Abstract
High-beta (β»ε/q2) large-aspect-ratio (ε«1) tokamak equilibria are shown to be always stable to ideal magnetohydrodynamics (MHD) modes that are localized about a flux surface. Both the ballooning and interchange modes are shown to be stable. This work uses the analytic high-beta large-aspect-ratio tokamak equilibria developed by Cowley et al. [Phys. Fluids B 3, 2069 (1991)], which are valid for arbitrary pressure and safety factor profiles. The stability results make no assumption about these profiles nor the shape of the boundary.
Original language | English (US) |
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Pages (from-to) | 3357-3362 |
Number of pages | 6 |
Journal | Physics of Fluids B |
Volume | 3 |
Issue number | 12 |
DOIs | |
State | Published - 1991 |
All Science Journal Classification (ASJC) codes
- Computational Mechanics
- Condensed Matter Physics
- Mechanics of Materials
- Physics and Astronomy(all)
- Fluid Flow and Transfer Processes