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Trapped electron stabilization of ballooning modes in low aspect ratio toroidal plasmas

机译:低纵横比环形等离子体中气球模式的俘获电子稳定性

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The kinetic effects of trapped electron dynamics and finite gyroradii and magnetic drift motion of ions are shown to give rise to a large parallel electric field and hence a parallel current that greatly enhances the stabilizing effect of field line tension for ballooning modes in low aspect ratio toroidal plasmas. For large aspect ratio the stabilizing effect increases (reduces) the beta(=2P/B-2) threshold for the first (second) stability of the kinetic ballooning mode (KBM) from the magnetohydrodynamics (MHD) beta threshold value by a factor proportional to the trapped electron density fraction. For small aspect ratio the stabilizing effect can greatly increase the beta threshold of the first stability of KBMs from the MHD beta threshold by S(c)similar or equal to1+(n(e)(eu))delta, where n(e)(eu) is the ratio of the total electron density to the untrapped electron density, and delta depends on the trapped electron dynamics and finite gyroradii and magnetic drift motion of ions. If n(e)(eu)much greater than1 as in the National Spherical Torus Experiment (NSTX) [M. Ono, Nucl. Fusion 40, 557 (2000)] with an aspect ratio of similar or equal to1.4, the KBM should be stable for betaless than or equal to1 for finite magnetic shear. Therefore, unstable KBMs are expected only in the weak shear region near the radial location of the minimum of the safety factor in NSTX reverse shear discharges. (C) 2004 American Institute of Physics.
机译:捕获的电子动力学,有限的陀螺半径和离子的磁漂移运动的动力学效应显示出产生了较大的平行电场,因此,平行电流极大地增强了对于低长宽比环型气球模式的场线张力的稳定作用血浆。对于较大的宽高比,稳定作用从磁流体动力学(MHD)β阈值增加(减少)了动态膨胀模式(KBM)的第一(第二)稳定性的beta(= 2P / B-2)阈值,比例成比例到捕获的电子密度分数。对于小长宽比,稳定效果可以将MHD beta阈值从KBD的第一个稳定性的beta阈值大大增加S(c)近似或等于1+(n(e)/ n(eu))delta,其中n(e )/ n(eu)是总电子密度与未俘获电子密度的比率,而增量取决于俘获电子的动力学,有限的陀螺半径和离子的磁漂移运动。如果n(e)/ n(eu)大于1,如国家球形圆环实验(NSTX)中所述[M.小野,Nucl。 [Fusion 40,557(2000)]的长宽比相似或等于1.4,对于有限的磁剪,KBM在beta小于或等于1时应保持稳定。因此,仅在NSTX反向剪切放电中安全系数最小值最小的径向位置附近的弱剪切区域中,会出现不稳定的KBM。 (C)2004美国物理研究所。

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