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Materials Science & Technology
The objectives of MSTD are: promote the advancement of materials science in Nuclear Science Technology; support the multidisciplines which constitute it; encourage research by providing a forum for the presentation, exchange, and documentation of relevant information; promote the interaction and communication among its members; and recognize and reward its members for significant contributions to the field of materials science in nuclear technology.
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2025 ANS Annual Conference
June 15–18, 2025
Chicago, IL|Chicago Marriott Downtown
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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!
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Fusion Science and Technology
Latest News
Smarter waste strategies: Helping deliver on the promise of advanced nuclear
At COP28, held in Dubai in 2023, a clear consensus emerged: Nuclear energy must be a cornerstone of the global clean energy transition. With electricity demand projected to soar as we decarbonize not just power but also industry, transport, and heat, the case for new nuclear is compelling. More than 20 countries committed to tripling global nuclear capacity by 2050. In the United States alone, the Department of Energy forecasts that the country’s current nuclear capacity could more than triple, adding 200 GW of new nuclear to the existing 95 GW by mid-century.
J. D. Galambos, L. John Perkins
Fusion Science and Technology | Volume 25 | Number 2 | March 1994 | Pages 176-181
Technical Paper | Fusion Reactor | doi.org/10.13182/FST94-A30266
Articles are hosted by Taylor and Francis Online.
If the next-step International Thermonuclear Experimental Reactor (ITER) is designed to operate at finite energy multiplication (Q ∼ 10 to 20), as opposed to ignition (Q ∼ ∞), appreciable reductions in size and cost will result. Ignition will be attainable in such a “high-Q targeted” device under slightly enhanced confinement conditions. For example, with the nominal design guidelines from the ITER Conceptual Design Activity (CDA), designing for Q = 15 instead of ignition results in ∼20% savings in size and cost. Ignition would still be achievable in such a reduced-size device if the L-mode energy confinement enhancement factor (i.e., H factor) is ∼15% higher than the assumed nominal value of 2.0. This size/cost impact is large compared to other sensitivities, and the range of H-fact or improvement needed to recoup ignition is small compared to the uncertainty in the confinement scalings themselves.