Abstract

Abstract. Magnetic reconnection can be a continuous or a transient process. Global magnetohydrodynamics (MHD) simulations are important tools to understand the relevant magnetic reconnection mechanisms and the resulting magnetic structures. We have studied magnetopause reconnection using a global 3-D MHD simulation in which the interplanetary magnetic field (IMF) has been set to large positive By and large negative Bz components, i.e., a south-duskward direction. Flux tubes have been observed even during these constant solar wind conditions. We have focused on the interlinked flux tubes event resulting from time-dependent, patchy and multiple reconnection. At the event onset, two reconnection modes seem to occur simultaneously: a time-dependent, patchy and multiple reconnection for the subsolar region; and, a steady and large-scale reconnection for the regions far from the subsolar site.

Highlights

  • Magnetic reconnection has been considered a dominant mechanism for solar wind mass, momentum and energy transfer to the magnetosphere

  • In this paper we investigate the formation of flux transfer events (FTEs) and magnetic reconnection at the subsolar magnetopause using a global 3-D MHD simulation under a large amplitude southduskward interplanetary magnetic field (IMF)

  • This paper presents results from a global 3-D MHD simulation under a large south-duskward IMF

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Summary

Introduction

Magnetic reconnection has been considered a dominant mechanism for solar wind mass, momentum and energy transfer to the magnetosphere. Flux tubes generated by the single and multiple X line models may have cross-sections of about 1 RE2, but long azimuthal extent along the magnetopause (Southwood et al, 1988; Scholer, 1988; Lee and Fu, 1985). Lee et al (1993) claim that the evolution of the interlinked flux tubes would be a consequence of further reconnection, leading to one tube connected only to the geomagnetic field and the other tube only to the IMF This characteristic may not be observed in a MHD simulation using localized sites of enhanced resistivity (Lee et al, 1993).

Simulation description
Results
Interlinked flux tubes
A glance after the interlinked flux tubes event
Conclusions

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