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Fusion Energy
This division promotes the development and timely introduction of fusion energy as a sustainable energy source with favorable economic, environmental, and safety attributes. The division cooperates with other organizations on common issues of multidisciplinary fusion science and technology, conducts professional meetings, and disseminates technical information in support of these goals. Members focus on the assessment and resolution of critical developmental issues for practical fusion energy applications.
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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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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.
D. H. J. Goodall, G. E. Austin, J. M. Weaver
Fusion Science and Technology | Volume 6 | Number 2 | September 1984 | Pages 393-398
Technical Paper | Selected papers from the Ninth International Vacuum Congress and the Fifth International Conference on Solid Surfaces (Madrid, Spain, September 26-October 1, 1983) | doi.org/10.13182/FST84-A23211
Articles are hosted by Taylor and Francis Online.
The DITE tokamak has a bundle divertor capable of operating in the maximum toroidal field of 2.7 T. A scanning infrared camera with a framing rate of 50 f.p.s. has been used to determine the power and power density at the divertor target. For discharges with 1.4 MW of neutral injection, peak diverted powers of nearly 400 kW were observed during the neutral injection period, representing 24% of the total input power. Power densities on the ion drift side of the target of up to 30 MW m−2 were measured for these discharges. Discharges without neutral injection show a maximum power diversion when the gas puffing is switched off.