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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.
Kiyoshi Yatsu, Leonid G. Bruskin, Teruji Cho, Minoru Hamada, Mafumi Hirata, Hitoshi Hojo, Makoto Ichimura, Kameo Ishii, Khairul M. Islam, Akiyoshi Itakura, Isao Katanuma, Yasuhito Kiwamoto, Junko Kohagura, Shigeyuki Kubota, Atsushi Mase, Yousuke Nakashima, Teruo Saito, Yoshiteru Sakamoto, Teruo Tamano, Yoshinori Tatematsu, Tokihiko Tokuzawa, Masayuki Yoshikawa
Fusion Science and Technology | Volume 35 | Number 1 | January 1999 | Pages 52-59
Invited Lectures | doi.org/10.13182/FST99-A11963826
Articles are hosted by Taylor and Francis Online.
Potential confinement of an ICRF-heated high-ion temperature plasma in GAMMA 10 is experimentally studied. The potential confinement was shown from data of one-end plugging and both-end plugging. The waveform of end loss current and an analysis of end loss ion energies have also indicated potential formation and confinement. The central cell line density increases 50% by the potential confinement. Some radial losses were observed in the anchor and/or plug/barrier regions and a rate of the radial loss was measured by using the data from one-end plugging. Under an experimental condition, the radial loss rate was estimated to be about 3%. In order to reduce the radial loss, conducting plates were installed adjacent to the plasma in the anchor transition region. The density increase of 60 % was attained after installation of the conducting plates and a higher density increase can be expected in the near future. The density increase was 50% before installation of the conducting plates. Controllability and reproducibility of the potential confinement are also improved after installation of the conducting plates.