Abstract

Abstract. Magnetic clouds (MCs) are large-scale magnetic flux ropes ejected from the Sun into the interplanetary space. They play a central role in solar–terrestrial relations as they can efficiently drive magnetic activity in the near-Earth environment. Their impact on the Earth's magnetosphere is often attributed to the presence of southward magnetic fields inside the MC, as observed in the upstream solar wind. However, when they arrive in the vicinity of the Earth, MCs first encounter the bow shock, which is expected to modify their properties, including their magnetic field strength and direction. If these changes are significant, they can in turn affect the interaction of the MC with the magnetosphere. In this paper, we use data from the Cluster and Geotail spacecraft inside the magnetosheath and from the Advanced Composition Explorer (ACE) upstream of the Earth's environment to investigate the impact of the bow shock's crossing on the magnetic structure of MCs. Through four example MCs, we show that the evolution of the MC's structure from the solar wind to the magnetosheath differs largely from one event to another. The smooth rotation of the MC can either be preserved inside the magnetosheath, be modified, i.e. the magnetic field still rotates slowly but at different angles, or even disappear. The alteration of the magnetic field orientation across the bow shock can vary with time during the MC's passage and with the location inside the magnetosheath. We examine the conditions encountered at the bow shock from direct observations, when Cluster or Geotail cross it, or indirectly by applying a magnetosheath model. We obtain a good agreement between the observed and modelled magnetic field direction and shock configuration, which varies from quasi-perpendicular to quasi-parallel in our study. We find that the variations in the angle between the magnetic fields in the solar wind and in the magnetosheath are anti-correlated with the variations in the shock obliquity. When the shock is in a quasi-parallel regime, the magnetic field direction varies significantly from the solar wind to the magnetosheath. In such cases, the magnetic field reaching the magnetopause cannot be approximated by the upstream magnetic field. Therefore, it is important to take into account the conditions at the bow shock when estimating the impact of an MC with the Earth's environment because these conditions are crucial in determining the magnetosheath magnetic field, which then interacts with the magnetosphere.

Highlights

  • Coronal mass ejections (CMEs) are tremendous eruptions in the solar corona during which the solar magnetic field and plasma are ejected into the interplanetary medium

  • The alteration of the magnetic field orientation across the bow shock can vary with time during the Magnetic clouds (MCs)’s passage and with the location inside the magnetosheath

  • We focus here on the magnetic structure of these MCs, i.e. the smooth rotation of their magnetic field, and how it evolves from the solar wind to the magnetosheath

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Summary

Introduction

Coronal mass ejections (CMEs) are tremendous eruptions in the solar corona during which the solar magnetic field and plasma are ejected into the interplanetary medium. Mach number conditions, which are often associated with MCs, accelerated flows, sometimes exceeding the solar wind speed, can be observed on the flanks of the magnetosheath and are attributed to the draping of the field lines (Lavraud and Borovsky, 2008; Lavraud et al, 2013) Such modifications of the magnetic field and velocity downstream of the bow shock are expected to affect the coupling between the solar wind and the magnetosphere (Lavraud and Borovsky, 2008). They investigate the impact of the bow shock’s crossing on synthetic flux ropes They find for certain flux ropes’ orientations that the direction of the MC’s magnetic field can vary significantly from the solar wind to the magnetosheath, sometimes exceeding 60◦ and occasionally causing a reversal of the Bz component.

Data sets
Description of the events
Event 1
Event 2: temporal variation of the MC’s structure
Event 3: spatial variation of the MC’s structure
Event 4: loss of the MC’s structure
Conditions at the bow shock
22 Apr 2001
Comparison with a magnetosheath model
20 May 2005 MC
22 April 2001 MC
22 January 2004 MC
Findings
Discussion and conclusions
Full Text
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