Abstract
Relaxation of plasmas via turbulence is treated by the use of a maximum entropy principle. The relaxed states are always stable to ideal modes. Taylor's theory of field reversal is extended to finite pressure plasmas and given a rigorous support by using symmetries in the equations to determine preferred conservation laws. Relaxed states of field reversed θ pinches are predicted, some with self-reversal of the magnetic field.
Original language | English (US) |
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Pages (from-to) | 1855-1862 |
Number of pages | 8 |
Journal | Physics of Fluids |
Volume | 25 |
Issue number | 10 |
DOIs | |
State | Published - 1982 |
ASJC Scopus subject areas
- Computational Mechanics
- Condensed Matter Physics
- Mechanics of Materials
- Mechanical Engineering
- Fluid Flow and Transfer Processes