Toroidal modeling of plasma response to RMP fields in ITER

被引:30
|
作者
Li, L. [1 ,2 ,3 ]
Liu, Y. Q. [4 ,5 ,6 ]
Wang, N. [2 ,7 ]
Kirk, A. [4 ]
Koslowski, H. R. [2 ]
Liang, Y. [1 ,2 ,8 ]
Loarte, A. [9 ]
Ryan, D. [4 ,10 ]
Zhong, F. C. [1 ,3 ]
机构
[1] Donghua Univ, Coll Sci, Shanghai 201620, Peoples R China
[2] Forschungszentrum Julich, Inst Energie & Klimaforsch Plasmaphys, Julich, Germany
[3] Minist Educ, Magnet Confinement Fus Res Ctr, Beijing, Peoples R China
[4] Culham Sci Ctr, CCFE, Abingdon OX14 3DB, Oxon, England
[5] Southwestern Inst Phys, POB 432, Chengdu 610041, Peoples R China
[6] Chalmers Univ Technol, Dept Earth & Space Sci, SE-41296 Gothenburg, Sweden
[7] Huazhong Univ Sci & Technol, State Key Lab Adv Electromagnet Engn & Technol, Wuhan 430074, Hubei, Peoples R China
[8] Chinese Acad Sci, Inst Plasma Phys, POB 1126, Hefei 230031, Peoples R China
[9] ITER Org, Route Vinon Sur Verdon,CS 90 046, F-13067 St Paul Les Durance, France
[10] Univ York, Dept Phys, York YO10 5DD, N Yorkshire, England
基金
中国国家自然科学基金;
关键词
RMP fields; plasma response; ELM control; ITER;
D O I
10.1088/1361-6587/aa5769
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
A systematic numerical study is carried out, computing the resistive plasma response to the resonant magnetic perturbation (RMP) fields for ITER plasmas, utilizing the toroidal code MARS-F (Liu et al 2000 Phys. Plasmas 7 3681). A number of factors are taken into account, including the variation of the plasma scenarios (from 15 MA Q = 10 inductive scenario to the 9 MA Q = 5 steady state scenario), the variation of the toroidal spectrum of the applied fields (n = 1, 2, 3, 4, with n being the toroidal mode number), the amplitude and phase variation of the currents in three rows of the RMP coils as designed for ITER, and finally a special case of mixed toroidal spectrum between the n = 3 and n = 4 RMP fields. Two-dimensional parameter scans, for the edge safety factor and the coil phasing between the upper and lower rows of coils, yield 'optimal' curves that maximize a set of figures of merit, that are defined in this work to measure the plasma response. Other two-dimensional scans of the relative coil current phasing among three rows of coils, at fixed coil currents amplitude, reveal a single optimum for each coil configuration with a given n number, for the 15 MA ITER inductive plasma. On the other hand, scanning of the coil current amplitude, at fixed coil phasing, shows either synergy or cancellation effect, for the field contributions between the off-middle rows and the middle row of the RMP coils. Finally, the mixed toroidal spectrum, by combining the n = 3 and the n = 4 RMP field, results in a substantial local reduction of the amplitude of the plasma surface displacement.
引用
收藏
页数:18
相关论文
共 50 条
  • [31] Modeling techniques for correcting measured data on the ITER toroidal field insert coil
    ITER International Team, Garching, Germany
    1600, 1418-1422 (June 2004):
  • [32] Observing and modeling the poloidal and toroidal fields of the solar dynamo
    Cameron, R. H.
    Duvall, T. L., Jr.
    Schuessler, M.
    Schunker, H.
    ASTRONOMY & ASTROPHYSICS, 2018, 609
  • [33] POLOIDAL AND TOROIDAL FIELDS IN GEOMAGNETIC-FIELD MODELING
    BACKUS, G
    REVIEWS OF GEOPHYSICS, 1986, 24 (01) : 75 - 109
  • [34] MODELING OF PLASMA START-UP IN ITER
    PILLSBURY, RD
    SCHULTZ, JH
    IEEE TRANSACTIONS ON MAGNETICS, 1992, 28 (02) : 1462 - 1465
  • [35] Observing and modeling the poloidal and toroidal fields of the solar dynamo
    Cameron, R.H.
    Duvall, T.L.
    Schüssler, M.
    Schunker, H.
    Astronomy and Astrophysics, 2018, 609
  • [36] ELM control with RMP: plasma response models and the role of edge peeling response
    Liu, Yueqiang
    Ham, C. J.
    Kirk, A.
    Li, Li
    Loarte, A.
    Ryan, D. A.
    Sun, Youwen
    Suttrop, W.
    Yang, Xu
    Zhou, Lina
    PLASMA PHYSICS AND CONTROLLED FUSION, 2016, 58 (11)
  • [37] Measurements and modelling of plasma response field to RMP on the COMPASS tokamak
    Markovic, T.
    Liu, Y. Q.
    Cahyna, P.
    Panek, R.
    Peterka, M.
    Aftanas, M.
    Bilkova, P.
    Bohm, P.
    Imrisek, M.
    Hacek, P.
    Havlicek, J.
    Havranek, A.
    Komm, M.
    Urban, J.
    Weinzettl, V.
    NUCLEAR FUSION, 2016, 56 (09)
  • [38] Comparison of edge plasma perturbation during ELM control using one vs. two toroidal rows of RMP coils in ITER similar shaped plasmas on DIII-D
    Fenstermacher, M. E.
    Evans, T. E.
    Osborne, T. H.
    Schaffer, M. J.
    deGrassie, J. S.
    Gohil, P.
    Groebner, R. J.
    Moyer, R. A.
    JOURNAL OF NUCLEAR MATERIALS, 2009, 390-91 : 793 - 796
  • [39] SOLPS-ITER modeling of deuterium throughput impact on the ITER SOL plasma
    Kaveeva, E.
    Makarov, S.
    Senichenkov, I.
    Rozhansky, V.
    Veselova, I.
    Bonnin, X.
    Pitts, R. A.
    NUCLEAR MATERIALS AND ENERGY, 2023, 35
  • [40] Plasma heat load in the toroidal gaps of the ITER-like plasma facing units in WEST tokamak
    Tichit, Q.
    Aumeunier, M. H.
    Corre, Y.
    Dejarnac, R.
    Dubus, L.
    Gaspar, J.
    Gerardin, J.
    Grosjean, A.
    Gunn, J. P.
    Juven, A.
    Krieger, K.
    Tsitrone, E.
    NUCLEAR MATERIALS AND ENERGY, 2025, 42