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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.
Gerasimos Tinios, Steve F. Horne, Ian H. Hutchinson, Stephen M. Wolfe
Fusion Science and Technology | Volume 30 | Number 2 | November 1996 | Pages 201-218
Technical Paper | Special Section: Plasma Control Issues for Tokamaks / Experimental Device | doi.org/10.13182/FST96-A30751
Articles are hosted by Taylor and Francis Online.
Linear control models are tested against experimental data from the Alcator C-Mod tokamak. A nonrigid, approximately flux-conserving, perturbed equilibrium plasma response model is used, together with a detailed toroidally symmetric model of the conducting vacuum vessel and the supporting superstructure, and experimentally determined power supply responses. Experiments are conducted with vertically unstable plasmas where the feedback is turned off and the plasma response is observed in an open-loop configuration. The agreement between theory and experiment is found to be very satisfactory, proving that the perturbed equilibrium plasma response model and a toroidally symmetric electromagnetic model of the vacuum vessel and the structure can be trusted for the purposes of calculations for control law design. The closed-loop behavior is also examined by injecting step perturbations into the desired vertical position of the plasma. The control hardware introduces nonlinearities that make it difficult to explain observed behavior with linear theory. Nonlinear simulation of the time evolution of the closed-loop experiments is able to account for the discrepancies between linear theory and experiment. Satisfactory agreement is then obtained between the model including the full multiple input/multiple output control system and the experimental observations.