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Fusion energy: Progress, partnerships, and the path to deployment
Over the past decade, fusion energy has moved decisively from scientific aspiration toward a credible pathway to a new energy technology. Thanks to long-term federal support, we have significantly advanced our fundamental understanding of plasma physics—the behavior of the superheated gases at the heart of fusion devices. This knowledge will enable the creation and control of fusion fuel under conditions required for future power plants. Our progress is exemplified by breakthroughs at the National Ignition Facility and the Joint European Torus.
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.