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Uranium prices steady as EIA releases annual market report
The end-of-July spot price for uranium was $86.36 per pound, as reported by Cameco—roughly the same as it has been since February. Analytics firm Trading Economics reported a uranium futures price of $86.60 per pound, a figure that also has been holding steady since early April.
These updates come as the U.S. Energy Information Administration has released its 2025 Uranium Marketing Annual Report, which examines in detail multiple aspects of the U.S. uranium market. Data are derived from answers given in the Uranium Marketing Annual Survey, which collects information on contracts, deliveries (during the past year and projected for the next 10 years), purchased enrichment services, inventories, fuel assembly usage, and market requirements.
J. J. MacFarlane, R. R. Peterson, P. Wang, G. A. Moses
Fusion Science and Technology | Volume 26 | Number 3 | November 1994 | Pages 886-890
Inertial Confinement Fusion Reactor, Reactor Target, and Driver | Proceedings of the Eleventh Topical Meeting on the Technology of Fusion Energy New Orleans, Louisiana June 19-23, 1994 | doi.org/10.13182/FST94-A40266
Articles are hosted by Taylor and Francis Online.
We present results from radiation-hydrodynamics calculations which show the central role resonant self-absorption plays in reducing radiative energy loss rates in high-gain ICF target chamber plasmas. Calculations were performed using a non-LTE radiative transfer model which we have recently coupled to our target chamber radiation-hydrodynamics code. The lower radiation fluxes escaping the plasma, which occur due to the self-absorption of line radiation in their optically thick cores, lead to significantly lower temperature increases at the surface of the target chamber first wall. The calculations were performed for the SIRIUS-P laser-driven direct-drive ICF power reactor. In this conceptual design study, high-gain targets release approximately 400 MJ of energy in the center of a gas-filled target chamber. The target debris ions and x-rays are stopped in the gas, and the energy is reradiated to the chamber wall over a much longer time scale. Because the time scales are comparable to the time it takes to thermally conduct energy away from the first surface, the thermal stresses and erosion rates for the first wall are greatly reduced.