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Magnetohydrodynamic equilibria of a cylindrical plasma with poloidal mass flow and arbitrary cross section shape

机译:圆柱形等离子体的磁流体动力学平衡   质量流量和任意截面形状

摘要

The equilibrium of a cylindrical plasma with purely poloidal mass flow andcross section of arbitrary shape is investigated within the framework of theideal MHD theory. For the system under consideration it is shown that onlyincompressible flows are possible and, conscequently, the general twodimensional flow equilibrium equations reduce to a single second-orderquasilinear partial differential equation for the poloidal magnetic fluxfunction $\psi$, in which four profile functionals of $\psi$ appear. Apart froma singularity occuring when the modulus of Mach number associated with theAlfv\'en velocity for the poloidal magnetic field is unity, this equation isalways elliptic and permits the construction of several classes of analyticsolutions. Specific exact equlibria for a plasma confined within a perfectlyconducting circular cylindrical boundary and having i) a flat current densityand ii) a peaked current density are obtained and studied.
机译:在理想的MHD理论的框架内,研究了具有纯极向质量流量和任意形状横截面的圆柱等离子体的平衡。对于所考虑的系统,表明只有不可压缩的流动是可能的,因此,一般的二维流动平衡方程简化为用于单极磁通函数$ \ psi $的单个二阶拟线性偏微分方程,其中四个轮廓函数为$ \ psi $出现。除了与极磁场的Alfv'en速度相关的马赫数模量为1时发生奇异性之外,该方程始终为椭圆形,并允许构造几类分析解。获得并研究了等离子体的特定精确平衡,该等离子体被限制在完全导电的圆柱形边界内,并且具有i)平坦的电流密度和ii)峰值电流密度。

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  • 作者单位
  • 年度 1996
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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