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A&A 440, 357-366 (2005)
DOI: 10.1051/0004-6361:20052985
Wave energy dissipation by phase mixing in magnetic coronal plasmas
I. J. D. Craig and G. FruitUniversity of Waikato, New Zealand
e-mail: fruit@waikato.ac.nz
(Received 4 March 2005 / Accepted 2 May 2005 )
Abstract
Wave energy dissipation by viscous and resistive damping in magnetic coronal plasmas is examined. We begin by pointing out that since the dimensionless viscous damping coefficient
is
generally much greater than the dimensionless resistivity
, viscous dissipation can be
expected to be the dominant mechanism in many coronal applications. A detailed analysis is presented
for the case of perpendicular polarized shear wave disturbances
which propagate in a horizontally stratified magnetic channel. We show that when the equilibrium
field contains a neutral line (specifically,
) the
development of small length scales by phase mixing
leads to
efficient wave energy losses: in particular, the bulk of the energy
losses take place over the time interval
.
However, the later stages of the decay depends critically on
whether viscosity or resistivity provides the dominant damping
mechanism. When resistivity is sufficiently small the decay rate
weakens at later times due to the emergence of a
self-similar mode which allows a separation of the global kinetic and magnetic energies
(
). If the resistivity is large enough but still not
dominant, self-similar behaviour can give way to monotonic exponential damping on the
visco-resistive length scale
. In either
case, provided only that
, energy equipartition
eventually breaks down and the remnants of the initial
wave energy wind up mainly in the magnetic field.
Key words: Sun: corona -- magnetohydrodynamics (MHD) -- waves
© ESO 2005
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