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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.
A. H. Kazi, C. R. Heimbach, R. C. Harrison
Nuclear Science and Engineering | Volume 85 | Number 4 | December 1983 | Pages 371-386
Technical Paper | doi.org/10.13182/NSE83-A18384
Articles are hosted by Taylor and Francis Online.
Neutron and gamma-ray tissue kerma and scalar spectrum measurements have been made at the Army Pulse Radiation Division (APRD), Aberdeen Proving Ground, to 1.6 km in air-over-ground geometry from a fission source and are compared to state-of-the-art transport calculations. Measurements have been made by the APRD staff as well as German, Canadian, and French scientists. A variety of integral detectors and differential spectrometers were used. Agreement among the various groups ranges from good to excellent. Calculations have been made in support of shielding programs and in connection with the Hiroshima-Nagasaki dose reevaluation effort. The DOT transport calculations have been performed at the Lawrence Livermore and Oak Ridge National Laboratories, the Defence Research Establishment, Ottawa, and at Science Applications, Inc. Monte Carlo calculations have been performed at Los Alamos National Laboratory. The calculations are generally consistent. Average calculated-to-measured kerma ratios range from 0.83 to 1.27. Calculated-to-measured neutron flux ratios vary from ∼0.6 near 1 keV and ∼0.8 near 5 MeV to ∼1.7 near 0.8 MeV. These spectral differences tend to cancel when determining tissue kerma, raising the possibility that some of the agreement in kerma may be fortuitous. Sources of possible discrepancies are discussed