Abstract

AbstractMercury is embedded in a tenuous and highly anisotropic sodium exosphere, generated mainly by plasma‐surface interactions. The absolute values of the sodium ion density are still under debate. Observations by MESSENGER's Fast Imaging Plasma Spectrometer (FIPS) instrument suggest the density of exospheric ions to be several orders of magnitude lower than the upstream solar wind density, indicating that the sodium exosphere has no substantial influence on the magnetospheric current systems. However, MESSENGER magnetic field observations of field line resonances revealed sodium ion densities comparable to the upstream solar wind density. To investigate how a dense exosphere would affect the current systems within Mercury's magnetosphere, we apply an established hybrid (kinetic ions, fluid electrons) model and conduct multiple model runs with gradually increasing exospheric density, ranging from no sodium ions at all to comet‐like configurations. We demonstrate how a sufficiently dense exosphere leads to self‐shielding of the sodium ion population from the ambient electric field and a significant inflation and symmetrization of Mercury's magnetosphere, which is decreasingly affected by the dipole offset. Once the sodium ion density is sufficiently high, Region 2 field‐aligned currents emerge close to the planet. The modeled Region 2 currents are located below the orbit of MESSENGER, thereby providing a possible explanation for the absence of these currents in observations. The sodium exosphere also closes a significant fraction of the Region 1 currents through Pedersen and Hall currents before the “guiding” magnetic field lines even reach the planetary surface. The modeled sodium ion and solar wind densities agree well with observations.

Highlights

  • IntroductionMercury's magnetic field at the equator is about 190 nT

  • Mercury, the first planet in our solar system, is the smallest in size with a radius of RM = 2,440 km (Smith et al, 2012) and the densest with its iron core taking up about 80% of its radius (Johnson et al, 2016)

  • Observations by MESSENGER's Fast Imaging Plasma Spectrometer (FIPS) instrument suggest the density of exospheric ions to be several orders of magnitude lower than the upstream solar wind density, indicating that the sodium exosphere has no substantial influence on the magnetospheric current systems

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Summary

Introduction

Mercury's magnetic field at the equator is about 190 nT It can either be described by a dipole that is antiparallel to its rotation axis, shifted northward by 0.2 RM (Anderson et al, 2012) or equivalently by a centered dipole superimposed with a significant quadrupole (Wicht & Heyner, 2017). The interaction of the weak Hermean magnetic field with the impinging solar wind results in a small magnetosphere that qualitatively resembles the Earth's magnetosphere. The high reconnection rate at Mercury is independent of the upstream interplanetary magnetic field (IMF) direction, and the Hermean magnetosphere is highly dynamic and susceptible to sudden variations of the upstream solar wind conditions (DiBraccio et al, 2013). Reconnection at the Hermean dayside magnetopause rather seems to be controlled by the difference in plasma β across the magnetopause (Poh et al, 2016)

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