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Russell, G.J.; Seeger, P.A.; Fluharty, R.G.
Los Alamos Scientific Lab., N.Mex. (USA)1977
Los Alamos Scientific Lab., N.Mex. (USA)1977
AbstractAbstract
[en] Parametric studies, using continuous-energy Monte Carlo codes, were done to optimize the neutronics of the Weapons Neutron Research (WNR) target and three possible target/moderator configurations: slab target/slab moderators, cylindrical target/cylindrical moderator, and cylindrical target/double-wing moderators. The energy range was 0.5 eV to 800 MeV. A general figure-of-merit (FOM) approach was used. The WNR facility performance can be doubled or tripled by optimizing the target and target/moderator configurations; this approach is more efficient than increasing the Clinton P. Anderson Meson Physics Facility (LAMPF) accelerator power by an equivalent factor. A bare target should be used for neutron energies above approximately 100 keV. The FOM for the slab target/slab moderator configuration is the best by a factor of at least 2 to 3 below approximately 1 keV. The total neutron leakage from 0.5 eV to 100 keV through a 100- by 100-mm area centered at the peak leakage is largest for the slab moderator, exceeding that of the cylindrical moderator and double-wing moderator by factors of 1.7 and 3.4, respectively. The neutron leakage at 1 eV from one 300- by 150-mm surface of a slab moderator is 1.5 times larger than that from one 155- by 150-mm surface of a cylindrical moderator. When compared with the 1-eV leakage from two 100- by 150-mm surfaces of a double-wing moderator, that from the slab moderator is 3.4 times larger. 107 figures, 13 tables
Primary Subject
Source
Mar 1977; 87 p; Available from NTIS., PC A05/MF A01
Record Type
Report
Report Number
Country of publication
ACCELERATOR FACILITIES, ANGULAR DISTRIBUTION, CONFIGURATION, LAMPF LINAC, MODERATORS, MONTE CARLO METHOD, NEUTRON FLUX, NEUTRON LEAKAGE, NEUTRON SOURCES, NEUTRON SPECTRA, NUCLEAR REACTION YIELD, OPTIMIZATION, PULSES, SPATIAL DISTRIBUTION, SPECIFICATIONS, TARGETS, TIME DEPENDENCE, TIME-OF-FLIGHT METHOD
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