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Finite beta stabilization of the kinetic ion mixing mode. (English) Zbl 0586.76075

The full finite-beta local dispersion relation of the ion mixing mode is derived and analyzed, using kinetic theory. The physical mechanism of finite-beta stabilization of a single (i.e., fixed wavenumber, \(k_ zr_ n\) and \(b_ i\) constant) ion mixing mode is discussed. The distortion of the resonant region, in velocity space (by \(\nabla B\) drifts) and the coupling to the shear Alfvén wave are shown to be the important stabilization mechanisms. It is found that high values of \(\beta\) \((\beta >\beta_ c\), where \(\beta_ c=0.1\to 1.0\), for relevant parameters) are necessary for stabilization.

MSC:

76E25 Stability and instability of magnetohydrodynamic and electrohydrodynamic flows
76X05 Ionized gas flow in electromagnetic fields; plasmic flow
82D10 Statistical mechanics of plasmas
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