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Title: Stability of force-free Taylor states in a new version of magnetic flux-averaged magnetohydrodynamics

Journal Article · · Physics of Plasmas
DOI:https://doi.org/10.1063/1.871833· OSTI ID:253482
 [1];  [2]
  1. Max-Planck-Insitut fur Plasmaphysik, EURATOM Association, D-8046, Garching (Germany)
  2. Laboratory of Plasma Studies, Cornell University, Ithaca, New York 14853 (United States)

It is observed that the recently developed magnetic flux-averaged magnetohydrodynamics (AMHD) [Phys. Plasmas {bold 1}, 2488 (1994)] is incompatible with Taylor{close_quote}s theorem, which states that the lowest-energy state of force-free equilibria based on the conservation of the helicity integral is absolutely stable for vanishingly small resistivity. By a modification of the Lagrangian from which AMHD is derived, a modified version of AMHD that is compatible with Taylor{close_quote}s theorem is obtained. It also provides an energy principle for examining the linear instability of resistive equilibria, which has a great advantage over resistive MHD. {copyright} {ital 1996 American Institute of Physics.}

DOE Contract Number:
FG02-93ER54221
OSTI ID:
253482
Journal Information:
Physics of Plasmas, Vol. 3, Issue 1; Other Information: PBD: Jan 1996
Country of Publication:
United States
Language:
English

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