
doi: 10.1063/1.864863
The response of a finite conductivity plasma to resonant magnetic perturbations is studied. The equations, which are derived for the time development of magnetic islands, help one to interpret the singular currents which occur under the assumption of perfect plasma conductivity. The relation to the Rutherford regime of resistive instabilities is given.
resonant magnetic perturbations, finite conductivity plasma, Ionized gas flow in electromagnetic fields; plasmic flow, magnetic islands, Magnetohydrodynamics and electrohydrodynamics, resistive instabilities
resonant magnetic perturbations, finite conductivity plasma, Ionized gas flow in electromagnetic fields; plasmic flow, magnetic islands, Magnetohydrodynamics and electrohydrodynamics, resistive instabilities
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