Techniques for controlling the instabilities that lead to major disruptions are reviewed and their applicability to different types of disruptions (density limit beta -limit, low-q, and disruptions driven by error fields) in investigated. Particular emphasis is given to schemes for controlling the m=2, n=1 resistive tearing mode, whether arising from error fields or from natural plasma instability.
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A.W. Morris (1992) studied this question.
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