Abstract

Context. Observations have shown that twisted magnetic fields naturally occur, and indeed are omnipresent in the Sun's atmosphere. It is therefore of great theoretical interest in solar atmospheric waves research to investigate the types of magnetohydrodynamic (MHD) wave modes that can propagate along twisted magnetic flux tubes. Aims. Within the framework of ideal MHD, the main aim of this work is to investigate small amplitude incompressible wave modes of twisted magnetic flux tubes with m more or equal 1. The axial magnetic field strength inside and outside the tube will be allowed to vary, to ensure the results will not be restricted to only cold plasma equilibria conditions. Methods. The dispersion equation for these incompressible linear MHD wave modes was derived analytically by implementing the long wavelength approximation. Results. It is shown, in the long wavelength limit, that both the frequency and radial velocity profile of the m = 1 kink mode are completely unaffected by the choice of internal background magnetic twist. However, fluting modes with m more or equal 2 are sensitive to the particular radial profile of magnetic twist chosen. Furthermore, due to background twist, a low frequency cut-off is introduced for fluting modes that is not present for kink modes. From an observational point of view, although magnetic twist does not affect the propagation of long wavelength kink modes, for fluting modes it will either work for or against the propagation, depending on the direction of wave travel relative to the sign of the background twist.

Highlights

  • An axially symmetric, vertical and magnetically twisted flux tube is a convenient model for analytical studies of various magnetohydrodynamic (MHD) perturbations

  • In contrast to the kink mode, Eq (41) shows that a low frequency cut-off is introduced for fluting modes due to background twist

  • Special attention was given to the problem of finding the eigenvalues and eigenfunctions of modes with m ≥ 1 in the long wavelength limit

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Summary

Introduction

Vertical and magnetically twisted flux tube is a convenient model for analytical studies of various magnetohydrodynamic (MHD) perturbations. Filippov (2007) and Vršnak (2008) assume that external magnetic field decreases with distance from the tube boundary inversely proportional to the radius, that is, as a function of 1/r This approximation was previously used by, for example, Erdélyi & Fedun (2006), Ruderman (2015), Giagkiozis et al (2015). Giagkiozis et al (2015) has shown that the wave solution for a background constant twist outside the tube is very close to the solution when the twist is proportional to 1/r From another point of view, by taking into account plasma conductivity, the external magnetic field does not penetrate significantly through the tube boundary and, can be neglected

Derivation of linear radial component wave equation
Boundary conditions
Comparison with previous results
Conclusions
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