Equilibria for the BIG DEE (Doublet III upgrade) are obtained which are optimized with respect to both shape and current profile for stability to ideal-MHD modes. With a wall reasonably far from the plasma surface, it is inferred that the external kink constrains q s to be above 2.0, where q s is the plasma surface value of the safety factor, and the ballooning mode limits the value of beta. Then, stable BIG DEE equilibria with beta at least as large as 17% can be found. The wall position necessary to stabilize the n = 1 and n = 2 kink modes is outside the coils and the equilibrium is stable for n ≥ 3 with a wall at infinity. This equilibrium is not in a separated second stability region and thus there are no problems regarding accessibility.
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Helton et al. (1985) studied this question.
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