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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.
Melvin M. Levine, Meyer Steinberg
Nuclear Science and Engineering | Volume 12 | Number 4 | April 1962 | Pages 498-504
Technical Paper | doi.org/10.13182/NSE62-A26097
Articles are hosted by Taylor and Francis Online.
A general solution for optimum design of a radiaton chemical reaction vessel having an internal uniform triangular array of long, thin γ-ray sources is derived. The dependence of chemical production rate on amount and distribution of radioactive material and on size and shape of vessel is accounted for. Values for two general design parameters (vessel efficiency, ψ, and unit cell efficiency, µ) as a function of the vessel diameter and source spacing are given and include radiation buildup. The rate equation expressed as a power law of the radiation intensity is combined with information on the dependence of cost of reactor vessel on volume and pressure. The total cost of source material and vessels is then minimized to determine optimum size and number of vessels and the number of curies of radiation. The rate and cost equations are applied to the radiation polymerization of ethylene. By the methods outlined here it is possible to determine the parameters of an optimum irradiation assembly. The dimensions of the vessel and source array and the quantity of radioactive source material necessary for a given rate of production are determined for the minimum cost condition.