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Study of electromagnetic microinstabilities in helical systems with the stellarator expansion method

机译:用恒星扩展方法研究螺旋系统中的电磁微不稳定性

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摘要

Electromagnetic microinstabilities in helical systems are studied by numerically solving integral eigenmode equations, which are derived from the ion gyrokinetic equation, the quasineutrality equation, the Amp?reu27s law, and the massless electron approximation. The stellarator expansion technique is used to evaluate finite-beta effects on the guiding-center drift in the helical configuration, where the toroidal plasma shift and the magnetic shear strongly influence the magnetic curvature and accordingly the stability of both magnetohydrodynamics (MHD) and kinetic modes. The kinetic integral equations are shown to reduce to the ideal MHD ballooning mode equation in the fluid limit, from which the Mercier criterion is obtained. For helical geometry like the Large Helical Device (LHD) [Motojima, et al., Nucl. Fusion 43, 1674 (2003)], it is confirmed that, when increasing the beta value, the ion temperature gradient mode is stabilized while the kinetic ballooning mode (KBM) is destabilized due to the unfavorable geodesic curvature resulting from the negative magnetic shear combined with the toroidal plasma shift. Also, dependencies of these kinetic-mode properties on the poloidal wave number and the magnetic shear are investigated. It is found that the KBM-unstable parameter region is narrower than the Mercier-unstable region in the LHD-like configuration.
机译:通过对积分本征模方程进行数值求解,研究了螺旋系统中的电磁微不稳定性,这些方程是从离子陀螺动力学方程,拟中性方程,安培定律和无质量电子近似推导而来的。恒星器扩展技术用于评估螺旋构型中引导中心漂移的有限贝塔效应,其中环形等离子体偏移和磁切变强烈影响磁曲率,进而影响磁流体动力学(MHD)和动力学模式的稳定性。示出了动力学积分方程,该流体积分方程在流体极限处简化为理想的MHD膨胀模式方程,由此获得了Mercier准则。对于像大型螺旋装置(LHD)这样的螺旋几何形状[Motojima等,Nucl。 [Fusion 43,1674(2003)],可以确定,当增加β值时,离子温度梯度模式稳定,而动态膨胀模式(KBM)由于负磁切变所带来的不利的测地曲率而不稳定。与环形血浆移位。而且,研究了这些动力学模式特性对极谱波数和磁剪切的依赖性。发现在类似LHD的配置中,KBM不稳定参数区域比Mercier不稳定区域更窄。

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    H. Sugama; T.-H. Watanabe;

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  • 年度 2004
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  • 原文格式 PDF
  • 正文语种 en
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