Confinement of a self‐stabilized tokamak under average magnetic well conditions
It is well known that the average favorable magnetic curvature of a tokamak is stabilizing with respect to pressure‐driven magnetohydrodynamic instabilities at low beta and that self‐stabilization occurs at finite beta in the so‐called second stability regime. Here it is self‐consistently investigat...
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Veröffentlicht in: | Phys. Fluids; (United States) 1988-01, Vol.31 (1), p.213-215 |
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Format: | Artikel |
Sprache: | eng |
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