Influence of elongation and triangularity on plasma response to resonant magnetic perturbations

被引:6
|
作者
Yang, Xu [1 ]
Liu, Yueqiang [2 ]
Xu, Wei [3 ]
He, Yuling [4 ]
Lu, Shuangshuang [5 ]
机构
[1] Chongqing Technol & Business Univ, Chongqing Engn Lab Detect Control & Integrated Sy, Chongqing 400067, Peoples R China
[2] Gen Atom, POB 85608, San Diego, CA 92186 USA
[3] Chongqing Technol & Business Univ, Natl Res Base Intelligent Mfg Serv, Chongqing 400067, Peoples R China
[4] South China Normal Univ, GPETR Ctr Quantum Precis Measurement, Guangdong Prov Key Lab Quantum Engn & Quantum Mat, SPTE, Guangzhou 510006, Peoples R China
[5] Dalian Univ Technol, Sch Phys & Optoelect Technol, Key Lab Mat Modificat Laser Ion & Elect Beams, Minist Educ, Dalian 116024, Peoples R China
基金
中国博士后科学基金; 中国国家自然科学基金;
关键词
elongation; triangularity; plasma response; resonant magnetic perturbation; DISCHARGES; STABILITY;
D O I
10.1088/1741-4326/ac2636
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Systematic toroidal modeling of the plasma response to the n = 1-4 (n is the toroidal mode number) resonant magnetic perturbation (RMP) field is carried out in order to understand the plasma-shaping effect on controlling the type-I edge-localized modes (ELMs) in tokamak experiments. Considered are large variations of the plasma elongation and triangularity at a fixed edge safety factor q (a), for limiter plasmas with both single-null (SN) and double-null (DN) divertor-like boundary shapes. Numerical results assuming conformal 3D RMP coils show that (i) the optimum coil phasing between the upper and lower rows for ELM control becomes increasingly sensitive to the plasma elongation with higher-n toroidal spectra, (ii) the optimum coil phasing is however essentially independent of the plasma triangularity for all n = 1-4 RMP fields, (iii) with the same coil current and the optimum coil phasing, high elongation generally favors ELM control but it may be more challenging for plasmas with intermediate elongation and with lower-n (n = 1-2) RMPs, and (iv) higher triangularity is generally always better for ELM control with all n = 1-4 fields for both DN and SN divertor-like plasma boundary shapes.
引用
收藏
页数:23
相关论文
共 50 条
  • [21] Plasma response to rotating resonant magnetic perturbations with a locked mode in the J-TEXT tokamak
    Wang, Nengchao
    Rao, Bo
    Hu, Qiming
    Ding, Yonghua
    Chen, Zhipeng
    Yang, Zhoujun
    Guo, Daojing
    Huang, Zhuo
    Ji, Xinke
    Li, Da
    Li, Jianchao
    Li, Mao
    Pan, Xiaoming
    Xu, Guo
    Yu, Q.
    Zhuang, G.
    Pan, Yuan
    Liang, Y.
    NUCLEAR FUSION, 2019, 59 (02)
  • [22] Influence of pedestal pressure on plasma response to resonant magnetic perturbation field
    Yang, Xu
    Yuan, Jiao
    Liu, Yueqiang
    He, Xin
    He, Yuling
    Xia, Guoliang
    Zhou, Lina
    Miao, Yutian
    EUROPEAN PHYSICAL JOURNAL-SPECIAL TOPICS, 2025,
  • [23] Plasma currents induced by resonant magnetic field perturbations in tokamaks
    Reiser, D.
    Chandra, D.
    PHYSICS OF PLASMAS, 2009, 16 (04)
  • [24] Modelling of the edge plasma of MAST in the presence of resonant magnetic perturbations
    Rozhansky, V.
    Molchanov, P.
    Kaveeva, E.
    Voskoboynikov, S.
    Kirk, A.
    Nardon, E.
    Coster, D.
    Tendler, M.
    NUCLEAR FUSION, 2011, 51 (08)
  • [25] Modeling of ITER Edge Plasma in the Presence of Resonant Magnetic Perturbations
    Rozhansky, V.
    Kaveeva, E.
    Veselova, I.
    Voskoboynikov, S.
    Coster, D.
    CONTRIBUTIONS TO PLASMA PHYSICS, 2016, 56 (6-8) : 587 - 591
  • [26] Influence of the resonant magnetic perturbations on transport in the Large Helical Device
    Jakubowski, M. W.
    Drewelow, P.
    Masuzaki, S.
    Tanaka, K.
    Pedersen, T. S.
    Akiyama, T.
    Bozhenkov, S.
    Dinklage, A.
    Kobayashi, M.
    Narushima, Y.
    Sakakibara, S.
    Suzuki, Y.
    Wolf, R.
    Yamada, H.
    NUCLEAR FUSION, 2013, 53 (11)
  • [27] Response of the poloidal rotation to resonant magnetic perturbations in the EAST tokamak
    Wang, S. F.
    Zhou, C.
    Liu, A. D.
    Zhuang, G.
    Sun, Y. W.
    Gu, S.
    Wang, S. X.
    Liu, H. Q.
    Dai, Z. L.
    Wang, H. H.
    Zhang, J.
    Zhong, X. M.
    Feng, X.
    Gao, L. T.
    Shi, W. X.
    Qiu, S. C.
    Li, L. X.
    Chen, X. Y.
    Zhang, Y. Y.
    Xie, P. C.
    Ye, C.
    Yang, H.
    PLASMA PHYSICS AND CONTROLLED FUSION, 2024, 66 (12)
  • [28] Quasi-linear MHD modelling of H-mode plasma response to resonant magnetic perturbations
    Nardon, E.
    Tamain, P.
    Becoulet, M.
    Huysmans, G.
    Waelbroeck, F. L.
    NUCLEAR FUSION, 2010, 50 (03)
  • [29] Plasma response to resonant magnetic perturbations near rotation zero-crossing in low torque plasmas
    Xie, Pengcheng
    Sun, Youwen
    Liu, Yueqiang
    Gu, Shuai
    Ma, Qun
    Ye, Cheng
    Wu, Xuemin
    Sheng, Hui
    PHYSICS OF PLASMAS, 2021, 28 (09)
  • [30] Plasma turbulence simulations in a diverted tokamak with applied resonant magnetic perturbations
    Boinnard, T.
    Coelho, A. J.
    Loizu, J.
    Ricci, P.
    NUCLEAR FUSION, 2023, 63 (07)