Abstract

Context. The induced magnetosphere of Venus is caused by the interaction of the solar wind and embedded interplanetary magnetic field with the exosphere and ionosphere of Venus. Solar Orbiter entered Venus’s magnetotail far downstream, > 70 Venus radii, of the planet and exited the magnetosphere over the north pole. This offered a unique view of the system over distances that had only been flown through before by three other missions, Mariner 10, Galileo, and BepiColombo. Aims. In this study, we study the large-scale structure and activity of the induced magnetosphere as well as the high-frequency plasma waves both in the magnetosphere and in a limited region upstream of the planet where interaction with Venus’s exosphere is expected. Methods. The large-scale structure of the magnetosphere was studied with low-pass filtered data and identified events are investigated with a minimum variance analysis as well as combined with plasma data. The high-frequency plasma waves were studied with spectral analysis. Results. We find that Venus’s magnetotail is very active during the Solar Orbiter flyby. Structures such as flux ropes and reconnection sites were encountered, in addition to a strong overdraping of the magnetic field downstream of the bow shock and planet. High-frequency plasma waves (up to six times the local proton cyclotron frequency) are observed in the magnetotail, which are identified as Doppler-shifted proton cyclotron waves, whereas in the upstream solar wind, these waves appear just below the proton cyclotron frequency (as expected) but are very patchy. The bow shock is quasi-perpendicular, however, expected mirror mode activity is not found directly behind it; instead, there is strong cyclotron wave power. This is most likely caused by the relatively low plasma-β behind the bow shock. Much further downstream, magnetic hole or mirror mode structures are identified in the magnetosheath.

Highlights

  • The interaction of the solar wind with the exosphere and ionosphere of Venus has given rise to the creation of a so-called induced magnetosphere

  • Further away from the planet, the interplanetary magnetic field (IMF) is transported by the solar wind velocity and gets draped around the planet leading to the creation of an induced magnetosphere

  • Where Bd and Bu are the downstream (12:39:40–12:39:46 UT) and upstream (12:39:54–12:40:00 UT) magnetic field vectors, respectively. This results in a normal direction nmc = ±(0.48, 0.61, −0.63), which results in an angle between normal and upstream magnetic field of ∠(B, nmc) ≈ 88◦, indicating a quasi-perpendicular bow shock

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Summary

Introduction

The interaction of the solar wind with the exosphere and ionosphere of Venus has given rise to the creation of a so-called induced magnetosphere (see e.g., Luhmann 1986; Phillips & McComas 1991; Bertucci et al 2011; Dubinin et al 2011; Futaana et al 2017). Downstream from the planet, a magnetotail is created, which consists of two lobes with oppositely directed magnetic fields, separated by a current sheet (e.g., Phillips & McComas 1991) Between these two lobes of stretched-out magnetic field and the bow shock exists the magnetosheath, where the slowed-down plasma gets accelerated back again to the pre-shocked solar wind velocity. The first flyby took place on 15 October 2020, approaching Venus from the upstream direction and leaving the neighbourhood of the planet via a long passage through the magnetotail During this flyby, evidence was found of draping in the magnetosheath in the direction perpendicular to the Venus-Sun line (Volwerk et al 2021), by field lines hanging up at Venus’s pile-up boundary on one side and being connected to the solar wind at the other, confirming previous finding with Venus Express (Delva et al 2017). Craft Potential (SCP; Khotyaintsev et al 2021; Hadid et al.2021)

Large structure of induced magnetosphere
Marked structures
Bow shock
High-frequency magnetic fluctuations
Ion cyclotron waves
Magnetosheath
Around the bow shock
Mirror modes and magnetic holes
Comparison with earlier missions
Conclusions
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