Difference between revisions of "MCNP Sim of Jack Converter"
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==Photon energy spectra from 42 MeV electrons== | ==Photon energy spectra from 42 MeV electrons== | ||
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[[File:42MeVJack photons.png | 1000 px]] | [[File:42MeVJack photons.png | 1000 px]] | ||
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+ | ==Misc== | ||
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+ | Below is a plot of the rate of neutron production as the beam traverses through the converter. Zero corresponds to where the beam enters the titanium window. | ||
+ | [[File:JackConverterNeutronProduction.png| 600 px]] |
Revision as of 20:43, 5 September 2018
Simulation inputs
MCNP input deck: File:MCNP Jack Converter.txt.
The cross-section plots below show that the vast majority photo-neutrons are produced by (G,n) on Tungsten-184.
Geometry
Materials legend for figures:
.
Assumptions
The beam spot size was given a diameter of 0.5 based off of the size of a burn mark on a converter that got hot during irradiation. Electrons are mono energetic.
Results
The plots below show the energy distribution for neutrons exiting the converter at three different intervals of their angle w.r.t. the incident electron beam. The neutron energy spectrum of the neutron-induced fission of U235 is also in each shown for comparison.
The mean and median energy of fission neutrons from U235 is 1.94 MeV and 1.66 MeV, respectively. The mean and median energy of produced neurons are also shown on each plot.
>6 MeV neutrons
With water in the converter (no significant difference with no water):
Neutron energy spectra from 42 MeV electrons
0.13-7 MeV neutrons
With water in the converter (no significant difference with no water):
0-0.1 MeV neutrons, with and without water
With water:
Without water:
Photon energy spectra from 42 MeV electrons
The plot below shows the energy distribution of photons exiting the converter for four different ranges of angle w.r.t. the incident electron beam
Misc
Below is a plot of the rate of neutron production as the beam traverses through the converter. Zero corresponds to where the beam enters the titanium window.