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Conference Spotlight
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.
R. A. Karam, K. D. Dance, T. Nakamura, J. E. Marshall
Nuclear Science and Engineering | Volume 40 | Number 3 | June 1970 | Pages 414-423
Technical Paper | doi.org/10.13182/NSE70-A20193
Articles are hosted by Taylor and Francis Online.
An integral transport method was developed and applied to the calculation of the central reactivity worths of various samples measured in a 2700-liter uranium-carbide fast core and in a 4000-liter UO2 fast core. The method was used to obtain corrections to multigroup first-order perturbation calculations, incorporating self-shielding effects inside and outside the sample, as well as scattering, fission, and edge-effect perturbations. Resonance interaction between a 238U sample and the 238U in the core as well as resonance self-shielding in the sample itself were explicitly considered. A similar treatment was used for 235U samples. ENDF/B data were used in all of the analyses. The calculated central worths of 10B and tantalum were in very good agreement with the measured values, indicating that the calculated value of βeff used to convert percent Δk/k to period measurements was reasonably accurate. The calculated worths of 235U were 5 to 10% greater than the measured values. The discrepancy between the calculated and measured values for 238U was 15 to 20%. The discrepancy for graphite in particular and scatterers in general was rather large, indicating that the distribution of the adjoint function is not adequately calculated.