Modeling the Emission of Energetic Neutral Atoms in Titan's Dynamic Magnetospheric Environment

IF 2.6 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Journal of Geophysical Research: Space Physics Pub Date : 2024-11-19 DOI:10.1029/2024JA033103
Tyler Tippens, Sven Simon, Elias Roussos
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Abstract

To provide context for Cassini observations of energetic neutral atoms (ENAs) generated by charge exchange between Titan's atmosphere and energetic magnetospheric ions, we compute synthetic ENA images for a variety of uniform and draped electromagnetic field configurations, flyby scenarios, and viewing geometries. Starting with the idealized case of the magnetospheric field near Titan pointing southward, we calculate the observable ENA emission morphology for a large set of detector locations, each mimicking the properties of Cassini's Ion and Neutral Camera. Regardless of whether the electromagnetic fields near Titan are treated as uniform or draped, ENA production occurs within a thin shell of radial thickness 85 km, located directly above the moon's exobase. The observable ENA morphology is largely controlled by the angle between the detector's boresight vector and Saturn's magnetospheric field. Both the radius and the sense of energetic ion gyration carve distinct gaps in the ENA emission pattern. Field line draping around Titan leaves a discernible imprint in the ENA emissions only for a narrow range of viewing geometries. We also apply the model to study the ENA images taken during the T20 and T24 flybys. During both encounters, the ambient magnetospheric field displayed frequent transitions between Saturn's northern and southern magnetodisk lobes. We show that the notion of a steady-state interaction between Titan and an averaged magnetospheric background field is not suitable to explain the observed ENA morphology. Instead, ambient field variations measured more than 1 hr before ENA image acquisition still leave an imprint in the emission pattern.

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土卫六动态磁层环境中的高能中性原子发射建模
为了给卡西尼号对土卫六大气层和高能磁层离子之间电荷交换产生的高能中性原子(ENAs)的观测提供背景信息,我们计算了各种均匀和悬垂电磁场配置、飞越情景和观测几何的合成ENAs图像。从土卫六附近磁层场指向南方的理想化情况开始,我们计算了大量探测器位置的可观测ENA发射形态,每个位置都模拟了卡西尼离子和中性相机的特性。无论土卫六附近的电磁场是被视为均匀的还是悬垂的,ENA 的产生都发生在位于月球外基正上方的一个径向厚度为 85 千米的薄壳内。可观测到的ENA形态在很大程度上受探测器孔径矢量与土星磁层场之间角度的控制。高能离子回旋的半径和感觉都在ENA发射模式中留下了明显的间隙。土卫六周围的磁场线只在较窄的观测几何范围内才会在ENA辐射中留下明显的印记。我们还将该模型应用于研究 T20 和 T24 飞越期间拍摄的ENA 图像。在这两次相遇中,环境磁层场在土星的南北磁盘叶之间频繁转换。我们的研究表明,土卫六与平均磁层背景场之间的稳态相互作用概念并不适合解释观测到的ENA形态。相反,在获取ENA图像前1个多小时测量到的环境磁场变化仍然在发射模式中留下了印记。
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来源期刊
Journal of Geophysical Research: Space Physics
Journal of Geophysical Research: Space Physics Earth and Planetary Sciences-Geophysics
CiteScore
5.30
自引率
35.70%
发文量
570
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