首页> 外文OA文献 >Effects of hot electrons on the stability of a closed field line plasma
【2h】

Effects of hot electrons on the stability of a closed field line plasma

机译:热电子对闭合场线等离子体稳定性的影响

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

Motivated by the electron cyclotron heating being employed on dipole experiments, the effects of a hot species on stability in closed magnetic field line geometry are investigated. The interchange stability of a plasma consisting of a fluid background with a population of kinetic hot electrons is considered. The species diamagnetic drift and magnetic drift frequencies are assumed to be of the same order, and the wave frequency is assumed to be much larger than the background drift frequencies. To illustrate the key physics issues and obtain an simpler understanding of instability mechanisms, we first examine the effects of hot electrons in cylindrical Z-pinch geometry. This linear approximation to a dipole preserves the essential feature of closed magnetic field lines. The absence of variations along the equilibrium magnetic field allows us to analytically derive an arbitrary total pressure dispersion relation, investigate a large variety of regimes, and explain the physical phenomena at work. Our analysis finds that two different types of resonant hot electron effects can modify the simple Magnetohydrodynamic (MHD) interchange stability condition. When the azimuthal magnetic field increases with radius, there is a critical pitch angle above which the magnetic drift of the hot electrons reverses. The interaction of the wave with the hot electrons with pitch angles near this critical value always results in instability. When the magnetic field decreases with radius, magnetic drift reversal is not possible and only low speed hot electrons interact with the wave. Destabilization by this weaker resonance effect can be avoided by carefully controlling the hot electron density and temperature profiles.
机译:在偶极实验中采用电子回旋加速器加热的动机,研究了热物质对封闭磁场线几何形状稳定性的影响。考虑了由流体本底和动力学热电子组成的等离子体的交换稳定性。假设种类的反磁性漂移和磁性漂移频率是相同数量级,并且假设波频率比背景漂移频率大得多。为了说明关键的物理问题并获得对不稳定性机理的更简单理解,我们首先检查圆柱形Z形捏合几何中热电子的影响。偶极子的线性近似保留了闭合磁场线的基本特征。沿着平衡磁场没有变化,这使我们能够分析得出任意的总压力色散关系,研究各种各样的状态,并解释工作中的物理现象。我们的分析发现,两种不同类型的共振热电子效应可以修改简单的磁流体动力学(MHD)交换稳定性条件。当方位磁场随半径增加时,存在一个临界俯仰角,在该临界俯仰角以上,热电子的磁漂移会反转。波与俯仰角接近此临界值的热电子的相互作用始终会导致不稳定。当磁场随半径减小时,不可能实现磁漂移反转,并且只有低速热电子与波相互作用。通过仔细控制热电子密度和温度曲线,可以避免这种较弱的共振效应造成的不稳定。

著录项

  • 作者

    Krasheninnikova Natalia S;

  • 作者单位
  • 年度 2006
  • 总页数
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号