ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 Nuclear Energy Conference & Expo (NECX)
August 24–27, 2026
Dallas, TX|Hilton Anatole
Latest Magazine Issues
Jun 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
August 2026
Nuclear Technology
July 2026
Fusion Science and Technology
Latest News
GAIN makes diverse selections for its third round of awards this year
The Department of Energy’s Gateway for Accelerated Innovation in Nuclear has recently awarded four third-round fiscal year 2026 vouchers to support the development of innovative nuclear technologies. Each company will get access to specific capabilities and expertise in the DOE’s national laboratory complex—in this round of awards Idaho National Laboratory, Oak Ridge National Laboratory, and Sandia National Laboratories are named—and will be responsible for a minimum 20 percent cost share, which can be an in-kind contribution.
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.