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Front-end nuclear fuel supply cooperation: Turning allied interdependence into strategic advantage
The global nuclear revival, which is fueled by unprecedented demand for firm, affordable, dispatchable power for artificial intelligence and data center build-out, energy security imperatives, and climate commitments, has exposed a structural reality of the Western fuel cycle: No single allied nation currently possesses the full suite of front-end capabilities. From mining through conversion, enrichment, fabrication, and the emerging deconversion and metallization steps required for reactor fuels, capability is distributed across Canada, France, Japan, the United Kingdom, and the United States (collectively, the “Sapporo Five”), as well as a small group of close partners.
Robert P. Rulko
Nuclear Science and Engineering | Volume 121 | Number 3 | December 1995 | Pages 371-392
Technical Paper | doi.org/10.13182/NSE95-A24141
Articles are hosted by Taylor and Francis Online.
Historically, the even-order PN equations have been considered a less accurate approximation to the transport equation than the odd-order PN-1 equations. This perception has stemmed from two apparent conceptual difficulties imposed by the even-order PN methods— the difficulty in prescribing rigorous boundary conditions for even-order PN equations that contain the odd number of angular flux moments and the discontinuous character of the even-order PN solutions at material interfaces. With the first one of the mentioned even-order PN conceptual problems, a presentation is made of a straightforward and physically-motivated variational procedure based on a new functional that leads from a multigroup planar geometry transport problem to a multigroup P2 problem with clearly and rigorously defined multigroup boundary conditions. These boundary conditions are new and allow neutron transfer between energy groups at the boundary. These boundary conditions are tested by comparing P2, P1, and SN calculations. Our results show that in the test problems considered, the multigroup P2 equations with variational boundary conditions are always more accurate than the P1 multigroup equations with Federighi-Pomraning or Marshak boundary conditions applied to each energy group.