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2025 ANS Winter Conference & Expo
November 8–12, 2025
Washington, DC|Washington Hilton
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Japan gets new U for enrichment as global power and fuel plans grow
President Trump is in Japan today, with a visit with new Prime Minister Sanae Takaichi on the agenda. Takaichi, who took office just last week as Japan’s first female prime minister, has already spoken in favor of nuclear energy and of accelerating the restart of Japan’s long-shuttered power reactors, as Reuters and others have reported. Much of the uranium to power those reactors will be enriched at Japan’s lone enrichment facility—part of Japan Nuclear Fuel Ltd.’s Rokkasho fuel complex—which accepted its first delivery of fresh uranium hexafluoride (UF₆) in 11 years earlier this month.
Ricardo Artigas, H. E. Hungerford
Nuclear Science and Engineering | Volume 36 | Number 3 | June 1969 | Pages 295-303
Technical Paper | doi.org/10.13182/NSE69-A18727
Articles are hosted by Taylor and Francis Online.
Expressions for the neutron flux at the exit of a cylindrical duct of radius δ and length l (with λ = δ2/l2), have been found by the use of the albedo concept and by the method of single-collision sources in the duct wall, based on monoenergetic integral transport theory. In contrast with other methods of solution, the isotropic area source of radius δ at the duct entrance is not approximated by a point source, and the numerical evaluation of integrals does not impose restrictions on the values of λ. Calculation of the neutron flux at the duct exit is expedited by the use of the tables given, which are a function of the duct geometry and were generated from the numerical evaluation of the integrals that appear in the expressions for the flux. Comparison of the results as predicted by the formulas developed in this paper and those predicted by already existing formulas with the results of a stochastic neutron-transport code indicates that the formulas developed here are always in better agreement with the results of the code. For values of λ < 1, the formulas developed here differ by a maximum of ± 10%, while the existing formulas differ by a maximum of more than 100%.