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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.
Gary J. Dau and Monte V. Davis
Nuclear Science and Engineering | Volume 25 | Number 3 | July 1966 | Pages 223-226
Technical Paper | doi.org/10.13182/NSE66-A17828
Articles are hosted by Taylor and Francis Online.
Theoretical development for the gamma-induced production of conduction band electrons in alumina is presented. Consideration of charge carrier mobility limited investigations to crystals having ionic bonding. Because of the difficulty in evaluating theoretical constants, all were combined and considered to be independent of temperature and radiation. This constant was evaluated experimentally. A model with a single trap depth was developed for predicting conductivity of ionic insulators as a function of temperature and radiation dose rate. The model is , where the first term on the right represents ionic conductivity of material external to a radiation field and the second term describes radiation-induced conductivity. Term P represents gamma dose rate in roentgen per hour, G is an experimentally determined constant, and W represents the energy necessary to raise trapped electrons into the conduction band. The temperature dependence of the mobility is represented by (T)3/2. Evaluation of experimental data for alumina gave W = 0.086 ± 0.014 eV and G = 7.4 × lO−21 (Ω−1cm−1K3/2R−1h).