mirror of
https://github.com/openmc-dev/openmc.git
synced 2026-07-26 05:05:30 -04:00
Added a scatter_shape parameter to the library format and the ability to read/write it (but do nothing with it aside from check for the default value). Also converted back from is checks in the python for a string to ==, since is does not work for many cases
This commit is contained in:
parent
29c48ee23e
commit
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6 changed files with 128 additions and 104 deletions
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@ -38,10 +38,10 @@ MGXS Library Specification
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The data within <library name> contains the temperature-dependent multi-group
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data for the nuclide or material that it represents.
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:Attributes: - **atomic_weight_ratio** (*double*) -- The atomic weight ratio (optional,
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i.e. it is not meaningful for material-wise data)
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- **fissionable** (*int*) -- Whether the dataset is fissionable
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(1) or not (0).
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:Attributes: - **atomic_weight_ratio** (*double*) -- The atomic weight ratio
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(optional, i.e. it is not meaningful for material-wise data).
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- **fissionable** (*bool*) -- Whether the dataset is fissionable
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(True) or not (False).
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- **representation** (*char[]*) -- The method used to generate and
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represent the multi-group cross sections. That is, whether they
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were generated with scalar flux weighting (or reduced to a
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@ -65,6 +65,15 @@ data for the nuclide or material that it represents.
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or number of points (depending on the value of `scatter_format`)
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used to describe the angular distribution associated with each
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group-to-group transfer probability.
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- **scatter_shape** (*char[]*) -- The shape of the provided
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scatter and multiplicity matrix. The values provided are strings
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describing the ordering the scattering array is provided in
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row-major (i.e., C/C++ and Python) indexing. Valid values are
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"[Order][G][G']" or "[Order][G'][G]" where "G'" denotes the
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secondary/outgoing energy groups, "G" denotes the incoming
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energy groups, and "Order" is the angular distribution index.
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This value is not required; if not the default value of
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"[Order][G][G']" will be assumed.
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**/<library name>/kTs/**
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@ -79,29 +88,29 @@ Temperature-dependent data, provided for temperature <TTT>K.
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:Datasets: - **total** (*double[]* or *double[][][]*) -- Total cross section.
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This is a 1-D vector if `representation` is "isotropic", or a 3-D
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vector if `representation` is "angle" with dimensions of
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[groups, azimuthal, polar].
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[groups][azimuthal][polar].
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- **absorption** (*double[]* or *double[][][]*) -- Absorption
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cross section.
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This is a 1-D vector if `representation` is "isotropic", or a 3-D
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vector if `representation` is "angle" with dimensions of
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[groups, azimuthal, polar].
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[groups][azimuthal][polar].
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- **fission** (*double[]* or *double[][][]*) -- Fission
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cross section.
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This is a 1-D vector if `representation` is "isotropic", or a 3-D
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vector if `representation` is "angle" with dimensions of
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[groups, azimuthal, polar]. This is only required if the dataset
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[groups][azimuthal][polar]. This is only required if the dataset
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is fissionable and fission-tallies are expected to be used.
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- **kappa-fission** (*double[]* or *double[][][]*) -- Kappa-Fission
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(energy-release from fission) cross section.
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This is a 1-D vector if `representation` is "isotropic", or a 3-D
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vector if `representation` is "angle" with dimensions of
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[groups, azimuthal, polar]. This is only required if the dataset
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[groups][azimuthal][polar]. This is only required if the dataset
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is fissionable and fission-tallies are expected to be used.
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- **chi** (*double[]* or *double[][][]*) -- Fission neutron energy
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spectra.
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This is a 1-D vector if `representation` is "isotropic", or a 3-D
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vector if `representation` is "angle" with dimensions of
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[groups, azimuthal, polar]. This is only required if the dataset
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[groups][azimuthal][polar]. This is only required if the dataset
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is fissionable and fission-tallies are expected to be used.
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- **nu-fission** (*double[]* to *double[][][][]*) -- Nu-Fission
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cross section.
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@ -119,34 +128,30 @@ Temperature-dependent data, provided for temperature <TTT>K.
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Data specific to neutron scattering for the temperature <TTT>K
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:Datasets: - **g_min** (*int[]* or *int[][][]*) --
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Minimum (most energetic) outgoing groups with non-zero values of
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the scattering matrix. These group numbers use the standard
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Minimum (most energetic) groups with non-zero values of
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the scattering matrix provided. If `scatter_shape` is
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"[Order][G][G']" then `g_min` will describe the minimum values
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of "G'" for each "G"; if `scatter_shape` is "[Order][G'][G]"
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then `g_min` will describe the minimum values of "G" for each "G'".
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These group numbers use the standard
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ordering where the fastest neutron energy group is group 1 while
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the slowest neutron energy group is group G.
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The dimensionality of `g_min` is:
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`g_min[g_in]`, or `g_min[num_polar][num_azimuthal][g_in]`.
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`g_min[g]`, or `g_min[num_polar][num_azimuthal][g]`.
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The former is used when `representation` is "isotropic", and the
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latter when `representation` is "angle".
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- **g_max** (*int[]* or *int[][][]*) --
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Maximum (least energetic) outgoing groups with non-zero values of
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the scattering matrix. These group numbers use the standard
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ordering where the fastest neutron energy group is group 1 while
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the slowest neutron energy group is group G.
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The dimensionality of `g_max` is:
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`g_max[g_in]`, or `g_max[num_polar][num_azimuthal][g_in]`.
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The former is used when `representation` is "isotropic", and the
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latter when `representation` is "angle".
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Similar to `g_min`, except this dataset describes the maximum
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(least energetic) groups with non-zero values of
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the scattering matrix.
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- **scatter_matrix** (*double[]*) -- Flattened representation of the
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scattering moment matrices. The pre-flattened array is shaped as
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follows (in row-major format):
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`scatter_matrix[order(+1)][g_in][g_out]`, or
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`scatter_matrix[num_polar][num_azimuthal][order(+1)][g_in][g_out]`
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The former is used when `representation` is "isotropic", and the
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latter when `representation` is "angle". Note that if the value of
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`scatter_format` is "legendre", the order dimension will be one
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larger than the value of `order`, otherwise it will match `order`.
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Finally, the g_out dimension has a dimensionality of
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`g_min` to `g_max`.
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scattering moment matrices. The pre-flattened array corresponds to
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the shape provied in `scatter_shape`, but if `representation` is
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"angle" the dimensionality in `scatter_shape` is prepended by
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"[num_polar][num_azimuthal]" dimensions. The right-most energy
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group dimension will only include the entries between `g_min` and
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`g_max`.
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dimension has a dimensionality of `g_min` to `g_max`.
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- **multiplicity_matrix** (*double[]*) -- Flattened representation of
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the scattering moment matrices. This dataset provides the code with
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a scaling factor to account for neutrons being produced in (n,xn)
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@ -154,9 +159,6 @@ Data specific to neutron scattering for the temperature <TTT>K
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for every Legendre moment or histogram/tabular bin. This dataset is
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optional, if it is not provided no multiplication (i.e., values of
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1.0) will be assumed.
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The pre-flattened array is shaped as follows (in row-major format):
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`multiplicity_matrix[g_in][g_out]`, or
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`multiplicity_matrix[num_polar][num_azimuthal][g_in][g_out]`
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The former is used when `representation` is "isotropic", and the
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latter when `representation` is "angle". Finally, the g_out
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dimension has a dimensionality of `g_min` to `g_max`.
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The pre-flattened array is shapes consistent with `scatter_matrix`
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except the "[Order]" dimension in `scatter_shape` is ignored since
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this data is assumed isotropic.
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@ -186,14 +186,14 @@ class Library(object):
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@property
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def domains(self):
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if self._domains is 'all':
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if self.domain_type is 'material':
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if self._domains == 'all':
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if self.domain_type == 'material':
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return self.openmc_geometry.get_all_materials()
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elif self.domain_type in ['cell', 'distribcell']:
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return self.openmc_geometry.get_all_material_cells()
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elif self.domain_type is 'universe':
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elif self.domain_type == 'universe':
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return self.openmc_geometry.get_all_universes()
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elif self.domain_type is 'mesh':
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elif self.domain_type == 'mesh':
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raise ValueError('Unable to get domains for Mesh domain type')
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else:
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raise ValueError('Unable to get domains without a domain type')
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@ -265,7 +265,7 @@ class Library(object):
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@mgxs_types.setter
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def mgxs_types(self, mgxs_types):
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all_mgxs_types = openmc.mgxs.MGXS_TYPES + openmc.mgxs.MDGXS_TYPES
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if mgxs_types is 'all':
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if mgxs_types == 'all':
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self._mgxs_types = all_mgxs_types
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else:
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cv.check_iterable_type('mgxs_types', mgxs_types, basestring)
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@ -277,7 +277,7 @@ class Library(object):
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def by_nuclide(self, by_nuclide):
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cv.check_type('by_nuclide', by_nuclide, bool)
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if by_nuclide == True and self.domain_type is 'mesh':
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if by_nuclide == True and self.domain_type == 'mesh':
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raise ValueError('Unable to create MGXS library by nuclide with '
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'mesh domain')
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@ -287,7 +287,7 @@ class Library(object):
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def domain_type(self, domain_type):
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cv.check_value('domain type', domain_type, openmc.mgxs.DOMAIN_TYPES)
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if self.by_nuclide == True and domain_type is 'mesh':
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if self.by_nuclide == True and domain_type == 'mesh':
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raise ValueError('Unable to create MGXS library by nuclide with '
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'mesh domain')
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@ -297,21 +297,21 @@ class Library(object):
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def domains(self, domains):
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# Use all materials, cells or universes in the geometry as domains
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if domains is 'all':
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if domains == 'all':
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self._domains = domains
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# User specified a list of material, cell or universe domains
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else:
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if self.domain_type is 'material':
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if self.domain_type == 'material':
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cv.check_iterable_type('domain', domains, openmc.Material)
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all_domains = self.openmc_geometry.get_all_materials()
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elif self.domain_type in ['cell', 'distribcell']:
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cv.check_iterable_type('domain', domains, openmc.Cell)
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all_domains = self.openmc_geometry.get_all_material_cells()
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elif self.domain_type is 'universe':
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elif self.domain_type == 'universe':
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cv.check_iterable_type('domain', domains, openmc.Universe)
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all_domains = self.openmc_geometry.get_all_universes()
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elif self.domain_type is 'mesh':
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elif self.domain_type == 'mesh':
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cv.check_iterable_type('domain', domains, openmc.Mesh)
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# The mesh and geometry are independent, so set all_domains
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@ -355,7 +355,7 @@ class Library(object):
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def correction(self, correction):
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cv.check_value('correction', correction, ('P0', None))
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if correction is 'P0' and self.legendre_order > 0:
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if correction == 'P0' and self.legendre_order > 0:
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warn('The P0 correction will be ignored since the scattering '
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'order "{}" is greater than zero'.format(self.legendre_order))
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@ -367,7 +367,7 @@ class Library(object):
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cv.check_greater_than('legendre_order', legendre_order, 0, equality=True)
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cv.check_less_than('legendre_order', legendre_order, 10, equality=True)
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if self.correction is 'P0' and legendre_order > 0:
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if self.correction == 'P0' and legendre_order > 0:
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msg = 'The P0 correction will be ignored since the scattering ' \
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'order {} is greater than zero'.format(self.legendre_order)
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warn(msg, RuntimeWarning)
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@ -505,7 +505,7 @@ class Library(object):
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self._openmc_geometry = statepoint.summary.openmc_geometry
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self._nuclides = statepoint.summary.nuclides
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if statepoint.run_mode is 'k-eigenvalue':
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if statepoint.run_mode == 'k-eigenvalue':
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self._keff = statepoint.k_combined[0]
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# Load tallies for each MGXS for each domain and mgxs type
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@ -543,13 +543,13 @@ class Library(object):
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"""
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if self.domain_type is 'material':
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if self.domain_type == 'material':
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cv.check_type('domain', domain, (openmc.Material, Integral))
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elif self.domain_type is 'cell' or self.domain_type is 'distribcell':
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elif self.domain_type == 'cell' or self.domain_type == 'distribcell':
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cv.check_type('domain', domain, (openmc.Cell, Integral))
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elif self.domain_type is 'universe':
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elif self.domain_type == 'universe':
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cv.check_type('domain', domain, (openmc.Universe, Integral))
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elif self.domain_type is 'mesh':
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elif self.domain_type == 'mesh':
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cv.check_type('domain', domain, (openmc.Mesh, Integral))
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# Check that requested domain is included in library
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@ -662,7 +662,7 @@ class Library(object):
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# Clone this Library to initialize the subdomain-averaged version
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subdomain_avg_library = copy.deepcopy(self)
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if subdomain_avg_library.domain_type is 'distribcell':
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if subdomain_avg_library.domain_type == 'distribcell':
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subdomain_avg_library.domain_type = 'cell'
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else:
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return subdomain_avg_library
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@ -671,7 +671,7 @@ class Library(object):
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for domain in self.domains:
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for mgxs_type in self.mgxs_types:
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mgxs = subdomain_avg_library.get_mgxs(domain, mgxs_type)
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if mgxs.domain_type is 'distribcell':
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if mgxs.domain_type == 'distribcell':
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avg_mgxs = mgxs.get_subdomain_avg_xs()
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subdomain_avg_library.all_mgxs[domain.id][mgxs_type] = avg_mgxs
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@ -751,7 +751,7 @@ class Library(object):
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for mgxs_type in self.mgxs_types:
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mgxs = self.all_mgxs[domain.id][mgxs_type]
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if subdomains is 'avg':
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if subdomains == 'avg':
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mgxs = mgxs.get_subdomain_avg_xs()
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mgxs.build_hdf5_store(filename, directory, xs_type=xs_type,
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@ -896,7 +896,7 @@ class Library(object):
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# Build & add metadata to XSdata object
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name = xsdata_name
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if nuclide is not 'total':
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if nuclide != 'total':
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name += '_' + nuclide
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xsdata = openmc.XSdata(name, self.energy_groups)
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@ -912,7 +912,7 @@ class Library(object):
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self.scatter_format = 'legendre'
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self.representation = 'isotropic'
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if nuclide is not 'total':
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if nuclide != 'total':
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xsdata.atomic_weight_ratio = self._nuclides[nuclide][1]
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if subdomain is None:
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@ -921,7 +921,7 @@ class Library(object):
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subdomain = [subdomain]
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# Now get xs data itself
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if 'nu-transport' in self.mgxs_types and self.correction is 'P0':
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if 'nu-transport' in self.mgxs_types and self.correction == 'P0':
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mymgxs = self.get_mgxs(domain, 'nu-transport')
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xsdata.set_total_mgxs(mymgxs, xs_type=xs_type, nuclide=[nuclide],
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subdomain=subdomain)
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@ -1056,7 +1056,7 @@ class Library(object):
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# Initialize file
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mgxs_file = openmc.MGXSLibrary(self.energy_groups)
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if self.domain_type is 'mesh':
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if self.domain_type == 'mesh':
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# Create the xsdata objects and add to the mgxs_file
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i = 0
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for domain in self.domains:
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@ -1089,7 +1089,7 @@ class Library(object):
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xsdata_name = 'set' + str(i + 1)
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else:
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xsdata_name = xsdata_names[i]
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if nuclide is not 'total':
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if nuclide != 'total':
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xsdata_name += '_' + nuclide
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xsdata = self.get_xsdata(domain, xsdata_name,
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@ -1159,14 +1159,14 @@ class Library(object):
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# the multiple meshes could be overlapping or in disparate regions
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# of the continuous energy model. The next step makes sure there is
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# only one before continuing.
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if self.domain_type is 'mesh':
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if self.domain_type == 'mesh':
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cv.check_length("domains", self.domains, 1, 1)
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# Get the MGXS File Data
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mgxs_file = self.create_mg_library('macro', xsdata_names)
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# Now move on the creating the geometry and assigning materials
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if self.domain_type is 'mesh':
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if self.domain_type == 'mesh':
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root = openmc.Universe(name='root', universe_id=0)
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# Add cells representative of the mesh with reflective BC
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@ -1212,13 +1212,13 @@ class Library(object):
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materials.append(material)
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# Differentiate Geometry with new Material
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if self.domain_type is 'material':
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if self.domain_type == 'material':
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# Fill all appropriate Cells with new Material
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for cell in all_cells:
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if cell.fill.id == domain.id:
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cell.fill = material
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elif self.domain_type is 'cell':
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elif self.domain_type == 'cell':
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for cell in all_cells:
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if cell.id == domain.id:
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cell.fill = material
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@ -1283,7 +1283,7 @@ class Library(object):
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('nu-transport' not in self.mgxs_types))):
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error_flag = True
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warn('A "nu-transport" MGXS type is required since a "P0" '
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'correction is applied, but a "nu-transport" MGXS is '
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'correction is applied, but a "nu-transport" MGXS == '
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'not provided.')
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elif (((self.correction is None) and
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('total' not in self.mgxs_types))):
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@ -8,7 +8,7 @@ import h5py
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import openmc
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import openmc.mgxs
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from openmc.checkvalue import check_type, check_value, check_greater_than, \
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check_less_than, check_iterable_type
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check_iterable_type
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if sys.version_info[0] >= 3:
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basestring = str
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@ -16,6 +16,7 @@ if sys.version_info[0] >= 3:
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# Supported incoming particle MGXS angular treatment representations
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_REPRESENTATIONS = ['isotropic', 'angle']
|
||||
_SCATTER_TYPES = ['tabular', 'legendre', 'histogram']
|
||||
_SCATTER_SHAPES = ["[Order][G][G']"]
|
||||
|
||||
|
||||
class XSdata(object):
|
||||
|
|
@ -51,6 +52,8 @@ class XSdata(object):
|
|||
Whether or not this is a fissionable data set.
|
||||
scatter_format : {'legendre', 'histogram', or 'tabular'}
|
||||
Angular distribution representation (legendre, histogram, or tabular)
|
||||
scatter_shapes : {"[Order][G][G']"}
|
||||
Dimensionality of the scattering and multiplicity matrices
|
||||
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
|
||||
|
|
@ -106,8 +109,8 @@ class XSdata(object):
|
|||
:attr:`XSdata.nu_fission` attribute instead.
|
||||
nu_fission : dict of numpy.ndarray
|
||||
Group-wise fission production cross section vector (i.e., if
|
||||
:attr:`XSdata.chi` is provided), or is the group-wise fission production
|
||||
matrix.
|
||||
:attr:`XSdata.chi` is provided), or is the group-wise fission
|
||||
production matrix.
|
||||
inverse_velocities : dict of numpy.ndarray
|
||||
Inverse of velocities, in units of sec/cm.
|
||||
|
||||
|
|
@ -142,6 +145,7 @@ class XSdata(object):
|
|||
self._atomic_weight_ratio = None
|
||||
self._fissionable = False
|
||||
self._scatter_format = 'legendre'
|
||||
self._scatter_shape = "[Order][G][G']"
|
||||
self._order = None
|
||||
self._num_polar = None
|
||||
self._num_azimuthal = None
|
||||
|
|
@ -184,6 +188,10 @@ class XSdata(object):
|
|||
def scatter_format(self):
|
||||
return self._scatter_format
|
||||
|
||||
@property
|
||||
def scatter_shape(self):
|
||||
return self._scatter_shape
|
||||
|
||||
@property
|
||||
def order(self):
|
||||
return self._order
|
||||
|
|
@ -242,28 +250,28 @@ class XSdata(object):
|
|||
|
||||
@property
|
||||
def vector_shape(self):
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
return (self.energy_groups.num_groups,)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
return (self.num_polar, self.num_azimuthal,
|
||||
self.energy_groups.num_groups)
|
||||
|
||||
@property
|
||||
def matrix_shape(self):
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
return (self.energy_groups.num_groups,
|
||||
self.energy_groups.num_groups)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
return (self.num_polar, self.num_azimuthal,
|
||||
self.energy_groups.num_groups,
|
||||
self.energy_groups.num_groups)
|
||||
|
||||
@property
|
||||
def pn_matrix_shape(self):
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
return (self.num_orders, self.energy_groups.num_groups,
|
||||
self.energy_groups.num_groups)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
return (self.num_polar, self.num_azimuthal, self.num_orders,
|
||||
self.energy_groups.num_groups,
|
||||
self.energy_groups.num_groups)
|
||||
|
|
@ -309,6 +317,12 @@ class XSdata(object):
|
|||
check_value('scatter_format', scatter_format, _SCATTER_TYPES)
|
||||
self._scatter_format = scatter_format
|
||||
|
||||
@scatter_shape.setter
|
||||
def scatter_shape(self, scatter_shape):
|
||||
# check to see it is of a valid type and value
|
||||
check_value('scatter_shape', scatter_shape, _SCATTER_SHAPES)
|
||||
self._scatter_shape = scatter_shape
|
||||
|
||||
@order.setter
|
||||
def order(self, order):
|
||||
# Check type and value
|
||||
|
|
@ -694,10 +708,10 @@ class XSdata(object):
|
|||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
self._total[i] = total.get_xs(nuclides=nuclide, xs_type=xs_type,
|
||||
subdomains=subdomain)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -740,11 +754,11 @@ class XSdata(object):
|
|||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
self._absorption[i] = absorption.get_xs(nuclides=nuclide,
|
||||
xs_type=xs_type,
|
||||
subdomains=subdomain)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -787,11 +801,11 @@ class XSdata(object):
|
|||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
self._fission[i] = fission.get_xs(nuclides=nuclide,
|
||||
xs_type=xs_type,
|
||||
subdomains=subdomain)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -835,11 +849,11 @@ class XSdata(object):
|
|||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
self._nu_fission[i] = nu_fission.get_xs(nuclides=nuclide,
|
||||
xs_type=xs_type,
|
||||
subdomains=subdomain)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -892,11 +906,11 @@ class XSdata(object):
|
|||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
self._kappa_fission[i] = k_fission.get_xs(nuclides=nuclide,
|
||||
xs_type=xs_type,
|
||||
subdomains=subdomain)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -943,10 +957,10 @@ class XSdata(object):
|
|||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
self._chi[i] = chi.get_xs(nuclides=nuclide,
|
||||
xs_type=xs_type, subdomains=subdomain)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -994,7 +1008,7 @@ class XSdata(object):
|
|||
check_type('temperature', temperature, Real)
|
||||
check_value('temperature', temperature, self.temperatures)
|
||||
|
||||
if self.scatter_format is not 'legendre':
|
||||
if self.scatter_format != 'legendre':
|
||||
msg = 'Anisotropic scattering representations other than ' \
|
||||
'Legendre expansions have not yet been implemented in ' \
|
||||
'openmc.mgxs.'
|
||||
|
|
@ -1011,7 +1025,7 @@ class XSdata(object):
|
|||
[self.order])
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
# Get the scattering orders in the outermost dimension
|
||||
self._scatter_matrix[i] = np.zeros((self.num_orders,
|
||||
self.energy_groups.num_groups,
|
||||
|
|
@ -1021,7 +1035,7 @@ class XSdata(object):
|
|||
scatter.get_xs(nuclides=nuclide, xs_type=xs_type,
|
||||
moment=moment, subdomains=subdomain)
|
||||
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
|
||||
|
|
@ -1089,7 +1103,7 @@ class XSdata(object):
|
|||
['universe', 'cell', 'material', 'mesh'])
|
||||
|
||||
i = np.where(self.temperatures == temperature)[0][0]
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
nuscatt = nuscatter.get_xs(nuclides=nuclide,
|
||||
xs_type=xs_type, moment=0,
|
||||
subdomains=subdomain)
|
||||
|
|
@ -1100,7 +1114,7 @@ class XSdata(object):
|
|||
xs_type=xs_type, moment=0,
|
||||
subdomains=subdomain)
|
||||
self._multiplicity_matrix[i] = np.divide(nuscatt, scatt)
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
msg = 'Angular-Dependent MGXS have not yet been implemented'
|
||||
raise ValueError(msg)
|
||||
self._multiplicity_matrix[i] = \
|
||||
|
|
@ -1123,7 +1137,7 @@ class XSdata(object):
|
|||
if self.representation is not None:
|
||||
grp.attrs['representation'] = np.array(self.representation,
|
||||
dtype='S')
|
||||
if self.representation is 'angle':
|
||||
if self.representation == 'angle':
|
||||
if self.num_azimuthal is not None:
|
||||
grp.attrs['num_azimuthal'] = self.num_azimuthal
|
||||
if self.num_polar is not None:
|
||||
|
|
@ -1131,6 +1145,9 @@ class XSdata(object):
|
|||
if self.scatter_format is not None:
|
||||
grp.attrs['scatter_format'] = np.array(self.scatter_format,
|
||||
dtype='S')
|
||||
if self.scatter_shape is not None:
|
||||
grp.attrs['scatter_shape'] = np.array(self.scatter_shape,
|
||||
dtype='S')
|
||||
if self.order is not None:
|
||||
grp.attrs['order'] = self.order
|
||||
|
||||
|
|
@ -1170,7 +1187,7 @@ class XSdata(object):
|
|||
|
||||
# Get the sparse scattering data to print to the library
|
||||
G = self.energy_groups.num_groups
|
||||
if self.representation is 'isotropic':
|
||||
if self.representation == 'isotropic':
|
||||
g_out_bounds = np.zeros((G, 2), dtype=np.int)
|
||||
for g_in in range(G):
|
||||
nz = np.nonzero(self._scatter_matrix[i][0, g_in, :])
|
||||
|
|
@ -1206,7 +1223,7 @@ class XSdata(object):
|
|||
scatt_grp.create_dataset("g_min", data=g_out_bounds[:, 0])
|
||||
scatt_grp.create_dataset("g_max", data=g_out_bounds[:, 1])
|
||||
|
||||
elif self.representation is 'angle':
|
||||
elif self.representation == 'angle':
|
||||
Np = self.num_polar
|
||||
Na = self.num_azimuthal
|
||||
g_out_bounds = np.zeros((Np, Na, G, 2), dtype=np.int)
|
||||
|
|
|
|||
|
|
@ -47,14 +47,12 @@ def parse_args():
|
|||
help='input XML file')
|
||||
parser.add_argument('-o', '--output', nargs='?', default='',
|
||||
help='output file, in HDF5 format')
|
||||
parser.add_argument('-c', '--compression', type=int,
|
||||
help='HDF5 Compression Level')
|
||||
args = vars(parser.parse_args())
|
||||
|
||||
if args['output'] is '':
|
||||
if args['output'] == '':
|
||||
filename = args['input'].name
|
||||
extension = filenameos.path.splitext()
|
||||
if extension is '.xml':
|
||||
if extension == '.xml':
|
||||
filename = filename[:filename.rfind('.')] + '.h5'
|
||||
args['output'] = filename
|
||||
|
||||
|
|
@ -75,7 +73,7 @@ def get_data(element, entry):
|
|||
return value
|
||||
|
||||
|
||||
if __name__ is '__main__':
|
||||
if __name__ == '__main__':
|
||||
args = parse_args()
|
||||
|
||||
# Parse the XML data.
|
||||
|
|
@ -117,7 +115,7 @@ if __name__ is '__main__':
|
|||
representation = get_data(xsdata_elem, 'representation')
|
||||
if representation is None:
|
||||
representation = 'isotropic'
|
||||
if representation is 'angle':
|
||||
if representation == 'angle':
|
||||
n_azi = int(get_data(xsdata_elem, 'num_azimuthal'))
|
||||
n_pol = int(get_data(xsdata_elem, 'num_polar'))
|
||||
|
||||
|
|
@ -146,14 +144,14 @@ if __name__ is '__main__':
|
|||
representation=representation))
|
||||
if awr is not None:
|
||||
xsd[-1].atomic_weight_ratio = awr
|
||||
if representation is 'angle':
|
||||
if representation == 'angle':
|
||||
xsd[-1].num_azimuthal = n_azi
|
||||
xsd[-1].num_polar = n_pol
|
||||
xsd[-1].scatter_format = scatter_format
|
||||
xsd[-1].order = order
|
||||
names.append(name)
|
||||
|
||||
if scatter_format is 'legendre':
|
||||
if scatter_format == 'legendre':
|
||||
order_dim = order + 1
|
||||
else:
|
||||
order_dim = order
|
||||
|
|
|
|||
|
|
@ -338,6 +338,13 @@ module mgxs_header
|
|||
else
|
||||
this % scatter_format = ANGLE_LEGENDRE
|
||||
end if
|
||||
if (attribute_exists(xs_id, "scatter_shape")) then
|
||||
call read_attribute(temp_str, xs_id, "scatter_shape")
|
||||
temp_str = trim(temp_str)
|
||||
if (to_lower(temp_str) /= "[order][g][g']") then
|
||||
call fatal_error("Invalid scatter_shape option!")
|
||||
end if
|
||||
end if
|
||||
if (attribute_exists(xs_id, "fissionable")) then
|
||||
call read_attribute(this % fissionable, xs_id, "fissionable")
|
||||
else
|
||||
|
|
|
|||
BIN
tests/1d_mgxs.h5
BIN
tests/1d_mgxs.h5
Binary file not shown.
Loading…
Add table
Add a link
Reference in a new issue