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Conference Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Fusion Science and Technology
August 2025
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The newest era of workforce development at ANS
As most attendees of this year’s ANS Annual Conference left breakfast in the Grand Ballroom of the Chicago Downtown Marriott to sit in on presentations covering everything from career pathways in fusion to recently digitized archival nuclear films, 40 of them made their way to the hotel’s fifth floor to take part in the second offering of Nuclear 101, a newly designed certification course that seeks to give professionals who are in or adjacent to the industry an in-depth understanding of the essentials of nuclear energy and engineering from some of the field’s leading experts.
Masahiro Kinoshita, Hiroshi Yoshida, Hidefumi Takeshita
Fusion Science and Technology | Volume 10 | Number 3 | November 1986 | Pages 462-473
Technical Paper | Tritium System | doi.org/10.13182/FST86-A24786
Articles are hosted by Taylor and Francis Online.
In the tritium breeding system for a fusion reactor, the addition of a large flow rate of hydrogen (H2) or deuterium (D2) to the helium purge gas is considered essential to avoid a large amount of tritium inventory. However, the tritium concentration in the hydrogen isotope mixture to be separated is reduced by two or three orders of magnitude by the addition. The effects of the drastic dilution of tritium by H2 or D2 on the isotope separation by cryogenic distillation are analyzed. The analysis is made under the conditions of the Japanese Fusion Engineering Reactor where the tritium production rate is 3 g/h. It is shown that the dilution requires a specific cascade in addition to the cascade in the mainstream fuel circulation system. The H2 addition is much more favorable than the D2 addition in terms of the cascade scale needed, tritium inventory within the cascade, and refrigeration capacity required. The dilution of tritium by H2 by two orders of magnitude requires a two-column cascade, and the tritium inventory and refrigeration capacity required are ∼8 g and 65 W, respectively. The dilution by three orders of magnitude requires a three-column cascade, and the values of the two parameters are ∼12 g and 630 W, respectively. In these cases, the tritium inventory and refrigeration capacity required for the cascade in the mainstream fuel circulation system are ∼70 g and 110 W, respectively. Thus, the dilution up to three orders of magnitude could pose no serious problem in the isotope separation.