Difference between revisions of "MCNP Sim of Jack Converter"
Line 50: | Line 50: | ||
Without water in the converter: | Without water in the converter: | ||
[[File:42MeVJackLin n(all erg)noH2O.png|1000px]] | [[File:42MeVJackLin n(all erg)noH2O.png|1000px]] | ||
+ | |||
+ | ===0-0.1 MeV neutrons, with and without water=== | ||
+ | With water: | ||
+ | |||
+ | [[File:42MeVJackLin n thermal(1).png|700px]] | ||
+ | |||
+ | Without water: | ||
+ | |||
+ | [[File:42MeVJackLin n thermal no H2O.png|700px]] | ||
==Misc== | ==Misc== |
Revision as of 19:38, 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.
Neutron energy spectra from 42 MeV electrons
0-7 MeV neutrons, with and without water
Without water in the converter:
0-0.1 MeV neutrons, with and without water
With water:
Without water:
Misc
The difference between the U235 neutron spectrum and the energy spectrum from the converter may be partially due to moderation of neutrons by H2O. The plot below demonstrates this point, which registers the energy of each photo-neutron immediately after emission, as opposed to after the photo-neutrons exit the converter.
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.
Photons
The plot below shows the energy distribution of photons exiting the converter at three different intervals of their angle w.r.t. the incident electron beam