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Title: Extending the collisional fluid equations into the long mean-free-path regime in toroidal plasmas. II. Frequency dependence

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.1947628· OSTI ID:20764399
 [1]
  1. Engineering Physics Department, University of Wisconsin, Madison, Wisconsin 53706 (United States)

In Part I [K. C. Shaing and D. A. Spong, Phys. Fluids B 2, 1190 (1990)], an expression for the pressure anisotropy that is valid in the plateau regime is derived from the linear drift kinetic equation that is driven by the plasma flows. To apply this expression to investigate the magnetohydrodynamic instabilities, a more general frequency-dependent pressure anisotropy is calculated here for both the plateau regime and the collisional fluid regime for toroidal plasmas with arbitrary symmetry property. It is found that when the growth rate of the mode is larger than the typical particle transit frequency and the collision frequency, the pressure anisotropy scales inversely with the mode growth rate instead of the collision frequency. It is also shown that when {nu}{sub k} in Eqs. (6) and (7) of a previous paper [K. C. Shaing, Phys. Fluids B 5, 3841 (1993)] is replaced by ({nu}{sub k}+{gamma}), equilibrium time-dependent plasma viscosities for toroidal plasmas are obtained. Here, {nu}{sub k} is the Coulomb collision frequency and {gamma} is the plasma flow damping rate.

OSTI ID:
20764399
Journal Information:
Physics of Plasmas, Vol. 12, Issue 7; Other Information: DOI: 10.1063/1.1947628; (c) 2005 American Institute of Physics; Country of input: International Atomic Energy Agency (IAEA); ISSN 1070-664X
Country of Publication:
United States
Language:
English