Ion Escape From Degenerate Induced Magnetospheres: The Case of Mars

Abstract When the cone angle of the interplanetary magnetic field (IMF) becomes small, induced magnetospheres of unmagnetized planets degenerate. Using hybrid simulations, we study ionospheric ion escape in a 4° cone angle case and compare it with the nominal 55° cone angle (Parker spiral) case. The total escape rate is , nearly an order of magnitude higher than the nominal rate of . The escape probability is four times higher. The unique feature of the degenerate induced magnetosphere is the upstream escape driven by the ambipolar electric field, contributing 42% to the total escape, a channel absent in the nominal case. Additionally, 52% of escape occurs through a cross‐flow plume, formed by the drift of ionospheric ions in the weak convective field and IMF. This channel is dominant, exhibiting an intensity seven times greater than that of the plume driven by the convective electric field in the nominal case.

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Publication Details

Journal
Geophysical Research Letters
Published
2025-06-19
DOI
https://doi.org/10.1029/2025gl116161
Primary Topic
Planetary Science and Exploration
Type
article
Field-Weighted Citation Impact
0.00

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article

Ion Escape From Degenerate Induced Magnetospheres: The Case of Mars

Mats Holmström, Xiao‐Dong Wang, H. Nilsson, Yoshifumi Futaana et al.
Geophysical Research Letters
Planetary Science and Exploration
article

Ion Escape From Degenerate Induced Magnetospheres: The Case of Mars

Mats Holmström, Xiao‐Dong Wang, H. Nilsson, Yoshifumi Futaana, C. M. Fowler, Robin Ramstad, Qi Zhang, S. Barabash
article en

Abstract

Abstract When the cone angle of the interplanetary magnetic field (IMF) becomes small, induced magnetospheres of unmagnetized planets degenerate. Using hybrid simulations, we study ionospheric ion escape in a 4° cone angle case and compare it with the nominal 55° cone angle (Parker spiral) case. The total escape rate is , nearly an order of magnitude higher than the nominal rate of . The escape probability is four times higher. The unique feature of the degenerate induced magnetosphere is the upstream escape driven by the ambipolar electric field, contributing 42% to the total escape, a channel absent in the nominal case. Additionally, 52% of escape occurs through a cross‐flow plume, formed by the drift of ionospheric ions in the weak convective field and IMF. This channel is dominant, exhibiting an intensity seven times greater than that of the plume driven by the convective electric field in the nominal case.

Geophysical Research LettersVol. 52(12)
West Virginia University (US), Swedish Institute of Space Physics (SE), University of Colorado Boulder (US), Laboratory for Atmospheric and Space Physics (US), Umeå University (SE)
U.S. Department of Energy, Swedish National Space Agency, Umeå Universitet, National Nuclear Security Administration
Openalex Percentile: Top 91%
Planetary Science and Exploration
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Ion Escape From Degenerate Induced Magnetospheres: The Case of Mars — Mats Holmström, Xiao‐Dong Wang, et al. · Geophysical Research Letters (2025) | TGRS Research Map | TGRS