ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
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Division Spotlight
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.
Meeting Spotlight
Conference on Nuclear Training and Education: A Biennial International Forum (CONTE 2025)
February 3–6, 2025
Amelia Island, FL|Omni Amelia Island Resort
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!
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Fusion Science and Technology
Latest News
Christmas Night
Twas the night before Christmas when all through the houseNo electrons were flowing through even my mouse.
All devices were plugged in by the chimney with careWith the hope that St. Nikola Tesla would share.
Daniel L. Jassby, John A. Schmidt
Fusion Science and Technology | Volume 40 | Number 1 | July 2001 | Pages 52-55
Technical Paper | doi.org/10.13182/FST01-A179
Articles are hosted by Taylor and Francis Online.
The electrical energy requirements and costs of accelerator transmutation of waste (ATW) and fusion plants designed to transmute nuclides of fission wastes are compared. Both systems use the same blanket concept, but tritium breeding is taken into account for the fusion system. The ATW and fusion plants are found to have the same electrical energy requirement per available blanket neutron when the blanket coverage is comparable and the fusion energy gain is near breakeven (Q [approximately equal to] 1), but the fusion plant has only a fraction of the energy requirement when Q >> 1. If the blanket thermal energy is converted to electricity, the fusion plant and ATW have comparable net electrical energy outputs per available neutron when Q 1.5 and the blanket neutron multiplication is large.