• Acta Physica Sinica
  • Vol. 69, Issue 5, 055201-1 (2020)
Jin Yang1、2, Jun Chen2、3, Fu-Di Wang2, Ying-Ying Li2, Bo Lyu2、*, Dong Xiang1、*, Xiang-Hui Yin4, Hong-Ming Zhang2, Jia Fu2, Hai-Qing Liu2, Qing Zang2, Yu-Qi Chu2, Jian-Wen Liu2, Xun-Yu Wang1、2, Bin Bin2, Liang He1、2, Shun-Kuan Wan2, Xue-Yu Gong1, and Min-You Ye3
Author Affiliations
  • 1School of Nuclear Science and Technology, University of South China, Hengyang 421001, China
  • 2Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031, China
  • 3Department of Engineering and Applied Physics, University of Science and Technology of China, Hefei 230026, China
  • 4School of Electrical Engineering, University of South China, Hengyang 421001, China
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    DOI: 10.7498/aps.69.20191716 Cite this Article
    Jin Yang, Jun Chen, Fu-Di Wang, Ying-Ying Li, Bo Lyu, Dong Xiang, Xiang-Hui Yin, Hong-Ming Zhang, Jia Fu, Hai-Qing Liu, Qing Zang, Yu-Qi Chu, Jian-Wen Liu, Xun-Yu Wang, Bin Bin, Liang He, Shun-Kuan Wan, Xue-Yu Gong, Min-You Ye. Experimental investigation of lower hybrid current drive induced plasma rotation on the experimental advanced superconducting tokamak[J]. Acta Physica Sinica, 2020, 69(5): 055201-1 Copy Citation Text show less
    Waveforms of typical parameters of an LHCD shot (#70938) on EAST: (a) Plasma current (black) and LHCD power)(blue); (b) loop voltage (black) and internal inductance (blue); (c) central line averaged electron density; (d) stored energy; (e) central ion (red) and electron (black) temperature; (f) the change of core toroidal rotation velocity.
    Fig. 1. Waveforms of typical parameters of an LHCD shot (#70938) on EAST: (a) Plasma current (black) and LHCD power)(blue); (b) loop voltage (black) and internal inductance (blue); (c) central line averaged electron density; (d) stored energy; (e) central ion (red) and electron (black) temperature; (f) the change of core toroidal rotation velocity.
    Waveforms of typical parameters at different LHCD power levels: (a) plasma current; (b) central line averaged electron density; (c) LHCD power; (d) the change of core toroidal rotation velocity.
    Fig. 2. Waveforms of typical parameters at different LHCD power levels: (a) plasma current; (b) central line averaged electron density; (c) LHCD power; (d) the change of core toroidal rotation velocity.
    The relationship between the change of core toroidal rotation velocity and LHCD power.
    Fig. 3. The relationship between the change of core toroidal rotation velocity and LHCD power.
    Profiles of safety factor at different LHCD powers.
    Fig. 4. Profiles of safety factor at different LHCD powers.
    Waveforms of typical parameters: (a) Electron temperature; (b) ion temperature; (c) toroidal rotation velocity; (d) LHCD power (black) and central line averaged electron density (blue).
    Fig. 5. Waveforms of typical parameters: (a) Electron temperature; (b) ion temperature; (c) toroidal rotation velocity; (d) LHCD power (black) and central line averaged electron density (blue).
    (a) Profile of toroidal velocity modulation amplitude; (b) profile of toroidal velocity phase transformation.
    Fig. 6. (a) Profile of toroidal velocity modulation amplitude; (b) profile of toroidal velocity phase transformation.
    (a) Profile of toroidal momentum diffusion coefficient; (b) profile of toroidal momentum pinch coefficient.
    Fig. 7. (a) Profile of toroidal momentum diffusion coefficient; (b) profile of toroidal momentum pinch coefficient.
    Jin Yang, Jun Chen, Fu-Di Wang, Ying-Ying Li, Bo Lyu, Dong Xiang, Xiang-Hui Yin, Hong-Ming Zhang, Jia Fu, Hai-Qing Liu, Qing Zang, Yu-Qi Chu, Jian-Wen Liu, Xun-Yu Wang, Bin Bin, Liang He, Shun-Kuan Wan, Xue-Yu Gong, Min-You Ye. Experimental investigation of lower hybrid current drive induced plasma rotation on the experimental advanced superconducting tokamak[J]. Acta Physica Sinica, 2020, 69(5): 055201-1
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