Abstract
The theory of curvature-driven instabilities is developed for a plasma interacting with a hot electron ring whose drift frequencies are larger than the growth rates predicted from conventional magnetohydrodynamic theory. A z-pinch model is used to emphasize the radial structure of the problem. Stability criteria are obtained for the five possible modes of instability: the conventional hot electron interchange, a high-frequency hot electron interchange (at frequencies larger than the ion cyclotron frequency), a compressional instability, a background pressure-driven interchange, and an interacting pressure-driven interchange. Numerical plots of the marginal stability boundaries are presented for parameter values corresponding to the EBT-S and EBT-P bumpy torus experiments.
| Original language | English |
|---|---|
| Pages (from-to) | 201-215 |
| Number of pages | 15 |
| Journal | Physics of Fluids |
| Volume | 26 |
| Issue number | 1 |
| DOIs | |
| State | Published - 1983 |
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