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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.
S. Cirant, J. Berrino, P. Buratti, G. D'Antona, F. Gandini, G. Granucci, E. Iannone, E. Lazzaro, V. Mellera, V. Muzzini, P. Smeulders, O. Tudisco
Fusion Science and Technology | Volume 53 | Number 1 | January 2008 | Pages 174-183
Technical Paper | Special Issue on Electron Cyclotron Wave Physics, Technology, and Applications - Part 2 | doi.org/10.13182/FST08-A1663
Articles are hosted by Taylor and Francis Online.
The paper describes experimental studies performed on the FTU tokamak on magnetohydrodynamic (MHD) instabilities and their active control by electron cyclotron (EC) heating and EC current drive (ECH/ECCD). It deals in particular with implementing of an automatic system that detects both the onset and localization of tearing modes and the localization of the EC power deposition and that is capable of actuating the stabilizing reaction with ECH/ECCD. The system is composed of a digital signal processor-based control unit to analyze electron temperature fluctuations (mostly from EC emission) and Mirnov coil data and to control gyrotron power supplies. The action is provided by an arrangement of four Gaussian beams at 140 GHz, coupling up to 1.6 MW power in total. The detection/reaction system, successfully tested in the experiments described, is very fast since no mirror motion is foreseen. In fact, the Gaussian beams are preliminarily oriented in an array covering the whole region where the mode is expected, and only the one closest to the mode is switched on at its appearance. The measurement of the deposition layer dep is performed by analyzing the transient response to modulated EC power. Different modulation waveforms are used, both periodic and pseudorandom, in order to select the most sensitive and fastest technique.