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Conference Spotlight
Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Fusion Science and Technology
August 2025
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The newest era of workforce development at ANS
As most attendees of this year’s ANS Annual Conference left breakfast in the Grand Ballroom of the Chicago Downtown Marriott to sit in on presentations covering everything from career pathways in fusion to recently digitized archival nuclear films, 40 of them made their way to the hotel’s fifth floor to take part in the second offering of Nuclear 101, a newly designed certification course that seeks to give professionals who are in or adjacent to the industry an in-depth understanding of the essentials of nuclear energy and engineering from some of the field’s leading experts.
V. Erckmann, G. Janzen, W. Kasparek, G. Müller, P. G. Schüller, K. Schwörer, M. Thumm, R. Wilhelm, W VII-A Team
Fusion Science and Technology | Volume 7 | Number 2 | March 1985 | Pages 275-282
Technical Paper | doi.org/10.13182/FST85-A24543
Articles are hosted by Taylor and Francis Online.
Plasma buildup and heating of ohmically heated currentless plasmas by electron cyclotron resonance heating (28 GHz, 200 kW, 40 ms) were investigated in the WENDELSTEIN VII-A stellarator. Two different kinds of wave launching were examined in detail. First, the gyrotron mode mixture, containing 50% of the total power in ordinary (O)-mode and 50% in extraordinary (X)-mode polarization, was irradiated from the low-field side. Then a linearly polarized wave in O-mode polarization was launched from the low-field side, the nonabsorbed fraction being reflected back to the plasma from the high-field side in X-mode polarization. An increase of the central electron temperature from 0.6 keV (first case) to 1.2 keV (second case) was observed, which is explained as being due to the narrow power deposition profile in the latter case rather than due to the slight increase of the heating efficiency from 40 to 50%. Strong evidence of parametric decay of the X-mode fraction is found. Transport calculations using neoclassical plateau coefficients for the electron heat conduction including ripple losses fit well with the measured profiles, if enhanced losses at the plasma edge are introduced.