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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.
Watanabe Osamu (19P39)
Fusion Science and Technology | Volume 51 | Number 2 | February 2007 | Pages 322-324
Technical Paper | Open Magnetic Systems for Plasma Confinement | doi.org/10.13182/FST07-A1389
Articles are hosted by Taylor and Francis Online.
An electric field distribution of a surface normal wave on a corrugated metal plate used for a surface wave oscillator was calculated. The surface wave oscillator is formed by the corrugated metal plate and a sheet electron beam. The direction of the beam propagation is parallel to the metal plate and perpendicular to the corrugation. In the vicinity of the sinusoidal corrugated metal plate, the electromagnetic wave of the surface normal mode which propagates parallel to the plate exists. From the surface normal mode computation, it was confirmed that an electric field distribution had a periodic component to the traveling direction of the beam. Cherenkov interaction should be excited by the electron beam passing in this periodic electric field region. The surface normal wave always exists only in a slow wave region, and has backward wave with the periodic boundary condition. This interaction becomes absolute instability, because the interaction is on the backward wave of the surface normal mode in the slow wave region. A strong oscillation by the surface normal wave should be generated, because the wave can generate the absolute instability of the Cherenkov interaction.