Issue |
A&A
Volume 402, Number 3, May II 2003
First Science with the ODIN satellite
|
|
---|---|---|
Page(s) | 1129 - 1143 | |
Section | The Sun | |
DOI | https://doi.org/10.1051/0004-6361:20030312 | |
Published online | 23 April 2003 |
Coupling of fast and Alfvén waves in a straight bounded magnetic field with density stratification
Departament de Física, Universitat de les Illes Balears, 07122 Palma de Mallorca, Spain e-mail: arregi@hubble.uib.es;ramon.oliver@uib.es;dfsjlb0@uib.es
Corresponding author: J. L. Ballester, dfsjlb0@uib.es
Received:
8
October
2002
Accepted:
14
February
2003
The theoretical understanding of the linear standing or propagating
magnetohydrodynamic waves in a variety of solar coronal structures is far from
complete since analytical solutions to the linearised MHD equations can only be
found for very simple magnetic configurations. In this paper, we use a
numerical code to solve the linear fast and Alfvén wave equations in a very
simple, bounded magnetic configuration that incorporates two features that are
not usually considered in similar works, namely the longitudinal magnetic
field component and wave propagation in the longitudinal direction (). We use a numerical code (Arregui et al. 2001) that has been modified by
including a staggered mesh that allows us to properly capture the spatial
behaviour of solutions to the wave equations. Coupling between fast and
Alfvén modes has been studied in detail and it has been found that it does
not take place when the longitudinal field component is zero and the frequency
of the fast mode is outside the Alfvén
continuum with the same spatial structure along field lines. Under these
circumstances, fast modes retain their global spatial behaviour and are also
characterised by
varying linearly with
, such as in a uniform
medium (although here the Alfvén speed changes exponentially in the direction
normal to field lines). Regarding mode coupling, its main feature is the blend
of fast and Alfvén solutions with close frequencies in some modes with a
mixture of their properties, namely discontinuities or jumps around certain
magnetic surfaces (such as in pure Alfvén waves), global spatial distribution
of the normal velocity component and non-zero density perturbations (such as in
fast waves).
Key words: magnetohydrodynamics (MHD) / methods: numerical / Sun: oscillations / Sun: magnetic fields
© ESO, 2003
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