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Conference Spotlight
2025 ANS Winter Conference & Expo
November 8–12, 2025
Washington, DC|Washington Hilton
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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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.
Chi-Jung Hsu
Nuclear Science and Engineering | Volume 26 | Number 3 | November 1966 | Pages 305-318
Technical Paper | doi.org/10.13182/NSE66-A17351
Articles are hosted by Taylor and Francis Online.
The heat transfer characteristics for the case of laminar flow through a hexagonal channel have been determined for the following conditions: The uniform heat flux on any one side of the hexagon is identical to that on the opposite side, and may be equal to or different than those on the two adjacent sides; both the velocity and temperature profiles are fully established; the heat transfer from the walls may or may not be accompanied by simultaneous internal heat generation in the flowing fluid. Fundamental temperature solution and equations are presented which may be used to predict the temperature field, or to calculate the difference between local wall temperature and the bulk fluid temperature for a variety of cases. Methods of predicting the variation of local wall temperature are illustrated for several typical cases, including the case of uniformly distributed wall heat flux. For the latter case, it was found that appreciable temperature variation exists along the periphery of the hexagon. The circumferential variation of the local Nusselt number and the mean Nusselt number are also reported, with and without internal heat generation.