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arXiv 1002.3499physics.plasm-phnlin.CD
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磁场在支撑等离子体压力间断的环形表面上延拓的Hamilton-Jacobi理论

Hamilton--Jacobi theory for continuation of magnetic field across a toroidal surface supporting a plasma pressure discontinuity

M. McGann, S. R. Hudson, R. L. Dewar, G. von Nessi

摘要:

消失的发散的总应力张量(磁加动力学)在附近的平衡等离子体包含一个环形表面的不连续性给出边界和跳跃条件,强烈约束允许的连续性的磁场在整个表面。边界条件允许的磁场两侧的不连续表面被描述的表面磁势,减少了连续性问题,解决一个哈密尔顿-雅可比方程。该方程的特征服从汉密尔顿运动方程,而一般环曲面上存在连续场的必要条件是该汉密尔顿系统的相空间中存在不变环面。从伯克霍夫定理可以看出,存在这样一个不变的环面,一般来说,也足以使延拓成为可能。一个重要的推论是不连续表面上的连续场的旋转变换一般必须是无理数。

英文摘要:

The vanishing of the divergence of the total stress tensor (magnetic plus kinetic) in a neighborhood of an equilibrium plasma containing a toroidal surface of discontinuity gives boundary and jump conditions that strongly constrain allowable continuations of the magnetic field across the surface. The boundary conditions allow the magnetic fields on either side of the discontinuity surface to be described by surface magnetic potentials, reducing the continuation problem to that of solving a Hamilton--Jacobi equation. The characteristics of this equation obey Hamiltonian equations of motion, and a necessary condition for the existence of a continued field across a general toroidal surface is that there exist invariant tori in the phase space of this Hamiltonian system. It is argued from the Birkhoff theorem that existence of such an invariant torus is also, in general, sufficient for continuation to be possible. An important corollary is that the rotational transform of the continued field on a surface of discontinuity must, generically, be irrational.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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