Numerical Calculations Demonstrating Complete Stabilization of the Ideal Magnetohydrodynamic Resistive Wall Mode by Longitudinal Flow

S. Smith, S.C. Jardin, J.P. Freidberg, L. Guazzotto

Princeton University. Plasma Physics Laboratory.

关键词: Finite Element Method, Kink Instability;    Resonance;    70 Plasma Physics And Fusion Technology;    Plasma;    Stability;   

RP-ID  :  PPPL-4409
RP-ID  :  DE-ACO2-09CH11466
RP-ID  :  953216

美国|英语

来源: UNT Digital Library

【 摘 要 】

The cylindrical ideal magnetohydrodynamic (MHD) stability problem, including ow and a resistive wall, is cast in the standard mathematical form, ωA⋅x = B⋅x, without discretizing the vacuum regions surrounding the plasma. This is accomplished by means of a finite element expansion for the plasma perturbations, by coupling the plasma surface perturbations to the resistive wall using a Green's function approach, and by expanding the unknown vector, x, to include the perturbed current in the resistive wall as an additional degree of freedom. The ideal MHD resistive wall mode (RWM) can be stabilized when the plasma has a uniform equilibrium ow such that the RWM frequency resonates with the plasma's Doppler-shifted sound continuum modes. The resonance induces a singularity in the parallel component of the plasma perturbations, which must be adequately resolved. Complete stabilization within the ideal MHD model (i.e. without parallel damping being added) is achieved as the grid spacing in the region of the resonance is extrapolated to 0 step size