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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.
D. Post, T. Ando, A. Antipenkov, S. Chiocchio, J. Dietz, G. Federici, M. Gouge, Yu. Igitkhanov, G. Janeschitz, A. Kukushkin, P. Ladd, J. Mandrekas, E. Martin, D. Mitin, H. Nakamura, H. Pacher, W. Stacey, M. Sugihara, R. Tivey
Fusion Science and Technology | Volume 30 | Number 3 | December 1996 | Pages 594-600
International Thermonuclear Experimental Reactor | doi.org/10.13182/FST96-A11963003
Articles are hosted by Taylor and Francis Online.
The ITER power and particle control system is designed to exhaust the 300 to 400 MW of alpha and auxiliary heating power and the 5 × 1020 He atoms per second created by the fusion reactions, to control the density and to fuel the plasma. The power and particle control system consists of a single null poloidal divertor, a set of active pumps with a total pumping speed of ~ 200 m3/s, and gas puffing and pellet fuelling systems. Atomic processes are used to spread out the heating power over the first wall and divertor walls, thereby reducing the peak heat loads on the divertor plates to acceptable levels. The divertor has a “vertical target” plate configuration and tight baffling to maximize the effectiveness of the atomic processes for energy losses in the divertor and to maximize the neutral pressure in the divertor and minimize the backflow of neutrals from the divertor to the main chamber.