Abstract
A kinetic ballooning mode equation retaining full finite ion Larmor radius and ion magnetic drift resonance effects is derived by employing the high n ballooning mode formalism. It is found that the critical β is smaller than the ideal magnetohydrodynamic critical β, except that when ηi = 0(ηi≡d 1n Ti/d 1n N), they are identical. The finite Larmor radius effects reduce the growth rate but do not stabilize the mode. The ion magnetic drift resonance effects are destabilizing.
| Original language | English |
|---|---|
| Pages (from-to) | 1020-1026 |
| Number of pages | 7 |
| Journal | Physics of Fluids |
| Volume | 25 |
| Issue number | 6 |
| DOIs | |
| Publication status | Published - 1982 |
All Science Journal Classification (ASJC) codes
- Computational Mechanics
- Condensed Matter Physics
- Mechanics of Materials
- Mechanical Engineering
- Fluid Flow and Transfer Processes