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Physics of Fluids B: Plasma Physics -- November 1990 -- Volume 2, Issue 11 pp. 2623-2635


Analytic boundary for resistive ballooning stability in the tokamak second-stable regime

G. Y. Fu and J. W. Van Dam
Institute for Fusion Studies, The University of Texas at Austin, Austin, Texas 78712
D. L. Holland, B. D. Fried, and A. Baños, Jr.
Department of Physics, University of California at Los Angeles, Los Angeles, California 90024-1547

(Received 19 April 1990; accepted 19 July 1990)

Analytical expressions for the marginal stability boundary for resistive ballooning modes at high beta are obtained in the limits of both large and small global shear. These results confirm the recent numerical finding of Sykes et al. [Plasma Phys. Controlled Fusion 29, 719 (1987)] that resistive ballooning modes are stable throughout most of the regime corresponding to ideal ballooning ``second stability'' in high-beta tokamaks. Physics of Fluids B: Plasma Physics is copyrighted by The American Institute of Physics.

DOI: 10.1063/1.859386
PACS: 52.30.Jb, 52.35.Py, 52.55.Fa        Additional Information


Citing Articles

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  1. Stability of short wavelength tearing and twisting modes
    F. L. Waelbroeck, Phys. Plasmas 6, 1208 (1999)


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