Influence of low-Z impurity on the stabilization of m/n=2/1 tearing/locked modes in EAST

被引:4
|
作者
Xu, Ming [1 ]
Liang, Yunfeng [1 ,2 ,3 ]
Wei, Lai [4 ]
Duan, Yanmin [1 ]
Shi, Tonghui [1 ]
Zhao, Hailin [1 ]
Xu, Liqing [1 ]
Zhou, Ruijie [1 ]
Zhang, Ling [1 ]
Gu, Shuai [1 ,5 ,6 ]
Gao, Wei [1 ]
Zhang, Yang [1 ]
Wang, Zhengxiong [4 ]
Zang, Qing [1 ]
Liu, Haiqing [1 ]
Sun, Youwen [1 ]
Zhang, Shoubiao [1 ]
Hu, Liqun [1 ]
Gong, Xianzu [1 ]
Xu, Guosheng [1 ]
Hu, Jiansen [1 ]
Wan, Baonian [1 ]
机构
[1] Chinese Acad Sci ASIPP, Inst Plasma Phys, Hefei 230031, Peoples R China
[2] Huazhong Univ Sci & Technol, Wuhan 430074, Peoples R China
[3] Forschungszentrum Julich, Inst Energie & Klimaforsch Plasmaphys, Partner Trilateral Euregio Cluster TEC, D-52425 Julich, Germany
[4] Dalian Univ Technol, Sch Phys, Dalian 116024, Peoples R China
[5] Gen Atom, POB 85608, San Diego, CA 92186 USA
[6] Oak Ridge Natl Lab, POB 2009, Oak Ridge, TN 37830 USA
关键词
low-Z impurity; tearing modes; locked mode; asymmetry; LOCKING;
D O I
10.1088/1741-4326/ac4acd
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
The impact of the low-Z impurity concentration on mode stabilization has been investigated in the EAST tokamak. A series of tearing modes (TMs) with multiple helicities are excited by the low-Z (carbon) impurity concentration, and the dominant mode structure features m/n = 2/1 magnetic islands that propagate in the electron diamagnetic drift direction (m and n are poloidal and toroidal mode numbers, respectively). The m/n = 2/1 locked modes (LMs) can be formed by the redistribution of low-Z impurity concentration, and are unlocked spontaneously due to the decrease in the impurity concentration, where the width of the magnetic islands can reach w approximate to 5 cm (w/a approximate to 0.1, a is the minor radius). The increase in the electromagnetic brake torque is the primary reason for the mode locking, and the 'O'-point of the m/n = 2/1 magnetic islands is locked by the tungsten protector limiter (toroidal position: -0.4 pi <= phi <= -0.3 pi) with separation of Delta phi approximate to 0. The 3D asymmetric structure of the m/n = 2/1 magnetic islands is formed for the interaction with the tungsten protector limiter, and the electromagnetic interaction decreases dramatically for the separation of Delta phi > 0.2 pi. The mode excitation and locking mechanisms can be illustrated by the 'hysteresis effect' between the low-Z impurity concentration and the width of the m/n = 2/1 magnetic islands; namely, the growth of magnetic islands is modulated by the low-Z impurity concentration, and the rotation velocity is decelerated accordingly. However, the intrinsic mechanism for the unlocking of m/n = 2/1 LMs is complicated by considering the concentration of the low-Z impurity, and the possible unlocking mechanism is discussed. Therefore, understanding the relationship between the impurities and magnetic islands is more important for optimization of the control techniques (resonant magnetic perturbations -> LMs, electron cyclotron resonant heating (ECRH) -> neoclassical tearing mode (NTM), impurity seeding -> major collapse, etc).
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页数:12
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