利用奥丁太空望远镜监测18年来木星平流层中水汽的演变

B. Benmahi, T. Cavali'e, M. Dobrijevic, N. Biver, K. Bermudez-Diaz, A. Sandqvist, E. Lellouch, R. Moreno, T. Fouchet, V. Hue, P. Hartogh, F. Billebaud, A. Lecacheux, A. Hjalmarson, U. Frisk, M. Olberg
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引用次数: 5

摘要

舒梅克-列维9号彗星于1994年7月撞击木星,在平流层留下了几种新的物质,其中包括水蒸气(H2O)。在光化学模型的帮助下,水可以作为木星平流层的动态示踪剂。在本文中,我们的目标是在H2O所在的水平上限制垂直涡流扩散(Kzz)。2002年至2019年,我们用奥丁太空望远镜监测了556.936 GHz的水盘平均辐射,覆盖了近20年。我们结合一维光化学和辐射传输模型对数据进行分析,以约束木星平流层中的垂直涡旋扩散。奥丁观测显示,2002年至2019年间,水的排放量几乎呈线性下降,约为40%。如果我们在2002年至2019年H2O向下扩散的压力范围内增加Kzz的大小,即从~0.2 mbar到~5 mbar,我们只能重现我们的时间序列。然而,这种改进的Kzz与碳氢化合物的观测结果不相容。我们发现,即使考虑到撞击纬度上最初大量的H2O和CO, H2O到CO2的光化学转化也不足以解释H2O线发射的逐渐下降,这表明存在额外的损失机制。我们从H2O的Odin观测得到的Kzz只能被看作是~0.2 mbar到~5 mbar压力范围内的上限。由水和碳氢化合物观测所得的解释之间的不相容可能是由于一维建模的限制。水的经向变化,最有可能是在极光纬度,需要评估并与碳氢化合物的经向变化进行比较,以量化自SL9撞击以来极光化学在水丰度的时间演变中的作用。用二维模型来模拟SL9物种的时间进化将是下一步。
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Monitoring of the evolution of H2O vapor in the stratosphere of Jupiter over an 18-yr period with the Odin space telescope
Comet Shoemaker-Levy 9 impacted Jupiter in July 1994, leaving its stratosphere with several new species, among them water vapor (H2O). With the aid of a photochemical model H2O can be used as a dynamical tracer in the jovian stratosphere. In this paper, we aim at constraining vertical eddy diffusion (Kzz) at the levels where H2O resides. We monitored the H2O disk-averaged emission at 556.936 GHz with the Odin space telescope between 2002 and 2019, covering nearly two decades. We analyzed the data with a combination of 1D photochemical and radiative transfer models to constrain vertical eddy diffusion in the stratosphere of Jupiter. The Odin observations show us that the emission of H2O has an almost linear decrease of about 40% between 2002 and 2019.We can only reproduce our time series if we increase the magnitude of Kzz in the pressure range where H2O diffuses downward from 2002 to 2019, i.e. from ~0.2 mbar to ~5 mbar. However, this modified Kzz is incompatible with hydrocarbon observations. We find that, even if allowance is made for the initially large abundances of H2O and CO at the impact latitudes, the photochemical conversion of H2O to CO2 is not sufficient to explain the progressive decline of the H2O line emission, suggestive of additional loss mechanisms. The Kzz we derived from the Odin observations of H2O can only be viewed as an upper limit in the ~0.2 mbar to ~5 mbar pressure range. The incompatibility between the interpretations made from H2O and hydrocarbon observations probably results from 1D modeling limitations. Meridional variability of H2O, most probably at auroral latitudes, would need to be assessed and compared with that of hydrocarbons to quantify the role of auroral chemistry in the temporal evolution of the H2O abundance since the SL9 impacts. Modeling the temporal evolution of SL9 species with a 2D model would be the next natural step.
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