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International Conference on Mathematics and Computational Methods Applied to Nuclear Science and Engineering (M&C 2025)
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Denver, CO|The Westin Denver Downtown
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The 2025 ANS election results are in!
Spring marks the passing of the torch for American Nuclear Society leadership. During this election cycle, ANS members voted for the newest vice president/president-elect, treasurer, and six board of director positions (four U.S., one non-U.S., one student). New professional division leadership was also decided on in this election, which opened February 25 and closed April 15. About 21 percent of eligible members of the Society voted—a similar turnout to last year.
Nobuyuki Asakura et al.
Fusion Science and Technology | Volume 63 | Number 1 | May 2013 | Pages 70-75
doi.org/10.13182/FST13-A16876
Articles are hosted by Taylor and Francis Online.
Design study of the magnetic configuration and divertor geometry for the “advanced divertor” in a Demo tokamak reactor is summarized. Equilibrium calculation code, TOSCA, was developed for the super-X divertor (SXD) design by introducing two parameters, i.e. location of the super-X null and a ratio of the poloidal magnetic fluxes at the super-X null to that at the separatrix. SXD has an advantage to increase connection length from the divertor null point to the divertor target (L//div), which is 1.6-1.8 times larger with increasing fSX, compared to that in the conventional long-leg divertor. Whereas flux expansion near the super-X null was increased, increase in the target wet area (Awet) was small. Snowflake divertor (SFD) magnetic configuration was produced by adjusting PFC locations and the current distribution. L//div was largely increased near the SF null in the conventional divertor size. Key issues remain: control scenario for SFnull and high plasma shaping should be developed, and appropriate SFD design is necessary. For the advanced divertor design, divertor coils inside TFC are preferable due to the maximum current and size.