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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.
L. P. Ku, P. R. Garabedian
Fusion Science and Technology | Volume 50 | Number 2 | August 2006 | Pages 207-215
Technical Paper | Stellarators | doi.org/10.13182/FST06-A1237
Articles are hosted by Taylor and Francis Online.
We have identified and developed new classes of quasi-axially symmetric configurations that have attractive properties from the standpoint of both near-term physics experiments and long-term power-producing reactors. These include configurations with very small aspect ratios (~2.5) having superior quasi-symmetry and energetic particle confinement characteristics, and configurations with strongly negative global magnetic shear from the shaping fields so that the overall rotational transform, when combined with the transform from bootstrap currents at finite plasma pressures, will have a small but positive shear, making the avoidance of low-order rational surfaces at a given operating beta possible. Additionally, we have found configurations with National Compact Stellarator Experiment-like characteristics but with the biased components in the magnetic spectrum that allow us to improve the confinement of energetic particles. For each new class of configurations, we have also designed coils to ensure that the new configurations are realizable and engineering-wise feasible. The coil designs typically have the properties of R/min(C-P) 6 and R/min(C-C) 10, where R is the plasma major radius and min(C-P) and min(C-C) are the minimum coil-to-plasma and coil-to-coil separations, respectively. These coil properties allow power-producing reactors to be designed with R < 9 m for deuterium-tritium plasmas with a full breeding blanket. The good quasi-axisymmetry limits the energy loss of alpha particles to below 10%.