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.
引用
收藏
页数:9
相关论文
共 50 条
  • [1] Rotation and radial electric field in the plasma edge with resonant magnetic perturbation at TEXTOR
    Coenen, J. W.
    Schmitz, O.
    Unterberg, B.
    Clever, M.
    Jakubowski, M. A.
    Samm, U.
    Schweer, B.
    Stoschus, H.
    Tokar, M.
    NUCLEAR FUSION, 2011, 51 (06)
  • [2] Influence of resonant magnetic perturbation on a rotating helical plasma
    Nishimura, S.
    Toda, S.
    Narushima, Y.
    Yagi, M.
    PLASMA PHYSICS AND CONTROLLED FUSION, 2013, 55 (01)
  • [3] Experimental observations of plasma edge magnetic field response to resonant magnetic perturbation on the TEXTOR Tokamak
    Yang, Y.
    Liang, Y.
    Sun, Y.
    Zhang, T.
    Pearson, J.
    Xu, Y.
    NUCLEAR FUSION, 2012, 52 (07)
  • [4] Influence of different DED base mode configurations on the radial electric field at the plasma edge of TEXTOR
    Wingen, A.
    Spatschek, K. H.
    NUCLEAR FUSION, 2010, 50 (03)
  • [5] 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,
  • [6] Formation of a three-dimensional scrape-off layer in a fast rotating resonant magnetic perturbation field at TEXTOR
    Stoschus, H.
    Schmitz, O.
    Unterberg, B.
    Jakubowski, M. W.
    Frerichs, H.
    Kruezi, U.
    Reiter, D.
    Samm, U.
    JOURNAL OF NUCLEAR MATERIALS, 2011, 415 (01) : S923 - S926
  • [7] The radial electric field as a measure for field penetration of resonant magnetic perturbations
    Mordijck, S.
    Moyer, R. A.
    Ferraro, N. M.
    Wade, M. R.
    Osborne, T. H.
    NUCLEAR FUSION, 2014, 54 (08)
  • [8] Continuum resonance induced electromagnetic torque by a rotating plasma response to static resonant magnetic perturbation field
    Liu, Yueqiang
    Connor, J. W.
    Cowley, S. C.
    Ham, C. J.
    Hastie, R. J.
    Hender, T. C.
    PHYSICS OF PLASMAS, 2012, 19 (10)
  • [9] Impact of stochastic magnetic fields on plasma rotation and radial electric fields in the plasma edge of the tokamak TEXTOR
    Unterberg, B.
    Busch, C.
    de Bock, M.
    Coenen, J. W.
    Finken, K. H.
    Jachmich, St.
    Jakubowski, M. W.
    Kikuchi, Y.
    Kraemer-Flecken, A.
    Lehnen, M.
    Samm, U.
    Schmitz, O.
    Soldatov, S.
    Tokar, M. Z.
    von Hellermann, M.
    Wolf, R. C.
    Xu, Y.
    JOURNAL OF NUCLEAR MATERIALS, 2007, 363 : 698 - 702
  • [10] Enhancement of helium exhaust by resonant magnetic perturbation fields at LHD and TEXTOR
    Schmitz, O.
    Ida, K.
    Kobayashi, M.
    Bader, A.
    Brezinsek, S.
    Evans, T. E.
    Funaba, H.
    Goto, M.
    Mitarai, O.
    Morisaki, T.
    Motojima, G.
    Nakamura, Y.
    Narushima, Y.
    Nicolai, D.
    Samm, U.
    Tanaka, H.
    Yamada, H.
    Yoshinuma, M.
    Xu, Y.
    NUCLEAR FUSION, 2016, 56 (10)