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Fusion Science and Technology
August 2026
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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.
F. Wagner, J. Baldzuhn, R. Brakel, B. Branas, R. Burhenn, J. Das, E. De La Luna, V. Erckmann, Y. Feng, S. Fiedler, L. Gianonne, P. Grigull, H.-J. Hartfuß, O. Heinrich, G. Herre, M. Hirsch, J.V. Hofmann, E. Holzhauer, R. Jaenicke, Ch. Konrad, G. Kocsis, W. Ohlendorf, P. Pech, F. Sardei, E. Wuersching, S. Zoletnik
Fusion Science and Technology | Volume 27 | Number 3 | April 1995 | Pages 32-39
Overview Paper | doi.org/10.13182/FST95-A11947043
Articles are hosted by Taylor and Francis Online.
We will give a summary on the status of H-mode studies on W7-AS stellarator. The major H-mode characteristics compare well with those known from the tokamak H-mode. All major characteristics of the H-mode are reproduced: The transition is spontaneous above a power and density threshold; particle and energy confinement improve simultaneously; a transport barrier at the edge develops with steep pressure gradients and ELMs appear; small scale fluctuations are strongly reduced and the development of a radial electric field is indicated by increased perpendicular impurity flow velocity. The temporal development of the transition seems to be distinctively slower than in tokamaks. The H-mode can be initiated by ECRH or NBI, respectively. The power threshold can be smaller than that of tokamaks. With ECRH, the density threshold is found to increase with heating power. The H-mode develops in small windows of the accessible iota range. These operational islands are characterised by a negative electric field already prior to the H-mode and a distinct maximum in space potential at the separatrix.