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Saturn's magnetosphere interaction with Titan for T9 encounter:3D hybrid modeling and comparison with CAPS observations

机译:土星与泰坦在T9上的磁层相互作用:3D混合建模和CAPS观测结果的比较

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摘要

Global dynamics of ionized and neutral gases in the environment of Titan plays an important role in the interaction of Saturn's magnetosphere with Titan. Several hybrid simulations of this problem have already been done (Brecht et al., 2000; Kallio et al., 2004; Modolo et al., 2007a; Simon et al., 2007a, 2007b; Modolo and Chanteur, 2008). Observational data from CAPS for the T9 encounter (Sittler et al., 2009) indicates an absence of O~+ heavy ions in the upstream that change the models of interaction which were discussed in current publications (Kallio et al., 2004; Modolo et al., 2007a; Simon et al., 2007a, 2007b; Ma et al., 2007; Szego et al., 2007). Further analysis of the CAPS data shows very low density or even an absence of H~+ ions in upstream. In this paper we discuss two models of the interaction of Saturn's magnetosphere with Titan: (A) high density of H~+ ions in the upstream flow (0.1 cm~(-3)), and (B) low density of H~+ ions in the upstream flow (0.02 cm~(-3)). The hybrid model employs a fluid description for electrons and neutrals, whereas a particle approach is used for ions. We also take into account charge-exchange and photoionization processes and solve self-consistently for electric and magnetic fields. The model atmosphere includes exospheric H~+, H_2~+, N_2~+ and CH_4~+ pickup ion production as well as an immobile background ionosphere and a shell distribution for active ionospheric ions (M_i = 28 amu). The hybrid model allows us to account for the realistic anisotropic ion velocity distribution that cannot be done in fluid simulations with isotropic temperatures. Our simulation shows an asymmetry of the ion density distribution and the magnetic field, including the formation of Alfven wing-like structures. The results of the ion dynamics in Titan's environment are compared with Cassini T9 encounter data (CAPS).
机译:土卫六环境中的电离和中性气体的整体动力学在土星磁层与土卫六的相互作用中起着重要作用。已经对该问题进行了几种混合模拟(Brecht等,2000; Kallio等,2004; Modolo等,2007a; Simon等,2007a,2007b; Modolo和Chanteur,2008)。来自CAPS的T9遭遇的观测数据(Sittler等,2009)表明,上游缺乏O〜+重离子,改变了相互作用模型,目前的出版物对此进行了讨论(Kallio等,2004; Modolo等)。等人,2007a; Simon等人,2007a,2007b; Ma等人,2007; Szego等人,2007)。对CAPS数据的进一步分析表明,上游的密度非常低,甚至没有H〜+离子。在本文中,我们讨论了土星磁层与泰坦相互作用的两种模型:(A)上游流中H〜+离子的高密度(0.1 cm〜(-3)),以及(B)H〜+低密度的离子在上游流动(0.02 cm〜(-3))。混合模型对电子和中性粒子采用流体描述,而对离子采用粒子方法。我们还考虑了电荷交换和光电离过程,并针对电场和磁场自洽地求解。模型大气包括大气层H〜+,H_2〜+,N_2〜+和CH_4〜+产生的离子,以及固定的背景电离层和活性电离层离子的壳层分布(M_i = 28 amu)。混合模型使我们能够说明在各向同性温度的流体模拟中无法实现的逼真的各向异性离子速度分布。我们的模拟显示了离子密度分布和磁场的不对称性,其中包括Alfven翼状结构的形成。将泰坦环境中离子动力学的结果与卡西尼T9遭遇数据(CAPS)进行了比较。

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  • 来源
    《Planetary and space science》 |2012年第1期|p.66-78|共13页
  • 作者单位

    The Goddard Planetary and Heliophysics Institute, University of Maryland, Baltimore County, USA,NASA Coddard Space Flight Center, Greenbelt, MD 20771, USA,Dialogue-Science, A.A. Dorodnitsyn Computing Center Russian Academy of Science, Vavilov Street 40, 119991 Moscow, Russia,Faculty of Problems of Physics and Power Engineering Moscow Institute of Physics and Technology, Russia,NASA GSFC, Code 673, Building 21, Room 247, 8800 Greenbelt Road, Greenbelt, MD 20771, USA;

    NASA Coddard Space Flight Center, Greenbelt, MD 20771, USA;

    NASA Coddard Space Flight Center, Greenbelt, MD 20771, USA;

    NASA Coddard Space Flight Center, Greenbelt, MD 20771, USA;

    NASA Coddard Space Flight Center, Greenbelt, MD 20771, USA;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    ionospheres; atmospheres; induced magnetospheres; magnetic barrier; alfven wing; plasma modeling;

    机译:电离层;气氛;感应磁层;磁障阿尔文翼等离子建模;

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