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2025 ANS Annual Conference
June 15–18, 2025
Chicago, IL|Chicago Marriott Downtown
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AI and productivity growth
Craig Piercycpiercy@ans.org
This month’s issue of Nuclear News focuses on supply and demand. The “supply” part of the story highlights nuclear’s continued success in providing electricity to the grid more than 90 percent of the time, while the “demand” part explores the seemingly insatiable appetite of hyperscale data centers for steady, carbon-free energy.
Technically, we are in the second year of our AI epiphany, the collective realization that Big Tech’s energy demands are so large that they cannot be met without a historic build-out of new generation capacity. Yet the enormity of it all still seems hard to grasp.
or the better part of two decades, U.S. electricity demand has been flat. Sure, we’ve seen annual fluctuations that correlate with weather patterns and the overall domestic economic performance, but the gigawatt-hours of electricity America consumed in 2021 are almost identical to our 2007 numbers.
W. Berkhahn, W. Ehrfeld, G. Krieg
Nuclear Technology | Volume 40 | Number 3 | October 1978 | Pages 329-340
Technical Paper | Isotope Separation | doi.org/10.13182/NT78-A26731
Articles are hosted by Taylor and Francis Online.
In the separation nozzle process, uranium isotope separation is based on the mass dependence of the centrifugal forces in a fast curved flow consisting of uranium hexafluoride and a light auxiliary gas that is admixed in a high molar excess. The objectives of this investigation are to determine the dependence of the separating characteristics of a centrifugal flow field on its spatial structure. Calculations were carried out for small UF6 mole fractions in the light auxiliary gas, so that the complicated ternary diffusion equations are reduced to two simple binary diffusion equations. The calculations show that isotope separation increases with the radial displacement of the UF6 streamlines relative to the auxiliary gas. Favorable initial distributions for a large radial shifting of UF6 exist when the flux, at the beginning of deflection, is high for small deflection radii, whereas at the end of deflection, the UF6 should be concentrated at large radii near the outer deflection wall. Consequently, a radial decrease of flow velocity, a high ratio of nozzle width to deflection radius, and high centrifugal fields at the end of deflection yield high separation effects. Taking into account the interdependence between the gas flow rate, the viscous losses, and the diffusion coefficient, the model developed can predict the influence of geometric parameters on the separating characteristics of the nozzle.