A mode equation for the resistive MHD ballooning mode in low beta tokamak magnetic geometry has been derived and analysed without imposing any ordering among the frequencies ω, ω o , (diamagnetic frequency) and ω D (magnetic drift frequency operator). Only a stable, ion diamagnetic mode has been found. The resistive ballooning mode is strongly stabilized by magnetic shear and toroidal effects.
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Hirose et al. (1989) studied this question.
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