pincell_msr_lump.ipynb

{
 "cells": [
  {
   "cell_type": "code",
   "execution_count": 2,
   "id": "8b2785df",
   "metadata": {},
   "outputs": [],
   "source": [
    "%matplotlib inline\n",
    "import os\n",
    "from math import pi\n",
    "import openmc\n",
    "import openmc.deplete\n",
    "import matplotlib.pyplot as plt\n",
    "import re\n",
    "from matplotlib.pyplot import Line2D"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 3,
   "id": "1288c79a",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/plain": [
       "0"
      ]
     },
     "execution_count": 3,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "os.system('rm *.h5 *.xml')"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "7ef97d0e-39ff-45cd-ae8b-bf10a84d8e72",
   "metadata": {},
   "source": [
    "We will add an arbitrary out-of-core fuel salt depletable material, with the same material definition and placed it outside of the core region (subjected to only decay). We will then set up transfer rates for the all fuel salt inventory from in-core to out-of core and vice versa as a function of their residence times. "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 4,
   "id": "45acfbc9",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Instantiate some Materials and register the appropriate Nuclides\n",
    "uf4 = openmc.Material(name='UF4')\n",
    "uf4.set_density('g/cm3', 4.5)\n",
    "uf4.add_element('U', 1., enrichment=2.4)\n",
    "uf4.add_element('F', 4.)\n",
    "\n",
    "helium = openmc.Material(name='Helium for gap')\n",
    "helium.set_density('g/cm3', 0.001598)\n",
    "helium.add_element('He', 2.4044e-4)\n",
    "\n",
    "zircaloy = openmc.Material(name='Zircaloy 4')\n",
    "zircaloy.set_density('g/cm3', 6.55)\n",
    "zircaloy.add_element('Sn', 0.014, 'wo')\n",
    "zircaloy.add_element('Fe', 0.00165, 'wo')\n",
    "zircaloy.add_element('Cr', 0.001, 'wo')\n",
    "zircaloy.add_element('Zr', 0.98335, 'wo')\n",
    "\n",
    "borated_water = openmc.Material(name='Borated water')\n",
    "borated_water.set_density('g/cm3', 0.740582)\n",
    "borated_water.add_element('B', 4.0e-5)\n",
    "borated_water.add_element('H', 5.0e-2)\n",
    "borated_water.add_element('O', 2.4e-2)\n",
    "borated_water.add_s_alpha_beta('c_H_in_H2O')\n",
    "\n",
    "ofc_uf4 = uf4.clone()\n",
    "ofc_uf4.name = 'UF4_ofc'\n",
    "# Define overall material\n",
    "material = openmc.Materials([uf4, helium, zircaloy, borated_water, ofc_uf4])"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 5,
   "id": "be80a9b7",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Define surfaces\n",
    "width = 1.25984\n",
    "height = 200\n",
    "ofc_r = 2\n",
    "fuel_or = openmc.ZCylinder(r=0.39218, name='Fuel OR')\n",
    "clad_ir = openmc.ZCylinder(r=0.40005, name='Clad IR')\n",
    "clad_or = openmc.ZCylinder(r=0.45720, name='Clad OR')\n",
    "wat_or = openmc.ZCylinder(r=width/2, name='H2O OR', boundary_type='reflective')\n",
    "interface = openmc.ZPlane(z0=-59, name='IF')\n",
    "z_top = openmc.ZPlane(z0=height/2, name='Pin TOP', boundary_type='vacuum')\n",
    "z_bot = openmc.ZPlane(z0=-height/2, name='Pin BOT', boundary_type='vacuum')\n",
    "ofc_surf = openmc.Sphere(x0 = 15, r = ofc_r, boundary_type = 'vacuum') \n",
    "\n",
    "# Define cells\n",
    "fuel = openmc.Cell(fill=uf4, region=-fuel_or & -z_top & +z_bot)\n",
    "gap = openmc.Cell(fill=helium, region=+fuel_or & -clad_ir & -z_top & +z_bot)\n",
    "clad = openmc.Cell(fill=zircaloy, region=+clad_ir & -clad_or & -z_top & +z_bot)\n",
    "water = openmc.Cell(fill=borated_water, region=+clad_or & -interface )\n",
    "gas = openmc.Cell(fill=helium, region=+clad_or & +interface)\n",
    "msr_uni = openmc.Universe(cells=(water, gas))\n",
    "msr = openmc.Cell(name=\"MSR\", fill=msr_uni, region=-wat_or & -z_top & +z_bot)\n",
    "ofc_fuel = openmc.Cell(fill=ofc_uf4, region=-ofc_surf)\n",
    "root = openmc.Universe(cells=[fuel, gap, clad, msr, ofc_fuel])\n",
    "# Define overall geometry\n",
    "geometry = openmc.Geometry(root)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 6,
   "id": "ffb4a60e",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Instantiate a Settings object, set all runtime parameters, and export to XML\n",
    "settings = openmc.Settings()\n",
    "settings.batches = 100\n",
    "settings.inactive = 10\n",
    "settings.particles = 1000\n",
    "\n",
    "# Create an initial uniform spatial source distribution over fissionable zones\n",
    "bounds = [-0.62992, -0.62992, -100, 0.62992, 0.62992, 100]\n",
    "uniform_dist = openmc.stats.Box(bounds[:3], bounds[3:], only_fissionable=True)\n",
    "settings.source = openmc.source.IndependentSource(space=uniform_dist)\n",
    "\n",
    "#Build the model\n",
    "model = openmc.Model(geometry=geometry, materials=material, settings=settings)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 7,
   "id": "be46b587",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/plain": [
       "<Axes: xlabel='x [cm]', ylabel='z [cm]'>"
      ]
     },
     "execution_count": 7,
     "metadata": {},
     "output_type": "execute_result"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 258.065x259.74 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "# Create plot\n",
    "colors = {uf4:'red', helium:'cyan', borated_water: 'blue', zircaloy: 'gray', ofc_uf4: 'red'}\n",
    "root.plot(width=(50, 50), origin=(0,0,0), pixels=(200, 200), basis='xz', color_by='material', colors=colors, legend=True)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 8,
   "id": "593dc3cc-6bb6-4eaf-becc-5567e624c4b1",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "                                %%%%%%%%%%%%%%%\n",
      "                           %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                        %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                      %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                    %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                   %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                    %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                     %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                 ###############      %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ##################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ###################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ####################     %%%%%%%%%%%%%%%%%%%%%%\n",
      "                #####################     %%%%%%%%%%%%%%%%%%%%%\n",
      "                ######################     %%%%%%%%%%%%%%%%%%%%\n",
      "                #######################     %%%%%%%%%%%%%%%%%%\n",
      "                 #######################     %%%%%%%%%%%%%%%%%\n",
      "                 ######################     %%%%%%%%%%%%%%%%%\n",
      "                  ####################     %%%%%%%%%%%%%%%%%\n",
      "                    #################     %%%%%%%%%%%%%%%%%\n",
      "                     ###############     %%%%%%%%%%%%%%%%\n",
      "                       ############     %%%%%%%%%%%%%%%\n",
      "                          ########     %%%%%%%%%%%%%%\n",
      "                                      %%%%%%%%%%%\n",
      "\n",
      "                 | The OpenMC Monte Carlo Code\n",
      "       Copyright | 2011-2024 MIT, UChicago Argonne LLC, and contributors\n",
      "         License | https://docs.openmc.org/en/latest/license.html\n",
      "         Version | 0.14.1-dev\n",
      "        Git SHA1 | d93ac83697e7fdb4fd4cc0f2705795398bf804bd\n",
      "       Date/Time | 2024-04-19 11:04:55\n",
      "   MPI Processes | 1\n",
      "  OpenMP Threads | 56\n",
      "\n",
      " Reading settings XML file...\n",
      " Reading cross sections XML file...\n",
      " Reading materials XML file...\n",
      " Reading geometry XML file...\n",
      " Reading U234 from /home/lorenzo/nuclear_data/endfb80_hdf5/U234.h5\n",
      " Reading U235 from /home/lorenzo/nuclear_data/endfb80_hdf5/U235.h5\n",
      " Reading U238 from /home/lorenzo/nuclear_data/endfb80_hdf5/U238.h5\n",
      " Reading F19 from /home/lorenzo/nuclear_data/endfb80_hdf5/F19.h5\n",
      " Reading U236 from /home/lorenzo/nuclear_data/endfb80_hdf5/U236.h5\n",
      " Reading He3 from /home/lorenzo/nuclear_data/endfb80_hdf5/He3.h5\n",
      " Reading He4 from /home/lorenzo/nuclear_data/endfb80_hdf5/He4.h5\n",
      " Reading Cr50 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr50.h5\n",
      " Reading Cr52 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr52.h5\n",
      " Reading Cr53 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr53.h5\n",
      " Reading Cr54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr54.h5\n",
      " Reading Fe54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe54.h5\n",
      " Reading Fe56 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe56.h5\n",
      " Reading Fe57 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe57.h5\n",
      " Reading Fe58 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe58.h5\n",
      " Reading Sn112 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn112.h5\n",
      " Reading Sn114 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn114.h5\n",
      " Reading Sn115 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn115.h5\n",
      " Reading Sn116 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn116.h5\n",
      " Reading Sn117 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn117.h5\n",
      " Reading Sn118 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn118.h5\n",
      " Reading Sn119 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn119.h5\n",
      " Reading Sn120 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn120.h5\n",
      " Reading Sn122 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn122.h5\n",
      " Reading Sn124 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn124.h5\n",
      " Reading Zr90 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr90.h5\n",
      " Reading Zr91 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr91.h5\n",
      " Reading Zr92 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr92.h5\n",
      " Reading Zr94 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr94.h5\n",
      " Reading Zr96 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr96.h5\n",
      " Reading B10 from /home/lorenzo/nuclear_data/endfb80_hdf5/B10.h5\n"
     ]
    },
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      " WARNING: Negative value(s) found on probability table for nuclide Zr96 at 294K\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      " Reading B11 from /home/lorenzo/nuclear_data/endfb80_hdf5/B11.h5\n",
      " Reading H1 from /home/lorenzo/nuclear_data/endfb80_hdf5/H1.h5\n",
      " Reading H2 from /home/lorenzo/nuclear_data/endfb80_hdf5/H2.h5\n",
      " Reading O16 from /home/lorenzo/nuclear_data/endfb80_hdf5/O16.h5\n",
      " Reading O17 from /home/lorenzo/nuclear_data/endfb80_hdf5/O17.h5\n",
      " Reading O18 from /home/lorenzo/nuclear_data/endfb80_hdf5/O18.h5\n",
      " Reading c_H_in_H2O from /home/lorenzo/nuclear_data/endfb80_hdf5/c_H_in_H2O.h5\n",
      " Minimum neutron data temperature: 294 K\n",
      " Maximum neutron data temperature: 294 K\n",
      " Preparing distributed cell instances...\n",
      " Reading plot XML file...\n",
      " Writing summary.h5 file...\n",
      "[openmc.deplete] t=0.0 s, dt=86400.0 s, source=100000.0\n",
      " Reading I135 from /home/lorenzo/nuclear_data/endfb80_hdf5/I135.h5\n",
      " Reading Xe135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe135.h5\n",
      " Reading Xe136 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe136.h5\n",
      " Reading Cs135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cs135.h5\n",
      " Reading Gd157 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd157.h5\n",
      " Reading Gd156 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd156.h5\n",
      " Reading Pu239 from /home/lorenzo/nuclear_data/endfb80_hdf5/Pu239.h5\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.55230\n",
      "        2/1    0.71581\n",
      "        3/1    0.84742\n",
      "        4/1    0.82083\n",
      "        5/1    0.88937\n",
      "        6/1    0.83661\n",
      "        7/1    0.90388\n",
      "        8/1    0.89892\n",
      "        9/1    0.84564\n",
      "       10/1    0.89387\n",
      "       11/1    0.81112\n",
      "       12/1    0.90903    0.86007 +/- 0.04896\n",
      "       13/1    0.82243    0.84752 +/- 0.03093\n",
      "       14/1    0.87888    0.85536 +/- 0.02323\n",
      "       15/1    0.85114    0.85452 +/- 0.01801\n",
      "       16/1    0.88721    0.85997 +/- 0.01569\n",
      "       17/1    0.88177    0.86308 +/- 0.01362\n",
      "       18/1    0.90888    0.86881 +/- 0.01311\n",
      "       19/1    0.83572    0.86513 +/- 0.01213\n",
      "       20/1    0.83936    0.86255 +/- 0.01115\n",
      "       21/1    0.94591    0.87013 +/- 0.01262\n",
      "       22/1    0.84293    0.86787 +/- 0.01174\n",
      "       23/1    0.88706    0.86934 +/- 0.01090\n",
      "       24/1    0.87462    0.86972 +/- 0.01010\n",
      "       25/1    0.77153    0.86317 +/- 0.01145\n",
      "       26/1    0.85637    0.86275 +/- 0.01072\n",
      "       27/1    0.80862    0.85956 +/- 0.01056\n",
      "       28/1    0.85113    0.85909 +/- 0.00997\n",
      "       29/1    0.83268    0.85770 +/- 0.00953\n",
      "       30/1    0.86520    0.85808 +/- 0.00905\n",
      "       31/1    0.93140    0.86157 +/- 0.00929\n",
      "       32/1    0.88934    0.86283 +/- 0.00895\n",
      "       33/1    0.87335    0.86329 +/- 0.00856\n",
      "       34/1    0.87573    0.86381 +/- 0.00821\n",
      "       35/1    0.91501    0.86586 +/- 0.00814\n",
      "       36/1    0.82385    0.86424 +/- 0.00799\n",
      "       37/1    0.82322    0.86272 +/- 0.00783\n",
      "       38/1    0.87062    0.86300 +/- 0.00755\n",
      "       39/1    0.86394    0.86304 +/- 0.00729\n",
      "       40/1    0.88725    0.86384 +/- 0.00709\n",
      "       41/1    0.88834    0.86463 +/- 0.00690\n",
      "       42/1    0.85313    0.86427 +/- 0.00669\n",
      "       43/1    0.93063    0.86629 +/- 0.00679\n",
      "       44/1    0.81729    0.86484 +/- 0.00674\n",
      "       45/1    0.79035    0.86272 +/- 0.00689\n",
      "       46/1    0.96206    0.86548 +/- 0.00724\n",
      "       47/1    0.88932    0.86612 +/- 0.00707\n",
      "       48/1    0.93670    0.86798 +/- 0.00713\n",
      "       49/1    0.88749    0.86848 +/- 0.00696\n",
      "       50/1    0.88210    0.86882 +/- 0.00679\n",
      "       51/1    0.83792    0.86806 +/- 0.00667\n",
      "       52/1    0.86035    0.86788 +/- 0.00651\n",
      "       53/1    0.83267    0.86706 +/- 0.00641\n",
      "       54/1    0.86629    0.86704 +/- 0.00626\n",
      "       55/1    0.83651    0.86637 +/- 0.00616\n",
      "       56/1    0.86899    0.86642 +/- 0.00602\n",
      "       57/1    0.86755    0.86645 +/- 0.00589\n",
      "       58/1    0.86296    0.86637 +/- 0.00577\n",
      "       59/1    0.90701    0.86720 +/- 0.00571\n",
      "       60/1    0.88598    0.86758 +/- 0.00561\n",
      "       61/1    0.83798    0.86700 +/- 0.00553\n",
      "       62/1    0.81695    0.86604 +/- 0.00551\n",
      "       63/1    0.90488    0.86677 +/- 0.00545\n",
      "       64/1    0.91599    0.86768 +/- 0.00543\n",
      "       65/1    0.85986    0.86754 +/- 0.00533\n",
      "       66/1    0.85999    0.86740 +/- 0.00523\n",
      "       67/1    0.88330    0.86768 +/- 0.00515\n",
      "       68/1    0.84368    0.86727 +/- 0.00508\n",
      "       69/1    0.86791    0.86728 +/- 0.00499\n",
      "       70/1    0.81372    0.86639 +/- 0.00499\n",
      "       71/1    0.87471    0.86652 +/- 0.00490\n",
      "       72/1    0.82349    0.86583 +/- 0.00487\n",
      "       73/1    0.92667    0.86679 +/- 0.00489\n",
      "       74/1    0.85169    0.86656 +/- 0.00482\n",
      "       75/1    0.83902    0.86614 +/- 0.00477\n",
      "       76/1    0.89600    0.86659 +/- 0.00471\n",
      "       77/1    0.86706    0.86659 +/- 0.00464\n",
      "       78/1    0.84111    0.86622 +/- 0.00459\n",
      "       79/1    0.80299    0.86530 +/- 0.00462\n",
      "       80/1    0.86359    0.86528 +/- 0.00455\n",
      "       81/1    0.80849    0.86448 +/- 0.00456\n",
      "       82/1    0.89804    0.86495 +/- 0.00452\n",
      "       83/1    0.86185    0.86490 +/- 0.00445\n",
      "       84/1    0.86501    0.86490 +/- 0.00439\n",
      "       85/1    0.84290    0.86461 +/- 0.00434\n",
      "       86/1    0.88679    0.86490 +/- 0.00430\n",
      "       87/1    0.92261    0.86565 +/- 0.00431\n",
      "       88/1    0.82757    0.86516 +/- 0.00428\n",
      "       89/1    0.87889    0.86534 +/- 0.00423\n",
      "       90/1    0.88855    0.86563 +/- 0.00418\n",
      "       91/1    0.85702    0.86552 +/- 0.00413\n",
      "       92/1    0.86806    0.86555 +/- 0.00408\n",
      "       93/1    0.88195    0.86575 +/- 0.00404\n",
      "       94/1    0.86865    0.86578 +/- 0.00399\n",
      "       95/1    0.89434    0.86612 +/- 0.00396\n",
      "       96/1    0.93531    0.86693 +/- 0.00399\n",
      "       97/1    0.91389    0.86747 +/- 0.00398\n",
      "       98/1    0.88900    0.86771 +/- 0.00395\n",
      "       99/1    0.86813    0.86771 +/- 0.00390\n",
      "      100/1    0.84827    0.86750 +/- 0.00386\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 3.0964e+00 seconds\n",
      "   Reading cross sections          = 3.0686e+00 seconds\n",
      " Total time in simulation          = 4.8926e+00 seconds\n",
      "   Time in transport only          = 4.7749e+00 seconds\n",
      "   Time in inactive batches        = 2.8074e-01 seconds\n",
      "   Time in active batches          = 4.6119e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1599e-02 seconds\n",
      "     Sampling source sites         = 9.5783e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5724e-03 seconds\n",
      "   Time accumulating tallies       = 8.6179e-02 seconds\n",
      "   Time writing statepoints        = 1.0635e-02 seconds\n",
      " Total time for finalization       = 1.6699e-04 seconds\n",
      " Total time elapsed                = 8.0204e+00 seconds\n",
      " Calculation Rate (inactive)       = 35619.6 particles/second\n",
      " Calculation Rate (active)         = 19514.9 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.87058 +/- 0.00340\n",
      " k-effective (Track-length)  = 0.86750 +/- 0.00386\n",
      " k-effective (Absorption)    = 0.88032 +/- 0.00359\n",
      " Combined k-effective        = 0.87426 +/- 0.00317\n",
      " Leakage Fraction            = 0.13803 +/- 0.00134\n",
      "\n",
      " Creating state point openmc_simulation_n0.h5...\n",
      "[openmc.deplete] t=86400.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.50806\n",
      "        2/1    0.63230\n",
      "        3/1    0.69701\n",
      "        4/1    0.81079\n",
      "        5/1    0.93274\n",
      "        6/1    0.83321\n",
      "        7/1    0.96314\n",
      "        8/1    0.94912\n",
      "        9/1    0.90540\n",
      "       10/1    0.86956\n",
      "       11/1    0.83414\n",
      "       12/1    0.84054    0.83734 +/- 0.00320\n",
      "       13/1    0.87119    0.84862 +/- 0.01143\n",
      "       14/1    0.89834    0.86105 +/- 0.01483\n",
      "       15/1    0.81754    0.85235 +/- 0.01441\n",
      "       16/1    0.86838    0.85502 +/- 0.01207\n",
      "       17/1    0.87626    0.85806 +/- 0.01064\n",
      "       18/1    0.81934    0.85322 +/- 0.01041\n",
      "       19/1    0.88481    0.85673 +/- 0.00983\n",
      "       20/1    0.86465    0.85752 +/- 0.00883\n",
      "       21/1    0.93744    0.86478 +/- 0.01079\n",
      "       22/1    0.86246    0.86459 +/- 0.00986\n",
      "       23/1    0.83949    0.86266 +/- 0.00927\n",
      "       24/1    0.93370    0.86773 +/- 0.00997\n",
      "       25/1    0.87229    0.86804 +/- 0.00929\n",
      "       26/1    0.81609    0.86479 +/- 0.00927\n",
      "       27/1    0.85221    0.86405 +/- 0.00874\n",
      "       28/1    0.86951    0.86435 +/- 0.00825\n",
      "       29/1    0.87150    0.86473 +/- 0.00781\n",
      "       30/1    0.88973    0.86598 +/- 0.00751\n",
      "       31/1    0.84004    0.86474 +/- 0.00725\n",
      "       32/1    0.84717    0.86395 +/- 0.00696\n",
      "       33/1    0.90349    0.86567 +/- 0.00687\n",
      "       34/1    0.85706    0.86531 +/- 0.00659\n",
      "       35/1    0.87759    0.86580 +/- 0.00634\n",
      "       36/1    0.87653    0.86621 +/- 0.00610\n",
      "       37/1    0.85567    0.86582 +/- 0.00589\n",
      "       38/1    0.87052    0.86599 +/- 0.00567\n",
      "       39/1    0.88793    0.86674 +/- 0.00553\n",
      "       40/1    0.85401    0.86632 +/- 0.00536\n",
      "       41/1    0.84051    0.86549 +/- 0.00525\n",
      "       42/1    0.79537    0.86330 +/- 0.00553\n",
      "       43/1    0.85048    0.86291 +/- 0.00538\n",
      "       44/1    0.84347    0.86234 +/- 0.00525\n",
      "       45/1    0.90915    0.86367 +/- 0.00527\n",
      "       46/1    0.82163    0.86251 +/- 0.00525\n",
      "       47/1    0.91525    0.86393 +/- 0.00530\n",
      "       48/1    0.81870    0.86274 +/- 0.00530\n",
      "       49/1    0.85609    0.86257 +/- 0.00516\n",
      "       50/1    0.90621    0.86366 +/- 0.00515\n",
      "       51/1    0.85370    0.86342 +/- 0.00503\n",
      "       52/1    0.84083    0.86288 +/- 0.00494\n",
      "       53/1    0.89194    0.86356 +/- 0.00487\n",
      "       54/1    0.85535    0.86337 +/- 0.00476\n",
      "       55/1    0.84042    0.86286 +/- 0.00468\n",
      "       56/1    0.84515    0.86248 +/- 0.00459\n",
      "       57/1    0.86674    0.86257 +/- 0.00449\n",
      "       58/1    0.85369    0.86238 +/- 0.00440\n",
      "       59/1    0.88565    0.86286 +/- 0.00434\n",
      "       60/1    0.82471    0.86209 +/- 0.00432\n",
      "       61/1    0.89567    0.86275 +/- 0.00428\n",
      "       62/1    0.88301    0.86314 +/- 0.00422\n",
      "       63/1    0.80540    0.86205 +/- 0.00428\n",
      "       64/1    0.86508    0.86211 +/- 0.00420\n",
      "       65/1    0.91138    0.86300 +/- 0.00422\n",
      "       66/1    0.84687    0.86272 +/- 0.00415\n",
      "       67/1    0.84292    0.86237 +/- 0.00409\n",
      "       68/1    0.84375    0.86205 +/- 0.00404\n",
      "       69/1    0.83812    0.86164 +/- 0.00399\n",
      "       70/1    0.84045    0.86129 +/- 0.00394\n",
      "       71/1    0.88418    0.86166 +/- 0.00389\n",
      "       72/1    0.84079    0.86133 +/- 0.00384\n",
      "       73/1    0.91448    0.86217 +/- 0.00387\n",
      "       74/1    0.83281    0.86171 +/- 0.00384\n",
      "       75/1    0.90642    0.86240 +/- 0.00384\n",
      "       76/1    0.85093    0.86223 +/- 0.00379\n",
      "       77/1    0.82462    0.86166 +/- 0.00377\n",
      "       78/1    0.91095    0.86239 +/- 0.00379\n",
      "       79/1    0.88209    0.86268 +/- 0.00374\n",
      "       80/1    0.81184    0.86195 +/- 0.00376\n",
      "       81/1    0.86221    0.86195 +/- 0.00371\n",
      "       82/1    0.92138    0.86278 +/- 0.00375\n",
      "       83/1    0.80252    0.86195 +/- 0.00379\n",
      "       84/1    0.85711    0.86189 +/- 0.00373\n",
      "       85/1    0.90975    0.86253 +/- 0.00374\n",
      "       86/1    0.90208    0.86305 +/- 0.00373\n",
      "       87/1    0.90329    0.86357 +/- 0.00371\n",
      "       88/1    0.85103    0.86341 +/- 0.00367\n",
      "       89/1    0.82958    0.86298 +/- 0.00365\n",
      "       90/1    0.90505    0.86351 +/- 0.00364\n",
      "       91/1    0.89412    0.86388 +/- 0.00362\n",
      "       92/1    0.85387    0.86376 +/- 0.00357\n",
      "       93/1    0.88736    0.86405 +/- 0.00354\n",
      "       94/1    0.81615    0.86348 +/- 0.00354\n",
      "       95/1    0.86475    0.86349 +/- 0.00350\n",
      "       96/1    0.85069    0.86334 +/- 0.00347\n",
      "       97/1    0.89034    0.86365 +/- 0.00344\n",
      "       98/1    0.84930    0.86349 +/- 0.00340\n",
      "       99/1    0.86752    0.86353 +/- 0.00337\n",
      "      100/1    0.81820    0.86303 +/- 0.00337\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.4555e+00 seconds\n",
      "   Time in transport only          = 4.3161e+00 seconds\n",
      "   Time in inactive batches        = 2.3580e-01 seconds\n",
      "   Time in active batches          = 4.2197e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0428e-02 seconds\n",
      "     Sampling source sites         = 8.5939e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5196e-03 seconds\n",
      "   Time accumulating tallies       = 1.1218e-01 seconds\n",
      "   Time writing statepoints        = 7.9787e-03 seconds\n",
      " Total time for finalization       = 1.0782e-04 seconds\n",
      " Total time elapsed                = 4.4948e+00 seconds\n",
      " Calculation Rate (inactive)       = 42408.1 particles/second\n",
      " Calculation Rate (active)         = 21328.3 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86066 +/- 0.00291\n",
      " k-effective (Track-length)  = 0.86303 +/- 0.00337\n",
      " k-effective (Absorption)    = 0.85843 +/- 0.00310\n",
      " Combined k-effective        = 0.86017 +/- 0.00232\n",
      " Leakage Fraction            = 0.14009 +/- 0.00129\n",
      "\n",
      " Creating state point openmc_simulation_n1.h5...\n",
      "[openmc.deplete] t=172800.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.50000\n",
      "        2/1    0.67230\n",
      "        3/1    0.81333\n",
      "        4/1    0.83116\n",
      "        5/1    0.84603\n",
      "        6/1    0.82412\n",
      "        7/1    0.83696\n",
      "        8/1    0.80864\n",
      "        9/1    0.83710\n",
      "       10/1    0.81911\n",
      "       11/1    0.84603\n",
      "       12/1    0.80245    0.82424 +/- 0.02179\n",
      "       13/1    0.85435    0.83428 +/- 0.01609\n",
      "       14/1    0.87757    0.84510 +/- 0.01570\n",
      "       15/1    0.81854    0.83979 +/- 0.01327\n",
      "       16/1    0.88028    0.84654 +/- 0.01277\n",
      "       17/1    0.83755    0.84525 +/- 0.01087\n",
      "       18/1    0.85025    0.84588 +/- 0.00943\n",
      "       19/1    0.82337    0.84338 +/- 0.00869\n",
      "       20/1    0.85897    0.84494 +/- 0.00792\n",
      "       21/1    0.81365    0.84209 +/- 0.00771\n",
      "       22/1    0.90952    0.84771 +/- 0.00901\n",
      "       23/1    0.86675    0.84918 +/- 0.00841\n",
      "       24/1    0.84361    0.84878 +/- 0.00780\n",
      "       25/1    0.83803    0.84806 +/- 0.00730\n",
      "       26/1    0.88247    0.85021 +/- 0.00716\n",
      "       27/1    0.85534    0.85051 +/- 0.00673\n",
      "       28/1    0.83554    0.84968 +/- 0.00640\n",
      "       29/1    0.87693    0.85112 +/- 0.00622\n",
      "       30/1    0.90068    0.85359 +/- 0.00640\n",
      "       31/1    0.90216    0.85591 +/- 0.00651\n",
      "       32/1    0.84618    0.85546 +/- 0.00622\n",
      "       33/1    0.93315    0.85884 +/- 0.00684\n",
      "       34/1    0.84767    0.85838 +/- 0.00657\n",
      "       35/1    0.80403    0.85620 +/- 0.00666\n",
      "       36/1    0.85647    0.85621 +/- 0.00640\n",
      "       37/1    0.86092    0.85639 +/- 0.00616\n",
      "       38/1    0.87483    0.85705 +/- 0.00597\n",
      "       39/1    0.85094    0.85684 +/- 0.00577\n",
      "       40/1    0.84368    0.85640 +/- 0.00559\n",
      "       41/1    0.83534    0.85572 +/- 0.00545\n",
      "       42/1    0.89596    0.85698 +/- 0.00542\n",
      "       43/1    0.80237    0.85532 +/- 0.00551\n",
      "       44/1    0.84478    0.85501 +/- 0.00536\n",
      "       45/1    0.88263    0.85580 +/- 0.00526\n",
      "       46/1    0.84709    0.85556 +/- 0.00512\n",
      "       47/1    0.86463    0.85580 +/- 0.00498\n",
      "       48/1    0.88020    0.85645 +/- 0.00489\n",
      "       49/1    0.82771    0.85571 +/- 0.00482\n",
      "       50/1    0.91407    0.85717 +/- 0.00492\n",
      "       51/1    0.91321    0.85853 +/- 0.00499\n",
      "       52/1    0.85098    0.85835 +/- 0.00487\n",
      "       53/1    0.85909    0.85837 +/- 0.00476\n",
      "       54/1    0.85456    0.85828 +/- 0.00465\n",
      "       55/1    0.86662    0.85847 +/- 0.00455\n",
      "       56/1    0.79767    0.85715 +/- 0.00464\n",
      "       57/1    0.81819    0.85632 +/- 0.00462\n",
      "       58/1    0.86482    0.85650 +/- 0.00452\n",
      "       59/1    0.85365    0.85644 +/- 0.00443\n",
      "       60/1    0.83314    0.85597 +/- 0.00437\n",
      "       61/1    0.87004    0.85625 +/- 0.00429\n",
      "       62/1    0.83331    0.85581 +/- 0.00423\n",
      "       63/1    0.81086    0.85496 +/- 0.00423\n",
      "       64/1    0.81488    0.85422 +/- 0.00422\n",
      "       65/1    0.78454    0.85295 +/- 0.00433\n",
      "       66/1    0.87513    0.85335 +/- 0.00427\n",
      "       67/1    0.87472    0.85372 +/- 0.00421\n",
      "       68/1    0.94228    0.85525 +/- 0.00441\n",
      "       69/1    0.85672    0.85527 +/- 0.00434\n",
      "       70/1    0.88222    0.85572 +/- 0.00429\n",
      "       71/1    0.92574    0.85687 +/- 0.00437\n",
      "       72/1    0.88145    0.85727 +/- 0.00432\n",
      "       73/1    0.88807    0.85776 +/- 0.00428\n",
      "       74/1    0.87056    0.85796 +/- 0.00421\n",
      "       75/1    0.85633    0.85793 +/- 0.00415\n",
      "       76/1    0.86664    0.85806 +/- 0.00409\n",
      "       77/1    0.84047    0.85780 +/- 0.00403\n",
      "       78/1    0.86840    0.85796 +/- 0.00398\n",
      "       79/1    0.85615    0.85793 +/- 0.00392\n",
      "       80/1    0.94059    0.85911 +/- 0.00404\n",
      "       81/1    0.88728    0.85951 +/- 0.00400\n",
      "       82/1    0.89945    0.86006 +/- 0.00398\n",
      "       83/1    0.84839    0.85990 +/- 0.00393\n",
      "       84/1    0.82529    0.85943 +/- 0.00391\n",
      "       85/1    0.77704    0.85834 +/- 0.00401\n",
      "       86/1    0.84615    0.85818 +/- 0.00396\n",
      "       87/1    0.82754    0.85778 +/- 0.00393\n",
      "       88/1    0.81986    0.85729 +/- 0.00391\n",
      "       89/1    0.81074    0.85670 +/- 0.00390\n",
      "       90/1    0.86281    0.85678 +/- 0.00385\n",
      "       91/1    0.83878    0.85656 +/- 0.00381\n",
      "       92/1    0.83633    0.85631 +/- 0.00377\n",
      "       93/1    0.87747    0.85656 +/- 0.00374\n",
      "       94/1    0.89484    0.85702 +/- 0.00372\n",
      "       95/1    0.81405    0.85651 +/- 0.00371\n",
      "       96/1    0.83776    0.85630 +/- 0.00367\n",
      "       97/1    0.82578    0.85595 +/- 0.00365\n",
      "       98/1    0.85177    0.85590 +/- 0.00361\n",
      "       99/1    0.83453    0.85566 +/- 0.00357\n",
      "      100/1    0.87937    0.85592 +/- 0.00354\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.6897e+00 seconds\n",
      "   Time in transport only          = 4.5179e+00 seconds\n",
      "   Time in inactive batches        = 2.3804e-01 seconds\n",
      "   Time in active batches          = 4.4517e+00 seconds\n",
      "   Time synchronizing fission bank = 1.2729e-02 seconds\n",
      "     Sampling source sites         = 1.0750e-02 seconds\n",
      "     SEND/RECV source sites        = 1.6005e-03 seconds\n",
      "   Time accumulating tallies       = 1.4251e-01 seconds\n",
      "   Time writing statepoints        = 7.7849e-03 seconds\n",
      " Total time for finalization       = 1.2343e-04 seconds\n",
      " Total time elapsed                = 4.7172e+00 seconds\n",
      " Calculation Rate (inactive)       = 42010.2 particles/second\n",
      " Calculation Rate (active)         = 20217.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.85655 +/- 0.00336\n",
      " k-effective (Track-length)  = 0.85592 +/- 0.00354\n",
      " k-effective (Absorption)    = 0.85151 +/- 0.00322\n",
      " Combined k-effective        = 0.85380 +/- 0.00265\n",
      " Leakage Fraction            = 0.13749 +/- 0.00126\n",
      "\n",
      " Creating state point openmc_simulation_n2.h5...\n",
      "[openmc.deplete] t=259200.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.54130\n",
      "        2/1    0.66035\n",
      "        3/1    0.76647\n",
      "        4/1    0.79829\n",
      "        5/1    0.76705\n",
      "        6/1    0.85986\n",
      "        7/1    0.88836\n",
      "        8/1    0.82032\n",
      "        9/1    0.83914\n",
      "       10/1    0.87351\n",
      "       11/1    0.86227\n",
      "       12/1    0.81926    0.84076 +/- 0.02150\n",
      "       13/1    0.89544    0.85899 +/- 0.02205\n",
      "       14/1    0.83257    0.85238 +/- 0.01693\n",
      "       15/1    0.85179    0.85226 +/- 0.01312\n",
      "       16/1    0.84263    0.85066 +/- 0.01083\n",
      "       17/1    0.84511    0.84987 +/- 0.00919\n",
      "       18/1    0.86623    0.85191 +/- 0.00821\n",
      "       19/1    0.89437    0.85663 +/- 0.00865\n",
      "       20/1    0.84886    0.85585 +/- 0.00777\n",
      "       21/1    0.84751    0.85509 +/- 0.00707\n",
      "       22/1    0.84215    0.85402 +/- 0.00654\n",
      "       23/1    0.77052    0.84759 +/- 0.00880\n",
      "       24/1    0.81061    0.84495 +/- 0.00857\n",
      "       25/1    0.85196    0.84542 +/- 0.00799\n",
      "       26/1    0.80174    0.84269 +/- 0.00796\n",
      "       27/1    0.81759    0.84121 +/- 0.00762\n",
      "       28/1    0.77620    0.83760 +/- 0.00804\n",
      "       29/1    0.76962    0.83402 +/- 0.00840\n",
      "       30/1    0.83751    0.83420 +/- 0.00797\n",
      "       31/1    0.87531    0.83616 +/- 0.00783\n",
      "       32/1    0.85077    0.83682 +/- 0.00750\n",
      "       33/1    0.85454    0.83759 +/- 0.00721\n",
      "       34/1    0.83081    0.83731 +/- 0.00691\n",
      "       35/1    0.75585    0.83405 +/- 0.00738\n",
      "       36/1    0.79627    0.83260 +/- 0.00724\n",
      "       37/1    0.85321    0.83336 +/- 0.00701\n",
      "       38/1    0.84271    0.83369 +/- 0.00676\n",
      "       39/1    0.89962    0.83597 +/- 0.00691\n",
      "       40/1    0.85102    0.83647 +/- 0.00669\n",
      "       41/1    0.82764    0.83618 +/- 0.00648\n",
      "       42/1    0.79437    0.83488 +/- 0.00641\n",
      "       43/1    0.82101    0.83446 +/- 0.00623\n",
      "       44/1    0.78847    0.83310 +/- 0.00619\n",
      "       45/1    0.80732    0.83237 +/- 0.00606\n",
      "       46/1    0.92040    0.83481 +/- 0.00637\n",
      "       47/1    0.94463    0.83778 +/- 0.00687\n",
      "       48/1    0.87188    0.83868 +/- 0.00675\n",
      "       49/1    0.77338    0.83700 +/- 0.00678\n",
      "       50/1    0.88589    0.83823 +/- 0.00672\n",
      "       51/1    0.88402    0.83934 +/- 0.00665\n",
      "       52/1    0.86889    0.84005 +/- 0.00653\n",
      "       53/1    0.82525    0.83970 +/- 0.00639\n",
      "       54/1    0.80894    0.83900 +/- 0.00628\n",
      "       55/1    0.90824    0.84054 +/- 0.00633\n",
      "       56/1    0.81618    0.84001 +/- 0.00621\n",
      "       57/1    0.87081    0.84067 +/- 0.00611\n",
      "       58/1    0.83088    0.84046 +/- 0.00599\n",
      "       59/1    0.82700    0.84019 +/- 0.00587\n",
      "       60/1    0.82539    0.83989 +/- 0.00576\n",
      "       61/1    0.76931    0.83851 +/- 0.00581\n",
      "       62/1    0.83740    0.83849 +/- 0.00570\n",
      "       63/1    0.88043    0.83928 +/- 0.00565\n",
      "       64/1    0.81456    0.83882 +/- 0.00556\n",
      "       65/1    0.87476    0.83947 +/- 0.00550\n",
      "       66/1    0.81062    0.83896 +/- 0.00542\n",
      "       67/1    0.83168    0.83883 +/- 0.00533\n",
      "       68/1    0.81481    0.83842 +/- 0.00525\n",
      "       69/1    0.81990    0.83810 +/- 0.00517\n",
      "       70/1    0.87470    0.83871 +/- 0.00512\n",
      "       71/1    0.88217    0.83943 +/- 0.00509\n",
      "       72/1    0.80549    0.83888 +/- 0.00503\n",
      "       73/1    0.86301    0.83926 +/- 0.00497\n",
      "       74/1    0.84245    0.83931 +/- 0.00489\n",
      "       75/1    0.84839    0.83945 +/- 0.00482\n",
      "       76/1    0.87148    0.83994 +/- 0.00477\n",
      "       77/1    0.89088    0.84070 +/- 0.00476\n",
      "       78/1    0.87206    0.84116 +/- 0.00471\n",
      "       79/1    0.89681    0.84196 +/- 0.00471\n",
      "       80/1    0.90906    0.84292 +/- 0.00474\n",
      "       81/1    0.84364    0.84293 +/- 0.00467\n",
      "       82/1    0.85661    0.84312 +/- 0.00461\n",
      "       83/1    0.87273    0.84353 +/- 0.00457\n",
      "       84/1    0.85307    0.84366 +/- 0.00450\n",
      "       85/1    0.82156    0.84336 +/- 0.00445\n",
      "       86/1    0.88670    0.84393 +/- 0.00443\n",
      "       87/1    0.87845    0.84438 +/- 0.00440\n",
      "       88/1    0.87640    0.84479 +/- 0.00436\n",
      "       89/1    0.87065    0.84512 +/- 0.00432\n",
      "       90/1    0.86786    0.84540 +/- 0.00427\n",
      "       91/1    0.82899    0.84520 +/- 0.00422\n",
      "       92/1    0.83230    0.84504 +/- 0.00417\n",
      "       93/1    0.83377    0.84491 +/- 0.00413\n",
      "       94/1    0.82312    0.84465 +/- 0.00409\n",
      "       95/1    0.82520    0.84442 +/- 0.00404\n",
      "       96/1    0.84067    0.84438 +/- 0.00400\n",
      "       97/1    0.80022    0.84387 +/- 0.00398\n",
      "       98/1    0.80180    0.84339 +/- 0.00397\n",
      "       99/1    0.83965    0.84335 +/- 0.00392\n",
      "      100/1    0.85139    0.84344 +/- 0.00388\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.3218e+00 seconds\n",
      "   Time in transport only          = 4.2232e+00 seconds\n",
      "   Time in inactive batches        = 2.2755e-01 seconds\n",
      "   Time in active batches          = 4.0942e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1261e-02 seconds\n",
      "     Sampling source sites         = 9.3505e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5386e-03 seconds\n",
      "   Time accumulating tallies       = 5.9929e-02 seconds\n",
      "   Time writing statepoints        = 1.5572e-02 seconds\n",
      " Total time for finalization       = 9.5532e-05 seconds\n",
      " Total time elapsed                = 4.3580e+00 seconds\n",
      " Calculation Rate (inactive)       = 43946.5 particles/second\n",
      " Calculation Rate (active)         = 21982.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.84265 +/- 0.00372\n",
      " k-effective (Track-length)  = 0.84344 +/- 0.00388\n",
      " k-effective (Absorption)    = 0.84636 +/- 0.00350\n",
      " Combined k-effective        = 0.84478 +/- 0.00298\n",
      " Leakage Fraction            = 0.13916 +/- 0.00128\n",
      "\n",
      " Creating state point openmc_simulation_n3.h5...\n",
      "[openmc.deplete] t=345600.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.50261\n",
      "        2/1    0.61659\n",
      "        3/1    0.72235\n",
      "        4/1    0.77766\n",
      "        5/1    0.91135\n",
      "        6/1    0.93872\n",
      "        7/1    0.84129\n",
      "        8/1    0.84685\n",
      "        9/1    0.80666\n",
      "       10/1    0.83596\n",
      "       11/1    0.83565\n",
      "       12/1    0.82372    0.82969 +/- 0.00596\n",
      "       13/1    0.83200    0.83046 +/- 0.00353\n",
      "       14/1    0.85312    0.83612 +/- 0.00619\n",
      "       15/1    0.85066    0.83903 +/- 0.00561\n",
      "       16/1    0.87342    0.84476 +/- 0.00734\n",
      "       17/1    0.85084    0.84563 +/- 0.00626\n",
      "       18/1    0.90004    0.85243 +/- 0.00870\n",
      "       19/1    0.88826    0.85641 +/- 0.00864\n",
      "       20/1    0.87981    0.85875 +/- 0.00808\n",
      "       21/1    0.79475    0.85293 +/- 0.00934\n",
      "       22/1    0.89647    0.85656 +/- 0.00927\n",
      "       23/1    0.92573    0.86188 +/- 0.01005\n",
      "       24/1    0.81436    0.85849 +/- 0.00990\n",
      "       25/1    0.88384    0.86018 +/- 0.00937\n",
      "       26/1    0.87421    0.86106 +/- 0.00881\n",
      "       27/1    0.83482    0.85951 +/- 0.00842\n",
      "       28/1    0.85641    0.85934 +/- 0.00794\n",
      "       29/1    0.84567    0.85862 +/- 0.00754\n",
      "       30/1    0.83054    0.85722 +/- 0.00729\n",
      "       31/1    0.77667    0.85338 +/- 0.00793\n",
      "       32/1    0.79095    0.85054 +/- 0.00807\n",
      "       33/1    0.85388    0.85069 +/- 0.00772\n",
      "       34/1    0.76830    0.84726 +/- 0.00815\n",
      "       35/1    0.90062    0.84939 +/- 0.00810\n",
      "       36/1    0.83854    0.84897 +/- 0.00779\n",
      "       37/1    0.79932    0.84713 +/- 0.00772\n",
      "       38/1    0.89427    0.84882 +/- 0.00763\n",
      "       39/1    0.86154    0.84926 +/- 0.00737\n",
      "       40/1    0.83169    0.84867 +/- 0.00715\n",
      "       41/1    0.89164    0.85006 +/- 0.00705\n",
      "       42/1    0.76101    0.84727 +/- 0.00737\n",
      "       43/1    0.85170    0.84741 +/- 0.00715\n",
      "       44/1    0.81197    0.84637 +/- 0.00701\n",
      "       45/1    0.86757    0.84697 +/- 0.00683\n",
      "       46/1    0.83530    0.84665 +/- 0.00665\n",
      "       47/1    0.81302    0.84574 +/- 0.00653\n",
      "       48/1    0.86183    0.84616 +/- 0.00637\n",
      "       49/1    0.85379    0.84636 +/- 0.00621\n",
      "       50/1    0.88525    0.84733 +/- 0.00613\n",
      "       51/1    0.83303    0.84698 +/- 0.00599\n",
      "       52/1    0.84287    0.84688 +/- 0.00584\n",
      "       53/1    0.87128    0.84745 +/- 0.00574\n",
      "       54/1    0.83449    0.84716 +/- 0.00561\n",
      "       55/1    0.85744    0.84738 +/- 0.00549\n",
      "       56/1    0.82461    0.84689 +/- 0.00539\n",
      "       57/1    0.77780    0.84542 +/- 0.00548\n",
      "       58/1    0.83466    0.84520 +/- 0.00537\n",
      "       59/1    0.78127    0.84389 +/- 0.00542\n",
      "       60/1    0.82930    0.84360 +/- 0.00531\n",
      "       61/1    0.89685    0.84464 +/- 0.00531\n",
      "       62/1    0.84507    0.84465 +/- 0.00521\n",
      "       63/1    0.87691    0.84526 +/- 0.00515\n",
      "       64/1    0.82472    0.84488 +/- 0.00506\n",
      "       65/1    0.82232    0.84447 +/- 0.00499\n",
      "       66/1    0.77823    0.84329 +/- 0.00504\n",
      "       67/1    0.81383    0.84277 +/- 0.00498\n",
      "       68/1    0.83421    0.84262 +/- 0.00489\n",
      "       69/1    0.82436    0.84231 +/- 0.00482\n",
      "       70/1    0.76926    0.84110 +/- 0.00489\n",
      "       71/1    0.84534    0.84116 +/- 0.00481\n",
      "       72/1    0.84237    0.84118 +/- 0.00473\n",
      "       73/1    0.83247    0.84105 +/- 0.00466\n",
      "       74/1    0.82591    0.84081 +/- 0.00459\n",
      "       75/1    0.83628    0.84074 +/- 0.00452\n",
      "       76/1    0.86479    0.84110 +/- 0.00447\n",
      "       77/1    0.83425    0.84100 +/- 0.00440\n",
      "       78/1    0.86166    0.84131 +/- 0.00435\n",
      "       79/1    0.91052    0.84231 +/- 0.00440\n",
      "       80/1    0.88278    0.84289 +/- 0.00437\n",
      "       81/1    0.87737    0.84337 +/- 0.00434\n",
      "       82/1    0.87931    0.84387 +/- 0.00431\n",
      "       83/1    0.86316    0.84414 +/- 0.00426\n",
      "       84/1    0.86378    0.84440 +/- 0.00421\n",
      "       85/1    0.81236    0.84397 +/- 0.00417\n",
      "       86/1    0.80173    0.84342 +/- 0.00415\n",
      "       87/1    0.81297    0.84302 +/- 0.00412\n",
      "       88/1    0.78318    0.84226 +/- 0.00414\n",
      "       89/1    0.84755    0.84232 +/- 0.00409\n",
      "       90/1    0.82448    0.84210 +/- 0.00404\n",
      "       91/1    0.85224    0.84223 +/- 0.00399\n",
      "       92/1    0.87695    0.84265 +/- 0.00397\n",
      "       93/1    0.81997    0.84238 +/- 0.00393\n",
      "       94/1    0.85612    0.84254 +/- 0.00388\n",
      "       95/1    0.90163    0.84323 +/- 0.00390\n",
      "       96/1    0.74285    0.84207 +/- 0.00403\n",
      "       97/1    0.84231    0.84207 +/- 0.00398\n",
      "       98/1    0.86028    0.84228 +/- 0.00394\n",
      "       99/1    0.82389    0.84207 +/- 0.00390\n",
      "      100/1    0.91500    0.84288 +/- 0.00394\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.6959e+00 seconds\n",
      "   Time in transport only          = 4.5486e+00 seconds\n",
      "   Time in inactive batches        = 2.7006e-01 seconds\n",
      "   Time in active batches          = 4.4259e+00 seconds\n",
      "   Time synchronizing fission bank = 1.3228e-02 seconds\n",
      "     Sampling source sites         = 1.1218e-02 seconds\n",
      "     SEND/RECV source sites        = 1.5879e-03 seconds\n",
      "   Time accumulating tallies       = 1.1360e-01 seconds\n",
      "   Time writing statepoints        = 9.5347e-03 seconds\n",
      " Total time for finalization       = 1.1356e-04 seconds\n",
      " Total time elapsed                = 4.7313e+00 seconds\n",
      " Calculation Rate (inactive)       = 37028.3 particles/second\n",
      " Calculation Rate (active)         = 20335.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.84756 +/- 0.00340\n",
      " k-effective (Track-length)  = 0.84288 +/- 0.00394\n",
      " k-effective (Absorption)    = 0.85177 +/- 0.00364\n",
      " Combined k-effective        = 0.84870 +/- 0.00300\n",
      " Leakage Fraction            = 0.13883 +/- 0.00114\n",
      "\n",
      " Creating state point openmc_simulation_n4.h5...\n",
      "[openmc.deplete] t=432000.0 (final operator evaluation)\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.52464\n",
      "        2/1    0.66396\n",
      "        3/1    0.75997\n",
      "        4/1    0.81762\n",
      "        5/1    0.79080\n",
      "        6/1    0.79719\n",
      "        7/1    0.84058\n",
      "        8/1    0.89457\n",
      "        9/1    0.87602\n",
      "       10/1    0.79190\n",
      "       11/1    0.89044\n",
      "       12/1    0.75483    0.82263 +/- 0.06780\n",
      "       13/1    0.83265    0.82597 +/- 0.03929\n",
      "       14/1    0.88418    0.84052 +/- 0.03136\n",
      "       15/1    0.86479    0.84538 +/- 0.02477\n",
      "       16/1    0.81151    0.83973 +/- 0.02100\n",
      "       17/1    0.82557    0.83771 +/- 0.01786\n",
      "       18/1    0.84485    0.83860 +/- 0.01550\n",
      "       19/1    0.81138    0.83558 +/- 0.01400\n",
      "       20/1    0.85383    0.83740 +/- 0.01265\n",
      "       21/1    0.86647    0.84005 +/- 0.01174\n",
      "       22/1    0.81713    0.83814 +/- 0.01089\n",
      "       23/1    0.85275    0.83926 +/- 0.01008\n",
      "       24/1    0.86851    0.84135 +/- 0.00956\n",
      "       25/1    0.84814    0.84180 +/- 0.00891\n",
      "       26/1    0.85268    0.84248 +/- 0.00837\n",
      "       27/1    0.91608    0.84681 +/- 0.00897\n",
      "       28/1    0.83835    0.84634 +/- 0.00847\n",
      "       29/1    0.81216    0.84454 +/- 0.00821\n",
      "       30/1    0.81024    0.84283 +/- 0.00798\n",
      "       31/1    0.79535    0.84057 +/- 0.00792\n",
      "       32/1    0.80667    0.83903 +/- 0.00771\n",
      "       33/1    0.84960    0.83948 +/- 0.00738\n",
      "       34/1    0.80292    0.83796 +/- 0.00723\n",
      "       35/1    0.82920    0.83761 +/- 0.00694\n",
      "       36/1    0.88990    0.83962 +/- 0.00696\n",
      "       37/1    0.82274    0.83900 +/- 0.00673\n",
      "       38/1    0.77730    0.83679 +/- 0.00685\n",
      "       39/1    0.85654    0.83747 +/- 0.00664\n",
      "       40/1    0.86892    0.83852 +/- 0.00650\n",
      "       41/1    0.90254    0.84059 +/- 0.00662\n",
      "       42/1    0.86666    0.84140 +/- 0.00646\n",
      "       43/1    0.86023    0.84197 +/- 0.00629\n",
      "       44/1    0.85197    0.84227 +/- 0.00611\n",
      "       45/1    0.79840    0.84101 +/- 0.00606\n",
      "       46/1    0.89092    0.84240 +/- 0.00605\n",
      "       47/1    0.91582    0.84438 +/- 0.00621\n",
      "       48/1    0.81594    0.84364 +/- 0.00609\n",
      "       49/1    0.81900    0.84300 +/- 0.00597\n",
      "       50/1    0.84671    0.84310 +/- 0.00582\n",
      "       51/1    0.88214    0.84405 +/- 0.00575\n",
      "       52/1    0.84352    0.84404 +/- 0.00561\n",
      "       53/1    0.86777    0.84459 +/- 0.00551\n",
      "       54/1    0.78129    0.84315 +/- 0.00557\n",
      "       55/1    0.85840    0.84349 +/- 0.00546\n",
      "       56/1    0.80863    0.84273 +/- 0.00539\n",
      "       57/1    0.82647    0.84238 +/- 0.00529\n",
      "       58/1    0.87793    0.84313 +/- 0.00523\n",
      "       59/1    0.81809    0.84261 +/- 0.00515\n",
      "       60/1    0.82066    0.84218 +/- 0.00506\n",
      "       61/1    0.82515    0.84184 +/- 0.00497\n",
      "       62/1    0.87484    0.84248 +/- 0.00492\n",
      "       63/1    0.87506    0.84309 +/- 0.00486\n",
      "       64/1    0.83154    0.84288 +/- 0.00478\n",
      "       65/1    0.76795    0.84151 +/- 0.00488\n",
      "       66/1    0.89135    0.84240 +/- 0.00488\n",
      "       67/1    0.82898    0.84217 +/- 0.00480\n",
      "       68/1    0.81531    0.84171 +/- 0.00473\n",
      "       69/1    0.83053    0.84152 +/- 0.00466\n",
      "       70/1    0.83328    0.84138 +/- 0.00458\n",
      "       71/1    0.78678    0.84048 +/- 0.00459\n",
      "       72/1    0.80836    0.83997 +/- 0.00455\n",
      "       73/1    0.80740    0.83945 +/- 0.00451\n",
      "       74/1    0.76353    0.83826 +/- 0.00459\n",
      "       75/1    0.88363    0.83896 +/- 0.00457\n",
      "       76/1    0.89715    0.83984 +/- 0.00459\n",
      "       77/1    0.88416    0.84050 +/- 0.00457\n",
      "       78/1    0.83159    0.84037 +/- 0.00450\n",
      "       79/1    0.89735    0.84120 +/- 0.00451\n",
      "       80/1    0.93387    0.84252 +/- 0.00464\n",
      "       81/1    0.82384    0.84226 +/- 0.00458\n",
      "       82/1    0.76773    0.84122 +/- 0.00464\n",
      "       83/1    0.86230    0.84151 +/- 0.00458\n",
      "       84/1    0.92572    0.84265 +/- 0.00466\n",
      "       85/1    0.79349    0.84200 +/- 0.00464\n",
      "       86/1    0.84166    0.84199 +/- 0.00458\n",
      "       87/1    0.79133    0.84133 +/- 0.00457\n",
      "       88/1    0.79088    0.84069 +/- 0.00456\n",
      "       89/1    0.85389    0.84085 +/- 0.00450\n",
      "       90/1    0.79765    0.84031 +/- 0.00448\n",
      "       91/1    0.82745    0.84015 +/- 0.00442\n",
      "       92/1    0.79995    0.83966 +/- 0.00440\n",
      "       93/1    0.82776    0.83952 +/- 0.00435\n",
      "       94/1    0.84485    0.83958 +/- 0.00430\n",
      "       95/1    0.90255    0.84032 +/- 0.00431\n",
      "       96/1    0.91112    0.84115 +/- 0.00434\n",
      "       97/1    0.82607    0.84097 +/- 0.00429\n",
      "       98/1    0.86315    0.84123 +/- 0.00425\n",
      "       99/1    0.85380    0.84137 +/- 0.00420\n",
      "      100/1    0.84776    0.84144 +/- 0.00416\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.5646e+00 seconds\n",
      "   Time in transport only          = 4.3749e+00 seconds\n",
      "   Time in inactive batches        = 2.5125e-01 seconds\n",
      "   Time in active batches          = 4.3133e+00 seconds\n",
      "   Time synchronizing fission bank = 1.2266e-02 seconds\n",
      "     Sampling source sites         = 1.0336e-02 seconds\n",
      "     SEND/RECV source sites        = 1.5405e-03 seconds\n",
      "   Time accumulating tallies       = 1.6028e-01 seconds\n",
      "   Time writing statepoints        = 5.7001e-03 seconds\n",
      " Total time for finalization       = 9.5813e-05 seconds\n",
      " Total time elapsed                = 4.5911e+00 seconds\n",
      " Calculation Rate (inactive)       = 39801.3 particles/second\n",
      " Calculation Rate (active)         = 20865.5 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.84206 +/- 0.00355\n",
      " k-effective (Track-length)  = 0.84144 +/- 0.00416\n",
      " k-effective (Absorption)    = 0.83859 +/- 0.00275\n",
      " Combined k-effective        = 0.83961 +/- 0.00255\n",
      " Leakage Fraction            = 0.13700 +/- 0.00138\n",
      "\n",
      " Creating state point openmc_simulation_n5.h5...\n"
     ]
    }
   ],
   "source": [
    "chain_file = '/home/lorenzo/ca_depletion_chains/chain_simple.xml'\n",
    "# Set material volume for depletion.\n",
    "uf4.volume = pi * fuel_or.r**2 * height\n",
    "ofc_uf4.volume  = 3*uf4.volume \n",
    "\n",
    "op = openmc.deplete.CoupledOperator(model, chain_file)\n",
    "# Perform simulation using the predictor algorithm\n",
    "time_steps = [1.0, 1.0, 1.0, 1.0, 1.0]  # days\n",
    "power = 1.0e5  # W\n",
    "integrator = openmc.deplete.PredictorIntegrator(op, time_steps, power, timestep_units='d')\n",
    "integrator.integrate()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 9,
   "id": "8068fa74-8aea-4a63-9b12-5808879ac56e",
   "metadata": {},
   "outputs": [],
   "source": [
    "res_ref = openmc.deplete.Results('depletion_results.h5')"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "9d54b8e6-6303-4989-bf2e-b3d4f4e77a4a",
   "metadata": {},
   "source": [
    "To simulate the continuous circulation of fuel salt from in-core to out-of-core and vice versa, we can set up inventory transfers, by making use of `TransferRates` methodology, with trasnfer rates $\\lambda_i$ defined as: \n",
    "\n",
    "\\begin{equation}\n",
    "\\lambda_i = \\frac{1}{V_i \\dot{m}_i}\n",
    "\\end{equation}\n",
    "\n",
    "where $V_i$ is the fuel salt volume of the material we're transferring from and $\\dot{m}_i$ the flow rate. \n",
    "\n",
    "In this example, we will set transfer rates from in-core to out-of-core and vice versa for the all fuel salt invetories, with the fuel salt out-of-core volume being 3 times larger than the one in-core.\n",
    "\n",
    "We also need to activate the `destination_material` argument to keep track of the transfers between different deplatable materials. "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 10,
   "id": "561fee7d",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "                                %%%%%%%%%%%%%%%\n",
      "                           %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                        %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                      %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                    %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                   %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                    %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                                     %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                 ###############      %%%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ##################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ###################     %%%%%%%%%%%%%%%%%%%%%%%\n",
      "                ####################     %%%%%%%%%%%%%%%%%%%%%%\n",
      "                #####################     %%%%%%%%%%%%%%%%%%%%%\n",
      "                ######################     %%%%%%%%%%%%%%%%%%%%\n",
      "                #######################     %%%%%%%%%%%%%%%%%%\n",
      "                 #######################     %%%%%%%%%%%%%%%%%\n",
      "                 ######################     %%%%%%%%%%%%%%%%%\n",
      "                  ####################     %%%%%%%%%%%%%%%%%\n",
      "                    #################     %%%%%%%%%%%%%%%%%\n",
      "                     ###############     %%%%%%%%%%%%%%%%\n",
      "                       ############     %%%%%%%%%%%%%%%\n",
      "                          ########     %%%%%%%%%%%%%%\n",
      "                                      %%%%%%%%%%%\n",
      "\n",
      "                 | The OpenMC Monte Carlo Code\n",
      "       Copyright | 2011-2024 MIT, UChicago Argonne LLC, and contributors\n",
      "         License | https://docs.openmc.org/en/latest/license.html\n",
      "         Version | 0.14.1-dev\n",
      "        Git SHA1 | d93ac83697e7fdb4fd4cc0f2705795398bf804bd\n",
      "       Date/Time | 2024-04-19 11:05:31\n",
      "   MPI Processes | 1\n",
      "  OpenMP Threads | 56\n",
      "\n",
      " Reading settings XML file...\n",
      " Reading cross sections XML file...\n",
      " Reading materials XML file...\n",
      " Reading geometry XML file...\n",
      " Reading U234 from /home/lorenzo/nuclear_data/endfb80_hdf5/U234.h5\n",
      " Reading U235 from /home/lorenzo/nuclear_data/endfb80_hdf5/U235.h5\n",
      " Reading U238 from /home/lorenzo/nuclear_data/endfb80_hdf5/U238.h5\n",
      " Reading F19 from /home/lorenzo/nuclear_data/endfb80_hdf5/F19.h5\n",
      " Reading U236 from /home/lorenzo/nuclear_data/endfb80_hdf5/U236.h5\n",
      " Reading He3 from /home/lorenzo/nuclear_data/endfb80_hdf5/He3.h5\n",
      " Reading He4 from /home/lorenzo/nuclear_data/endfb80_hdf5/He4.h5\n",
      " Reading Cr50 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr50.h5\n",
      " Reading Cr52 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr52.h5\n",
      " Reading Cr53 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr53.h5\n",
      " Reading Cr54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cr54.h5\n",
      " Reading Fe54 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe54.h5\n",
      " Reading Fe56 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe56.h5\n",
      " Reading Fe57 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe57.h5\n",
      " Reading Fe58 from /home/lorenzo/nuclear_data/endfb80_hdf5/Fe58.h5\n",
      " Reading Sn112 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn112.h5\n",
      " Reading Sn114 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn114.h5\n",
      " Reading Sn115 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn115.h5\n",
      " Reading Sn116 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn116.h5\n",
      " Reading Sn117 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn117.h5\n",
      " Reading Sn118 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn118.h5\n",
      " Reading Sn119 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn119.h5\n",
      " Reading Sn120 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn120.h5\n",
      " Reading Sn122 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn122.h5\n",
      " Reading Sn124 from /home/lorenzo/nuclear_data/endfb80_hdf5/Sn124.h5\n",
      " Reading Zr90 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr90.h5\n",
      " Reading Zr91 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr91.h5\n",
      " Reading Zr92 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr92.h5\n",
      " Reading Zr94 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr94.h5\n",
      " Reading Zr96 from /home/lorenzo/nuclear_data/endfb80_hdf5/Zr96.h5\n",
      " Reading B10 from /home/lorenzo/nuclear_data/endfb80_hdf5/B10.h5\n"
     ]
    },
    {
     "name": "stderr",
     "output_type": "stream",
     "text": [
      " WARNING: Negative value(s) found on probability table for nuclide Zr96 at 294K\n"
     ]
    },
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      " Reading B11 from /home/lorenzo/nuclear_data/endfb80_hdf5/B11.h5\n",
      " Reading H1 from /home/lorenzo/nuclear_data/endfb80_hdf5/H1.h5\n",
      " Reading H2 from /home/lorenzo/nuclear_data/endfb80_hdf5/H2.h5\n",
      " Reading O16 from /home/lorenzo/nuclear_data/endfb80_hdf5/O16.h5\n",
      " Reading O17 from /home/lorenzo/nuclear_data/endfb80_hdf5/O17.h5\n",
      " Reading O18 from /home/lorenzo/nuclear_data/endfb80_hdf5/O18.h5\n",
      " Reading c_H_in_H2O from /home/lorenzo/nuclear_data/endfb80_hdf5/c_H_in_H2O.h5\n",
      " Minimum neutron data temperature: 0 K\n",
      " Maximum neutron data temperature: 1.7976931348623157e+308 K\n",
      " Preparing distributed cell instances...\n",
      " Reading plot XML file...\n",
      " Writing summary.h5 file...\n",
      "[openmc.deplete] t=0.0 s, dt=86400.0 s, source=100000.0\n",
      " Reading I135 from /home/lorenzo/nuclear_data/endfb80_hdf5/I135.h5\n",
      " Reading Xe135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe135.h5\n",
      " Reading Xe136 from /home/lorenzo/nuclear_data/endfb80_hdf5/Xe136.h5\n",
      " Reading Cs135 from /home/lorenzo/nuclear_data/endfb80_hdf5/Cs135.h5\n",
      " Reading Gd157 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd157.h5\n",
      " Reading Gd156 from /home/lorenzo/nuclear_data/endfb80_hdf5/Gd156.h5\n",
      " Reading Pu239 from /home/lorenzo/nuclear_data/endfb80_hdf5/Pu239.h5\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.55230\n",
      "        2/1    0.71581\n",
      "        3/1    0.84742\n",
      "        4/1    0.82083\n",
      "        5/1    0.88937\n",
      "        6/1    0.83661\n",
      "        7/1    0.90388\n",
      "        8/1    0.89892\n",
      "        9/1    0.84564\n",
      "       10/1    0.89387\n",
      "       11/1    0.81112\n",
      "       12/1    0.90903    0.86007 +/- 0.04896\n",
      "       13/1    0.82243    0.84752 +/- 0.03093\n",
      "       14/1    0.87888    0.85536 +/- 0.02323\n",
      "       15/1    0.85114    0.85452 +/- 0.01801\n",
      "       16/1    0.88721    0.85997 +/- 0.01569\n",
      "       17/1    0.88177    0.86308 +/- 0.01362\n",
      "       18/1    0.90888    0.86881 +/- 0.01311\n",
      "       19/1    0.83572    0.86513 +/- 0.01213\n",
      "       20/1    0.83936    0.86255 +/- 0.01115\n",
      "       21/1    0.94591    0.87013 +/- 0.01262\n",
      "       22/1    0.84293    0.86787 +/- 0.01174\n",
      "       23/1    0.88706    0.86934 +/- 0.01090\n",
      "       24/1    0.87462    0.86972 +/- 0.01010\n",
      "       25/1    0.77153    0.86317 +/- 0.01145\n",
      "       26/1    0.85637    0.86275 +/- 0.01072\n",
      "       27/1    0.80862    0.85956 +/- 0.01056\n",
      "       28/1    0.85113    0.85909 +/- 0.00997\n",
      "       29/1    0.83268    0.85770 +/- 0.00953\n",
      "       30/1    0.86520    0.85808 +/- 0.00905\n",
      "       31/1    0.93140    0.86157 +/- 0.00929\n",
      "       32/1    0.88934    0.86283 +/- 0.00895\n",
      "       33/1    0.87335    0.86329 +/- 0.00856\n",
      "       34/1    0.87573    0.86381 +/- 0.00821\n",
      "       35/1    0.91501    0.86586 +/- 0.00814\n",
      "       36/1    0.82385    0.86424 +/- 0.00799\n",
      "       37/1    0.82322    0.86272 +/- 0.00783\n",
      "       38/1    0.87062    0.86300 +/- 0.00755\n",
      "       39/1    0.86394    0.86304 +/- 0.00729\n",
      "       40/1    0.88725    0.86384 +/- 0.00709\n",
      "       41/1    0.88834    0.86463 +/- 0.00690\n",
      "       42/1    0.85313    0.86427 +/- 0.00669\n",
      "       43/1    0.93063    0.86629 +/- 0.00679\n",
      "       44/1    0.81729    0.86484 +/- 0.00674\n",
      "       45/1    0.79035    0.86272 +/- 0.00689\n",
      "       46/1    0.96206    0.86548 +/- 0.00724\n",
      "       47/1    0.88932    0.86612 +/- 0.00707\n",
      "       48/1    0.93670    0.86798 +/- 0.00713\n",
      "       49/1    0.88749    0.86848 +/- 0.00696\n",
      "       50/1    0.88210    0.86882 +/- 0.00679\n",
      "       51/1    0.83792    0.86806 +/- 0.00667\n",
      "       52/1    0.86035    0.86788 +/- 0.00651\n",
      "       53/1    0.83267    0.86706 +/- 0.00641\n",
      "       54/1    0.86629    0.86704 +/- 0.00626\n",
      "       55/1    0.83651    0.86637 +/- 0.00616\n",
      "       56/1    0.86899    0.86642 +/- 0.00602\n",
      "       57/1    0.86755    0.86645 +/- 0.00589\n",
      "       58/1    0.86296    0.86637 +/- 0.00577\n",
      "       59/1    0.90701    0.86720 +/- 0.00571\n",
      "       60/1    0.88598    0.86758 +/- 0.00561\n",
      "       61/1    0.83798    0.86700 +/- 0.00553\n",
      "       62/1    0.81695    0.86604 +/- 0.00551\n",
      "       63/1    0.90488    0.86677 +/- 0.00545\n",
      "       64/1    0.91599    0.86768 +/- 0.00543\n",
      "       65/1    0.85986    0.86754 +/- 0.00533\n",
      "       66/1    0.85999    0.86740 +/- 0.00523\n",
      "       67/1    0.88330    0.86768 +/- 0.00515\n",
      "       68/1    0.84368    0.86727 +/- 0.00508\n",
      "       69/1    0.86791    0.86728 +/- 0.00499\n",
      "       70/1    0.81372    0.86639 +/- 0.00499\n",
      "       71/1    0.87471    0.86652 +/- 0.00490\n",
      "       72/1    0.82349    0.86583 +/- 0.00487\n",
      "       73/1    0.92667    0.86679 +/- 0.00489\n",
      "       74/1    0.85169    0.86656 +/- 0.00482\n",
      "       75/1    0.83902    0.86614 +/- 0.00477\n",
      "       76/1    0.89600    0.86659 +/- 0.00471\n",
      "       77/1    0.86706    0.86659 +/- 0.00464\n",
      "       78/1    0.84111    0.86622 +/- 0.00459\n",
      "       79/1    0.80299    0.86530 +/- 0.00462\n",
      "       80/1    0.86359    0.86528 +/- 0.00455\n",
      "       81/1    0.80849    0.86448 +/- 0.00456\n",
      "       82/1    0.89804    0.86495 +/- 0.00452\n",
      "       83/1    0.86185    0.86490 +/- 0.00445\n",
      "       84/1    0.86501    0.86490 +/- 0.00439\n",
      "       85/1    0.84290    0.86461 +/- 0.00434\n",
      "       86/1    0.88679    0.86490 +/- 0.00430\n",
      "       87/1    0.92261    0.86565 +/- 0.00431\n",
      "       88/1    0.82757    0.86516 +/- 0.00428\n",
      "       89/1    0.87889    0.86534 +/- 0.00423\n",
      "       90/1    0.88855    0.86563 +/- 0.00418\n",
      "       91/1    0.85702    0.86552 +/- 0.00413\n",
      "       92/1    0.86806    0.86555 +/- 0.00408\n",
      "       93/1    0.88195    0.86575 +/- 0.00404\n",
      "       94/1    0.86865    0.86578 +/- 0.00399\n",
      "       95/1    0.89434    0.86612 +/- 0.00396\n",
      "       96/1    0.93531    0.86693 +/- 0.00399\n",
      "       97/1    0.91389    0.86747 +/- 0.00398\n",
      "       98/1    0.88900    0.86771 +/- 0.00395\n",
      "       99/1    0.86813    0.86771 +/- 0.00390\n",
      "      100/1    0.84827    0.86750 +/- 0.00386\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 3.1905e+00 seconds\n",
      "   Reading cross sections          = 3.1691e+00 seconds\n",
      " Total time in simulation          = 4.9281e+00 seconds\n",
      "   Time in transport only          = 4.7773e+00 seconds\n",
      "   Time in inactive batches        = 2.7597e-01 seconds\n",
      "   Time in active batches          = 4.6521e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0960e-02 seconds\n",
      "     Sampling source sites         = 9.1688e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5092e-03 seconds\n",
      "   Time accumulating tallies       = 1.2215e-01 seconds\n",
      "   Time writing statepoints        = 5.9944e-03 seconds\n",
      " Total time for finalization       = 9.9481e-05 seconds\n",
      " Total time elapsed                = 8.1428e+00 seconds\n",
      " Calculation Rate (inactive)       = 36235.2 particles/second\n",
      " Calculation Rate (active)         = 19346 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.87058 +/- 0.00340\n",
      " k-effective (Track-length)  = 0.86750 +/- 0.00386\n",
      " k-effective (Absorption)    = 0.88032 +/- 0.00359\n",
      " Combined k-effective        = 0.87426 +/- 0.00317\n",
      " Leakage Fraction            = 0.13803 +/- 0.00134\n",
      "\n",
      " Creating state point openmc_simulation_n0.h5...\n",
      "[openmc.deplete] t=86400.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.51016\n",
      "        2/1    0.70694\n",
      "        3/1    0.80137\n",
      "        4/1    0.85213\n",
      "        5/1    0.90322\n",
      "        6/1    0.84716\n",
      "        7/1    0.86525\n",
      "        8/1    0.82738\n",
      "        9/1    0.85755\n",
      "       10/1    0.79667\n",
      "       11/1    0.95124\n",
      "       12/1    0.81329    0.88226 +/- 0.06897\n",
      "       13/1    0.85976    0.87476 +/- 0.04052\n",
      "       14/1    0.88503    0.87733 +/- 0.02877\n",
      "       15/1    0.82440    0.86674 +/- 0.02467\n",
      "       16/1    0.88798    0.87028 +/- 0.02045\n",
      "       17/1    0.86665    0.86976 +/- 0.01729\n",
      "       18/1    0.88484    0.87165 +/- 0.01509\n",
      "       19/1    0.82405    0.86636 +/- 0.01432\n",
      "       20/1    0.83838    0.86356 +/- 0.01311\n",
      "       21/1    0.80969    0.85866 +/- 0.01283\n",
      "       22/1    0.88293    0.86069 +/- 0.01189\n",
      "       23/1    0.85553    0.86029 +/- 0.01094\n",
      "       24/1    0.86503    0.86063 +/- 0.01014\n",
      "       25/1    0.83238    0.85875 +/- 0.00962\n",
      "       26/1    0.85018    0.85821 +/- 0.00902\n",
      "       27/1    0.82265    0.85612 +/- 0.00872\n",
      "       28/1    0.85389    0.85600 +/- 0.00823\n",
      "       29/1    0.84142    0.85523 +/- 0.00782\n",
      "       30/1    0.88500    0.85672 +/- 0.00757\n",
      "       31/1    0.83268    0.85557 +/- 0.00729\n",
      "       32/1    0.81093    0.85354 +/- 0.00724\n",
      "       33/1    0.83567    0.85277 +/- 0.00696\n",
      "       34/1    0.84217    0.85232 +/- 0.00668\n",
      "       35/1    0.91541    0.85485 +/- 0.00688\n",
      "       36/1    0.84167    0.85434 +/- 0.00663\n",
      "       37/1    0.90148    0.85609 +/- 0.00662\n",
      "       38/1    0.86654    0.85646 +/- 0.00639\n",
      "       39/1    0.92671    0.85888 +/- 0.00662\n",
      "       40/1    0.88573    0.85978 +/- 0.00646\n",
      "       41/1    0.86234    0.85986 +/- 0.00625\n",
      "       42/1    0.83850    0.85919 +/- 0.00609\n",
      "       43/1    0.89684    0.86033 +/- 0.00601\n",
      "       44/1    0.88790    0.86114 +/- 0.00589\n",
      "       45/1    0.91692    0.86274 +/- 0.00593\n",
      "       46/1    0.85332    0.86248 +/- 0.00577\n",
      "       47/1    0.88679    0.86313 +/- 0.00565\n",
      "       48/1    0.96352    0.86577 +/- 0.00610\n",
      "       49/1    0.84305    0.86519 +/- 0.00597\n",
      "       50/1    0.82926    0.86429 +/- 0.00589\n",
      "       51/1    0.93361    0.86598 +/- 0.00599\n",
      "       52/1    0.86829    0.86604 +/- 0.00584\n",
      "       53/1    0.84471    0.86554 +/- 0.00573\n",
      "       54/1    0.89608    0.86624 +/- 0.00564\n",
      "       55/1    0.85306    0.86594 +/- 0.00552\n",
      "       56/1    0.90137    0.86671 +/- 0.00545\n",
      "       57/1    0.86772    0.86674 +/- 0.00534\n",
      "       58/1    0.83584    0.86609 +/- 0.00526\n",
      "       59/1    0.83518    0.86546 +/- 0.00519\n",
      "       60/1    0.90007    0.86615 +/- 0.00514\n",
      "       61/1    0.89436    0.86671 +/- 0.00506\n",
      "       62/1    0.90947    0.86753 +/- 0.00503\n",
      "       63/1    0.80117    0.86628 +/- 0.00509\n",
      "       64/1    0.86368    0.86623 +/- 0.00500\n",
      "       65/1    0.87915    0.86646 +/- 0.00491\n",
      "       66/1    0.88242    0.86675 +/- 0.00483\n",
      "       67/1    0.87332    0.86686 +/- 0.00475\n",
      "       68/1    0.80271    0.86576 +/- 0.00480\n",
      "       69/1    0.86925    0.86582 +/- 0.00471\n",
      "       70/1    0.83929    0.86537 +/- 0.00466\n",
      "       71/1    0.89176    0.86581 +/- 0.00460\n",
      "       72/1    0.84971    0.86555 +/- 0.00453\n",
      "       73/1    0.85257    0.86534 +/- 0.00446\n",
      "       74/1    0.85054    0.86511 +/- 0.00440\n",
      "       75/1    0.88424    0.86540 +/- 0.00434\n",
      "       76/1    0.89588    0.86587 +/- 0.00430\n",
      "       77/1    0.86930    0.86592 +/- 0.00424\n",
      "       78/1    0.81709    0.86520 +/- 0.00423\n",
      "       79/1    0.90094    0.86572 +/- 0.00420\n",
      "       80/1    0.86868    0.86576 +/- 0.00414\n",
      "       81/1    0.83006    0.86526 +/- 0.00412\n",
      "       82/1    0.93226    0.86619 +/- 0.00416\n",
      "       83/1    0.84296    0.86587 +/- 0.00412\n",
      "       84/1    0.80604    0.86506 +/- 0.00414\n",
      "       85/1    0.85575    0.86494 +/- 0.00409\n",
      "       86/1    0.88612    0.86522 +/- 0.00404\n",
      "       87/1    0.84585    0.86496 +/- 0.00400\n",
      "       88/1    0.83857    0.86463 +/- 0.00396\n",
      "       89/1    0.89261    0.86498 +/- 0.00393\n",
      "       90/1    0.84147    0.86469 +/- 0.00389\n",
      "       91/1    0.93667    0.86557 +/- 0.00394\n",
      "       92/1    0.88567    0.86582 +/- 0.00390\n",
      "       93/1    0.88113    0.86600 +/- 0.00386\n",
      "       94/1    0.88969    0.86629 +/- 0.00382\n",
      "       95/1    0.91403    0.86685 +/- 0.00382\n",
      "       96/1    0.87702    0.86697 +/- 0.00378\n",
      "       97/1    0.89574    0.86730 +/- 0.00375\n",
      "       98/1    0.85853    0.86720 +/- 0.00371\n",
      "       99/1    0.84607    0.86696 +/- 0.00367\n",
      "      100/1    0.86847    0.86698 +/- 0.00363\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 5.4366e+00 seconds\n",
      "   Time in transport only          = 5.3499e+00 seconds\n",
      "   Time in inactive batches        = 2.3458e-01 seconds\n",
      "   Time in active batches          = 5.2020e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0546e-02 seconds\n",
      "     Sampling source sites         = 8.7760e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4892e-03 seconds\n",
      "   Time accumulating tallies       = 6.2211e-02 seconds\n",
      "   Time writing statepoints        = 4.2708e-03 seconds\n",
      " Total time for finalization       = 7.4982e-05 seconds\n",
      " Total time elapsed                = 5.4602e+00 seconds\n",
      " Calculation Rate (inactive)       = 42629.2 particles/second\n",
      " Calculation Rate (active)         = 17301.1 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.87030 +/- 0.00339\n",
      " k-effective (Track-length)  = 0.86698 +/- 0.00363\n",
      " k-effective (Absorption)    = 0.86418 +/- 0.00283\n",
      " Combined k-effective        = 0.86594 +/- 0.00235\n",
      " Leakage Fraction            = 0.13900 +/- 0.00132\n",
      "\n",
      " Creating state point openmc_simulation_n1.h5...\n",
      "[openmc.deplete] t=172800.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.51290\n",
      "        2/1    0.68004\n",
      "        3/1    0.73043\n",
      "        4/1    0.83011\n",
      "        5/1    0.88751\n",
      "        6/1    0.84468\n",
      "        7/1    0.85009\n",
      "        8/1    0.86270\n",
      "        9/1    0.84556\n",
      "       10/1    0.87429\n",
      "       11/1    0.83501\n",
      "       12/1    0.84418    0.83960 +/- 0.00459\n",
      "       13/1    0.90367    0.86096 +/- 0.02152\n",
      "       14/1    0.81253    0.84885 +/- 0.01945\n",
      "       15/1    0.82517    0.84411 +/- 0.01579\n",
      "       16/1    0.84450    0.84418 +/- 0.01289\n",
      "       17/1    0.92632    0.85591 +/- 0.01601\n",
      "       18/1    0.81887    0.85128 +/- 0.01462\n",
      "       19/1    0.84845    0.85097 +/- 0.01290\n",
      "       20/1    0.90304    0.85618 +/- 0.01266\n",
      "       21/1    0.85003    0.85562 +/- 0.01146\n",
      "       22/1    0.80624    0.85150 +/- 0.01124\n",
      "       23/1    0.87828    0.85356 +/- 0.01055\n",
      "       24/1    0.94236    0.85991 +/- 0.01164\n",
      "       25/1    0.83760    0.85842 +/- 0.01094\n",
      "       26/1    0.91545    0.86198 +/- 0.01084\n",
      "       27/1    0.84193    0.86080 +/- 0.01025\n",
      "       28/1    0.84823    0.86010 +/- 0.00969\n",
      "       29/1    0.84891    0.85952 +/- 0.00918\n",
      "       30/1    0.86882    0.85998 +/- 0.00872\n",
      "       31/1    0.81165    0.85768 +/- 0.00861\n",
      "       32/1    0.89898    0.85956 +/- 0.00842\n",
      "       33/1    0.88321    0.86058 +/- 0.00811\n",
      "       34/1    0.86071    0.86059 +/- 0.00777\n",
      "       35/1    0.91614    0.86281 +/- 0.00777\n",
      "       36/1    0.82472    0.86135 +/- 0.00761\n",
      "       37/1    0.90443    0.86294 +/- 0.00750\n",
      "       38/1    0.86868    0.86315 +/- 0.00723\n",
      "       39/1    0.88191    0.86379 +/- 0.00700\n",
      "       40/1    0.85588    0.86353 +/- 0.00677\n",
      "       41/1    0.91490    0.86519 +/- 0.00675\n",
      "       42/1    0.88905    0.86593 +/- 0.00658\n",
      "       43/1    0.89898    0.86693 +/- 0.00646\n",
      "       44/1    0.83802    0.86608 +/- 0.00632\n",
      "       45/1    0.87816    0.86643 +/- 0.00615\n",
      "       46/1    0.86566    0.86641 +/- 0.00598\n",
      "       47/1    0.87392    0.86661 +/- 0.00582\n",
      "       48/1    0.84233    0.86597 +/- 0.00570\n",
      "       49/1    0.93627    0.86777 +/- 0.00583\n",
      "       50/1    0.91034    0.86884 +/- 0.00579\n",
      "       51/1    0.86047    0.86863 +/- 0.00565\n",
      "       52/1    0.93583    0.87023 +/- 0.00574\n",
      "       53/1    0.85841    0.86996 +/- 0.00561\n",
      "       54/1    0.84105    0.86930 +/- 0.00552\n",
      "       55/1    0.85792    0.86905 +/- 0.00540\n",
      "       56/1    0.82157    0.86802 +/- 0.00538\n",
      "       57/1    0.81515    0.86689 +/- 0.00539\n",
      "       58/1    0.85273    0.86660 +/- 0.00528\n",
      "       59/1    0.87543    0.86678 +/- 0.00517\n",
      "       60/1    0.80586    0.86556 +/- 0.00521\n",
      "       61/1    0.85865    0.86542 +/- 0.00511\n",
      "       62/1    0.85879    0.86530 +/- 0.00502\n",
      "       63/1    0.86765    0.86534 +/- 0.00492\n",
      "       64/1    0.88001    0.86561 +/- 0.00484\n",
      "       65/1    0.86598    0.86562 +/- 0.00475\n",
      "       66/1    0.85402    0.86541 +/- 0.00467\n",
      "       67/1    0.88263    0.86571 +/- 0.00459\n",
      "       68/1    0.87730    0.86591 +/- 0.00452\n",
      "       69/1    0.84724    0.86560 +/- 0.00445\n",
      "       70/1    0.88188    0.86587 +/- 0.00439\n",
      "       71/1    0.89216    0.86630 +/- 0.00433\n",
      "       72/1    0.89626    0.86678 +/- 0.00429\n",
      "       73/1    0.82885    0.86618 +/- 0.00427\n",
      "       74/1    0.90183    0.86674 +/- 0.00423\n",
      "       75/1    0.86786    0.86676 +/- 0.00417\n",
      "       76/1    0.83642    0.86630 +/- 0.00413\n",
      "       77/1    0.84216    0.86594 +/- 0.00409\n",
      "       78/1    0.86197    0.86588 +/- 0.00402\n",
      "       79/1    0.88573    0.86616 +/- 0.00398\n",
      "       80/1    0.88082    0.86637 +/- 0.00392\n",
      "       81/1    0.90282    0.86689 +/- 0.00390\n",
      "       82/1    0.87113    0.86695 +/- 0.00385\n",
      "       83/1    0.89318    0.86731 +/- 0.00381\n",
      "       84/1    0.88723    0.86757 +/- 0.00377\n",
      "       85/1    0.89619    0.86796 +/- 0.00374\n",
      "       86/1    0.87435    0.86804 +/- 0.00369\n",
      "       87/1    0.91946    0.86871 +/- 0.00370\n",
      "       88/1    0.82690    0.86817 +/- 0.00369\n",
      "       89/1    0.93251    0.86899 +/- 0.00374\n",
      "       90/1    0.82554    0.86844 +/- 0.00373\n",
      "       91/1    0.91377    0.86900 +/- 0.00373\n",
      "       92/1    0.85771    0.86887 +/- 0.00368\n",
      "       93/1    0.82072    0.86829 +/- 0.00368\n",
      "       94/1    0.82137    0.86773 +/- 0.00368\n",
      "       95/1    0.84943    0.86751 +/- 0.00365\n",
      "       96/1    0.83907    0.86718 +/- 0.00362\n",
      "       97/1    0.85934    0.86709 +/- 0.00358\n",
      "       98/1    0.89312    0.86739 +/- 0.00355\n",
      "       99/1    0.91106    0.86788 +/- 0.00354\n",
      "      100/1    0.84876    0.86767 +/- 0.00351\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.5446e+00 seconds\n",
      "   Time in transport only          = 4.4635e+00 seconds\n",
      "   Time in inactive batches        = 2.2799e-01 seconds\n",
      "   Time in active batches          = 4.3166e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0397e-02 seconds\n",
      "     Sampling source sites         = 8.5678e-03 seconds\n",
      "     SEND/RECV source sites        = 1.5270e-03 seconds\n",
      "   Time accumulating tallies       = 5.6442e-02 seconds\n",
      "   Time writing statepoints        = 3.6652e-03 seconds\n",
      " Total time for finalization       = 8.2690e-05 seconds\n",
      " Total time elapsed                = 4.5674e+00 seconds\n",
      " Calculation Rate (inactive)       = 43862.1 particles/second\n",
      " Calculation Rate (active)         = 20849.6 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86857 +/- 0.00341\n",
      " k-effective (Track-length)  = 0.86767 +/- 0.00351\n",
      " k-effective (Absorption)    = 0.86511 +/- 0.00326\n",
      " Combined k-effective        = 0.86656 +/- 0.00274\n",
      " Leakage Fraction            = 0.13682 +/- 0.00126\n",
      "\n",
      " Creating state point openmc_simulation_n2.h5...\n",
      "[openmc.deplete] t=259200.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.53631\n",
      "        2/1    0.67717\n",
      "        3/1    0.74156\n",
      "        4/1    0.85831\n",
      "        5/1    0.86116\n",
      "        6/1    0.92384\n",
      "        7/1    0.82118\n",
      "        8/1    0.85597\n",
      "        9/1    0.82158\n",
      "       10/1    0.90193\n",
      "       11/1    0.86630\n",
      "       12/1    0.86227    0.86429 +/- 0.00202\n",
      "       13/1    0.86326    0.86394 +/- 0.00121\n",
      "       14/1    0.90492    0.87419 +/- 0.01028\n",
      "       15/1    0.87778    0.87490 +/- 0.00799\n",
      "       16/1    0.78856    0.86051 +/- 0.01580\n",
      "       17/1    0.87400    0.86244 +/- 0.01349\n",
      "       18/1    0.85914    0.86203 +/- 0.01169\n",
      "       19/1    0.89518    0.86571 +/- 0.01095\n",
      "       20/1    0.89813    0.86895 +/- 0.01032\n",
      "       21/1    0.86179    0.86830 +/- 0.00935\n",
      "       22/1    0.88816    0.86996 +/- 0.00870\n",
      "       23/1    0.92937    0.87453 +/- 0.00921\n",
      "       24/1    0.82504    0.87099 +/- 0.00923\n",
      "       25/1    0.88852    0.87216 +/- 0.00868\n",
      "       26/1    0.88287    0.87283 +/- 0.00814\n",
      "       27/1    0.82472    0.87000 +/- 0.00816\n",
      "       28/1    0.89422    0.87135 +/- 0.00781\n",
      "       29/1    0.85093    0.87027 +/- 0.00746\n",
      "       30/1    0.86899    0.87021 +/- 0.00708\n",
      "       31/1    0.87952    0.87065 +/- 0.00675\n",
      "       32/1    0.90425    0.87218 +/- 0.00661\n",
      "       33/1    0.87715    0.87239 +/- 0.00632\n",
      "       34/1    0.83801    0.87096 +/- 0.00622\n",
      "       35/1    0.84527    0.86993 +/- 0.00605\n",
      "       36/1    0.92065    0.87188 +/- 0.00614\n",
      "       37/1    0.79037    0.86887 +/- 0.00663\n",
      "       38/1    0.86177    0.86861 +/- 0.00639\n",
      "       39/1    0.92960    0.87072 +/- 0.00652\n",
      "       40/1    0.84093    0.86972 +/- 0.00638\n",
      "       41/1    0.87279    0.86982 +/- 0.00617\n",
      "       42/1    0.79403    0.86745 +/- 0.00642\n",
      "       43/1    0.83144    0.86636 +/- 0.00632\n",
      "       44/1    0.88679    0.86696 +/- 0.00616\n",
      "       45/1    0.84685    0.86639 +/- 0.00601\n",
      "       46/1    0.80119    0.86458 +/- 0.00612\n",
      "       47/1    0.88905    0.86524 +/- 0.00598\n",
      "       48/1    0.86050    0.86511 +/- 0.00583\n",
      "       49/1    0.89533    0.86589 +/- 0.00573\n",
      "       50/1    0.84866    0.86546 +/- 0.00560\n",
      "       51/1    0.85892    0.86530 +/- 0.00546\n",
      "       52/1    0.95752    0.86749 +/- 0.00577\n",
      "       53/1    0.90078    0.86827 +/- 0.00568\n",
      "       54/1    0.88381    0.86862 +/- 0.00556\n",
      "       55/1    0.87178    0.86869 +/- 0.00544\n",
      "       56/1    0.87943    0.86893 +/- 0.00532\n",
      "       57/1    0.86808    0.86891 +/- 0.00521\n",
      "       58/1    0.86353    0.86880 +/- 0.00510\n",
      "       59/1    0.90334    0.86950 +/- 0.00505\n",
      "       60/1    0.91260    0.87036 +/- 0.00502\n",
      "       61/1    0.84378    0.86984 +/- 0.00495\n",
      "       62/1    0.86135    0.86968 +/- 0.00485\n",
      "       63/1    0.83051    0.86894 +/- 0.00482\n",
      "       64/1    0.81437    0.86793 +/- 0.00483\n",
      "       65/1    0.86570    0.86789 +/- 0.00475\n",
      "       66/1    0.81972    0.86703 +/- 0.00474\n",
      "       67/1    0.82453    0.86628 +/- 0.00471\n",
      "       68/1    0.90264    0.86691 +/- 0.00468\n",
      "       69/1    0.83374    0.86635 +/- 0.00463\n",
      "       70/1    0.91277    0.86712 +/- 0.00462\n",
      "       71/1    0.84606    0.86677 +/- 0.00455\n",
      "       72/1    0.86861    0.86680 +/- 0.00448\n",
      "       73/1    0.79077    0.86560 +/- 0.00457\n",
      "       74/1    0.86860    0.86564 +/- 0.00450\n",
      "       75/1    0.85597    0.86550 +/- 0.00443\n",
      "       76/1    0.80515    0.86458 +/- 0.00446\n",
      "       77/1    0.85487    0.86444 +/- 0.00439\n",
      "       78/1    0.85813    0.86434 +/- 0.00433\n",
      "       79/1    0.83846    0.86397 +/- 0.00428\n",
      "       80/1    0.82474    0.86341 +/- 0.00426\n",
      "       81/1    0.90091    0.86394 +/- 0.00423\n",
      "       82/1    0.93114    0.86487 +/- 0.00428\n",
      "       83/1    0.86368    0.86485 +/- 0.00422\n",
      "       84/1    0.85067    0.86466 +/- 0.00416\n",
      "       85/1    0.87457    0.86479 +/- 0.00411\n",
      "       86/1    0.84431    0.86452 +/- 0.00406\n",
      "       87/1    0.88805    0.86483 +/- 0.00402\n",
      "       88/1    0.91257    0.86544 +/- 0.00402\n",
      "       89/1    0.82479    0.86493 +/- 0.00400\n",
      "       90/1    0.80157    0.86414 +/- 0.00403\n",
      "       91/1    0.86690    0.86417 +/- 0.00398\n",
      "       92/1    0.86427    0.86417 +/- 0.00393\n",
      "       93/1    0.88714    0.86445 +/- 0.00389\n",
      "       94/1    0.85061    0.86428 +/- 0.00385\n",
      "       95/1    0.87652    0.86443 +/- 0.00381\n",
      "       96/1    0.89711    0.86481 +/- 0.00378\n",
      "       97/1    0.82913    0.86440 +/- 0.00376\n",
      "       98/1    0.85758    0.86432 +/- 0.00372\n",
      "       99/1    0.86300    0.86430 +/- 0.00367\n",
      "      100/1    0.82278    0.86384 +/- 0.00366\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 5.4941e+00 seconds\n",
      "   Time in transport only          = 5.3814e+00 seconds\n",
      "   Time in inactive batches        = 2.3373e-01 seconds\n",
      "   Time in active batches          = 5.2604e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0497e-02 seconds\n",
      "     Sampling source sites         = 8.7398e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4789e-03 seconds\n",
      "   Time accumulating tallies       = 8.8203e-02 seconds\n",
      "   Time writing statepoints        = 3.8005e-03 seconds\n",
      " Total time for finalization       = 7.8056e-05 seconds\n",
      " Total time elapsed                = 5.5169e+00 seconds\n",
      " Calculation Rate (inactive)       = 42784.7 particles/second\n",
      " Calculation Rate (active)         = 17109 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86055 +/- 0.00341\n",
      " k-effective (Track-length)  = 0.86384 +/- 0.00366\n",
      " k-effective (Absorption)    = 0.86214 +/- 0.00329\n",
      " Combined k-effective        = 0.86212 +/- 0.00284\n",
      " Leakage Fraction            = 0.13661 +/- 0.00112\n",
      "\n",
      " Creating state point openmc_simulation_n3.h5...\n",
      "[openmc.deplete] t=345600.0 s, dt=86400.0 s, source=100000.0\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.51573\n",
      "        2/1    0.63741\n",
      "        3/1    0.81771\n",
      "        4/1    0.79048\n",
      "        5/1    0.85198\n",
      "        6/1    0.87127\n",
      "        7/1    0.86124\n",
      "        8/1    0.85646\n",
      "        9/1    0.84656\n",
      "       10/1    0.90441\n",
      "       11/1    0.88057\n",
      "       12/1    0.81505    0.84781 +/- 0.03276\n",
      "       13/1    0.84845    0.84802 +/- 0.01891\n",
      "       14/1    0.86205    0.85153 +/- 0.01383\n",
      "       15/1    0.89161    0.85955 +/- 0.01338\n",
      "       16/1    0.85460    0.85872 +/- 0.01095\n",
      "       17/1    0.82221    0.85351 +/- 0.01063\n",
      "       18/1    0.84403    0.85232 +/- 0.00928\n",
      "       19/1    0.85103    0.85218 +/- 0.00818\n",
      "       20/1    0.86276    0.85324 +/- 0.00740\n",
      "       21/1    0.91647    0.85898 +/- 0.00882\n",
      "       22/1    0.91086    0.86331 +/- 0.00914\n",
      "       23/1    0.88970    0.86534 +/- 0.00865\n",
      "       24/1    0.81994    0.86210 +/- 0.00864\n",
      "       25/1    0.85056    0.86133 +/- 0.00808\n",
      "       26/1    0.87392    0.86211 +/- 0.00760\n",
      "       27/1    0.82456    0.85990 +/- 0.00747\n",
      "       28/1    0.83464    0.85850 +/- 0.00718\n",
      "       29/1    0.82292    0.85663 +/- 0.00705\n",
      "       30/1    0.85656    0.85662 +/- 0.00669\n",
      "       31/1    0.78367    0.85315 +/- 0.00725\n",
      "       32/1    0.86261    0.85358 +/- 0.00692\n",
      "       33/1    0.89403    0.85534 +/- 0.00684\n",
      "       34/1    0.86256    0.85564 +/- 0.00656\n",
      "       35/1    0.88158    0.85668 +/- 0.00638\n",
      "       36/1    0.90865    0.85868 +/- 0.00644\n",
      "       37/1    0.85924    0.85870 +/- 0.00620\n",
      "       38/1    0.88264    0.85955 +/- 0.00604\n",
      "       39/1    0.83641    0.85875 +/- 0.00588\n",
      "       40/1    0.89551    0.85998 +/- 0.00581\n",
      "       41/1    0.87451    0.86045 +/- 0.00564\n",
      "       42/1    0.86217    0.86050 +/- 0.00546\n",
      "       43/1    0.82014    0.85928 +/- 0.00543\n",
      "       44/1    0.84926    0.85898 +/- 0.00528\n",
      "       45/1    0.90426    0.86028 +/- 0.00529\n",
      "       46/1    0.91148    0.86170 +/- 0.00533\n",
      "       47/1    0.94148    0.86386 +/- 0.00561\n",
      "       48/1    0.94755    0.86606 +/- 0.00589\n",
      "       49/1    0.82631    0.86504 +/- 0.00583\n",
      "       50/1    0.87837    0.86537 +/- 0.00569\n",
      "       51/1    0.85872    0.86521 +/- 0.00555\n",
      "       52/1    0.89466    0.86591 +/- 0.00546\n",
      "       53/1    0.82618    0.86499 +/- 0.00541\n",
      "       54/1    0.86210    0.86492 +/- 0.00529\n",
      "       55/1    0.78926    0.86324 +/- 0.00544\n",
      "       56/1    0.86412    0.86326 +/- 0.00532\n",
      "       57/1    0.87516    0.86351 +/- 0.00521\n",
      "       58/1    0.84133    0.86305 +/- 0.00512\n",
      "       59/1    0.81891    0.86215 +/- 0.00510\n",
      "       60/1    0.84392    0.86179 +/- 0.00501\n",
      "       61/1    0.86661    0.86188 +/- 0.00491\n",
      "       62/1    0.88291    0.86228 +/- 0.00483\n",
      "       63/1    0.83937    0.86185 +/- 0.00476\n",
      "       64/1    0.91057    0.86275 +/- 0.00476\n",
      "       65/1    0.90780    0.86357 +/- 0.00474\n",
      "       66/1    0.88181    0.86390 +/- 0.00467\n",
      "       67/1    0.86447    0.86391 +/- 0.00458\n",
      "       68/1    0.86618    0.86395 +/- 0.00450\n",
      "       69/1    0.79032    0.86270 +/- 0.00460\n",
      "       70/1    0.85570    0.86258 +/- 0.00452\n",
      "       71/1    0.85695    0.86249 +/- 0.00445\n",
      "       72/1    0.87981    0.86277 +/- 0.00439\n",
      "       73/1    0.82138    0.86211 +/- 0.00437\n",
      "       74/1    0.92151    0.86304 +/- 0.00440\n",
      "       75/1    0.84579    0.86278 +/- 0.00434\n",
      "       76/1    0.89389    0.86325 +/- 0.00430\n",
      "       77/1    0.84558    0.86298 +/- 0.00424\n",
      "       78/1    0.82290    0.86239 +/- 0.00422\n",
      "       79/1    0.95613    0.86375 +/- 0.00437\n",
      "       80/1    0.86835    0.86382 +/- 0.00431\n",
      "       81/1    0.84894    0.86361 +/- 0.00425\n",
      "       82/1    0.85451    0.86348 +/- 0.00420\n",
      "       83/1    0.85334    0.86334 +/- 0.00414\n",
      "       84/1    0.79849    0.86247 +/- 0.00418\n",
      "       85/1    0.84912    0.86229 +/- 0.00413\n",
      "       86/1    0.83408    0.86192 +/- 0.00409\n",
      "       87/1    0.88999    0.86228 +/- 0.00405\n",
      "       88/1    0.82774    0.86184 +/- 0.00402\n",
      "       89/1    0.84519    0.86163 +/- 0.00398\n",
      "       90/1    0.88805    0.86196 +/- 0.00394\n",
      "       91/1    0.87083    0.86207 +/- 0.00389\n",
      "       92/1    0.82218    0.86158 +/- 0.00388\n",
      "       93/1    0.87666    0.86176 +/- 0.00383\n",
      "       94/1    0.89480    0.86216 +/- 0.00381\n",
      "       95/1    0.84975    0.86201 +/- 0.00377\n",
      "       96/1    0.82337    0.86156 +/- 0.00375\n",
      "       97/1    0.79882    0.86084 +/- 0.00377\n",
      "       98/1    0.81644    0.86034 +/- 0.00377\n",
      "       99/1    0.87955    0.86055 +/- 0.00373\n",
      "      100/1    0.85891    0.86053 +/- 0.00369\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 4.7870e+00 seconds\n",
      "   Time in transport only          = 4.6013e+00 seconds\n",
      "   Time in inactive batches        = 2.7343e-01 seconds\n",
      "   Time in active batches          = 4.5136e+00 seconds\n",
      "   Time synchronizing fission bank = 1.0618e-02 seconds\n",
      "     Sampling source sites         = 8.8503e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4946e-03 seconds\n",
      "   Time accumulating tallies       = 1.6245e-01 seconds\n",
      "   Time writing statepoints        = 3.7253e-03 seconds\n",
      " Total time for finalization       = 7.9788e-05 seconds\n",
      " Total time elapsed                = 4.8100e+00 seconds\n",
      " Calculation Rate (inactive)       = 36572.8 particles/second\n",
      " Calculation Rate (active)         = 19939.8 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.85514 +/- 0.00316\n",
      " k-effective (Track-length)  = 0.86053 +/- 0.00369\n",
      " k-effective (Absorption)    = 0.85535 +/- 0.00326\n",
      " Combined k-effective        = 0.85638 +/- 0.00263\n",
      " Leakage Fraction            = 0.13937 +/- 0.00126\n",
      "\n",
      " Creating state point openmc_simulation_n4.h5...\n",
      "[openmc.deplete] t=432000.0 (final operator evaluation)\n",
      " Maximum neutron transport energy: 20000000 eV for F19\n",
      " Initializing source particles...\n",
      "\n",
      " ====================>     K EIGENVALUE SIMULATION     <====================\n",
      "\n",
      "  Bat./Gen.      k            Average k\n",
      "  =========   ========   ====================\n",
      "        1/1    0.52929\n",
      "        2/1    0.65018\n",
      "        3/1    0.79092\n",
      "        4/1    0.78805\n",
      "        5/1    0.85448\n",
      "        6/1    0.83576\n",
      "        7/1    0.83555\n",
      "        8/1    0.86517\n",
      "        9/1    0.81786\n",
      "       10/1    0.87969\n",
      "       11/1    0.87942\n",
      "       12/1    0.84904    0.86423 +/- 0.01519\n",
      "       13/1    0.80998    0.84615 +/- 0.02010\n",
      "       14/1    0.81959    0.83951 +/- 0.01569\n",
      "       15/1    0.88925    0.84946 +/- 0.01570\n",
      "       16/1    0.89167    0.85649 +/- 0.01463\n",
      "       17/1    0.86846    0.85820 +/- 0.01248\n",
      "       18/1    0.93765    0.86813 +/- 0.01468\n",
      "       19/1    0.88106    0.86957 +/- 0.01302\n",
      "       20/1    0.89128    0.87174 +/- 0.01185\n",
      "       21/1    0.88121    0.87260 +/- 0.01075\n",
      "       22/1    0.88452    0.87360 +/- 0.00987\n",
      "       23/1    0.82184    0.86961 +/- 0.00991\n",
      "       24/1    0.81971    0.86605 +/- 0.00984\n",
      "       25/1    0.83965    0.86429 +/- 0.00933\n",
      "       26/1    0.86634    0.86442 +/- 0.00873\n",
      "       27/1    0.81151    0.86131 +/- 0.00877\n",
      "       28/1    0.81254    0.85860 +/- 0.00870\n",
      "       29/1    0.91685    0.86166 +/- 0.00878\n",
      "       30/1    0.84178    0.86067 +/- 0.00839\n",
      "       31/1    0.83156    0.85928 +/- 0.00810\n",
      "       32/1    0.89961    0.86112 +/- 0.00794\n",
      "       33/1    0.84805    0.86055 +/- 0.00761\n",
      "       34/1    0.87475    0.86114 +/- 0.00731\n",
      "       35/1    0.85297    0.86081 +/- 0.00702\n",
      "       36/1    0.84896    0.86036 +/- 0.00676\n",
      "       37/1    0.84090    0.85964 +/- 0.00654\n",
      "       38/1    0.82969    0.85857 +/- 0.00639\n",
      "       39/1    0.78410    0.85600 +/- 0.00668\n",
      "       40/1    0.85758    0.85605 +/- 0.00646\n",
      "       41/1    0.86748    0.85642 +/- 0.00625\n",
      "       42/1    0.87658    0.85705 +/- 0.00609\n",
      "       43/1    0.86491    0.85729 +/- 0.00591\n",
      "       44/1    0.91856    0.85909 +/- 0.00601\n",
      "       45/1    0.83861    0.85851 +/- 0.00586\n",
      "       46/1    0.91179    0.85999 +/- 0.00589\n",
      "       47/1    0.94436    0.86227 +/- 0.00616\n",
      "       48/1    0.89727    0.86319 +/- 0.00607\n",
      "       49/1    0.83781    0.86254 +/- 0.00595\n",
      "       50/1    0.82844    0.86168 +/- 0.00586\n",
      "       51/1    0.89673    0.86254 +/- 0.00578\n",
      "       52/1    0.87875    0.86292 +/- 0.00565\n",
      "       53/1    0.87622    0.86323 +/- 0.00553\n",
      "       54/1    0.82034    0.86226 +/- 0.00549\n",
      "       55/1    0.86909    0.86241 +/- 0.00537\n",
      "       56/1    0.86387    0.86244 +/- 0.00525\n",
      "       57/1    0.91784    0.86362 +/- 0.00527\n",
      "       58/1    0.84622    0.86326 +/- 0.00517\n",
      "       59/1    0.80746    0.86212 +/- 0.00519\n",
      "       60/1    0.89928    0.86286 +/- 0.00514\n",
      "       61/1    0.88420    0.86328 +/- 0.00505\n",
      "       62/1    0.89694    0.86393 +/- 0.00500\n",
      "       63/1    0.84067    0.86349 +/- 0.00492\n",
      "       64/1    0.87897    0.86378 +/- 0.00484\n",
      "       65/1    0.87450    0.86397 +/- 0.00475\n",
      "       66/1    0.88888    0.86442 +/- 0.00469\n",
      "       67/1    0.86764    0.86447 +/- 0.00461\n",
      "       68/1    0.79939    0.86335 +/- 0.00466\n",
      "       69/1    0.88619    0.86374 +/- 0.00460\n",
      "       70/1    0.90379    0.86441 +/- 0.00457\n",
      "       71/1    0.88902    0.86481 +/- 0.00452\n",
      "       72/1    0.90760    0.86550 +/- 0.00449\n",
      "       73/1    0.81380    0.86468 +/- 0.00450\n",
      "       74/1    0.86162    0.86463 +/- 0.00443\n",
      "       75/1    0.91761    0.86545 +/- 0.00443\n",
      "       76/1    0.86718    0.86547 +/- 0.00437\n",
      "       77/1    0.84629    0.86519 +/- 0.00431\n",
      "       78/1    0.89843    0.86567 +/- 0.00428\n",
      "       79/1    0.91041    0.86632 +/- 0.00426\n",
      "       80/1    0.82745    0.86577 +/- 0.00424\n",
      "       81/1    0.84979    0.86554 +/- 0.00418\n",
      "       82/1    0.84725    0.86529 +/- 0.00413\n",
      "       83/1    0.84941    0.86507 +/- 0.00408\n",
      "       84/1    0.92326    0.86586 +/- 0.00410\n",
      "       85/1    0.79993    0.86498 +/- 0.00414\n",
      "       86/1    0.89054    0.86531 +/- 0.00410\n",
      "       87/1    0.84567    0.86506 +/- 0.00405\n",
      "       88/1    0.82389    0.86453 +/- 0.00404\n",
      "       89/1    0.82355    0.86401 +/- 0.00402\n",
      "       90/1    0.87340    0.86413 +/- 0.00397\n",
      "       91/1    0.84962    0.86395 +/- 0.00393\n",
      "       92/1    0.87283    0.86406 +/- 0.00388\n",
      "       93/1    0.87540    0.86420 +/- 0.00383\n",
      "       94/1    0.90460    0.86468 +/- 0.00382\n",
      "       95/1    0.88844    0.86496 +/- 0.00378\n",
      "       96/1    0.88484    0.86519 +/- 0.00375\n",
      "       97/1    0.89063    0.86548 +/- 0.00371\n",
      "       98/1    0.81006    0.86485 +/- 0.00373\n",
      "       99/1    0.78947    0.86400 +/- 0.00378\n",
      "      100/1    0.83465    0.86368 +/- 0.00375\n",
      " Creating state point statepoint.100.h5...\n",
      "\n",
      " =======================>     TIMING STATISTICS     <=======================\n",
      "\n",
      " Total time for initialization     = 0.0000e+00 seconds\n",
      "   Reading cross sections          = 0.0000e+00 seconds\n",
      " Total time in simulation          = 5.6781e+00 seconds\n",
      "   Time in transport only          = 5.4435e+00 seconds\n",
      "   Time in inactive batches        = 2.4367e-01 seconds\n",
      "   Time in active batches          = 5.4344e+00 seconds\n",
      "   Time synchronizing fission bank = 1.1002e-02 seconds\n",
      "     Sampling source sites         = 9.1709e-03 seconds\n",
      "     SEND/RECV source sites        = 1.4549e-03 seconds\n",
      "   Time accumulating tallies       = 2.0683e-01 seconds\n",
      "   Time writing statepoints        = 4.1388e-03 seconds\n",
      " Total time for finalization       = 8.8879e-05 seconds\n",
      " Total time elapsed                = 5.7012e+00 seconds\n",
      " Calculation Rate (inactive)       = 41038.8 particles/second\n",
      " Calculation Rate (active)         = 16561.2 particles/second\n",
      "\n",
      " ============================>     RESULTS     <============================\n",
      "\n",
      " k-effective (Collision)     = 0.86300 +/- 0.00365\n",
      " k-effective (Track-length)  = 0.86368 +/- 0.00375\n",
      " k-effective (Absorption)    = 0.85797 +/- 0.00360\n",
      " Combined k-effective        = 0.86060 +/- 0.00308\n",
      " Leakage Fraction            = 0.13613 +/- 0.00116\n",
      "\n",
      " Creating state point openmc_simulation_n5.h5...\n"
     ]
    }
   ],
   "source": [
    "# Transfer all elements from in-core to out-of-core and vice-versa\n",
    "all_elements = list(openmc.data.ELEMENT_SYMBOL.values())\n",
    "all_elements.remove('He') #still haven't figure out here\n",
    "flow_rate = 0.1 #litres/sec\n",
    "lambda_in = 1 / (uf4.volume / 1000 / flow_rate)\n",
    "lambda_out = 1 / (ofc_uf4.volume / 1000 / flow_rate)\n",
    "op = openmc.deplete.CoupledOperator(model, chain_file)\n",
    "integrator = openmc.deplete.PredictorIntegrator(op, time_steps, power, timestep_units='d')\n",
    "integrator.add_transfer_rate(uf4, all_elements, lambda_in, destination_material=ofc_uf4)\n",
    "integrator.add_transfer_rate(ofc_uf4, all_elements, lambda_out, destination_material=uf4)\n",
    "integrator.integrate()"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 12,
   "id": "728f9857",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    },
    {
     "data": {
      "image/png": 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",
      "text/plain": [
       "<Figure size 640x480 with 1 Axes>"
      ]
     },
     "metadata": {},
     "output_type": "display_data"
    }
   ],
   "source": [
    "res_lump = openmc.deplete.Results('depletion_results.h5')\n",
    "\n",
    "time, xe135_ref_c = res_ref.get_atoms(uf4, 'Xe135')\n",
    "_, xe135_ref_ofc = res_ref.get_atoms(ofc_uf4, 'Xe135')\n",
    "_, xe135_lump_c = res_lump.get_atoms(uf4, 'Xe135')\n",
    "_, xe135_lump_ofc = res_lump.get_atoms(ofc_uf4, 'Xe135')\n",
    "_, u235_ref_c = res_ref.get_atoms(uf4, 'U235')\n",
    "_, u235_ref_ofc = res_ref.get_atoms(ofc_uf4, 'U235')\n",
    "_, u235_lump_c = res_lump.get_atoms(uf4, 'U235')\n",
    "_, u235_lump_ofc = res_lump.get_atoms(ofc_uf4, 'U235')\n",
    "\n",
    "line1 = Line2D([0], [0], color='black')\n",
    "line2 = Line2D([0], [0], linestyle='--', color='black')\n",
    "line3 = Line2D([0], [0], color='r')\n",
    "line4 = Line2D([0], [0], color='g')\n",
    "labels1 = ['In core', 'ofc core']\n",
    "labels2 = ['w/o lump', 'w lump']\n",
    "fig, ax = plt.subplots()\n",
    "ax.plot(xe135_ref_c, color='r')\n",
    "ax.plot(xe135_ref_ofc, '--', color='r')\n",
    "ax.plot(xe135_lump_c, color='g')\n",
    "ax.plot(xe135_lump_ofc, '--', color='g')\n",
    "leg1=plt.legend([line1, line2],labels1,loc='lower center')\n",
    "leg2=plt.legend([line3, line4],labels2,loc='center right')\n",
    "ax.add_artist(leg1)\n",
    "ax.add_artist(leg2)\n",
    "ax.set_xlabel('Time [d]')\n",
    "ax.set_ylabel('Xe135 number of atoms')\n",
    "#ax.set_yscale('log')\n",
    "plt.show()\n",
    "\n",
    "line1 = Line2D([0], [0], color='black')\n",
    "line2 = Line2D([0], [0], linestyle='--', color='black')\n",
    "line3 = Line2D([0], [0], color='r')\n",
    "line4 = Line2D([0], [0], color='g')\n",
    "labels1 = ['In core', 'ofc core']\n",
    "labels2 = ['w/o lump', 'w lump']\n",
    "fig, ax = plt.subplots()\n",
    "ax.plot(u235_ref_c, color='r')\n",
    "ax.plot(u235_ref_ofc, '--', color='r')\n",
    "ax.plot(u235_lump_c, color='g')\n",
    "ax.plot(u235_lump_ofc, '--', color='g')\n",
    "leg1=plt.legend([line1, line2],labels1,loc='lower center')\n",
    "leg2=plt.legend([line3, line4],labels2,loc='center right')\n",
    "ax.add_artist(leg1)\n",
    "ax.add_artist(leg2)\n",
    "ax.set_xlabel('Time [d]')\n",
    "ax.set_ylabel('U235 number of atoms')\n",
    "ax.set_yscale('log')\n",
    "plt.show()"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "10340d1e-b8b8-42f3-9d09-05aa4e3573a0",
   "metadata": {},
   "source": [
    "As expected, in the lump case Xe135 starts accumulate early on in the out-of-core zone, due to the lower circulation time than in-core and no presence of neutron absorption reactions (decay-only region). \n",
    "On the other hand, U235 distribution between in-core and out-of-core is initially the same for the two cases and we start observing the small effect of fresh fissile being transferred from the out-of-core to the the in-core region in the lump case, only after 1 simulation day. "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": null,
   "id": "ea63a27e-4944-4419-ae31-9ff0d90c22db",
   "metadata": {},
   "outputs": [],
   "source": []
  }
 ],
 "metadata": {
  "kernelspec": {
   "display_name": "Python 3 (ipykernel)",
   "language": "python",
   "name": "python3"
  },
  "language_info": {
   "codemirror_mode": {
    "name": "ipython",
    "version": 3
   },
   "file_extension": ".py",
   "mimetype": "text/x-python",
   "name": "python",
   "nbconvert_exporter": "python",
   "pygments_lexer": "ipython3",
   "version": "3.10.12"
  }
 },
 "nbformat": 4,
 "nbformat_minor": 5
}