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Title: Ballooning mode stability in the Hall-magnetohydrodynamics model

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.1851993· OSTI ID:20698363
;  [1]
  1. Courant Institute of Mathematical Sciences, New York University, New York, New York 10012 (United States)

The governing equations of the ballooning modes are derived within the Hall-magneto-hydrodynamics (HMHD) model and given a standard Hamiltonian form, which is then used to derive sufficient conditions for stability. In most cases, ideal magnetohydrodynamics (MHD) stability implies HMHD stability, as is the case for tokamak configurations if the pressure is a monotone increasing function of density and the entropy is monotone decreasing. The same result holds for general MHD plasmas with constant entropy and for incompressible plasmas. However, in the case of (compressible) closed-line systems such as the field-reversed configuration, or in a typical magnetospheric magnetic field, MHD ballooning stability does not guarantee HMHD stability. For the explicitly solvable configuration of the Z pinch it is in fact shown that the plasma can be MHD stable but HMHD unstable.

OSTI ID:
20698363
Journal Information:
Physics of Plasmas, Vol. 12, Issue 3; Other Information: DOI: 10.1063/1.1851993; (c) 2005 American Institute of Physics; Country of input: International Atomic Energy Agency (IAEA); ISSN 1070-664X
Country of Publication:
United States
Language:
English