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Ion Dynamics at the Magnetopause of Ganymede
We study the dynamics of the thermal O(+) and H(+) ions at Ganymede's magnetopause when Ganymede is inside and outside of the Jovian plasma sheet using a three‐dimensional hybrid model of plasma (kinetic ions, fluid electrons). We present the global structure of the electric fields and power de...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9286830/ https://www.ncbi.nlm.nih.gov/pubmed/35865030 http://dx.doi.org/10.1029/2021JA029863 |
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author | Fatemi, S. Poppe, A. R. Vorburger, A. Lindkvist, J. Hamrin, M. |
author_facet | Fatemi, S. Poppe, A. R. Vorburger, A. Lindkvist, J. Hamrin, M. |
author_sort | Fatemi, S. |
collection | PubMed |
description | We study the dynamics of the thermal O(+) and H(+) ions at Ganymede's magnetopause when Ganymede is inside and outside of the Jovian plasma sheet using a three‐dimensional hybrid model of plasma (kinetic ions, fluid electrons). We present the global structure of the electric fields and power density (E ⋅ J) in the magnetosphere of Ganymede and show that the power density at the magnetopause is mainly positive and on average is +0.95 and +0.75 nW/m(3) when Ganymede is inside and outside the Jovian plasma sheet, respectively, but locally it reaches over +20 nW/m(3). Our kinetic simulations show that ion velocity distributions at the vicinity of the upstream magnetopause of Ganymede are highly non‐Maxwellian. We investigate the energization of the ions interacting with the magnetopause and find that the energy of those particles on average increases by a factor of 8 and 30 for the O(+) and H(+) ions, respectively. The energy of these ions is mostly within 1–100 keV for both species after interaction with the magnetopause, but a few percentages reach to 0.1–1 MeV. Our kinetic simulations show that a small fraction ([Formula: see text] 25%) of the corotating Jovian plasma reach the magnetopause, but among those >50% cross the high‐power density regions at the magnetopause and gain energy. Finally, we compare our simulation results with Galileo observations of Ganymede's magnetopause crossings (i.e., G8 and G28 flybys). There is an excellent agreement between our simulations and observations, particularly our simulations fully capture the size and structure of the magnetosphere. |
format | Online Article Text |
id | pubmed-9286830 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-92868302022-07-19 Ion Dynamics at the Magnetopause of Ganymede Fatemi, S. Poppe, A. R. Vorburger, A. Lindkvist, J. Hamrin, M. J Geophys Res Space Phys Research Article We study the dynamics of the thermal O(+) and H(+) ions at Ganymede's magnetopause when Ganymede is inside and outside of the Jovian plasma sheet using a three‐dimensional hybrid model of plasma (kinetic ions, fluid electrons). We present the global structure of the electric fields and power density (E ⋅ J) in the magnetosphere of Ganymede and show that the power density at the magnetopause is mainly positive and on average is +0.95 and +0.75 nW/m(3) when Ganymede is inside and outside the Jovian plasma sheet, respectively, but locally it reaches over +20 nW/m(3). Our kinetic simulations show that ion velocity distributions at the vicinity of the upstream magnetopause of Ganymede are highly non‐Maxwellian. We investigate the energization of the ions interacting with the magnetopause and find that the energy of those particles on average increases by a factor of 8 and 30 for the O(+) and H(+) ions, respectively. The energy of these ions is mostly within 1–100 keV for both species after interaction with the magnetopause, but a few percentages reach to 0.1–1 MeV. Our kinetic simulations show that a small fraction ([Formula: see text] 25%) of the corotating Jovian plasma reach the magnetopause, but among those >50% cross the high‐power density regions at the magnetopause and gain energy. Finally, we compare our simulation results with Galileo observations of Ganymede's magnetopause crossings (i.e., G8 and G28 flybys). There is an excellent agreement between our simulations and observations, particularly our simulations fully capture the size and structure of the magnetosphere. John Wiley and Sons Inc. 2022-01-18 2022-01 /pmc/articles/PMC9286830/ /pubmed/35865030 http://dx.doi.org/10.1029/2021JA029863 Text en © 2022 The Authors. https://creativecommons.org/licenses/by-nc/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by-nc/4.0/ (https://creativecommons.org/licenses/by-nc/4.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited and is not used for commercial purposes. |
spellingShingle | Research Article Fatemi, S. Poppe, A. R. Vorburger, A. Lindkvist, J. Hamrin, M. Ion Dynamics at the Magnetopause of Ganymede |
title | Ion Dynamics at the Magnetopause of Ganymede |
title_full | Ion Dynamics at the Magnetopause of Ganymede |
title_fullStr | Ion Dynamics at the Magnetopause of Ganymede |
title_full_unstemmed | Ion Dynamics at the Magnetopause of Ganymede |
title_short | Ion Dynamics at the Magnetopause of Ganymede |
title_sort | ion dynamics at the magnetopause of ganymede |
topic | Research Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9286830/ https://www.ncbi.nlm.nih.gov/pubmed/35865030 http://dx.doi.org/10.1029/2021JA029863 |
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