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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.
Eduardo V. Depiante, John E. Meyer
Nuclear Science and Engineering | Volume 104 | Number 2 | February 1990 | Pages 153-168
Technical Paper | doi.org/10.13182/NSE90-A23712
Articles are hosted by Taylor and Francis Online.
The analysis of transients in nuclear power plants is a complex problem normally requiring use of simulation tools. Although analog computers have been used for dynamic simulation, the most common approach involves use of a digital computer. An alternative method to attack the same problem, known as parity simulation, is described. Parity simulation, which originated in the study of electronic network transients, exploits the concept of electrical analogs of a physical system. Electrical analogs of the components of a system are constructed and interconnected in a highly user-oriented facility known as a parity simulator. The application of parity simulation to transient thermal-hydraulic single-phase flow is described. The development of a single-phase incompressible flow element is described. The governing mass, momentum, and energy equations along with other conditions are applied to a pipe section. The resulting model is then used to construct a circuit analog. The proposed circuit analog requires nonstandard components, the design and implementation of which is discussed. Subsequently, a formulation for single-phase compressible flow is given. Results obtained for different cases are presented. Comparison with reference numerical solutions shows general agreement.