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2026 Nuclear Energy Conference & Expo (NECX)
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.
R. E. MacPherson, Jr., H. D. Stuart
Nuclear Science and Engineering | Volume 12 | Number 2 | February 1962 | Pages 225-233
Technical Paper | doi.org/10.13182/NSE62-A26061
Articles are hosted by Taylor and Francis Online.
Gas-cooled reactor systems can benefit from the use of internal metallic-foil insulations which take advantage of the relatively low thermal conductivity of the coolant gas itself. Tests have shown that, for design purposes, Nusselt, Grashof, and Prandtl number correlations for vertical gas spaces form a good basis for finding optimum foil spacing and for approximating insulation performance. Tests were conducted chiefly on a spirally wrapped foil arrangement in which in. spacing between adjacent foil turns was maintained by strips of corrugated sheet metal 1 in. in width. Results from this arrangement in an atmosphere of helium have shown gross effective thermal conductivity values to be approximately 150% of the values for the gas itself at pressures below 200 psia. From 200 psia to 1000 psia, conductivity increases with pressure to values approximately twice those for the gas itself. For the specific geometry tested effective conductivity was shown to be a function of mean insulation temperature, gas pressure, temperature gradient across the insulant, and insulation thickness.