Abstract
The Flux Conserving Tokamak (FCT) model suggested that rapid heating would yield equilibria with high relative energy density (..beta.. = 2p/B/sup 2/) while nonetheless allowing control over q, the so-called safety factor for instability within the ideal magnetohydrodynamic (MHD) plasma model. In this study, we show that this is adequate to provide stability to ..beta.. values of 10%, if there is a conducting metal shell in the vicinity of the plasma.
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