Suppr超能文献

木卫三磁层顶的离子动力学

Ion Dynamics at the Magnetopause of Ganymede.

作者信息

Fatemi S, Poppe A R, Vorburger A, Lindkvist J, Hamrin M

机构信息

Department of Physics Umeå University Umeå Sweden.

Space Sciences Laboratory University of California at Berkeley Berkeley CA USA.

出版信息

J Geophys Res Space Phys. 2022 Jan;127(1):e2021JA029863. doi: 10.1029/2021JA029863. Epub 2022 Jan 18.

Abstract

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 ( ⋅ ) 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 when Ganymede is inside and outside the Jovian plasma sheet, respectively, but locally it reaches over +20 nW/m. 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 ( 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.

摘要

我们使用等离子体三维混合模型(动力学离子、流体电子)研究了木卫三位于木星等离子体片内外时,木卫三磁层顶处热氧离子和氢离子的动力学。我们展示了木卫三磁层中电场和功率密度( ⋅ )的整体结构,并表明当木卫三位于木星等离子体片内和外时,磁层顶处的功率密度主要为正,平均分别为 +0.95 和 +0.75 nW/m,但局部可超过 +20 nW/m。我们的动力学模拟表明,木卫三上游磁层顶附近的离子速度分布高度非麦克斯韦分布。我们研究了与磁层顶相互作用的离子的能量增加情况,发现这些粒子的能量对于氧离子和氢离子平均分别增加了 8 倍和 30 倍。与磁层顶相互作用后,这两种离子的能量大多在 1 - 100 keV 范围内,但有少数百分比达到 0.1 - 1 MeV。我们的动力学模拟表明,一小部分( 25%)共转的木星等离子体到达磁层顶,但其中超过 >50%穿过磁层顶的高功率密度区域并获得能量。最后,我们将模拟结果与伽利略号对木卫三磁层顶穿越(即 G8 和 G28 飞越)的观测进行了比较。我们的模拟与观测结果非常吻合,特别是我们的模拟完全捕捉到了磁层的大小和结构。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a559/9286830/74b9f411d751/JGRA-127-0-g011.jpg

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验