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A&A 490, 493-500 (2008)
DOI: 10.1051/0004-6361:200809605
On the linear theory of Kelvin-Helmholtz instabilities of relativistic magnetohydrodynamic planar flows
Z. Osmanov1, A. Mignone1, 2, S. Massaglia1, G. Bodo2, and A. Ferrari11 Dipartimento di Fisica Generale, Universitá degli Studi di Torino, via Pietro Giuria 1, 10125 Torino, Italy
e-mail: z.osmanov@astro-ge.org; osmanov@ph.unito.it
2 INAF/Osservatorio Astronomico di Torino, Strada Osservatorio 20, 10025 Pino Torinese, Italy
Received 19 February 2008 / Accepted 1 August 2008
Abstract
Aims. We investigate the linear stability properties of the plane interface separating two
relativistic magnetized flows in motion with respect to each other.
The two flows are governed by the (special) relativistic equations
for a magnetized perfect gas in the infinite conductivity approximation.
Methods. By adopting the vortex-sheet approximation, the relativistic magnetohydrodynamics
equations are linearized around the equilibrium
state and the corresponding dispersion relation is derived and discussed.
The behavior of the configuration and the regimes of instability are investigated
following the effects of four physical parameters: the flow velocity,
the relativistic and Alfvénic Mach numbers, and the inclination of
the wave vector on the plane of the interface.
Results. From the numerical solution of the dispersion relation, we find
in general two separate regions of instability, associated with the
slow and fast magnetosonic modes respectively.
Modes parallel to the flow velocity are destabilized only for
sufficiently low magnetization.
For the latter case, stabilization is attained, in addition, at
sufficiently large relativistic velocities between the two flows in relative motion.
Conclusions. We briefly comment the relevance of these results to the study of the
stability of astrophysical jets.
Key words: magnetohydrodynamics (MHD) -- instabilities -- plasmas
© ESO 2008
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