ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 Nuclear Energy Conference & Expo (NECX)
August 24–27, 2026
Dallas, TX|Hilton Anatole
Latest Magazine Issues
Aug 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
September 2026
Nuclear Technology
Fusion Science and Technology
August 2026
Latest News
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.
B. Coppi, P. Detragiache, S. Migliuolo, M. Nassi,, B. Rogers
Fusion Science and Technology | Volume 25 | Number 3 | May 1994 | Pages 353-367
Technical Paper | Alpha-Particle Special / Experimental Device | doi.org/10.13182/FST94-A30292
Articles are hosted by Taylor and Francis Online.
The Ignitor experiment has been designed to achieve fusion burn and ignition conditions in a high-density deuterium-tritium (D-T) plasma with a compact high magnetic field confinement configuration. The recent addition of a powerful system of radio-frequency heating to the design of Ignitor allows the investigation of physics issues relevant to advanced D-3He reactors and the second stability region forfinite-β plasmas. To maximize the production of D-3He power, a lower density regime is considered (e.g., n0 ≃ 3 × 1020 m−3) than that found to be optimal for D-T ignition (n0 ≃ 1 × 1021 m−3). This allows a relatively large population of 3He nuclei at high energies ≳0.65 MeV to be produced by a high density of injected power at the 3He ion cyclotron frequency (up to 18 MW injected in the plasma column of volume ≲10 m3). The investigation of second stability region access can be carried out in relatively low magnetic field and plasma current regimes with the added benefit that the duration of the plasma discharge can be extended over relatively long times. In fact, the Ignitor magnets can be brought down to an initial temperature of 30 K by gas-helium cooling. The low aspect ratio (≃2.8) and elongated plasma cross section of Ignitor make it suitable to reach both finite-β conditions and interesting plasma regimes at the same time. The Candor concept is the next step in the evolution of the Ignitor program. Candor is capable of producing plasma currents up to 25 MA with toroidal magnetic fields BT ≃ 13 T. Unlike Ignitor, Candor would operate with values of βp around 1.5 and with the central part of the plasma column in the second stability region. The D-3He ignition in this case can be reached by a combination of ICRF heating and alpha-particle heating due to D-T fusion reactions.