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Update tally arithmetic notebook to fix an error in thermal flux
utilization. Also make equations prettier.
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1 changed files with 32 additions and 25 deletions
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@ -572,7 +572,7 @@
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" Copyright: 2011-2015 Massachusetts Institute of Technology\n",
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" License: http://mit-crpg.github.io/openmc/license.html\n",
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" Version: 0.6.2\n",
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" Date/Time: 2015-08-10 06:51:18\n",
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" Date/Time: 2015-08-10 13:21:32\n",
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" MPI Processes: 4\n",
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"\n",
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" ===========================================================================\n",
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@ -628,20 +628,20 @@
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"\n",
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" =======================> TIMING STATISTICS <=======================\n",
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"\n",
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" Total time for initialization = 8.9900E-01 seconds\n",
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" Reading cross sections = 2.5700E-01 seconds\n",
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" Total time in simulation = 9.5070E+00 seconds\n",
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" Time in transport only = 8.6890E+00 seconds\n",
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" Time in inactive batches = 1.0080E+00 seconds\n",
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" Time in active batches = 8.4990E+00 seconds\n",
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" Time synchronizing fission bank = 7.8300E-01 seconds\n",
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" Sampling source sites = 4.4000E-02 seconds\n",
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" SEND/RECV source sites = 0.0000E+00 seconds\n",
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" Time accumulating tallies = 3.0000E-03 seconds\n",
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" Total time for initialization = 1.4260E+00 seconds\n",
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" Reading cross sections = 3.8800E-01 seconds\n",
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" Total time in simulation = 9.0700E+00 seconds\n",
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" Time in transport only = 8.3270E+00 seconds\n",
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" Time in inactive batches = 1.4110E+00 seconds\n",
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" Time in active batches = 7.6590E+00 seconds\n",
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" Time synchronizing fission bank = 6.7300E-01 seconds\n",
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" Sampling source sites = 1.1000E-02 seconds\n",
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" SEND/RECV source sites = 2.0000E-03 seconds\n",
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" Time accumulating tallies = 1.0000E-03 seconds\n",
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" Total time for finalization = 2.0000E-03 seconds\n",
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" Total time elapsed = 1.0410E+01 seconds\n",
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" Calculation Rate (inactive) = 12400.8 neutrons/second\n",
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" Calculation Rate (active) = 4412.28 neutrons/second\n",
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" Total time elapsed = 1.0500E+01 seconds\n",
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" Calculation Rate (inactive) = 8858.97 neutrons/second\n",
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" Calculation Rate (active) = 4896.20 neutrons/second\n",
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"\n",
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" ============================> RESULTS <============================\n",
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"\n",
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@ -726,7 +726,8 @@
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"metadata": {},
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"source": [
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"We have a tally of the total fission rate and the total absorption rate, so we can calculate k-infinity as:\n",
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"$$k_\\infty = \\frac{\\nu \\Sigma_f \\phi}{\\Sigma_a \\phi}$$"
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"$$k_\\infty = \\frac{\\langle \\nu \\Sigma_f \\phi \\rangle}{\\langle \\Sigma_a \\phi \\rangle}$$\n",
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"In this notation, $\\langle \\cdot \\rangle^a_b$ represents an OpenMC that is integrated over region $a$ and energy range $b$. If $a$ or $b$ is not reported, it means the value represents an integral over all space or all energy, respectively."
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]
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},
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{
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@ -794,7 +795,7 @@
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"source": [
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"Notice that even though the neutron production rate and absorption rate are separate tallies, we still get a first-order estimate of the uncertainty on the quotient of them automatically!\n",
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"\n",
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"Now, let's analyze of few of the classic factors in the four-factor formula, starting with the resonance escape probability, which we'll define as $$p=\\frac{\\Sigma_{a,thermal}\\phi}{\\Sigma_a\\phi}$$"
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"Now, let's analyze of few of the classic factors in the four-factor formula, starting with the resonance escape probability, which we'll define as $$p=\\frac{\\langle\\Sigma_a\\phi\\rangle_T}{\\langle\\Sigma_a\\phi\\rangle}$$ where the subscript $T$ means thermal energies."
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]
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},
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{
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@ -860,7 +861,7 @@
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"metadata": {},
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"source": [
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"The fast fission factor can be calculated as\n",
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"$$\\epsilon=\\frac{\\Sigma_f\\phi}{\\Sigma_{f,thermal}\\phi}$$"
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"$$\\epsilon=\\frac{\\langle\\Sigma_f\\phi\\rangle}{\\langle\\Sigma_f\\phi\\rangle_T}$$"
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]
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},
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{
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@ -927,8 +928,8 @@
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"metadata": {},
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"source": [
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"The thermal flux utilization is calculated as\n",
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"$$f=\\frac{\\Sigma_{a,thermal}^F\\phi}{\\Sigma_a\\phi}$$\n",
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"where $F$ denotes fuel."
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"$$f=\\frac{\\langle\\Sigma_a\\phi\\rangle^F_T}{\\langle\\Sigma_a\\phi\\rangle_T}$$\n",
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"where the superscript $F$ denotes fuel."
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]
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},
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{
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@ -946,6 +947,8 @@
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" <thead>\n",
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" <tr style=\"text-align: right;\">\n",
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" <th></th>\n",
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" <th>energy [MeV]</th>\n",
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" <th>cell</th>\n",
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" <th>nuclide</th>\n",
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" <th>score</th>\n",
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" <th>mean</th>\n",
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@ -957,24 +960,28 @@
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" <th></th>\n",
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" <th></th>\n",
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" <th></th>\n",
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" <th></th>\n",
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" <th></th>\n",
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" </tr>\n",
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" </thead>\n",
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" <tbody>\n",
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" <tr>\n",
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" <th>0</th>\n",
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" <td>0.0e+00 - 6.2e-01</td>\n",
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" <td>10000</td>\n",
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" <td>total</td>\n",
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" <td>absorption</td>\n",
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" <td>0.769263</td>\n",
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" <td>0.004172</td>\n",
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" <td>0.802094</td>\n",
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" <td>0.004432</td>\n",
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" </tr>\n",
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" </tbody>\n",
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"</table>\n",
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"</div>"
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],
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"text/plain": [
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" nuclide score mean std. dev.\n",
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"bin \n",
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"0 total absorption 0.769263 0.004172"
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" energy [MeV] cell nuclide score mean std. dev.\n",
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"bin \n",
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"0 0.0e+00 - 6.2e-01 10000 total absorption 0.802094 0.004432"
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]
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},
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"execution_count": 29,
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@ -985,7 +992,7 @@
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"source": [
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"# Compute thermal flux utilization factor using tally arithmetic\n",
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"fuel_therm_abs_rate = sp.get_tally(name='fuel therm. abs. rate')\n",
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"therm_util = fuel_therm_abs_rate / abs_rate\n",
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"therm_util = fuel_therm_abs_rate / therm_abs_rate\n",
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"therm_util.get_pandas_dataframe()"
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]
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},
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