Impact of resistive MHD plasma response on perturbation field sidebands

被引:2
|
作者
Orlov, D. M. [1 ]
Evans, T. E. [2 ]
Moyer, R. A. [1 ]
Lyons, B. C. [2 ,3 ]
Ferraro, N. M. [4 ]
Park, G-Y [5 ]
机构
[1] Univ Calif San Diego, La Jolla, CA 92093 USA
[2] Gen Atom Co, San Diego, CA USA
[3] Oak Ridge Inst Sci Educ, Oak Ridge, TN USA
[4] Princeton Plasma Phys Lab, POB 451, Princeton, NJ 08543 USA
[5] Natl Fus Res Inst, Daejeon, South Korea
关键词
resonant magnetic perturbation; edge stochastic layer; ELM control; plasma response; tokamak; TOKAMAK; EDGE;
D O I
10.1088/0741-3335/58/7/075009
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
Single fluid linear simulations of a KSTAR RMP ELM suppressed discharge with the M3D-C-1 resistive magnetohydrodynamic code have been performed for the first time. The simulations show that the application of the n = 1 perturbation using the KSTAR in-vessel control coils (IVCC), which apply modest levels of n = 3 sidebands (similar to 20% of the n = 1), leads to levels of n = 3 sideband that are comparable to the n = 1 when plasma response is included. This is due to the reduced level of screening of the rational-surface-resonant n = 3 component relative to the rational-surface-resonant n = 1 component. The n = 3 sidebands could play a similar role in ELM suppression on KSTAR as the toroidal sidebands (n = 1, 2, 4) in DIII-D n = 3 ELM suppression with missing I-coil segments (Paz Soldan et al 2014 Nucl. Fusion 54 073013). This result may help to explain the uniqueness of ELM suppression with n = 1 perturbations in KSTAR since the effective perturbation
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页数:7
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