
doi: 10.1063/1.871585
handle: 11858/00-001M-0000-0027-8C9E-A
Magnetic perturbations that drive islands are shielded from a rotating plasma by either a torque limit or an equilibrium limit. The physics of the shielding is given in a simple slab model along with the mechanism by which the shielding currents are maintained. Shielding currents in a channel of width Δ are damped by a resistance η/Δ with η the resistivity. If an island is shielded in a nearly ideal plasma, η/Δ=(μ0/π)VpAM2p with VpA the poloidal Alfvén speed, Mp≡v⊥/VpA, and v⊥ the speed of the cross-field flow at the resonance surface.
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