Abstract

Abstract. Electron distributions in the magnetosheath display a number of far from equilibrium features. It has been suggested that one factor influencing these distributions may be the large distances separating locations at which electrons with different energies and pitch angles must cross the bowshock in order to reach a given point in the magnetosheath. The overall heating requirements at these distant locations depends strongly on the shock geometry. In the absence of collisions or other isotropization processes this suggests that the convolution of electrons arriving from different locations should give rise to asymmetries in the distribution functions. Moreover, such cross-talk could influence the relative electron to ion heating, rendering the shock heating problem intrinsically non-local in contrast to classic shock physics. Here, we study electron distributions measured simultaneously by the Plasma Electron and Current Experiment (PEACE) on board the Cluster spacecraft and the Electrostatic Analyser (ESA) on board THEMIS b during a time interval in which both the Cluster spacecraft and THEMIS b are in the magnetosheath, close to the bowshock, and during which the local magnetic field orientation makes it likely that electron trajectories may connect both spacecraft. We find that the relevant portions of the velocity distributions of such electrons measured by each spacecraft display remarkable similarities. We map trajectories of electrons arriving at each spacecraft back to the locations at which they crossed the bowshock, as a function of pitch angle and energy. We then use the Rankine-Hugoniot relations to estimate the heating of electrons and compare this with temperature asymmetries actually observed. We conclude that the electron distributions and temperatures in the magnetosheath depend heavily on non-local shock properties.

Highlights

  • The supersonic solar wind is interrupted upstream of the Earth at the bowshock, where the plasma’s flow is slowed, heated and deflected about the magnetopause, which separates the solar and terrestrial magnetic fields

  • This builds on suggestions based on observations of magnetosheath electron distributions (Paschmann et al, 1980; Feldman et al, 1983; Masood and Schwartz, 2008) that the electron heating is influenced by intrinsically global processes

  • We show that features in the electron distribution such as asymmetries about the pitch angle α = 90◦ can successfully be explained by comparing these with the total heating predicted by the RankineHugoniot relations at crossing locations

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Summary

Introduction

The supersonic solar wind is interrupted upstream of the Earth at the bowshock, where the plasma’s flow is slowed, heated and deflected about the magnetopause, which separates the solar and terrestrial magnetic fields. In this paper we will investigate the impact of the global, curved nature of the bow shock on the shock-related electron heating and dynamics This builds on suggestions based on observations of magnetosheath electron distributions (Paschmann et al, 1980; Feldman et al, 1983; Masood and Schwartz, 2008) that the electron heating is influenced by intrinsically global processes. Electrons travel along magnetic field lines which meet the bowshock at locations which may be separated by large distances, where the shock conditions are different. Distributions of electrons whose trajectories connecting both spacecraft are studied, Rankine-Hugoniot predictions of total heating at bowshock crossing locations are related to distribution asymmetries in Sect.

Data sets
Rankine-Hugoniot relations
Electron trajectories
Results
Bowshock crossing locations for electrons
THEMIS and Cluster electron distributions
Comparison of Rankine-Hugoniot predictions with spacecraft data
Conclusion
Full Text
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