTH) @@ -264,16 +269,17 @@ contains case (ESTIMATOR_COLLISION) call write_dataset(tally_group, "estimator", "collision") end select - call write_dataset(tally_group, "n_realizations", tally%n_realizations) - call write_dataset(tally_group, "n_filters", tally%n_filters) + call write_dataset(tally_group, "n_realizations", & + tally % n_realizations) + call write_dataset(tally_group, "n_filters", tally % n_filters) ! Write filter information - FILTER_LOOP: do j = 1, tally%n_filters + FILTER_LOOP: do j = 1, tally % n_filters filter_group = create_group(tally_group, "filter " // & trim(to_str(j))) ! Write name of type - select case (tally%filters(j)%type) + select case (tally % filters(j) % type) case(FILTER_UNIVERSE) call write_dataset(filter_group, "type", "universe") case(FILTER_MATERIAL) @@ -302,36 +308,37 @@ contains call write_dataset(filter_group, "type", "delayedgroup") end select - call write_dataset(filter_group, "n_bins", tally%filters(j)%n_bins) + call write_dataset(filter_group, "n_bins", & + tally % filters(j) % n_bins) if (tally % filters(j) % type == FILTER_ENERGYIN .or. & tally % filters(j) % type == FILTER_ENERGYOUT .or. & tally % filters(j) % type == FILTER_MU .or. & tally % filters(j) % type == FILTER_POLAR .or. & tally % filters(j) % type == FILTER_AZIMUTHAL) then call write_dataset(filter_group, "bins", & - tally%filters(j)%real_bins) + tally % filters(j) % real_bins) else call write_dataset(filter_group, "bins", & - tally%filters(j)%int_bins) + tally % filters(j) % int_bins) end if call close_group(filter_group) end do FILTER_LOOP ! Set up nuclide bin array and then write - allocate(str_array(tally%n_nuclide_bins)) - NUCLIDE_LOOP: do j = 1, tally%n_nuclide_bins - if (tally%nuclide_bins(j) > 0) then + allocate(str_array(tally % n_nuclide_bins)) + NUCLIDE_LOOP: do j = 1, tally % n_nuclide_bins + if (tally % nuclide_bins(j) > 0) then ! Get index in cross section listings for this nuclide - i_list = nuclides(tally%nuclide_bins(j))%listing + i_list = nuclides(tally % nuclide_bins(j)) % listing ! Determine position of . in alias string (e.g. "U-235.71c"). If ! no . is found, just use the entire string. - i_xs = index(xs_listings(i_list)%alias, '.') + i_xs = index(xs_listings(i_list) % alias, '.') if (i_xs > 0) then - str_array(j) = xs_listings(i_list)%alias(1:i_xs - 1) + str_array(j) = xs_listings(i_list) % alias(1:i_xs - 1) else - str_array(j) = xs_listings(i_list)%alias + str_array(j) = xs_listings(i_list) % alias end if else str_array(j) = 'total' @@ -346,33 +353,33 @@ contains tally_derivs(tally % deriv) % id) end if - ! Write scores. - call write_dataset(tally_group, "n_score_bins", tally%n_score_bins) - allocate(str_array(size(tally%score_bins))) - do j = 1, size(tally%score_bins) - str_array(j) = reaction_name(tally%score_bins(j)) + call write_dataset(tally_group, "n_score_bins", tally % n_score_bins) + allocate(str_array(size(tally % score_bins))) + do j = 1, size(tally % score_bins) + str_array(j) = reaction_name(tally % score_bins(j)) end do call write_dataset(tally_group, "score_bins", str_array) - call write_dataset(tally_group, "n_user_score_bins", tally%n_user_score_bins) + call write_dataset(tally_group, "n_user_score_bins", & + tally % n_user_score_bins) deallocate(str_array) ! Write explicit moment order strings for each score bin k = 1 - allocate(str_array(tally%n_score_bins)) - MOMENT_LOOP: do j = 1, tally%n_user_score_bins - select case(tally%score_bins(k)) + allocate(str_array(tally % n_score_bins)) + MOMENT_LOOP: do j = 1, tally % n_user_score_bins + select case(tally % score_bins(k)) case (SCORE_SCATTER_N, SCORE_NU_SCATTER_N) - str_array(k) = 'P' // trim(to_str(tally%moment_order(k))) + str_array(k) = 'P' // trim(to_str(tally % moment_order(k))) k = k + 1 case (SCORE_SCATTER_PN, SCORE_NU_SCATTER_PN) - do n_order = 0, tally%moment_order(k) + do n_order = 0, tally % moment_order(k) str_array(k) = 'P' // trim(to_str(n_order)) k = k + 1 end do case (SCORE_SCATTER_YN, SCORE_NU_SCATTER_YN, SCORE_FLUX_YN, & SCORE_TOTAL_YN) - do n_order = 0, tally%moment_order(k) + do n_order = 0, tally % moment_order(k) do nm_order = -n_order, n_order str_array(k) = 'Y' // trim(to_str(n_order)) // ',' // & trim(to_str(nm_order)) @@ -424,8 +431,9 @@ contains tally => tallies(i) ! Write sum and sum_sq for each bin - tally_group = open_group(tallies_group, "tally " // to_str(tally%id)) - call write_dataset(tally_group, "results", tally%results) + tally_group = open_group(tallies_group, "tally " & + // to_str(tally % id)) + call write_dataset(tally_group, "results", tally % results) call close_group(tally_group) end do TALLY_RESULTS @@ -435,13 +443,45 @@ contains end if call close_group(tallies_group) + + ! Write out the runtime metrics. + runtime_group = create_group(file_id, "runtime") + call write_dataset(runtime_group, "total initialization", & + time_initialize % get_value()) + call write_dataset(runtime_group, "reading cross sections", & + time_read_xs % get_value()) + call write_dataset(runtime_group, "simulation", & + time_inactive % get_value() + time_active % get_value()) + call write_dataset(runtime_group, "transport", & + time_transport % get_value()) + if (run_mode == MODE_EIGENVALUE) then + call write_dataset(runtime_group, "inactive batches", & + time_inactive % get_value()) + end if + call write_dataset(runtime_group, "active batches", & + time_active % get_value()) + if (run_mode == MODE_EIGENVALUE) then + call write_dataset(runtime_group, "synchronizing fission bank", & + time_bank % get_value()) + call write_dataset(runtime_group, "sampling source sites", & + time_bank_sample % get_value()) + call write_dataset(runtime_group, "SEND-RECV source sites", & + time_bank_sendrecv % get_value()) + end if + call write_dataset(runtime_group, "accumulating tallies", & + time_tallies % get_value()) + if (cmfd_run) then + call write_dataset(runtime_group, "CMFD", time_cmfd % get_value()) + call write_dataset(runtime_group, "CMFD building matrices", & + time_cmfdbuild % get_value()) + call write_dataset(runtime_group, "CMFD solving matrices", & + time_cmfdsolve % get_value()) + end if + call write_dataset(runtime_group, "total", time_total % get_value()) + call close_group(runtime_group) + call file_close(file_id) end if - - if (master .and. n_tallies > 0) then - deallocate(id_array) - end if - end subroutine write_state_point !=============================================================================== @@ -687,6 +727,7 @@ contains integer(HID_T) :: tally_group real(8) :: real_array(3) logical :: source_present + integer :: sp_run_CE character(MAX_WORD_LEN) :: word type(TallyObject), pointer :: tally @@ -698,7 +739,10 @@ contains file_id = file_open(path_state_point, 'r', parallel=.true.) ! Read filetype - call read_dataset(file_id, "filetype", int_array(1)) + call read_dataset(file_id, "filetype", word) + if (word /= 'statepoint') then + call fatal_error("OpenMC tried to restart from a non-statepoint file.") + end if ! Read revision number for state point file and make sure it matches with ! current version @@ -711,6 +755,17 @@ contains ! Read and overwrite random number seed call read_dataset(file_id, "seed", seed) + ! It is not impossible for a state point to be generated from a CE run but + ! to be loaded in to an MG run (or vice versa), check to prevent that. + call read_dataset(file_id, "run_CE", sp_run_CE) + if (sp_run_CE == 0 .and. run_CE) then + call fatal_error("State point file is from multi-group run but & + & current run is continous-energy!") + else if (sp_run_CE == 1 .and. .not. run_CE) then + call fatal_error("State point file is from continuous-energy run but & + & current run is multi-group!") + end if + ! Read and overwrite run information except number of batches call read_dataset(file_id, "run_mode", word) select case(word) @@ -784,8 +839,13 @@ contains &file") end if - ! Read tallies to master + ! Read tallies to master. If we are using Parallel HDF5, all processes + ! need to be included in the HDF5 calls. +#ifdef PHDF5 + if (.true.) then +#else if (master) then +#endif ! Read number of realizations for global tallies call read_dataset(file_id, "n_realizations", n_realizations, indep=.true.) @@ -795,7 +855,8 @@ contains ! Check if tally results are present tallies_group = open_group(file_id, "tallies") - call read_dataset(file_id, "tallies_present", int_array(1), indep=.true.) + call read_dataset(tallies_group, "tallies_present", int_array(1), & + indep=.true.) ! Read in sum and sum squared if (int_array(1) == 1) then @@ -803,10 +864,12 @@ contains ! Set pointer to tally tally => tallies(i) - ! Read sum and sum_sq for each bin + ! Read sum, sum_sq, and N for each bin tally_group = open_group(tallies_group, "tally " // & - trim(to_str(tally%id))) - call read_dataset(tally_group, "results", tally%results) + trim(to_str(tally % id))) + call read_dataset(tally_group, "results", tally % results) + call read_dataset(tally_group, "n_realizations", & + tally % n_realizations) call close_group(tally_group) end do TALLY_RESULTS end if diff --git a/src/summary.F90 b/src/summary.F90 index 4ebf5fdfd..a1f024df8 100644 --- a/src/summary.F90 +++ b/src/summary.F90 @@ -1,18 +1,19 @@ module summary - use ace_header, only: Reaction, UrrData, Nuclide use constants use endf, only: reaction_name use geometry_header, only: Cell, Universe, Lattice, RectLattice, & - &HexLattice + &HexLattice, BASE_UNIVERSE use global use hdf5_interface use material_header, only: Material use mesh_header, only: RegularMesh + use nuclide_header use output, only: time_stamp use surface_header use string, only: to_str use tally_header, only: TallyObject + use output, only: find_offset use hdf5 @@ -37,6 +38,12 @@ contains ! Write header information call write_header(file_id) + if (run_CE) then + call write_dataset(file_id, "run_CE", 1) + else + call write_dataset(file_id, "run_CE", 0) + end if + ! Write number of particles call write_dataset(file_id, "n_particles", n_particles) call write_dataset(file_id, "n_batches", n_batches) @@ -488,7 +495,11 @@ contains ! Copy ZAID for each nuclide to temporary array allocate(nucnames(m%n_nuclides)) do j = 1, m%n_nuclides - i_list = nuclides(m%nuclide(j))%listing + if (run_CE) then + i_list = nuclides(m%nuclide(j))%listing + else + i_list = nuclides_MG(m%nuclide(j))%obj%listing + end if nucnames(j) = xs_listings(i_list)%alias end do @@ -531,6 +542,10 @@ contains type(RegularMesh), pointer :: m type(TallyObject), pointer :: t + integer :: offset ! distibcell offset + character(MAX_LINE_LEN), allocatable :: paths(:) ! distribcell paths array + character(MAX_LINE_LEN) :: path ! distribcell path + tallies_group = create_group(file_id, "tallies") ! Write total number of meshes @@ -573,21 +588,40 @@ contains ! Write number of filters call write_dataset(tally_group, "n_filters", t%n_filters) - FILTER_LOOP: do j = 1, t%n_filters + FILTER_LOOP: do j = 1, t % n_filters filter_group = create_group(tally_group, "filter " // trim(to_str(j))) ! Write number of bins for this filter - call write_dataset(filter_group, "n_bins", t%filters(j)%n_bins) + call write_dataset(filter_group, "n_bins", t % filters(j) % n_bins) ! Write filter bins - if (t%filters(j)%type == FILTER_ENERGYIN .or. & - t%filters(j)%type == FILTER_ENERGYOUT .or. & - t%filters(j)%type == FILTER_MU .or. & - t%filters(j)%type == FILTER_POLAR .or. & - t%filters(j)%type == FILTER_AZIMUTHAL) then - call write_dataset(filter_group, "bins", t%filters(j)%real_bins) + if (t % filters(j) % type == FILTER_ENERGYIN .or. & + t % filters(j)% type == FILTER_ENERGYOUT .or. & + t % filters(j) % type == FILTER_MU .or. & + t % filters(j) % type == FILTER_POLAR .or. & + t % filters(j) % type == FILTER_AZIMUTHAL) then + call write_dataset(filter_group, "bins", t % filters(j) % real_bins) else - call write_dataset(filter_group, "bins", t%filters(j)%int_bins) + call write_dataset(filter_group, "bins", t % filters(j) % int_bins) + end if + + ! Write paths to reach each distribcell instance + if (t % filters(j) % type == FILTER_DISTRIBCELL) then + ! Allocate array of strings for each distribcell path + allocate(paths(t % filters(j) % n_bins)) + + ! Store path for each distribcell instance + do k = 1, t % filters(j) % n_bins + path = '' + offset = 1 + call find_offset(t % filters(j) % int_bins(1), & + universes(BASE_UNIVERSE), k, offset, path) + paths(k) = path + end do + + ! Write array of distribcell paths to summary file + call write_dataset(filter_group, "paths", paths) + deallocate(paths) end if ! Write name of type @@ -691,63 +725,4 @@ contains end subroutine write_tallies -!=============================================================================== -! WRITE_TIMING -!=============================================================================== - - subroutine write_timing(file_id) - integer(HID_T), intent(in) :: file_id - - integer(8) :: total_particles - integer(HID_T) :: time_group - real(8) :: speed - - time_group = create_group(file_id, "timing") - - ! Write timing data - call write_dataset(time_group, "time_initialize", time_initialize%elapsed) - call write_dataset(time_group, "time_read_xs", time_read_xs%elapsed) - call write_dataset(time_group, "time_transport", time_transport%elapsed) - call write_dataset(time_group, "time_bank", time_bank%elapsed) - call write_dataset(time_group, "time_bank_sample", time_bank_sample%elapsed) - call write_dataset(time_group, "time_bank_sendrecv", time_bank_sendrecv%elapsed) - call write_dataset(time_group, "time_tallies", time_tallies%elapsed) - call write_dataset(time_group, "time_inactive", time_inactive%elapsed) - call write_dataset(time_group, "time_active", time_active%elapsed) - call write_dataset(time_group, "time_finalize", time_finalize%elapsed) - call write_dataset(time_group, "time_total", time_total%elapsed) - - ! Add descriptions to timing data - call write_attribute_string(time_group, "time_initialize", "description", & - "Total time elapsed for initialization (s)") - call write_attribute_string(time_group, "time_read_xs", "description", & - "Time reading cross-section libraries (s)") - call write_attribute_string(time_group, "time_transport", "description", & - "Time in transport only (s)") - call write_attribute_string(time_group, "time_bank", "description", & - "Total time synchronizing fission bank (s)") - call write_attribute_string(time_group, "time_bank_sample", "description", & - "Time between generations sampling source sites (s)") - call write_attribute_string(time_group, "time_bank_sendrecv", "description", & - "Time between generations SEND/RECVing source sites (s)") - call write_attribute_string(time_group, "time_tallies", "description", & - "Time between batches accumulating tallies (s)") - call write_attribute_string(time_group, "time_inactive", "description", & - "Total time in inactive batches (s)") - call write_attribute_string(time_group, "time_active", "description", & - "Total time in active batches (s)") - call write_attribute_string(time_group, "time_finalize", "description", & - "Total time for finalization (s)") - call write_attribute_string(time_group, "time_total", "description", & - "Total time elapsed (s)") - - ! Write calculation rate - total_particles = n_particles * n_batches * gen_per_batch - speed = real(total_particles) / (time_inactive%elapsed + & - time_active%elapsed) - call write_dataset(time_group, "neutrons_per_second", speed) - - call close_group(time_group) - end subroutine write_timing - end module summary diff --git a/src/surface_header.F90 b/src/surface_header.F90 index 76562f493..468655217 100644 --- a/src/surface_header.F90 +++ b/src/surface_header.F90 @@ -19,34 +19,34 @@ module surface_header contains procedure :: sense procedure :: reflect - procedure(iEvaluate), deferred :: evaluate - procedure(iDistance), deferred :: distance - procedure(iNormal), deferred :: normal + procedure(surface_evaluate_), deferred :: evaluate + procedure(surface_distance_), deferred :: distance + procedure(surface_normal_), deferred :: normal end type Surface abstract interface - pure function iEvaluate(this, xyz) result(f) + pure function surface_evaluate_(this, xyz) result(f) import Surface class(Surface), intent(in) :: this real(8), intent(in) :: xyz(3) real(8) :: f - end function iEvaluate + end function surface_evaluate_ - pure function iDistance(this, xyz, uvw, coincident) result(d) + pure function surface_distance_(this, xyz, uvw, coincident) result(d) import Surface class(Surface), intent(in) :: this real(8), intent(in) :: xyz(3) real(8), intent(in) :: uvw(3) logical, intent(in) :: coincident real(8) :: d - end function iDistance + end function surface_distance_ - pure function iNormal(this, xyz) result(uvw) + pure function surface_normal_(this, xyz) result(uvw) import Surface class(Surface), intent(in) :: this real(8), intent(in) :: xyz(3) real(8) :: uvw(3) - end function iNormal + end function surface_normal_ end interface !=============================================================================== diff --git a/src/tally.F90 b/src/tally.F90 index eeaa8770a..072fb7c0c 100644 --- a/src/tally.F90 +++ b/src/tally.F90 @@ -1,8 +1,8 @@ module tally - use ace_header, only: Reaction use constants use cross_section, only: multipole_deriv_eval + use endf_header, only: Constant1D use error, only: fatal_error use geometry_header use global @@ -16,8 +16,6 @@ module tally use search, only: binary_search use string, only: to_str use tally_header, only: TallyResult, TallyMapItem, TallyMapElement - use fission, only: nu_total, nu_delayed, yield_delayed - use interpolation, only: interpolate_tab1 #ifdef MPI use message_passing @@ -26,17 +24,58 @@ module tally implicit none integer :: position(N_FILTER_TYPES - 3) = 0 ! Tally map positioning array + !$omp threadprivate(position) + procedure(score_general_), pointer :: score_general => null() + procedure(get_scoring_bins_), pointer :: get_scoring_bins => null() + + abstract interface + subroutine score_general_(p, t, start_index, filter_index, i_nuclide, & + atom_density, flux) + import Particle + import TallyObject + type(Particle), intent(in) :: p + type(TallyObject), intent(inout) :: t + integer, intent(in) :: start_index + integer, intent(in) :: i_nuclide + integer, intent(in) :: filter_index ! for % results + real(8), intent(in) :: flux ! flux estimate + real(8), intent(in) :: atom_density ! atom/b-cm + end subroutine score_general_ + + subroutine get_scoring_bins_(p, i_tally, found_bin) + import Particle + type(Particle), intent(in) :: p + integer, intent(in) :: i_tally + logical, intent(out) :: found_bin + end subroutine get_scoring_bins_ + end interface + contains !=============================================================================== -! SCORE_GENERAL adds scores to the tally array for the given filter and nuclide. -! This will work for either analog or tracklength tallies. Note that +! INIT_TALLY_ROUTINES Sets the procedure pointers needed for minimizing code +! with the CE and MG modes. +!=============================================================================== + + subroutine init_tally_routines() + if (run_CE) then + score_general => score_general_ce + get_scoring_bins => get_scoring_bins_ce + else + score_general => score_general_mg + get_scoring_bins => get_scoring_bins_mg + end if + end subroutine init_tally_routines + +!=============================================================================== +! SCORE_GENERAL* adds scores to the tally array for the given filter and +! nuclide. This will work for either analog or tracklength tallies. Note that ! atom_density and flux are not used for analog tallies. !=============================================================================== - subroutine score_general(p, t, start_index, filter_index, i_nuclide, & + subroutine score_general_ce(p, t, start_index, filter_index, i_nuclide, & atom_density, flux) type(Particle), intent(in) :: p type(TallyObject), intent(inout) :: t @@ -49,8 +88,6 @@ contains integer :: i ! loop index for scoring bins integer :: l ! loop index for nuclides in material integer :: m ! loop index for reactions - integer :: n ! loop index for legendre order - integer :: num_nm ! Number of N,M orders in harmonic integer :: q ! loop index for scoring bins integer :: i_nuc ! index in nuclides array (from material) integer :: i_energy ! index in nuclide energy grid @@ -65,7 +102,6 @@ contains real(8) :: score ! analog tally score real(8) :: macro_total ! material macro total xs real(8) :: macro_scatt ! material macro scatt xs - real(8) :: uvw(3) ! particle direction real(8) :: E ! particle energy i = 0 @@ -127,7 +163,6 @@ contains case (SCORE_INVERSE_VELOCITY) - ! make sure the correct energy is used if (t % estimator == ESTIMATOR_TRACKLENGTH) then E = p % E @@ -209,9 +244,9 @@ contains ! Only analog estimators are available. ! Skip any event where the particle didn't scatter if (p % event /= EVENT_SCATTER) cycle SCORE_LOOP - ! For scattering production, we need to use the pre-collision - ! weight times the multiplicity as the estimate for the number of - ! neutrons exiting a reaction with neutrons in the exit channel + ! For scattering production, we need to use the pre-collision weight + ! times the yield as the estimate for the number of neutrons exiting a + ! reaction with neutrons in the exit channel if (p % event_MT == ELASTIC .or. p % event_MT == N_LEVEL .or. & (p % event_MT >= N_N1 .and. p % event_MT <= N_NC)) then ! Don't waste time on very common reactions we know have multiplicities @@ -221,16 +256,17 @@ contains m = nuclides(p%event_nuclide)%reaction_index% & get_key(p % event_MT) - ! Get multiplicity and apply to score + ! Get yield and apply to score associate (rxn => nuclides(p%event_nuclide)%reactions(m)) - if (rxn % multiplicity_with_E) then - ! Then the multiplicity was already incorporated in to p % wgt - ! per the scattering routine, + select type (yield => rxn % products(1) % yield) + type is (Constant1D) + ! Grab the yield from the reaction + score = p % last_wgt * yield % y + class default + ! the yield was already incorporated in to p % wgt per the + ! scattering routine score = p % wgt - else - ! Grab the multiplicity from the rxn - score = p % last_wgt * rxn % multiplicity - end if + end select end associate end if @@ -243,7 +279,7 @@ contains cycle SCORE_LOOP end if ! For scattering production, we need to use the pre-collision - ! weight times the multiplicity as the estimate for the number of + ! weight times the yield as the estimate for the number of ! neutrons exiting a reaction with neutrons in the exit channel if (p % event_MT == ELASTIC .or. p % event_MT == N_LEVEL .or. & (p % event_MT >= N_N1 .and. p % event_MT <= N_NC)) then @@ -254,16 +290,17 @@ contains m = nuclides(p%event_nuclide)%reaction_index% & get_key(p % event_MT) - ! Get multiplicity and apply to score + ! Get yield and apply to score associate (rxn => nuclides(p%event_nuclide)%reactions(m)) - if (rxn % multiplicity_with_E) then - ! Then the multiplicity was already incorporated in to p % wgt - ! per the scattering routine, + select type (yield => rxn % products(1) % yield) + type is (Constant1D) + ! Grab the yield from the reaction + score = p % last_wgt * yield % y + class default + ! the yield was already incorporated in to p % wgt per the + ! scattering routine score = p % wgt - else - ! Grab the multiplicity from the rxn - score = p % last_wgt * rxn % multiplicity - end if + end select end associate end if @@ -276,7 +313,7 @@ contains cycle SCORE_LOOP end if ! For scattering production, we need to use the pre-collision - ! weight times the multiplicity as the estimate for the number of + ! weight times the yield as the estimate for the number of ! neutrons exiting a reaction with neutrons in the exit channel if (p % event_MT == ELASTIC .or. p % event_MT == N_LEVEL .or. & (p % event_MT >= N_N1 .and. p % event_MT <= N_NC)) then @@ -287,16 +324,17 @@ contains m = nuclides(p%event_nuclide)%reaction_index% & get_key(p % event_MT) - ! Get multiplicity and apply to score + ! Get yield and apply to score associate (rxn => nuclides(p%event_nuclide)%reactions(m)) - if (rxn % multiplicity_with_E) then - ! Then the multiplicity was already incorporated in to p % wgt - ! per the scattering routine, + select type (yield => rxn % products(1) % yield) + type is (Constant1D) + ! Grab the yield from the reaction + score = p % last_wgt * yield % y + class default + ! the yield was already incorporated in to p % wgt per the + ! scattering routine score = p % wgt - else - ! Grab the multiplicity from the rxn - score = p % last_wgt * rxn % multiplicity - end if + end select end associate end if @@ -388,7 +426,7 @@ contains ! neutrons were emitted with different energies, multiple ! outgoing energy bins may have been scored to. The following ! logic treats this special case and results to multiple bins - call score_fission_eout(p, t, score_index) + call score_fission_eout_ce(p, t, score_index) cycle SCORE_LOOP end if end if @@ -463,12 +501,11 @@ contains d = t % filters(dg_filter) % int_bins(d_bin) ! Compute the yield for this delayed group - yield = yield_delayed(nuclides(p % event_nuclide), E, d) + yield = nuclides(p % event_nuclide) % nu(E, EMISSION_DELAYED, d) ! Compute the score and tally to bin score = p % absorb_wgt * yield * micro_xs(p % event_nuclide) & - % fission * nu_delayed(nuclides(p % event_nuclide), E) / & - micro_xs(p % event_nuclide) % absorption + % fission / micro_xs(p % event_nuclide) % absorption call score_fission_delayed_dg(t, d_bin, score, score_index) end do cycle SCORE_LOOP @@ -476,9 +513,9 @@ contains ! If the delayed group filter is not present, compute the score ! by multiplying the absorbed weight by the fraction of the ! delayed-nu-fission xs to the absorption xs - score = p % absorb_wgt * micro_xs(p % event_nuclide) & - % fission * nu_delayed(nuclides(p % event_nuclide), E) / & - micro_xs(p % event_nuclide) % absorption + score = p % absorb_wgt * micro_xs(p % event_nuclide) % fission & + * nuclides(p % event_nuclide) % nu(E, EMISSION_DELAYED) & + / micro_xs(p % event_nuclide) % absorption end if end if else @@ -528,11 +565,11 @@ contains d = t % filters(dg_filter) % int_bins(d_bin) ! Compute the yield for this delayed group - yield = yield_delayed(nuclides(i_nuclide), E, d) + yield = nuclides(i_nuclide) % nu(E, EMISSION_DELAYED, d) ! Compute the score and tally to bin - score = micro_xs(i_nuclide) % fission * yield & - * nu_delayed(nuclides(i_nuclide), E) * atom_density * flux + score = micro_xs(i_nuclide) % fission * yield * & + atom_density * flux call score_fission_delayed_dg(t, d_bin, score, score_index) end do cycle SCORE_LOOP @@ -540,8 +577,8 @@ contains ! If the delayed group filter is not present, compute the score ! by multiplying the delayed-nu-fission macro xs by the flux - score = micro_xs(i_nuclide) % fission * & - nu_delayed(nuclides(i_nuclide), E) * atom_density * flux + score = micro_xs(i_nuclide) % fission * nuclides(i_nuclide) % & + nu(E, EMISSION_DELAYED) * atom_density * flux end if ! Tally is on total nuclides @@ -566,11 +603,10 @@ contains d = t % filters(dg_filter) % int_bins(d_bin) ! Get the yield for the desired nuclide and delayed group - yield = yield_delayed(nuclides(i_nuc), E, d) + yield = nuclides(i_nuc) % nu(E, EMISSION_DELAYED, d) ! Compute the score and tally to bin - score = micro_xs(i_nuc) % fission * yield & - * nu_delayed(nuclides(i_nuc), E) * atom_density_ * flux + score = micro_xs(i_nuc) % fission * yield * atom_density_ * flux call score_fission_delayed_dg(t, d_bin, score, score_index) end do end do @@ -589,8 +625,8 @@ contains i_nuc = materials(p % material) % nuclide(l) ! Accumulate the contribution from each nuclide - score = score + micro_xs(i_nuc) % fission & - * nu_delayed(nuclides(i_nuc), E) * atom_density_ * flux + score = score + micro_xs(i_nuc) % fission * nuclides(i_nuc) % & + nu(E, EMISSION_DELAYED) * atom_density_ * flux end do end if end if @@ -741,7 +777,6 @@ contains end if end if - end select !######################################################################### @@ -754,101 +789,570 @@ contains !######################################################################### ! Expand score if necessary and add to tally results. + call expand_and_score(p, t, score_index, filter_index, score_bin, & + score, i) + + end do SCORE_LOOP + end subroutine score_general_ce + + subroutine score_general_mg(p, t, start_index, filter_index, i_nuclide, & + atom_density, flux) + type(Particle), intent(in) :: p + type(TallyObject), intent(inout) :: t + integer, intent(in) :: start_index + integer, intent(in) :: i_nuclide + integer, intent(in) :: filter_index ! for % results + real(8), intent(in) :: flux ! flux estimate + real(8), intent(in) :: atom_density ! atom/b-cm + + integer :: i ! loop index for scoring bins + integer :: q ! loop index for scoring bins + integer :: score_bin ! scoring bin, e.g. SCORE_FLUX + integer :: score_index ! scoring bin index + real(8) :: score ! analog tally score + real(8) :: macro_total ! material macro total xs + real(8) :: macro_scatt ! material macro scatt xs + real(8) :: micro_abs ! nuclidic microscopic abs + real(8) :: p_uvw(3) ! Particle's current uvw + + ! Set the direction, if needed for nuclidic data, so that nuc % get_xs + ! knows wihch direction it should be using for direction-dependent + ! mgxs + if (i_nuclide > 0) then + p_uvw = p % coord(p % n_coord) % uvw + end if + + i = 0 + SCORE_LOOP: do q = 1, t % n_user_score_bins + i = i + 1 + + ! determine what type of score bin + score_bin = t % score_bins(i) + + ! determine scoring bin index + score_index = start_index + i + + !######################################################################### + ! Determine appropirate scoring value. select case(score_bin) - case (SCORE_SCATTER_N, SCORE_NU_SCATTER_N) - ! Find the scattering order for a singly requested moment, and - ! store its moment contribution. - if (t % moment_order(i) == 1) then - score = score * p % mu ! avoid function call overhead + case (SCORE_FLUX, SCORE_FLUX_YN) + if (t % estimator == ESTIMATOR_ANALOG) then + ! All events score to a flux bin. We actually use a collision + ! estimator in place of an analog one since there is no way to count + ! 'events' exactly for the flux + if (survival_biasing) then + ! We need to account for the fact that some weight was already + ! absorbed + score = p % last_wgt + p % absorb_wgt + else + score = p % last_wgt + end if + score = score / material_xs % total + else - score = score * calc_pn(t % moment_order(i), p % mu) - endif -!$omp atomic - t % results(score_index, filter_index) % value = & - t % results(score_index, filter_index) % value + score - - - case(SCORE_SCATTER_YN, SCORE_NU_SCATTER_YN) - score_index = score_index - 1 - num_nm = 1 - ! Find the order for a collection of requested moments - ! and store the moment contribution of each - do n = 0, t % moment_order(i) - ! determine scoring bin index - score_index = score_index + num_nm - ! Update number of total n,m bins for this n (m = [-n: n]) - num_nm = 2 * n + 1 - - ! multiply score by the angular flux moments and store -!$omp critical (score_general_scatt_yn) - t % results(score_index: score_index + num_nm - 1, filter_index) & - % value = t & - % results(score_index: score_index + num_nm - 1, filter_index)& - % value & - + score * calc_pn(n, p % mu) * calc_rn(n, p % last_uvw) -!$omp end critical (score_general_scatt_yn) - end do - i = i + (t % moment_order(i) + 1)**2 - 1 - - - case(SCORE_FLUX_YN, SCORE_TOTAL_YN) - score_index = score_index - 1 - num_nm = 1 - if (t % estimator == ESTIMATOR_ANALOG .or. & - t % estimator == ESTIMATOR_COLLISION) then - uvw = p % last_uvw - else if (t % estimator == ESTIMATOR_TRACKLENGTH) then - uvw = p % coord(1) % uvw + ! For flux, we need no cross section + score = flux end if - ! Find the order for a collection of requested moments - ! and store the moment contribution of each - do n = 0, t % moment_order(i) - ! determine scoring bin index - score_index = score_index + num_nm - ! Update number of total n,m bins for this n (m = [-n: n]) - num_nm = 2 * n + 1 - - ! multiply score by the angular flux moments and store -!$omp critical (score_general_flux_tot_yn) - t % results(score_index: score_index + num_nm - 1, filter_index) & - % value = t & - % results(score_index: score_index + num_nm - 1, filter_index)& - % value & - + score * calc_rn(n, uvw) -!$omp end critical (score_general_flux_tot_yn) - end do - i = i + (t % moment_order(i) + 1)**2 - 1 - case (SCORE_SCATTER_PN, SCORE_NU_SCATTER_PN) - score_index = score_index - 1 - ! Find the scattering order for a collection of requested moments - ! and store the moment contribution of each - do n = 0, t % moment_order(i) - ! determine scoring bin index - score_index = score_index + 1 + case (SCORE_TOTAL, SCORE_TOTAL_YN) + if (t % estimator == ESTIMATOR_ANALOG) then + ! All events will score to the total reaction rate. We can just + ! use the weight of the particle entering the collision as the + ! score + if (survival_biasing) then + ! We need to account for the fact that some weight was already + ! absorbed + score = p % last_wgt + p % absorb_wgt + else + score = p % last_wgt + end if - ! get the score and tally it -!$omp atomic - t % results(score_index, filter_index) % value = & - t % results(score_index, filter_index) % value & - + score * calc_pn(n, p % mu) - end do - i = i + t % moment_order(i) + else + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = nuc % get_xs(p % g, 'total', UVW=p_uvw) * & + atom_density * flux + end associate + else + score = material_xs % total * flux + end if + end if - case default -!$omp atomic - t % results(score_index, filter_index) % value = & - t % results(score_index, filter_index) % value + score + case (SCORE_INVERSE_VELOCITY) + if (t % estimator == ESTIMATOR_ANALOG) then + ! All events score to an inverse velocity bin. We actually use a + ! collision estimator in place of an analog one since there is no way + ! to count 'events' exactly for the inverse velocity + if (survival_biasing) then + ! We need to account for the fact that some weight was already + ! absorbed + score = p % last_wgt + p % absorb_wgt + else + score = p % last_wgt + end if + score = score * inverse_velocities(p % last_g) + else + ! For inverse velocity, we need no cross section + score = score * inverse_velocities(p % g) + end if + + + case (SCORE_SCATTER, SCORE_SCATTER_N) + if (t % estimator == ESTIMATOR_ANALOG) then + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) cycle SCORE_LOOP + ! Since only scattering events make it here, again we can use + ! the weight entering the collision as the estimator for the + ! reaction rate + score = p % last_wgt + + else + ! Note SCORE_SCATTER_N not available for tracklength/collision. + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = nuc % get_xs(p % g, 'scatter', UVW=p_uvw) * & + atom_density * flux + end associate + else + ! Get the scattering x/s (stored in % elastic) + score = material_xs % elastic * flux + end if + end if + + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = score * nuc % get_xs(p % g, 'f_mu/mult', p % last_g, & + p % last_uvw, p % mu) + end associate + else + score = score / & + macro_xs(p % material) % obj % get_xs(p % g, 'mult', & + p % last_g, & + p % last_uvw) + end if + + + case (SCORE_SCATTER_PN) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) then + i = i + t % moment_order(i) + cycle SCORE_LOOP + end if + ! Since only scattering events make it here, again we can use + ! the weight entering the collision as the estimator for the + ! reaction rate + score = p % last_wgt + + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = score * nuc % get_xs(p % g, 'f_mu/mult', p % last_g, & + p % last_uvw, p % mu) + end associate + else + score = score / & + macro_xs(p % material) % obj % get_xs(p % g, 'mult', & + p % last_g, & + p % last_uvw) + end if + + + case (SCORE_SCATTER_YN) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) then + i = i + (t % moment_order(i) + 1)**2 - 1 + cycle SCORE_LOOP + end if + ! Since only scattering events make it here, again we can use + ! the weight entering the collision as the estimator for the + ! reaction rate + score = p % last_wgt + + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = score * nuc % get_xs(p % g, 'f_mu/mult', p % last_g, & + p % last_uvw, p % mu) + end associate + else + score = score / & + macro_xs(p % material) % obj % get_xs(p % g, 'mult', & + p % last_g, & + p % last_uvw) + end if + + + case (SCORE_NU_SCATTER, SCORE_NU_SCATTER_N) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) cycle SCORE_LOOP + ! For scattering production, we need to use the pre-collision + ! weight times the multiplicity as the estimate for the number of + ! neutrons exiting a reaction with neutrons in the exit channel + score = p % wgt + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = score * nuc % get_xs(p % g, 'f_mu', p % last_g, & + p % last_uvw, p % mu) + end associate + end if + + + case (SCORE_NU_SCATTER_PN) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) then + i = i + t % moment_order(i) + cycle SCORE_LOOP + end if + ! For scattering production, we need to use the pre-collision + ! weight times the multiplicity as the estimate for the number of + ! neutrons exiting a reaction with neutrons in the exit channel + score = p % wgt + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = score * nuc % get_xs(p % g, 'f_mu', p % last_g, & + p % last_uvw, p % mu) + end associate + end if + + + case (SCORE_NU_SCATTER_YN) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) then + i = i + (t % moment_order(i) + 1)**2 - 1 + cycle SCORE_LOOP + end if + ! For scattering production, we need to use the pre-collision + ! weight times the multiplicity as the estimate for the number of + ! neutrons exiting a reaction with neutrons in the exit channel + score = p % wgt + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = score * nuc % get_xs(p % g, 'f_mu', p % last_g, & + p % last_uvw, p % mu) + end associate + end if + + + case (SCORE_TRANSPORT) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) cycle SCORE_LOOP + ! get material macros + macro_total = material_xs % total + macro_scatt = material_xs % elastic + ! Score total rate - p1 scatter rate Note estimator needs to be + ! adjusted since tallying is only occuring when a scatter has + ! happened. Effectively this means multiplying the estimator by + ! total/scatter macro + score = (macro_total - p % mu * macro_scatt) * (ONE / macro_scatt) + + + case (SCORE_N_1N) + ! Only analog estimators are available. + ! Skip any event where the particle didn't scatter + if (p % event /= EVENT_SCATTER) cycle SCORE_LOOP + ! Skip any events where weight of particle changed + if (p % wgt /= p % last_wgt) cycle SCORE_LOOP + ! All events that reach this point are (n,1n) reactions + score = p % last_wgt + + + case (SCORE_ABSORPTION) + if (t % estimator == ESTIMATOR_ANALOG) then + if (survival_biasing) then + ! No absorption events actually occur if survival biasing is on -- + ! just use weight absorbed in survival biasing + score = p % absorb_wgt + else + ! Skip any event where the particle wasn't absorbed + if (p % event == EVENT_SCATTER) cycle SCORE_LOOP + ! All fission and absorption events will contribute here, so we + ! can just use the particle's weight entering the collision + score = p % last_wgt + end if + + else + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = nuc % get_xs(p % g, 'absorption', UVW=p_uvw) & + * atom_density * flux + end associate + else + score = material_xs % absorption * flux + end if + end if + + + case (SCORE_FISSION) + if (t % estimator == ESTIMATOR_ANALOG) then + if (survival_biasing) then + ! No fission events occur if survival biasing is on -- need to + ! calculate fraction of absorptions that would have resulted in + ! fission + associate (nuc => nuclides_MG(i_nuclide) % obj) + micro_abs = nuc % get_xs(p % g, 'absorption', UVW=p_uvw) + if (micro_abs > ZERO) then + score = p % absorb_wgt * & + nuc % get_xs(p % g, 'fission', UVW=p_uvw) & + / micro_abs + else + score = ZERO + end if + end associate + else + ! Skip any non-absorption events + if (p % event == EVENT_SCATTER) cycle SCORE_LOOP + ! All fission events will contribute, so again we can use + ! particle's weight entering the collision as the estimate for the + ! fission reaction rate + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = p % last_wgt & + * nuc % get_xs(p % g, 'fission', UVW=p_uvw) & + / nuc % get_xs(p % g, 'absorption', UVW=p_uvw) + end associate + end if + + else + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = nuc % get_xs(p % g, 'fission', UVW=p_uvw) * & + atom_density * flux + end associate + else + score = flux * macro_xs(p % material) % obj % get_xs(p % g, & + 'fission', UVW=p_uvw) + + end if + end if + + + case (SCORE_NU_FISSION) + if (t % estimator == ESTIMATOR_ANALOG) then + if (survival_biasing .or. p % fission) then + if (t % find_filter(FILTER_ENERGYOUT) > 0) then + ! Normally, we only need to make contributions to one scoring + ! bin. However, in the case of fission, since multiple fission + ! neutrons were emitted with different energies, multiple + ! outgoing energy bins may have been scored to. The following + ! logic treats this special case and results to multiple bins + call score_fission_eout_mg(p, t, score_index) + cycle SCORE_LOOP + end if + end if + if (survival_biasing) then + ! No fission events occur if survival biasing is on -- need to + ! calculate fraction of absorptions that would have resulted in + ! nu-fission + associate (nuc => nuclides_MG(i_nuclide) % obj) + micro_abs = nuc % get_xs(p % g, 'absorption', UVW=p_uvw) + if (micro_abs > ZERO) then + score = p % absorb_wgt * & + nuc % get_xs(p % g, 'fission', UVW=p_uvw) / & + micro_abs + else + score = ZERO + end if + end associate + else + ! Skip any non-fission events + if (.not. p % fission) cycle SCORE_LOOP + ! If there is no outgoing energy filter, than we only need to + ! score to one bin. For the score to be 'analog', we need to + ! score the number of particles that were banked in the fission + ! bank. Since this was weighted by 1/keff, we multiply by keff + ! to get the proper score. + score = keff * p % wgt_bank + end if + + else + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = nuc % get_xs(p % g, 'nu_fission', UVW=p_uvw) & + * atom_density * flux + end associate + else + score = material_xs % nu_fission * flux + end if + end if + + + case (SCORE_KAPPA_FISSION) + ! Determine kappa-fission cross section + score = ZERO + if (t % estimator == ESTIMATOR_ANALOG) then + if (survival_biasing) then + ! No fission events occur if survival biasing is on -- need to + ! calculate fraction of absorptions that would have resulted in + ! fission scale by kappa-fission + associate (nuc => nuclides_MG(i_nuclide) % obj) + micro_abs = nuc % get_xs(p % g, 'absorption', UVW=p_uvw) + if (micro_abs > ZERO) then + score = p % absorb_wgt * & + nuc % get_xs(p % g, 'k_fission', UVW=p_uvw) / & + micro_abs + end if + end associate + else + ! Skip any non-absorption events + if (p % event == EVENT_SCATTER) cycle SCORE_LOOP + ! All fission events will contribute, so again we can use + ! particle's weight entering the collision as the estimate for + ! the fission energy production rate + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = p % last_wgt * & + nuc % get_xs(p % g, 'k_fission', UVW=p_uvw) / & + nuc % get_xs(p % g, 'absorption', UVW=p_uvw) + end associate + end if + + else + if (i_nuclide > 0) then + associate (nuc => nuclides_MG(i_nuclide) % obj) + score = nuc % get_xs(p % g, 'k_fission', UVW=p_uvw) & + * atom_density * flux + end associate + else + score = flux * macro_xs(p % material) % obj % get_xs(p % g, & + 'k_fission', UVW=p_uvw) + end if + end if + + + case (SCORE_EVENTS) + ! Simply count number of scoring events + score = ONE end select + + !######################################################################### + ! Expand score if necessary and add to tally results. + call expand_and_score(p, t, score_index, filter_index, score_bin, & + score, i) + end do SCORE_LOOP - end subroutine score_general + end subroutine score_general_mg + +!=============================================================================== +! EXPAND_AND_SCORE takes a previously determined score value and adjusts it +! if necessary (for functional expansion weighting), and then adds the resultant +! value to the tally results array. +!=============================================================================== + + subroutine expand_and_score(p, t, score_index, filter_index, score_bin, & + score, i) + type(Particle), intent(in) :: p + type(TallyObject), intent(inout) :: t + integer, intent(inout) :: score_index + integer, intent(in) :: filter_index ! for % results + integer, intent(in) :: score_bin ! score of concern + real(8), intent(inout) :: score ! data to score + integer, intent(inout) :: i ! Working index + + integer :: num_nm ! Number of N,M orders in harmonic + integer :: n ! Moment loop index + real(8) :: uvw(3) + + select case(score_bin) + case (SCORE_SCATTER_N, SCORE_NU_SCATTER_N) + ! Find the scattering order for a singly requested moment, and + ! store its moment contribution. + if (t % moment_order(i) == 1) then + score = score * p % mu ! avoid function call overhead + else + score = score * calc_pn(t % moment_order(i), p % mu) + endif +!$omp atomic + t % results(score_index, filter_index) % value = & + t % results(score_index, filter_index) % value + score + + + case(SCORE_SCATTER_YN, SCORE_NU_SCATTER_YN) + score_index = score_index - 1 + num_nm = 1 + ! Find the order for a collection of requested moments + ! and store the moment contribution of each + do n = 0, t % moment_order(i) + ! determine scoring bin index + score_index = score_index + num_nm + ! Update number of total n,m bins for this n (m = [-n: n]) + num_nm = 2 * n + 1 + + ! multiply score by the angular flux moments and store +!$omp critical (score_general_scatt_yn) + t % results(score_index: score_index + num_nm - 1, filter_index) & + % value = t & + % results(score_index: score_index + num_nm - 1, filter_index)& + % value & + + score * calc_pn(n, p % mu) * calc_rn(n, p % last_uvw) +!$omp end critical (score_general_scatt_yn) + end do + i = i + (t % moment_order(i) + 1)**2 - 1 + + + case(SCORE_FLUX_YN, SCORE_TOTAL_YN) + score_index = score_index - 1 + num_nm = 1 + if (t % estimator == ESTIMATOR_ANALOG .or. & + t % estimator == ESTIMATOR_COLLISION) then + uvw = p % last_uvw + else if (t % estimator == ESTIMATOR_TRACKLENGTH) then + uvw = p % coord(1) % uvw + end if + ! Find the order for a collection of requested moments + ! and store the moment contribution of each + do n = 0, t % moment_order(i) + ! determine scoring bin index + score_index = score_index + num_nm + ! Update number of total n,m bins for this n (m = [-n: n]) + num_nm = 2 * n + 1 + + ! multiply score by the angular flux moments and store +!$omp critical (score_general_flux_tot_yn) + t % results(score_index: score_index + num_nm - 1, filter_index) & + % value = t & + % results(score_index: score_index + num_nm - 1, filter_index)& + % value & + + score * calc_rn(n, uvw) +!$omp end critical (score_general_flux_tot_yn) + end do + i = i + (t % moment_order(i) + 1)**2 - 1 + + + case (SCORE_SCATTER_PN, SCORE_NU_SCATTER_PN) + score_index = score_index - 1 + ! Find the scattering order for a collection of requested moments + ! and store the moment contribution of each + do n = 0, t % moment_order(i) + ! determine scoring bin index + score_index = score_index + 1 + + ! get the score and tally it +!$omp atomic + t % results(score_index, filter_index) % value = & + t % results(score_index, filter_index) % value & + + score * calc_pn(n, p % mu) + end do + i = i + t % moment_order(i) + + + case default +!$omp atomic + t % results(score_index, filter_index) % value = & + t % results(score_index, filter_index) % value + score + + + end select + + end subroutine expand_and_score !=============================================================================== ! SCORE_ALL_NUCLIDES tallies individual nuclide reaction rates specifically when @@ -1017,7 +1521,7 @@ contains ! neutrons produced with different energies. !=============================================================================== - subroutine score_fission_eout(p, t, i_score) + subroutine score_fission_eout_ce(p, t, i_score) type(Particle), intent(in) :: p type(TallyObject), intent(inout) :: t integer, intent(in) :: i_score ! index for score @@ -1076,7 +1580,70 @@ contains ! reset outgoing energy bin and score index matching_bins(i) = bin_energyout - end subroutine score_fission_eout + end subroutine score_fission_eout_ce + + subroutine score_fission_eout_mg(p, t, i_score) + type(Particle), intent(in) :: p + type(TallyObject), intent(inout) :: t + integer, intent(in) :: i_score ! index for score + + integer :: i ! index of outgoing energy filter + integer :: n ! number of energies on filter + integer :: k ! loop index for bank sites + integer :: bin_energyout ! original outgoing energy bin + integer :: i_filter ! index for matching filter bin combination + real(8) :: score ! actual score + integer :: gout ! energy group of fission bank site + real(8) :: E_out + + ! save original outgoing energy bin and score index + i = t % find_filter(FILTER_ENERGYOUT) + bin_energyout = matching_bins(i) + + ! Get number of energies on filter + n = size(t % filters(i) % real_bins) + + ! Since the creation of fission sites is weighted such that it is + ! expected to create n_particles sites, we need to multiply the + ! score by keff to get the true nu-fission rate. Otherwise, the sum + ! of all nu-fission rates would be ~1.0. + + ! loop over number of particles banked + do k = 1, p % n_bank + ! determine score based on bank site weight and keff + score = keff * fission_bank(n_bank - p % n_bank + k) % wgt + + if (t % energyout_matches_groups) then + ! determine outgoing energy from fission bank + gout = int(fission_bank(n_bank - p % n_bank + k) % E) + + ! change outgoing energy bin + matching_bins(i) = gout + else + ! determine outgoing energy from fission bank + E_out = fission_bank(n_bank - p % n_bank + k) % E + + ! check if outgoing energy is within specified range on filter + if (E_out < t % filters(i) % real_bins(1) .or. & + E_out > t % filters(i) % real_bins(n)) cycle + + ! change outgoing energy bin + matching_bins(i) = binary_search(t % filters(i) % real_bins, n, E_out) + end if + + ! determine scoring index + i_filter = sum((matching_bins(1:t%n_filters) - 1) * t % stride) + 1 + + ! Add score to tally +!$omp atomic + t % results(i_score, i_filter) % value = & + t % results(i_score, i_filter) % value + score + end do + + ! reset outgoing energy bin and score index + matching_bins(i) = bin_energyout + + end subroutine score_fission_eout_mg !=============================================================================== ! SCORE_FISSION_DELAYED_EOUT handles a special case where we need to store @@ -1356,7 +1923,7 @@ contains real(8) :: phi type(TallyObject), pointer :: t type(RegularMesh), pointer :: m - type(Material), pointer :: mat + type(Material), pointer :: mat t => tallies(i_tally) matching_bins(1:t%n_filters) = 1 @@ -1718,7 +2285,7 @@ contains ! for a tally based on the particle's current attributes. !=============================================================================== - subroutine get_scoring_bins(p, i_tally, found_bin) + subroutine get_scoring_bins_ce(p, i_tally, found_bin) type(Particle), intent(in) :: p integer, intent(in) :: i_tally @@ -1924,7 +2491,223 @@ contains end do FILTER_LOOP - end subroutine get_scoring_bins + end subroutine get_scoring_bins_ce + + subroutine get_scoring_bins_mg(p, i_tally, found_bin) + + type(Particle), intent(in) :: p + integer, intent(in) :: i_tally + logical, intent(out) :: found_bin + + integer :: i ! loop index for filters + integer :: j + integer :: n ! number of bins for single filter + integer :: distribcell_index ! index in distribcell arrays + integer :: offset ! offset for distribcell + real(8) :: theta, phi ! Polar and Azimuthal Angles, respectively + real(8) :: E + type(TallyObject), pointer :: t + type(RegularMesh), pointer :: m + + found_bin = .true. + t => tallies(i_tally) + matching_bins(1:t%n_filters) = 1 + + FILTER_LOOP: do i = 1, t % n_filters + + select case (t % filters(i) % type) + case (FILTER_MESH) + ! determine mesh bin + m => meshes(t % filters(i) % int_bins(1)) + + ! Determine if we're in the mesh first + call get_mesh_bin(m, p % coord(1) % xyz, matching_bins(i)) + + case (FILTER_UNIVERSE) + ! determine next universe bin + ! TODO: Account for multiple universes when performing this filter + matching_bins(i) = get_next_bin(FILTER_UNIVERSE, & + p % coord(p % n_coord) % universe, i_tally) + + case (FILTER_MATERIAL) + if (p % material == MATERIAL_VOID) then + matching_bins(i) = NO_BIN_FOUND + else + matching_bins(i) = get_next_bin(FILTER_MATERIAL, & + p % material, i_tally) + endif + + case (FILTER_CELL) + ! determine next cell bin + do j = 1, p % n_coord + position(FILTER_CELL) = 0 + matching_bins(i) = get_next_bin(FILTER_CELL, & + p % coord(j) % cell, i_tally) + if (matching_bins(i) /= NO_BIN_FOUND) exit + end do + + case (FILTER_DISTRIBCELL) + ! determine next distribcell bin + distribcell_index = cells(t % filters(i) % int_bins(1)) & + % distribcell_index + matching_bins(i) = NO_BIN_FOUND + offset = 0 + do j = 1, p % n_coord + if (cells(p % coord(j) % cell) % type == CELL_FILL) then + offset = offset + cells(p % coord(j) % cell) % & + offset(distribcell_index) + elseif(cells(p % coord(j) % cell) % type == CELL_LATTICE) then + if (lattices(p % coord(j + 1) % lattice) % obj & + % are_valid_indices([& + p % coord(j + 1) % lattice_x, & + p % coord(j + 1) % lattice_y, & + p % coord(j + 1) % lattice_z])) then + offset = offset + lattices(p % coord(j + 1) % lattice) % obj % & + offset(distribcell_index, & + p % coord(j + 1) % lattice_x, & + p % coord(j + 1) % lattice_y, & + p % coord(j + 1) % lattice_z) + end if + end if + if (t % filters(i) % int_bins(1) == p % coord(j) % cell) then + matching_bins(i) = offset + 1 + exit + end if + end do + + case (FILTER_CELLBORN) + ! determine next cellborn bin + matching_bins(i) = get_next_bin(FILTER_CELLBORN, & + p % cell_born, i_tally) + + case (FILTER_SURFACE) + ! determine next surface bin + matching_bins(i) = get_next_bin(FILTER_SURFACE, & + p % surface, i_tally) + + case (FILTER_ENERGYIN) + if (t % energy_matches_groups) then + ! make sure the correct energy group is used + ! Since all groups are filters, the filter bin is the group + if (t % estimator == ESTIMATOR_TRACKLENGTH) then + matching_bins(i) = p % g + else + matching_bins(i) = p % last_g + end if + ! Tallies are ordered in increasing groups, group indices + ! however are the opposite, so switch + matching_bins(i) = energy_groups - matching_bins(i) + 1 + else + ! make sure the correct energy is used + if (t % estimator == ESTIMATOR_TRACKLENGTH) then + E = p % E + else + E = p % last_E + end if + n = t % filters(i) % n_bins + + ! check if energy of the particle is within energy bins + if (E < t % filters(i) % real_bins(1) .or. & + E > t % filters(i) % real_bins(n + 1)) then + matching_bins(i) = NO_BIN_FOUND + else + ! search to find incoming energy bin + matching_bins(i) = binary_search(t % filters(i) % real_bins, & + n + 1, E) + end if + end if + + + case (FILTER_ENERGYOUT) + if (t % energyout_matches_groups) then + ! Since all groups are filters, the filter bin is the group + matching_bins(i) = p % g + + ! Tallies are ordered in increasing groups, group indices + ! however are the opposite, so switch + matching_bins(i) = energy_groups - matching_bins(i) + 1 + else + ! determine outgoing energy bin + n = t % filters(i) % n_bins + + ! check if energy of the particle is within energy bins + if (p % E < t % filters(i) % real_bins(1) .or. & + p % E > t % filters(i) % real_bins(n + 1)) then + matching_bins(i) = NO_BIN_FOUND + else + ! search to find incoming energy bin + matching_bins(i) = binary_search(t % filters(i) % real_bins, & + n + 1, p % E) + end if + end if + + + case (FILTER_MU) + ! determine mu bin + n = t % filters(i) % n_bins + + ! check if particle is within mu bins + if (p % mu < t % filters(i) % real_bins(1) .or. & + p % mu > t % filters(i) % real_bins(n + 1)) then + matching_bins(i) = NO_BIN_FOUND + else + ! search to find mu bin + matching_bins(i) = binary_search(t % filters(i) % real_bins, & + n + 1, p % mu) + end if + + case (FILTER_POLAR) + ! make sure the correct direction vector is used + if (t % estimator == ESTIMATOR_TRACKLENGTH) then + theta = acos(p % coord(1) % uvw(3)) + else + theta = acos(p % last_uvw(3)) + end if + + ! determine polar angle bin + n = t % filters(i) % n_bins + + ! check if particle is within polar angle bins + if (theta < t % filters(i) % real_bins(1) .or. & + theta > t % filters(i) % real_bins(n + 1)) then + matching_bins(i) = NO_BIN_FOUND + else + ! search to find polar angle bin + matching_bins(i) = binary_search(t % filters(i) % real_bins, & + n + 1, theta) + end if + + case (FILTER_AZIMUTHAL) + ! make sure the correct direction vector is used + if (t % estimator == ESTIMATOR_TRACKLENGTH) then + phi = atan2(p % coord(1) % uvw(2), p % coord(1) % uvw(1)) + else + phi = atan2(p % last_uvw(2), p % last_uvw(1)) + end if + ! determine mu bin + n = t % filters(i) % n_bins + + ! check if particle is within azimuthal angle bins + if (phi < t % filters(i) % real_bins(1) .or. & + phi > t % filters(i) % real_bins(n + 1)) then + matching_bins(i) = NO_BIN_FOUND + else + ! search to find azimuthal angle bin + matching_bins(i) = binary_search(t % filters(i) % real_bins, & + n + 1, phi) + end if + + end select + + ! If the current filter didn't match, exit this subroutine + if (matching_bins(i) == NO_BIN_FOUND) then + found_bin = .false. + return + end if + + end do FILTER_LOOP + + end subroutine get_scoring_bins_mg !=============================================================================== ! SCORE_SURFACE_CURRENT tallies surface crossings in a mesh tally by manually diff --git a/src/tally_header.F90 b/src/tally_header.F90 index 7d7bb6484..09cbf286c 100644 --- a/src/tally_header.F90 +++ b/src/tally_header.F90 @@ -141,6 +141,10 @@ module tally_header ! Index for the TallyDerivative for differential tallies. integer :: deriv = NONE + + ! Multi-Group Specific Information To Enable Rapid Tallying + logical :: energy_matches_groups = .false. + logical :: energyout_matches_groups = .false. end type TallyObject end module tally_header diff --git a/src/track_output.F90 b/src/track_output.F90 index 1665ac25e..141173862 100644 --- a/src/track_output.F90 +++ b/src/track_output.F90 @@ -7,8 +7,8 @@ module track_output use global use hdf5_interface - use particle_header, only: Particle - use string, only: to_str + use particle_header, only: Particle + use string, only: to_str use hdf5 diff --git a/src/tracking.F90 b/src/tracking.F90 index de2c54a75..d25019759 100644 --- a/src/tracking.F90 +++ b/src/tracking.F90 @@ -1,23 +1,25 @@ module tracking - use constants, only: MODE_EIGENVALUE - use cross_section, only: calculate_xs - use error, only: fatal_error, warning - use geometry, only: find_cell, distance_to_boundary, cross_surface, & - cross_lattice, check_cell_overlap - use geometry_header, only: Universe, BASE_UNIVERSE + use constants, only: MODE_EIGENVALUE + use cross_section, only: calculate_xs + use error, only: fatal_error, warning + use geometry, only: find_cell, distance_to_boundary, cross_surface, & + cross_lattice, check_cell_overlap + use geometry_header, only: Universe, BASE_UNIVERSE use global - use output, only: write_message - use particle_header, only: LocalCoord, Particle - use physics, only: collision - use random_lcg, only: prn - use string, only: to_str + use macroxs_header, only: MacroXS + use output, only: write_message + use particle_header, only: LocalCoord, Particle + use physics, only: collision + use physics_mg, only: collision_mg + use random_lcg, only: prn + use string, only: to_str + use track_output, only: initialize_particle_track, write_particle_track, & + add_particle_track, finalize_particle_track use tally, only: score_analog_tally, score_tracklength_tally, & score_collision_tally, score_surface_current, & score_track_derivative, & score_collision_derivative, zero_flux_derivs - use track_output, only: initialize_particle_track, write_particle_track, & - add_particle_track, finalize_particle_track implicit none @@ -55,7 +57,9 @@ contains total_weight = total_weight + p % wgt ! Force calculation of cross-sections by setting last energy to zero - micro_xs % last_E = ZERO + if (run_CE) then + micro_xs % last_E = ZERO + end if ! Prepare to write out particle track. if (p % write_track) then @@ -84,11 +88,24 @@ contains if (check_overlaps) call check_cell_overlap(p) - ! Calculate microscopic and macroscopic cross sections -- note: if the - ! material is the same as the last material and the energy of the - ! particle hasn't changed, we don't need to lookup cross sections again. - - if (p % material /= p % last_material) call calculate_xs(p) + ! Calculate microscopic and macroscopic cross sections + if (run_CE) then + ! If the material is the same as the last material and the energy of the + ! particle hasn't changed, we don't need to lookup cross sections again. + if (p % material /= p % last_material) call calculate_xs(p) + else + ! Since the MGXS can be angle dependent, this needs to be done + ! After every collision for the MGXS mode + if (p % material /= MATERIAL_VOID) then + call macro_xs(p % material) % obj % calculate_xs(p % g, & + p % coord(p % n_coord) % uvw, material_xs) + else + material_xs % total = ZERO + material_xs % elastic = ZERO + material_xs % absorption = ZERO + material_xs % nu_fission = ZERO + end if + end if ! Find the distance to the nearest boundary call distance_to_boundary(p, d_boundary, surface_crossed, & @@ -110,8 +127,10 @@ contains end do ! Score track-length tallies - if (active_tracklength_tallies % size() > 0) & - call score_tracklength_tally(p, distance) + if (active_tracklength_tallies % size() > 0) then + call score_tracklength_tally(p, distance) + end if + ! Score track-length estimate of k-eff if (run_mode == MODE_EIGENVALUE) then @@ -159,12 +178,15 @@ contains ! Clear surface component p % surface = NONE - call collision(p) + if (run_CE) then + call collision(p) + else + call collision_mg(p) + end if ! Score collision estimator tallies -- this is done after a collision ! has occurred rather than before because we need information on the ! outgoing energy for any tallies with an outgoing energy filter - if (active_collision_tallies % size() > 0) call score_collision_tally(p) if (active_analog_tallies % size() > 0) call score_analog_tally(p) @@ -211,7 +233,8 @@ contains ! Check for secondary particles if this particle is dead if (.not. p % alive) then if (p % n_secondary > 0) then - call p % initialize_from_source(p % secondary_bank(p % n_secondary)) + call p % initialize_from_source(p % secondary_bank(p % n_secondary), & + run_CE, energy_bin_avg) p % n_secondary = p % n_secondary - 1 n_event = 0 diff --git a/src/trigger.F90 b/src/trigger.F90 index 73cb0c7ef..ed362154b 100644 --- a/src/trigger.F90 +++ b/src/trigger.F90 @@ -6,12 +6,12 @@ module trigger use constants use global - use string, only: to_str - use output, only: warning, write_message - use mesh, only: mesh_indices_to_bin - use mesh_header, only: RegularMesh - use trigger_header, only: TriggerObject - use tally, only: TallyObject + use string, only: to_str + use output, only: warning, write_message + use mesh, only: mesh_indices_to_bin + use mesh_header, only: RegularMesh + use trigger_header, only: TriggerObject + use tally, only: TallyObject implicit none diff --git a/src/urr_header.F90 b/src/urr_header.F90 new file mode 100644 index 000000000..96e182d2e --- /dev/null +++ b/src/urr_header.F90 @@ -0,0 +1,20 @@ +module urr_header + + implicit none + +!=============================================================================== +! URRDATA contains probability tables for the unresolved resonance range. +!=============================================================================== + + type UrrData + integer :: n_energy ! # of incident neutron energies + integer :: n_prob ! # of probabilities + integer :: interp ! inteprolation (2=lin-lin, 5=log-log) + integer :: inelastic_flag ! inelastic competition flag + integer :: absorption_flag ! other absorption flag + logical :: multiply_smooth ! multiply by smooth cross section? + real(8), allocatable :: energy(:) ! incident energies + real(8), allocatable :: prob(:,:,:) ! actual probabibility tables + end type UrrData + +end module urr_header diff --git a/tests/1d_mgxs.xml b/tests/1d_mgxs.xml new file mode 100644 index 000000000..33b20464b --- /dev/null +++ b/tests/1d_mgxs.xml @@ -0,0 +1,9859 @@ + + + 1 + 0.0000000E+00 2.0000000E+01 + + + uo2_iso.71c + uo2_iso.71c + 2.5300000E-08 + 5 + true + isotropic + + 4.1022364E-01 + + + 3.4687432E-02 + + + 4.9631431E-02 + + + 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1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + 1.0000000E+00 + + + + + \ No newline at end of file diff --git a/tests/input_set.py b/tests/input_set.py index c13a4f9cc..daff38ba1 100644 --- a/tests/input_set.py +++ b/tests/input_set.py @@ -572,3 +572,92 @@ class InputSet(object): plot.color = 'mat' self.plots.add_plot(plot) + +class MGInputSet(InputSet): + def build_default_materials_and_geometry(self): + # Define materials needed for 1D/1G slab problem + uo2_data = openmc.Macroscopic('uo2_iso', '71c') + uo2 = openmc.Material(name='UO2', material_id=1) + uo2.set_density('macro', 1.0) + uo2.add_macroscopic(uo2_data) + + clad_data = openmc.Macroscopic('clad_ang_mu', '71c') + clad = openmc.Material(name='Clad', material_id=2) + clad.set_density('macro', 1.0) + clad.add_macroscopic(clad_data) + + water_data = openmc.Macroscopic('lwtr_iso_mu', '71c') + water = openmc.Material(name='LWTR', material_id=3) + water.set_density('macro', 1.0) + water.add_macroscopic(water_data) + + # Define the materials file. + self.materials.default_xs = '71c' + self.materials.add_materials((uo2, clad, water)) + + # Define surfaces. + + # Assembly/Problem Boundary + left = openmc.XPlane(x0=0.0, surface_id=200, + boundary_type='reflective') + right = openmc.XPlane(x0=10.0, surface_id=201, + boundary_type='reflective') + bottom = openmc.YPlane(y0=0.0, surface_id=300, + boundary_type='reflective') + top = openmc.YPlane(y0=10.0, surface_id=301, + boundary_type='reflective') + + down = openmc.ZPlane(z0=0.0, surface_id=0, + boundary_type='reflective') + fuel_clad_intfc = openmc.ZPlane(z0=2.0, surface_id=1) + clad_lwtr_intfc = openmc.ZPlane(z0=2.4, surface_id=2) + up = openmc.ZPlane(z0=5.0, surface_id=3, + boundary_type='reflective') + + # Define cells + c1 = openmc.Cell(cell_id=1) + c1.region = +left & -right & +bottom & -top & +down & -fuel_clad_intfc + c1.fill = uo2 + c2 = openmc.Cell(cell_id=2) + c2.region = +left & -right & +bottom & -top & +fuel_clad_intfc & -clad_lwtr_intfc + c2.fill = clad + c3 = openmc.Cell(cell_id=3) + c3.region = +left & -right & +bottom & -top & +clad_lwtr_intfc & -up + c3.fill = water + + # Define root universe. + root = openmc.Universe(universe_id=0, name='root universe') + + root.add_cells((c1,c2,c3)) + + # Define the geometry file. + geometry = openmc.Geometry() + geometry.root_universe = root + + self.geometry.geometry = geometry + + + def build_default_settings(self): + self.settings.batches = 10 + self.settings.inactive = 5 + self.settings.particles = 100 + self.settings.source = Source(space=Box([0.0, 0.0, 0.0], + [10.0, 10.0, 2.0])) + self.settings.energy_mode = "multi-group" + self.settings.cross_sections = "../1d_mgxs.xml" + + def build_defualt_plots(self): + plot = openmc.Plot() + plot.filename = 'mat' + plot.origin = (5.0, 5.0, 2.5) + plot.width = (2.5, 2.5) + plot.basis = 'xz' + plot.pixels = (3000, 3000) + plot.color = 'mat' + + self.plots.add_plot(plot) + + + + + diff --git a/tests/run_tests.py b/tests/run_tests.py index 48fc23d4a..5a04f340a 100755 --- a/tests/run_tests.py +++ b/tests/run_tests.py @@ -300,9 +300,12 @@ if options.list_build_configs: # Delete items of dictionary that don't match regular expression if options.build_config is not None: + to_delete = [] for key in tests: if not re.search(options.build_config, key): - del tests[key] + to_delete.append(key) + for key in to_delete: + del tests[key] # Check for dashboard and determine whether to push results to server # Note that there are only 3 basic dashboards: @@ -363,10 +366,14 @@ sourcepoint_batch|statepoint_interval|survival_biasing|\ tally_assumesep|translation|uniform_fs|universe|void" # Delete items of dictionary if valgrind or coverage and not in script mode +to_delete = [] if not script_mode: for key in tests: if re.search('valgrind|coverage', key): - del tests[key] + to_delete.append(key) + +for key in to_delete: + del tests[key] # Check if tests empty if len(list(tests.keys())) == 0: diff --git a/tests/test_asymmetric_lattice/results_true.dat b/tests/test_asymmetric_lattice/results_true.dat index ec4b88388..a33b9c9e5 100644 --- a/tests/test_asymmetric_lattice/results_true.dat +++ b/tests/test_asymmetric_lattice/results_true.dat @@ -1 +1 @@ -b5f96919ca474cd1c9c9d0acde3b8aac4a1cf636443c72a38b6c5a4221a8ce3e90182aaef2f664e44b9175ca257a89db2328b63e19388ee0e5006de4b3d92ce6 \ No newline at end of file +bc8bef8121f9b6470e4fea817a4e48eabb1ecba1f42761a4cbd77d71181bf9e1612df4a3d6ddfbcd08a3086ac873e5f3c3e560bf96b2b7c959a2f7aad7e4e08d \ No newline at end of file diff --git a/tests/test_asymmetric_lattice/test_asymmetric_lattice.py b/tests/test_asymmetric_lattice/test_asymmetric_lattice.py index 5a1d47ef8..fdb21db33 100644 --- a/tests/test_asymmetric_lattice/test_asymmetric_lattice.py +++ b/tests/test_asymmetric_lattice/test_asymmetric_lattice.py @@ -19,13 +19,10 @@ class AsymmetricLatticeTestHarness(PyAPITestHarness): # Build full core geometry from underlying input set self._input_set.build_default_materials_and_geometry() - # Extract all universes from the full core geometry - geometry = self._input_set.geometry.geometry - all_univs = geometry.get_all_universes() - # Extract universes encapsulating fuel and water assemblies - water = all_univs[7] - fuel = all_univs[8] + geometry = self._input_set.geometry.geometry + water = geometry.get_universes_by_name('water assembly (hot)')[0] + fuel = geometry.get_universes_by_name('fuel assembly (hot)')[0] # Construct a 3x3 lattice of fuel assemblies core_lat = openmc.RectLattice(name='3x3 Core Lattice', lattice_id=202) @@ -102,9 +99,10 @@ class AsymmetricLatticeTestHarness(PyAPITestHarness): outstr += ', '.join(map(str, tally.std_dev.flatten())) + '\n' # Extract fuel assembly lattices from the summary - all_cells = su.openmc_geometry.get_all_cells() - fuel = all_cells[80].fill - core = all_cells[1].fill + core = su.get_cell_by_id(1) + fuel = su.get_cell_by_id(80) + fuel = fuel.fill + core = core.fill # Append a string of lattice distribcell offsets to the string outstr += ', '.join(map(str, fuel.offsets.flatten())) + '\n' diff --git a/tests/test_cmfd_feed/results_true.dat b/tests/test_cmfd_feed/results_true.dat index 9c109db6a..4579fa545 100644 --- a/tests/test_cmfd_feed/results_true.dat +++ b/tests/test_cmfd_feed/results_true.dat @@ -1,128 +1,128 @@ k-combined: -1.168349E+00 1.145333E-02 +1.169891E+00 6.289481E-03 tally 1: -1.167844E+01 -1.366808E+01 -2.141846E+01 -4.598143E+01 -2.928738E+01 -8.615095E+01 -3.513015E+01 -1.241914E+02 -3.715164E+01 -1.384553E+02 -3.639309E+01 -1.327919E+02 -3.370872E+01 -1.138391E+02 -2.875251E+01 -8.292323E+01 -2.117740E+01 -4.512961E+01 -1.130554E+01 -1.289872E+01 +1.173921E+01 +1.385460E+01 +2.164076E+01 +4.699369E+01 +2.906462E+01 +8.464935E+01 +3.382312E+01 +1.147095E+02 +3.632006E+01 +1.323878E+02 +3.655412E+01 +1.341064E+02 +3.347756E+01 +1.124264E+02 +2.931337E+01 +8.607243E+01 +2.182947E+01 +4.789563E+01 +1.147668E+01 +1.325716E+01 tally 2: -2.339531E+01 -2.755922E+01 -1.646762E+01 -1.365289E+01 -2.146174E+00 -2.369613E-01 -4.309769E+01 -9.312913E+01 -3.054873E+01 -4.681242E+01 -4.076365E+00 -8.462370E-01 -5.840647E+01 -1.715260E+02 -4.161366E+01 -8.713062E+01 -5.382541E+00 -1.473814E+00 -6.927641E+01 -2.411359E+02 -4.943841E+01 -1.228850E+02 -6.282202E+00 -1.990021E+00 -7.308593E+01 -2.678848E+02 -5.202069E+01 -1.357621E+02 -6.826145E+00 -2.353974E+00 -7.117026E+01 -2.543546E+02 -5.068896E+01 -1.290261E+02 -6.342979E+00 -2.033850E+00 -6.615720E+01 -2.193712E+02 -4.725156E+01 -1.119514E+02 -6.024815E+00 -1.833752E+00 -5.738164E+01 -1.651944E+02 -4.081217E+01 -8.360122E+01 -5.326191E+00 -1.435896E+00 -4.208669E+01 -8.911740E+01 -2.994944E+01 -4.517409E+01 -3.905846E+00 -7.855247E-01 -2.273578E+01 -2.615080E+01 -1.603853E+01 -1.303560E+01 -2.160924E+00 -2.473278E-01 +2.298190E+01 +2.667071E+01 +1.600292E+01 +1.293670E+01 +2.252427E+00 +2.605738E-01 +4.268506E+01 +9.161215E+01 +3.022909E+01 +4.598915E+01 +3.873926E+00 +7.615035E-01 +5.680399E+01 +1.623878E+02 +4.033805E+01 +8.196263E+01 +5.280610E+00 +1.414008E+00 +6.814741E+01 +2.331778E+02 +4.851618E+01 +1.182330E+02 +6.261805E+00 +1.983205E+00 +7.392922E+01 +2.740255E+02 +5.253586E+01 +1.384152E+02 +6.733810E+00 +2.278242E+00 +7.332860E+01 +2.698608E+02 +5.227405E+01 +1.371810E+02 +6.714658E+00 +2.273652E+00 +6.830172E+01 +2.340687E+02 +4.867159E+01 +1.188724E+02 +6.215002E+00 +1.956978E+00 +5.885634E+01 +1.736180E+02 +4.170434E+01 +8.719622E+01 +5.253064E+00 +1.396224E+00 +4.372001E+01 +9.593570E+01 +3.106511E+01 +4.844647E+01 +3.817991E+00 +7.509063E-01 +2.338260E+01 +2.752103E+01 +1.636606E+01 +1.347591E+01 +2.220013E+00 +2.515671E-01 tally 3: -1.584939E+01 -1.265206E+01 -1.096930E+00 -6.173135E-02 -2.940258E+01 -4.337818E+01 -1.932931E+00 -1.884749E-01 -4.008186E+01 -8.086427E+01 -2.512704E+00 -3.189987E-01 -4.759648E+01 -1.139252E+02 -3.041630E+00 -4.683237E-01 -5.006181E+01 -1.257467E+02 -3.137042E+00 -4.981005E-01 -4.883211E+01 -1.197646E+02 -3.130686E+00 -4.987337E-01 -4.550029E+01 -1.038199E+02 -2.853740E+00 -4.127265E-01 -3.937822E+01 -7.785807E+01 -2.488983E+00 -3.156421E-01 -2.884912E+01 -4.192640E+01 -1.855316E+00 -1.745109E-01 -1.543635E+01 -1.208459E+01 -1.025635E+00 -5.351565E-02 +1.538752E+01 +1.196478E+01 +1.079685E+00 +6.010786E-02 +2.911906E+01 +4.269070E+01 +1.822657E+00 +1.671851E-01 +3.885421E+01 +7.608218E+01 +2.541517E+00 +3.262452E-01 +4.673300E+01 +1.097036E+02 +2.885308E+00 +4.214444E-01 +5.059247E+01 +1.283984E+02 +3.222797E+00 +5.237329E-01 +5.034856E+01 +1.272538E+02 +3.230225E+00 +5.273425E-01 +4.688476E+01 +1.103152E+02 +2.941287E+00 +4.363750E-01 +4.013746E+01 +8.077506E+01 +2.634234E+00 +3.520271E-01 +2.996995E+01 +4.510282E+01 +1.946504E+00 +1.919104E-01 +1.575153E+01 +1.248536E+01 +1.020705E+00 +5.413570E-02 tally 4: 0.000000E+00 0.000000E+00 @@ -160,8 +160,8 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -3.119914E+00 -4.908283E-01 +3.049469E+00 +4.677325E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -208,10 +208,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -5.567786E+00 -1.556825E+00 -2.766088E+00 -3.864023E-01 +5.514939E+00 +1.528899E+00 +2.770358E+00 +3.879191E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -256,10 +256,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -7.491891E+00 -2.819491E+00 -5.235154E+00 -1.377898E+00 +7.294002E+00 +2.675589E+00 +5.032131E+00 +1.275040E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -304,10 +304,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -8.810357E+00 -3.898704E+00 -7.233068E+00 -2.630659E+00 +8.668860E+00 +3.776102E+00 +7.036008E+00 +2.490719E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -352,10 +352,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -9.374583E+00 -4.414420E+00 -8.565683E+00 -3.687428E+00 +9.345868E+00 +4.380719E+00 +8.352414E+00 +3.501945E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -400,10 +400,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -9.001252E+00 -4.073267E+00 -8.974821E+00 -4.050120E+00 +9.223771E+00 +4.270119E+00 +9.093766E+00 +4.158282E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -448,10 +448,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -8.236452E+00 -3.401934E+00 -9.042286E+00 -4.102906E+00 +8.530966E+00 +3.651778E+00 +9.219150E+00 +4.264346E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -496,10 +496,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -7.028546E+00 -2.482380E+00 -8.577643E+00 -3.691947E+00 +7.204424E+00 +2.604203E+00 +8.690373E+00 +3.785262E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -544,10 +544,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -5.159585E+00 -1.342512E+00 -7.389236E+00 -2.745028E+00 +5.326721E+00 +1.426975E+00 +7.513640E+00 +2.833028E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -592,10 +592,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -2.762685E+00 -3.914181E-01 -5.471849E+00 -1.509910E+00 +2.847310E+00 +4.090440E-01 +5.661144E+00 +1.607138E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -642,8 +642,8 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -3.038522E+00 -4.643520E-01 +3.025812E+00 +4.597241E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -662,114 +662,114 @@ k cmfd 0.000000E+00 0.000000E+00 0.000000E+00 -1.180802E+00 -1.162698E+00 -1.162794E+00 -1.159752E+00 -1.152596E+00 -1.151652E+00 -1.148131E+00 -1.151875E+00 -1.151434E+00 -1.158833E+00 -1.160751E+00 -1.155305E+00 -1.155356E+00 -1.158866E+00 -1.161574E+00 -1.154691E+00 +1.170416E+00 +1.172966E+00 +1.165537E+00 +1.170979E+00 +1.161922E+00 +1.157523E+00 +1.158873E+00 +1.162877E+00 +1.167102E+00 +1.168130E+00 +1.170570E+00 +1.168115E+00 +1.174081E+00 +1.169458E+00 +1.167848E+00 +1.165116E+00 cmfd entropy 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -3.214195E+00 -3.225164E+00 -3.227316E+00 -3.225663E+00 -3.226390E+00 -3.225832E+00 -3.226707E+00 -3.227866E+00 -3.229948E+00 -3.229269E+00 -3.230044E+00 -3.231568E+00 -3.234694E+00 -3.234771E+00 -3.234915E+00 -3.235876E+00 +3.203643E+00 +3.207943E+00 +3.213367E+00 +3.214360E+00 +3.219634E+00 +3.222232E+00 +3.221744E+00 +3.224544E+00 +3.225990E+00 +3.227769E+00 +3.227417E+00 +3.230728E+00 +3.231662E+00 +3.233316E+00 +3.233193E+00 +3.232564E+00 cmfd balance 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -4.742525E-03 -2.646417E-03 -1.981783E-03 -1.856593E-03 -1.797685E-03 -2.122587E-03 -1.200823E-03 -2.177249E-03 -1.442840E-03 -1.477754E-03 -1.236325E-03 -1.048988E-03 -8.395164E-04 -7.380254E-04 -7.742837E-04 -8.235911E-04 +4.009063E-03 +4.431773E-03 +3.152698E-03 +3.510424E-03 +2.052087E-03 +2.068633E-03 +1.502416E-03 +1.589822E-03 +1.566016E-03 +1.219159E-03 +1.017888E-03 +9.771569E-04 +1.010126E-03 +1.073397E-03 +1.172784E-03 +9.827488E-04 cmfd dominance ratio 0.000E+00 0.000E+00 0.000E+00 0.000E+00 - 5.467E-01 - 5.518E-01 - 5.535E-01 - 5.500E-01 + 5.397E-01 + 5.425E-01 5.481E-01 - 5.478E-01 - 5.467E-01 - 5.465E-01 - 5.493E-01 - 5.488E-01 - 5.491E-01 + 5.473E-01 5.503E-01 - 5.529E-01 - 5.531E-01 - 5.534E-01 - 5.552E-01 + 5.502E-01 + 5.483E-01 + 5.520E-01 + 5.505E-01 + 3.216E-01 + 5.373E-01 + 5.517E-01 + 5.508E-01 + 5.524E-01 + 5.524E-01 + 5.523E-01 cmfd openmc source comparison 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -9.168094E-03 -5.978693E-03 -4.369223E-03 -4.546309E-03 -4.222522E-03 -4.221686E-03 -4.604208E-03 -3.950286E-03 -2.939283E-03 -3.667020E-03 -2.592899E-03 -2.272158E-03 -1.229170E-03 -1.114150E-03 -1.060490E-03 -1.714222E-03 +6.959835E-03 +5.655657E-03 +3.886178E-03 +4.035110E-03 +3.043277E-03 +5.455479E-03 +4.515313E-03 +2.439842E-03 +2.114036E-03 +2.673135E-03 +2.431753E-03 +4.330931E-03 +3.404650E-03 +3.680302E-03 +3.309625E-03 +3.705544E-03 cmfd source -4.724285E-02 -8.305825E-02 -1.081058E-01 -1.314542E-01 -1.357299E-01 -1.359417E-01 -1.240918E-01 -1.087580E-01 -8.111239E-02 -4.450518E-02 +4.697085E-02 +7.920706E-02 +1.107968E-01 +1.250932E-01 +1.383930E-01 +1.380648E-01 +1.246874E-01 +1.113705E-01 +8.203754E-02 +4.337882E-02 diff --git a/tests/test_cmfd_nofeed/results_true.dat b/tests/test_cmfd_nofeed/results_true.dat index 308dd7d82..d8a17d676 100644 --- a/tests/test_cmfd_nofeed/results_true.dat +++ b/tests/test_cmfd_nofeed/results_true.dat @@ -1,128 +1,128 @@ k-combined: -1.171115E+00 6.173328E-03 +1.167381E+00 9.433736E-03 tally 1: -1.151618E+01 -1.331859E+01 -2.120660E+01 -4.514836E+01 -2.759616E+01 -7.639131E+01 -3.216668E+01 -1.036501E+02 -3.664720E+01 -1.345450E+02 -3.771246E+01 -1.424209E+02 -3.523750E+01 -1.245225E+02 -2.973298E+01 -8.860064E+01 -2.152108E+01 -4.647187E+01 -1.169538E+01 -1.375047E+01 +1.196136E+01 +1.442468E+01 +2.133857E+01 +4.600706E+01 +2.874353E+01 +8.287538E+01 +3.400779E+01 +1.158949E+02 +3.736443E+01 +1.398466E+02 +3.705095E+01 +1.376767E+02 +3.486173E+01 +1.220362E+02 +2.910935E+01 +8.507181E+01 +2.034762E+01 +4.156717E+01 +1.074970E+01 +1.160733E+01 tally 2: -2.274639E+01 -2.606952E+01 -1.588200E+01 -1.270445E+01 -2.140989E+00 -2.357207E-01 -4.205792E+01 -8.880940E+01 -2.970000E+01 -4.427086E+01 -3.919645E+00 -7.773724E-01 -5.560960E+01 -1.559764E+02 -3.947900E+01 -7.872700E+01 -5.238942E+00 -1.400918E+00 -6.492259E+01 -2.117369E+02 -4.612200E+01 -1.069035E+02 -5.989449E+00 -1.813201E+00 -7.217377E+01 -2.608499E+02 -5.148500E+01 -1.327923E+02 -6.607336E+00 -2.205529E+00 -7.305896E+01 -2.681514E+02 -5.187500E+01 -1.352457E+02 -6.722921E+00 -2.290262E+00 -6.884269E+01 -2.380550E+02 -4.904800E+01 -1.208314E+02 -6.177320E+00 -1.927173E+00 -5.902100E+01 -1.748370E+02 -4.201000E+01 -8.858460E+01 -5.542381E+00 -1.549108E+00 -4.268091E+01 -9.151405E+01 -3.029500E+01 -4.614050E+01 -3.822093E+00 -7.420139E-01 -2.362279E+01 -2.812041E+01 -1.653100E+01 -1.377737E+01 -2.336090E+00 -2.851840E-01 +2.321994E+01 +2.726751E+01 +1.624000E+01 +1.334217E+01 +2.239367E+00 +2.607315E-01 +4.184801E+01 +8.813953E+01 +2.955600E+01 +4.401685E+01 +3.937924E+00 +7.877545E-01 +5.620223E+01 +1.589242E+02 +3.981400E+01 +7.983679E+01 +5.183337E+00 +1.367303E+00 +6.834724E+01 +2.342244E+02 +4.869600E+01 +1.189597E+02 +6.288549E+00 +1.997858E+00 +7.481522E+01 +2.802998E+02 +5.346500E+01 +1.431835E+02 +6.691123E+00 +2.252645E+00 +7.381412E+01 +2.733775E+02 +5.269700E+01 +1.393729E+02 +6.846095E+00 +2.360683E+00 +6.907775E+01 +2.396751E+02 +4.918500E+01 +1.215909E+02 +6.400076E+00 +2.073871E+00 +5.783260E+01 +1.680814E+02 +4.107800E+01 +8.480751E+01 +5.269220E+00 +1.404986E+00 +4.120212E+01 +8.516646E+01 +2.930300E+01 +4.310295E+01 +3.730803E+00 +7.015777E-01 +2.228419E+01 +2.504033E+01 +1.554100E+01 +1.217931E+01 +2.126451E+00 +2.315275E-01 tally 3: -1.524100E+01 -1.171023E+01 -1.071050E+00 -5.839198E-02 -2.862800E+01 -4.113148E+01 -1.892774E+00 -1.812712E-01 -3.804600E+01 -7.316097E+01 -2.423654E+00 -2.968521E-01 -4.434600E+01 -9.882906E+01 -2.823929E+00 -4.033633E-01 -4.955300E+01 -1.230293E+02 -3.226029E+00 -5.265680E-01 -4.999400E+01 -1.256474E+02 -3.232464E+00 -5.286388E-01 -4.724300E+01 -1.121029E+02 -3.015553E+00 -4.606928E-01 -4.051300E+01 -8.239672E+01 -2.592073E+00 -3.412174E-01 -2.912700E+01 -4.265700E+01 -1.875109E+00 -1.785438E-01 -1.593500E+01 -1.280638E+01 -1.038638E+00 -5.538157E-02 +1.561100E+01 +1.233967E+01 +1.095984E+00 +6.181387E-02 +2.847800E+01 +4.088161E+01 +1.815210E+00 +1.669969E-01 +3.834200E+01 +7.408022E+01 +2.446117E+00 +3.017834E-01 +4.687600E+01 +1.102381E+02 +2.954924E+00 +4.412809E-01 +5.155100E+01 +1.331461E+02 +3.204714E+00 +5.178544E-01 +5.067700E+01 +1.289238E+02 +3.246710E+00 +5.326374E-01 +4.738600E+01 +1.128834E+02 +3.035962E+00 +4.640211E-01 +3.953600E+01 +7.858196E+01 +2.507574E+00 +3.186456E-01 +2.819300E+01 +3.991455E+01 +1.846612E+00 +1.725570E-01 +1.497500E+01 +1.131312E+01 +9.213728E-01 +4.422001E-02 tally 4: 0.000000E+00 0.000000E+00 @@ -160,8 +160,8 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -3.065000E+00 -4.742170E-01 +3.090000E+00 +4.810640E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -208,10 +208,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -5.420000E+00 -1.474674E+00 -2.693000E+00 -3.667090E-01 +5.555000E+00 +1.551579E+00 +2.833000E+00 +4.078910E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -256,10 +256,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -7.243000E+00 -2.637431E+00 -5.092000E+00 -1.305200E+00 +7.271000E+00 +2.659755E+00 +5.095000E+00 +1.310819E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -304,10 +304,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -8.280000E+00 -3.445670E+00 -6.765000E+00 -2.307253E+00 +8.577000E+00 +3.703215E+00 +7.026000E+00 +2.486552E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -352,10 +352,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -8.980000E+00 -4.046484E+00 -8.108000E+00 -3.299338E+00 +9.393000E+00 +4.422429E+00 +8.572000E+00 +3.680852E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -400,10 +400,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -9.016000E+00 -4.079320E+00 -8.962000E+00 -4.034032E+00 +9.265000E+00 +4.305625E+00 +9.261000E+00 +4.304411E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -448,10 +448,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -8.465000E+00 -3.595665E+00 -9.296000E+00 -4.340524E+00 +8.535000E+00 +3.659395E+00 +9.303000E+00 +4.350791E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -496,10 +496,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -7.247000E+00 -2.638527E+00 -8.865000E+00 -3.946315E+00 +7.104000E+00 +2.544182E+00 +8.693000E+00 +3.799545E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -544,10 +544,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -5.179000E+00 -1.353661E+00 -7.492000E+00 -2.817588E+00 +5.168000E+00 +1.344390E+00 +7.334000E+00 +2.700052E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -592,10 +592,10 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -2.821000E+00 -4.067990E-01 -5.617000E+00 -1.587757E+00 +2.724000E+00 +3.745680E-01 +5.416000E+00 +1.471086E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -642,8 +642,8 @@ tally 4: 0.000000E+00 0.000000E+00 0.000000E+00 -3.134000E+00 -4.937920E-01 +2.960000E+00 +4.397840E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -662,114 +662,114 @@ k cmfd 0.000000E+00 0.000000E+00 0.000000E+00 -1.180802E+00 -1.163440E+00 -1.148572E+00 -1.151423E+00 -1.143374E+00 -1.144091E+00 -1.146212E+00 -1.144900E+00 -1.153511E+00 -1.158766E+00 -1.159179E+00 -1.156627E+00 -1.160647E+00 -1.162860E+00 -1.164312E+00 -1.164928E+00 +1.170416E+00 +1.172572E+00 +1.171159E+00 +1.170281E+00 +1.159698E+00 +1.151967E+00 +1.146706E+00 +1.147137E+00 +1.152154E+00 +1.156980E+00 +1.156370E+00 +1.155975E+00 +1.155295E+00 +1.154881E+00 +1.153714E+00 +1.159485E+00 cmfd entropy 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -3.214195E+00 -3.222259E+00 -3.225989E+00 -3.230436E+00 -3.228875E+00 -3.229003E+00 -3.228502E+00 -3.230397E+00 -3.231417E+00 -3.231192E+00 -3.229995E+00 -3.229396E+00 -3.228730E+00 -3.228091E+00 -3.227600E+00 -3.229723E+00 +3.203643E+00 +3.204555E+00 +3.210935E+00 +3.213980E+00 +3.219204E+00 +3.222234E+00 +3.226210E+00 +3.226808E+00 +3.224445E+00 +3.222460E+00 +3.222458E+00 +3.222447E+00 +3.220832E+00 +3.220841E+00 +3.221580E+00 +3.220523E+00 cmfd balance 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -4.742525E-03 -3.110598E-03 -2.490108E-03 -2.114137E-03 -2.190200E-03 -3.281877E-03 -2.219193E-03 -2.458372E-03 -2.200863E-03 -2.181858E-03 -2.064212E-03 -1.961178E-03 -1.713250E-03 -1.665361E-03 -1.436016E-03 -1.193462E-03 +4.009063E-03 +4.869662E-03 +2.997290E-03 +2.711191E-03 +1.688329E-03 +1.855396E-03 +1.403977E-03 +1.398430E-03 +1.818402E-03 +1.761252E-03 +1.646650E-03 +1.480120E-03 +1.399560E-03 +1.400162E-03 +1.178362E-03 +1.292279E-03 cmfd dominance ratio 0.000E+00 0.000E+00 0.000E+00 0.000E+00 - 5.467E-01 - 5.505E-01 - 5.514E-01 + 5.397E-01 + 5.405E-01 + 5.412E-01 + 5.428E-01 + 5.460E-01 + 4.531E-01 + 5.528E-01 5.531E-01 - 5.529E-01 - 5.501E-01 - 5.484E-01 - 5.500E-01 - 5.506E-01 - 5.508E-01 - 5.504E-01 - 5.500E-01 - 5.480E-01 - 5.482E-01 - 5.475E-01 5.493E-01 + 5.468E-01 + 5.482E-01 + 5.487E-01 + 5.471E-01 + 5.465E-01 + 5.461E-01 + 5.443E-01 cmfd openmc source comparison 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -9.168094E-03 -5.976241E-03 -4.426550E-03 -4.107499E-03 -4.957716E-03 -4.026213E-03 -3.986000E-03 -2.702714E-03 -3.619345E-03 -4.909616E-03 -3.355042E-03 -2.945724E-03 -3.010811E-03 -2.965662E-03 -2.673073E-03 -1.669634E-03 +6.959835E-03 +5.494668E-03 +4.076255E-03 +4.451120E-03 +3.035589E-03 +3.391773E-03 +1.907995E-03 +2.482495E-03 +2.994917E-03 +3.104683E-03 +2.309343E-03 +2.151358E-03 +2.348850E-03 +1.976731E-03 +2.080638E-03 +2.301327E-03 cmfd source -4.539734E-02 -8.104913E-02 -1.045143E-01 -1.221516E-01 -1.398002E-01 -1.400323E-01 -1.304628E-01 -1.120006E-01 -8.038230E-02 -4.420934E-02 +4.638920E-02 +7.751172E-02 +1.056089E-01 +1.282509E-01 +1.396713E-01 +1.415740E-01 +1.323405E-01 +1.092839E-01 +7.981779E-02 +3.955174E-02 diff --git a/tests/test_complex_cell/results_true.dat b/tests/test_complex_cell/results_true.dat index 97f228e3e..da3acd2aa 100644 --- a/tests/test_complex_cell/results_true.dat +++ b/tests/test_complex_cell/results_true.dat @@ -1,11 +1,11 @@ k-combined: -2.565769E-01 8.980879E-04 +2.531110E-01 3.041974E-03 tally 1: -2.584080E+00 -1.335682E+00 -2.763580E+00 -1.528633E+00 -1.007148E+00 -2.031543E-01 -1.113696E-01 -2.485351E-03 +2.594626E+00 +1.346701E+00 +2.683653E+00 +1.440725E+00 +9.933862E-01 +1.977011E-01 +1.112289E-01 +2.476655E-03 diff --git a/tests/test_confidence_intervals/results_true.dat b/tests/test_confidence_intervals/results_true.dat index fb13bdad2..e519180c8 100644 --- a/tests/test_confidence_intervals/results_true.dat +++ b/tests/test_confidence_intervals/results_true.dat @@ -1,5 +1,5 @@ k-combined: -2.913599E-01 6.738749E-03 +2.955487E-01 7.001017E-03 tally 1: -6.420923E+01 -5.190738E+02 +6.492201E+01 +5.290724E+02 diff --git a/tests/test_density/results_true.dat b/tests/test_density/results_true.dat index 1dbadc039..65135bbc9 100644 --- a/tests/test_density/results_true.dat +++ b/tests/test_density/results_true.dat @@ -1,2 +1,2 @@ k-combined: -1.088237E+00 1.999252E-02 +1.102244E+00 1.114944E-02 diff --git a/tests/test_distribmat/results_true.dat b/tests/test_distribmat/results_true.dat index 73a48907c..15a00ee7d 100644 --- a/tests/test_distribmat/results_true.dat +++ b/tests/test_distribmat/results_true.dat @@ -1,11 +1,10 @@ k-combined: -1.309285E+00 1.263629E-02 +1.291341E+00 1.269369E-02 Cell ID = 11 Name = Material = [2, 3, void, 2] Region = -10000 - Temperature = [ 293.60594237 293.60594237 0. 293.60594237] Rotation = None Translation = None Offset = None diff --git a/tests/test_eigenvalue_genperbatch/results_true.dat b/tests/test_eigenvalue_genperbatch/results_true.dat index 9e87c901d..846a17e08 100644 --- a/tests/test_eigenvalue_genperbatch/results_true.dat +++ b/tests/test_eigenvalue_genperbatch/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.015627E-01 5.978844E-03 +3.001412E-01 2.669737E-03 diff --git a/tests/test_eigenvalue_no_inactive/results_true.dat b/tests/test_eigenvalue_no_inactive/results_true.dat index fbbe84cc3..2b4373e7e 100644 --- a/tests/test_eigenvalue_no_inactive/results_true.dat +++ b/tests/test_eigenvalue_no_inactive/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.130246E-01 6.960311E-03 +3.080574E-01 6.889659E-03 diff --git a/tests/test_energy_grid/results_true.dat b/tests/test_energy_grid/results_true.dat index 9556a981b..0a607592c 100644 --- a/tests/test_energy_grid/results_true.dat +++ b/tests/test_energy_grid/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.155788E-01 7.559348E-03 +3.330789E-01 2.216495E-03 diff --git a/tests/test_energy_laws/results_true.dat b/tests/test_energy_laws/results_true.dat index 48eb6bc81..02465fa79 100644 --- a/tests/test_energy_laws/results_true.dat +++ b/tests/test_energy_laws/results_true.dat @@ -1,2 +1,2 @@ k-combined: -2.130076E+00 1.938907E-03 +2.122164E+00 1.946222E-02 diff --git a/tests/test_entropy/results_true.dat b/tests/test_entropy/results_true.dat index 8b37789c3..e3e0daea0 100644 --- a/tests/test_entropy/results_true.dat +++ b/tests/test_entropy/results_true.dat @@ -1,13 +1,13 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 entropy: -7.608094E+00 -8.167702E+00 -8.273634E+00 -8.239452E+00 -8.234598E+00 -8.278421E+00 -8.260773E+00 -8.351860E+00 -8.303719E+00 -8.271058E+00 +7.601626E+00 +8.085658E+00 +8.263983E+00 +8.284792E+00 +8.420379E+00 +8.302840E+00 +8.316079E+00 +8.299781E+00 +8.329297E+00 +8.361325E+00 diff --git a/tests/test_filter_distribcell/case-1/results_true.dat b/tests/test_filter_distribcell/case-1/results_true.dat index 49bf3ed4e..a1f062e1b 100644 --- a/tests/test_filter_distribcell/case-1/results_true.dat +++ b/tests/test_filter_distribcell/case-1/results_true.dat @@ -1,14 +1,14 @@ k-combined: 0.000000E+00 0.000000E+00 tally 1: -1.440759E-02 -2.075788E-04 -1.222930E-02 -1.495558E-04 -1.407292E-02 -1.980471E-04 -1.034365E-02 -1.069911E-04 +1.548980E-02 +2.399339E-04 +1.278780E-02 +1.635279E-04 +1.426319E-02 +2.034385E-04 +1.018927E-02 +1.038213E-04 tally 2: -5.105347E-02 -2.606457E-03 +5.273007E-02 +2.780460E-03 diff --git a/tests/test_filter_distribcell/case-2/results_true.dat b/tests/test_filter_distribcell/case-2/results_true.dat index bb2f498cb..4e2583f3e 100644 --- a/tests/test_filter_distribcell/case-2/results_true.dat +++ b/tests/test_filter_distribcell/case-2/results_true.dat @@ -1,11 +1,11 @@ k-combined: 0.000000E+00 0.000000E+00 tally 1: -7.326285E-03 -5.367445E-05 -8.565980E-03 -7.337601E-05 -9.027116E-03 -8.148882E-05 -8.045879E-03 -6.473617E-05 +7.588170E-03 +5.758032E-05 +8.402486E-03 +7.060177E-05 +8.682518E-03 +7.538613E-05 +8.119997E-03 +6.593435E-05 diff --git a/tests/test_filter_distribcell/case-3/results_true.dat b/tests/test_filter_distribcell/case-3/results_true.dat index f5f85d29f..32c1fced1 100644 --- a/tests/test_filter_distribcell/case-3/results_true.dat +++ b/tests/test_filter_distribcell/case-3/results_true.dat @@ -1 +1 @@ -6008cf2ba8eecaaa5a600fa337cf54cef018e98bdba8e3bd26c6f44587376a838d5bc5e86301b2e308f9eb248e3efafd45a5336f4023d962d7921d158a621e0c \ No newline at end of file +7bef4810e3bba5df56fef96d9a946dc8dc8ac136ba5282d2975456f3de8fc47ea4ba557d6c83d0938579e11e2a0da5e8e4d03b3cd1f0c0d969d25c218b2ec0bc \ No newline at end of file diff --git a/tests/test_filter_distribcell/case-4/results_true.dat b/tests/test_filter_distribcell/case-4/results_true.dat index b8bd2b339..88e78d757 100644 --- a/tests/test_filter_distribcell/case-4/results_true.dat +++ b/tests/test_filter_distribcell/case-4/results_true.dat @@ -1,17 +1,17 @@ k-combined: 0.000000E+00 0.000000E+00 tally 1: -2.166056E-02 -4.691799E-04 -2.281665E-02 -5.205994E-04 -1.938848E-02 -3.759132E-04 -3.055366E-02 -9.335264E-04 -2.338209E-02 -5.467222E-04 -2.719869E-02 -7.397689E-04 -1.895698E-02 -3.593670E-04 +2.265319E-02 +5.131669E-04 +2.026852E-02 +4.108129E-04 +2.051718E-02 +4.209546E-04 +3.015130E-02 +9.091009E-04 +2.356397E-02 +5.552606E-04 +2.558974E-02 +6.548348E-04 +2.012046E-02 +4.048330E-04 diff --git a/tests/test_filter_mesh_2d/results_true.dat b/tests/test_filter_mesh_2d/results_true.dat index 21946086b..f4c597952 100644 --- a/tests/test_filter_mesh_2d/results_true.dat +++ b/tests/test_filter_mesh_2d/results_true.dat @@ -1,5 +1,5 @@ k-combined: -1.005983E+00 2.248579E-02 +9.581522E-01 4.261830E-02 tally 1: 0.000000E+00 0.000000E+00 @@ -45,10 +45,6 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -3.228098E-02 -1.042062E-03 -3.222708E-01 -1.038585E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -57,8 +53,16 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 +1.474078E-01 +2.172907E-02 +6.386562E-02 +4.078817E-03 0.000000E+00 0.000000E+00 +2.905797E-02 +8.443654E-04 +7.532560E-03 +5.673946E-05 0.000000E+00 0.000000E+00 0.000000E+00 @@ -67,6 +71,10 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 +1.149324E-01 +1.320945E-02 +2.465048E-02 +3.049063E-04 0.000000E+00 0.000000E+00 0.000000E+00 @@ -75,14 +83,20 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -8.182335E-01 -3.748630E-01 -2.711997E-01 -5.338821E-02 -3.359680E-01 -5.168399E-02 0.000000E+00 0.000000E+00 +7.002118E-02 +4.902965E-03 +5.128548E-01 +1.258296E-01 +1.379070E+00 +4.300261E-01 +1.040956E+00 +3.089102E-01 +1.237157E+00 +6.284409E-01 +9.539296E-01 +5.206980E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -91,12 +105,30 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 +2.001407E+00 +1.600000E+00 +7.159080E-01 +2.988090E-01 0.000000E+00 0.000000E+00 -3.706070E-01 -1.373496E-01 0.000000E+00 0.000000E+00 +3.473499E-01 +1.206520E-01 +1.597805E-01 +1.297695E-02 +1.438568E-01 +1.597365E-02 +8.612279E-02 +5.910825E-03 +9.004671E-01 +2.791173E-01 +6.485841E+00 +1.046238E+01 +6.743595E+00 +1.135216E+01 +7.681046E-01 +1.896252E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -107,143 +139,40 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 +9.572791E-01 +8.942065E-01 0.000000E+00 0.000000E+00 -3.931419E-01 -9.002841E-02 -1.092722E+00 -3.733055E-01 -2.384227E+00 -1.926937E+00 -9.101131E-01 -3.634496E-01 -3.284661E-01 -1.078900E-01 0.000000E+00 0.000000E+00 -6.885295E-02 -4.740728E-03 0.000000E+00 0.000000E+00 -2.419633E-02 -5.854622E-04 -9.286912E-02 -7.247209E-03 -5.629729E-01 -9.281109E-02 -7.345786E-01 -1.755550E-01 -1.219449E-01 -1.487057E-02 +5.299733E-01 +2.205463E-01 +1.349846E+00 +6.808561E-01 +6.874433E-01 +2.287801E-01 +5.651386E-01 +1.286874E-01 +5.729905E-01 +2.680764E-01 +5.509254E-01 +1.200498E-01 +1.494910E+00 +6.327940E-01 +2.444256E-01 +2.804968E-02 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-7.875036E-03 -2.836364E-01 -3.508209E-02 -4.509177E-01 -7.393615E-02 -1.077505E+00 -3.209541E-01 -1.204982E-02 -1.451982E-04 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -2.502937E-01 -5.035125E-02 -1.367234E+00 -5.128884E-01 -5.563575E-01 -2.510519E-01 -3.174809E-01 -1.007941E-01 -9.152129E-01 -2.609325E-01 -9.040668E-01 -2.263595E-01 -7.868812E-01 -2.436310E-01 0.000000E+00 0.000000E+00 0.000000E+00 @@ -467,60 +444,22 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -3.390904E-01 -4.907887E-02 -6.577001E-01 -2.346964E-01 -1.023735E-01 -8.287220E-03 -1.499600E-02 -2.248801E-04 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -1.395650E-01 -1.947839E-02 -1.040555E+00 -3.043523E-01 -1.426976E+00 -6.218295E-01 -8.342758E-01 -2.539692E-01 -3.101170E-01 -9.617255E-02 -6.319919E-02 -3.629541E-03 -1.292774E-01 -8.674372E-03 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -9.056616E-01 -4.198926E-01 -7.349640E-02 -5.401721E-03 -5.146331E-01 -1.555789E-01 -2.464783E-01 -5.430051E-02 -7.263842E-02 -5.276340E-03 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -9.587357E-01 -4.992769E-01 -1.756477E+00 -7.884472E-01 -2.541705E-01 -4.325743E-02 0.000000E+00 0.000000E+00 0.000000E+00 @@ -528,19 +467,17 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 +1.678278E-01 +2.097037E-02 +5.312751E-02 +1.423243E-03 +3.374418E-01 +1.138670E-01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 -9.496519E-02 -4.948061E-03 -1.596404E-01 -2.548506E-02 -2.454011E-02 -6.022168E-04 -1.235276E-01 -1.525907E-02 0.000000E+00 0.000000E+00 0.000000E+00 @@ -551,8 +488,71 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -2.422913E-01 -5.870510E-02 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +5.208007E-01 +2.057626E-01 +1.050464E+00 +5.524605E-01 +7.171591E-02 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0.000000E+00 @@ -9087,8 +8969,6 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -1.596404E-01 -2.548506E-02 0.000000E+00 0.000000E+00 0.000000E+00 @@ -9115,8 +8995,6 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -2.454011E-02 -6.022168E-04 0.000000E+00 0.000000E+00 0.000000E+00 @@ -9149,8 +9027,134 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -1.235276E-01 -1.525907E-02 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 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+0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 @@ -9359,10 +9363,6 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -1.668786E-02 -2.784846E-04 -2.256035E-01 -5.089693E-02 0.000000E+00 0.000000E+00 0.000000E+00 diff --git a/tests/test_fixed_source/results_true.dat b/tests/test_fixed_source/results_true.dat index b3def050e..c7ddf3c0b 100644 --- a/tests/test_fixed_source/results_true.dat +++ b/tests/test_fixed_source/results_true.dat @@ -1,6 +1,6 @@ tally 1: -4.563929E+02 -2.091711E+04 +4.518784E+02 +2.056386E+04 leakage: -9.780000E+00 -9.566400E+00 +9.750000E+00 +9.508100E+00 diff --git a/tests/test_infinite_cell/results_true.dat b/tests/test_infinite_cell/results_true.dat index 0b8d92951..b909c92bb 100644 --- a/tests/test_infinite_cell/results_true.dat +++ b/tests/test_infinite_cell/results_true.dat @@ -1,2 +1,2 @@ k-combined: -9.788797E-02 1.378250E-03 +9.893460E-02 1.178316E-03 diff --git a/tests/test_iso_in_lab/inputs_true.dat b/tests/test_iso_in_lab/inputs_true.dat new file mode 100644 index 000000000..9a21b06f1 --- /dev/null +++ b/tests/test_iso_in_lab/inputs_true.dat @@ -0,0 +1 @@ +e0409e0660d58857a6a96ff5cb539ccc41c82f0e443e8081ee00bbee7b6c81b0ad43c870950ae37d4a18c329067b09479a27aa171c3a3f5771f53b384496fe61 \ No newline at end of file diff --git a/tests/test_iso_in_lab/results_true.dat b/tests/test_iso_in_lab/results_true.dat new file mode 100644 index 000000000..354ccb0f8 --- /dev/null +++ b/tests/test_iso_in_lab/results_true.dat @@ -0,0 +1,2 @@ +k-combined: +9.638450E-01 1.237705E-02 diff --git a/tests/test_iso_in_lab/test_iso_in_lab.py b/tests/test_iso_in_lab/test_iso_in_lab.py new file mode 100644 index 000000000..b60daea11 --- /dev/null +++ b/tests/test_iso_in_lab/test_iso_in_lab.py @@ -0,0 +1,26 @@ +#!/usr/bin/env python + +import os +import sys +import glob +import hashlib +sys.path.insert(0, os.pardir) +from testing_harness import PyAPITestHarness +import openmc +import openmc.mgxs + + +class IsoInLabTestHarness(PyAPITestHarness): + + def _build_inputs(self): + """Write input XML files with iso-in-lab scattering.""" + + self._input_set.build_default_materials_and_geometry() + self._input_set.build_default_settings() + self._input_set.materials.make_isotropic_in_lab() + self._input_set.export() + + +if __name__ == '__main__': + harness = IsoInLabTestHarness('statepoint.10.*') + harness.main() diff --git a/tests/test_lattice/results_true.dat b/tests/test_lattice/results_true.dat index cf51dd5d7..1d3d47fc4 100644 --- a/tests/test_lattice/results_true.dat +++ b/tests/test_lattice/results_true.dat @@ -1,2 +1,2 @@ k-combined: -1.042388E+00 1.575316E-01 +9.413559E-01 6.157522E-02 diff --git a/tests/test_lattice_hex/results_true.dat b/tests/test_lattice_hex/results_true.dat index b88285ff2..4ba727dbf 100644 --- a/tests/test_lattice_hex/results_true.dat +++ b/tests/test_lattice_hex/results_true.dat @@ -1,2 +1,2 @@ k-combined: -2.831014E-01 2.269849E-02 +2.496460E-01 1.257055E-02 diff --git a/tests/test_lattice_mixed/results_true.dat b/tests/test_lattice_mixed/results_true.dat index 7cea76ba0..d3c19b11a 100644 --- a/tests/test_lattice_mixed/results_true.dat +++ b/tests/test_lattice_mixed/results_true.dat @@ -1,2 +1,2 @@ k-combined: -9.922449E-01 1.281824E-02 +9.790311E-01 9.660522E-03 diff --git a/tests/test_lattice_multiple/results_true.dat b/tests/test_lattice_multiple/results_true.dat index 6caffdd95..5c00c4486 100644 --- a/tests/test_lattice_multiple/results_true.dat +++ b/tests/test_lattice_multiple/results_true.dat @@ -1,2 +1,2 @@ k-combined: -1.005983E+00 2.248579E-02 +9.581522E-01 4.261830E-02 diff --git a/tests/test_mg_basic/inputs_true.dat b/tests/test_mg_basic/inputs_true.dat new file mode 100644 index 000000000..fdbdb1c96 --- /dev/null +++ b/tests/test_mg_basic/inputs_true.dat @@ -0,0 +1 @@ +04b4a5099f0097bbe02983c67dea691d0d0d4ece7fb7c264b9b2c29955baa9e870b6fa999480da08ead1e5a0c078ae33ce1b0a5c8594ad465aedf9bf3933e104 \ No newline at end of file diff --git a/tests/test_mg_basic/results_true.dat b/tests/test_mg_basic/results_true.dat new file mode 100644 index 000000000..35f3e73d4 --- /dev/null +++ b/tests/test_mg_basic/results_true.dat @@ -0,0 +1,2 @@ +k-combined: +1.045320E+00 5.851680E-02 diff --git a/tests/test_mg_basic/test_mg_basic.py b/tests/test_mg_basic/test_mg_basic.py new file mode 100644 index 000000000..1a49ee8a8 --- /dev/null +++ b/tests/test_mg_basic/test_mg_basic.py @@ -0,0 +1,17 @@ +#!/usr/bin/env python + +import os +import sys +sys.path.insert(0, os.pardir) +from testing_harness import TestHarness, PyAPITestHarness +import openmc + + +class MGBasicTestHarness(PyAPITestHarness): + def _build_inputs(self): + super(MGBasicTestHarness, self)._build_inputs() + + +if __name__ == '__main__': + harness = MGBasicTestHarness('statepoint.10.*', False, mg=True) + harness.main() diff --git a/tests/test_mg_max_order/inputs_true.dat b/tests/test_mg_max_order/inputs_true.dat new file mode 100644 index 000000000..1ad336e19 --- /dev/null +++ b/tests/test_mg_max_order/inputs_true.dat @@ -0,0 +1 @@ +abe20c626d613e73ccb1a3f8468ad1b9aecca528afa9e8131a411d754eb86b8ab64a6fb1fdc9c0b8b8158ff7c82f548de5912041bf035aa5a2d4532cfe0c9510 \ No newline at end of file diff --git a/tests/test_mg_max_order/results_true.dat b/tests/test_mg_max_order/results_true.dat new file mode 100644 index 000000000..1b2300560 --- /dev/null +++ b/tests/test_mg_max_order/results_true.dat @@ -0,0 +1,2 @@ +k-combined: +1.083030E+00 1.855038E-02 diff --git a/tests/test_mg_max_order/test_mg_max_order.py b/tests/test_mg_max_order/test_mg_max_order.py new file mode 100644 index 000000000..2f5ee4e4e --- /dev/null +++ b/tests/test_mg_max_order/test_mg_max_order.py @@ -0,0 +1,85 @@ +#!/usr/bin/env python + +import os +import sys +sys.path.insert(0, os.pardir) +from testing_harness import TestHarness, PyAPITestHarness +from input_set import MGInputSet +import openmc + +class MGNuclideInputSet(MGInputSet): + def build_default_materials_and_geometry(self): + # Define materials needed for 1D/1G slab problem + uo2_data = openmc.Macroscopic('uo2_iso', '71c') + uo2 = openmc.Material(name='UO2', material_id=1) + uo2.set_density('macro', 1.0) + uo2.add_macroscopic(uo2_data) + + clad_data = openmc.Macroscopic('clad_iso', '71c') + clad = openmc.Material(name='Clad', material_id=2) + clad.set_density('macro', 1.0) + clad.add_macroscopic(clad_data) + + water_data = openmc.Macroscopic('lwtr_iso', '71c') + water = openmc.Material(name='LWTR', material_id=3) + water.set_density('macro', 1.0) + water.add_macroscopic(water_data) + + # Define the materials file. + self.materials.default_xs = '71c' + self.materials.add_materials((uo2, clad, water)) + + # Define surfaces. + + # Assembly/Problem Boundary + left = openmc.XPlane(x0=0.0, surface_id=200, + boundary_type='reflective') + right = openmc.XPlane(x0=10.0, surface_id=201, + boundary_type='reflective') + bottom = openmc.YPlane(y0=0.0, surface_id=300, + boundary_type='reflective') + top = openmc.YPlane(y0=10.0, surface_id=301, + boundary_type='reflective') + + down = openmc.ZPlane(z0=0.0, surface_id=0, + boundary_type='reflective') + fuel_clad_intfc = openmc.ZPlane(z0=2.0, surface_id=1) + clad_lwtr_intfc = openmc.ZPlane(z0=2.4, surface_id=2) + up = openmc.ZPlane(z0=5.0, surface_id=3, + boundary_type='reflective') + + # Define cells + c1 = openmc.Cell(cell_id=1) + c1.region = +left & -right & +bottom & -top & +down & -fuel_clad_intfc + c1.fill = uo2 + c2 = openmc.Cell(cell_id=2) + c2.region = +left & -right & +bottom & -top & +fuel_clad_intfc & -clad_lwtr_intfc + c2.fill = clad + c3 = openmc.Cell(cell_id=3) + c3.region = +left & -right & +bottom & -top & +clad_lwtr_intfc & -up + c3.fill = water + + # Define root universe. + root = openmc.Universe(universe_id=0, name='root universe') + + root.add_cells((c1,c2,c3)) + + # Define the geometry file. + geometry = openmc.Geometry() + geometry.root_universe = root + + self.geometry.geometry = geometry + +class MGMaxOrderTestHarness(PyAPITestHarness): + def __init__(self, statepoint_name, tallies_present, mg=False): + PyAPITestHarness.__init__(self, statepoint_name, tallies_present) + self._input_set = MGNuclideInputSet() + + def _build_inputs(self): + super(MGMaxOrderTestHarness, self)._build_inputs() + # Set P1 scattering + self._input_set.settings.max_order = 1 + +if __name__ == '__main__': + harness = MGMaxOrderTestHarness('statepoint.10.*', False, mg=True) + harness.main() diff --git a/tests/test_mg_nuclide/inputs_true.dat b/tests/test_mg_nuclide/inputs_true.dat new file mode 100644 index 000000000..eb643bbaf --- /dev/null +++ b/tests/test_mg_nuclide/inputs_true.dat @@ -0,0 +1 @@ +c9f9e7211bfb2af58130bedfd64592d093b7bfa424953eba433ecf08940595a96b8de7a892f12d1ab465cebd8e5dd784114c1b1299b534ed329df92752c9ed1f \ No newline at end of file diff --git a/tests/test_mg_nuclide/results_true.dat b/tests/test_mg_nuclide/results_true.dat new file mode 100644 index 000000000..5b60cef22 --- /dev/null +++ b/tests/test_mg_nuclide/results_true.dat @@ -0,0 +1,2 @@ +k-combined: +1.380785E-01 5.556526E-03 diff --git a/tests/test_mg_nuclide/test_mg_nuclide.py b/tests/test_mg_nuclide/test_mg_nuclide.py new file mode 100644 index 000000000..deb784bad --- /dev/null +++ b/tests/test_mg_nuclide/test_mg_nuclide.py @@ -0,0 +1,84 @@ +#!/usr/bin/env python + +import os +import sys +sys.path.insert(0, os.pardir) +from testing_harness import TestHarness, PyAPITestHarness +from input_set import MGInputSet +import openmc + +class MGNuclideInputSet(MGInputSet): + def build_default_materials_and_geometry(self): + # Define materials needed for 1D/1G slab problem + # This time do using nuclide, not macroscopic + uo2 = openmc.Material(name='UO2', material_id=1) + uo2.set_density('g/cm3', 1.0) + uo2.add_nuclide("uo2_iso", 1.0) + + clad = openmc.Material(name='Clad', material_id=2) + clad.set_density('g/cm3', 1.0) + clad.add_nuclide("clad_ang_mu", 1.0) + + water_data = openmc.Nuclide('lwtr_iso_mu', '71c') + water = openmc.Material(name='LWTR', material_id=3) + water.set_density('g/cm3', 1.0) + water.add_nuclide("lwtr_iso_mu", 1.0) + + # Define the materials file. + self.materials.default_xs = '71c' + self.materials.add_materials((uo2, clad, water)) + + # Define surfaces. + + # Assembly/Problem Boundary + left = openmc.XPlane(x0=0.0, surface_id=200, + boundary_type='reflective') + right = openmc.XPlane(x0=10.0, surface_id=201, + boundary_type='reflective') + bottom = openmc.YPlane(y0=0.0, surface_id=300, + boundary_type='reflective') + top = openmc.YPlane(y0=10.0, surface_id=301, + boundary_type='reflective') + + down = openmc.ZPlane(z0=0.0, surface_id=0, + boundary_type='reflective') + fuel_clad_intfc = openmc.ZPlane(z0=2.0, surface_id=1) + clad_lwtr_intfc = openmc.ZPlane(z0=2.4, surface_id=2) + up = openmc.ZPlane(z0=5.0, surface_id=3, + boundary_type='reflective') + + # Define cells + c1 = openmc.Cell(cell_id=1) + c1.region = +left & -right & +bottom & -top & +down & -fuel_clad_intfc + c1.fill = uo2 + c2 = openmc.Cell(cell_id=2) + c2.region = +left & -right & +bottom & -top & +fuel_clad_intfc & -clad_lwtr_intfc + c2.fill = clad + c3 = openmc.Cell(cell_id=3) + c3.region = +left & -right & +bottom & -top & +clad_lwtr_intfc & -up + c3.fill = water + + # Define root universe. + root = openmc.Universe(universe_id=0, name='root universe') + + root.add_cells((c1,c2,c3)) + + # Define the geometry file. + geometry = openmc.Geometry() + geometry.root_universe = root + + self.geometry.geometry = geometry + +class MGNuclideTestHarness(PyAPITestHarness): + def __init__(self, statepoint_name, tallies_present, mg=False): + PyAPITestHarness.__init__(self, statepoint_name, tallies_present) + self._input_set = MGNuclideInputSet() + + def _build_inputs(self): + super(MGNuclideTestHarness, self)._build_inputs() + + + +if __name__ == '__main__': + harness = MGNuclideTestHarness('statepoint.10.*', False, mg=True) + harness.main() diff --git a/tests/test_mg_tallies/inputs_true.dat b/tests/test_mg_tallies/inputs_true.dat new file mode 100644 index 000000000..304d2e888 --- /dev/null +++ b/tests/test_mg_tallies/inputs_true.dat @@ -0,0 +1 @@ +ca8490e0e4549fed727ddc75b6d92cfe5162e11b905218a0afaa3ce2ee0763e2ff38074de27aaa678818624f49c5823650475dfa8f66f502a98fc03145399c0d \ No newline at end of file diff --git a/tests/test_mg_tallies/results_true.dat b/tests/test_mg_tallies/results_true.dat new file mode 100644 index 000000000..0cb47a712 --- /dev/null +++ b/tests/test_mg_tallies/results_true.dat @@ -0,0 +1,2906 @@ +k-combined: +1.045320E+00 5.851680E-02 +tally 1: +2.286064E+00 +1.057353E+00 +6.503987E-02 +8.851627E-04 +3.376363E+00 +2.323627E+00 +2.733240E-02 +1.607534E-04 +6.776283E-02 +9.880704E-04 +2.391658E+00 +1.201477E+00 +7.241106E-02 +1.103780E-03 +3.614949E+00 +2.730438E+00 +3.146867E-02 +2.110753E-04 +7.801752E-02 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+0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +tally 2: +4.283244E+01 +3.698890E+02 +4.285612E+01 +3.702981E+02 +6.926001E+00 +9.669342E+00 +6.926497E+00 +9.670727E+00 +1.223563E+02 +3.025594E+03 +1.223563E+02 +3.025594E+03 diff --git a/tests/test_mg_tallies/test_mg_tallies.py b/tests/test_mg_tallies/test_mg_tallies.py new file mode 100644 index 000000000..c54fb4d32 --- /dev/null +++ b/tests/test_mg_tallies/test_mg_tallies.py @@ -0,0 +1,59 @@ +#!/usr/bin/env python + +import os +import sys +sys.path.insert(0, os.pardir) +from testing_harness import TestHarness, PyAPITestHarness +import openmc + + +class MGTalliesTestHarness(PyAPITestHarness): + def _build_inputs(self): + # Instantiate a tally mesh + mesh = openmc.Mesh(mesh_id=1) + mesh.type = 'regular' + mesh.dimension = [17, 17, 1] + mesh.lower_left = [0.0, 0.0, 0.0] + mesh.upper_right = [21.42, 21.42, 100.0] + + # Instantiate some tally filters + energy_filter = openmc.Filter(type='energy', + bins=[0.0, 20.0]) + energyout_filter = openmc.Filter(type='energyout', + bins=[0.0, 20.0]) + mesh_filter = openmc.Filter() + mesh_filter.mesh = mesh + + mat_filter = openmc.Filter(type='material', bins=[1,2,3]) + + tally1 = openmc.Tally(tally_id=1) + tally1.add_filter(mesh_filter) + tally1.add_score('total') + tally1.add_score('absorption') + tally1.add_score('flux') + tally1.add_score('fission') + tally1.add_score('nu-fission') + + tally2 = openmc.Tally(tally_id=2) + tally2.add_filter(mat_filter) + tally2.add_filter(energy_filter) + tally2.add_filter(energyout_filter) + tally2.add_score('scatter') + tally2.add_score('nu-scatter') + + self._input_set.tallies = openmc.TalliesFile() + self._input_set.tallies.add_mesh(mesh) + self._input_set.tallies.add_tally(tally1) + self._input_set.tallies.add_tally(tally2) + + super(MGTalliesTestHarness, self)._build_inputs() + + def _cleanup(self): + super(MGTalliesTestHarness, self)._cleanup() + f = os.path.join(os.getcwd(), 'tallies.xml') + if os.path.exists(f): os.remove(f) + + +if __name__ == '__main__': + harness = MGTalliesTestHarness('statepoint.10.*', True, mg=True) + harness.main() diff --git a/tests/test_mgxs_library_condense/results_true.dat b/tests/test_mgxs_library_condense/results_true.dat index 45891fc30..438215372 100644 --- a/tests/test_mgxs_library_condense/results_true.dat +++ b/tests/test_mgxs_library_condense/results_true.dat @@ -1,49 +1,49 @@ material group in nuclide mean std. dev. -0 1 1 total 0.419289 0.01638 material group in nuclide mean std. dev. -0 1 1 total 0.07774 0.003273 material group in group out nuclide mean std. dev. -0 1 1 1 total 0.352665 0.015654 material group out nuclide mean std. dev. -0 1 1 total 1 0.119622 material group in nuclide mean std. dev. -0 2 1 total 0.247316 0.009562 material group in nuclide mean std. dev. -0 2 1 total 0 0 material group in group out nuclide mean std. dev. -0 2 1 1 total 0.244838 0.009996 material group out nuclide mean std. dev. -0 2 1 total 0 0 material group in nuclide mean std. dev. -0 3 1 total 0.409938 0.042262 material group in nuclide mean std. dev. -0 3 1 total 0 0 material group in group out nuclide mean std. dev. -0 3 1 1 total 0.403354 0.041386 material group out nuclide mean std. dev. -0 3 1 total 0 0 material group in nuclide mean std. dev. -0 4 1 total 0.344007 0.05352 material group in nuclide mean std. dev. -0 4 1 total 0 0 material group in group out nuclide mean std. dev. -0 4 1 1 total 0.340438 0.052067 material group out nuclide mean std. dev. -0 4 1 total 0 0 material group in nuclide mean std. dev. -0 5 1 total 0 0 material group in nuclide mean std. dev. -0 5 1 total 0 0 material group in group out nuclide mean std. dev. -0 5 1 1 total 0 0 material group out nuclide mean std. dev. -0 5 1 total 0 0 material group in nuclide mean std. dev. -0 6 1 total 0 0 material group in nuclide mean std. dev. -0 6 1 total 0 0 material group in group out nuclide mean std. dev. -0 6 1 1 total 0 0 material group out nuclide mean std. dev. -0 6 1 total 0 0 material group in nuclide mean std. dev. -0 7 1 total 0 0 material group in nuclide mean std. dev. -0 7 1 total 0 0 material group in group out nuclide mean std. dev. -0 7 1 1 total 0 0 material group out nuclide mean std. dev. -0 7 1 total 0 0 material group in nuclide mean std. dev. -0 8 1 total 0 0 material group in nuclide mean std. dev. -0 8 1 total 0 0 material group in group out nuclide mean std. dev. -0 8 1 1 total 0 0 material group out nuclide mean std. dev. -0 8 1 total 0 0 material group in nuclide mean std. dev. -0 9 1 total 0.751873 0.559701 material group in nuclide mean std. dev. -0 9 1 total 0 0 material group in group out nuclide mean std. dev. -0 9 1 1 total 0.695491 0.50757 material group out nuclide mean std. dev. -0 9 1 total 0 0 material group in nuclide mean std. dev. -0 10 1 total 0 0 material group in nuclide mean std. dev. -0 10 1 total 0 0 material group in group out nuclide mean std. dev. -0 10 1 1 total 0 0 material group out nuclide mean std. dev. -0 10 1 total 0 0 material group in nuclide mean std. dev. -0 11 1 total 0.457329 0.403578 material group in nuclide mean std. dev. -0 11 1 total 0 0 material group in group out nuclide mean std. dev. -0 11 1 1 total 0.446737 0.392775 material group out nuclide mean std. dev. -0 11 1 total 0 0 material group in nuclide mean std. dev. -0 12 1 total 0.574978 0.38864 material group in nuclide mean std. dev. -0 12 1 total 0 0 material group in group out nuclide mean std. dev. -0 12 1 1 total 0.559478 0.377512 material group out nuclide mean std. dev. -0 12 1 total 0 0 \ No newline at end of file +0 1 1 total 0.412084 0.02359 material group in nuclide mean std. dev. +0 1 1 total 0.076425 0.003691 material group in group out nuclide mean std. dev. +0 1 1 1 total 0.345643 0.021487 material group out nuclide mean std. dev. +0 1 1 total 1.0 0.055333 material group in nuclide mean std. dev. +0 2 1 total 0.241262 0.00841 material group in nuclide mean std. dev. +0 2 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 2 1 1 total 0.241262 0.00841 material group out nuclide mean std. dev. +0 2 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 3 1 total 0.400028 0.034667 material group in nuclide mean std. dev. +0 3 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 3 1 1 total 0.393462 0.033646 material group out nuclide mean std. dev. +0 3 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 4 1 total 0.377402 0.072937 material group in nuclide mean std. dev. +0 4 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 4 1 1 total 0.371473 0.071226 material group out nuclide mean std. dev. +0 4 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 5 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 5 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 5 1 1 total 0.0 0.0 material group out nuclide mean std. dev. +0 5 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 6 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 6 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 6 1 1 total 0.0 0.0 material group out nuclide mean std. dev. +0 6 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 7 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 7 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 7 1 1 total 0.0 0.0 material group out nuclide mean std. dev. +0 7 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 8 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 8 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 8 1 1 total 0.0 0.0 material group out nuclide mean std. dev. +0 8 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 9 1 total 0.600536 0.748875 material group in nuclide mean std. dev. +0 9 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 9 1 1 total 0.600536 0.748875 material group out nuclide mean std. dev. +0 9 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 10 1 total 0.235515 0.613974 material group in nuclide mean std. dev. +0 10 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 10 1 1 total 0.235515 0.613974 material group out nuclide mean std. dev. +0 10 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 11 1 total 0.510145 0.741941 material group in nuclide mean std. dev. +0 11 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 11 1 1 total 0.491857 0.715554 material group out nuclide mean std. dev. +0 11 1 total 0.0 0.0 material group in nuclide mean std. dev. +0 12 1 total 0.73836 0.825631 material group in nuclide mean std. dev. +0 12 1 total 0.0 0.0 material group in group out nuclide mean std. dev. +0 12 1 1 total 0.723265 0.808231 material group out nuclide mean std. dev. +0 12 1 total 0.0 0.0 \ No newline at end of file diff --git a/tests/test_mgxs_library_distribcell/results_true.dat b/tests/test_mgxs_library_distribcell/results_true.dat index 4936da4ce..0d5c7c7b4 100644 --- a/tests/test_mgxs_library_distribcell/results_true.dat +++ b/tests/test_mgxs_library_distribcell/results_true.dat @@ -1,5 +1,5 @@ - sum(distribcell) group in nuclide mean std. dev. -0 sum(0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, ... 1 total 0.720213 1.424323 sum(distribcell) group in nuclide mean std. dev. -0 sum(0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, ... 1 total 0 0 sum(distribcell) group in group out nuclide mean std. dev. -0 sum(0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, ... 1 1 total 0.70466 1.403916 sum(distribcell) group out nuclide mean std. dev. -0 sum(0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, ... 1 total 0 0 \ No newline at end of file + avg(distribcell) group in nuclide mean std. dev. +0 (0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13,... 1 total 0.718919 0.520644 avg(distribcell) group in nuclide mean std. dev. +0 (0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13,... 1 total 0.0 0.0 avg(distribcell) group in group out nuclide mean std. dev. +0 (0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13,... 1 1 total 0.695166 0.510606 avg(distribcell) group out nuclide mean std. dev. +0 (0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13,... 1 total 0.0 0.0 \ No newline at end of file diff --git a/tests/test_mgxs_library_hdf5/results_true.dat b/tests/test_mgxs_library_hdf5/results_true.dat index eec581046..e19b9ffa5 100644 --- a/tests/test_mgxs_library_hdf5/results_true.dat +++ b/tests/test_mgxs_library_hdf5/results_true.dat @@ -1,56 +1,56 @@ domain=1 type=transport -[ 0.38437891 0.81208747] -[ 0.01648997 0.07418959] +[ 0.37274472 0.86160691] +[ 0.02426918 0.03234902] domain=1 type=nu-fission -[ 0.02127008 0.69604034] -[ 0.0008939 0.05345764] +[ 0.02178897 0.71407658] +[ 0.00118187 0.04055185] domain=1 type=nu-scatter matrix -[[ 3.49923892e-01 1.73140769e-04] - [ 1.94810926e-03 3.79607212e-01]] -[[ 0.01664928 0.0001732 ] - [ 0.00195193 0.04007819]] +[[ 0.3373971 0.00155945] + [ 0. 0.42205129]] +[[ 0.02303884 0.00051015] + [ 0. 0.02161702]] domain=1 type=chi [ 1. 0.] -[ 0.11962178 0. ] +[ 0.05533329 0. ] domain=2 type=transport -[ 0.24504295 0.26645769] -[ 0.00882749 0.05220872] +[ 0.23725441 0.28593027] +[ 0.00818357 0.04879593] domain=2 type=nu-fission [ 0. 0.] [ 0. 0.] domain=2 type=nu-scatter matrix -[[ 0.24365718 0. ] - [ 0. 0.25478661]] -[[ 0.00908307 0. ] - [ 0. 0.05556256]] +[[ 0.23725441 0. ] + [ 0. 0.28593027]] +[[ 0.00818357 0. ] + [ 0. 0.04879593]] domain=2 type=chi [ 0. 0.] [ 0. 0.] domain=3 type=transport -[ 0.28227749 1.42731974] -[ 0.03724175 0.24712746] +[ 0.28690578 1.41815062] +[ 0.02740142 0.26530756] domain=3 type=nu-fission [ 0. 0.] [ 0. 0.] domain=3 type=nu-scatter matrix -[[ 0.25396726 0.02727268] - [ 0. 1.37652669]] -[[ 0.03617307 0.00180698] - [ 0. 0.2402569 ]] +[[ 0.25993686 0.02618721] + [ 0. 1.35952132]] +[[ 0.02611466 0.00166461] + [ 0. 0.2585046 ]] domain=3 type=chi [ 0. 0.] [ 0. 0.] domain=4 type=transport -[ 0.25572316 1.17976682] -[ 0.05191655 0.22938034] +[ 0.24244686 1.25395921] +[ 0.06103082 0.38836257] domain=4 type=nu-fission [ 0. 0.] [ 0. 0.] domain=4 type=nu-scatter matrix -[[ 0.23297756 0.02228141] - [ 0. 1.14680862]] -[[ 0.04977114 0.00262525] - [ 0. 0.22219839]] +[[ 0.2179296 0.023662 ] + [ 0. 1.21507398]] +[[ 0.0585649 0.00308328] + [ 0. 0.3810251 ]] domain=4 type=chi [ 0. 0.] [ 0. 0.] @@ -111,58 +111,58 @@ domain=8 type=chi [ 0. 0.] [ 0. 0.] domain=9 type=transport -[ 0.50403601 1.68709544] -[ 0.37962374 2.53662237] +[ 0.60053598 0. ] +[ 0.74887543 0. ] domain=9 type=nu-fission [ 0. 0.] [ 0. 0.] domain=9 type=nu-scatter matrix -[[ 0.50403601 0. ] - [ 0. 1.41795483]] -[[ 0.37962374 0. ] - [ 0. 2.15802716]] +[[ 0.60053598 0. ] + [ 0. 0. ]] +[[ 0.74887543 0. ] + [ 0. 0. ]] domain=9 type=chi [ 0. 0.] [ 0. 0.] domain=10 type=transport -[ 0. 0.] -[ 0. 0.] +[ 0.23551495 0. ] +[ 0.61397415 0. ] domain=10 type=nu-fission [ 0. 0.] [ 0. 0.] domain=10 type=nu-scatter matrix -[[ 0. 0.] - [ 0. 0.]] -[[ 0. 0.] - [ 0. 0.]] +[[ 0.23551495 0. ] + [ 0. 0. ]] +[[ 0.61397415 0. ] + [ 0. 0. ]] domain=10 type=chi [ 0. 0.] [ 0. 0.] domain=11 type=transport -[ 0.30282618 1.00614519] -[ 0.40131081 1.09163785] +[ 0.18632392 0.94598628] +[ 0.63212919 1.59113341] domain=11 type=nu-fission [ 0. 0.] [ 0. 0.] domain=11 type=nu-scatter matrix -[[ 0.27567871 0.02714747] - [ 0. 0.95792921]] -[[ 0.38567601 0.02000859] - [ 0. 1.05195936]] +[[ 0.15444875 0.03187517] + [ 0. 0.90308451]] +[[ 0.59768579 0.0450783 ] + [ 0. 1.53214394]] domain=11 type=chi [ 0. 0.] [ 0. 0.] domain=12 type=transport -[ 0.25593293 1.11334475] -[ 0.26842571 0.98867569] +[ 0.21329208 1.3909745 ] +[ 0.27144387 2.13734565] domain=12 type=nu-fission [ 0. 0.] [ 0. 0.] domain=12 type=nu-scatter matrix -[[ 0.22631045 0.02962248] - [ 0. 1.07168976]] -[[ 0.25487194 0.0177599 ] - [ 0. 0.95829029]] +[[ 0.18605249 0.02723959] + [ 0. 1.35711799]] +[[ 0.25763254 0.02955488] + [ 0. 2.08984614]] domain=12 type=chi [ 0. 0.] [ 0. 0.] diff --git a/tests/test_mgxs_library_no_nuclides/results_true.dat b/tests/test_mgxs_library_no_nuclides/results_true.dat index 761851268..442b8ac7b 100644 --- a/tests/test_mgxs_library_no_nuclides/results_true.dat +++ b/tests/test_mgxs_library_no_nuclides/results_true.dat @@ -1,121 +1,121 @@ material group in nuclide mean std. dev. -1 1 1 total 0.384379 0.01649 -0 1 2 total 0.812087 0.07419 material group in nuclide mean std. dev. -1 1 1 total 0.02127 0.000894 -0 1 2 total 0.69604 0.053458 material group in group out nuclide mean std. dev. -3 1 1 1 total 0.349924 0.016649 -2 1 1 2 total 0.000173 0.000173 -1 1 2 1 total 0.001948 0.001952 -0 1 2 2 total 0.379607 0.040078 material group out nuclide mean std. dev. -1 1 1 total 1 0.119622 -0 1 2 total 0 0.000000 material group in nuclide mean std. dev. -1 2 1 total 0.245043 0.008827 -0 2 2 total 0.266458 0.052209 material group in nuclide mean std. dev. -1 2 1 total 0 0 -0 2 2 total 0 0 material group in group out nuclide mean std. dev. -3 2 1 1 total 0.243657 0.009083 +1 1 1 total 0.372745 0.024269 +0 1 2 total 0.861607 0.032349 material group in nuclide mean std. dev. +1 1 1 total 0.021789 0.001182 +0 1 2 total 0.714077 0.040552 material group in group out nuclide mean std. dev. +3 1 1 1 total 0.337397 0.023039 +2 1 1 2 total 0.001559 0.000510 +1 1 2 1 total 0.000000 0.000000 +0 1 2 2 total 0.422051 0.021617 material group out nuclide mean std. dev. +1 1 1 total 1.0 0.055333 +0 1 2 total 0.0 0.000000 material group in nuclide mean std. dev. +1 2 1 total 0.237254 0.008184 +0 2 2 total 0.285930 0.048796 material group in nuclide mean std. dev. +1 2 1 total 0.0 0.0 +0 2 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 2 1 1 total 0.237254 0.008184 2 2 1 2 total 0.000000 0.000000 1 2 2 1 total 0.000000 0.000000 -0 2 2 2 total 0.254787 0.055563 material group out nuclide mean std. dev. -1 2 1 total 0 0 -0 2 2 total 0 0 material group in nuclide mean std. dev. -1 3 1 total 0.282277 0.037242 -0 3 2 total 1.427320 0.247127 material group in nuclide mean std. dev. -1 3 1 total 0 0 -0 3 2 total 0 0 material group in group out nuclide mean std. dev. -3 3 1 1 total 0.253967 0.036173 -2 3 1 2 total 0.027273 0.001807 +0 2 2 2 total 0.285930 0.048796 material group out nuclide mean std. dev. +1 2 1 total 0.0 0.0 +0 2 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 3 1 total 0.286906 0.027401 +0 3 2 total 1.418151 0.265308 material group in nuclide mean std. dev. +1 3 1 total 0.0 0.0 +0 3 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 3 1 1 total 0.259937 0.026115 +2 3 1 2 total 0.026187 0.001665 1 3 2 1 total 0.000000 0.000000 -0 3 2 2 total 1.376527 0.240257 material group out nuclide mean std. dev. -1 3 1 total 0 0 -0 3 2 total 0 0 material group in nuclide mean std. dev. -1 4 1 total 0.255723 0.051917 -0 4 2 total 1.179767 0.229380 material group in nuclide mean std. dev. -1 4 1 total 0 0 -0 4 2 total 0 0 material group in group out nuclide mean std. dev. -3 4 1 1 total 0.232978 0.049771 -2 4 1 2 total 0.022281 0.002625 +0 3 2 2 total 1.359521 0.258505 material group out nuclide mean std. dev. +1 3 1 total 0.0 0.0 +0 3 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 4 1 total 0.242447 0.061031 +0 4 2 total 1.253959 0.388363 material group in nuclide mean std. dev. +1 4 1 total 0.0 0.0 +0 4 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 4 1 1 total 0.217930 0.058565 +2 4 1 2 total 0.023662 0.003083 1 4 2 1 total 0.000000 0.000000 -0 4 2 2 total 1.146809 0.222198 material group out nuclide mean std. dev. -1 4 1 total 0 0 -0 4 2 total 0 0 material group in nuclide mean std. dev. -1 5 1 total 0 0 -0 5 2 total 0 0 material group in nuclide mean std. dev. -1 5 1 total 0 0 -0 5 2 total 0 0 material group in group out nuclide mean std. dev. -3 5 1 1 total 0 0 -2 5 1 2 total 0 0 -1 5 2 1 total 0 0 -0 5 2 2 total 0 0 material group out nuclide mean std. dev. -1 5 1 total 0 0 -0 5 2 total 0 0 material group in nuclide mean std. dev. -1 6 1 total 0 0 -0 6 2 total 0 0 material group in nuclide mean std. dev. -1 6 1 total 0 0 -0 6 2 total 0 0 material group in group out nuclide mean std. dev. -3 6 1 1 total 0 0 -2 6 1 2 total 0 0 -1 6 2 1 total 0 0 -0 6 2 2 total 0 0 material group out nuclide mean std. dev. -1 6 1 total 0 0 -0 6 2 total 0 0 material group in nuclide mean std. dev. -1 7 1 total 0 0 -0 7 2 total 0 0 material group in nuclide mean std. dev. -1 7 1 total 0 0 -0 7 2 total 0 0 material group in group out nuclide mean std. dev. -3 7 1 1 total 0 0 -2 7 1 2 total 0 0 -1 7 2 1 total 0 0 -0 7 2 2 total 0 0 material group out nuclide mean std. dev. -1 7 1 total 0 0 -0 7 2 total 0 0 material group in nuclide mean std. dev. -1 8 1 total 0 0 -0 8 2 total 0 0 material group in nuclide mean std. dev. -1 8 1 total 0 0 -0 8 2 total 0 0 material group in group out nuclide mean std. dev. -3 8 1 1 total 0 0 -2 8 1 2 total 0 0 -1 8 2 1 total 0 0 -0 8 2 2 total 0 0 material group out nuclide mean std. dev. -1 8 1 total 0 0 -0 8 2 total 0 0 material group in nuclide mean std. dev. -1 9 1 total 0.504036 0.379624 -0 9 2 total 1.687095 2.536622 material group in nuclide mean std. dev. -1 9 1 total 0 0 -0 9 2 total 0 0 material group in group out nuclide mean std. dev. -3 9 1 1 total 0.504036 0.379624 +0 4 2 2 total 1.215074 0.381025 material group out nuclide mean std. dev. +1 4 1 total 0.0 0.0 +0 4 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 5 1 total 0.0 0.0 +0 5 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 5 1 total 0.0 0.0 +0 5 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 5 1 1 total 0.0 0.0 +2 5 1 2 total 0.0 0.0 +1 5 2 1 total 0.0 0.0 +0 5 2 2 total 0.0 0.0 material group out nuclide mean std. dev. +1 5 1 total 0.0 0.0 +0 5 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 6 1 total 0.0 0.0 +0 6 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 6 1 total 0.0 0.0 +0 6 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 6 1 1 total 0.0 0.0 +2 6 1 2 total 0.0 0.0 +1 6 2 1 total 0.0 0.0 +0 6 2 2 total 0.0 0.0 material group out nuclide mean std. dev. +1 6 1 total 0.0 0.0 +0 6 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 7 1 total 0.0 0.0 +0 7 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 7 1 total 0.0 0.0 +0 7 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 7 1 1 total 0.0 0.0 +2 7 1 2 total 0.0 0.0 +1 7 2 1 total 0.0 0.0 +0 7 2 2 total 0.0 0.0 material group out nuclide mean std. dev. +1 7 1 total 0.0 0.0 +0 7 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 8 1 total 0.0 0.0 +0 8 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 8 1 total 0.0 0.0 +0 8 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 8 1 1 total 0.0 0.0 +2 8 1 2 total 0.0 0.0 +1 8 2 1 total 0.0 0.0 +0 8 2 2 total 0.0 0.0 material group out nuclide mean std. dev. +1 8 1 total 0.0 0.0 +0 8 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 9 1 total 0.600536 0.748875 +0 9 2 total 0.000000 0.000000 material group in nuclide mean std. dev. +1 9 1 total 0.0 0.0 +0 9 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 9 1 1 total 0.600536 0.748875 2 9 1 2 total 0.000000 0.000000 1 9 2 1 total 0.000000 0.000000 -0 9 2 2 total 1.417955 2.158027 material group out nuclide mean std. dev. -1 9 1 total 0 0 -0 9 2 total 0 0 material group in nuclide mean std. dev. -1 10 1 total 0 0 -0 10 2 total 0 0 material group in nuclide mean std. dev. -1 10 1 total 0 0 -0 10 2 total 0 0 material group in group out nuclide mean std. dev. -3 10 1 1 total 0 0 -2 10 1 2 total 0 0 -1 10 2 1 total 0 0 -0 10 2 2 total 0 0 material group out nuclide mean std. dev. -1 10 1 total 0 0 -0 10 2 total 0 0 material group in nuclide mean std. dev. -1 11 1 total 0.302826 0.401311 -0 11 2 total 1.006145 1.091638 material group in nuclide mean std. dev. -1 11 1 total 0 0 -0 11 2 total 0 0 material group in group out nuclide mean std. dev. -3 11 1 1 total 0.275679 0.385676 -2 11 1 2 total 0.027147 0.020009 +0 9 2 2 total 0.000000 0.000000 material group out nuclide mean std. dev. +1 9 1 total 0.0 0.0 +0 9 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 10 1 total 0.235515 0.613974 +0 10 2 total 0.000000 0.000000 material group in nuclide mean std. dev. +1 10 1 total 0.0 0.0 +0 10 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 10 1 1 total 0.235515 0.613974 +2 10 1 2 total 0.000000 0.000000 +1 10 2 1 total 0.000000 0.000000 +0 10 2 2 total 0.000000 0.000000 material group out nuclide mean std. dev. +1 10 1 total 0.0 0.0 +0 10 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 11 1 total 0.186324 0.632129 +0 11 2 total 0.945986 1.591133 material group in nuclide mean std. dev. +1 11 1 total 0.0 0.0 +0 11 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 11 1 1 total 0.154449 0.597686 +2 11 1 2 total 0.031875 0.045078 1 11 2 1 total 0.000000 0.000000 -0 11 2 2 total 0.957929 1.051959 material group out nuclide mean std. dev. -1 11 1 total 0 0 -0 11 2 total 0 0 material group in nuclide mean std. dev. -1 12 1 total 0.255933 0.268426 -0 12 2 total 1.113345 0.988676 material group in nuclide mean std. dev. -1 12 1 total 0 0 -0 12 2 total 0 0 material group in group out nuclide mean std. dev. -3 12 1 1 total 0.226310 0.254872 -2 12 1 2 total 0.029622 0.017760 +0 11 2 2 total 0.903085 1.532144 material group out nuclide mean std. dev. +1 11 1 total 0.0 0.0 +0 11 2 total 0.0 0.0 material group in nuclide mean std. dev. +1 12 1 total 0.213292 0.271444 +0 12 2 total 1.390975 2.137346 material group in nuclide mean std. dev. +1 12 1 total 0.0 0.0 +0 12 2 total 0.0 0.0 material group in group out nuclide mean std. dev. +3 12 1 1 total 0.186052 0.257633 +2 12 1 2 total 0.027240 0.029555 1 12 2 1 total 0.000000 0.000000 -0 12 2 2 total 1.071690 0.958290 material group out nuclide mean std. dev. -1 12 1 total 0 0 -0 12 2 total 0 0 \ No newline at end of file +0 12 2 2 total 1.357118 2.089846 material group out nuclide mean std. dev. +1 12 1 total 0.0 0.0 +0 12 2 total 0.0 0.0 \ No newline at end of file diff --git a/tests/test_mgxs_library_nuclides/results_true.dat b/tests/test_mgxs_library_nuclides/results_true.dat index 23ac0e423..145521964 100644 --- a/tests/test_mgxs_library_nuclides/results_true.dat +++ b/tests/test_mgxs_library_nuclides/results_true.dat @@ -1,47 +1,47 @@ material group in nuclide mean std. dev. -34 1 1 U-234 0.000000 0.000000 -35 1 1 U-235 0.008559 0.001742 -36 1 1 U-236 0.002643 0.000794 -37 1 1 U-238 0.213622 0.010911 +34 1 1 U-234 0.000173 0.000173 +35 1 1 U-235 0.010677 0.001889 +36 1 1 U-236 0.002390 0.001055 +37 1 1 U-238 0.213680 0.013272 38 1 1 Np-237 0.000000 0.000000 39 1 1 Pu-238 0.000000 0.000000 -40 1 1 Pu-239 0.005787 0.001050 -41 1 1 Pu-240 0.005702 0.000850 -42 1 1 Pu-241 0.000869 0.000366 -43 1 1 Pu-242 0.000655 0.000537 -44 1 1 Am-241 0.000000 0.000000 +40 1 1 Pu-239 0.002911 0.000639 +41 1 1 Pu-240 0.004426 0.000806 +42 1 1 Pu-241 0.000690 0.000387 +43 1 1 Pu-242 0.000000 0.000000 +44 1 1 Am-241 0.000173 0.000173 45 1 1 Am-242m 0.000000 0.000000 46 1 1 Am-243 0.000000 0.000000 47 1 1 Cm-242 0.000000 0.000000 48 1 1 Cm-243 0.000000 0.000000 49 1 1 Cm-244 0.000000 0.000000 50 1 1 Cm-245 0.000000 0.000000 -51 1 1 Mo-95 0.000302 0.000216 -52 1 1 Tc-99 0.000782 0.000434 -53 1 1 Ru-101 0.000346 0.000212 -54 1 1 Ru-103 0.000000 0.000000 +51 1 1 Mo-95 0.000000 0.000000 +52 1 1 Tc-99 0.000173 0.000173 +53 1 1 Ru-101 0.000238 0.000254 +54 1 1 Ru-103 0.000002 0.000243 55 1 1 Ag-109 0.000000 0.000000 56 1 1 Xe-135 0.000000 0.000000 -57 1 1 Cs-133 0.000189 0.000264 -58 1 1 Nd-143 0.000721 0.000364 -59 1 1 Nd-145 0.000637 0.000253 -60 1 1 Sm-147 0.000009 0.000238 +57 1 1 Cs-133 0.000347 0.000213 +58 1 1 Nd-143 0.000447 0.000292 +59 1 1 Nd-145 0.000564 0.000294 +60 1 1 Sm-147 0.000000 0.000000 61 1 1 Sm-149 0.000000 0.000000 -62 1 1 Sm-150 0.000003 0.000243 +62 1 1 Sm-150 0.000472 0.000239 63 1 1 Sm-151 0.000000 0.000000 -64 1 1 Sm-152 0.000874 0.000388 +64 1 1 Sm-152 0.000492 0.000352 65 1 1 Eu-153 0.000173 0.000173 66 1 1 Gd-155 0.000000 0.000000 -67 1 1 O-16 0.142506 0.008222 -0 1 2 U-234 0.001948 0.001952 -1 1 2 U-235 0.179956 0.028209 -2 1 2 U-236 0.000000 0.000000 -3 1 2 U-238 0.239279 0.039048 +67 1 1 O-16 0.134715 0.009801 +0 1 2 U-234 0.000000 0.000000 +1 1 2 U-235 0.199907 0.007776 +2 1 2 U-236 0.001501 0.002037 +3 1 2 U-238 0.255355 0.029743 4 1 2 Np-237 0.000000 0.000000 5 1 2 Pu-238 0.000000 0.000000 -6 1 2 Pu-239 0.159745 0.015751 -7 1 2 Pu-240 0.007792 0.003677 -8 1 2 Pu-241 0.017533 0.003806 +6 1 2 Pu-239 0.160378 0.011366 +7 1 2 Pu-240 0.007920 0.003710 +8 1 2 Pu-241 0.017820 0.003733 9 1 2 Pu-242 0.000000 0.000000 10 1 2 Am-241 0.000000 0.000000 11 1 2 Am-242m 0.000000 0.000000 @@ -50,40 +50,40 @@ 14 1 2 Cm-243 0.000000 0.000000 15 1 2 Cm-244 0.000000 0.000000 16 1 2 Cm-245 0.000000 0.000000 -17 1 2 Mo-95 0.002250 0.004232 -18 1 2 Tc-99 0.003544 0.002528 +17 1 2 Mo-95 0.000000 0.000000 +18 1 2 Tc-99 0.000000 0.000000 19 1 2 Ru-101 0.000000 0.000000 20 1 2 Ru-103 0.000000 0.000000 21 1 2 Ag-109 0.000000 0.000000 -22 1 2 Xe-135 0.027274 0.004025 +22 1 2 Xe-135 0.013860 0.003976 23 1 2 Cs-133 0.000000 0.000000 -24 1 2 Nd-143 0.006532 0.002517 -25 1 2 Nd-145 0.001948 0.001952 +24 1 2 Nd-143 0.003960 0.002427 +25 1 2 Nd-145 0.000000 0.000000 26 1 2 Sm-147 0.000000 0.000000 -27 1 2 Sm-149 0.007792 0.005701 +27 1 2 Sm-149 0.001980 0.001981 28 1 2 Sm-150 0.000000 0.000000 -29 1 2 Sm-151 0.000000 0.000000 +29 1 2 Sm-151 0.001980 0.001981 30 1 2 Sm-152 0.000000 0.000000 -31 1 2 Eu-153 0.001686 0.001968 +31 1 2 Eu-153 0.000000 0.000000 32 1 2 Gd-155 0.000000 0.000000 -33 1 2 O-16 0.154807 0.023798 material group in nuclide mean std. dev. -34 1 1 U-234 6.771527e-06 2.982583e-07 -35 1 1 U-235 9.687933e-03 4.305720e-04 -36 1 1 U-236 6.279974e-05 3.653120e-06 -37 1 1 U-238 6.335930e-03 4.715525e-04 -38 1 1 Np-237 1.237030e-05 6.333955e-07 -39 1 1 Pu-238 7.369063e-06 5.017525e-07 -40 1 1 Pu-239 4.007893e-03 2.607619e-04 -41 1 1 Pu-240 6.479096e-05 3.728060e-06 -42 1 1 Pu-241 1.074454e-03 4.688479e-05 -43 1 1 Pu-242 5.512610e-06 2.976651e-07 -44 1 1 Am-241 1.088373e-06 8.489934e-08 -45 1 1 Am-242m 1.143307e-06 9.912400e-08 -46 1 1 Am-243 7.745526e-07 5.413923e-08 -47 1 1 Cm-242 4.311566e-07 1.922427e-08 -48 1 1 Cm-243 2.363328e-07 2.235666e-08 -49 1 1 Cm-244 2.840125e-07 2.412051e-08 -50 1 1 Cm-245 3.017505e-07 1.594090e-08 +33 1 2 O-16 0.196946 0.014729 material group in nuclide mean std. dev. +34 1 1 U-234 7.274440e-06 4.419477e-07 +35 1 1 U-235 9.587803e-03 5.936922e-04 +36 1 1 U-236 7.566099e-05 7.523935e-06 +37 1 1 U-238 7.178367e-03 6.505680e-04 +38 1 1 Np-237 1.315682e-05 8.036501e-07 +39 1 1 Pu-238 7.746151e-06 3.992835e-07 +40 1 1 Pu-239 3.805294e-03 3.637600e-04 +41 1 1 Pu-240 6.941319e-05 4.729737e-06 +42 1 1 Pu-241 1.033844e-03 9.083913e-05 +43 1 1 Pu-242 5.995332e-06 3.821721e-07 +44 1 1 Am-241 1.148585e-06 8.271648e-08 +45 1 1 Am-242m 1.100215e-06 6.159956e-08 +46 1 1 Am-243 8.323826e-07 5.841792e-08 +47 1 1 Cm-242 5.088970e-07 5.258007e-08 +48 1 1 Cm-243 2.245435e-07 1.459025e-08 +49 1 1 Cm-244 2.993206e-07 2.746129e-08 +50 1 1 Cm-245 3.063611e-07 3.057751e-08 51 1 1 Mo-95 0.000000e+00 0.000000e+00 52 1 1 Tc-99 0.000000e+00 0.000000e+00 53 1 1 Ru-101 0.000000e+00 0.000000e+00 @@ -101,23 +101,23 @@ 65 1 1 Eu-153 0.000000e+00 0.000000e+00 66 1 1 Gd-155 0.000000e+00 0.000000e+00 67 1 1 O-16 0.000000e+00 0.000000e+00 -0 1 2 U-234 4.267300e-07 3.529845e-08 -1 1 2 U-235 3.629246e-01 2.964548e-02 -2 1 2 U-236 5.921657e-06 4.881464e-07 -3 1 2 U-238 5.196256e-07 4.286610e-08 -4 1 2 Np-237 2.424211e-07 1.741823e-08 -5 1 2 Pu-238 3.255627e-05 2.692686e-06 -6 1 2 Pu-239 2.868384e-01 2.056896e-02 -7 1 2 Pu-240 4.398266e-06 3.658267e-07 -8 1 2 Pu-241 4.607239e-02 3.797176e-03 -9 1 2 Pu-242 8.451967e-08 6.979002e-09 -10 1 2 Am-241 4.678607e-06 3.253889e-07 -11 1 2 Am-242m 1.417675e-04 1.218350e-05 -12 1 2 Am-243 7.648834e-08 6.303843e-09 -13 1 2 Cm-242 9.433314e-07 7.794362e-08 -14 1 2 Cm-243 1.767995e-06 1.454123e-07 -15 1 2 Cm-244 1.533962e-07 1.266951e-08 -16 1 2 Cm-245 1.145063e-05 9.419051e-07 +0 1 2 U-234 4.408576e-07 2.828309e-08 +1 1 2 U-235 3.768094e-01 2.445671e-02 +2 1 2 U-236 6.097538e-06 3.733038e-07 +3 1 2 U-238 5.353074e-07 3.310544e-08 +4 1 2 Np-237 2.702971e-07 2.098939e-08 +5 1 2 Pu-238 3.463109e-05 2.638394e-06 +6 1 2 Pu-239 2.889643e-01 1.376004e-02 +7 1 2 Pu-240 4.533642e-06 2.544289e-07 +8 1 2 Pu-241 4.809366e-02 2.778345e-03 +9 1 2 Pu-242 8.715325e-08 5.460893e-09 +10 1 2 Am-241 4.611736e-06 2.155039e-07 +11 1 2 Am-242m 1.428047e-04 8.436437e-06 +12 1 2 Am-243 7.883895e-08 4.734503e-09 +13 1 2 Cm-242 9.731025e-07 6.143750e-08 +14 1 2 Cm-243 1.825830e-06 1.074849e-07 +15 1 2 Cm-244 1.581823e-07 9.938064e-09 +16 1 2 Cm-245 1.213386e-05 8.812019e-07 17 1 2 Mo-95 0.000000e+00 0.000000e+00 18 1 2 Tc-99 0.000000e+00 0.000000e+00 19 1 2 Ru-101 0.000000e+00 0.000000e+00 @@ -136,15 +136,15 @@ 32 1 2 Gd-155 0.000000e+00 0.000000e+00 33 1 2 O-16 0.000000e+00 0.000000e+00 material group in group out nuclide mean std. dev. 102 1 1 1 U-234 0.000000 0.000000 -103 1 1 1 U-235 0.002846 0.001185 -104 1 1 1 U-236 0.001951 0.000829 -105 1 1 1 U-238 0.197520 0.011618 +103 1 1 1 U-235 0.003226 0.001139 +104 1 1 1 U-236 0.001697 0.000923 +105 1 1 1 U-238 0.194620 0.013297 106 1 1 1 Np-237 0.000000 0.000000 107 1 1 1 Pu-238 0.000000 0.000000 -108 1 1 1 Pu-239 0.001285 0.000461 -109 1 1 1 Pu-240 0.001027 0.000635 -110 1 1 1 Pu-241 0.000004 0.000242 -111 1 1 1 Pu-242 0.000481 0.000372 +108 1 1 1 Pu-239 0.001005 0.000477 +109 1 1 1 Pu-240 0.001307 0.000295 +110 1 1 1 Pu-241 0.000344 0.000244 +111 1 1 1 Pu-242 0.000000 0.000000 112 1 1 1 Am-241 0.000000 0.000000 113 1 1 1 Am-242m 0.000000 0.000000 114 1 1 1 Am-243 0.000000 0.000000 @@ -152,27 +152,27 @@ 116 1 1 1 Cm-243 0.000000 0.000000 117 1 1 1 Cm-244 0.000000 0.000000 118 1 1 1 Cm-245 0.000000 0.000000 -119 1 1 1 Mo-95 0.000302 0.000216 -120 1 1 1 Tc-99 0.000262 0.000195 -121 1 1 1 Ru-101 0.000000 0.000000 -122 1 1 1 Ru-103 0.000000 0.000000 +119 1 1 1 Mo-95 0.000000 0.000000 +120 1 1 1 Tc-99 0.000000 0.000000 +121 1 1 1 Ru-101 0.000238 0.000254 +122 1 1 1 Ru-103 0.000002 0.000243 123 1 1 1 Ag-109 0.000000 0.000000 124 1 1 1 Xe-135 0.000000 0.000000 -125 1 1 1 Cs-133 0.000016 0.000234 -126 1 1 1 Nd-143 0.000721 0.000364 -127 1 1 1 Nd-145 0.000463 0.000281 -128 1 1 1 Sm-147 0.000009 0.000238 +125 1 1 1 Cs-133 0.000000 0.000000 +126 1 1 1 Nd-143 0.000447 0.000292 +127 1 1 1 Nd-145 0.000564 0.000294 +128 1 1 1 Sm-147 0.000000 0.000000 129 1 1 1 Sm-149 0.000000 0.000000 -130 1 1 1 Sm-150 0.000003 0.000243 +130 1 1 1 Sm-150 0.000299 0.000238 131 1 1 1 Sm-151 0.000000 0.000000 -132 1 1 1 Sm-152 0.000700 0.000424 +132 1 1 1 Sm-152 0.000492 0.000352 133 1 1 1 Eu-153 0.000000 0.000000 134 1 1 1 Gd-155 0.000000 0.000000 -135 1 1 1 O-16 0.142333 0.008156 +135 1 1 1 O-16 0.133156 0.009821 68 1 1 2 U-234 0.000000 0.000000 69 1 1 2 U-235 0.000000 0.000000 70 1 1 2 U-236 0.000000 0.000000 -71 1 1 2 U-238 0.000000 0.000000 +71 1 1 2 U-238 0.000173 0.000173 72 1 1 2 Np-237 0.000000 0.000000 73 1 1 2 Pu-238 0.000000 0.000000 74 1 1 2 Pu-239 0.000000 0.000000 @@ -202,7 +202,7 @@ 98 1 1 2 Sm-152 0.000000 0.000000 99 1 1 2 Eu-153 0.000000 0.000000 100 1 1 2 Gd-155 0.000000 0.000000 -101 1 1 2 O-16 0.000173 0.000173 +101 1 1 2 O-16 0.001386 0.000446 34 1 2 1 U-234 0.000000 0.000000 35 1 2 1 U-235 0.000000 0.000000 36 1 2 1 U-236 0.000000 0.000000 @@ -236,11 +236,11 @@ 64 1 2 1 Sm-152 0.000000 0.000000 65 1 2 1 Eu-153 0.000000 0.000000 66 1 2 1 Gd-155 0.000000 0.000000 -67 1 2 1 O-16 0.001948 0.001952 +67 1 2 1 O-16 0.000000 0.000000 0 1 2 2 U-234 0.000000 0.000000 -1 1 2 2 U-235 0.010470 0.006106 -2 1 2 2 U-236 0.000000 0.000000 -3 1 2 2 U-238 0.208109 0.039197 +1 1 2 2 U-235 0.003889 0.003962 +2 1 2 2 U-236 0.001501 0.002037 +3 1 2 2 U-238 0.219715 0.025984 4 1 2 2 Np-237 0.000000 0.000000 5 1 2 2 Pu-238 0.000000 0.000000 6 1 2 2 Pu-239 0.000000 0.000000 @@ -254,116 +254,116 @@ 14 1 2 2 Cm-243 0.000000 0.000000 15 1 2 2 Cm-244 0.000000 0.000000 16 1 2 2 Cm-245 0.000000 0.000000 -17 1 2 2 Mo-95 0.000302 0.002551 -18 1 2 2 Tc-99 0.003544 0.002528 +17 1 2 2 Mo-95 0.000000 0.000000 +18 1 2 2 Tc-99 0.000000 0.000000 19 1 2 2 Ru-101 0.000000 0.000000 20 1 2 2 Ru-103 0.000000 0.000000 21 1 2 2 Ag-109 0.000000 0.000000 22 1 2 2 Xe-135 0.000000 0.000000 23 1 2 2 Cs-133 0.000000 0.000000 -24 1 2 2 Nd-143 0.002636 0.002073 +24 1 2 2 Nd-143 0.000000 0.000000 25 1 2 2 Nd-145 0.000000 0.000000 26 1 2 2 Sm-147 0.000000 0.000000 27 1 2 2 Sm-149 0.000000 0.000000 28 1 2 2 Sm-150 0.000000 0.000000 29 1 2 2 Sm-151 0.000000 0.000000 30 1 2 2 Sm-152 0.000000 0.000000 -31 1 2 2 Eu-153 0.001686 0.001968 +31 1 2 2 Eu-153 0.000000 0.000000 32 1 2 2 Gd-155 0.000000 0.000000 -33 1 2 2 O-16 0.152859 0.022894 material group out nuclide mean std. dev. -34 1 1 U-234 0 0.000000 -35 1 1 U-235 1 0.127079 -36 1 1 U-236 0 0.000000 -37 1 1 U-238 1 0.153215 -38 1 1 Np-237 0 0.000000 -39 1 1 Pu-238 0 0.000000 -40 1 1 Pu-239 1 0.150979 -41 1 1 Pu-240 0 0.000000 -42 1 1 Pu-241 1 0.203534 -43 1 1 Pu-242 0 0.000000 -44 1 1 Am-241 0 0.000000 -45 1 1 Am-242m 0 0.000000 -46 1 1 Am-243 0 0.000000 -47 1 1 Cm-242 0 0.000000 -48 1 1 Cm-243 0 0.000000 -49 1 1 Cm-244 0 0.000000 -50 1 1 Cm-245 0 0.000000 -51 1 1 Mo-95 0 0.000000 -52 1 1 Tc-99 0 0.000000 -53 1 1 Ru-101 0 0.000000 -54 1 1 Ru-103 0 0.000000 -55 1 1 Ag-109 0 0.000000 -56 1 1 Xe-135 0 0.000000 -57 1 1 Cs-133 0 0.000000 -58 1 1 Nd-143 0 0.000000 -59 1 1 Nd-145 0 0.000000 -60 1 1 Sm-147 0 0.000000 -61 1 1 Sm-149 0 0.000000 -62 1 1 Sm-150 0 0.000000 -63 1 1 Sm-151 0 0.000000 -64 1 1 Sm-152 0 0.000000 -65 1 1 Eu-153 0 0.000000 -66 1 1 Gd-155 0 0.000000 -67 1 1 O-16 0 0.000000 -0 1 2 U-234 0 0.000000 -1 1 2 U-235 0 0.000000 -2 1 2 U-236 0 0.000000 -3 1 2 U-238 0 0.000000 -4 1 2 Np-237 0 0.000000 -5 1 2 Pu-238 0 0.000000 -6 1 2 Pu-239 0 0.000000 -7 1 2 Pu-240 0 0.000000 -8 1 2 Pu-241 0 0.000000 -9 1 2 Pu-242 0 0.000000 -10 1 2 Am-241 0 0.000000 -11 1 2 Am-242m 0 0.000000 -12 1 2 Am-243 0 0.000000 -13 1 2 Cm-242 0 0.000000 -14 1 2 Cm-243 0 0.000000 -15 1 2 Cm-244 0 0.000000 -16 1 2 Cm-245 0 0.000000 -17 1 2 Mo-95 0 0.000000 -18 1 2 Tc-99 0 0.000000 -19 1 2 Ru-101 0 0.000000 -20 1 2 Ru-103 0 0.000000 -21 1 2 Ag-109 0 0.000000 -22 1 2 Xe-135 0 0.000000 -23 1 2 Cs-133 0 0.000000 -24 1 2 Nd-143 0 0.000000 -25 1 2 Nd-145 0 0.000000 -26 1 2 Sm-147 0 0.000000 -27 1 2 Sm-149 0 0.000000 -28 1 2 Sm-150 0 0.000000 -29 1 2 Sm-151 0 0.000000 -30 1 2 Sm-152 0 0.000000 -31 1 2 Eu-153 0 0.000000 -32 1 2 Gd-155 0 0.000000 -33 1 2 O-16 0 0.000000 material group in nuclide mean std. dev. -5 2 1 Zr-90 0.118578 0.008347 -6 2 1 Zr-91 0.040887 0.002988 -7 2 1 Zr-92 0.033882 0.004365 -8 2 1 Zr-94 0.046281 0.005422 -9 2 1 Zr-96 0.005415 0.002113 -0 2 2 Zr-90 0.122479 0.032627 -1 2 2 Zr-91 0.035669 0.009683 -2 2 2 Zr-92 0.049331 0.021936 -3 2 2 Zr-94 0.058978 0.020081 +33 1 2 2 O-16 0.196946 0.014729 material group out nuclide mean std. dev. +34 1 1 U-234 0.0 0.000000 +35 1 1 U-235 1.0 0.066362 +36 1 1 U-236 0.0 0.000000 +37 1 1 U-238 1.0 0.093082 +38 1 1 Np-237 0.0 0.000000 +39 1 1 Pu-238 0.0 0.000000 +40 1 1 Pu-239 1.0 0.104567 +41 1 1 Pu-240 0.0 0.000000 +42 1 1 Pu-241 1.0 0.263696 +43 1 1 Pu-242 0.0 0.000000 +44 1 1 Am-241 0.0 0.000000 +45 1 1 Am-242m 0.0 0.000000 +46 1 1 Am-243 0.0 0.000000 +47 1 1 Cm-242 0.0 0.000000 +48 1 1 Cm-243 0.0 0.000000 +49 1 1 Cm-244 0.0 0.000000 +50 1 1 Cm-245 0.0 0.000000 +51 1 1 Mo-95 0.0 0.000000 +52 1 1 Tc-99 0.0 0.000000 +53 1 1 Ru-101 0.0 0.000000 +54 1 1 Ru-103 0.0 0.000000 +55 1 1 Ag-109 0.0 0.000000 +56 1 1 Xe-135 0.0 0.000000 +57 1 1 Cs-133 0.0 0.000000 +58 1 1 Nd-143 0.0 0.000000 +59 1 1 Nd-145 0.0 0.000000 +60 1 1 Sm-147 0.0 0.000000 +61 1 1 Sm-149 0.0 0.000000 +62 1 1 Sm-150 0.0 0.000000 +63 1 1 Sm-151 0.0 0.000000 +64 1 1 Sm-152 0.0 0.000000 +65 1 1 Eu-153 0.0 0.000000 +66 1 1 Gd-155 0.0 0.000000 +67 1 1 O-16 0.0 0.000000 +0 1 2 U-234 0.0 0.000000 +1 1 2 U-235 0.0 0.000000 +2 1 2 U-236 0.0 0.000000 +3 1 2 U-238 0.0 0.000000 +4 1 2 Np-237 0.0 0.000000 +5 1 2 Pu-238 0.0 0.000000 +6 1 2 Pu-239 0.0 0.000000 +7 1 2 Pu-240 0.0 0.000000 +8 1 2 Pu-241 0.0 0.000000 +9 1 2 Pu-242 0.0 0.000000 +10 1 2 Am-241 0.0 0.000000 +11 1 2 Am-242m 0.0 0.000000 +12 1 2 Am-243 0.0 0.000000 +13 1 2 Cm-242 0.0 0.000000 +14 1 2 Cm-243 0.0 0.000000 +15 1 2 Cm-244 0.0 0.000000 +16 1 2 Cm-245 0.0 0.000000 +17 1 2 Mo-95 0.0 0.000000 +18 1 2 Tc-99 0.0 0.000000 +19 1 2 Ru-101 0.0 0.000000 +20 1 2 Ru-103 0.0 0.000000 +21 1 2 Ag-109 0.0 0.000000 +22 1 2 Xe-135 0.0 0.000000 +23 1 2 Cs-133 0.0 0.000000 +24 1 2 Nd-143 0.0 0.000000 +25 1 2 Nd-145 0.0 0.000000 +26 1 2 Sm-147 0.0 0.000000 +27 1 2 Sm-149 0.0 0.000000 +28 1 2 Sm-150 0.0 0.000000 +29 1 2 Sm-151 0.0 0.000000 +30 1 2 Sm-152 0.0 0.000000 +31 1 2 Eu-153 0.0 0.000000 +32 1 2 Gd-155 0.0 0.000000 +33 1 2 O-16 0.0 0.000000 material group in nuclide mean std. dev. +5 2 1 Zr-90 0.104734 0.008915 +6 2 1 Zr-91 0.036155 0.003735 +7 2 1 Zr-92 0.042422 0.003029 +8 2 1 Zr-94 0.046148 0.006251 +9 2 1 Zr-96 0.007794 0.001536 +0 2 2 Zr-90 0.121688 0.034934 +1 2 2 Zr-91 0.061792 0.024317 +2 2 2 Zr-92 0.041633 0.016323 +3 2 2 Zr-94 0.060818 0.021483 4 2 2 Zr-96 0.000000 0.000000 material group in nuclide mean std. dev. -5 2 1 Zr-90 0 0 -6 2 1 Zr-91 0 0 -7 2 1 Zr-92 0 0 -8 2 1 Zr-94 0 0 -9 2 1 Zr-96 0 0 -0 2 2 Zr-90 0 0 -1 2 2 Zr-91 0 0 -2 2 2 Zr-92 0 0 -3 2 2 Zr-94 0 0 -4 2 2 Zr-96 0 0 material group in group out nuclide mean std. dev. -15 2 1 1 Zr-90 0.118578 0.008347 -16 2 1 1 Zr-91 0.039963 0.003053 -17 2 1 1 Zr-92 0.033882 0.004365 -18 2 1 1 Zr-94 0.046281 0.005422 -19 2 1 1 Zr-96 0.004953 0.002087 +5 2 1 Zr-90 0.0 0.0 +6 2 1 Zr-91 0.0 0.0 +7 2 1 Zr-92 0.0 0.0 +8 2 1 Zr-94 0.0 0.0 +9 2 1 Zr-96 0.0 0.0 +0 2 2 Zr-90 0.0 0.0 +1 2 2 Zr-91 0.0 0.0 +2 2 2 Zr-92 0.0 0.0 +3 2 2 Zr-94 0.0 0.0 +4 2 2 Zr-96 0.0 0.0 material group in group out nuclide mean std. dev. +15 2 1 1 Zr-90 0.104734 0.008915 +16 2 1 1 Zr-91 0.036155 0.003735 +17 2 1 1 Zr-92 0.042422 0.003029 +18 2 1 1 Zr-94 0.046148 0.006251 +19 2 1 1 Zr-96 0.007794 0.001536 10 2 1 2 Zr-90 0.000000 0.000000 11 2 1 2 Zr-91 0.000000 0.000000 12 2 1 2 Zr-92 0.000000 0.000000 @@ -374,1007 +374,1007 @@ 7 2 2 1 Zr-92 0.000000 0.000000 8 2 2 1 Zr-94 0.000000 0.000000 9 2 2 1 Zr-96 0.000000 0.000000 -0 2 2 2 Zr-90 0.122479 0.032627 -1 2 2 2 Zr-91 0.023998 0.011915 -2 2 2 2 Zr-92 0.049331 0.021936 -3 2 2 2 Zr-94 0.058978 0.020081 +0 2 2 2 Zr-90 0.121688 0.034934 +1 2 2 2 Zr-91 0.061792 0.024317 +2 2 2 2 Zr-92 0.041633 0.016323 +3 2 2 2 Zr-94 0.060818 0.021483 4 2 2 2 Zr-96 0.000000 0.000000 material group out nuclide mean std. dev. -5 2 1 Zr-90 0 0 -6 2 1 Zr-91 0 0 -7 2 1 Zr-92 0 0 -8 2 1 Zr-94 0 0 -9 2 1 Zr-96 0 0 -0 2 2 Zr-90 0 0 -1 2 2 Zr-91 0 0 -2 2 2 Zr-92 0 0 -3 2 2 Zr-94 0 0 -4 2 2 Zr-96 0 0 material group in nuclide mean std. dev. -4 3 1 H-1 0.206179 0.034791 -5 3 1 O-16 0.075190 0.004750 -6 3 1 B-10 0.000741 0.000470 -7 3 1 B-11 0.000167 0.000208 -0 3 2 H-1 1.323003 0.239067 -1 3 2 O-16 0.071243 0.013291 -2 3 2 B-10 0.033075 0.004283 -3 3 2 B-11 0.000000 0.000000 material group in nuclide mean std. dev. -4 3 1 H-1 0 0 -5 3 1 O-16 0 0 -6 3 1 B-10 0 0 -7 3 1 B-11 0 0 -0 3 2 H-1 0 0 -1 3 2 O-16 0 0 -2 3 2 B-10 0 0 -3 3 2 B-11 0 0 material group in group out nuclide mean std. dev. -12 3 1 1 H-1 0.178758 0.033618 -13 3 1 1 O-16 0.075042 0.004782 +5 2 1 Zr-90 0.0 0.0 +6 2 1 Zr-91 0.0 0.0 +7 2 1 Zr-92 0.0 0.0 +8 2 1 Zr-94 0.0 0.0 +9 2 1 Zr-96 0.0 0.0 +0 2 2 Zr-90 0.0 0.0 +1 2 2 Zr-91 0.0 0.0 +2 2 2 Zr-92 0.0 0.0 +3 2 2 Zr-94 0.0 0.0 +4 2 2 Zr-96 0.0 0.0 material group in nuclide mean std. dev. +4 3 1 H-1 0.207103 0.023028 +5 3 1 O-16 0.079282 0.005197 +6 3 1 B-10 0.000521 0.000244 +7 3 1 B-11 0.000000 0.000000 +0 3 2 H-1 1.283344 0.250946 +1 3 2 O-16 0.085363 0.014001 +2 3 2 B-10 0.049249 0.008232 +3 3 2 B-11 0.000195 0.001527 material group in nuclide mean std. dev. +4 3 1 H-1 0.0 0.0 +5 3 1 O-16 0.0 0.0 +6 3 1 B-10 0.0 0.0 +7 3 1 B-11 0.0 0.0 +0 3 2 H-1 0.0 0.0 +1 3 2 O-16 0.0 0.0 +2 3 2 B-10 0.0 0.0 +3 3 2 B-11 0.0 0.0 material group in group out nuclide mean std. dev. +12 3 1 1 H-1 0.181306 0.022102 +13 3 1 1 O-16 0.078631 0.005044 14 3 1 1 B-10 0.000000 0.000000 -15 3 1 1 B-11 0.000167 0.000208 -8 3 1 2 H-1 0.027124 0.001806 -9 3 1 2 O-16 0.000148 0.000148 +15 3 1 1 B-11 0.000000 0.000000 +8 3 1 2 H-1 0.025666 0.001582 +9 3 1 2 O-16 0.000521 0.000131 10 3 1 2 B-10 0.000000 0.000000 11 3 1 2 B-11 0.000000 0.000000 4 3 2 1 H-1 0.000000 0.000000 5 3 2 1 O-16 0.000000 0.000000 6 3 2 1 B-10 0.000000 0.000000 7 3 2 1 B-11 0.000000 0.000000 -0 3 2 2 H-1 1.305284 0.235145 -1 3 2 2 O-16 0.071243 0.013291 +0 3 2 2 H-1 1.273963 0.250623 +1 3 2 2 O-16 0.085363 0.014001 2 3 2 2 B-10 0.000000 0.000000 -3 3 2 2 B-11 0.000000 0.000000 material group out nuclide mean std. dev. -4 3 1 H-1 0 0 -5 3 1 O-16 0 0 -6 3 1 B-10 0 0 -7 3 1 B-11 0 0 -0 3 2 H-1 0 0 -1 3 2 O-16 0 0 -2 3 2 B-10 0 0 -3 3 2 B-11 0 0 material group in nuclide mean std. dev. -4 4 1 H-1 0.188813 0.045599 -5 4 1 O-16 0.066636 0.008217 -6 4 1 B-10 0.000232 0.000233 -7 4 1 B-11 0.000042 0.000300 -0 4 2 H-1 1.088920 0.221595 -1 4 2 O-16 0.064481 0.014318 -2 4 2 B-10 0.026367 0.010478 +3 3 2 2 B-11 0.000195 0.001527 material group out nuclide mean std. dev. +4 3 1 H-1 0.0 0.0 +5 3 1 O-16 0.0 0.0 +6 3 1 B-10 0.0 0.0 +7 3 1 B-11 0.0 0.0 +0 3 2 H-1 0.0 0.0 +1 3 2 O-16 0.0 0.0 +2 3 2 B-10 0.0 0.0 +3 3 2 B-11 0.0 0.0 material group in nuclide mean std. dev. +4 4 1 H-1 0.175242 0.053715 +5 4 1 O-16 0.066545 0.010083 +6 4 1 B-10 0.000570 0.000352 +7 4 1 B-11 0.000089 0.000346 +0 4 2 H-1 1.142895 0.365140 +1 4 2 O-16 0.085141 0.028073 +2 4 2 B-10 0.025923 0.007276 3 4 2 B-11 0.000000 0.000000 material group in nuclide mean std. dev. -4 4 1 H-1 0 0 -5 4 1 O-16 0 0 -6 4 1 B-10 0 0 -7 4 1 B-11 0 0 -0 4 2 H-1 0 0 -1 4 2 O-16 0 0 -2 4 2 B-10 0 0 -3 4 2 B-11 0 0 material group in group out nuclide mean std. dev. -12 4 1 1 H-1 0.166764 0.043861 -13 4 1 1 O-16 0.066172 0.007943 +4 4 1 H-1 0.0 0.0 +5 4 1 O-16 0.0 0.0 +6 4 1 B-10 0.0 0.0 +7 4 1 B-11 0.0 0.0 +0 4 2 H-1 0.0 0.0 +1 4 2 O-16 0.0 0.0 +2 4 2 B-10 0.0 0.0 +3 4 2 B-11 0.0 0.0 material group in group out nuclide mean std. dev. +12 4 1 1 H-1 0.151295 0.051491 +13 4 1 1 O-16 0.066545 0.010083 14 4 1 1 B-10 0.000000 0.000000 -15 4 1 1 B-11 0.000042 0.000300 -8 4 1 2 H-1 0.021817 0.002327 -9 4 1 2 O-16 0.000464 0.000466 +15 4 1 1 B-11 0.000089 0.000346 +8 4 1 2 H-1 0.023662 0.003083 +9 4 1 2 O-16 0.000000 0.000000 10 4 1 2 B-10 0.000000 0.000000 11 4 1 2 B-11 0.000000 0.000000 4 4 2 1 H-1 0.000000 0.000000 5 4 2 1 O-16 0.000000 0.000000 6 4 2 1 B-10 0.000000 0.000000 7 4 2 1 B-11 0.000000 0.000000 -0 4 2 2 H-1 1.082328 0.222438 -1 4 2 2 O-16 0.064481 0.014318 +0 4 2 2 H-1 1.129933 0.361681 +1 4 2 2 O-16 0.085141 0.028073 2 4 2 2 B-10 0.000000 0.000000 3 4 2 2 B-11 0.000000 0.000000 material group out nuclide mean std. dev. -4 4 1 H-1 0 0 -5 4 1 O-16 0 0 -6 4 1 B-10 0 0 -7 4 1 B-11 0 0 -0 4 2 H-1 0 0 -1 4 2 O-16 0 0 -2 4 2 B-10 0 0 -3 4 2 B-11 0 0 material group in nuclide mean std. dev. -27 5 1 Fe-54 0 0 -28 5 1 Fe-56 0 0 -29 5 1 Fe-57 0 0 -30 5 1 Fe-58 0 0 -31 5 1 Ni-58 0 0 -32 5 1 Ni-60 0 0 -33 5 1 Ni-61 0 0 -34 5 1 Ni-62 0 0 -35 5 1 Ni-64 0 0 -36 5 1 Mn-55 0 0 -37 5 1 Mo-92 0 0 -38 5 1 Mo-94 0 0 -39 5 1 Mo-95 0 0 -40 5 1 Mo-96 0 0 -41 5 1 Mo-97 0 0 -42 5 1 Mo-98 0 0 -43 5 1 Mo-100 0 0 -44 5 1 Si-28 0 0 -45 5 1 Si-29 0 0 -46 5 1 Si-30 0 0 -47 5 1 Cr-50 0 0 -48 5 1 Cr-52 0 0 -49 5 1 Cr-53 0 0 -50 5 1 Cr-54 0 0 -51 5 1 C-Nat 0 0 -52 5 1 Cu-63 0 0 -53 5 1 Cu-65 0 0 -0 5 2 Fe-54 0 0 -1 5 2 Fe-56 0 0 -2 5 2 Fe-57 0 0 -3 5 2 Fe-58 0 0 -4 5 2 Ni-58 0 0 -5 5 2 Ni-60 0 0 -6 5 2 Ni-61 0 0 -7 5 2 Ni-62 0 0 -8 5 2 Ni-64 0 0 -9 5 2 Mn-55 0 0 -10 5 2 Mo-92 0 0 -11 5 2 Mo-94 0 0 -12 5 2 Mo-95 0 0 -13 5 2 Mo-96 0 0 -14 5 2 Mo-97 0 0 -15 5 2 Mo-98 0 0 -16 5 2 Mo-100 0 0 -17 5 2 Si-28 0 0 -18 5 2 Si-29 0 0 -19 5 2 Si-30 0 0 -20 5 2 Cr-50 0 0 -21 5 2 Cr-52 0 0 -22 5 2 Cr-53 0 0 -23 5 2 Cr-54 0 0 -24 5 2 C-Nat 0 0 -25 5 2 Cu-63 0 0 -26 5 2 Cu-65 0 0 material group in nuclide mean std. dev. -27 5 1 Fe-54 0 0 -28 5 1 Fe-56 0 0 -29 5 1 Fe-57 0 0 -30 5 1 Fe-58 0 0 -31 5 1 Ni-58 0 0 -32 5 1 Ni-60 0 0 -33 5 1 Ni-61 0 0 -34 5 1 Ni-62 0 0 -35 5 1 Ni-64 0 0 -36 5 1 Mn-55 0 0 -37 5 1 Mo-92 0 0 -38 5 1 Mo-94 0 0 -39 5 1 Mo-95 0 0 -40 5 1 Mo-96 0 0 -41 5 1 Mo-97 0 0 -42 5 1 Mo-98 0 0 -43 5 1 Mo-100 0 0 -44 5 1 Si-28 0 0 -45 5 1 Si-29 0 0 -46 5 1 Si-30 0 0 -47 5 1 Cr-50 0 0 -48 5 1 Cr-52 0 0 -49 5 1 Cr-53 0 0 -50 5 1 Cr-54 0 0 -51 5 1 C-Nat 0 0 -52 5 1 Cu-63 0 0 -53 5 1 Cu-65 0 0 -0 5 2 Fe-54 0 0 -1 5 2 Fe-56 0 0 -2 5 2 Fe-57 0 0 -3 5 2 Fe-58 0 0 -4 5 2 Ni-58 0 0 -5 5 2 Ni-60 0 0 -6 5 2 Ni-61 0 0 -7 5 2 Ni-62 0 0 -8 5 2 Ni-64 0 0 -9 5 2 Mn-55 0 0 -10 5 2 Mo-92 0 0 -11 5 2 Mo-94 0 0 -12 5 2 Mo-95 0 0 -13 5 2 Mo-96 0 0 -14 5 2 Mo-97 0 0 -15 5 2 Mo-98 0 0 -16 5 2 Mo-100 0 0 -17 5 2 Si-28 0 0 -18 5 2 Si-29 0 0 -19 5 2 Si-30 0 0 -20 5 2 Cr-50 0 0 -21 5 2 Cr-52 0 0 -22 5 2 Cr-53 0 0 -23 5 2 Cr-54 0 0 -24 5 2 C-Nat 0 0 -25 5 2 Cu-63 0 0 -26 5 2 Cu-65 0 0 material group in group out nuclide mean std. dev. -81 5 1 1 Fe-54 0 0 -82 5 1 1 Fe-56 0 0 -83 5 1 1 Fe-57 0 0 -84 5 1 1 Fe-58 0 0 -85 5 1 1 Ni-58 0 0 -86 5 1 1 Ni-60 0 0 -87 5 1 1 Ni-61 0 0 -88 5 1 1 Ni-62 0 0 -89 5 1 1 Ni-64 0 0 -90 5 1 1 Mn-55 0 0 -91 5 1 1 Mo-92 0 0 -92 5 1 1 Mo-94 0 0 -93 5 1 1 Mo-95 0 0 -94 5 1 1 Mo-96 0 0 -95 5 1 1 Mo-97 0 0 -96 5 1 1 Mo-98 0 0 -97 5 1 1 Mo-100 0 0 -98 5 1 1 Si-28 0 0 -99 5 1 1 Si-29 0 0 -100 5 1 1 Si-30 0 0 -101 5 1 1 Cr-50 0 0 -102 5 1 1 Cr-52 0 0 -103 5 1 1 Cr-53 0 0 -104 5 1 1 Cr-54 0 0 -105 5 1 1 C-Nat 0 0 -106 5 1 1 Cu-63 0 0 -107 5 1 1 Cu-65 0 0 -54 5 1 2 Fe-54 0 0 -55 5 1 2 Fe-56 0 0 -56 5 1 2 Fe-57 0 0 -57 5 1 2 Fe-58 0 0 -58 5 1 2 Ni-58 0 0 -59 5 1 2 Ni-60 0 0 -60 5 1 2 Ni-61 0 0 -61 5 1 2 Ni-62 0 0 -62 5 1 2 Ni-64 0 0 -63 5 1 2 Mn-55 0 0 -64 5 1 2 Mo-92 0 0 -65 5 1 2 Mo-94 0 0 -66 5 1 2 Mo-95 0 0 -67 5 1 2 Mo-96 0 0 -68 5 1 2 Mo-97 0 0 -69 5 1 2 Mo-98 0 0 -70 5 1 2 Mo-100 0 0 -71 5 1 2 Si-28 0 0 -72 5 1 2 Si-29 0 0 -73 5 1 2 Si-30 0 0 -74 5 1 2 Cr-50 0 0 -75 5 1 2 Cr-52 0 0 -76 5 1 2 Cr-53 0 0 -77 5 1 2 Cr-54 0 0 -78 5 1 2 C-Nat 0 0 -79 5 1 2 Cu-63 0 0 -80 5 1 2 Cu-65 0 0 -27 5 2 1 Fe-54 0 0 -28 5 2 1 Fe-56 0 0 -29 5 2 1 Fe-57 0 0 -30 5 2 1 Fe-58 0 0 -31 5 2 1 Ni-58 0 0 -32 5 2 1 Ni-60 0 0 -33 5 2 1 Ni-61 0 0 -34 5 2 1 Ni-62 0 0 -35 5 2 1 Ni-64 0 0 -36 5 2 1 Mn-55 0 0 -37 5 2 1 Mo-92 0 0 -38 5 2 1 Mo-94 0 0 -39 5 2 1 Mo-95 0 0 -40 5 2 1 Mo-96 0 0 -41 5 2 1 Mo-97 0 0 -42 5 2 1 Mo-98 0 0 -43 5 2 1 Mo-100 0 0 -44 5 2 1 Si-28 0 0 -45 5 2 1 Si-29 0 0 -46 5 2 1 Si-30 0 0 -47 5 2 1 Cr-50 0 0 -48 5 2 1 Cr-52 0 0 -49 5 2 1 Cr-53 0 0 -50 5 2 1 Cr-54 0 0 -51 5 2 1 C-Nat 0 0 -52 5 2 1 Cu-63 0 0 -53 5 2 1 Cu-65 0 0 -0 5 2 2 Fe-54 0 0 -1 5 2 2 Fe-56 0 0 -2 5 2 2 Fe-57 0 0 -3 5 2 2 Fe-58 0 0 -4 5 2 2 Ni-58 0 0 -5 5 2 2 Ni-60 0 0 -6 5 2 2 Ni-61 0 0 -7 5 2 2 Ni-62 0 0 -8 5 2 2 Ni-64 0 0 -9 5 2 2 Mn-55 0 0 -10 5 2 2 Mo-92 0 0 -11 5 2 2 Mo-94 0 0 -12 5 2 2 Mo-95 0 0 -13 5 2 2 Mo-96 0 0 -14 5 2 2 Mo-97 0 0 -15 5 2 2 Mo-98 0 0 -16 5 2 2 Mo-100 0 0 -17 5 2 2 Si-28 0 0 -18 5 2 2 Si-29 0 0 -19 5 2 2 Si-30 0 0 -20 5 2 2 Cr-50 0 0 -21 5 2 2 Cr-52 0 0 -22 5 2 2 Cr-53 0 0 -23 5 2 2 Cr-54 0 0 -24 5 2 2 C-Nat 0 0 -25 5 2 2 Cu-63 0 0 -26 5 2 2 Cu-65 0 0 material group out nuclide mean std. dev. -27 5 1 Fe-54 0 0 -28 5 1 Fe-56 0 0 -29 5 1 Fe-57 0 0 -30 5 1 Fe-58 0 0 -31 5 1 Ni-58 0 0 -32 5 1 Ni-60 0 0 -33 5 1 Ni-61 0 0 -34 5 1 Ni-62 0 0 -35 5 1 Ni-64 0 0 -36 5 1 Mn-55 0 0 -37 5 1 Mo-92 0 0 -38 5 1 Mo-94 0 0 -39 5 1 Mo-95 0 0 -40 5 1 Mo-96 0 0 -41 5 1 Mo-97 0 0 -42 5 1 Mo-98 0 0 -43 5 1 Mo-100 0 0 -44 5 1 Si-28 0 0 -45 5 1 Si-29 0 0 -46 5 1 Si-30 0 0 -47 5 1 Cr-50 0 0 -48 5 1 Cr-52 0 0 -49 5 1 Cr-53 0 0 -50 5 1 Cr-54 0 0 -51 5 1 C-Nat 0 0 -52 5 1 Cu-63 0 0 -53 5 1 Cu-65 0 0 -0 5 2 Fe-54 0 0 -1 5 2 Fe-56 0 0 -2 5 2 Fe-57 0 0 -3 5 2 Fe-58 0 0 -4 5 2 Ni-58 0 0 -5 5 2 Ni-60 0 0 -6 5 2 Ni-61 0 0 -7 5 2 Ni-62 0 0 -8 5 2 Ni-64 0 0 -9 5 2 Mn-55 0 0 -10 5 2 Mo-92 0 0 -11 5 2 Mo-94 0 0 -12 5 2 Mo-95 0 0 -13 5 2 Mo-96 0 0 -14 5 2 Mo-97 0 0 -15 5 2 Mo-98 0 0 -16 5 2 Mo-100 0 0 -17 5 2 Si-28 0 0 -18 5 2 Si-29 0 0 -19 5 2 Si-30 0 0 -20 5 2 Cr-50 0 0 -21 5 2 Cr-52 0 0 -22 5 2 Cr-53 0 0 -23 5 2 Cr-54 0 0 -24 5 2 C-Nat 0 0 -25 5 2 Cu-63 0 0 -26 5 2 Cu-65 0 0 material group in nuclide mean std. dev. -21 6 1 H-1 0 0 -22 6 1 O-16 0 0 -23 6 1 B-10 0 0 -24 6 1 B-11 0 0 -25 6 1 Fe-54 0 0 -26 6 1 Fe-56 0 0 -27 6 1 Fe-57 0 0 -28 6 1 Fe-58 0 0 -29 6 1 Ni-58 0 0 -30 6 1 Ni-60 0 0 -31 6 1 Ni-61 0 0 -32 6 1 Ni-62 0 0 -33 6 1 Ni-64 0 0 -34 6 1 Mn-55 0 0 -35 6 1 Si-28 0 0 -36 6 1 Si-29 0 0 -37 6 1 Si-30 0 0 -38 6 1 Cr-50 0 0 -39 6 1 Cr-52 0 0 -40 6 1 Cr-53 0 0 -41 6 1 Cr-54 0 0 -0 6 2 H-1 0 0 -1 6 2 O-16 0 0 -2 6 2 B-10 0 0 -3 6 2 B-11 0 0 -4 6 2 Fe-54 0 0 -5 6 2 Fe-56 0 0 -6 6 2 Fe-57 0 0 -7 6 2 Fe-58 0 0 -8 6 2 Ni-58 0 0 -9 6 2 Ni-60 0 0 -10 6 2 Ni-61 0 0 -11 6 2 Ni-62 0 0 -12 6 2 Ni-64 0 0 -13 6 2 Mn-55 0 0 -14 6 2 Si-28 0 0 -15 6 2 Si-29 0 0 -16 6 2 Si-30 0 0 -17 6 2 Cr-50 0 0 -18 6 2 Cr-52 0 0 -19 6 2 Cr-53 0 0 -20 6 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 6 1 H-1 0 0 -22 6 1 O-16 0 0 -23 6 1 B-10 0 0 -24 6 1 B-11 0 0 -25 6 1 Fe-54 0 0 -26 6 1 Fe-56 0 0 -27 6 1 Fe-57 0 0 -28 6 1 Fe-58 0 0 -29 6 1 Ni-58 0 0 -30 6 1 Ni-60 0 0 -31 6 1 Ni-61 0 0 -32 6 1 Ni-62 0 0 -33 6 1 Ni-64 0 0 -34 6 1 Mn-55 0 0 -35 6 1 Si-28 0 0 -36 6 1 Si-29 0 0 -37 6 1 Si-30 0 0 -38 6 1 Cr-50 0 0 -39 6 1 Cr-52 0 0 -40 6 1 Cr-53 0 0 -41 6 1 Cr-54 0 0 -0 6 2 H-1 0 0 -1 6 2 O-16 0 0 -2 6 2 B-10 0 0 -3 6 2 B-11 0 0 -4 6 2 Fe-54 0 0 -5 6 2 Fe-56 0 0 -6 6 2 Fe-57 0 0 -7 6 2 Fe-58 0 0 -8 6 2 Ni-58 0 0 -9 6 2 Ni-60 0 0 -10 6 2 Ni-61 0 0 -11 6 2 Ni-62 0 0 -12 6 2 Ni-64 0 0 -13 6 2 Mn-55 0 0 -14 6 2 Si-28 0 0 -15 6 2 Si-29 0 0 -16 6 2 Si-30 0 0 -17 6 2 Cr-50 0 0 -18 6 2 Cr-52 0 0 -19 6 2 Cr-53 0 0 -20 6 2 Cr-54 0 0 material group in group out nuclide mean std. dev. -63 6 1 1 H-1 0 0 -64 6 1 1 O-16 0 0 -65 6 1 1 B-10 0 0 -66 6 1 1 B-11 0 0 -67 6 1 1 Fe-54 0 0 -68 6 1 1 Fe-56 0 0 -69 6 1 1 Fe-57 0 0 -70 6 1 1 Fe-58 0 0 -71 6 1 1 Ni-58 0 0 -72 6 1 1 Ni-60 0 0 -73 6 1 1 Ni-61 0 0 -74 6 1 1 Ni-62 0 0 -75 6 1 1 Ni-64 0 0 -76 6 1 1 Mn-55 0 0 -77 6 1 1 Si-28 0 0 -78 6 1 1 Si-29 0 0 -79 6 1 1 Si-30 0 0 -80 6 1 1 Cr-50 0 0 -81 6 1 1 Cr-52 0 0 -82 6 1 1 Cr-53 0 0 -83 6 1 1 Cr-54 0 0 -42 6 1 2 H-1 0 0 -43 6 1 2 O-16 0 0 -44 6 1 2 B-10 0 0 -45 6 1 2 B-11 0 0 -46 6 1 2 Fe-54 0 0 -47 6 1 2 Fe-56 0 0 -48 6 1 2 Fe-57 0 0 -49 6 1 2 Fe-58 0 0 -50 6 1 2 Ni-58 0 0 -51 6 1 2 Ni-60 0 0 -52 6 1 2 Ni-61 0 0 -53 6 1 2 Ni-62 0 0 -54 6 1 2 Ni-64 0 0 -55 6 1 2 Mn-55 0 0 -56 6 1 2 Si-28 0 0 -57 6 1 2 Si-29 0 0 -58 6 1 2 Si-30 0 0 -59 6 1 2 Cr-50 0 0 -60 6 1 2 Cr-52 0 0 -61 6 1 2 Cr-53 0 0 -62 6 1 2 Cr-54 0 0 -21 6 2 1 H-1 0 0 -22 6 2 1 O-16 0 0 -23 6 2 1 B-10 0 0 -24 6 2 1 B-11 0 0 -25 6 2 1 Fe-54 0 0 -26 6 2 1 Fe-56 0 0 -27 6 2 1 Fe-57 0 0 -28 6 2 1 Fe-58 0 0 -29 6 2 1 Ni-58 0 0 -30 6 2 1 Ni-60 0 0 -31 6 2 1 Ni-61 0 0 -32 6 2 1 Ni-62 0 0 -33 6 2 1 Ni-64 0 0 -34 6 2 1 Mn-55 0 0 -35 6 2 1 Si-28 0 0 -36 6 2 1 Si-29 0 0 -37 6 2 1 Si-30 0 0 -38 6 2 1 Cr-50 0 0 -39 6 2 1 Cr-52 0 0 -40 6 2 1 Cr-53 0 0 -41 6 2 1 Cr-54 0 0 -0 6 2 2 H-1 0 0 -1 6 2 2 O-16 0 0 -2 6 2 2 B-10 0 0 -3 6 2 2 B-11 0 0 -4 6 2 2 Fe-54 0 0 -5 6 2 2 Fe-56 0 0 -6 6 2 2 Fe-57 0 0 -7 6 2 2 Fe-58 0 0 -8 6 2 2 Ni-58 0 0 -9 6 2 2 Ni-60 0 0 -10 6 2 2 Ni-61 0 0 -11 6 2 2 Ni-62 0 0 -12 6 2 2 Ni-64 0 0 -13 6 2 2 Mn-55 0 0 -14 6 2 2 Si-28 0 0 -15 6 2 2 Si-29 0 0 -16 6 2 2 Si-30 0 0 -17 6 2 2 Cr-50 0 0 -18 6 2 2 Cr-52 0 0 -19 6 2 2 Cr-53 0 0 -20 6 2 2 Cr-54 0 0 material group out nuclide mean std. dev. -21 6 1 H-1 0 0 -22 6 1 O-16 0 0 -23 6 1 B-10 0 0 -24 6 1 B-11 0 0 -25 6 1 Fe-54 0 0 -26 6 1 Fe-56 0 0 -27 6 1 Fe-57 0 0 -28 6 1 Fe-58 0 0 -29 6 1 Ni-58 0 0 -30 6 1 Ni-60 0 0 -31 6 1 Ni-61 0 0 -32 6 1 Ni-62 0 0 -33 6 1 Ni-64 0 0 -34 6 1 Mn-55 0 0 -35 6 1 Si-28 0 0 -36 6 1 Si-29 0 0 -37 6 1 Si-30 0 0 -38 6 1 Cr-50 0 0 -39 6 1 Cr-52 0 0 -40 6 1 Cr-53 0 0 -41 6 1 Cr-54 0 0 -0 6 2 H-1 0 0 -1 6 2 O-16 0 0 -2 6 2 B-10 0 0 -3 6 2 B-11 0 0 -4 6 2 Fe-54 0 0 -5 6 2 Fe-56 0 0 -6 6 2 Fe-57 0 0 -7 6 2 Fe-58 0 0 -8 6 2 Ni-58 0 0 -9 6 2 Ni-60 0 0 -10 6 2 Ni-61 0 0 -11 6 2 Ni-62 0 0 -12 6 2 Ni-64 0 0 -13 6 2 Mn-55 0 0 -14 6 2 Si-28 0 0 -15 6 2 Si-29 0 0 -16 6 2 Si-30 0 0 -17 6 2 Cr-50 0 0 -18 6 2 Cr-52 0 0 -19 6 2 Cr-53 0 0 -20 6 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 7 1 H-1 0 0 -22 7 1 O-16 0 0 -23 7 1 B-10 0 0 -24 7 1 B-11 0 0 -25 7 1 Fe-54 0 0 -26 7 1 Fe-56 0 0 -27 7 1 Fe-57 0 0 -28 7 1 Fe-58 0 0 -29 7 1 Ni-58 0 0 -30 7 1 Ni-60 0 0 -31 7 1 Ni-61 0 0 -32 7 1 Ni-62 0 0 -33 7 1 Ni-64 0 0 -34 7 1 Mn-55 0 0 -35 7 1 Si-28 0 0 -36 7 1 Si-29 0 0 -37 7 1 Si-30 0 0 -38 7 1 Cr-50 0 0 -39 7 1 Cr-52 0 0 -40 7 1 Cr-53 0 0 -41 7 1 Cr-54 0 0 -0 7 2 H-1 0 0 -1 7 2 O-16 0 0 -2 7 2 B-10 0 0 -3 7 2 B-11 0 0 -4 7 2 Fe-54 0 0 -5 7 2 Fe-56 0 0 -6 7 2 Fe-57 0 0 -7 7 2 Fe-58 0 0 -8 7 2 Ni-58 0 0 -9 7 2 Ni-60 0 0 -10 7 2 Ni-61 0 0 -11 7 2 Ni-62 0 0 -12 7 2 Ni-64 0 0 -13 7 2 Mn-55 0 0 -14 7 2 Si-28 0 0 -15 7 2 Si-29 0 0 -16 7 2 Si-30 0 0 -17 7 2 Cr-50 0 0 -18 7 2 Cr-52 0 0 -19 7 2 Cr-53 0 0 -20 7 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 7 1 H-1 0 0 -22 7 1 O-16 0 0 -23 7 1 B-10 0 0 -24 7 1 B-11 0 0 -25 7 1 Fe-54 0 0 -26 7 1 Fe-56 0 0 -27 7 1 Fe-57 0 0 -28 7 1 Fe-58 0 0 -29 7 1 Ni-58 0 0 -30 7 1 Ni-60 0 0 -31 7 1 Ni-61 0 0 -32 7 1 Ni-62 0 0 -33 7 1 Ni-64 0 0 -34 7 1 Mn-55 0 0 -35 7 1 Si-28 0 0 -36 7 1 Si-29 0 0 -37 7 1 Si-30 0 0 -38 7 1 Cr-50 0 0 -39 7 1 Cr-52 0 0 -40 7 1 Cr-53 0 0 -41 7 1 Cr-54 0 0 -0 7 2 H-1 0 0 -1 7 2 O-16 0 0 -2 7 2 B-10 0 0 -3 7 2 B-11 0 0 -4 7 2 Fe-54 0 0 -5 7 2 Fe-56 0 0 -6 7 2 Fe-57 0 0 -7 7 2 Fe-58 0 0 -8 7 2 Ni-58 0 0 -9 7 2 Ni-60 0 0 -10 7 2 Ni-61 0 0 -11 7 2 Ni-62 0 0 -12 7 2 Ni-64 0 0 -13 7 2 Mn-55 0 0 -14 7 2 Si-28 0 0 -15 7 2 Si-29 0 0 -16 7 2 Si-30 0 0 -17 7 2 Cr-50 0 0 -18 7 2 Cr-52 0 0 -19 7 2 Cr-53 0 0 -20 7 2 Cr-54 0 0 material group in group out nuclide mean std. dev. -63 7 1 1 H-1 0 0 -64 7 1 1 O-16 0 0 -65 7 1 1 B-10 0 0 -66 7 1 1 B-11 0 0 -67 7 1 1 Fe-54 0 0 -68 7 1 1 Fe-56 0 0 -69 7 1 1 Fe-57 0 0 -70 7 1 1 Fe-58 0 0 -71 7 1 1 Ni-58 0 0 -72 7 1 1 Ni-60 0 0 -73 7 1 1 Ni-61 0 0 -74 7 1 1 Ni-62 0 0 -75 7 1 1 Ni-64 0 0 -76 7 1 1 Mn-55 0 0 -77 7 1 1 Si-28 0 0 -78 7 1 1 Si-29 0 0 -79 7 1 1 Si-30 0 0 -80 7 1 1 Cr-50 0 0 -81 7 1 1 Cr-52 0 0 -82 7 1 1 Cr-53 0 0 -83 7 1 1 Cr-54 0 0 -42 7 1 2 H-1 0 0 -43 7 1 2 O-16 0 0 -44 7 1 2 B-10 0 0 -45 7 1 2 B-11 0 0 -46 7 1 2 Fe-54 0 0 -47 7 1 2 Fe-56 0 0 -48 7 1 2 Fe-57 0 0 -49 7 1 2 Fe-58 0 0 -50 7 1 2 Ni-58 0 0 -51 7 1 2 Ni-60 0 0 -52 7 1 2 Ni-61 0 0 -53 7 1 2 Ni-62 0 0 -54 7 1 2 Ni-64 0 0 -55 7 1 2 Mn-55 0 0 -56 7 1 2 Si-28 0 0 -57 7 1 2 Si-29 0 0 -58 7 1 2 Si-30 0 0 -59 7 1 2 Cr-50 0 0 -60 7 1 2 Cr-52 0 0 -61 7 1 2 Cr-53 0 0 -62 7 1 2 Cr-54 0 0 -21 7 2 1 H-1 0 0 -22 7 2 1 O-16 0 0 -23 7 2 1 B-10 0 0 -24 7 2 1 B-11 0 0 -25 7 2 1 Fe-54 0 0 -26 7 2 1 Fe-56 0 0 -27 7 2 1 Fe-57 0 0 -28 7 2 1 Fe-58 0 0 -29 7 2 1 Ni-58 0 0 -30 7 2 1 Ni-60 0 0 -31 7 2 1 Ni-61 0 0 -32 7 2 1 Ni-62 0 0 -33 7 2 1 Ni-64 0 0 -34 7 2 1 Mn-55 0 0 -35 7 2 1 Si-28 0 0 -36 7 2 1 Si-29 0 0 -37 7 2 1 Si-30 0 0 -38 7 2 1 Cr-50 0 0 -39 7 2 1 Cr-52 0 0 -40 7 2 1 Cr-53 0 0 -41 7 2 1 Cr-54 0 0 -0 7 2 2 H-1 0 0 -1 7 2 2 O-16 0 0 -2 7 2 2 B-10 0 0 -3 7 2 2 B-11 0 0 -4 7 2 2 Fe-54 0 0 -5 7 2 2 Fe-56 0 0 -6 7 2 2 Fe-57 0 0 -7 7 2 2 Fe-58 0 0 -8 7 2 2 Ni-58 0 0 -9 7 2 2 Ni-60 0 0 -10 7 2 2 Ni-61 0 0 -11 7 2 2 Ni-62 0 0 -12 7 2 2 Ni-64 0 0 -13 7 2 2 Mn-55 0 0 -14 7 2 2 Si-28 0 0 -15 7 2 2 Si-29 0 0 -16 7 2 2 Si-30 0 0 -17 7 2 2 Cr-50 0 0 -18 7 2 2 Cr-52 0 0 -19 7 2 2 Cr-53 0 0 -20 7 2 2 Cr-54 0 0 material group out nuclide mean std. dev. -21 7 1 H-1 0 0 -22 7 1 O-16 0 0 -23 7 1 B-10 0 0 -24 7 1 B-11 0 0 -25 7 1 Fe-54 0 0 -26 7 1 Fe-56 0 0 -27 7 1 Fe-57 0 0 -28 7 1 Fe-58 0 0 -29 7 1 Ni-58 0 0 -30 7 1 Ni-60 0 0 -31 7 1 Ni-61 0 0 -32 7 1 Ni-62 0 0 -33 7 1 Ni-64 0 0 -34 7 1 Mn-55 0 0 -35 7 1 Si-28 0 0 -36 7 1 Si-29 0 0 -37 7 1 Si-30 0 0 -38 7 1 Cr-50 0 0 -39 7 1 Cr-52 0 0 -40 7 1 Cr-53 0 0 -41 7 1 Cr-54 0 0 -0 7 2 H-1 0 0 -1 7 2 O-16 0 0 -2 7 2 B-10 0 0 -3 7 2 B-11 0 0 -4 7 2 Fe-54 0 0 -5 7 2 Fe-56 0 0 -6 7 2 Fe-57 0 0 -7 7 2 Fe-58 0 0 -8 7 2 Ni-58 0 0 -9 7 2 Ni-60 0 0 -10 7 2 Ni-61 0 0 -11 7 2 Ni-62 0 0 -12 7 2 Ni-64 0 0 -13 7 2 Mn-55 0 0 -14 7 2 Si-28 0 0 -15 7 2 Si-29 0 0 -16 7 2 Si-30 0 0 -17 7 2 Cr-50 0 0 -18 7 2 Cr-52 0 0 -19 7 2 Cr-53 0 0 -20 7 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 8 1 H-1 0 0 -22 8 1 O-16 0 0 -23 8 1 B-10 0 0 -24 8 1 B-11 0 0 -25 8 1 Fe-54 0 0 -26 8 1 Fe-56 0 0 -27 8 1 Fe-57 0 0 -28 8 1 Fe-58 0 0 -29 8 1 Ni-58 0 0 -30 8 1 Ni-60 0 0 -31 8 1 Ni-61 0 0 -32 8 1 Ni-62 0 0 -33 8 1 Ni-64 0 0 -34 8 1 Mn-55 0 0 -35 8 1 Si-28 0 0 -36 8 1 Si-29 0 0 -37 8 1 Si-30 0 0 -38 8 1 Cr-50 0 0 -39 8 1 Cr-52 0 0 -40 8 1 Cr-53 0 0 -41 8 1 Cr-54 0 0 -0 8 2 H-1 0 0 -1 8 2 O-16 0 0 -2 8 2 B-10 0 0 -3 8 2 B-11 0 0 -4 8 2 Fe-54 0 0 -5 8 2 Fe-56 0 0 -6 8 2 Fe-57 0 0 -7 8 2 Fe-58 0 0 -8 8 2 Ni-58 0 0 -9 8 2 Ni-60 0 0 -10 8 2 Ni-61 0 0 -11 8 2 Ni-62 0 0 -12 8 2 Ni-64 0 0 -13 8 2 Mn-55 0 0 -14 8 2 Si-28 0 0 -15 8 2 Si-29 0 0 -16 8 2 Si-30 0 0 -17 8 2 Cr-50 0 0 -18 8 2 Cr-52 0 0 -19 8 2 Cr-53 0 0 -20 8 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 8 1 H-1 0 0 -22 8 1 O-16 0 0 -23 8 1 B-10 0 0 -24 8 1 B-11 0 0 -25 8 1 Fe-54 0 0 -26 8 1 Fe-56 0 0 -27 8 1 Fe-57 0 0 -28 8 1 Fe-58 0 0 -29 8 1 Ni-58 0 0 -30 8 1 Ni-60 0 0 -31 8 1 Ni-61 0 0 -32 8 1 Ni-62 0 0 -33 8 1 Ni-64 0 0 -34 8 1 Mn-55 0 0 -35 8 1 Si-28 0 0 -36 8 1 Si-29 0 0 -37 8 1 Si-30 0 0 -38 8 1 Cr-50 0 0 -39 8 1 Cr-52 0 0 -40 8 1 Cr-53 0 0 -41 8 1 Cr-54 0 0 -0 8 2 H-1 0 0 -1 8 2 O-16 0 0 -2 8 2 B-10 0 0 -3 8 2 B-11 0 0 -4 8 2 Fe-54 0 0 -5 8 2 Fe-56 0 0 -6 8 2 Fe-57 0 0 -7 8 2 Fe-58 0 0 -8 8 2 Ni-58 0 0 -9 8 2 Ni-60 0 0 -10 8 2 Ni-61 0 0 -11 8 2 Ni-62 0 0 -12 8 2 Ni-64 0 0 -13 8 2 Mn-55 0 0 -14 8 2 Si-28 0 0 -15 8 2 Si-29 0 0 -16 8 2 Si-30 0 0 -17 8 2 Cr-50 0 0 -18 8 2 Cr-52 0 0 -19 8 2 Cr-53 0 0 -20 8 2 Cr-54 0 0 material group in group out nuclide mean std. dev. -63 8 1 1 H-1 0 0 -64 8 1 1 O-16 0 0 -65 8 1 1 B-10 0 0 -66 8 1 1 B-11 0 0 -67 8 1 1 Fe-54 0 0 -68 8 1 1 Fe-56 0 0 -69 8 1 1 Fe-57 0 0 -70 8 1 1 Fe-58 0 0 -71 8 1 1 Ni-58 0 0 -72 8 1 1 Ni-60 0 0 -73 8 1 1 Ni-61 0 0 -74 8 1 1 Ni-62 0 0 -75 8 1 1 Ni-64 0 0 -76 8 1 1 Mn-55 0 0 -77 8 1 1 Si-28 0 0 -78 8 1 1 Si-29 0 0 -79 8 1 1 Si-30 0 0 -80 8 1 1 Cr-50 0 0 -81 8 1 1 Cr-52 0 0 -82 8 1 1 Cr-53 0 0 -83 8 1 1 Cr-54 0 0 -42 8 1 2 H-1 0 0 -43 8 1 2 O-16 0 0 -44 8 1 2 B-10 0 0 -45 8 1 2 B-11 0 0 -46 8 1 2 Fe-54 0 0 -47 8 1 2 Fe-56 0 0 -48 8 1 2 Fe-57 0 0 -49 8 1 2 Fe-58 0 0 -50 8 1 2 Ni-58 0 0 -51 8 1 2 Ni-60 0 0 -52 8 1 2 Ni-61 0 0 -53 8 1 2 Ni-62 0 0 -54 8 1 2 Ni-64 0 0 -55 8 1 2 Mn-55 0 0 -56 8 1 2 Si-28 0 0 -57 8 1 2 Si-29 0 0 -58 8 1 2 Si-30 0 0 -59 8 1 2 Cr-50 0 0 -60 8 1 2 Cr-52 0 0 -61 8 1 2 Cr-53 0 0 -62 8 1 2 Cr-54 0 0 -21 8 2 1 H-1 0 0 -22 8 2 1 O-16 0 0 -23 8 2 1 B-10 0 0 -24 8 2 1 B-11 0 0 -25 8 2 1 Fe-54 0 0 -26 8 2 1 Fe-56 0 0 -27 8 2 1 Fe-57 0 0 -28 8 2 1 Fe-58 0 0 -29 8 2 1 Ni-58 0 0 -30 8 2 1 Ni-60 0 0 -31 8 2 1 Ni-61 0 0 -32 8 2 1 Ni-62 0 0 -33 8 2 1 Ni-64 0 0 -34 8 2 1 Mn-55 0 0 -35 8 2 1 Si-28 0 0 -36 8 2 1 Si-29 0 0 -37 8 2 1 Si-30 0 0 -38 8 2 1 Cr-50 0 0 -39 8 2 1 Cr-52 0 0 -40 8 2 1 Cr-53 0 0 -41 8 2 1 Cr-54 0 0 -0 8 2 2 H-1 0 0 -1 8 2 2 O-16 0 0 -2 8 2 2 B-10 0 0 -3 8 2 2 B-11 0 0 -4 8 2 2 Fe-54 0 0 -5 8 2 2 Fe-56 0 0 -6 8 2 2 Fe-57 0 0 -7 8 2 2 Fe-58 0 0 -8 8 2 2 Ni-58 0 0 -9 8 2 2 Ni-60 0 0 -10 8 2 2 Ni-61 0 0 -11 8 2 2 Ni-62 0 0 -12 8 2 2 Ni-64 0 0 -13 8 2 2 Mn-55 0 0 -14 8 2 2 Si-28 0 0 -15 8 2 2 Si-29 0 0 -16 8 2 2 Si-30 0 0 -17 8 2 2 Cr-50 0 0 -18 8 2 2 Cr-52 0 0 -19 8 2 2 Cr-53 0 0 -20 8 2 2 Cr-54 0 0 material group out nuclide mean std. dev. -21 8 1 H-1 0 0 -22 8 1 O-16 0 0 -23 8 1 B-10 0 0 -24 8 1 B-11 0 0 -25 8 1 Fe-54 0 0 -26 8 1 Fe-56 0 0 -27 8 1 Fe-57 0 0 -28 8 1 Fe-58 0 0 -29 8 1 Ni-58 0 0 -30 8 1 Ni-60 0 0 -31 8 1 Ni-61 0 0 -32 8 1 Ni-62 0 0 -33 8 1 Ni-64 0 0 -34 8 1 Mn-55 0 0 -35 8 1 Si-28 0 0 -36 8 1 Si-29 0 0 -37 8 1 Si-30 0 0 -38 8 1 Cr-50 0 0 -39 8 1 Cr-52 0 0 -40 8 1 Cr-53 0 0 -41 8 1 Cr-54 0 0 -0 8 2 H-1 0 0 -1 8 2 O-16 0 0 -2 8 2 B-10 0 0 -3 8 2 B-11 0 0 -4 8 2 Fe-54 0 0 -5 8 2 Fe-56 0 0 -6 8 2 Fe-57 0 0 -7 8 2 Fe-58 0 0 -8 8 2 Ni-58 0 0 -9 8 2 Ni-60 0 0 -10 8 2 Ni-61 0 0 -11 8 2 Ni-62 0 0 -12 8 2 Ni-64 0 0 -13 8 2 Mn-55 0 0 -14 8 2 Si-28 0 0 -15 8 2 Si-29 0 0 -16 8 2 Si-30 0 0 -17 8 2 Cr-50 0 0 -18 8 2 Cr-52 0 0 -19 8 2 Cr-53 0 0 -20 8 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 9 1 H-1 0.106160 0.179178 -22 9 1 O-16 0.272020 0.171699 +4 4 1 H-1 0.0 0.0 +5 4 1 O-16 0.0 0.0 +6 4 1 B-10 0.0 0.0 +7 4 1 B-11 0.0 0.0 +0 4 2 H-1 0.0 0.0 +1 4 2 O-16 0.0 0.0 +2 4 2 B-10 0.0 0.0 +3 4 2 B-11 0.0 0.0 material group in nuclide mean std. dev. +27 5 1 Fe-54 0.0 0.0 +28 5 1 Fe-56 0.0 0.0 +29 5 1 Fe-57 0.0 0.0 +30 5 1 Fe-58 0.0 0.0 +31 5 1 Ni-58 0.0 0.0 +32 5 1 Ni-60 0.0 0.0 +33 5 1 Ni-61 0.0 0.0 +34 5 1 Ni-62 0.0 0.0 +35 5 1 Ni-64 0.0 0.0 +36 5 1 Mn-55 0.0 0.0 +37 5 1 Mo-92 0.0 0.0 +38 5 1 Mo-94 0.0 0.0 +39 5 1 Mo-95 0.0 0.0 +40 5 1 Mo-96 0.0 0.0 +41 5 1 Mo-97 0.0 0.0 +42 5 1 Mo-98 0.0 0.0 +43 5 1 Mo-100 0.0 0.0 +44 5 1 Si-28 0.0 0.0 +45 5 1 Si-29 0.0 0.0 +46 5 1 Si-30 0.0 0.0 +47 5 1 Cr-50 0.0 0.0 +48 5 1 Cr-52 0.0 0.0 +49 5 1 Cr-53 0.0 0.0 +50 5 1 Cr-54 0.0 0.0 +51 5 1 C-Nat 0.0 0.0 +52 5 1 Cu-63 0.0 0.0 +53 5 1 Cu-65 0.0 0.0 +0 5 2 Fe-54 0.0 0.0 +1 5 2 Fe-56 0.0 0.0 +2 5 2 Fe-57 0.0 0.0 +3 5 2 Fe-58 0.0 0.0 +4 5 2 Ni-58 0.0 0.0 +5 5 2 Ni-60 0.0 0.0 +6 5 2 Ni-61 0.0 0.0 +7 5 2 Ni-62 0.0 0.0 +8 5 2 Ni-64 0.0 0.0 +9 5 2 Mn-55 0.0 0.0 +10 5 2 Mo-92 0.0 0.0 +11 5 2 Mo-94 0.0 0.0 +12 5 2 Mo-95 0.0 0.0 +13 5 2 Mo-96 0.0 0.0 +14 5 2 Mo-97 0.0 0.0 +15 5 2 Mo-98 0.0 0.0 +16 5 2 Mo-100 0.0 0.0 +17 5 2 Si-28 0.0 0.0 +18 5 2 Si-29 0.0 0.0 +19 5 2 Si-30 0.0 0.0 +20 5 2 Cr-50 0.0 0.0 +21 5 2 Cr-52 0.0 0.0 +22 5 2 Cr-53 0.0 0.0 +23 5 2 Cr-54 0.0 0.0 +24 5 2 C-Nat 0.0 0.0 +25 5 2 Cu-63 0.0 0.0 +26 5 2 Cu-65 0.0 0.0 material group in nuclide mean std. dev. +27 5 1 Fe-54 0.0 0.0 +28 5 1 Fe-56 0.0 0.0 +29 5 1 Fe-57 0.0 0.0 +30 5 1 Fe-58 0.0 0.0 +31 5 1 Ni-58 0.0 0.0 +32 5 1 Ni-60 0.0 0.0 +33 5 1 Ni-61 0.0 0.0 +34 5 1 Ni-62 0.0 0.0 +35 5 1 Ni-64 0.0 0.0 +36 5 1 Mn-55 0.0 0.0 +37 5 1 Mo-92 0.0 0.0 +38 5 1 Mo-94 0.0 0.0 +39 5 1 Mo-95 0.0 0.0 +40 5 1 Mo-96 0.0 0.0 +41 5 1 Mo-97 0.0 0.0 +42 5 1 Mo-98 0.0 0.0 +43 5 1 Mo-100 0.0 0.0 +44 5 1 Si-28 0.0 0.0 +45 5 1 Si-29 0.0 0.0 +46 5 1 Si-30 0.0 0.0 +47 5 1 Cr-50 0.0 0.0 +48 5 1 Cr-52 0.0 0.0 +49 5 1 Cr-53 0.0 0.0 +50 5 1 Cr-54 0.0 0.0 +51 5 1 C-Nat 0.0 0.0 +52 5 1 Cu-63 0.0 0.0 +53 5 1 Cu-65 0.0 0.0 +0 5 2 Fe-54 0.0 0.0 +1 5 2 Fe-56 0.0 0.0 +2 5 2 Fe-57 0.0 0.0 +3 5 2 Fe-58 0.0 0.0 +4 5 2 Ni-58 0.0 0.0 +5 5 2 Ni-60 0.0 0.0 +6 5 2 Ni-61 0.0 0.0 +7 5 2 Ni-62 0.0 0.0 +8 5 2 Ni-64 0.0 0.0 +9 5 2 Mn-55 0.0 0.0 +10 5 2 Mo-92 0.0 0.0 +11 5 2 Mo-94 0.0 0.0 +12 5 2 Mo-95 0.0 0.0 +13 5 2 Mo-96 0.0 0.0 +14 5 2 Mo-97 0.0 0.0 +15 5 2 Mo-98 0.0 0.0 +16 5 2 Mo-100 0.0 0.0 +17 5 2 Si-28 0.0 0.0 +18 5 2 Si-29 0.0 0.0 +19 5 2 Si-30 0.0 0.0 +20 5 2 Cr-50 0.0 0.0 +21 5 2 Cr-52 0.0 0.0 +22 5 2 Cr-53 0.0 0.0 +23 5 2 Cr-54 0.0 0.0 +24 5 2 C-Nat 0.0 0.0 +25 5 2 Cu-63 0.0 0.0 +26 5 2 Cu-65 0.0 0.0 material group in group out nuclide mean std. dev. +81 5 1 1 Fe-54 0.0 0.0 +82 5 1 1 Fe-56 0.0 0.0 +83 5 1 1 Fe-57 0.0 0.0 +84 5 1 1 Fe-58 0.0 0.0 +85 5 1 1 Ni-58 0.0 0.0 +86 5 1 1 Ni-60 0.0 0.0 +87 5 1 1 Ni-61 0.0 0.0 +88 5 1 1 Ni-62 0.0 0.0 +89 5 1 1 Ni-64 0.0 0.0 +90 5 1 1 Mn-55 0.0 0.0 +91 5 1 1 Mo-92 0.0 0.0 +92 5 1 1 Mo-94 0.0 0.0 +93 5 1 1 Mo-95 0.0 0.0 +94 5 1 1 Mo-96 0.0 0.0 +95 5 1 1 Mo-97 0.0 0.0 +96 5 1 1 Mo-98 0.0 0.0 +97 5 1 1 Mo-100 0.0 0.0 +98 5 1 1 Si-28 0.0 0.0 +99 5 1 1 Si-29 0.0 0.0 +100 5 1 1 Si-30 0.0 0.0 +101 5 1 1 Cr-50 0.0 0.0 +102 5 1 1 Cr-52 0.0 0.0 +103 5 1 1 Cr-53 0.0 0.0 +104 5 1 1 Cr-54 0.0 0.0 +105 5 1 1 C-Nat 0.0 0.0 +106 5 1 1 Cu-63 0.0 0.0 +107 5 1 1 Cu-65 0.0 0.0 +54 5 1 2 Fe-54 0.0 0.0 +55 5 1 2 Fe-56 0.0 0.0 +56 5 1 2 Fe-57 0.0 0.0 +57 5 1 2 Fe-58 0.0 0.0 +58 5 1 2 Ni-58 0.0 0.0 +59 5 1 2 Ni-60 0.0 0.0 +60 5 1 2 Ni-61 0.0 0.0 +61 5 1 2 Ni-62 0.0 0.0 +62 5 1 2 Ni-64 0.0 0.0 +63 5 1 2 Mn-55 0.0 0.0 +64 5 1 2 Mo-92 0.0 0.0 +65 5 1 2 Mo-94 0.0 0.0 +66 5 1 2 Mo-95 0.0 0.0 +67 5 1 2 Mo-96 0.0 0.0 +68 5 1 2 Mo-97 0.0 0.0 +69 5 1 2 Mo-98 0.0 0.0 +70 5 1 2 Mo-100 0.0 0.0 +71 5 1 2 Si-28 0.0 0.0 +72 5 1 2 Si-29 0.0 0.0 +73 5 1 2 Si-30 0.0 0.0 +74 5 1 2 Cr-50 0.0 0.0 +75 5 1 2 Cr-52 0.0 0.0 +76 5 1 2 Cr-53 0.0 0.0 +77 5 1 2 Cr-54 0.0 0.0 +78 5 1 2 C-Nat 0.0 0.0 +79 5 1 2 Cu-63 0.0 0.0 +80 5 1 2 Cu-65 0.0 0.0 +27 5 2 1 Fe-54 0.0 0.0 +28 5 2 1 Fe-56 0.0 0.0 +29 5 2 1 Fe-57 0.0 0.0 +30 5 2 1 Fe-58 0.0 0.0 +31 5 2 1 Ni-58 0.0 0.0 +32 5 2 1 Ni-60 0.0 0.0 +33 5 2 1 Ni-61 0.0 0.0 +34 5 2 1 Ni-62 0.0 0.0 +35 5 2 1 Ni-64 0.0 0.0 +36 5 2 1 Mn-55 0.0 0.0 +37 5 2 1 Mo-92 0.0 0.0 +38 5 2 1 Mo-94 0.0 0.0 +39 5 2 1 Mo-95 0.0 0.0 +40 5 2 1 Mo-96 0.0 0.0 +41 5 2 1 Mo-97 0.0 0.0 +42 5 2 1 Mo-98 0.0 0.0 +43 5 2 1 Mo-100 0.0 0.0 +44 5 2 1 Si-28 0.0 0.0 +45 5 2 1 Si-29 0.0 0.0 +46 5 2 1 Si-30 0.0 0.0 +47 5 2 1 Cr-50 0.0 0.0 +48 5 2 1 Cr-52 0.0 0.0 +49 5 2 1 Cr-53 0.0 0.0 +50 5 2 1 Cr-54 0.0 0.0 +51 5 2 1 C-Nat 0.0 0.0 +52 5 2 1 Cu-63 0.0 0.0 +53 5 2 1 Cu-65 0.0 0.0 +0 5 2 2 Fe-54 0.0 0.0 +1 5 2 2 Fe-56 0.0 0.0 +2 5 2 2 Fe-57 0.0 0.0 +3 5 2 2 Fe-58 0.0 0.0 +4 5 2 2 Ni-58 0.0 0.0 +5 5 2 2 Ni-60 0.0 0.0 +6 5 2 2 Ni-61 0.0 0.0 +7 5 2 2 Ni-62 0.0 0.0 +8 5 2 2 Ni-64 0.0 0.0 +9 5 2 2 Mn-55 0.0 0.0 +10 5 2 2 Mo-92 0.0 0.0 +11 5 2 2 Mo-94 0.0 0.0 +12 5 2 2 Mo-95 0.0 0.0 +13 5 2 2 Mo-96 0.0 0.0 +14 5 2 2 Mo-97 0.0 0.0 +15 5 2 2 Mo-98 0.0 0.0 +16 5 2 2 Mo-100 0.0 0.0 +17 5 2 2 Si-28 0.0 0.0 +18 5 2 2 Si-29 0.0 0.0 +19 5 2 2 Si-30 0.0 0.0 +20 5 2 2 Cr-50 0.0 0.0 +21 5 2 2 Cr-52 0.0 0.0 +22 5 2 2 Cr-53 0.0 0.0 +23 5 2 2 Cr-54 0.0 0.0 +24 5 2 2 C-Nat 0.0 0.0 +25 5 2 2 Cu-63 0.0 0.0 +26 5 2 2 Cu-65 0.0 0.0 material group out nuclide mean std. dev. +27 5 1 Fe-54 0.0 0.0 +28 5 1 Fe-56 0.0 0.0 +29 5 1 Fe-57 0.0 0.0 +30 5 1 Fe-58 0.0 0.0 +31 5 1 Ni-58 0.0 0.0 +32 5 1 Ni-60 0.0 0.0 +33 5 1 Ni-61 0.0 0.0 +34 5 1 Ni-62 0.0 0.0 +35 5 1 Ni-64 0.0 0.0 +36 5 1 Mn-55 0.0 0.0 +37 5 1 Mo-92 0.0 0.0 +38 5 1 Mo-94 0.0 0.0 +39 5 1 Mo-95 0.0 0.0 +40 5 1 Mo-96 0.0 0.0 +41 5 1 Mo-97 0.0 0.0 +42 5 1 Mo-98 0.0 0.0 +43 5 1 Mo-100 0.0 0.0 +44 5 1 Si-28 0.0 0.0 +45 5 1 Si-29 0.0 0.0 +46 5 1 Si-30 0.0 0.0 +47 5 1 Cr-50 0.0 0.0 +48 5 1 Cr-52 0.0 0.0 +49 5 1 Cr-53 0.0 0.0 +50 5 1 Cr-54 0.0 0.0 +51 5 1 C-Nat 0.0 0.0 +52 5 1 Cu-63 0.0 0.0 +53 5 1 Cu-65 0.0 0.0 +0 5 2 Fe-54 0.0 0.0 +1 5 2 Fe-56 0.0 0.0 +2 5 2 Fe-57 0.0 0.0 +3 5 2 Fe-58 0.0 0.0 +4 5 2 Ni-58 0.0 0.0 +5 5 2 Ni-60 0.0 0.0 +6 5 2 Ni-61 0.0 0.0 +7 5 2 Ni-62 0.0 0.0 +8 5 2 Ni-64 0.0 0.0 +9 5 2 Mn-55 0.0 0.0 +10 5 2 Mo-92 0.0 0.0 +11 5 2 Mo-94 0.0 0.0 +12 5 2 Mo-95 0.0 0.0 +13 5 2 Mo-96 0.0 0.0 +14 5 2 Mo-97 0.0 0.0 +15 5 2 Mo-98 0.0 0.0 +16 5 2 Mo-100 0.0 0.0 +17 5 2 Si-28 0.0 0.0 +18 5 2 Si-29 0.0 0.0 +19 5 2 Si-30 0.0 0.0 +20 5 2 Cr-50 0.0 0.0 +21 5 2 Cr-52 0.0 0.0 +22 5 2 Cr-53 0.0 0.0 +23 5 2 Cr-54 0.0 0.0 +24 5 2 C-Nat 0.0 0.0 +25 5 2 Cu-63 0.0 0.0 +26 5 2 Cu-65 0.0 0.0 material group in nuclide mean std. dev. +21 6 1 H-1 0.0 0.0 +22 6 1 O-16 0.0 0.0 +23 6 1 B-10 0.0 0.0 +24 6 1 B-11 0.0 0.0 +25 6 1 Fe-54 0.0 0.0 +26 6 1 Fe-56 0.0 0.0 +27 6 1 Fe-57 0.0 0.0 +28 6 1 Fe-58 0.0 0.0 +29 6 1 Ni-58 0.0 0.0 +30 6 1 Ni-60 0.0 0.0 +31 6 1 Ni-61 0.0 0.0 +32 6 1 Ni-62 0.0 0.0 +33 6 1 Ni-64 0.0 0.0 +34 6 1 Mn-55 0.0 0.0 +35 6 1 Si-28 0.0 0.0 +36 6 1 Si-29 0.0 0.0 +37 6 1 Si-30 0.0 0.0 +38 6 1 Cr-50 0.0 0.0 +39 6 1 Cr-52 0.0 0.0 +40 6 1 Cr-53 0.0 0.0 +41 6 1 Cr-54 0.0 0.0 +0 6 2 H-1 0.0 0.0 +1 6 2 O-16 0.0 0.0 +2 6 2 B-10 0.0 0.0 +3 6 2 B-11 0.0 0.0 +4 6 2 Fe-54 0.0 0.0 +5 6 2 Fe-56 0.0 0.0 +6 6 2 Fe-57 0.0 0.0 +7 6 2 Fe-58 0.0 0.0 +8 6 2 Ni-58 0.0 0.0 +9 6 2 Ni-60 0.0 0.0 +10 6 2 Ni-61 0.0 0.0 +11 6 2 Ni-62 0.0 0.0 +12 6 2 Ni-64 0.0 0.0 +13 6 2 Mn-55 0.0 0.0 +14 6 2 Si-28 0.0 0.0 +15 6 2 Si-29 0.0 0.0 +16 6 2 Si-30 0.0 0.0 +17 6 2 Cr-50 0.0 0.0 +18 6 2 Cr-52 0.0 0.0 +19 6 2 Cr-53 0.0 0.0 +20 6 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 6 1 H-1 0.0 0.0 +22 6 1 O-16 0.0 0.0 +23 6 1 B-10 0.0 0.0 +24 6 1 B-11 0.0 0.0 +25 6 1 Fe-54 0.0 0.0 +26 6 1 Fe-56 0.0 0.0 +27 6 1 Fe-57 0.0 0.0 +28 6 1 Fe-58 0.0 0.0 +29 6 1 Ni-58 0.0 0.0 +30 6 1 Ni-60 0.0 0.0 +31 6 1 Ni-61 0.0 0.0 +32 6 1 Ni-62 0.0 0.0 +33 6 1 Ni-64 0.0 0.0 +34 6 1 Mn-55 0.0 0.0 +35 6 1 Si-28 0.0 0.0 +36 6 1 Si-29 0.0 0.0 +37 6 1 Si-30 0.0 0.0 +38 6 1 Cr-50 0.0 0.0 +39 6 1 Cr-52 0.0 0.0 +40 6 1 Cr-53 0.0 0.0 +41 6 1 Cr-54 0.0 0.0 +0 6 2 H-1 0.0 0.0 +1 6 2 O-16 0.0 0.0 +2 6 2 B-10 0.0 0.0 +3 6 2 B-11 0.0 0.0 +4 6 2 Fe-54 0.0 0.0 +5 6 2 Fe-56 0.0 0.0 +6 6 2 Fe-57 0.0 0.0 +7 6 2 Fe-58 0.0 0.0 +8 6 2 Ni-58 0.0 0.0 +9 6 2 Ni-60 0.0 0.0 +10 6 2 Ni-61 0.0 0.0 +11 6 2 Ni-62 0.0 0.0 +12 6 2 Ni-64 0.0 0.0 +13 6 2 Mn-55 0.0 0.0 +14 6 2 Si-28 0.0 0.0 +15 6 2 Si-29 0.0 0.0 +16 6 2 Si-30 0.0 0.0 +17 6 2 Cr-50 0.0 0.0 +18 6 2 Cr-52 0.0 0.0 +19 6 2 Cr-53 0.0 0.0 +20 6 2 Cr-54 0.0 0.0 material group in group out nuclide mean std. dev. +63 6 1 1 H-1 0.0 0.0 +64 6 1 1 O-16 0.0 0.0 +65 6 1 1 B-10 0.0 0.0 +66 6 1 1 B-11 0.0 0.0 +67 6 1 1 Fe-54 0.0 0.0 +68 6 1 1 Fe-56 0.0 0.0 +69 6 1 1 Fe-57 0.0 0.0 +70 6 1 1 Fe-58 0.0 0.0 +71 6 1 1 Ni-58 0.0 0.0 +72 6 1 1 Ni-60 0.0 0.0 +73 6 1 1 Ni-61 0.0 0.0 +74 6 1 1 Ni-62 0.0 0.0 +75 6 1 1 Ni-64 0.0 0.0 +76 6 1 1 Mn-55 0.0 0.0 +77 6 1 1 Si-28 0.0 0.0 +78 6 1 1 Si-29 0.0 0.0 +79 6 1 1 Si-30 0.0 0.0 +80 6 1 1 Cr-50 0.0 0.0 +81 6 1 1 Cr-52 0.0 0.0 +82 6 1 1 Cr-53 0.0 0.0 +83 6 1 1 Cr-54 0.0 0.0 +42 6 1 2 H-1 0.0 0.0 +43 6 1 2 O-16 0.0 0.0 +44 6 1 2 B-10 0.0 0.0 +45 6 1 2 B-11 0.0 0.0 +46 6 1 2 Fe-54 0.0 0.0 +47 6 1 2 Fe-56 0.0 0.0 +48 6 1 2 Fe-57 0.0 0.0 +49 6 1 2 Fe-58 0.0 0.0 +50 6 1 2 Ni-58 0.0 0.0 +51 6 1 2 Ni-60 0.0 0.0 +52 6 1 2 Ni-61 0.0 0.0 +53 6 1 2 Ni-62 0.0 0.0 +54 6 1 2 Ni-64 0.0 0.0 +55 6 1 2 Mn-55 0.0 0.0 +56 6 1 2 Si-28 0.0 0.0 +57 6 1 2 Si-29 0.0 0.0 +58 6 1 2 Si-30 0.0 0.0 +59 6 1 2 Cr-50 0.0 0.0 +60 6 1 2 Cr-52 0.0 0.0 +61 6 1 2 Cr-53 0.0 0.0 +62 6 1 2 Cr-54 0.0 0.0 +21 6 2 1 H-1 0.0 0.0 +22 6 2 1 O-16 0.0 0.0 +23 6 2 1 B-10 0.0 0.0 +24 6 2 1 B-11 0.0 0.0 +25 6 2 1 Fe-54 0.0 0.0 +26 6 2 1 Fe-56 0.0 0.0 +27 6 2 1 Fe-57 0.0 0.0 +28 6 2 1 Fe-58 0.0 0.0 +29 6 2 1 Ni-58 0.0 0.0 +30 6 2 1 Ni-60 0.0 0.0 +31 6 2 1 Ni-61 0.0 0.0 +32 6 2 1 Ni-62 0.0 0.0 +33 6 2 1 Ni-64 0.0 0.0 +34 6 2 1 Mn-55 0.0 0.0 +35 6 2 1 Si-28 0.0 0.0 +36 6 2 1 Si-29 0.0 0.0 +37 6 2 1 Si-30 0.0 0.0 +38 6 2 1 Cr-50 0.0 0.0 +39 6 2 1 Cr-52 0.0 0.0 +40 6 2 1 Cr-53 0.0 0.0 +41 6 2 1 Cr-54 0.0 0.0 +0 6 2 2 H-1 0.0 0.0 +1 6 2 2 O-16 0.0 0.0 +2 6 2 2 B-10 0.0 0.0 +3 6 2 2 B-11 0.0 0.0 +4 6 2 2 Fe-54 0.0 0.0 +5 6 2 2 Fe-56 0.0 0.0 +6 6 2 2 Fe-57 0.0 0.0 +7 6 2 2 Fe-58 0.0 0.0 +8 6 2 2 Ni-58 0.0 0.0 +9 6 2 2 Ni-60 0.0 0.0 +10 6 2 2 Ni-61 0.0 0.0 +11 6 2 2 Ni-62 0.0 0.0 +12 6 2 2 Ni-64 0.0 0.0 +13 6 2 2 Mn-55 0.0 0.0 +14 6 2 2 Si-28 0.0 0.0 +15 6 2 2 Si-29 0.0 0.0 +16 6 2 2 Si-30 0.0 0.0 +17 6 2 2 Cr-50 0.0 0.0 +18 6 2 2 Cr-52 0.0 0.0 +19 6 2 2 Cr-53 0.0 0.0 +20 6 2 2 Cr-54 0.0 0.0 material group out nuclide mean std. dev. +21 6 1 H-1 0.0 0.0 +22 6 1 O-16 0.0 0.0 +23 6 1 B-10 0.0 0.0 +24 6 1 B-11 0.0 0.0 +25 6 1 Fe-54 0.0 0.0 +26 6 1 Fe-56 0.0 0.0 +27 6 1 Fe-57 0.0 0.0 +28 6 1 Fe-58 0.0 0.0 +29 6 1 Ni-58 0.0 0.0 +30 6 1 Ni-60 0.0 0.0 +31 6 1 Ni-61 0.0 0.0 +32 6 1 Ni-62 0.0 0.0 +33 6 1 Ni-64 0.0 0.0 +34 6 1 Mn-55 0.0 0.0 +35 6 1 Si-28 0.0 0.0 +36 6 1 Si-29 0.0 0.0 +37 6 1 Si-30 0.0 0.0 +38 6 1 Cr-50 0.0 0.0 +39 6 1 Cr-52 0.0 0.0 +40 6 1 Cr-53 0.0 0.0 +41 6 1 Cr-54 0.0 0.0 +0 6 2 H-1 0.0 0.0 +1 6 2 O-16 0.0 0.0 +2 6 2 B-10 0.0 0.0 +3 6 2 B-11 0.0 0.0 +4 6 2 Fe-54 0.0 0.0 +5 6 2 Fe-56 0.0 0.0 +6 6 2 Fe-57 0.0 0.0 +7 6 2 Fe-58 0.0 0.0 +8 6 2 Ni-58 0.0 0.0 +9 6 2 Ni-60 0.0 0.0 +10 6 2 Ni-61 0.0 0.0 +11 6 2 Ni-62 0.0 0.0 +12 6 2 Ni-64 0.0 0.0 +13 6 2 Mn-55 0.0 0.0 +14 6 2 Si-28 0.0 0.0 +15 6 2 Si-29 0.0 0.0 +16 6 2 Si-30 0.0 0.0 +17 6 2 Cr-50 0.0 0.0 +18 6 2 Cr-52 0.0 0.0 +19 6 2 Cr-53 0.0 0.0 +20 6 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 7 1 H-1 0.0 0.0 +22 7 1 O-16 0.0 0.0 +23 7 1 B-10 0.0 0.0 +24 7 1 B-11 0.0 0.0 +25 7 1 Fe-54 0.0 0.0 +26 7 1 Fe-56 0.0 0.0 +27 7 1 Fe-57 0.0 0.0 +28 7 1 Fe-58 0.0 0.0 +29 7 1 Ni-58 0.0 0.0 +30 7 1 Ni-60 0.0 0.0 +31 7 1 Ni-61 0.0 0.0 +32 7 1 Ni-62 0.0 0.0 +33 7 1 Ni-64 0.0 0.0 +34 7 1 Mn-55 0.0 0.0 +35 7 1 Si-28 0.0 0.0 +36 7 1 Si-29 0.0 0.0 +37 7 1 Si-30 0.0 0.0 +38 7 1 Cr-50 0.0 0.0 +39 7 1 Cr-52 0.0 0.0 +40 7 1 Cr-53 0.0 0.0 +41 7 1 Cr-54 0.0 0.0 +0 7 2 H-1 0.0 0.0 +1 7 2 O-16 0.0 0.0 +2 7 2 B-10 0.0 0.0 +3 7 2 B-11 0.0 0.0 +4 7 2 Fe-54 0.0 0.0 +5 7 2 Fe-56 0.0 0.0 +6 7 2 Fe-57 0.0 0.0 +7 7 2 Fe-58 0.0 0.0 +8 7 2 Ni-58 0.0 0.0 +9 7 2 Ni-60 0.0 0.0 +10 7 2 Ni-61 0.0 0.0 +11 7 2 Ni-62 0.0 0.0 +12 7 2 Ni-64 0.0 0.0 +13 7 2 Mn-55 0.0 0.0 +14 7 2 Si-28 0.0 0.0 +15 7 2 Si-29 0.0 0.0 +16 7 2 Si-30 0.0 0.0 +17 7 2 Cr-50 0.0 0.0 +18 7 2 Cr-52 0.0 0.0 +19 7 2 Cr-53 0.0 0.0 +20 7 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 7 1 H-1 0.0 0.0 +22 7 1 O-16 0.0 0.0 +23 7 1 B-10 0.0 0.0 +24 7 1 B-11 0.0 0.0 +25 7 1 Fe-54 0.0 0.0 +26 7 1 Fe-56 0.0 0.0 +27 7 1 Fe-57 0.0 0.0 +28 7 1 Fe-58 0.0 0.0 +29 7 1 Ni-58 0.0 0.0 +30 7 1 Ni-60 0.0 0.0 +31 7 1 Ni-61 0.0 0.0 +32 7 1 Ni-62 0.0 0.0 +33 7 1 Ni-64 0.0 0.0 +34 7 1 Mn-55 0.0 0.0 +35 7 1 Si-28 0.0 0.0 +36 7 1 Si-29 0.0 0.0 +37 7 1 Si-30 0.0 0.0 +38 7 1 Cr-50 0.0 0.0 +39 7 1 Cr-52 0.0 0.0 +40 7 1 Cr-53 0.0 0.0 +41 7 1 Cr-54 0.0 0.0 +0 7 2 H-1 0.0 0.0 +1 7 2 O-16 0.0 0.0 +2 7 2 B-10 0.0 0.0 +3 7 2 B-11 0.0 0.0 +4 7 2 Fe-54 0.0 0.0 +5 7 2 Fe-56 0.0 0.0 +6 7 2 Fe-57 0.0 0.0 +7 7 2 Fe-58 0.0 0.0 +8 7 2 Ni-58 0.0 0.0 +9 7 2 Ni-60 0.0 0.0 +10 7 2 Ni-61 0.0 0.0 +11 7 2 Ni-62 0.0 0.0 +12 7 2 Ni-64 0.0 0.0 +13 7 2 Mn-55 0.0 0.0 +14 7 2 Si-28 0.0 0.0 +15 7 2 Si-29 0.0 0.0 +16 7 2 Si-30 0.0 0.0 +17 7 2 Cr-50 0.0 0.0 +18 7 2 Cr-52 0.0 0.0 +19 7 2 Cr-53 0.0 0.0 +20 7 2 Cr-54 0.0 0.0 material group in group out nuclide mean std. dev. +63 7 1 1 H-1 0.0 0.0 +64 7 1 1 O-16 0.0 0.0 +65 7 1 1 B-10 0.0 0.0 +66 7 1 1 B-11 0.0 0.0 +67 7 1 1 Fe-54 0.0 0.0 +68 7 1 1 Fe-56 0.0 0.0 +69 7 1 1 Fe-57 0.0 0.0 +70 7 1 1 Fe-58 0.0 0.0 +71 7 1 1 Ni-58 0.0 0.0 +72 7 1 1 Ni-60 0.0 0.0 +73 7 1 1 Ni-61 0.0 0.0 +74 7 1 1 Ni-62 0.0 0.0 +75 7 1 1 Ni-64 0.0 0.0 +76 7 1 1 Mn-55 0.0 0.0 +77 7 1 1 Si-28 0.0 0.0 +78 7 1 1 Si-29 0.0 0.0 +79 7 1 1 Si-30 0.0 0.0 +80 7 1 1 Cr-50 0.0 0.0 +81 7 1 1 Cr-52 0.0 0.0 +82 7 1 1 Cr-53 0.0 0.0 +83 7 1 1 Cr-54 0.0 0.0 +42 7 1 2 H-1 0.0 0.0 +43 7 1 2 O-16 0.0 0.0 +44 7 1 2 B-10 0.0 0.0 +45 7 1 2 B-11 0.0 0.0 +46 7 1 2 Fe-54 0.0 0.0 +47 7 1 2 Fe-56 0.0 0.0 +48 7 1 2 Fe-57 0.0 0.0 +49 7 1 2 Fe-58 0.0 0.0 +50 7 1 2 Ni-58 0.0 0.0 +51 7 1 2 Ni-60 0.0 0.0 +52 7 1 2 Ni-61 0.0 0.0 +53 7 1 2 Ni-62 0.0 0.0 +54 7 1 2 Ni-64 0.0 0.0 +55 7 1 2 Mn-55 0.0 0.0 +56 7 1 2 Si-28 0.0 0.0 +57 7 1 2 Si-29 0.0 0.0 +58 7 1 2 Si-30 0.0 0.0 +59 7 1 2 Cr-50 0.0 0.0 +60 7 1 2 Cr-52 0.0 0.0 +61 7 1 2 Cr-53 0.0 0.0 +62 7 1 2 Cr-54 0.0 0.0 +21 7 2 1 H-1 0.0 0.0 +22 7 2 1 O-16 0.0 0.0 +23 7 2 1 B-10 0.0 0.0 +24 7 2 1 B-11 0.0 0.0 +25 7 2 1 Fe-54 0.0 0.0 +26 7 2 1 Fe-56 0.0 0.0 +27 7 2 1 Fe-57 0.0 0.0 +28 7 2 1 Fe-58 0.0 0.0 +29 7 2 1 Ni-58 0.0 0.0 +30 7 2 1 Ni-60 0.0 0.0 +31 7 2 1 Ni-61 0.0 0.0 +32 7 2 1 Ni-62 0.0 0.0 +33 7 2 1 Ni-64 0.0 0.0 +34 7 2 1 Mn-55 0.0 0.0 +35 7 2 1 Si-28 0.0 0.0 +36 7 2 1 Si-29 0.0 0.0 +37 7 2 1 Si-30 0.0 0.0 +38 7 2 1 Cr-50 0.0 0.0 +39 7 2 1 Cr-52 0.0 0.0 +40 7 2 1 Cr-53 0.0 0.0 +41 7 2 1 Cr-54 0.0 0.0 +0 7 2 2 H-1 0.0 0.0 +1 7 2 2 O-16 0.0 0.0 +2 7 2 2 B-10 0.0 0.0 +3 7 2 2 B-11 0.0 0.0 +4 7 2 2 Fe-54 0.0 0.0 +5 7 2 2 Fe-56 0.0 0.0 +6 7 2 2 Fe-57 0.0 0.0 +7 7 2 2 Fe-58 0.0 0.0 +8 7 2 2 Ni-58 0.0 0.0 +9 7 2 2 Ni-60 0.0 0.0 +10 7 2 2 Ni-61 0.0 0.0 +11 7 2 2 Ni-62 0.0 0.0 +12 7 2 2 Ni-64 0.0 0.0 +13 7 2 2 Mn-55 0.0 0.0 +14 7 2 2 Si-28 0.0 0.0 +15 7 2 2 Si-29 0.0 0.0 +16 7 2 2 Si-30 0.0 0.0 +17 7 2 2 Cr-50 0.0 0.0 +18 7 2 2 Cr-52 0.0 0.0 +19 7 2 2 Cr-53 0.0 0.0 +20 7 2 2 Cr-54 0.0 0.0 material group out nuclide mean std. dev. +21 7 1 H-1 0.0 0.0 +22 7 1 O-16 0.0 0.0 +23 7 1 B-10 0.0 0.0 +24 7 1 B-11 0.0 0.0 +25 7 1 Fe-54 0.0 0.0 +26 7 1 Fe-56 0.0 0.0 +27 7 1 Fe-57 0.0 0.0 +28 7 1 Fe-58 0.0 0.0 +29 7 1 Ni-58 0.0 0.0 +30 7 1 Ni-60 0.0 0.0 +31 7 1 Ni-61 0.0 0.0 +32 7 1 Ni-62 0.0 0.0 +33 7 1 Ni-64 0.0 0.0 +34 7 1 Mn-55 0.0 0.0 +35 7 1 Si-28 0.0 0.0 +36 7 1 Si-29 0.0 0.0 +37 7 1 Si-30 0.0 0.0 +38 7 1 Cr-50 0.0 0.0 +39 7 1 Cr-52 0.0 0.0 +40 7 1 Cr-53 0.0 0.0 +41 7 1 Cr-54 0.0 0.0 +0 7 2 H-1 0.0 0.0 +1 7 2 O-16 0.0 0.0 +2 7 2 B-10 0.0 0.0 +3 7 2 B-11 0.0 0.0 +4 7 2 Fe-54 0.0 0.0 +5 7 2 Fe-56 0.0 0.0 +6 7 2 Fe-57 0.0 0.0 +7 7 2 Fe-58 0.0 0.0 +8 7 2 Ni-58 0.0 0.0 +9 7 2 Ni-60 0.0 0.0 +10 7 2 Ni-61 0.0 0.0 +11 7 2 Ni-62 0.0 0.0 +12 7 2 Ni-64 0.0 0.0 +13 7 2 Mn-55 0.0 0.0 +14 7 2 Si-28 0.0 0.0 +15 7 2 Si-29 0.0 0.0 +16 7 2 Si-30 0.0 0.0 +17 7 2 Cr-50 0.0 0.0 +18 7 2 Cr-52 0.0 0.0 +19 7 2 Cr-53 0.0 0.0 +20 7 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 8 1 H-1 0.0 0.0 +22 8 1 O-16 0.0 0.0 +23 8 1 B-10 0.0 0.0 +24 8 1 B-11 0.0 0.0 +25 8 1 Fe-54 0.0 0.0 +26 8 1 Fe-56 0.0 0.0 +27 8 1 Fe-57 0.0 0.0 +28 8 1 Fe-58 0.0 0.0 +29 8 1 Ni-58 0.0 0.0 +30 8 1 Ni-60 0.0 0.0 +31 8 1 Ni-61 0.0 0.0 +32 8 1 Ni-62 0.0 0.0 +33 8 1 Ni-64 0.0 0.0 +34 8 1 Mn-55 0.0 0.0 +35 8 1 Si-28 0.0 0.0 +36 8 1 Si-29 0.0 0.0 +37 8 1 Si-30 0.0 0.0 +38 8 1 Cr-50 0.0 0.0 +39 8 1 Cr-52 0.0 0.0 +40 8 1 Cr-53 0.0 0.0 +41 8 1 Cr-54 0.0 0.0 +0 8 2 H-1 0.0 0.0 +1 8 2 O-16 0.0 0.0 +2 8 2 B-10 0.0 0.0 +3 8 2 B-11 0.0 0.0 +4 8 2 Fe-54 0.0 0.0 +5 8 2 Fe-56 0.0 0.0 +6 8 2 Fe-57 0.0 0.0 +7 8 2 Fe-58 0.0 0.0 +8 8 2 Ni-58 0.0 0.0 +9 8 2 Ni-60 0.0 0.0 +10 8 2 Ni-61 0.0 0.0 +11 8 2 Ni-62 0.0 0.0 +12 8 2 Ni-64 0.0 0.0 +13 8 2 Mn-55 0.0 0.0 +14 8 2 Si-28 0.0 0.0 +15 8 2 Si-29 0.0 0.0 +16 8 2 Si-30 0.0 0.0 +17 8 2 Cr-50 0.0 0.0 +18 8 2 Cr-52 0.0 0.0 +19 8 2 Cr-53 0.0 0.0 +20 8 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 8 1 H-1 0.0 0.0 +22 8 1 O-16 0.0 0.0 +23 8 1 B-10 0.0 0.0 +24 8 1 B-11 0.0 0.0 +25 8 1 Fe-54 0.0 0.0 +26 8 1 Fe-56 0.0 0.0 +27 8 1 Fe-57 0.0 0.0 +28 8 1 Fe-58 0.0 0.0 +29 8 1 Ni-58 0.0 0.0 +30 8 1 Ni-60 0.0 0.0 +31 8 1 Ni-61 0.0 0.0 +32 8 1 Ni-62 0.0 0.0 +33 8 1 Ni-64 0.0 0.0 +34 8 1 Mn-55 0.0 0.0 +35 8 1 Si-28 0.0 0.0 +36 8 1 Si-29 0.0 0.0 +37 8 1 Si-30 0.0 0.0 +38 8 1 Cr-50 0.0 0.0 +39 8 1 Cr-52 0.0 0.0 +40 8 1 Cr-53 0.0 0.0 +41 8 1 Cr-54 0.0 0.0 +0 8 2 H-1 0.0 0.0 +1 8 2 O-16 0.0 0.0 +2 8 2 B-10 0.0 0.0 +3 8 2 B-11 0.0 0.0 +4 8 2 Fe-54 0.0 0.0 +5 8 2 Fe-56 0.0 0.0 +6 8 2 Fe-57 0.0 0.0 +7 8 2 Fe-58 0.0 0.0 +8 8 2 Ni-58 0.0 0.0 +9 8 2 Ni-60 0.0 0.0 +10 8 2 Ni-61 0.0 0.0 +11 8 2 Ni-62 0.0 0.0 +12 8 2 Ni-64 0.0 0.0 +13 8 2 Mn-55 0.0 0.0 +14 8 2 Si-28 0.0 0.0 +15 8 2 Si-29 0.0 0.0 +16 8 2 Si-30 0.0 0.0 +17 8 2 Cr-50 0.0 0.0 +18 8 2 Cr-52 0.0 0.0 +19 8 2 Cr-53 0.0 0.0 +20 8 2 Cr-54 0.0 0.0 material group in group out nuclide mean std. dev. +63 8 1 1 H-1 0.0 0.0 +64 8 1 1 O-16 0.0 0.0 +65 8 1 1 B-10 0.0 0.0 +66 8 1 1 B-11 0.0 0.0 +67 8 1 1 Fe-54 0.0 0.0 +68 8 1 1 Fe-56 0.0 0.0 +69 8 1 1 Fe-57 0.0 0.0 +70 8 1 1 Fe-58 0.0 0.0 +71 8 1 1 Ni-58 0.0 0.0 +72 8 1 1 Ni-60 0.0 0.0 +73 8 1 1 Ni-61 0.0 0.0 +74 8 1 1 Ni-62 0.0 0.0 +75 8 1 1 Ni-64 0.0 0.0 +76 8 1 1 Mn-55 0.0 0.0 +77 8 1 1 Si-28 0.0 0.0 +78 8 1 1 Si-29 0.0 0.0 +79 8 1 1 Si-30 0.0 0.0 +80 8 1 1 Cr-50 0.0 0.0 +81 8 1 1 Cr-52 0.0 0.0 +82 8 1 1 Cr-53 0.0 0.0 +83 8 1 1 Cr-54 0.0 0.0 +42 8 1 2 H-1 0.0 0.0 +43 8 1 2 O-16 0.0 0.0 +44 8 1 2 B-10 0.0 0.0 +45 8 1 2 B-11 0.0 0.0 +46 8 1 2 Fe-54 0.0 0.0 +47 8 1 2 Fe-56 0.0 0.0 +48 8 1 2 Fe-57 0.0 0.0 +49 8 1 2 Fe-58 0.0 0.0 +50 8 1 2 Ni-58 0.0 0.0 +51 8 1 2 Ni-60 0.0 0.0 +52 8 1 2 Ni-61 0.0 0.0 +53 8 1 2 Ni-62 0.0 0.0 +54 8 1 2 Ni-64 0.0 0.0 +55 8 1 2 Mn-55 0.0 0.0 +56 8 1 2 Si-28 0.0 0.0 +57 8 1 2 Si-29 0.0 0.0 +58 8 1 2 Si-30 0.0 0.0 +59 8 1 2 Cr-50 0.0 0.0 +60 8 1 2 Cr-52 0.0 0.0 +61 8 1 2 Cr-53 0.0 0.0 +62 8 1 2 Cr-54 0.0 0.0 +21 8 2 1 H-1 0.0 0.0 +22 8 2 1 O-16 0.0 0.0 +23 8 2 1 B-10 0.0 0.0 +24 8 2 1 B-11 0.0 0.0 +25 8 2 1 Fe-54 0.0 0.0 +26 8 2 1 Fe-56 0.0 0.0 +27 8 2 1 Fe-57 0.0 0.0 +28 8 2 1 Fe-58 0.0 0.0 +29 8 2 1 Ni-58 0.0 0.0 +30 8 2 1 Ni-60 0.0 0.0 +31 8 2 1 Ni-61 0.0 0.0 +32 8 2 1 Ni-62 0.0 0.0 +33 8 2 1 Ni-64 0.0 0.0 +34 8 2 1 Mn-55 0.0 0.0 +35 8 2 1 Si-28 0.0 0.0 +36 8 2 1 Si-29 0.0 0.0 +37 8 2 1 Si-30 0.0 0.0 +38 8 2 1 Cr-50 0.0 0.0 +39 8 2 1 Cr-52 0.0 0.0 +40 8 2 1 Cr-53 0.0 0.0 +41 8 2 1 Cr-54 0.0 0.0 +0 8 2 2 H-1 0.0 0.0 +1 8 2 2 O-16 0.0 0.0 +2 8 2 2 B-10 0.0 0.0 +3 8 2 2 B-11 0.0 0.0 +4 8 2 2 Fe-54 0.0 0.0 +5 8 2 2 Fe-56 0.0 0.0 +6 8 2 2 Fe-57 0.0 0.0 +7 8 2 2 Fe-58 0.0 0.0 +8 8 2 2 Ni-58 0.0 0.0 +9 8 2 2 Ni-60 0.0 0.0 +10 8 2 2 Ni-61 0.0 0.0 +11 8 2 2 Ni-62 0.0 0.0 +12 8 2 2 Ni-64 0.0 0.0 +13 8 2 2 Mn-55 0.0 0.0 +14 8 2 2 Si-28 0.0 0.0 +15 8 2 2 Si-29 0.0 0.0 +16 8 2 2 Si-30 0.0 0.0 +17 8 2 2 Cr-50 0.0 0.0 +18 8 2 2 Cr-52 0.0 0.0 +19 8 2 2 Cr-53 0.0 0.0 +20 8 2 2 Cr-54 0.0 0.0 material group out nuclide mean std. dev. +21 8 1 H-1 0.0 0.0 +22 8 1 O-16 0.0 0.0 +23 8 1 B-10 0.0 0.0 +24 8 1 B-11 0.0 0.0 +25 8 1 Fe-54 0.0 0.0 +26 8 1 Fe-56 0.0 0.0 +27 8 1 Fe-57 0.0 0.0 +28 8 1 Fe-58 0.0 0.0 +29 8 1 Ni-58 0.0 0.0 +30 8 1 Ni-60 0.0 0.0 +31 8 1 Ni-61 0.0 0.0 +32 8 1 Ni-62 0.0 0.0 +33 8 1 Ni-64 0.0 0.0 +34 8 1 Mn-55 0.0 0.0 +35 8 1 Si-28 0.0 0.0 +36 8 1 Si-29 0.0 0.0 +37 8 1 Si-30 0.0 0.0 +38 8 1 Cr-50 0.0 0.0 +39 8 1 Cr-52 0.0 0.0 +40 8 1 Cr-53 0.0 0.0 +41 8 1 Cr-54 0.0 0.0 +0 8 2 H-1 0.0 0.0 +1 8 2 O-16 0.0 0.0 +2 8 2 B-10 0.0 0.0 +3 8 2 B-11 0.0 0.0 +4 8 2 Fe-54 0.0 0.0 +5 8 2 Fe-56 0.0 0.0 +6 8 2 Fe-57 0.0 0.0 +7 8 2 Fe-58 0.0 0.0 +8 8 2 Ni-58 0.0 0.0 +9 8 2 Ni-60 0.0 0.0 +10 8 2 Ni-61 0.0 0.0 +11 8 2 Ni-62 0.0 0.0 +12 8 2 Ni-64 0.0 0.0 +13 8 2 Mn-55 0.0 0.0 +14 8 2 Si-28 0.0 0.0 +15 8 2 Si-29 0.0 0.0 +16 8 2 Si-30 0.0 0.0 +17 8 2 Cr-50 0.0 0.0 +18 8 2 Cr-52 0.0 0.0 +19 8 2 Cr-53 0.0 0.0 +20 8 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 9 1 H-1 0.150655 0.480993 +22 9 1 O-16 0.116221 0.114089 23 9 1 B-10 0.000000 0.000000 24 9 1 B-11 0.000000 0.000000 25 9 1 Fe-54 0.000000 0.000000 -26 9 1 Fe-56 0.000000 0.000000 +26 9 1 Fe-56 0.186217 0.199795 27 9 1 Fe-57 0.000000 0.000000 28 9 1 Fe-58 0.000000 0.000000 29 9 1 Ni-58 0.000000 0.000000 @@ -1382,17 +1382,17 @@ 31 9 1 Ni-61 0.000000 0.000000 32 9 1 Ni-62 0.000000 0.000000 33 9 1 Ni-64 0.000000 0.000000 -34 9 1 Mn-55 0.085133 0.082479 +34 9 1 Mn-55 0.000000 0.000000 35 9 1 Si-28 0.000000 0.000000 36 9 1 Si-29 0.000000 0.000000 37 9 1 Si-30 0.000000 0.000000 38 9 1 Cr-50 0.000000 0.000000 39 9 1 Cr-52 0.000000 0.000000 -40 9 1 Cr-53 0.040723 0.079827 +40 9 1 Cr-53 0.147443 0.139574 41 9 1 Cr-54 0.000000 0.000000 -0 9 2 H-1 1.417955 2.158027 +0 9 2 H-1 0.000000 0.000000 1 9 2 O-16 0.000000 0.000000 -2 9 2 B-10 0.269141 0.380622 +2 9 2 B-10 0.000000 0.000000 3 9 2 B-11 0.000000 0.000000 4 9 2 Fe-54 0.000000 0.000000 5 9 2 Fe-56 0.000000 0.000000 @@ -1411,54 +1411,54 @@ 18 9 2 Cr-52 0.000000 0.000000 19 9 2 Cr-53 0.000000 0.000000 20 9 2 Cr-54 0.000000 0.000000 material group in nuclide mean std. dev. -21 9 1 H-1 0 0 -22 9 1 O-16 0 0 -23 9 1 B-10 0 0 -24 9 1 B-11 0 0 -25 9 1 Fe-54 0 0 -26 9 1 Fe-56 0 0 -27 9 1 Fe-57 0 0 -28 9 1 Fe-58 0 0 -29 9 1 Ni-58 0 0 -30 9 1 Ni-60 0 0 -31 9 1 Ni-61 0 0 -32 9 1 Ni-62 0 0 -33 9 1 Ni-64 0 0 -34 9 1 Mn-55 0 0 -35 9 1 Si-28 0 0 -36 9 1 Si-29 0 0 -37 9 1 Si-30 0 0 -38 9 1 Cr-50 0 0 -39 9 1 Cr-52 0 0 -40 9 1 Cr-53 0 0 -41 9 1 Cr-54 0 0 -0 9 2 H-1 0 0 -1 9 2 O-16 0 0 -2 9 2 B-10 0 0 -3 9 2 B-11 0 0 -4 9 2 Fe-54 0 0 -5 9 2 Fe-56 0 0 -6 9 2 Fe-57 0 0 -7 9 2 Fe-58 0 0 -8 9 2 Ni-58 0 0 -9 9 2 Ni-60 0 0 -10 9 2 Ni-61 0 0 -11 9 2 Ni-62 0 0 -12 9 2 Ni-64 0 0 -13 9 2 Mn-55 0 0 -14 9 2 Si-28 0 0 -15 9 2 Si-29 0 0 -16 9 2 Si-30 0 0 -17 9 2 Cr-50 0 0 -18 9 2 Cr-52 0 0 -19 9 2 Cr-53 0 0 -20 9 2 Cr-54 0 0 material group in group out nuclide mean std. dev. -63 9 1 1 H-1 0.106160 0.179178 -64 9 1 1 O-16 0.272020 0.171699 +21 9 1 H-1 0.0 0.0 +22 9 1 O-16 0.0 0.0 +23 9 1 B-10 0.0 0.0 +24 9 1 B-11 0.0 0.0 +25 9 1 Fe-54 0.0 0.0 +26 9 1 Fe-56 0.0 0.0 +27 9 1 Fe-57 0.0 0.0 +28 9 1 Fe-58 0.0 0.0 +29 9 1 Ni-58 0.0 0.0 +30 9 1 Ni-60 0.0 0.0 +31 9 1 Ni-61 0.0 0.0 +32 9 1 Ni-62 0.0 0.0 +33 9 1 Ni-64 0.0 0.0 +34 9 1 Mn-55 0.0 0.0 +35 9 1 Si-28 0.0 0.0 +36 9 1 Si-29 0.0 0.0 +37 9 1 Si-30 0.0 0.0 +38 9 1 Cr-50 0.0 0.0 +39 9 1 Cr-52 0.0 0.0 +40 9 1 Cr-53 0.0 0.0 +41 9 1 Cr-54 0.0 0.0 +0 9 2 H-1 0.0 0.0 +1 9 2 O-16 0.0 0.0 +2 9 2 B-10 0.0 0.0 +3 9 2 B-11 0.0 0.0 +4 9 2 Fe-54 0.0 0.0 +5 9 2 Fe-56 0.0 0.0 +6 9 2 Fe-57 0.0 0.0 +7 9 2 Fe-58 0.0 0.0 +8 9 2 Ni-58 0.0 0.0 +9 9 2 Ni-60 0.0 0.0 +10 9 2 Ni-61 0.0 0.0 +11 9 2 Ni-62 0.0 0.0 +12 9 2 Ni-64 0.0 0.0 +13 9 2 Mn-55 0.0 0.0 +14 9 2 Si-28 0.0 0.0 +15 9 2 Si-29 0.0 0.0 +16 9 2 Si-30 0.0 0.0 +17 9 2 Cr-50 0.0 0.0 +18 9 2 Cr-52 0.0 0.0 +19 9 2 Cr-53 0.0 0.0 +20 9 2 Cr-54 0.0 0.0 material group in group out nuclide mean std. dev. +63 9 1 1 H-1 0.150655 0.480993 +64 9 1 1 O-16 0.116221 0.114089 65 9 1 1 B-10 0.000000 0.000000 66 9 1 1 B-11 0.000000 0.000000 67 9 1 1 Fe-54 0.000000 0.000000 -68 9 1 1 Fe-56 0.000000 0.000000 +68 9 1 1 Fe-56 0.186217 0.199795 69 9 1 1 Fe-57 0.000000 0.000000 70 9 1 1 Fe-58 0.000000 0.000000 71 9 1 1 Ni-58 0.000000 0.000000 @@ -1466,13 +1466,13 @@ 73 9 1 1 Ni-61 0.000000 0.000000 74 9 1 1 Ni-62 0.000000 0.000000 75 9 1 1 Ni-64 0.000000 0.000000 -76 9 1 1 Mn-55 0.085133 0.082479 +76 9 1 1 Mn-55 0.000000 0.000000 77 9 1 1 Si-28 0.000000 0.000000 78 9 1 1 Si-29 0.000000 0.000000 79 9 1 1 Si-30 0.000000 0.000000 80 9 1 1 Cr-50 0.000000 0.000000 81 9 1 1 Cr-52 0.000000 0.000000 -82 9 1 1 Cr-53 0.040723 0.079827 +82 9 1 1 Cr-53 0.147443 0.139574 83 9 1 1 Cr-54 0.000000 0.000000 42 9 1 2 H-1 0.000000 0.000000 43 9 1 2 O-16 0.000000 0.000000 @@ -1516,7 +1516,7 @@ 39 9 2 1 Cr-52 0.000000 0.000000 40 9 2 1 Cr-53 0.000000 0.000000 41 9 2 1 Cr-54 0.000000 0.000000 -0 9 2 2 H-1 1.417955 2.158027 +0 9 2 2 H-1 0.000000 0.000000 1 9 2 2 O-16 0.000000 0.000000 2 9 2 2 B-10 0.000000 0.000000 3 9 2 2 B-11 0.000000 0.000000 @@ -1537,304 +1537,304 @@ 18 9 2 2 Cr-52 0.000000 0.000000 19 9 2 2 Cr-53 0.000000 0.000000 20 9 2 2 Cr-54 0.000000 0.000000 material group out nuclide mean std. dev. -21 9 1 H-1 0 0 -22 9 1 O-16 0 0 -23 9 1 B-10 0 0 -24 9 1 B-11 0 0 -25 9 1 Fe-54 0 0 -26 9 1 Fe-56 0 0 -27 9 1 Fe-57 0 0 -28 9 1 Fe-58 0 0 -29 9 1 Ni-58 0 0 -30 9 1 Ni-60 0 0 -31 9 1 Ni-61 0 0 -32 9 1 Ni-62 0 0 -33 9 1 Ni-64 0 0 -34 9 1 Mn-55 0 0 -35 9 1 Si-28 0 0 -36 9 1 Si-29 0 0 -37 9 1 Si-30 0 0 -38 9 1 Cr-50 0 0 -39 9 1 Cr-52 0 0 -40 9 1 Cr-53 0 0 -41 9 1 Cr-54 0 0 -0 9 2 H-1 0 0 -1 9 2 O-16 0 0 -2 9 2 B-10 0 0 -3 9 2 B-11 0 0 -4 9 2 Fe-54 0 0 -5 9 2 Fe-56 0 0 -6 9 2 Fe-57 0 0 -7 9 2 Fe-58 0 0 -8 9 2 Ni-58 0 0 -9 9 2 Ni-60 0 0 -10 9 2 Ni-61 0 0 -11 9 2 Ni-62 0 0 -12 9 2 Ni-64 0 0 -13 9 2 Mn-55 0 0 -14 9 2 Si-28 0 0 -15 9 2 Si-29 0 0 -16 9 2 Si-30 0 0 -17 9 2 Cr-50 0 0 -18 9 2 Cr-52 0 0 -19 9 2 Cr-53 0 0 -20 9 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 10 1 H-1 0 0 -22 10 1 O-16 0 0 -23 10 1 B-10 0 0 -24 10 1 B-11 0 0 -25 10 1 Fe-54 0 0 -26 10 1 Fe-56 0 0 -27 10 1 Fe-57 0 0 -28 10 1 Fe-58 0 0 -29 10 1 Ni-58 0 0 -30 10 1 Ni-60 0 0 -31 10 1 Ni-61 0 0 -32 10 1 Ni-62 0 0 -33 10 1 Ni-64 0 0 -34 10 1 Mn-55 0 0 -35 10 1 Si-28 0 0 -36 10 1 Si-29 0 0 -37 10 1 Si-30 0 0 -38 10 1 Cr-50 0 0 -39 10 1 Cr-52 0 0 -40 10 1 Cr-53 0 0 -41 10 1 Cr-54 0 0 -0 10 2 H-1 0 0 -1 10 2 O-16 0 0 -2 10 2 B-10 0 0 -3 10 2 B-11 0 0 -4 10 2 Fe-54 0 0 -5 10 2 Fe-56 0 0 -6 10 2 Fe-57 0 0 -7 10 2 Fe-58 0 0 -8 10 2 Ni-58 0 0 -9 10 2 Ni-60 0 0 -10 10 2 Ni-61 0 0 -11 10 2 Ni-62 0 0 -12 10 2 Ni-64 0 0 -13 10 2 Mn-55 0 0 -14 10 2 Si-28 0 0 -15 10 2 Si-29 0 0 -16 10 2 Si-30 0 0 -17 10 2 Cr-50 0 0 -18 10 2 Cr-52 0 0 -19 10 2 Cr-53 0 0 -20 10 2 Cr-54 0 0 material group in nuclide mean std. dev. -21 10 1 H-1 0 0 -22 10 1 O-16 0 0 -23 10 1 B-10 0 0 -24 10 1 B-11 0 0 -25 10 1 Fe-54 0 0 -26 10 1 Fe-56 0 0 -27 10 1 Fe-57 0 0 -28 10 1 Fe-58 0 0 -29 10 1 Ni-58 0 0 -30 10 1 Ni-60 0 0 -31 10 1 Ni-61 0 0 -32 10 1 Ni-62 0 0 -33 10 1 Ni-64 0 0 -34 10 1 Mn-55 0 0 -35 10 1 Si-28 0 0 -36 10 1 Si-29 0 0 -37 10 1 Si-30 0 0 -38 10 1 Cr-50 0 0 -39 10 1 Cr-52 0 0 -40 10 1 Cr-53 0 0 -41 10 1 Cr-54 0 0 -0 10 2 H-1 0 0 -1 10 2 O-16 0 0 -2 10 2 B-10 0 0 -3 10 2 B-11 0 0 -4 10 2 Fe-54 0 0 -5 10 2 Fe-56 0 0 -6 10 2 Fe-57 0 0 -7 10 2 Fe-58 0 0 -8 10 2 Ni-58 0 0 -9 10 2 Ni-60 0 0 -10 10 2 Ni-61 0 0 -11 10 2 Ni-62 0 0 -12 10 2 Ni-64 0 0 -13 10 2 Mn-55 0 0 -14 10 2 Si-28 0 0 -15 10 2 Si-29 0 0 -16 10 2 Si-30 0 0 -17 10 2 Cr-50 0 0 -18 10 2 Cr-52 0 0 -19 10 2 Cr-53 0 0 -20 10 2 Cr-54 0 0 material group in group out nuclide mean std. dev. -63 10 1 1 H-1 0 0 -64 10 1 1 O-16 0 0 -65 10 1 1 B-10 0 0 -66 10 1 1 B-11 0 0 -67 10 1 1 Fe-54 0 0 -68 10 1 1 Fe-56 0 0 -69 10 1 1 Fe-57 0 0 -70 10 1 1 Fe-58 0 0 -71 10 1 1 Ni-58 0 0 -72 10 1 1 Ni-60 0 0 -73 10 1 1 Ni-61 0 0 -74 10 1 1 Ni-62 0 0 -75 10 1 1 Ni-64 0 0 -76 10 1 1 Mn-55 0 0 -77 10 1 1 Si-28 0 0 -78 10 1 1 Si-29 0 0 -79 10 1 1 Si-30 0 0 -80 10 1 1 Cr-50 0 0 -81 10 1 1 Cr-52 0 0 -82 10 1 1 Cr-53 0 0 -83 10 1 1 Cr-54 0 0 -42 10 1 2 H-1 0 0 -43 10 1 2 O-16 0 0 -44 10 1 2 B-10 0 0 -45 10 1 2 B-11 0 0 -46 10 1 2 Fe-54 0 0 -47 10 1 2 Fe-56 0 0 -48 10 1 2 Fe-57 0 0 -49 10 1 2 Fe-58 0 0 -50 10 1 2 Ni-58 0 0 -51 10 1 2 Ni-60 0 0 -52 10 1 2 Ni-61 0 0 -53 10 1 2 Ni-62 0 0 -54 10 1 2 Ni-64 0 0 -55 10 1 2 Mn-55 0 0 -56 10 1 2 Si-28 0 0 -57 10 1 2 Si-29 0 0 -58 10 1 2 Si-30 0 0 -59 10 1 2 Cr-50 0 0 -60 10 1 2 Cr-52 0 0 -61 10 1 2 Cr-53 0 0 -62 10 1 2 Cr-54 0 0 -21 10 2 1 H-1 0 0 -22 10 2 1 O-16 0 0 -23 10 2 1 B-10 0 0 -24 10 2 1 B-11 0 0 -25 10 2 1 Fe-54 0 0 -26 10 2 1 Fe-56 0 0 -27 10 2 1 Fe-57 0 0 -28 10 2 1 Fe-58 0 0 -29 10 2 1 Ni-58 0 0 -30 10 2 1 Ni-60 0 0 -31 10 2 1 Ni-61 0 0 -32 10 2 1 Ni-62 0 0 -33 10 2 1 Ni-64 0 0 -34 10 2 1 Mn-55 0 0 -35 10 2 1 Si-28 0 0 -36 10 2 1 Si-29 0 0 -37 10 2 1 Si-30 0 0 -38 10 2 1 Cr-50 0 0 -39 10 2 1 Cr-52 0 0 -40 10 2 1 Cr-53 0 0 -41 10 2 1 Cr-54 0 0 -0 10 2 2 H-1 0 0 -1 10 2 2 O-16 0 0 -2 10 2 2 B-10 0 0 -3 10 2 2 B-11 0 0 -4 10 2 2 Fe-54 0 0 -5 10 2 2 Fe-56 0 0 -6 10 2 2 Fe-57 0 0 -7 10 2 2 Fe-58 0 0 -8 10 2 2 Ni-58 0 0 -9 10 2 2 Ni-60 0 0 -10 10 2 2 Ni-61 0 0 -11 10 2 2 Ni-62 0 0 -12 10 2 2 Ni-64 0 0 -13 10 2 2 Mn-55 0 0 -14 10 2 2 Si-28 0 0 -15 10 2 2 Si-29 0 0 -16 10 2 2 Si-30 0 0 -17 10 2 2 Cr-50 0 0 -18 10 2 2 Cr-52 0 0 -19 10 2 2 Cr-53 0 0 -20 10 2 2 Cr-54 0 0 material group out nuclide mean std. dev. -21 10 1 H-1 0 0 -22 10 1 O-16 0 0 -23 10 1 B-10 0 0 -24 10 1 B-11 0 0 -25 10 1 Fe-54 0 0 -26 10 1 Fe-56 0 0 -27 10 1 Fe-57 0 0 -28 10 1 Fe-58 0 0 -29 10 1 Ni-58 0 0 -30 10 1 Ni-60 0 0 -31 10 1 Ni-61 0 0 -32 10 1 Ni-62 0 0 -33 10 1 Ni-64 0 0 -34 10 1 Mn-55 0 0 -35 10 1 Si-28 0 0 -36 10 1 Si-29 0 0 -37 10 1 Si-30 0 0 -38 10 1 Cr-50 0 0 -39 10 1 Cr-52 0 0 -40 10 1 Cr-53 0 0 -41 10 1 Cr-54 0 0 -0 10 2 H-1 0 0 -1 10 2 O-16 0 0 -2 10 2 B-10 0 0 -3 10 2 B-11 0 0 -4 10 2 Fe-54 0 0 -5 10 2 Fe-56 0 0 -6 10 2 Fe-57 0 0 -7 10 2 Fe-58 0 0 -8 10 2 Ni-58 0 0 -9 10 2 Ni-60 0 0 -10 10 2 Ni-61 0 0 -11 10 2 Ni-62 0 0 -12 10 2 Ni-64 0 0 -13 10 2 Mn-55 0 0 -14 10 2 Si-28 0 0 -15 10 2 Si-29 0 0 -16 10 2 Si-30 0 0 -17 10 2 Cr-50 0 0 -18 10 2 Cr-52 0 0 -19 10 2 Cr-53 0 0 -20 10 2 Cr-54 0 0 material group in nuclide mean std. dev. -9 11 1 H-1 0.138558 0.260695 -10 11 1 O-16 0.042575 0.049271 +21 9 1 H-1 0.0 0.0 +22 9 1 O-16 0.0 0.0 +23 9 1 B-10 0.0 0.0 +24 9 1 B-11 0.0 0.0 +25 9 1 Fe-54 0.0 0.0 +26 9 1 Fe-56 0.0 0.0 +27 9 1 Fe-57 0.0 0.0 +28 9 1 Fe-58 0.0 0.0 +29 9 1 Ni-58 0.0 0.0 +30 9 1 Ni-60 0.0 0.0 +31 9 1 Ni-61 0.0 0.0 +32 9 1 Ni-62 0.0 0.0 +33 9 1 Ni-64 0.0 0.0 +34 9 1 Mn-55 0.0 0.0 +35 9 1 Si-28 0.0 0.0 +36 9 1 Si-29 0.0 0.0 +37 9 1 Si-30 0.0 0.0 +38 9 1 Cr-50 0.0 0.0 +39 9 1 Cr-52 0.0 0.0 +40 9 1 Cr-53 0.0 0.0 +41 9 1 Cr-54 0.0 0.0 +0 9 2 H-1 0.0 0.0 +1 9 2 O-16 0.0 0.0 +2 9 2 B-10 0.0 0.0 +3 9 2 B-11 0.0 0.0 +4 9 2 Fe-54 0.0 0.0 +5 9 2 Fe-56 0.0 0.0 +6 9 2 Fe-57 0.0 0.0 +7 9 2 Fe-58 0.0 0.0 +8 9 2 Ni-58 0.0 0.0 +9 9 2 Ni-60 0.0 0.0 +10 9 2 Ni-61 0.0 0.0 +11 9 2 Ni-62 0.0 0.0 +12 9 2 Ni-64 0.0 0.0 +13 9 2 Mn-55 0.0 0.0 +14 9 2 Si-28 0.0 0.0 +15 9 2 Si-29 0.0 0.0 +16 9 2 Si-30 0.0 0.0 +17 9 2 Cr-50 0.0 0.0 +18 9 2 Cr-52 0.0 0.0 +19 9 2 Cr-53 0.0 0.0 +20 9 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +21 10 1 H-1 0.123944 0.541390 +22 10 1 O-16 0.000000 0.000000 +23 10 1 B-10 0.000000 0.000000 +24 10 1 B-11 0.000000 0.000000 +25 10 1 Fe-54 0.000000 0.000000 +26 10 1 Fe-56 0.000000 0.000000 +27 10 1 Fe-57 0.000000 0.000000 +28 10 1 Fe-58 0.000000 0.000000 +29 10 1 Ni-58 0.000000 0.000000 +30 10 1 Ni-60 0.000000 0.000000 +31 10 1 Ni-61 0.000000 0.000000 +32 10 1 Ni-62 0.000000 0.000000 +33 10 1 Ni-64 0.000000 0.000000 +34 10 1 Mn-55 0.000000 0.000000 +35 10 1 Si-28 0.000000 0.000000 +36 10 1 Si-29 0.000000 0.000000 +37 10 1 Si-30 0.000000 0.000000 +38 10 1 Cr-50 0.111571 0.138458 +39 10 1 Cr-52 0.000000 0.000000 +40 10 1 Cr-53 0.000000 0.000000 +41 10 1 Cr-54 0.000000 0.000000 +0 10 2 H-1 0.000000 0.000000 +1 10 2 O-16 0.000000 0.000000 +2 10 2 B-10 0.000000 0.000000 +3 10 2 B-11 0.000000 0.000000 +4 10 2 Fe-54 0.000000 0.000000 +5 10 2 Fe-56 0.000000 0.000000 +6 10 2 Fe-57 0.000000 0.000000 +7 10 2 Fe-58 0.000000 0.000000 +8 10 2 Ni-58 0.000000 0.000000 +9 10 2 Ni-60 0.000000 0.000000 +10 10 2 Ni-61 0.000000 0.000000 +11 10 2 Ni-62 0.000000 0.000000 +12 10 2 Ni-64 0.000000 0.000000 +13 10 2 Mn-55 0.000000 0.000000 +14 10 2 Si-28 0.000000 0.000000 +15 10 2 Si-29 0.000000 0.000000 +16 10 2 Si-30 0.000000 0.000000 +17 10 2 Cr-50 0.000000 0.000000 +18 10 2 Cr-52 0.000000 0.000000 +19 10 2 Cr-53 0.000000 0.000000 +20 10 2 Cr-54 0.000000 0.000000 material group in nuclide mean std. dev. +21 10 1 H-1 0.0 0.0 +22 10 1 O-16 0.0 0.0 +23 10 1 B-10 0.0 0.0 +24 10 1 B-11 0.0 0.0 +25 10 1 Fe-54 0.0 0.0 +26 10 1 Fe-56 0.0 0.0 +27 10 1 Fe-57 0.0 0.0 +28 10 1 Fe-58 0.0 0.0 +29 10 1 Ni-58 0.0 0.0 +30 10 1 Ni-60 0.0 0.0 +31 10 1 Ni-61 0.0 0.0 +32 10 1 Ni-62 0.0 0.0 +33 10 1 Ni-64 0.0 0.0 +34 10 1 Mn-55 0.0 0.0 +35 10 1 Si-28 0.0 0.0 +36 10 1 Si-29 0.0 0.0 +37 10 1 Si-30 0.0 0.0 +38 10 1 Cr-50 0.0 0.0 +39 10 1 Cr-52 0.0 0.0 +40 10 1 Cr-53 0.0 0.0 +41 10 1 Cr-54 0.0 0.0 +0 10 2 H-1 0.0 0.0 +1 10 2 O-16 0.0 0.0 +2 10 2 B-10 0.0 0.0 +3 10 2 B-11 0.0 0.0 +4 10 2 Fe-54 0.0 0.0 +5 10 2 Fe-56 0.0 0.0 +6 10 2 Fe-57 0.0 0.0 +7 10 2 Fe-58 0.0 0.0 +8 10 2 Ni-58 0.0 0.0 +9 10 2 Ni-60 0.0 0.0 +10 10 2 Ni-61 0.0 0.0 +11 10 2 Ni-62 0.0 0.0 +12 10 2 Ni-64 0.0 0.0 +13 10 2 Mn-55 0.0 0.0 +14 10 2 Si-28 0.0 0.0 +15 10 2 Si-29 0.0 0.0 +16 10 2 Si-30 0.0 0.0 +17 10 2 Cr-50 0.0 0.0 +18 10 2 Cr-52 0.0 0.0 +19 10 2 Cr-53 0.0 0.0 +20 10 2 Cr-54 0.0 0.0 material group in group out nuclide mean std. dev. +63 10 1 1 H-1 0.123944 0.541390 +64 10 1 1 O-16 0.000000 0.000000 +65 10 1 1 B-10 0.000000 0.000000 +66 10 1 1 B-11 0.000000 0.000000 +67 10 1 1 Fe-54 0.000000 0.000000 +68 10 1 1 Fe-56 0.000000 0.000000 +69 10 1 1 Fe-57 0.000000 0.000000 +70 10 1 1 Fe-58 0.000000 0.000000 +71 10 1 1 Ni-58 0.000000 0.000000 +72 10 1 1 Ni-60 0.000000 0.000000 +73 10 1 1 Ni-61 0.000000 0.000000 +74 10 1 1 Ni-62 0.000000 0.000000 +75 10 1 1 Ni-64 0.000000 0.000000 +76 10 1 1 Mn-55 0.000000 0.000000 +77 10 1 1 Si-28 0.000000 0.000000 +78 10 1 1 Si-29 0.000000 0.000000 +79 10 1 1 Si-30 0.000000 0.000000 +80 10 1 1 Cr-50 0.111571 0.138458 +81 10 1 1 Cr-52 0.000000 0.000000 +82 10 1 1 Cr-53 0.000000 0.000000 +83 10 1 1 Cr-54 0.000000 0.000000 +42 10 1 2 H-1 0.000000 0.000000 +43 10 1 2 O-16 0.000000 0.000000 +44 10 1 2 B-10 0.000000 0.000000 +45 10 1 2 B-11 0.000000 0.000000 +46 10 1 2 Fe-54 0.000000 0.000000 +47 10 1 2 Fe-56 0.000000 0.000000 +48 10 1 2 Fe-57 0.000000 0.000000 +49 10 1 2 Fe-58 0.000000 0.000000 +50 10 1 2 Ni-58 0.000000 0.000000 +51 10 1 2 Ni-60 0.000000 0.000000 +52 10 1 2 Ni-61 0.000000 0.000000 +53 10 1 2 Ni-62 0.000000 0.000000 +54 10 1 2 Ni-64 0.000000 0.000000 +55 10 1 2 Mn-55 0.000000 0.000000 +56 10 1 2 Si-28 0.000000 0.000000 +57 10 1 2 Si-29 0.000000 0.000000 +58 10 1 2 Si-30 0.000000 0.000000 +59 10 1 2 Cr-50 0.000000 0.000000 +60 10 1 2 Cr-52 0.000000 0.000000 +61 10 1 2 Cr-53 0.000000 0.000000 +62 10 1 2 Cr-54 0.000000 0.000000 +21 10 2 1 H-1 0.000000 0.000000 +22 10 2 1 O-16 0.000000 0.000000 +23 10 2 1 B-10 0.000000 0.000000 +24 10 2 1 B-11 0.000000 0.000000 +25 10 2 1 Fe-54 0.000000 0.000000 +26 10 2 1 Fe-56 0.000000 0.000000 +27 10 2 1 Fe-57 0.000000 0.000000 +28 10 2 1 Fe-58 0.000000 0.000000 +29 10 2 1 Ni-58 0.000000 0.000000 +30 10 2 1 Ni-60 0.000000 0.000000 +31 10 2 1 Ni-61 0.000000 0.000000 +32 10 2 1 Ni-62 0.000000 0.000000 +33 10 2 1 Ni-64 0.000000 0.000000 +34 10 2 1 Mn-55 0.000000 0.000000 +35 10 2 1 Si-28 0.000000 0.000000 +36 10 2 1 Si-29 0.000000 0.000000 +37 10 2 1 Si-30 0.000000 0.000000 +38 10 2 1 Cr-50 0.000000 0.000000 +39 10 2 1 Cr-52 0.000000 0.000000 +40 10 2 1 Cr-53 0.000000 0.000000 +41 10 2 1 Cr-54 0.000000 0.000000 +0 10 2 2 H-1 0.000000 0.000000 +1 10 2 2 O-16 0.000000 0.000000 +2 10 2 2 B-10 0.000000 0.000000 +3 10 2 2 B-11 0.000000 0.000000 +4 10 2 2 Fe-54 0.000000 0.000000 +5 10 2 2 Fe-56 0.000000 0.000000 +6 10 2 2 Fe-57 0.000000 0.000000 +7 10 2 2 Fe-58 0.000000 0.000000 +8 10 2 2 Ni-58 0.000000 0.000000 +9 10 2 2 Ni-60 0.000000 0.000000 +10 10 2 2 Ni-61 0.000000 0.000000 +11 10 2 2 Ni-62 0.000000 0.000000 +12 10 2 2 Ni-64 0.000000 0.000000 +13 10 2 2 Mn-55 0.000000 0.000000 +14 10 2 2 Si-28 0.000000 0.000000 +15 10 2 2 Si-29 0.000000 0.000000 +16 10 2 2 Si-30 0.000000 0.000000 +17 10 2 2 Cr-50 0.000000 0.000000 +18 10 2 2 Cr-52 0.000000 0.000000 +19 10 2 2 Cr-53 0.000000 0.000000 +20 10 2 2 Cr-54 0.000000 0.000000 material group out nuclide mean std. dev. +21 10 1 H-1 0.0 0.0 +22 10 1 O-16 0.0 0.0 +23 10 1 B-10 0.0 0.0 +24 10 1 B-11 0.0 0.0 +25 10 1 Fe-54 0.0 0.0 +26 10 1 Fe-56 0.0 0.0 +27 10 1 Fe-57 0.0 0.0 +28 10 1 Fe-58 0.0 0.0 +29 10 1 Ni-58 0.0 0.0 +30 10 1 Ni-60 0.0 0.0 +31 10 1 Ni-61 0.0 0.0 +32 10 1 Ni-62 0.0 0.0 +33 10 1 Ni-64 0.0 0.0 +34 10 1 Mn-55 0.0 0.0 +35 10 1 Si-28 0.0 0.0 +36 10 1 Si-29 0.0 0.0 +37 10 1 Si-30 0.0 0.0 +38 10 1 Cr-50 0.0 0.0 +39 10 1 Cr-52 0.0 0.0 +40 10 1 Cr-53 0.0 0.0 +41 10 1 Cr-54 0.0 0.0 +0 10 2 H-1 0.0 0.0 +1 10 2 O-16 0.0 0.0 +2 10 2 B-10 0.0 0.0 +3 10 2 B-11 0.0 0.0 +4 10 2 Fe-54 0.0 0.0 +5 10 2 Fe-56 0.0 0.0 +6 10 2 Fe-57 0.0 0.0 +7 10 2 Fe-58 0.0 0.0 +8 10 2 Ni-58 0.0 0.0 +9 10 2 Ni-60 0.0 0.0 +10 10 2 Ni-61 0.0 0.0 +11 10 2 Ni-62 0.0 0.0 +12 10 2 Ni-64 0.0 0.0 +13 10 2 Mn-55 0.0 0.0 +14 10 2 Si-28 0.0 0.0 +15 10 2 Si-29 0.0 0.0 +16 10 2 Si-30 0.0 0.0 +17 10 2 Cr-50 0.0 0.0 +18 10 2 Cr-52 0.0 0.0 +19 10 2 Cr-53 0.0 0.0 +20 10 2 Cr-54 0.0 0.0 material group in nuclide mean std. dev. +9 11 1 H-1 0.131470 0.476035 +10 11 1 O-16 0.028684 0.043000 11 11 1 B-10 0.000000 0.000000 12 11 1 B-11 0.000000 0.000000 -13 11 1 Zr-90 0.041034 0.049102 -14 11 1 Zr-91 0.027328 0.021092 -15 11 1 Zr-92 0.009788 0.009282 -16 11 1 Zr-94 0.043543 0.036697 +13 11 1 Zr-90 0.021980 0.039963 +14 11 1 Zr-91 0.000000 0.000000 +15 11 1 Zr-92 0.000000 0.000000 +16 11 1 Zr-94 0.004191 0.087344 17 11 1 Zr-96 0.000000 0.000000 -0 11 2 H-1 0.824153 0.917955 -1 11 2 O-16 0.041986 0.060727 -2 11 2 B-10 0.048216 0.042726 +0 11 2 H-1 0.687243 1.239217 +1 11 2 O-16 0.000000 0.000000 +2 11 2 B-10 0.042902 0.060672 3 11 2 B-11 0.000000 0.000000 -4 11 2 Zr-90 0.048596 0.067712 +4 11 2 Zr-90 0.039576 0.105193 5 11 2 Zr-91 0.000000 0.000000 -6 11 2 Zr-92 0.000000 0.000000 -7 11 2 Zr-94 0.043195 0.041363 +6 11 2 Zr-92 0.084226 0.103161 +7 11 2 Zr-94 0.092039 0.125985 8 11 2 Zr-96 0.000000 0.000000 material group in nuclide mean std. dev. -9 11 1 H-1 0 0 -10 11 1 O-16 0 0 -11 11 1 B-10 0 0 -12 11 1 B-11 0 0 -13 11 1 Zr-90 0 0 -14 11 1 Zr-91 0 0 -15 11 1 Zr-92 0 0 -16 11 1 Zr-94 0 0 -17 11 1 Zr-96 0 0 -0 11 2 H-1 0 0 -1 11 2 O-16 0 0 -2 11 2 B-10 0 0 -3 11 2 B-11 0 0 -4 11 2 Zr-90 0 0 -5 11 2 Zr-91 0 0 -6 11 2 Zr-92 0 0 -7 11 2 Zr-94 0 0 -8 11 2 Zr-96 0 0 material group in group out nuclide mean std. dev. -27 11 1 1 H-1 0.111411 0.247294 -28 11 1 1 O-16 0.042575 0.049271 +9 11 1 H-1 0.0 0.0 +10 11 1 O-16 0.0 0.0 +11 11 1 B-10 0.0 0.0 +12 11 1 B-11 0.0 0.0 +13 11 1 Zr-90 0.0 0.0 +14 11 1 Zr-91 0.0 0.0 +15 11 1 Zr-92 0.0 0.0 +16 11 1 Zr-94 0.0 0.0 +17 11 1 Zr-96 0.0 0.0 +0 11 2 H-1 0.0 0.0 +1 11 2 O-16 0.0 0.0 +2 11 2 B-10 0.0 0.0 +3 11 2 B-11 0.0 0.0 +4 11 2 Zr-90 0.0 0.0 +5 11 2 Zr-91 0.0 0.0 +6 11 2 Zr-92 0.0 0.0 +7 11 2 Zr-94 0.0 0.0 +8 11 2 Zr-96 0.0 0.0 material group in group out nuclide mean std. dev. +27 11 1 1 H-1 0.099594 0.442578 +28 11 1 1 O-16 0.028684 0.043000 29 11 1 1 B-10 0.000000 0.000000 30 11 1 1 B-11 0.000000 0.000000 -31 11 1 1 Zr-90 0.041034 0.049102 -32 11 1 1 Zr-91 0.027328 0.021092 -33 11 1 1 Zr-92 0.009788 0.009282 -34 11 1 1 Zr-94 0.043543 0.036697 +31 11 1 1 Zr-90 0.021980 0.039963 +32 11 1 1 Zr-91 0.000000 0.000000 +33 11 1 1 Zr-92 0.000000 0.000000 +34 11 1 1 Zr-94 0.004191 0.087344 35 11 1 1 Zr-96 0.000000 0.000000 -18 11 1 2 H-1 0.027147 0.020009 +18 11 1 2 H-1 0.031875 0.045078 19 11 1 2 O-16 0.000000 0.000000 20 11 1 2 B-10 0.000000 0.000000 21 11 1 2 B-11 0.000000 0.000000 @@ -1852,79 +1852,79 @@ 15 11 2 1 Zr-92 0.000000 0.000000 16 11 2 1 Zr-94 0.000000 0.000000 17 11 2 1 Zr-96 0.000000 0.000000 -0 11 2 2 H-1 0.824153 0.917955 -1 11 2 2 O-16 0.041986 0.060727 +0 11 2 2 H-1 0.687243 1.239217 +1 11 2 2 O-16 0.000000 0.000000 2 11 2 2 B-10 0.000000 0.000000 3 11 2 2 B-11 0.000000 0.000000 -4 11 2 2 Zr-90 0.048596 0.067712 +4 11 2 2 Zr-90 0.039576 0.105193 5 11 2 2 Zr-91 0.000000 0.000000 -6 11 2 2 Zr-92 0.000000 0.000000 -7 11 2 2 Zr-94 0.043195 0.041363 +6 11 2 2 Zr-92 0.084226 0.103161 +7 11 2 2 Zr-94 0.092039 0.125985 8 11 2 2 Zr-96 0.000000 0.000000 material group out nuclide mean std. dev. -9 11 1 H-1 0 0 -10 11 1 O-16 0 0 -11 11 1 B-10 0 0 -12 11 1 B-11 0 0 -13 11 1 Zr-90 0 0 -14 11 1 Zr-91 0 0 -15 11 1 Zr-92 0 0 -16 11 1 Zr-94 0 0 -17 11 1 Zr-96 0 0 -0 11 2 H-1 0 0 -1 11 2 O-16 0 0 -2 11 2 B-10 0 0 -3 11 2 B-11 0 0 -4 11 2 Zr-90 0 0 -5 11 2 Zr-91 0 0 -6 11 2 Zr-92 0 0 -7 11 2 Zr-94 0 0 -8 11 2 Zr-96 0 0 material group in nuclide mean std. dev. -9 12 1 H-1 0.151924 0.200147 -10 12 1 O-16 0.039280 0.026086 +9 11 1 H-1 0.0 0.0 +10 11 1 O-16 0.0 0.0 +11 11 1 B-10 0.0 0.0 +12 11 1 B-11 0.0 0.0 +13 11 1 Zr-90 0.0 0.0 +14 11 1 Zr-91 0.0 0.0 +15 11 1 Zr-92 0.0 0.0 +16 11 1 Zr-94 0.0 0.0 +17 11 1 Zr-96 0.0 0.0 +0 11 2 H-1 0.0 0.0 +1 11 2 O-16 0.0 0.0 +2 11 2 B-10 0.0 0.0 +3 11 2 B-11 0.0 0.0 +4 11 2 Zr-90 0.0 0.0 +5 11 2 Zr-91 0.0 0.0 +6 11 2 Zr-92 0.0 0.0 +7 11 2 Zr-94 0.0 0.0 +8 11 2 Zr-96 0.0 0.0 material group in nuclide mean std. dev. +9 12 1 H-1 0.098944 0.178543 +10 12 1 O-16 0.013270 0.020403 11 12 1 B-10 0.000000 0.000000 12 12 1 B-11 0.000000 0.000000 -13 12 1 Zr-90 0.017578 0.022079 -14 12 1 Zr-91 0.039984 0.025285 -15 12 1 Zr-92 0.001172 0.006230 -16 12 1 Zr-94 0.001668 0.005966 -17 12 1 Zr-96 0.004328 0.005325 -0 12 2 H-1 0.942412 0.866849 -1 12 2 O-16 0.047438 0.048161 -2 12 2 B-10 0.041655 0.031202 +13 12 1 Zr-90 0.089997 0.075538 +14 12 1 Zr-91 0.000000 0.000000 +15 12 1 Zr-92 0.003501 0.017031 +16 12 1 Zr-94 0.004850 0.016327 +17 12 1 Zr-96 0.002730 0.017476 +0 12 2 H-1 1.261686 1.980336 +1 12 2 O-16 0.079159 0.104796 +2 12 2 B-10 0.016928 0.023940 3 12 2 B-11 0.000000 0.000000 -4 12 2 Zr-90 0.021193 0.017456 -5 12 2 Zr-91 0.007901 0.009268 -6 12 2 Zr-92 0.009422 0.012802 -7 12 2 Zr-94 0.043324 0.027551 +4 12 2 Zr-90 0.000000 0.000000 +5 12 2 Zr-91 0.033201 0.040665 +6 12 2 Zr-92 0.000000 0.000000 +7 12 2 Zr-94 0.000000 0.000000 8 12 2 Zr-96 0.000000 0.000000 material group in nuclide mean std. dev. -9 12 1 H-1 0 0 -10 12 1 O-16 0 0 -11 12 1 B-10 0 0 -12 12 1 B-11 0 0 -13 12 1 Zr-90 0 0 -14 12 1 Zr-91 0 0 -15 12 1 Zr-92 0 0 -16 12 1 Zr-94 0 0 -17 12 1 Zr-96 0 0 -0 12 2 H-1 0 0 -1 12 2 O-16 0 0 -2 12 2 B-10 0 0 -3 12 2 B-11 0 0 -4 12 2 Zr-90 0 0 -5 12 2 Zr-91 0 0 -6 12 2 Zr-92 0 0 -7 12 2 Zr-94 0 0 -8 12 2 Zr-96 0 0 material group in group out nuclide mean std. dev. -27 12 1 1 H-1 0.122301 0.187298 -28 12 1 1 O-16 0.039280 0.026086 +9 12 1 H-1 0.0 0.0 +10 12 1 O-16 0.0 0.0 +11 12 1 B-10 0.0 0.0 +12 12 1 B-11 0.0 0.0 +13 12 1 Zr-90 0.0 0.0 +14 12 1 Zr-91 0.0 0.0 +15 12 1 Zr-92 0.0 0.0 +16 12 1 Zr-94 0.0 0.0 +17 12 1 Zr-96 0.0 0.0 +0 12 2 H-1 0.0 0.0 +1 12 2 O-16 0.0 0.0 +2 12 2 B-10 0.0 0.0 +3 12 2 B-11 0.0 0.0 +4 12 2 Zr-90 0.0 0.0 +5 12 2 Zr-91 0.0 0.0 +6 12 2 Zr-92 0.0 0.0 +7 12 2 Zr-94 0.0 0.0 +8 12 2 Zr-96 0.0 0.0 material group in group out nuclide mean std. dev. +27 12 1 1 H-1 0.071704 0.167588 +28 12 1 1 O-16 0.013270 0.020403 29 12 1 1 B-10 0.000000 0.000000 30 12 1 1 B-11 0.000000 0.000000 -31 12 1 1 Zr-90 0.017578 0.022079 -32 12 1 1 Zr-91 0.039984 0.025285 -33 12 1 1 Zr-92 0.001172 0.006230 -34 12 1 1 Zr-94 0.001668 0.005966 -35 12 1 1 Zr-96 0.004328 0.005325 -18 12 1 2 H-1 0.029622 0.017760 +31 12 1 1 Zr-90 0.089997 0.075538 +32 12 1 1 Zr-91 0.000000 0.000000 +33 12 1 1 Zr-92 0.003501 0.017031 +34 12 1 1 Zr-94 0.004850 0.016327 +35 12 1 1 Zr-96 0.002730 0.017476 +18 12 1 2 H-1 0.027240 0.029555 19 12 1 2 O-16 0.000000 0.000000 20 12 1 2 B-10 0.000000 0.000000 21 12 1 2 B-11 0.000000 0.000000 @@ -1942,30 +1942,30 @@ 15 12 2 1 Zr-92 0.000000 0.000000 16 12 2 1 Zr-94 0.000000 0.000000 17 12 2 1 Zr-96 0.000000 0.000000 -0 12 2 2 H-1 0.942412 0.866849 -1 12 2 2 O-16 0.047438 0.048161 +0 12 2 2 H-1 1.244758 1.956675 +1 12 2 2 O-16 0.079159 0.104796 2 12 2 2 B-10 0.000000 0.000000 3 12 2 2 B-11 0.000000 0.000000 -4 12 2 2 Zr-90 0.021193 0.017456 -5 12 2 2 Zr-91 0.007901 0.009268 -6 12 2 2 Zr-92 0.009422 0.012802 -7 12 2 2 Zr-94 0.043324 0.027551 +4 12 2 2 Zr-90 0.000000 0.000000 +5 12 2 2 Zr-91 0.033201 0.040665 +6 12 2 2 Zr-92 0.000000 0.000000 +7 12 2 2 Zr-94 0.000000 0.000000 8 12 2 2 Zr-96 0.000000 0.000000 material group out nuclide mean std. dev. -9 12 1 H-1 0 0 -10 12 1 O-16 0 0 -11 12 1 B-10 0 0 -12 12 1 B-11 0 0 -13 12 1 Zr-90 0 0 -14 12 1 Zr-91 0 0 -15 12 1 Zr-92 0 0 -16 12 1 Zr-94 0 0 -17 12 1 Zr-96 0 0 -0 12 2 H-1 0 0 -1 12 2 O-16 0 0 -2 12 2 B-10 0 0 -3 12 2 B-11 0 0 -4 12 2 Zr-90 0 0 -5 12 2 Zr-91 0 0 -6 12 2 Zr-92 0 0 -7 12 2 Zr-94 0 0 -8 12 2 Zr-96 0 0 \ No newline at end of file +9 12 1 H-1 0.0 0.0 +10 12 1 O-16 0.0 0.0 +11 12 1 B-10 0.0 0.0 +12 12 1 B-11 0.0 0.0 +13 12 1 Zr-90 0.0 0.0 +14 12 1 Zr-91 0.0 0.0 +15 12 1 Zr-92 0.0 0.0 +16 12 1 Zr-94 0.0 0.0 +17 12 1 Zr-96 0.0 0.0 +0 12 2 H-1 0.0 0.0 +1 12 2 O-16 0.0 0.0 +2 12 2 B-10 0.0 0.0 +3 12 2 B-11 0.0 0.0 +4 12 2 Zr-90 0.0 0.0 +5 12 2 Zr-91 0.0 0.0 +6 12 2 Zr-92 0.0 0.0 +7 12 2 Zr-94 0.0 0.0 +8 12 2 Zr-96 0.0 0.0 \ No newline at end of file diff --git a/tests/test_multipole/results_true.dat b/tests/test_multipole/results_true.dat index 19dd4d26b..83d7e762e 100644 --- a/tests/test_multipole/results_true.dat +++ b/tests/test_multipole/results_true.dat @@ -1,12 +1,12 @@ k-combined: -1.445285E+00 9.521660E-03 +1.457760E+00 1.119659E-02 Cell ID = 11 Name = Material = 2 Region = -10000 - Temperature = [ 500. 0. 700. 800.] Rotation = None + Temperature = [ 500. 0. 700. 800.] Translation = None Offset = None Distribcell index= 1 diff --git a/tests/test_multipole/test_multipole.py b/tests/test_multipole/test_multipole.py index ea3108557..f1deb92cb 100644 --- a/tests/test_multipole/test_multipole.py +++ b/tests/test_multipole/test_multipole.py @@ -1,5 +1,4 @@ #!/usr/bin/env python - import os import sys sys.path.insert(0, os.pardir) @@ -9,7 +8,7 @@ from openmc.stats import Box from openmc.source import Source -class DistribmatTestHarness(PyAPITestHarness): +class MultipoleTestHarness(PyAPITestHarness): def _build_inputs(self): #################### # Materials @@ -116,8 +115,15 @@ class DistribmatTestHarness(PyAPITestHarness): plots_file.export_to_xml() + def execute_test(self): + if not 'OPENMC_MULTIPOLE_LIBRARY' in os.environ: + raise RuntimeError("The 'OPENMC_MULTIPOLE_LIBRARY' environment " + "variable must be specified for this test.") + else: + super(MultipoleTestHarness, self).execute_test() + def _get_results(self): - outstr = super(DistribmatTestHarness, self)._get_results() + outstr = super(MultipoleTestHarness, self)._get_results() su = openmc.Summary('summary.h5') outstr += str(su.get_cell_by_id(11)) return outstr @@ -126,9 +132,9 @@ class DistribmatTestHarness(PyAPITestHarness): f = os.path.join(os.getcwd(), 'plots.xml') if os.path.exists(f): os.remove(f) - super(DistribmatTestHarness, self)._cleanup() + super(MultipoleTestHarness, self)._cleanup() if __name__ == '__main__': - harness = DistribmatTestHarness('statepoint.5.*') + harness = MultipoleTestHarness('statepoint.5.*') harness.main() diff --git a/tests/test_natural_element/results_true.dat b/tests/test_natural_element/results_true.dat index 1c8668e12..cc4a12f74 100644 --- a/tests/test_natural_element/results_true.dat +++ b/tests/test_natural_element/results_true.dat @@ -1,2 +1,2 @@ k-combined: -1.013112E+00 2.551515E-02 +1.034427E+00 1.583807E-02 diff --git a/tests/test_output/results_true.dat b/tests/test_output/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_output/results_true.dat +++ b/tests/test_output/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_particle_restart_eigval/results_true.dat b/tests/test_particle_restart_eigval/results_true.dat index f34397853..2bc463293 100644 --- a/tests/test_particle_restart_eigval/results_true.dat +++ b/tests/test_particle_restart_eigval/results_true.dat @@ -1,16 +1,16 @@ current batch: -9.000000E+00 +1.000000E+01 current gen: 1.000000E+00 particle id: -5.550000E+02 +1.030000E+03 run mode: k-eigenvalue particle weight: 1.000000E+00 particle energy: -2.831611E-01 +3.158576E+00 particle xyz: -4.973847E+01 6.971699E+00 -5.201827E+01 +5.846530E+01 -3.717881E+01 -3.787515E+00 particle uvw: -6.945105E-01 6.295355E-01 -3.483393E-01 +6.197114E-01 -2.450461E-01 -7.455939E-01 diff --git a/tests/test_particle_restart_eigval/test_particle_restart_eigval.py b/tests/test_particle_restart_eigval/test_particle_restart_eigval.py index 139cb2b9f..59f76d93b 100644 --- a/tests/test_particle_restart_eigval/test_particle_restart_eigval.py +++ b/tests/test_particle_restart_eigval/test_particle_restart_eigval.py @@ -7,5 +7,5 @@ from testing_harness import ParticleRestartTestHarness if __name__ == '__main__': - harness = ParticleRestartTestHarness('particle_9_555.*') + harness = ParticleRestartTestHarness('particle_10_1030.*') harness.main() diff --git a/tests/test_quadric_surfaces/results_true.dat b/tests/test_quadric_surfaces/results_true.dat index b2e02fdbb..1f0dd5426 100644 --- a/tests/test_quadric_surfaces/results_true.dat +++ b/tests/test_quadric_surfaces/results_true.dat @@ -1,2 +1,2 @@ k-combined: -9.706301E-01 4.351374E-02 +9.570770E-01 2.513234E-02 diff --git a/tests/test_reflective_plane/results_true.dat b/tests/test_reflective_plane/results_true.dat index c5ba8e63f..4860c1ed9 100644 --- a/tests/test_reflective_plane/results_true.dat +++ b/tests/test_reflective_plane/results_true.dat @@ -1,2 +1,2 @@ k-combined: -2.276127E+00 4.678320E-03 +2.271202E+00 3.876146E-03 diff --git a/tests/test_resonance_scattering/geometry.xml b/tests/test_resonance_scattering/geometry.xml deleted file mode 100644 index bc56030e1..000000000 --- a/tests/test_resonance_scattering/geometry.xml +++ /dev/null @@ -1,8 +0,0 @@ - - - - - - - - diff --git a/tests/test_resonance_scattering/inputs_true.dat b/tests/test_resonance_scattering/inputs_true.dat new file mode 100644 index 000000000..f2a875c7e --- /dev/null +++ b/tests/test_resonance_scattering/inputs_true.dat @@ -0,0 +1 @@ +ece83bb075ed8144af89ce7cebf1577dcb2489d2e9ce4afbe61a3e4398837e7a9aaa2ae0cea0a6542f51ca5e0d119b570c675ed1dca0d74237cd5fdce0b606a3 \ No newline at end of file diff --git a/tests/test_resonance_scattering/materials.xml b/tests/test_resonance_scattering/materials.xml deleted file mode 100644 index 52a8c04be..000000000 --- a/tests/test_resonance_scattering/materials.xml +++ /dev/null @@ -1,9 +0,0 @@ - - - - - - - - - diff --git a/tests/test_resonance_scattering/results_true.dat b/tests/test_resonance_scattering/results_true.dat index 0dda991ca..e7056e4fa 100644 --- a/tests/test_resonance_scattering/results_true.dat +++ b/tests/test_resonance_scattering/results_true.dat @@ -1,2 +1,2 @@ k-combined: -6.842112E-02 8.480934E-04 +1.440556E+00 6.383274E-02 diff --git a/tests/test_resonance_scattering/settings.xml b/tests/test_resonance_scattering/settings.xml deleted file mode 100644 index 7ce4f23ac..000000000 --- a/tests/test_resonance_scattering/settings.xml +++ /dev/null @@ -1,27 +0,0 @@ - - - - - - U-238 - cxs - 92238.71c - 92238.71c - 5.0e-6 - 40.0e-6 - - - - - 10 - 5 - 1000 - - - - - -4 -4 -4 4 4 4 - - - - diff --git a/tests/test_resonance_scattering/test_resonance_scattering.py b/tests/test_resonance_scattering/test_resonance_scattering.py index 2a595f3e6..d977488bf 100644 --- a/tests/test_resonance_scattering/test_resonance_scattering.py +++ b/tests/test_resonance_scattering/test_resonance_scattering.py @@ -3,9 +3,81 @@ import os import sys sys.path.insert(0, os.pardir) -from testing_harness import TestHarness +from testing_harness import PyAPITestHarness +import openmc + + +class ResonanceScatteringTestHarness(PyAPITestHarness): + def _build_inputs(self): + # Materials + mat = openmc.Material(material_id=1) + mat.set_density('g/cc', 1.0) + mat.add_nuclide('U-238', 1.0) + mat.add_nuclide('U-235', 0.02) + mat.add_nuclide('Pu-239', 0.02) + mat.add_nuclide('H-1', 20.0) + + mats_file = openmc.MaterialsFile() + mats_file.default_xs = '71c' + mats_file.add_material(mat) + mats_file.export_to_xml() + + # Geometry + dumb_surface = openmc.XPlane(x0=100) + dumb_surface.boundary_type = 'reflective' + + c1 = openmc.Cell(cell_id=1) + c1.fill = mat + c1.region = -dumb_surface + + root_univ = openmc.Universe(universe_id=0) + root_univ.add_cell(c1) + + geometry = openmc.Geometry() + geometry.root_universe = root_univ + geo_file = openmc.GeometryFile() + geo_file.geometry = geometry + geo_file.export_to_xml() + + # Settings + nuclide = openmc.Nuclide('U-238', '71c') + nuclide.zaid = 92238 + res_scatt_dbrc = openmc.ResonanceScattering() + res_scatt_dbrc.nuclide = nuclide + res_scatt_dbrc.nuclide_0K = nuclide # This is a bad idea! Just for tests + res_scatt_dbrc.method = 'DBRC' + res_scatt_dbrc.E_min = 1e-6 + res_scatt_dbrc.E_max = 210e-6 + + nuclide = openmc.Nuclide('U-235', '71c') + nuclide.zaid = 92235 + res_scatt_wcm = openmc.ResonanceScattering() + res_scatt_wcm.nuclide = nuclide + res_scatt_wcm.nuclide_0K = nuclide + res_scatt_wcm.method = 'WCM' + res_scatt_wcm.E_min = 1e-6 + res_scatt_wcm.E_max = 210e-6 + + nuclide = openmc.Nuclide('Pu-239', '71c') + nuclide.zaid = 94239 + res_scatt_ares = openmc.ResonanceScattering() + res_scatt_ares.nuclide = nuclide + res_scatt_ares.nuclide_0K = nuclide + res_scatt_ares.method = 'ARES' + res_scatt_ares.E_min = 1e-6 + res_scatt_ares.E_max = 210e-6 + + sets_file = openmc.SettingsFile() + sets_file.batches = 10 + sets_file.inactive = 5 + sets_file.particles = 1000 + sets_file.source = openmc.source.Source( + space=openmc.stats.Box([-4, -4, -4], [4, 4, 4])) + sets_file.resonance_scattering = [res_scatt_dbrc, res_scatt_wcm, + res_scatt_ares] + sets_file.export_to_xml() if __name__ == '__main__': - harness = TestHarness('statepoint.10.*') + harness = ResonanceScatteringTestHarness('statepoint.10.*') harness.main() diff --git a/tests/test_rotation/results_true.dat b/tests/test_rotation/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_rotation/results_true.dat +++ b/tests/test_rotation/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_salphabeta/results_true.dat b/tests/test_salphabeta/results_true.dat index 926af89bc..fb691f168 100644 --- a/tests/test_salphabeta/results_true.dat +++ b/tests/test_salphabeta/results_true.dat @@ -1,2 +1,2 @@ k-combined: -8.350634E-01 6.010639E-02 +8.331430E-01 3.074913E-03 diff --git a/tests/test_score_current/results_true.dat b/tests/test_score_current/results_true.dat index 936e2d04b..d3ac03a70 100644 --- a/tests/test_score_current/results_true.dat +++ b/tests/test_score_current/results_true.dat @@ -1 +1 @@ -1e6945632c55491d4584f4976cc6f5c7340874703cfaf739dd956b7124b4260955efb5b6ba041b32536f9a74572d071e0293dced55a41ea305223f698b734c2a \ No newline at end of file +a9310752363eb059ff40f16ac9716b41ccab6ec6607d29f498069318745e485d18d784264304cc2586865bd58cef7587203cc22a1d485c58ddd63c14c0defdb9 \ No newline at end of file diff --git a/tests/test_seed/results_true.dat b/tests/test_seed/results_true.dat index df79ce1ce..35e9c968b 100644 --- a/tests/test_seed/results_true.dat +++ b/tests/test_seed/results_true.dat @@ -1,2 +1,2 @@ k-combined: -2.951164E-01 2.504580E-03 +3.131925E-01 7.639726E-03 diff --git a/tests/test_source/inputs_true.dat b/tests/test_source/inputs_true.dat index 01130ed2e..69a1e2ea8 100644 --- a/tests/test_source/inputs_true.dat +++ b/tests/test_source/inputs_true.dat @@ -1 +1 @@ -5c2fdde85affcd44c1b02c07c300acb8e5c189c1adbf7aa079e37a68e8b8313678fc292bd7f6e0d0957f723e05b8146bd165cf3315dde5f6b2f88ebc954cd65e \ No newline at end of file +526c91551d9a80dc01216e5cb04162253f12ec684cc2b4912ca18cfc510f1ea2e5303029f1c1607882082b0c2c8a47f25dd5be14678f449a1579e3601d1bdec5 \ No newline at end of file diff --git a/tests/test_source/results_true.dat b/tests/test_source/results_true.dat index 18fb895f7..e7ef218ad 100644 --- a/tests/test_source/results_true.dat +++ b/tests/test_source/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.014392E-01 7.185055E-03 +3.026614E-01 3.952004E-03 diff --git a/tests/test_source_file/results_true.dat b/tests/test_source_file/results_true.dat index fee61dda2..782e47176 100644 --- a/tests/test_source_file/results_true.dat +++ b/tests/test_source_file/results_true.dat @@ -1,2 +1,2 @@ k-combined: -2.962911E-01 4.073420E-03 +2.939526E-01 6.311736E-03 diff --git a/tests/test_sourcepoint_latest/results_true.dat b/tests/test_sourcepoint_latest/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_sourcepoint_latest/results_true.dat +++ b/tests/test_sourcepoint_latest/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_sourcepoint_restart/results_true.dat b/tests/test_sourcepoint_restart/results_true.dat index 0e4eef9a9..49afeb1d5 100644 --- a/tests/test_sourcepoint_restart/results_true.dat +++ b/tests/test_sourcepoint_restart/results_true.dat @@ -1,16 +1,16 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 tally 1: -7.000000E-03 -2.100000E-05 -1.127639E-03 -7.464355E-07 --1.264355E-03 -1.192757E-06 -8.769846E-04 -1.117508E-06 -3.359153E-03 -4.366438E-06 +1.100000E-02 +3.700000E-05 +1.307570E-03 +2.851451E-06 +1.564980E-03 +2.368303E-06 +3.138136E-03 +5.769887E-06 +7.719235E-03 +2.632583E-05 0.000000E+00 0.000000E+00 0.000000E+00 @@ -19,50 +19,38 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 -6.107648E-04 -3.730336E-07 +2.976389E-04 +8.858892E-08 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +0.000000E+00 +8.816169E-04 +7.772484E-07 1.000000E-03 1.000000E-06 -6.713061E-04 -4.506518E-07 -1.759778E-04 -3.096817E-08 --2.506458E-04 -6.282332E-08 -6.069794E-04 -3.684240E-07 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 +8.782909E-04 +7.713950E-07 +6.570925E-04 +4.317705E-07 +3.763366E-04 +1.416293E-07 0.000000E+00 0.000000E+00 7.000000E-03 1.500000E-05 -4.398928E-03 -8.198908E-06 -1.784486E-03 -3.422315E-06 -8.494423E-04 -9.262242E-07 -4.566637E-03 -5.646039E-06 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -6.069794E-04 -3.684240E-07 -0.000000E+00 -0.000000E+00 +3.445754E-03 +3.819507E-06 +2.124056E-03 +1.976201E-06 +1.542203E-03 +1.531669E-06 +4.135720E-03 +4.532612E-06 0.000000E+00 0.000000E+00 0.000000E+00 @@ -71,6 +59,8 @@ tally 1: 0.000000E+00 0.000000E+00 0.000000E+00 +5.874391E-04 +1.725424E-07 0.000000E+00 0.000000E+00 0.000000E+00 @@ -79,18 +69,28 @@ tally 1: 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-0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -3.000000E-03 -9.000000E-06 -2.576209E-03 -6.636855E-06 -1.844839E-03 -3.403429E-06 -9.997002E-04 -9.994005E-07 -1.240803E-03 -1.539593E-06 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -3.102008E-04 -9.622454E-08 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 1.000000E-03 1.000000E-06 -1.590395E-04 -2.529356E-08 --4.620597E-04 -2.134991E-07 --2.285026E-04 -5.221342E-08 -3.102008E-04 -9.622454E-08 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 -0.000000E+00 +-3.865739E-04 +1.494394E-07 +-2.758409E-04 +7.608820E-08 +4.354374E-04 +1.896058E-07 +5.871337E-04 +3.447260E-07 0.000000E+00 0.000000E+00 0.000000E+00 @@ -2402,11 +2402,11 @@ tally 1: 0.000000E+00 0.000000E+00 tally 2: -2.288800E-01 -2.621372E-02 -2.489848E-01 -3.102301E-02 -1.451035E+00 -1.053707E+00 -1.618797E+01 -1.311489E+02 +5.656887E-01 +6.401442E-02 +6.158976E-01 +7.588371E-02 +3.588479E+00 +2.575762E+00 +4.003041E+01 +3.205440E+02 diff --git a/tests/test_statepoint_restart/test_statepoint_restart.py b/tests/test_statepoint_restart/test_statepoint_restart.py index 59b77a821..c842689d9 100644 --- a/tests/test_statepoint_restart/test_statepoint_restart.py +++ b/tests/test_statepoint_restart/test_statepoint_restart.py @@ -10,6 +10,11 @@ from openmc.executor import Executor class StatepointRestartTestHarness(TestHarness): + def __init__(self, final_sp, restart_sp, tallies_present=False): + super(StatepointRestartTestHarness, self).__init__(final_sp, + tallies_present) + self._restart_sp = restart_sp + def execute_test(self): """Run OpenMC with the appropriate arguments and check the outputs.""" try: @@ -40,7 +45,9 @@ class StatepointRestartTestHarness(TestHarness): def _run_openmc_restart(self): # Get the name of the statepoint file. - statepoint = glob.glob(os.path.join(os.getcwd(), self._sp_name)) + statepoint = glob.glob(os.path.join(os.getcwd(), self._restart_sp)) + assert len(statepoint) == 1 + statepoint = statepoint[0] # Run OpenMC executor = Executor() @@ -52,11 +59,13 @@ class StatepointRestartTestHarness(TestHarness): mpi_exec=self._opts.mpi_exec) else: - returncode = executor.run_simulation(openmc_exec=self._opts.exe) + returncode = executor.run_simulation(openmc_exec=self._opts.exe, + restart_file=statepoint) assert returncode == 0, 'OpenMC did not exit successfully.' if __name__ == '__main__': - harness = StatepointRestartTestHarness('statepoint.07.*', True) + harness = StatepointRestartTestHarness('statepoint.10.h5', + 'statepoint.07.h5', True) harness.main() diff --git a/tests/test_statepoint_sourcesep/results_true.dat b/tests/test_statepoint_sourcesep/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_statepoint_sourcesep/results_true.dat +++ b/tests/test_statepoint_sourcesep/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_survival_biasing/results_true.dat b/tests/test_survival_biasing/results_true.dat index 3e327841a..e44ec289a 100644 --- a/tests/test_survival_biasing/results_true.dat +++ b/tests/test_survival_biasing/results_true.dat @@ -1,20 +1,20 @@ k-combined: -9.997733E-01 2.995572E-02 +9.686215E-01 1.511499E-02 tally 1: -4.354055E+01 -3.793645E+02 -1.808636E+01 -6.546005E+01 -2.234465E+00 -9.989832E-01 -1.937431E+00 -7.510380E-01 -5.021671E+00 -5.045425E+00 -3.506791E-02 -2.460654E-04 -3.752351E+02 -2.817188E+04 +4.243782E+01 +3.604528E+02 +1.770205E+01 +6.273029E+01 +2.176094E+00 +9.477949E-01 +1.881775E+00 +7.087350E-01 +4.868971E+00 +4.744828E+00 +3.400887E-02 +2.314715E-04 +3.644408E+02 +2.658287E+04 tally 2: -1.808636E+01 -6.546005E+01 +1.770205E+01 +6.273029E+01 diff --git a/tests/test_tallies/results_true.dat b/tests/test_tallies/results_true.dat index 4f8b3956b..fd5eb91a1 100644 --- a/tests/test_tallies/results_true.dat +++ b/tests/test_tallies/results_true.dat @@ -1 +1 @@ -5be9b80ecc189d4ee3a6a228d97b0c76b6b47e5204a86ecf03b8faa65c499f6861ffd85c153084bafd0835d10dfacc14f28802901ce966c8a803d60d0c2f42e5 \ No newline at end of file +9f14aaa1694489032b3ce193ad29ecf6ac8976c88c2dd6b26d4c30ae88348e249a9b702b1d39c22204350b8f3bd689800c1b6a6003f19c7bdaf64084a209a2cc \ No newline at end of file diff --git a/tests/test_tallies/test_tallies.py b/tests/test_tallies/test_tallies.py index 9fca93bca..81e8641de 100644 --- a/tests/test_tallies/test_tallies.py +++ b/tests/test_tallies/test_tallies.py @@ -23,19 +23,19 @@ class TalliesTestHarness(PyAPITestHarness): azimuthal_bins = (-3.1416, -1.8850, -0.6283, 0.6283, 1.8850, 3.1416) azimuthal_filter1 = Filter(type='azimuthal', bins=azimuthal_bins) azimuthal_tally1 = Tally() - azimuthal_tally1.add_filter(azimuthal_filter1) - azimuthal_tally1.add_score('flux') + azimuthal_tally1.filters = [azimuthal_filter1] + azimuthal_tally1.scores = ['flux'] azimuthal_tally1.estimator = 'tracklength' azimuthal_tally2 = Tally() - azimuthal_tally2.add_filter(azimuthal_filter1) - azimuthal_tally2.add_score('flux') + azimuthal_tally2.filters = [azimuthal_filter1] + azimuthal_tally2.scores = ['flux'] azimuthal_tally2.estimator = 'analog' azimuthal_filter2 = Filter(type='azimuthal', bins=(5,)) azimuthal_tally3 = Tally() - azimuthal_tally3.add_filter(azimuthal_filter2) - azimuthal_tally3.add_score('flux') + azimuthal_tally3.filters = [azimuthal_filter2] + azimuthal_tally3.scores = ['flux'] azimuthal_tally3.estimator = 'tracklength' mesh_2x2 = Mesh(mesh_id=1) @@ -44,154 +44,129 @@ class TalliesTestHarness(PyAPITestHarness): mesh_2x2.dimension = [2, 2] mesh_filter = Filter(type='mesh', bins=(1,)) azimuthal_tally4 = Tally() - azimuthal_tally4.add_filter(azimuthal_filter2) - azimuthal_tally4.add_filter(mesh_filter) - azimuthal_tally4.add_score('flux') + azimuthal_tally4.filters = [azimuthal_filter2, mesh_filter] + azimuthal_tally4.scores = ['flux'] azimuthal_tally4.estimator = 'tracklength' cellborn_tally = Tally() - cellborn_tally.add_filter(Filter(type='cellborn', bins=(10, 21, 22, 23))) - cellborn_tally.add_score('total') + cellborn_tally.filters = [Filter(type='cellborn', bins=(10, 21, 22, 23))] + cellborn_tally.scores = ['total'] dg_tally = Tally() - dg_tally.add_filter(Filter(type='delayedgroup', bins=(1, 2, 3, 4, 5, 6))) - dg_tally.add_score('delayed-nu-fission') + dg_tally.filters = [Filter(type='delayedgroup', bins=(1, 2, 3, 4, 5, 6))] + dg_tally.scores = ['delayed-nu-fission'] four_groups = (0.0, 0.253e-6, 1.0e-3, 1.0, 20.0) energy_filter = Filter(type='energy', bins=four_groups) energy_tally = Tally() - energy_tally.add_filter(energy_filter) - energy_tally.add_score('total') + energy_tally.filters = [energy_filter] + energy_tally.scores = ['total'] energyout_filter = Filter(type='energyout', bins=four_groups) energyout_tally = Tally() - energyout_tally.add_filter(energyout_filter) - energyout_tally.add_score('scatter') + energyout_tally.filters = [energyout_filter] + energyout_tally.scores = ['scatter'] transfer_tally = Tally() - transfer_tally.add_filter(energy_filter) - transfer_tally.add_filter(energyout_filter) - transfer_tally.add_score('scatter') - transfer_tally.add_score('nu-fission') + transfer_tally.filters = [energy_filter, energyout_filter] + transfer_tally.scores = ['scatter', 'nu-fission'] material_tally = Tally() - material_tally.add_filter(Filter(type='material', bins=(1, 2, 3, 4))) - material_tally.add_score('total') + material_tally.filters = [Filter(type='material', bins=(1, 2, 3, 4))] + material_tally.scores = ['total'] mu_tally1 = Tally() - mu_tally1.add_filter(Filter(type='mu', bins=(-1.0, -0.5, 0.0, 0.5, 1.0))) - mu_tally1.add_score('scatter') - mu_tally1.add_score('nu-scatter') + mu_tally1.filters = [Filter(type='mu', bins=(-1.0, -0.5, 0.0, 0.5, 1.0))] + mu_tally1.scores = ['scatter', 'nu-scatter'] mu_filter = Filter(type='mu', bins=(5,)) mu_tally2 = Tally() - mu_tally2.add_filter(mu_filter) - mu_tally2.add_score('scatter') - mu_tally2.add_score('nu-scatter') + mu_tally2.filters = [mu_filter] + mu_tally2.scores = ['scatter', 'nu-scatter'] mu_tally3 = Tally() - mu_tally3.add_filter(mu_filter) - mu_tally3.add_filter(mesh_filter) - mu_tally3.add_score('scatter') - mu_tally3.add_score('nu-scatter') + mu_tally3.filters = [mu_filter, mesh_filter] + mu_tally3.scores = ['scatter', 'nu-scatter'] polar_bins = (0.0, 0.6283, 1.2566, 1.8850, 2.5132, 3.1416) polar_filter = Filter(type='polar', bins=polar_bins) polar_tally1 = Tally() - polar_tally1.add_filter(polar_filter) - polar_tally1.add_score('flux') + polar_tally1.filters = [polar_filter] + polar_tally1.scores = ['flux'] polar_tally1.estimator = 'tracklength' polar_tally2 = Tally() - polar_tally2.add_filter(polar_filter) - polar_tally2.add_score('flux') + polar_tally2.filters = [polar_filter] + polar_tally2.scores = ['flux'] polar_tally2.estimator = 'analog' polar_filter2 = Filter(type='polar', bins=(5,)) polar_tally3 = Tally() - polar_tally3.add_filter(polar_filter2) - polar_tally3.add_score('flux') + polar_tally3.filters = [polar_filter2] + polar_tally3.scores = ['flux'] polar_tally3.estimator = 'tracklength' polar_tally4 = Tally() - polar_tally4.add_filter(polar_filter2) - polar_tally4.add_filter(mesh_filter) - polar_tally4.add_score('flux') + polar_tally4.filters = [polar_filter2, mesh_filter] + polar_tally4.scores = ['flux'] polar_tally4.estimator = 'tracklength' universe_tally = Tally() - universe_tally.add_filter(Filter(type='universe', bins=(1, 2, 3, 4))) - universe_tally.add_score('total') + universe_tally.filters = [Filter(type='universe', bins=(1, 2, 3, 4))] + universe_tally.scores = ['total'] cell_filter = Filter(type='cell', bins=(10, 21, 22, 23)) score_tallies = [Tally(), Tally(), Tally()] for t in score_tallies: - t.add_filter(cell_filter) - t.add_score('absorption') - t.add_score('delayed-nu-fission') - t.add_score('events') - t.add_score('fission') - t.add_score('inverse-velocity') - t.add_score('kappa-fission') - t.add_score('(n,2n)') - t.add_score('(n,n1)') - t.add_score('(n,gamma)') - t.add_score('nu-fission') - t.add_score('scatter') - t.add_score('elastic') - t.add_score('total') + t.filters = [cell_filter] + t.scores = ['absorption', 'delayed-nu-fission', 'events', 'fission', + 'inverse-velocity', 'kappa-fission', '(n,2n)', '(n,n1)', + '(n,gamma)', 'nu-fission', 'scatter', 'elastic', 'total'] score_tallies[0].estimator = 'tracklength' score_tallies[1].estimator = 'analog' score_tallies[2].estimator = 'collision' cell_filter2 = Filter(type='cell', bins=(21, 22, 23, 27, 28, 29)) flux_tallies = [Tally() for i in range(4)] - [t.add_filter(cell_filter2) for t in flux_tallies] - flux_tallies[0].add_score('flux') - [t.add_score('flux-y5') for t in flux_tallies[1:]] + for t in flux_tallies: + t.filters = [cell_filter2] + flux_tallies[0].scores = ['flux'] + for t in flux_tallies[1:]: + t.scores = ['flux-y5'] flux_tallies[1].estimator = 'tracklength' flux_tallies[2].estimator = 'analog' flux_tallies[3].estimator = 'collision' scatter_tally1 = Tally() - scatter_tally1.add_filter(cell_filter) - scatter_tally1.add_score('scatter') - scatter_tally1.add_score('scatter-1') - scatter_tally1.add_score('scatter-2') - scatter_tally1.add_score('scatter-3') - scatter_tally1.add_score('scatter-4') - scatter_tally1.add_score('nu-scatter') - scatter_tally1.add_score('nu-scatter-1') - scatter_tally1.add_score('nu-scatter-2') - scatter_tally1.add_score('nu-scatter-3') - scatter_tally1.add_score('nu-scatter-4') + scatter_tally1.filters = [cell_filter] + scatter_tally1.scores = ['scatter', 'scatter-1', 'scatter-2', 'scatter-3', + 'scatter-4', 'nu-scatter', 'nu-scatter-1', + 'nu-scatter-2', 'nu-scatter-3', 'nu-scatter-4'] scatter_tally2 = Tally() - scatter_tally2.add_filter(cell_filter) - scatter_tally2.add_score('scatter-p4') - scatter_tally2.add_score('scatter-y4') - scatter_tally2.add_score('nu-scatter-p4') - scatter_tally2.add_score('nu-scatter-y3') + scatter_tally2.filters = [cell_filter] + scatter_tally2.scores = ['scatter-p4', 'scatter-y4', 'nu-scatter-p4', + 'nu-scatter-y3'] total_tallies = [Tally() for i in range(4)] - [t.add_filter(cell_filter) for t in total_tallies] - total_tallies[0].add_score('total') - [t.add_score('total-y4') for t in total_tallies[1:]] - [t.add_nuclide('U-235') for t in total_tallies[1:]] - [t.add_nuclide('total') for t in total_tallies[1:]] + for t in total_tallies: + t.filters = [cell_filter] + total_tallies[0].scores = ['total'] + for t in total_tallies[1:]: + t.scores = ['total-y4'] + t.nuclides = ['U-235', 'total'] total_tallies[1].estimator = 'tracklength' total_tallies[2].estimator = 'analog' total_tallies[3].estimator = 'collision' questionable_tally = Tally() - questionable_tally.add_score('transport') - questionable_tally.add_score('n1n') + questionable_tally.scores = ['transport', 'n1n'] all_nuclide_tallies = [Tally(), Tally()] for t in all_nuclide_tallies: - t.add_filter(cell_filter) - t.add_nuclide('all') - t.add_score('total') + t.filters = [cell_filter] + t.nuclides = ['all'] + t.scores = ['total'] all_nuclide_tallies[0].estimator = 'tracklength' all_nuclide_tallies[0].estimator = 'collision' diff --git a/tests/test_tally_aggregation/results_true.dat b/tests/test_tally_aggregation/results_true.dat index cde3e281c..6c2d7a519 100644 --- a/tests/test_tally_aggregation/results_true.dat +++ b/tests/test_tally_aggregation/results_true.dat @@ -1 +1 @@ -ba8bfe764fcc0484a4fdab8fdc4ff8ad0e4a98b1ff33e8687899c8cc6bf80cb28b3a59aeaec84bd74681b8b5f19f714292ccaa9c9d4ba852b2cc29872f612e10 \ No newline at end of file +840d2648f9ba782926c71baa84e5a2ad31331e156740a3d1e9d86af8f1f0d301ef8c0f69474975d365dbcf8d229a68c62d3e60286d18045e5254373f4e1010bf \ No newline at end of file diff --git a/tests/test_tally_aggregation/test_tally_aggregation.py b/tests/test_tally_aggregation/test_tally_aggregation.py index a5c8d9414..7d682b698 100644 --- a/tests/test_tally_aggregation/test_tally_aggregation.py +++ b/tests/test_tally_aggregation/test_tally_aggregation.py @@ -30,13 +30,9 @@ class TallyAggregationTestHarness(PyAPITestHarness): # Initialized the tallies tally = openmc.Tally(name='distribcell tally') - tally.add_filter(energy_filter) - tally.add_filter(distrib_filter) - tally.add_score('nu-fission') - tally.add_score('total') - tally.add_nuclide(u235) - tally.add_nuclide(u238) - tally.add_nuclide(pu239) + tally.filters = [energy_filter, distrib_filter] + tally.scores = ['nu-fission', 'total'] + tally.nuclides = [u235, u238, pu239] tallies_file.add_tally(tally) # Export tallies to file diff --git a/tests/test_tally_arithmetic/results_true.dat b/tests/test_tally_arithmetic/results_true.dat index ded2efa66..ef2741cc1 100644 --- a/tests/test_tally_arithmetic/results_true.dat +++ b/tests/test_tally_arithmetic/results_true.dat @@ -1,134 +1,134 @@ -[[[ 8.90240785e-05 8.31464209e-11 4.41507090e-05 4.12357364e-11] - [ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 4.69276830e-05 4.38293656e-11 2.35903380e-05 2.20328275e-11] - [ 3.84607356e-05 3.15690405e-05 1.93340411e-05 1.58696166e-05]] +[[[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 8.90240785e-05 8.31464209e-11 4.41507090e-05 4.12357364e-11] - [ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 4.69276830e-05 4.38293656e-11 2.35903380e-05 2.20328275e-11] - [ 3.84607356e-05 3.15690405e-05 1.93340411e-05 1.58696166e-05]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 8.90240785e-05 8.31464209e-11 4.41507090e-05 4.12357364e-11] - [ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 4.69276830e-05 4.38293656e-11 2.35903380e-05 2.20328275e-11] - [ 3.84607356e-05 3.15690405e-05 1.93340411e-05 1.58696166e-05]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] ..., - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]]][[[ 8.90240785e-05 8.31464209e-11 4.41507090e-05 4.12357364e-11] - [ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 4.69276830e-05 4.38293656e-11 2.35903380e-05 2.20328275e-11] - [ 3.84607356e-05 3.15690405e-05 1.93340411e-05 1.58696166e-05]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]]][[[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 8.90240785e-05 8.31464209e-11 4.41507090e-05 4.12357364e-11] - [ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 4.69276830e-05 4.38293656e-11 2.35903380e-05 2.20328275e-11] - [ 3.84607356e-05 3.15690405e-05 1.93340411e-05 1.58696166e-05]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 8.90240785e-05 8.31464209e-11 4.41507090e-05 4.12357364e-11] - [ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 4.69276830e-05 4.38293656e-11 2.35903380e-05 2.20328275e-11] - [ 3.84607356e-05 3.15690405e-05 1.93340411e-05 1.58696166e-05]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] ..., - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]]][[[ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]]][[[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 7.29618709e-05 5.98879928e-05 3.61847984e-05 2.97009235e-05] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] ..., - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00 0.00000000e+00]]][[[ 0.00000000e+00 4.41507090e-05 0.00000000e+00] - [ 0.00000000e+00 3.61847984e-05 0.00000000e+00] - [ 0.00000000e+00 2.35903380e-05 0.00000000e+00] - [ 0.00000000e+00 1.93340411e-05 0.00000000e+00]] + [[ 0. 0. 0. 0.] + [ 0. 0. 0. 0.] + [ 0. 0. 0. 0.]]][[[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 4.41507090e-05 0.00000000e+00] - [ 0.00000000e+00 3.61847984e-05 0.00000000e+00] - [ 0.00000000e+00 2.35903380e-05 0.00000000e+00] - [ 0.00000000e+00 1.93340411e-05 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 4.41507090e-05 0.00000000e+00] - [ 0.00000000e+00 3.61847984e-05 0.00000000e+00] - [ 0.00000000e+00 2.35903380e-05 0.00000000e+00] - [ 0.00000000e+00 1.93340411e-05 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] ..., - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]]][[[ 0.00000000e+00 3.61847984e-05 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]]][[[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 3.61847984e-05 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 3.61847984e-05 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] ..., - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]] + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]] - [[ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00] - [ 0.00000000e+00 0.00000000e+00 0.00000000e+00]]] \ No newline at end of file + [[ 0. 0. 0.] + [ 0. 0. 0.] + [ 0. 0. 0.]]] \ No newline at end of file diff --git a/tests/test_tally_arithmetic/test_tally_arithmetic.py b/tests/test_tally_arithmetic/test_tally_arithmetic.py index 1954334b7..cf8d012e8 100644 --- a/tests/test_tally_arithmetic/test_tally_arithmetic.py +++ b/tests/test_tally_arithmetic/test_tally_arithmetic.py @@ -40,22 +40,15 @@ class TallyArithmeticTestHarness(PyAPITestHarness): # Initialized the tallies tally = openmc.Tally(name='tally 1') - tally.add_filter(material_filter) - tally.add_filter(energy_filter) - tally.add_filter(distrib_filter) - tally.add_score('nu-fission') - tally.add_score('total') - tally.add_nuclide(u235) - tally.add_nuclide(pu239) + tally.filters = [material_filter, energy_filter, distrib_filter] + tally.scores = ['nu-fission', 'total'] + tally.nuclides = [u235, pu239] tallies_file.add_tally(tally) tally = openmc.Tally(name='tally 2') - tally.add_filter(energy_filter) - tally.add_filter(mesh_filter) - tally.add_score('total') - tally.add_score('fission') - tally.add_nuclide(u238) - tally.add_nuclide(u235) + tally.filters = [energy_filter, mesh_filter] + tally.scores = ['total', 'fission'] + tally.nuclides = [u238, u235] tallies_file.add_tally(tally) tallies_file.add_mesh(mesh) diff --git a/tests/test_tally_assumesep/results_true.dat b/tests/test_tally_assumesep/results_true.dat index 4835227f2..7262a88a0 100644 --- a/tests/test_tally_assumesep/results_true.dat +++ b/tests/test_tally_assumesep/results_true.dat @@ -1,11 +1,11 @@ k-combined: -1.005983E+00 2.248579E-02 +9.581522E-01 4.261830E-02 tally 1: -1.423676E+01 -4.330937E+01 +1.529084E+01 +4.769011E+01 tally 2: -2.914798E+00 -1.831649E+00 +3.198905E+00 +2.114129E+00 tally 3: -4.088282E+01 -3.662539E+02 +4.510603E+01 +4.183089E+02 diff --git a/tests/test_tally_nuclides/results_true.dat b/tests/test_tally_nuclides/results_true.dat index b8e903049..36250aba7 100644 --- a/tests/test_tally_nuclides/results_true.dat +++ b/tests/test_tally_nuclides/results_true.dat @@ -1,28 +1,28 @@ k-combined: -9.851180E-01 1.587642E-02 +9.752414E-01 4.425137E-02 tally 1: -7.516940E+00 -1.149356E+01 -1.700884E+00 -5.835345E-01 -1.635327E+00 -5.385674E-01 -5.816056E+00 -6.901370E+00 -7.516940E+00 -1.149356E+01 -1.700884E+00 -5.835345E-01 -1.635327E+00 -5.385674E-01 -5.816056E+00 -6.901370E+00 +6.903183E+00 +9.661095E+00 +1.569337E+00 +4.971849E-01 +1.521894E+00 +4.673221E-01 +5.333846E+00 +5.778631E+00 +6.903183E+00 +9.661095E+00 +1.569337E+00 +4.971849E-01 +1.521894E+00 +4.673221E-01 +5.333846E+00 +5.778631E+00 tally 2: -7.516940E+00 -1.149356E+01 -1.700884E+00 -5.835345E-01 -1.635327E+00 -5.385674E-01 -5.816056E+00 -6.901370E+00 +6.903183E+00 +9.661095E+00 +1.569337E+00 +4.971849E-01 +1.521894E+00 +4.673221E-01 +5.333846E+00 +5.778631E+00 diff --git a/tests/test_tally_slice_merge/inputs_true.dat b/tests/test_tally_slice_merge/inputs_true.dat new file mode 100644 index 000000000..29f0f1d82 --- /dev/null +++ b/tests/test_tally_slice_merge/inputs_true.dat @@ -0,0 +1 @@ +8d1ab9e4add51b99045e990ac9c3dad9447e9720d811bc430d4bfdd7c2c035424bcb7750e4a4d0ec0460ea1ef4be46ac58372ed01d55f5d8cfeebbce75559066 \ No newline at end of file diff --git a/tests/test_tally_slice_merge/results_true.dat b/tests/test_tally_slice_merge/results_true.dat new file mode 100644 index 000000000..ed04152d4 --- /dev/null +++ b/tests/test_tally_slice_merge/results_true.dat @@ -0,0 +1,49 @@ + energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 21 U-235 fission 1.08e-01 7.94e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 21 U-235 nu-fission 2.64e-01 1.94e-02 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 21 U-238 fission 1.51e-07 1.00e-08 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 21 U-238 nu-fission 3.76e-07 2.50e-08 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 21 U-235 fission 3.12e-02 2.56e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 21 U-235 nu-fission 7.65e-02 6.24e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 21 U-238 fission 2.00e-02 1.30e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 21 U-238 nu-fission 5.56e-02 3.78e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 27 U-235 fission 4.43e-02 7.21e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 27 U-235 nu-fission 1.08e-01 1.76e-02 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 27 U-238 fission 6.14e-08 9.64e-09 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 27 U-238 nu-fission 1.53e-07 2.40e-08 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 27 U-235 fission 1.39e-02 1.06e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 27 U-235 nu-fission 3.40e-02 2.61e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 27 U-238 fission 9.72e-03 1.21e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 6.25e-07 2.00e+01 27 U-238 nu-fission 2.71e-02 3.80e-03 energy low [MeV] energy high [MeV] cell nuclide score mean std. dev. +0 0.00e+00 6.25e-07 21 U-235 fission 1.08e-01 7.94e-03 +1 0.00e+00 6.25e-07 21 U-235 nu-fission 2.64e-01 1.94e-02 +2 0.00e+00 6.25e-07 21 U-238 fission 1.51e-07 1.00e-08 +3 0.00e+00 6.25e-07 21 U-238 nu-fission 3.76e-07 2.50e-08 +4 0.00e+00 6.25e-07 27 U-235 fission 4.43e-02 7.21e-03 +5 0.00e+00 6.25e-07 27 U-235 nu-fission 1.08e-01 1.76e-02 +6 0.00e+00 6.25e-07 27 U-238 fission 6.14e-08 9.64e-09 +7 0.00e+00 6.25e-07 27 U-238 nu-fission 1.53e-07 2.40e-08 +8 6.25e-07 2.00e+01 21 U-235 fission 3.12e-02 2.56e-03 +9 6.25e-07 2.00e+01 21 U-235 nu-fission 7.65e-02 6.24e-03 +10 6.25e-07 2.00e+01 21 U-238 fission 2.00e-02 1.30e-03 +11 6.25e-07 2.00e+01 21 U-238 nu-fission 5.56e-02 3.78e-03 +12 6.25e-07 2.00e+01 27 U-235 fission 1.39e-02 1.06e-03 +13 6.25e-07 2.00e+01 27 U-235 nu-fission 3.40e-02 2.61e-03 +14 6.25e-07 2.00e+01 27 U-238 fission 9.72e-03 1.21e-03 +15 6.25e-07 2.00e+01 27 U-238 nu-fission 2.71e-02 3.80e-03 sum(distribcell) energy low [MeV] energy high [MeV] nuclide score mean std. dev. +0 (0, 100, 2000, 30000) 0.00e+00 6.25e-07 U-235 fission 0.00e+00 0.00e+00 +1 (0, 100, 2000, 30000) 0.00e+00 6.25e-07 U-235 nu-fission 0.00e+00 0.00e+00 +2 (0, 100, 2000, 30000) 0.00e+00 6.25e-07 U-238 fission 0.00e+00 0.00e+00 +3 (0, 100, 2000, 30000) 0.00e+00 6.25e-07 U-238 nu-fission 0.00e+00 0.00e+00 +4 (0, 100, 2000, 30000) 6.25e-07 2.00e+01 U-235 fission 0.00e+00 0.00e+00 +5 (0, 100, 2000, 30000) 6.25e-07 2.00e+01 U-235 nu-fission 0.00e+00 0.00e+00 +6 (0, 100, 2000, 30000) 6.25e-07 2.00e+01 U-238 fission 0.00e+00 0.00e+00 +7 (0, 100, 2000, 30000) 6.25e-07 2.00e+01 U-238 nu-fission 0.00e+00 0.00e+00 +8 (500, 5000, 50000) 0.00e+00 6.25e-07 U-235 fission 0.00e+00 0.00e+00 +9 (500, 5000, 50000) 0.00e+00 6.25e-07 U-235 nu-fission 0.00e+00 0.00e+00 +10 (500, 5000, 50000) 0.00e+00 6.25e-07 U-238 fission 0.00e+00 0.00e+00 +11 (500, 5000, 50000) 0.00e+00 6.25e-07 U-238 nu-fission 0.00e+00 0.00e+00 +12 (500, 5000, 50000) 6.25e-07 2.00e+01 U-235 fission 0.00e+00 0.00e+00 +13 (500, 5000, 50000) 6.25e-07 2.00e+01 U-235 nu-fission 0.00e+00 0.00e+00 +14 (500, 5000, 50000) 6.25e-07 2.00e+01 U-238 fission 0.00e+00 0.00e+00 +15 (500, 5000, 50000) 6.25e-07 2.00e+01 U-238 nu-fission 0.00e+00 0.00e+00 \ No newline at end of file diff --git a/tests/test_tally_slice_merge/test_tally_slice_merge.py b/tests/test_tally_slice_merge/test_tally_slice_merge.py new file mode 100644 index 000000000..79acf182d --- /dev/null +++ b/tests/test_tally_slice_merge/test_tally_slice_merge.py @@ -0,0 +1,165 @@ +#!/usr/bin/env python + +import os +import sys +import glob +import hashlib +import itertools +sys.path.insert(0, os.pardir) +from testing_harness import PyAPITestHarness +import openmc + + +class TallySliceMergeTestHarness(PyAPITestHarness): + def _build_inputs(self): + + # The summary.h5 file needs to be created to read in the tallies + self._input_set.settings.output = {'summary': True} + + # Initialize the tallies file + tallies_file = openmc.TalliesFile() + + # Define nuclides and scores to add to both tallies + self.nuclides = ['U-235', 'U-238'] + self.scores = ['fission', 'nu-fission'] + + # Define filters for energy and spatial domain + + low_energy = openmc.Filter(type='energy', bins=[0., 0.625e-6]) + high_energy = openmc.Filter(type='energy', bins=[0.625e-6, 20.]) + merged_energies = low_energy.merge(high_energy) + + cell_21 = openmc.Filter(type='cell', bins=[21]) + cell_27 = openmc.Filter(type='cell', bins=[27]) + distribcell_filter = openmc.Filter(type='distribcell', bins=[21]) + + self.cell_filters = [cell_21, cell_27] + self.energy_filters = [low_energy, high_energy] + + # Initialize cell tallies with filters, nuclides and scores + tallies = [] + for cell_filter in self.energy_filters: + for energy_filter in self.cell_filters: + for nuclide in self.nuclides: + for score in self.scores: + tally = openmc.Tally() + tally.estimator = 'tracklength' + tally.add_score(score) + tally.add_nuclide(nuclide) + tally.add_filter(cell_filter) + tally.add_filter(energy_filter) + tallies.append(tally) + + # Merge all cell tallies together + while len(tallies) != 1: + halfway = int(len(tallies) / 2) + zip_split = zip(tallies[:halfway], tallies[halfway:]) + tallies = list(map(lambda xy: xy[0].merge(xy[1]), zip_split)) + + # Specify a name for the tally + tallies[0].name = 'cell tally' + + # Initialize a distribcell tally + distribcell_tally = openmc.Tally(name='distribcell tally') + distribcell_tally.estimator = 'tracklength' + distribcell_tally.add_filter(distribcell_filter) + distribcell_tally.add_filter(merged_energies) + for score in self.scores: + distribcell_tally.add_score(score) + for nuclide in self.nuclides: + distribcell_tally.add_nuclide(nuclide) + + # Add tallies to a TalliesFile + tallies_file = openmc.TalliesFile() + tallies_file.add_tally(tallies[0]) + tallies_file.add_tally(distribcell_tally) + + # Export tallies to file + self._input_set.tallies = tallies_file + super(TallySliceMergeTestHarness, self)._build_inputs() + + def _get_results(self, hash_output=False): + """Digest info in the statepoint and return as a string.""" + + # Read the statepoint file. + statepoint = glob.glob(os.path.join(os.getcwd(), self._sp_name))[0] + sp = openmc.StatePoint(statepoint) + + # Read the summary file. + summary = glob.glob(os.path.join(os.getcwd(), 'summary.h5'))[0] + su = openmc.Summary(summary) + sp.link_with_summary(su) + + # Extract the cell tally + tallies = [sp.get_tally(name='cell tally')] + + # Slice the tallies by cell filter bins + cell_filter_prod = itertools.product(tallies, self.cell_filters) + tallies = map(lambda tf: tf[0].get_slice(filters=[tf[1].type], + filter_bins=[tf[1].get_bin(0)]), cell_filter_prod) + + # Slice the tallies by energy filter bins + energy_filter_prod = itertools.product(tallies, self.energy_filters) + tallies = map(lambda tf: tf[0].get_slice(filters=[tf[1].type], + filter_bins=[(tf[1].get_bin(0),)]), energy_filter_prod) + + # Slice the tallies by nuclide + nuclide_prod = itertools.product(tallies, self.nuclides) + tallies = map(lambda tn: tn[0].get_slice(nuclides=[tn[1]]), nuclide_prod) + + # Slice the tallies by score + score_prod = itertools.product(tallies, self.scores) + tallies = map(lambda ts: ts[0].get_slice(scores=[ts[1]]), score_prod) + tallies = list(tallies) + + # Initialize an output string + outstr = '' + + # Append sliced Tally Pandas DataFrames to output string + for tally in tallies: + df = tally.get_pandas_dataframe() + outstr += df.to_string() + + # Merge all tallies together + while len(tallies) != 1: + halfway = int(len(tallies) / 2) + zip_split = zip(tallies[:halfway], tallies[halfway:]) + tallies = list(map(lambda xy: xy[0].merge(xy[1]), zip_split)) + + # Append merged Tally Pandas DataFrame to output string + df = tallies[0].get_pandas_dataframe() + outstr += df.to_string() + + # Extract the distribcell tally + distribcell_tally = sp.get_tally(name='distribcell tally') + + # Sum up a few subdomains from the distribcell tally + sum1 = distribcell_tally.summation(filter_type='distribcell', + filter_bins=[0,100,2000,30000]) + # Sum up a few subdomains from the distribcell tally + sum2 = distribcell_tally.summation(filter_type='distribcell', + filter_bins=[500,5000,50000]) + + # Merge the distribcell tally slices + merge_tally = sum1.merge(sum2) + + # Append merged Tally Pandas DataFrame to output string + df = merge_tally.get_pandas_dataframe() + outstr += df.to_string() + + # Hash the results if necessary + if hash_output: + sha512 = hashlib.sha512() + sha512.update(outstr.encode('utf-8')) + outstr = sha512.hexdigest() + + return outstr + + def _cleanup(self): + super(TallySliceMergeTestHarness, self)._cleanup() + f = os.path.join(os.getcwd(), 'tallies.xml') + if os.path.exists(f): os.remove(f) + +if __name__ == '__main__': + harness = TallySliceMergeTestHarness('statepoint.10.h5', True) + harness.main() diff --git a/tests/test_trace/results_true.dat b/tests/test_trace/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_trace/results_true.dat +++ b/tests/test_trace/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_translation/results_true.dat b/tests/test_translation/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_translation/results_true.dat +++ b/tests/test_translation/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_trigger_batch_interval/results_true.dat b/tests/test_trigger_batch_interval/results_true.dat index c901e1e54..af6eea623 100644 --- a/tests/test_trigger_batch_interval/results_true.dat +++ b/tests/test_trigger_batch_interval/results_true.dat @@ -1,28 +1,28 @@ k-combined: -9.875001E-01 3.961945E-03 +9.722624E-01 1.010453E-02 tally 1: -2.128147E+01 -3.021699E+01 -4.842434E+00 -1.563989E+00 -4.695086E+00 -1.470132E+00 -1.643904E+01 -1.803258E+01 -2.128147E+01 -3.021699E+01 -4.842434E+00 -1.563989E+00 -4.695086E+00 -1.470132E+00 -1.643904E+01 -1.803258E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 tally 2: -2.128147E+01 -3.021699E+01 -4.842434E+00 -1.563989E+00 -4.695086E+00 -1.470132E+00 -1.643904E+01 -1.803258E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 diff --git a/tests/test_trigger_batch_interval/test_trigger_batch_interval.py b/tests/test_trigger_batch_interval/test_trigger_batch_interval.py index 59b900e50..a0b2119de 100644 --- a/tests/test_trigger_batch_interval/test_trigger_batch_interval.py +++ b/tests/test_trigger_batch_interval/test_trigger_batch_interval.py @@ -7,5 +7,5 @@ from testing_harness import TestHarness if __name__ == '__main__': - harness = TestHarness('statepoint.20.*', True) + harness = TestHarness('statepoint.15.*', True) harness.main() diff --git a/tests/test_trigger_no_batch_interval/results_true.dat b/tests/test_trigger_no_batch_interval/results_true.dat index d06a91646..af6eea623 100644 --- a/tests/test_trigger_no_batch_interval/results_true.dat +++ b/tests/test_trigger_no_batch_interval/results_true.dat @@ -1,28 +1,28 @@ k-combined: -9.853099E-01 3.825057E-03 +9.722624E-01 1.010453E-02 tally 1: -2.409492E+01 -3.417475E+01 -5.477076E+00 -1.765385E+00 -5.309347E+00 -1.658803E+00 -1.861784E+01 -2.040621E+01 -2.409492E+01 -3.417475E+01 -5.477076E+00 -1.765385E+00 -5.309347E+00 -1.658803E+00 -1.861784E+01 -2.040621E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 tally 2: -2.409492E+01 -3.417475E+01 -5.477076E+00 -1.765385E+00 -5.309347E+00 -1.658803E+00 -1.861784E+01 -2.040621E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 diff --git a/tests/test_trigger_no_batch_interval/test_trigger_no_batch_interval.py b/tests/test_trigger_no_batch_interval/test_trigger_no_batch_interval.py index f9cb68d62..a0b2119de 100644 --- a/tests/test_trigger_no_batch_interval/test_trigger_no_batch_interval.py +++ b/tests/test_trigger_no_batch_interval/test_trigger_no_batch_interval.py @@ -7,5 +7,5 @@ from testing_harness import TestHarness if __name__ == '__main__': - harness = TestHarness('statepoint.22.*', True) + harness = TestHarness('statepoint.15.*', True) harness.main() diff --git a/tests/test_trigger_no_status/results_true.dat b/tests/test_trigger_no_status/results_true.dat index 0b541099b..c7f1b407a 100644 --- a/tests/test_trigger_no_status/results_true.dat +++ b/tests/test_trigger_no_status/results_true.dat @@ -1,28 +1,28 @@ k-combined: -9.906276E-01 1.800527E-03 +9.733783E-01 1.678094E-02 tally 1: -7.043320E+00 -9.922203E+00 -1.610208E+00 -5.185662E-01 -1.564118E+00 -4.893096E-01 -5.433111E+00 -5.904259E+00 -7.043320E+00 -9.922203E+00 -1.610208E+00 -5.185662E-01 -1.564118E+00 -4.893096E-01 -5.433111E+00 -5.904259E+00 +6.901811E+00 +9.536643E+00 +1.572259E+00 +4.947922E-01 +1.527087E+00 +4.667459E-01 +5.329553E+00 +5.686973E+00 +6.901811E+00 +9.536643E+00 +1.572259E+00 +4.947922E-01 +1.527087E+00 +4.667459E-01 +5.329553E+00 +5.686973E+00 tally 2: -7.043320E+00 -9.922203E+00 -1.610208E+00 -5.185662E-01 -1.564118E+00 -4.893096E-01 -5.433111E+00 -5.904259E+00 +6.901811E+00 +9.536643E+00 +1.572259E+00 +4.947922E-01 +1.527087E+00 +4.667459E-01 +5.329553E+00 +5.686973E+00 diff --git a/tests/test_trigger_tallies/results_true.dat b/tests/test_trigger_tallies/results_true.dat index 0519260dd..af6eea623 100644 --- a/tests/test_trigger_tallies/results_true.dat +++ b/tests/test_trigger_tallies/results_true.dat @@ -1,28 +1,28 @@ k-combined: -9.875396E-01 4.095985E-03 +9.722624E-01 1.010453E-02 tally 1: -1.415943E+01 -2.006888E+01 -3.225529E+00 -1.040975E+00 -3.128858E+00 -9.794019E-01 -1.093390E+01 -1.196901E+01 -1.415943E+01 -2.006888E+01 -3.225529E+00 -1.040975E+00 -3.128858E+00 -9.794019E-01 -1.093390E+01 -1.196901E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 tally 2: -1.415943E+01 -2.006888E+01 -3.225529E+00 -1.040975E+00 -3.128858E+00 -9.794019E-01 -1.093390E+01 -1.196901E+01 +1.392936E+01 +1.941888E+01 +3.159556E+00 +9.989777E-01 +3.063616E+00 +9.391667E-01 +1.076980E+01 +1.160931E+01 diff --git a/tests/test_uniform_fs/results_true.dat b/tests/test_uniform_fs/results_true.dat index a29a363b2..d27d63f56 100644 --- a/tests/test_uniform_fs/results_true.dat +++ b/tests/test_uniform_fs/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.546115E-01 2.982307E-03 +3.634132E-01 6.507584E-03 diff --git a/tests/test_union_energy_grids/results_true.dat b/tests/test_union_energy_grids/results_true.dat index 9556a981b..0a607592c 100644 --- a/tests/test_union_energy_grids/results_true.dat +++ b/tests/test_union_energy_grids/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.155788E-01 7.559348E-03 +3.330789E-01 2.216495E-03 diff --git a/tests/test_universe/results_true.dat b/tests/test_universe/results_true.dat index 5263a6b7f..7b2fbf37f 100644 --- a/tests/test_universe/results_true.dat +++ b/tests/test_universe/results_true.dat @@ -1,2 +1,2 @@ k-combined: -3.021779E-01 3.813358E-03 +2.943619E-01 3.309635E-03 diff --git a/tests/test_void/results_true.dat b/tests/test_void/results_true.dat index 4e99b8676..48be2778a 100644 --- a/tests/test_void/results_true.dat +++ b/tests/test_void/results_true.dat @@ -1,2 +1,2 @@ k-combined: -1.045350E+00 2.750547E-02 +1.062505E+00 2.674375E-02 diff --git a/tests/testing_harness.py b/tests/testing_harness.py index 66cadfe63..7d6dbc914 100644 --- a/tests/testing_harness.py +++ b/tests/testing_harness.py @@ -12,7 +12,7 @@ import sys import numpy as np sys.path.insert(0, os.path.join(os.pardir, os.pardir)) -from input_set import InputSet +from input_set import InputSet, MGInputSet from openmc.statepoint import StatePoint from openmc.executor import Executor import openmc.particle_restart as pr @@ -243,12 +243,14 @@ class ParticleRestartTestHarness(TestHarness): class PyAPITestHarness(TestHarness): - def __init__(self, statepoint_name, tallies_present=False): + def __init__(self, statepoint_name, tallies_present=False, mg=False): super(PyAPITestHarness, self).__init__(statepoint_name, tallies_present) self.parser.add_option('--build-inputs', dest='build_only', action='store_true', default=False) - self._input_set = InputSet() - + if mg: + self._input_set = MGInputSet() + else: + self._input_set = InputSet() def main(self): """Accept commandline arguments and either run or update tests.""" (self._opts, self._args) = self.parser.parse_args()