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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.
V. Basiuk, A. Bécoulet, T. Hutter, G. Martin, A. L. Pecquet, B. Saoutic
Fusion Science and Technology | Volume 26 | Number 3 | November 1994 | Pages 222-226
Technical Paper | Experimental Device | doi.org/10.13182/FST94-A30324
Articles are hosted by Taylor and Francis Online.
During additional heating in Tore Supra [ion cyclotron resonance frequency (ICRF) or neutral beam injection], fast ion losses due to the toroidal field ripple were clearly measured by a set of graphite probes. This detector collects the flow of fast ions entering a vertical port and usually shows a maximum flux for ions originating from the vicinity of surface δ* = 0. During the monster sawteeth regime, achieved with ICRF, a remarkable phenomenon was observed: an ejection of fast ions that were not correlated with any measured magnetohydrodynamic activity. The radial distribution of these ions was quite different from the distribution usually observed exhibiting a peak located in the central section of the plasma. A new diagnostic is being constructed for measurement of the energy distribution of these ions, from 80 keV (energy of the neutral beam injected in Tore Supra) up to 1 MeV (expected during ICRF). The principle of the diagnostic is the identification of the ions through their energy by using their Larmor radius (ρ = 1.3 cm for 100 keV → ρ = 3.6 cm for 700 keV, B = 4T). The detector is made of a hollow graphite cylinder with a small entrance slot, located in a vertical port on the ion drift side. An array of six metallic collectors placed inside the graphite cylinder intercepts the ions. The current on each collector was estimated at 10 → 100 nA, during ICRF heating. The energy resolution of this diagnostic is expected to be ∼20 keV for the lowest energy range and 100 keV for the highest energy range. This type of elementary detector might be extrapolated for the measurements of alpha-particle losses in future deuterium-tritium experiments. It should also be suitable for studies of stochastic ripple diffusion.