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 Annual Conference
May 31–June 3, 2026
Denver, CO|Sheraton Denver
Standards Program
The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
Latest Magazine Issues
Dec 2025
Jul 2025
Latest Journal Issues
Nuclear Science and Engineering
December 2025
Nuclear Technology
Fusion Science and Technology
November 2025
Latest News
Deep Fission to break ground this week
With about seven months left in the race to bring DOE-authorized test reactors on line by July 4, 2026, via the Reactor Pilot Program, Deep Fission has announced that it will break ground on its associated project on December 9 in Parsons, Kansas. It’s one of many companies in the program that has made significant headway in recent months.
S.C. McCool, A.J. Wootton, R.V. Bravenec, P.H. Edmonds, K.W. Gentle, H. Huang, J.W. Jagger, B. Richards, David W. Ross, E.R. Solano, J. Uglum, P.M. Valanju
Fusion Science and Technology | Volume 27 | Number 3 | April 1995 | Pages 444-450
Advanced Tokamak And Steady-State Sustainment Systems | doi.org/10.13182/FST95-A11947125
Articles are hosted by Taylor and Francis Online.
Recent favorable results on START have caused renewed interest in low aspect ratio tokamaks. To design an economical next-step spherical tokamak to study confinement scaling and high beta plasmas, we have developed a transport scaling and device optimization code. This code OPT, benchmarked against START, includes 10 empirical confinement scaling laws and essential tokamak physics such as stability limits. Parameters are optimized separately for each scaling law and physics goal. Using OPT we find for R/a=1.2 to 2.0 one can achieve βN=5 and <β>=30% with just two neutral beams (PNB<3.5 MW) for Ip≥0.75 MA, and Ro≥0.6 m. In contrast, if one insists on using the nominal device parameters, Ip=1 MA and Ro=0.8 m, with each scaling law, achieving βN=5 requires typically PNB⋍7.5 MW.