Plasma instability

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Instabilities in plasmas are often referred to as 'modes'. Strictly speaking, these terms correspond to different concepts:

  • Instability: the existence of an instability is determined by calculating the growth rate of an infinitesimal perturbation. If this growth rate is positive, the perturbation is unstable.
  • Mode: a (normal) mode is a (global) solution of a (linear) evolution equation. Typically, this solution is a (standing or propagating) wave. The linearity of the equation allows any solution to be decomposed into a sum of mutually orthogonal normal modes. If the equation is non-linear, the term 'mode' has to be used with caution.

Plasma instabilities can be classified into a number of types according to their drive (or free energy source):

  • Rayleigh-Taylor instabilities due to density gradients or boundaries, associated with non-electromagnetic forces (e.g., gravity)
  • Gradient driven instabilities, associated with thermodynamic forces due to gradients in an otherwise Maxwellian plasma
  • Kinetic instabilities, associated with deviations from Maxwellianity, i.e., the anisotropy of the velocity distribution function
  • Streaming instabilities, associated with energetic particles or electric currents interacting with the plasma, producing waves

Below is a list of some instabilities relevant to fusion plasmas (to be completed).

  • Alfvén eigenmodes
  • Ballooning instability
  • Drift wave instability
  • Edge Localized Modes
  • Electron Temperature Gradient instability
  • Flute instability
  • Geodesic Acoustic Mode
  • Interchange instability
  • Ion Temperature Gradient instability
  • Kink instability
  • Sausage instability
  • Tearing mode instability, see also Magnetic island
  • Whistler mode

See also