Influence of rotating resonant magnetic perturbation on the plasma radial electric field on TEXTOR

被引:5
|
作者
Zhang, T. [1 ]
Liang, Y. [1 ]
Sun, Y. [1 ]
Kraemer-Flecken, A. [1 ]
Soldatov, S. [1 ,2 ]
Nardon, E. [3 ]
Tamain, P. [3 ]
Waelbroeck, F. L. [4 ]
Yang, Y. [1 ,5 ]
Pearson, J. [1 ]
Koslowski, H. R. [1 ]
机构
[1] Forschungszentrum Julich GmbH, Inst Energy & Climate Res Plasma Phys, Assoc EURATOM FZJ, Julich, Germany
[2] Univ Ghent, Dept Appl Phys, B-9000 Ghent, Belgium
[3] CEN Cadarache, Assoc EURATOM CEA, F-13108 St Paul Les Durance, France
[4] Univ Texas Austin, Inst Fus Studies, Austin, TX 78712 USA
[5] Chinese Acad Sci, Inst Plasma Phys, Hefei 230031, Anhui, Peoples R China
关键词
DYNAMIC ERGODIC DIVERTOR; TOKAMAK PLASMA; TEARING MODES; ERROR-FIELD; TRANSPORT; TURBULENCE; EDGE; REFLECTOMETRY; STABILITY; PROFILE;
D O I
10.1088/0029-5515/52/7/074013
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 plasma radial electric field (E-r ) has been changed by applying an n = 1 counter-rotating resonant magnetic perturbation (RMP) field with a frequency of 5 kHz in ohmic plasmas on TEXTOR. The change in the E-r (Delta E-r) is negative, different from the observations in previous experiments where Delta E-r was always positive when a static or low frequency (similar to 1 kHz) rotating RMP field was applied in the plasma on TEXTOR. The Er profile in the present experiment shows two distinct evolution stages. In the first stage, Delta E-r from the q = 2 to q = 3 surfaces have a similar decrease as the amplitude of the 5 kHz counter-rotating field increases. In the second stage, the decrease rate of Delta E-r is faster for the positions closer to the q = 2 surface. As a result, the E-r around the q = 2 surface has a significant change in this second stage while no change of E-r is observed near the q = 3 surface even after the excitation of an m/n = 2/1 tearing mode. A reduced MHD code, 4FC, has been used to model the experiment. Two simulations have been performed. The first one is by applying a single 2/1 perturbation while both, 2/1 and 3/1 perturbations, have been applied in the second simulation. The result from the second simulation is qualitatively consistent with the experimental observations while the first simulation including only a single 2/1 perturbation cannot explain the evolution of the E-r profile in the second stage as observed in the experiment.
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页数:9
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