托卡马克边缘等离子体非线性漂阻气胀模式的三维流体模拟

P. Guzdar, J. Drake, D. McCarthy, A. Hassam, C. Liu
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引用次数: 224

摘要

本文完成了托卡马克边缘等离子体中由漂移-阻力气球模式产生的湍流和剪切流的三维研究。流体模拟表明,当自一致产生的剪切流被抑制时,在非线性状态下密度波动可以达到10% ~ 15%。这些模式也被发现会产生极性不对称的粒子输运。这些波动的特征尺度长度在横贯B的平面上是各向同性的,小于沿场线的连接长度。剪切极向流是由雷诺应力和斯特林格机制共同驱动的。在自一致剪切流的存在下,横向谱在b方向上不再各向同性,涡旋在极向方向上被拉长。此外,密度和势的波动水平以及相关的粒子输运都大大降低。这些特征在质量上是一致的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Three‐dimensional fluid simulations of the nonlinear drift‐resistive ballooning modes in tokamak edge plasmas
A three‐dimensional study of the turbulence and sheared flow generated by the drift‐resistive ballooning modes in tokamak edge plasmas has been completed. The fluid simulations show that 10%–15% percent density fluctuations can develop in the nonlinear state when the self‐consistently generated shear flow is suppressed. These modes are also found to give rise to poloidally asymmetric particle transport. Characteristic scale lengths of these fluctuations are isotropic in the plane transverse to B and smaller than the connection length along the field line. Sheared poloidal flow is self‐consistently driven by both the Reynolds stress and the Stringer mechanisms. In the presence of self‐consistent shear flow, the transverse spectrum is no longer isotropic transverse to B. The vortices become elongated in the poloidal direction. Also, there is a substantial reduction in both the level of fluctuations of the density and potential and the associated particle transport. These features are in qualitative agreemen...
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