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August 24–27, 2026
Dallas, TX|Hilton Anatole
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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.
M. Z. Youssef, R. W. Conn
Nuclear Science and Engineering | Volume 74 | Number 2 | May 1980 | Pages 130-139
Technical Paper | doi.org/10.13182/NSE80-A19628
Articles are hosted by Taylor and Francis Online.
A separation technique that divides the transport equation into two parts is developed to analyze fusion-fission hybrid systems. The transport of fusion-produced neutrons (first generation neutrons) is separately calculated and a fission neutron source is generated. The behavior of the second and subsequent generations of neutrons is obtained using fewer energy groups and a low order treatment for scattering. As usual, integral parameters are the summation of the contributions from the two parts. A sensitivity theory consistent with the separation technique is used to evaluate the relative sensitivity coefficient of a reaction rate to perturbations in the system. Relations between different adjoint fluxes are derived in the context of the separation technique. The technique is applied to show that the use of a low-order scattering description when solving the second part of the problem leads to small errors in the value of the fissile fuel production rate in a hybrid. Variation of this production rate with time can approximately be accounted for using the beginning-of-life values of the forward flux of the first part (related to fusion neutrons), the adjoint flux of the system, and the time-dependent source of the second part (related to subsequent fission generations).