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Phys. Plasmas 5, 2921 (1998); http://dx.doi.org/10.1063/1.873014 (11 pages)
Toroidally localized and nonlocalized ballooning instabilities in a stellarator
(Received 19 January 1998; accepted 27 April 1998)
It is shown that the coexistence of toroidally nonlocalized ideal-hydromagnetic ballooning instabilities, with a quasidiscrete spectrum, and toroidally localized ballooning instabilities with a broad continuous spectrum, as predicted by Dewar and Glasser [Phys. Fluids 26, 3038 (1983)] can be realized in a Mercier-unstable equilibrium case modeling the Large Helical Device (LHD) [A. Iiyoshi et al., Fusion Technol. 17, 148 (1990)] with a broad pressure profile. The quasidiscrete, interchange branch corresponds to extended modes that can be understood on the basis of a ripple-averaged ballooning equation, whereas the broad-continuum, ballooning branch corresponds to modes localized along a flux tube. The physical origin of the two branches is discussed. © 1998 American Institute of Physics.
© 1998 American Institute of Physics
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R. L. Dewar and A. H. Glasser, Phys. Fluids 26, 3038 (1983)PFLDAS000026000010003038000001.
N. Nakajima, Phys. Plasmas 3, 4556 (1996)PHPAEN000003000012004556000001.
A. H. Boozer, Phys. Fluids 25, 520 (1982)PFLDAS000025000003000520000001.
R. L. Dewar, D. A. Monticello, and W. N.-C. Sy, Phys. Fluids 27, 1723 (1984)PFLDAS000027000007001723000001.
E. D. Fredrickson, K. M. McGuire, Z. Y. Chang, A. Janos, J. Manickam, G. Taylor, S. Mironov, I. Semenov, D. Kislov, and D. Martynov, Phys. Plasmas 3, 2620 (1996)PHPAEN000003000007002620000001.
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