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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.
A. H. Spano
Nuclear Science and Engineering | Volume 15 | Number 1 | January 1963 | Pages 37-51
Technical Paper | doi.org/10.13182/NSE63-A26262
Articles are hosted by Taylor and Francis Online.
Knowledge of the Doppler coefficient associated with the nonuniform temperature distribution conditions obtained in a reactor runaway is of importance to reactor safety considerations of low-enrichment oxide cores. Measurement of this dynamic coefficient has been made at Spert in an investigation of the kinetic behavior of a water-moderated, UO2-fuel-rod reactor, by means of self-limiting power excursion tests covering a range of initial asymptotic reactor periods from 31 sec to 3.2 msec. In the long-period region, reactor shutdown was provided both by various heat-transfer-dependent mechanisms effecting loss of moderator from the core and by Doppler broadening. In the short-period region below 7 msec, where the reactor period is small compared to the thermal time constant of the UO2 fuel rods and reactor shutdown is provided essentially by the Doppler reactivity alone, the data indicate Rc(tm) = −6.2 , where Rc(tm) and Em are, respectively, the compensated reactivity and energy (Mw-sec) at the time of peak power. An additional reactivity effect, positive in sign and resulting from systematic bowing of the fuel rods during the transient power burst, yielded a significant change in burst shape behavior. The fuel rod bowing effect was separated from other feedback effects by performing two series of tests, with and without mechanical constraints on the fuel rods. In the shortest period test, the maximum power was about 7500 Mw, the total energy released in the burst was about 110 Mw-sec, and the maximum pressure measured was less than 8 psi. No damage occurred as a consequence of this or any other test.