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The busyness of the nuclear fuel supply chain
Ken Petersenpresident@ans.org
With all that is happening in the industry these days, the nuclear fuel supply chain is still a hot topic. The Russian assault in Ukraine continues to upend the “where” and “how” of attaining nuclear fuel—and it has also motivated U.S. legislators to act.
Two years into the Russian war with Ukraine, things are different. The Inflation Reduction Act was passed in 2022, authorizing $700 million in funding to support production of high-assay low-enriched uranium in the United States. Meanwhile, the Department of Energy this January issued a $500 million request for proposals to stimulate new HALEU production. The Emergency National Security Supplemental Appropriations Act of 2024 includes $2.7 billion in funding for new uranium enrichment production. This funding was diverted from the Civil Nuclear Credits program and will only be released if there is a ban on importing Russian uranium into the United States—which could happen by the time this column is published, as legislation that bans Russian uranium has passed the House as of this writing and is headed for the Senate. Also being considered is legislation that would sanction Russian uranium. Alternatively, the Biden-Harris administration may choose to ban Russian uranium without legislation in order to obtain access to the $2.7 billion in funding.
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.