Abstract

AbstractThis paper investigates the excitation of waveguide modes in a nonuniform dipole equilibrium and, further, their coupling to field line resonances (FLRs). Waveguide modes are fast compressional ultralow frequency (ULF) waves, whose structure depends upon the magnetospheric equilibrium and the solar wind driving conditions. Using magnetohydrodynamic simulations, we consider how the structure of the excited waveguide mode is affected by various forms of magnetopause driving. We find that the waveguide supports a set of normal modes that are determined by the equilibrium. However, the particular normal modes that are excited are determined by the structure of the magnetopause driver. A full understanding of the spatial structure of the normal modes is required in order to predict where coupling to FLRs will occur. We show that symmetric pressure driving about the noon meridian can excite normal modes which remain around to drive resonances for longer than antisymmetric driving. Further, the critical quantity in terms of efficient coupling is the magnetic pressure gradient aligned with the resonance.

Highlights

  • The propagation of fast magnetohydrodynamic (MHD) waves in the outer magnetosphere has been studied extensively

  • This paper investigates the excitation of waveguide modes in a nonuniform dipole equilibrium and, further, their coupling to field line resonances (FLRs)

  • Waveguide modes are fast compressional ultralow frequency (ULF) waves, whose structure depends upon the magnetospheric equilibrium and the solar wind driving conditions

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Summary

Introduction

The propagation of fast magnetohydrodynamic (MHD) waves in the outer magnetosphere has been studied extensively. The cavity supports a discrete set of normal modes since the azimuthal wavenumber is, by the nature of the closed system, quantized This is well elucidated in simulations presented by Wright and Rickard (1995), where a cavity is driven with a solar wind-like broadband spectrum. The value of specific parameters used in each of the simulations will be stated in the corresponding section

Changing the Alfvén Speed Gradient
Effect of Driver Symmetry
Changing the Driver Location
Fast Mode Nodal Structure
Findings
Concluding Remarks
Full Text
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