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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.
Raymond L. Murray, Carroll R. Bingham, Chreston F. Martin
Nuclear Science and Engineering | Volume 18 | Number 4 | April 1964 | Pages 481-490
Technical Paper | doi.org/10.13182/NSE64-A18767
Articles are hosted by Taylor and Francis Online.
Solutions of the reactor kinetics equations for the reactivity variation required to achieve specified power responses are presented. This inverse approach is shown to extend the physical understanding of reactor behavior, to have utility in reactor operations, and to admit closed solutions for many otherwise non-linear problems. The inverse method is demonstrated by several examples: heating of a reactor at constant power, a ramp power rise followed by a constant level or by a linear drop, an oscillatory power, and a smooth transition betwen levels. Effects of a negative temperature coefficient may be described in terms of an additional fictitious delayed group. The constant-period response is shown to be optimum for a transition between two power levels.