Io’s SO2 and NaCl Wind Fields from ALMA

Alexander E. Thelen, Katherine de Kleer, Martin A. Cordiner, Imke de Pater, Arielle Moullet and Statia Luszcz-Cook
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Abstract

We present spatially resolved measurements of SO2 and NaCl winds on Io at several unique points in its orbit: before and after eclipse and at maximum eastern and western elongation. The derived wind fields represent a unique case of meteorology in a rarified, volcanic atmosphere. Through the use of Doppler shift measurements in emission spectra obtained with the Atacama Large Millimeter/submillimeter Array between ~346 and 430 GHz (~0.70–0.87 mm), line-of-sight winds up to ~−100 m s−1 in the approaching direction and >250 m s−1 in the receding direction were derived for SO2 at altitudes of ~10–50 km, while NaCl winds consistently reached ~∣150–200∣ m s−1 in localized regions up to ~30 km above the surface. The wind distributions measured at maximum east and west Jovian elongations and on the sub-Jovian hemisphere pre- and posteclipse were found to be significantly different and complex, corroborating the results of simulations that include surface temperature and frost distribution, volcanic activity, and interactions with the Jovian magnetosphere. Further, the wind speeds of SO2 and NaCl are often inconsistent in direction and magnitude, indicating that the processes that drive the winds for the two molecular species are different and potentially uncoupled; while the SO2 wind field can be explained through a combination of sublimation-driven winds, plasma torus interactions, and plume activity, the NaCl winds appear to be primarily driven by the plasma torus.
从 ALMA 探测到的木卫二二氧化硫和氯化钠风场
我们展示了木卫一轨道上几个独特点的SO2和NaCl风的空间分辨率测量结果:日食前后和最大东伸长和最大西伸长。衍生的风场代表了稀薄的火山大气中气象学的一个独特案例。通过对阿塔卡马大型毫米/亚毫米阵列在~346 ~ 430 GHz (~0.70 ~ 0.87 mm)范围内获得的发射光谱进行多普勒频移测量,得出了在~10 ~ 50 km高度上,SO2接近方向的视距风速可达~−100 m s−1,后退方向的视距风速可达~ 250 m s−1,而在距离地面~30 km的局部区域,NaCl风速始终达到~∣150 ~ 200∣m s−1。在日蚀前后,在木星最大的东、西延伸处和次木星半球上测量到的风分布明显不同且复杂,证实了模拟结果,包括表面温度和霜冻分布、火山活动以及与木星磁层的相互作用。此外,SO2和NaCl的风速在方向和量级上往往不一致,这表明驱动这两种分子物种的风的过程是不同的,可能是不耦合的;SO2风场可以通过升华驱动风、等离子体环面相互作用和羽流活动的组合来解释,而NaCl风似乎主要是由等离子体环面驱动的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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