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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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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.
S. Kobayashi, T. Shimizu, Y. Seki
Fusion Science and Technology | Volume 15 | Number 2 | March 1989 | Pages 1008-1012
Safety And Environment — II | doi.org/10.13182/FST89-A39825
Articles are hosted by Taylor and Francis Online.
If a loss-of-coolant accident occurs in a fusion reactor, the temperature in the vacuum vessel will rise. If the decay heat is not removed, then the plasma vacuum boundary may melt. In this paper, the effects of the decay heat in a LOCA are analysed numerically based on the Fusion Experimental Reactor (FER). ... the fusion power: ∼ 460 MW. In the case of a loss-of-coolant accident with the plasma shut down, it is assumed that the decay heat is removed by the radiation of the divertor only. If the radiant effect is a quarter of the black radiation, the divertor plate will not melt, because the temperature rise is less than 150 K. Secondly, it is assumed that the decay heat is removed by the radiation between the outer shield and the heat shield. When the initial shield temperature is low and the amount of the shield is large, the temperature rise is negligible, because the heat capacity is large enough to absorb the heat. The effect of the natural convection outside of the cryostat is negligible to remove the heat.