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{
"cells": [
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Pre-requisites\n",
"\n",
"This Notebook requires the following to be installed on one's machine:\n",
"\n",
"* **openmc**\n",
"* **beavrs**\n",
"\n",
"**NOTE**: You can install the `beavrs` Python module by running the following in the terminal:\n",
"\n",
"```\n",
"$ python setup.py install --user\n",
"```"
]
},
{
"cell_type": "code",
"execution_count": 1,
"metadata": {},
"outputs": [],
"source": [
"import openmc\n",
"import beavrs.builder\n",
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"from beavrs.constants import Constants\n",
"from IPython.display import Image\n",
"\n",
"c = Constants(150,0)"
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]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Create BEAVRS Model"
]
},
{
"cell_type": "code",
"execution_count": 2,
"metadata": {},
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"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
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"Cannot have a negative S position. S set to 0\n",
"Cannot have a negative SS position. SS set to 0\n",
" RCCA Positions\n",
" A: 228 B: 228 C: 228 D: 228\n",
" SA: 228 SB: 228 SC: 228 SD: 228 SE: 228\n"
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]
}
],
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"source": [
"# Instantiate a BEAVRS object from the mit-crpg/PWR_benchmarks repository\n",
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"b = beavrs.builder.BEAVRS(0)"
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]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"The BEAVRS model represented by variable `b` encapsulates the fully-detailed 3D BEAVRS core geometry and materials built using the OpenMC Python API."
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Create \"geometry.xml\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"We wish to extract a fuel pin from the BEAVRS `Geometry` object for our simulation."
]
},
{
"cell_type": "code",
"execution_count": 3,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# User-specified enrichment of 1.6, 2.4 or 3.1 percent\n",
"enrichment = 1.6"
]
},
{
"cell_type": "code",
"execution_count": 4,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Extract fuel pin of interest from BEAVRS model\n",
"pin_name = 'Fuel rod active region - {}% enr'.format(enrichment)\n",
"pin = b.openmc_geometry.get_universes_by_name(pin_name)[0]"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"We can inspect our chosen fuel pin using OpenMC's built-in string representation for the object:"
]
},
{
"cell_type": "code",
"execution_count": 5,
"metadata": {},
"outputs": [
{
"data": {
"text/plain": [
"Universe\n",
"\tID =\t8\n",
"\tName =\tFuel rod active region - 1.6% enr\n",
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"\tGeom =\tCSG\n",
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"\tCells =\t[52, 53, 54]"
]
},
"execution_count": 5,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"pin"
]
},
{
"cell_type": "code",
"execution_count": 6,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
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"{52: Cell\n",
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"\tID =\t52\n",
"\tName =\tFuel rod active region - 1.6% enr radial 0: Fuel 1.6%\n",
"\tFill =\tMaterial 9\n",
"\tRegion =\t-35\n",
"\tRotation =\tNone\n",
"\tTemperature =\tNone\n",
"\tTranslation =\tNone\n",
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"\tVolume =\tNone\n",
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", 53: Cell\n",
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"\tID =\t53\n",
"\tName =\tFuel rod active region - 1.6% enr radial 1: Helium\n",
"\tFill =\tMaterial 5\n",
"\tRegion =\t(35 -36)\n",
"\tRotation =\tNone\n",
"\tTemperature =\tNone\n",
"\tTranslation =\tNone\n",
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"\tVolume =\tNone\n",
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", 54: Cell\n",
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"\tID =\t54\n",
"\tName =\tFuel rod active region - 1.6% enr radial outer: Zircaloy 4\n",
"\tFill =\tMaterial 7\n",
"\tRegion =\t36\n",
"\tRotation =\tNone\n",
"\tTemperature =\tNone\n",
"\tTranslation =\tNone\n",
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"\tVolume =\tNone\n",
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"}\n"
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]
}
],
"source": [
"print(pin.cells)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"We need to wrap the fuel region with water to make a complete fuel pin:"
]
},
{
"cell_type": "code",
"execution_count": 7,
"metadata": {},
"outputs": [],
"source": [
"# Create surface as the boundary of clad and cell pitches\n",
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"fuel_clad_OR = openmc.ZCylinder(name='Fuel clad OR', r=c.cladOR)\n",
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"pin_sides = openmc.model.RectangularPrism(c.pinPitch, c.pinPitch,\n",
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" boundary_type='reflective')\n",
"# Create a cell filled by the fuel pin\n",
"fuel_cell = openmc.Cell(name='Fuel cell',\n",
" fill=pin,\n",
" region=-fuel_clad_OR\n",
" )\n",
"water_cell = openmc.Cell(name='Water',\n",
" fill=b.mats['Borated Water'],\n",
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" region=+fuel_clad_OR & -pin_sides\n",
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" )"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Then we construct a sub-geometry encapsulating only this fuel pin. We will do this by first creating a \"root\" universe and add our cells to it:"
]
},
{
"cell_type": "code",
"execution_count": 8,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Create a \"root\" universe with ID=0 and add the \"root\" cell to it\n",
"root_univ = openmc.Universe(name='root universe', cells=[fuel_cell, water_cell])"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Lastly, the \"root\" universe must be attached to a new OpenMC `Geometry` object representing this new sub-geometry:"
]
},
{
"cell_type": "code",
"execution_count": 9,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Create an OpenMC Geometry around root Universe\n",
"sub_geometry = openmc.Geometry(root_univ)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Finally, we are ready to create a \"geometry.xml\" input file for OpenMC! We simply export it to XML as follows:"
]
},
{
"cell_type": "code",
"execution_count": 10,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Export the OpenMC Geometry to a \"geometry.xml\" file\n",
"sub_geometry.export_to_xml()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Create \"materials.xml\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Now we need to create materials for our geometry. This is very easy to do with the `b.write_openmc_materials()` routine. The one disadvantage of this is that it will write *all* materials for the entire BEAVRS geometry to a \"materials.xml\" file, most of which are not used in our sub-geometry for a single fuel pin. Instead, we can write out only those materials that are in our geometry as follows:"
]
},
{
"cell_type": "code",
"execution_count": 11,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Get a list of all OpenMC Materials\n",
"all_materials = sub_geometry.get_all_materials()\n",
"\n",
"# Create a MaterialsFile object\n",
"materials = openmc.Materials(all_materials.values())\n",
"\n",
"# Export the OpenMC Materials to a \"materials.xml\" file\n",
"materials.export_to_xml()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Create \"settings.xml\" "
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Now for the easy part :-) Let's create a \"settings.xml\" file:"
]
},
{
"cell_type": "code",
"execution_count": 12,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Create a MaterialsFile object\n",
"settings = openmc.Settings()\n",
"\n",
"# Set any settings of interest\n",
"settings.batches = 150\n",
"settings.inactive = 10\n",
"settings.particles = 1000\n",
"\n",
"# Use a bounding box to define the starting source distribution\n",
"lower_left = [c.pinPitch/2, c.pinPitch/2, c.fuel_ActiveFuel_bot]\n",
"upper_right = [c.pinPitch/2, c.pinPitch/2, c.fuel_ActiveFuel_top]\n",
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"settings.source = openmc.source.IndependentSource(space=openmc.stats.Point((0, 0, 0)))\n",
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"\n",
"# Export the settings to a \"settings.xml\" file\n",
"settings.export_to_xml()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Create \"plots.xml\""
]
},
{
"cell_type": "code",
"execution_count": 13,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Create a single plot using default paramters (basis='xy', origin=(0,0,0))\n",
"plot = openmc.Plot(plot_id=1)\n",
"plot.width = [c.pinPitch, c.pinPitch]\n",
"\n",
"# Create a PlotsFile object and add our plot to it\n",
"plot_file = openmc.Plots([plot])\n",
"\n",
"# Export the plots to a \"plots.xml\" file\n",
"plot_file.export_to_xml()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"With the \"plots.xml\" file, we can now generate and view the plot. We must first instantiate an `openmc.Executor` object and then ask it to plot the geometry(equivalent to running `openmc -p` from within the terminal)."
]
},
{
"cell_type": "code",
"execution_count": 14,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Run openmc in plotting mode\n",
"openmc.plot_geometry(output=False)"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"OpenMC outputs plots in .ppm format, which can be converted into a compressed format like .png with the convert utility. We can view the .png image inline using the `IPython.display.Image` class as follows:"
]
},
{
"cell_type": "code",
"execution_count": 15,
"metadata": {},
"outputs": [
{
"data": {
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"image/png": "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"text/plain": [
"<IPython.core.display.Image object>"
]
},
"execution_count": 15,
"metadata": {
"image/png": {
"height": 250,
"width": 250
}
},
"output_type": "execute_result"
}
],
"source": [
"# Display the plot inline\n",
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"Image(filename='plot_1.png', width=250, height=250)"
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]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Create \"tallies.xml\""
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Perhaps you'd like a tally in one of the cells. First, we need to extract the cell(s) of interest:"
]
},
{
"cell_type": "code",
"execution_count": 16,
"metadata": {},
"outputs": [],
"source": [
"all_material_cells = sub_geometry.get_all_material_cells()\n",
"\n",
"cell_name = 'Fuel rod active region - 1.6% enr radial 0: Fuel 1.6%'\n",
"for id, cell in all_material_cells.items():\n",
" if cell.name == cell_name:\n",
" my_cell = cell"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Let's tally the fast/thermal scatter and absorption rates for all nuclides in our cell. We create a `Tally` to do so as follows:"
]
},
{
"cell_type": "code",
"execution_count": 17,
"metadata": {},
"outputs": [],
"source": [
"# Instantiate a really cool tally\n",
"tally = openmc.Tally(name='a really cool tally')\n",
"\n",
"# Instantiate a cell filter\n",
"cell_filter = openmc.CellFilter(bins=[my_cell.id])\n",
"\n",
"# Instantiate energy filter\n",
"energy_filter = openmc.EnergyFilter([0., 0.625e-6, 20.])\n",
"\n",
"tally.filters = [cell_filter, energy_filter]\n",
"\n",
"# Add the scores of interest to the tally\n",
"tally.scores = ['scatter', 'absorption']\n",
"\n",
"# Add all nuclides to the tally for kicks\n",
"tally.nuclides = my_cell.fill.get_nuclides()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"Next, we simply need to add our `Tally` object(s) to a `TalliesFile` object and export them to a \"tallies.xml\" file:"
]
},
{
"cell_type": "code",
"execution_count": 18,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Instantiate an empty TalliesFile\n",
"tallies_file = openmc.Tallies()\n",
"\n",
"# Add our tally(ies) to the file\n",
"tallies_file.append(tally)\n",
"\n",
"# Export the tallies to a \"tallies.xml\" file\n",
"tallies_file.export_to_xml()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Run OpenMC!"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"We can run OpenMC from within the notebook if we wish. Wow, isn't this so much more powerful than ASCII!"
]
},
{
"cell_type": "code",
"execution_count": 19,
"metadata": {},
"outputs": [
{
"name": "stdout",
"output_type": "stream",
"text": [
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" %%%%%%%%%%%%%%%\n",
" %%%%%%%%%%%%%%%%%%%%%%%%\n",
" %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
" %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
" %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
" %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%\n",
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" %%%%%%%%%%%%%%%%%%%%%%%%\n",
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" %%%%%%%%%%%%%%%%%%%%%%%%\n",
" ############### %%%%%%%%%%%%%%%%%%%%%%%%\n",
" ################## %%%%%%%%%%%%%%%%%%%%%%%\n",
" ################### %%%%%%%%%%%%%%%%%%%%%%%\n",
" #################### %%%%%%%%%%%%%%%%%%%%%%\n",
" ##################### %%%%%%%%%%%%%%%%%%%%%\n",
" ###################### %%%%%%%%%%%%%%%%%%%%\n",
" ####################### %%%%%%%%%%%%%%%%%%\n",
" ####################### %%%%%%%%%%%%%%%%%\n",
" ###################### %%%%%%%%%%%%%%%%%\n",
" #################### %%%%%%%%%%%%%%%%%\n",
" ################# %%%%%%%%%%%%%%%%%\n",
" ############### %%%%%%%%%%%%%%%%\n",
" ############ %%%%%%%%%%%%%%%\n",
" ######## %%%%%%%%%%%%%%\n",
" %%%%%%%%%%%\n",
2018-08-29 08:31:36 -07:00
"\n",
2023-11-16 00:11:41 -08:00
" | The OpenMC Monte Carlo Code\n",
" Copyright | 2011-2023 MIT, UChicago Argonne LLC, and contributors\n",
" License | https://docs.openmc.org/en/latest/license.html\n",
2024-02-02 01:06:22 -08:00
" Version | 0.14.0\n",
" Git SHA1 | e1a8ee7794b441c992426f17fafe216391cbba83\n",
" Date/Time | 2024-02-02 00:48:52\n",
" MPI Processes | 2\n",
" OpenMP Threads | 2\n",
2018-08-29 08:31:36 -07:00
"\n",
" Reading settings XML file...\n",
" Reading cross sections XML file...\n",
" Reading materials XML file...\n",
" Reading geometry XML file...\n",
2023-11-16 00:11:41 -08:00
" Reading He3 from /opt/xdata/endfb-vii.1-hdf5/neutron/He3.h5\n",
" Reading He4 from /opt/xdata/endfb-vii.1-hdf5/neutron/He4.h5\n",
" Reading O16 from /opt/xdata/endfb-vii.1-hdf5/neutron/O16.h5\n",
" Reading O17 from /opt/xdata/endfb-vii.1-hdf5/neutron/O17.h5\n",
" Reading Cr50 from /opt/xdata/endfb-vii.1-hdf5/neutron/Cr50.h5\n",
" Reading Cr52 from /opt/xdata/endfb-vii.1-hdf5/neutron/Cr52.h5\n",
" Reading Cr53 from /opt/xdata/endfb-vii.1-hdf5/neutron/Cr53.h5\n",
" Reading Cr54 from /opt/xdata/endfb-vii.1-hdf5/neutron/Cr54.h5\n",
" Reading Fe54 from /opt/xdata/endfb-vii.1-hdf5/neutron/Fe54.h5\n",
" Reading Fe56 from /opt/xdata/endfb-vii.1-hdf5/neutron/Fe56.h5\n",
" Reading Fe57 from /opt/xdata/endfb-vii.1-hdf5/neutron/Fe57.h5\n",
" Reading Fe58 from /opt/xdata/endfb-vii.1-hdf5/neutron/Fe58.h5\n",
" Reading Zr90 from /opt/xdata/endfb-vii.1-hdf5/neutron/Zr90.h5\n",
" Reading Zr91 from /opt/xdata/endfb-vii.1-hdf5/neutron/Zr91.h5\n",
" Reading Zr92 from /opt/xdata/endfb-vii.1-hdf5/neutron/Zr92.h5\n",
" Reading Zr94 from /opt/xdata/endfb-vii.1-hdf5/neutron/Zr94.h5\n",
" Reading Zr96 from /opt/xdata/endfb-vii.1-hdf5/neutron/Zr96.h5\n",
" Reading Sn112 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn112.h5\n",
" Reading Sn114 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn114.h5\n",
" Reading Sn115 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn115.h5\n",
" Reading Sn116 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn116.h5\n",
" Reading Sn117 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn117.h5\n",
" Reading Sn118 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn118.h5\n",
" Reading Sn119 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn119.h5\n",
" Reading Sn120 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn120.h5\n",
" Reading Sn122 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn122.h5\n",
" Reading Sn124 from /opt/xdata/endfb-vii.1-hdf5/neutron/Sn124.h5\n",
" Reading U234 from /opt/xdata/endfb-vii.1-hdf5/neutron/U234.h5\n",
" Reading U235 from /opt/xdata/endfb-vii.1-hdf5/neutron/U235.h5\n",
" Reading U238 from /opt/xdata/endfb-vii.1-hdf5/neutron/U238.h5\n",
" Reading U236 from /opt/xdata/endfb-vii.1-hdf5/neutron/U236.h5\n",
" Reading B10 from /opt/xdata/endfb-vii.1-hdf5/neutron/B10.h5\n",
" Reading B11 from /opt/xdata/endfb-vii.1-hdf5/neutron/B11.h5\n",
" Reading H1 from /opt/xdata/endfb-vii.1-hdf5/neutron/H1.h5\n",
" Reading H2 from /opt/xdata/endfb-vii.1-hdf5/neutron/H2.h5\n",
" Reading c_H_in_H2O from /opt/xdata/endfb-vii.1-hdf5/neutron/c_H_in_H2O.h5\n",
" Minimum neutron data temperature: 294 K\n",
" Maximum neutron data temperature: 294 K\n",
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" Reading tallies XML file...\n",
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" Preparing distributed cell instances...\n",
" Reading plot XML file...\n",
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" Writing summary.h5 file...\n",
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" Maximum neutron transport energy: 20000000 eV for He3\n",
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" Initializing source particles...\n",
"\n",
" ====================> K EIGENVALUE SIMULATION <====================\n",
"\n",
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" Bat./Gen. k Average k\n",
" ========= ======== ====================\n",
" 1/1 1.02645\n",
" 2/1 0.99765\n",
" 3/1 1.01443\n",
" 4/1 0.99315\n",
" 5/1 1.00349\n",
" 6/1 1.04760\n",
" 7/1 0.97568\n",
" 8/1 1.01985\n",
" 9/1 1.02142\n",
" 10/1 1.06754\n",
" 11/1 1.00976\n",
" 12/1 1.01636 1.01306 +/- 0.00330\n",
" 13/1 0.99644 1.00752 +/- 0.00586\n",
" 14/1 1.06645 1.02225 +/- 0.01530\n",
" 15/1 0.96294 1.01039 +/- 0.01677\n",
" 16/1 1.01583 1.01130 +/- 0.01372\n",
" 17/1 1.00515 1.01042 +/- 0.01163\n",
" 18/1 1.00582 1.00984 +/- 0.01009\n",
" 19/1 1.04966 1.01427 +/- 0.00994\n",
" 20/1 0.99010 1.01185 +/- 0.00921\n",
" 21/1 1.02895 1.01341 +/- 0.00848\n",
" 22/1 1.03273 1.01502 +/- 0.00790\n",
" 23/1 1.00194 1.01401 +/- 0.00734\n",
" 24/1 1.05051 1.01662 +/- 0.00728\n",
" 25/1 1.06279 1.01970 +/- 0.00744\n",
" 26/1 1.03726 1.02079 +/- 0.00705\n",
" 27/1 1.02463 1.02102 +/- 0.00662\n",
" 28/1 1.03113 1.02158 +/- 0.00627\n",
" 29/1 1.03525 1.02230 +/- 0.00597\n",
" 30/1 1.00092 1.02123 +/- 0.00577\n",
" 31/1 1.06995 1.02355 +/- 0.00596\n",
" 32/1 1.02330 1.02354 +/- 0.00568\n",
" 33/1 1.05108 1.02474 +/- 0.00556\n",
" 34/1 1.03009 1.02496 +/- 0.00533\n",
" 35/1 1.02828 1.02509 +/- 0.00511\n",
" 36/1 1.07762 1.02711 +/- 0.00531\n",
" 37/1 1.01539 1.02668 +/- 0.00513\n",
" 38/1 1.03572 1.02700 +/- 0.00495\n",
" 39/1 1.01042 1.02643 +/- 0.00481\n",
" 40/1 1.03149 1.02660 +/- 0.00465\n",
" 41/1 0.99594 1.02561 +/- 0.00461\n",
" 42/1 1.04728 1.02629 +/- 0.00451\n",
" 43/1 1.05021 1.02701 +/- 0.00443\n",
" 44/1 1.13894 1.03030 +/- 0.00541\n",
" 45/1 1.02891 1.03026 +/- 0.00526\n",
" 46/1 0.95904 1.02829 +/- 0.00548\n",
" 47/1 1.02866 1.02830 +/- 0.00533\n",
" 48/1 1.01773 1.02802 +/- 0.00519\n",
" 49/1 1.00524 1.02743 +/- 0.00509\n",
" 50/1 1.06765 1.02844 +/- 0.00507\n",
" 51/1 1.02869 1.02845 +/- 0.00494\n",
" 52/1 0.98567 1.02743 +/- 0.00493\n",
" 53/1 1.04195 1.02777 +/- 0.00482\n",
" 54/1 0.98990 1.02690 +/- 0.00479\n",
" 55/1 1.05027 1.02742 +/- 0.00471\n",
" 56/1 1.01671 1.02719 +/- 0.00461\n",
" 57/1 1.01896 1.02702 +/- 0.00452\n",
" 58/1 1.02964 1.02707 +/- 0.00442\n",
" 59/1 1.06027 1.02775 +/- 0.00438\n",
" 60/1 0.94151 1.02602 +/- 0.00463\n",
" 61/1 1.04427 1.02638 +/- 0.00455\n",
" 62/1 1.00755 1.02602 +/- 0.00448\n",
" 63/1 1.03042 1.02610 +/- 0.00439\n",
" 64/1 1.06065 1.02674 +/- 0.00436\n",
" 65/1 1.09489 1.02798 +/- 0.00445\n",
" 66/1 0.94093 1.02643 +/- 0.00464\n",
" 67/1 1.02360 1.02638 +/- 0.00456\n",
" 68/1 1.05913 1.02694 +/- 0.00452\n",
" 69/1 1.03014 1.02700 +/- 0.00444\n",
" 70/1 1.06483 1.02763 +/- 0.00441\n",
" 71/1 1.06306 1.02821 +/- 0.00438\n",
" 72/1 0.95143 1.02697 +/- 0.00448\n",
" 73/1 1.02068 1.02687 +/- 0.00441\n",
" 74/1 0.99676 1.02640 +/- 0.00436\n",
" 75/1 1.05533 1.02684 +/- 0.00432\n",
" 76/1 0.97821 1.02611 +/- 0.00432\n",
" 77/1 1.10001 1.02721 +/- 0.00439\n",
" 78/1 1.01191 1.02698 +/- 0.00433\n",
" 79/1 1.07679 1.02771 +/- 0.00433\n",
" 80/1 0.99926 1.02730 +/- 0.00429\n",
" 81/1 1.01963 1.02719 +/- 0.00423\n",
" 82/1 1.03189 1.02726 +/- 0.00417\n",
" 83/1 1.04160 1.02745 +/- 0.00412\n",
" 84/1 1.00441 1.02714 +/- 0.00407\n",
" 85/1 0.97796 1.02649 +/- 0.00407\n",
" 86/1 0.97930 1.02587 +/- 0.00407\n",
" 87/1 1.01974 1.02579 +/- 0.00401\n",
" 88/1 1.07295 1.02639 +/- 0.00401\n",
" 89/1 1.04861 1.02667 +/- 0.00397\n",
" 90/1 1.03532 1.02678 +/- 0.00392\n",
" 91/1 0.97870 1.02619 +/- 0.00391\n",
" 92/1 1.00144 1.02588 +/- 0.00388\n",
" 93/1 1.03796 1.02603 +/- 0.00383\n",
" 94/1 1.00525 1.02578 +/- 0.00380\n",
" 95/1 1.04720 1.02603 +/- 0.00376\n",
" 96/1 1.02944 1.02607 +/- 0.00372\n",
" 97/1 1.07814 1.02667 +/- 0.00372\n",
" 98/1 0.98386 1.02619 +/- 0.00371\n",
" 99/1 0.99942 1.02589 +/- 0.00368\n",
" 100/1 1.06482 1.02632 +/- 0.00367\n",
" 101/1 1.05862 1.02667 +/- 0.00364\n",
" 102/1 1.02241 1.02663 +/- 0.00360\n",
" 103/1 1.03319 1.02670 +/- 0.00356\n",
" 104/1 1.06903 1.02715 +/- 0.00356\n",
" 105/1 1.05246 1.02741 +/- 0.00353\n",
" 106/1 1.00136 1.02714 +/- 0.00350\n",
" 107/1 1.05601 1.02744 +/- 0.00348\n",
" 108/1 0.96755 1.02683 +/- 0.00350\n",
" 109/1 1.06354 1.02720 +/- 0.00348\n",
" 110/1 1.06919 1.02762 +/- 0.00347\n",
" 111/1 1.04993 1.02784 +/- 0.00344\n",
" 112/1 1.08810 1.02843 +/- 0.00346\n",
" 113/1 1.05241 1.02866 +/- 0.00343\n",
" 114/1 0.97746 1.02817 +/- 0.00344\n",
" 115/1 0.98790 1.02779 +/- 0.00343\n",
" 116/1 1.08795 1.02836 +/- 0.00344\n",
" 117/1 1.02201 1.02830 +/- 0.00341\n",
" 118/1 0.97152 1.02777 +/- 0.00342\n",
" 119/1 0.98537 1.02738 +/- 0.00341\n",
" 120/1 1.03938 1.02749 +/- 0.00338\n",
" 121/1 1.02718 1.02749 +/- 0.00335\n",
" 122/1 1.03585 1.02756 +/- 0.00332\n",
" 123/1 1.02970 1.02758 +/- 0.00329\n",
" 124/1 1.05110 1.02779 +/- 0.00327\n",
" 125/1 0.96037 1.02720 +/- 0.00329\n",
" 126/1 0.97982 1.02679 +/- 0.00329\n",
" 127/1 1.06303 1.02710 +/- 0.00327\n",
" 128/1 1.06496 1.02742 +/- 0.00326\n",
" 129/1 1.07217 1.02780 +/- 0.00326\n",
" 130/1 1.06084 1.02808 +/- 0.00324\n",
" 131/1 1.03487 1.02813 +/- 0.00321\n",
" 132/1 0.97656 1.02771 +/- 0.00322\n",
" 133/1 1.00767 1.02755 +/- 0.00319\n",
" 134/1 0.98553 1.02721 +/- 0.00319\n",
" 135/1 1.00056 1.02699 +/- 0.00317\n",
" 136/1 1.04770 1.02716 +/- 0.00315\n",
" 137/1 1.00243 1.02696 +/- 0.00313\n",
" 138/1 1.04823 1.02713 +/- 0.00311\n",
" 139/1 0.96607 1.02666 +/- 0.00312\n",
" 140/1 1.05028 1.02684 +/- 0.00310\n",
" 141/1 1.02018 1.02679 +/- 0.00308\n",
" 142/1 1.05010 1.02696 +/- 0.00306\n",
" 143/1 0.94602 1.02635 +/- 0.00310\n",
" 144/1 0.99193 1.02610 +/- 0.00308\n",
" 145/1 1.08497 1.02653 +/- 0.00309\n",
" 146/1 1.08954 1.02700 +/- 0.00310\n",
" 147/1 1.01307 1.02690 +/- 0.00308\n",
" 148/1 1.05130 1.02707 +/- 0.00307\n",
" 149/1 0.96176 1.02660 +/- 0.00308\n",
" 150/1 1.06671 1.02689 +/- 0.00307\n",
2018-08-29 08:31:36 -07:00
" Creating state point statepoint.150.h5...\n",
"\n",
" =======================> TIMING STATISTICS <=======================\n",
"\n",
2024-02-02 01:06:22 -08:00
" Total time for initialization = 2.3583e+00 seconds\n",
" Reading cross sections = 2.3309e+00 seconds\n",
" Total time in simulation = 1.0739e+01 seconds\n",
" Time in transport only = 1.0461e+01 seconds\n",
" Time in inactive batches = 6.4227e-01 seconds\n",
" Time in active batches = 1.0096e+01 seconds\n",
" Time synchronizing fission bank = 2.4140e-01 seconds\n",
" Sampling source sites = 6.2924e-03 seconds\n",
" SEND/RECV source sites = 1.6094e-03 seconds\n",
" Time accumulating tallies = 1.4377e-02 seconds\n",
" Time writing statepoints = 9.8511e-03 seconds\n",
" Total time for finalization = 1.9690e-04 seconds\n",
" Total time elapsed = 1.3108e+01 seconds\n",
" Calculation Rate (inactive) = 15569.8 particles/second\n",
" Calculation Rate (active) = 13866.5 particles/second\n",
2018-08-29 08:31:36 -07:00
"\n",
" ============================> RESULTS <============================\n",
"\n",
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" k-effective (Collision) = 1.03023 +/- 0.00292\n",
" k-effective (Track-length) = 1.02689 +/- 0.00307\n",
" k-effective (Absorption) = 1.03192 +/- 0.00284\n",
" Combined k-effective = 1.03033 +/- 0.00237\n",
" Leakage Fraction = 0.00000 +/- 0.00000\n",
2018-08-29 08:31:36 -07:00
"\n"
]
}
],
"source": [
"# Run OpenMC with 2 MPI processes\n",
2024-02-02 01:06:22 -08:00
"openmc.run(mpi_args=['mpiexec', '-n', '2'], threads=2)"
2018-08-29 08:31:36 -07:00
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"## Analyze Tally Data"
]
},
{
"cell_type": "code",
"execution_count": 20,
"metadata": {
"collapsed": true
},
"outputs": [],
"source": [
"# Instantiate a StatePoint object\n",
"from openmc.statepoint import StatePoint\n",
"filename = 'statepoint.{}.h5'.format(settings.batches)\n",
"sp = StatePoint(filename)"
]
},
{
"cell_type": "code",
"execution_count": 21,
"metadata": {},
"outputs": [
{
"data": {
"text/plain": [
"{1: Tally\n",
" \tID =\t1\n",
" \tName =\ta really cool tally\n",
" \tFilters =\tCellFilter, EnergyFilter\n",
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" \tNuclides =\tO16 O17 U234 U235 U238 U236\n",
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" \tScores =\t['scatter', 'absorption']\n",
2024-02-02 01:06:22 -08:00
" \tEstimator =\ttracklength\n",
" \tMultiply dens. =\tTrue}"
2018-08-29 08:31:36 -07:00
]
},
"execution_count": 21,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"# Inspect the StatePoint's tallies\n",
"sp.tallies"
]
},
{
"cell_type": "code",
"execution_count": 22,
"metadata": {},
"outputs": [
{
"data": {
"text/html": [
"<div>\n",
"<style scoped>\n",
" .dataframe tbody tr th:only-of-type {\n",
" vertical-align: middle;\n",
" }\n",
"\n",
" .dataframe tbody tr th {\n",
" vertical-align: top;\n",
" }\n",
"\n",
" .dataframe thead th {\n",
" text-align: right;\n",
" }\n",
"</style>\n",
"<table border=\"1\" class=\"dataframe\">\n",
" <thead>\n",
" <tr style=\"text-align: right;\">\n",
" <th></th>\n",
" <th>cell</th>\n",
" <th>energy low [eV]</th>\n",
" <th>energy high [eV]</th>\n",
" <th>nuclide</th>\n",
" <th>score</th>\n",
" <th>mean</th>\n",
" <th>std. dev.</th>\n",
" </tr>\n",
" </thead>\n",
" <tbody>\n",
" <tr>\n",
" <th>0</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>O16</td>\n",
" <td>scatter</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>1</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>O16</td>\n",
" <td>absorption</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>2</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>O17</td>\n",
" <td>scatter</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>3</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>O17</td>\n",
" <td>absorption</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>4</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U234</td>\n",
" <td>scatter</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>5</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U234</td>\n",
" <td>absorption</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>6</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U235</td>\n",
" <td>scatter</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>7</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U235</td>\n",
" <td>absorption</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>8</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U238</td>\n",
" <td>scatter</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>9</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U238</td>\n",
" <td>absorption</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>10</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U236</td>\n",
" <td>scatter</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>11</th>\n",
" <td>52</td>\n",
" <td>0.000000e+00</td>\n",
" <td>6.250000e-07</td>\n",
" <td>U236</td>\n",
" <td>absorption</td>\n",
" <td>0.000000</td>\n",
" <td>0.000000e+00</td>\n",
" </tr>\n",
" <tr>\n",
" <th>12</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>O16</td>\n",
" <td>scatter</td>\n",
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" <td>0.672540</td>\n",
" <td>1.885498e-03</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>13</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>O16</td>\n",
" <td>absorption</td>\n",
" <td>0.000016</td>\n",
2023-11-16 00:11:41 -08:00
" <td>5.425475e-08</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>14</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>O17</td>\n",
" <td>scatter</td>\n",
" <td>0.000247</td>\n",
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" <td>6.935285e-07</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>15</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>O17</td>\n",
" <td>absorption</td>\n",
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" <td>0.000008</td>\n",
" <td>2.583810e-08</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>16</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U234</td>\n",
" <td>scatter</td>\n",
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" <td>0.000259</td>\n",
" <td>2.090607e-06</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>17</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U234</td>\n",
" <td>absorption</td>\n",
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" <td>0.001129</td>\n",
" <td>1.535991e-05</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>18</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U235</td>\n",
" <td>scatter</td>\n",
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" <td>0.019562</td>\n",
" <td>5.609057e-05</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>19</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U235</td>\n",
" <td>absorption</td>\n",
2023-11-16 00:11:41 -08:00
" <td>0.436195</td>\n",
" <td>1.511962e-03</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>20</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U238</td>\n",
" <td>scatter</td>\n",
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" <td>0.773617</td>\n",
" <td>2.185517e-03</td>\n",
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" </tr>\n",
" <tr>\n",
" <th>21</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U238</td>\n",
" <td>absorption</td>\n",
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" <td>0.164795</td>\n",
" <td>7.169391e-04</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>22</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U236</td>\n",
" <td>scatter</td>\n",
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" <td>0.000070</td>\n",
" <td>4.220446e-07</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" <tr>\n",
" <th>23</th>\n",
" <td>52</td>\n",
" <td>6.250000e-07</td>\n",
" <td>2.000000e+01</td>\n",
" <td>U236</td>\n",
" <td>absorption</td>\n",
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" <td>0.000166</td>\n",
" <td>4.473711e-06</td>\n",
2018-08-29 08:31:36 -07:00
" </tr>\n",
" </tbody>\n",
"</table>\n",
"</div>"
],
"text/plain": [
" cell energy low [eV] energy high [eV] nuclide score mean \\\n",
"0 52 0.00e+00 6.25e-07 O16 scatter 0.00e+00 \n",
"1 52 0.00e+00 6.25e-07 O16 absorption 0.00e+00 \n",
"2 52 0.00e+00 6.25e-07 O17 scatter 0.00e+00 \n",
"3 52 0.00e+00 6.25e-07 O17 absorption 0.00e+00 \n",
"4 52 0.00e+00 6.25e-07 U234 scatter 0.00e+00 \n",
"5 52 0.00e+00 6.25e-07 U234 absorption 0.00e+00 \n",
"6 52 0.00e+00 6.25e-07 U235 scatter 0.00e+00 \n",
"7 52 0.00e+00 6.25e-07 U235 absorption 0.00e+00 \n",
"8 52 0.00e+00 6.25e-07 U238 scatter 0.00e+00 \n",
"9 52 0.00e+00 6.25e-07 U238 absorption 0.00e+00 \n",
"10 52 0.00e+00 6.25e-07 U236 scatter 0.00e+00 \n",
"11 52 0.00e+00 6.25e-07 U236 absorption 0.00e+00 \n",
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"12 52 6.25e-07 2.00e+01 O16 scatter 6.73e-01 \n",
"13 52 6.25e-07 2.00e+01 O16 absorption 1.58e-05 \n",
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"14 52 6.25e-07 2.00e+01 O17 scatter 2.47e-04 \n",
2023-11-16 00:11:41 -08:00
"15 52 6.25e-07 2.00e+01 O17 absorption 7.50e-06 \n",
"16 52 6.25e-07 2.00e+01 U234 scatter 2.59e-04 \n",
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"17 52 6.25e-07 2.00e+01 U234 absorption 1.13e-03 \n",
2023-11-16 00:11:41 -08:00
"18 52 6.25e-07 2.00e+01 U235 scatter 1.96e-02 \n",
"19 52 6.25e-07 2.00e+01 U235 absorption 4.36e-01 \n",
"20 52 6.25e-07 2.00e+01 U238 scatter 7.74e-01 \n",
"21 52 6.25e-07 2.00e+01 U238 absorption 1.65e-01 \n",
"22 52 6.25e-07 2.00e+01 U236 scatter 6.99e-05 \n",
"23 52 6.25e-07 2.00e+01 U236 absorption 1.66e-04 \n",
2018-08-29 08:31:36 -07:00
"\n",
" std. dev. \n",
"0 0.00e+00 \n",
"1 0.00e+00 \n",
"2 0.00e+00 \n",
"3 0.00e+00 \n",
"4 0.00e+00 \n",
"5 0.00e+00 \n",
"6 0.00e+00 \n",
"7 0.00e+00 \n",
"8 0.00e+00 \n",
"9 0.00e+00 \n",
"10 0.00e+00 \n",
"11 0.00e+00 \n",
2023-11-16 00:11:41 -08:00
"12 1.89e-03 \n",
"13 5.43e-08 \n",
"14 6.94e-07 \n",
"15 2.58e-08 \n",
"16 2.09e-06 \n",
"17 1.54e-05 \n",
"18 5.61e-05 \n",
"19 1.51e-03 \n",
"20 2.19e-03 \n",
"21 7.17e-04 \n",
"22 4.22e-07 \n",
"23 4.47e-06 "
2018-08-29 08:31:36 -07:00
]
},
"execution_count": 22,
"metadata": {},
"output_type": "execute_result"
}
],
"source": [
"# Get a Pandas DataFrame of the tally data\n",
"tally = sp.get_tally(name='a really cool tally')\n",
"tally.get_pandas_dataframe()"
]
},
{
"cell_type": "markdown",
"metadata": {},
"source": [
"And I'll leave it up to you at this point :-)"
]
}
],
"metadata": {
"kernelspec": {
"display_name": "Python 3",
"language": "python",
"name": "python3"
},
"language_info": {
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"name": "ipython",
"version": 3
},
"file_extension": ".py",
"mimetype": "text/x-python",
"name": "python",
"nbconvert_exporter": "python",
"pygments_lexer": "ipython3",
2024-02-02 01:06:22 -08:00
"version": "3.12.1"
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