Johnson Robert E
University of Virginia, Charlottesville, VA 22904, USA Department of Physics, New York University, New York, NY 10003, USA.
Philos Trans A Math Phys Eng Sci. 2009 Feb 28;367(1889):753-71. doi: 10.1098/rsta.2008.0244.
Titan is an important endpoint for understanding atmospheric evolution. Prior to Cassini's arrival at Saturn, modelling based on Voyager data indicated that the hydrogen escape rate was large (1-3x1028amus-1), but the escape rates for carbon and nitrogen species were relatively small (5x1026amus-1) and dominated by atmospheric sputtering. Recent analysis of the structure of Titan's thermosphere and corona attained from the Ion and Neutral Mass Spectrometer and the Huygens Atmospheric Structure Instrument on Cassini have led to substantially larger estimates of the loss rate for heavy species (0.3-5x1028amus-1). At the largest rate suggested, a mass that is a significant fraction of the present atmosphere would have been lost to space in 4Gyr; hence, understanding the nature of the processes driving escape is critical. The recent estimates of neutral escape are reviewed here, with particular emphasis on plasma-induced sputtering and heating. Whereas the loss of hydrogen is clearly indicated by the altitude dependence of the H2 density, three different one-dimensional models were used to estimate the heavy-molecule loss rate using the Cassini data for atmospheric density versus altitude. The solar heating rate and the nitrogen density profile versus altitude were used in a fluid dynamic model to extract an average net upward flux below the exobase; the diffusion of methane through nitrogen was described below the exobase using a model that allowed for outward flow; and the coronal structure above the exobase was simulated by presuming that the observed atmospheric structure was due to solar- and plasma-induced hot particle production. In the latter, it was hypothesized that hot recoils from photochemistry or plasma-ion-induced heating were required. In the other two models, the upward flow extracted is driven by heat conduction from below, which is assumed to continue to act above the nominal exobase, producing a process referred to as 'slow hydrodynamic' escape. These models and the resulting loss rates are reviewed and compared. It is pointed out that preliminary estimates of the composition of the magnetospheric plasma at Titan's orbit appear to be inconsistent with the largest loss rates suggested for the heavy species, and the mean upward flow extracted in the one-dimensional models could be consistent with atmospheric loss by other mechanisms or with transport to other regions of Titan's atmosphere.
土卫六是理解大气演化的一个重要观测对象。在卡西尼号抵达土星之前,基于旅行者号数据的模型表明氢逃逸率很高(1 - 3×10²⁸ 原子/秒),但碳和氮物种的逃逸率相对较低(5×10²⁶ 原子/秒),且主要由大气溅射主导。最近对卡西尼号上的离子和中性质量谱仪以及惠更斯大气结构仪器所获得的土卫六热层和日冕结构的分析,使得对重元素损失率的估计大幅提高(0.3 - 5×10²⁸ 原子/秒)。按照所提出的最大速率计算,在40亿年的时间里,当前大气中相当一部分质量会散失到太空中;因此,了解驱动逃逸过程的本质至关重要。本文回顾了近期对中性逃逸的估计,特别强调了等离子体诱导的溅射和加热。虽然氢的损失通过H₂密度随高度的变化清晰显示,但使用卡西尼号获取的大气密度与高度的数据,运用三种不同的一维模型来估计重分子的损失率。在流体动力学模型中,利用太阳加热率和氮密度随高度的分布来提取外逸层底部以下的平均净向上通量;在外逸层底部以下,使用一个考虑向外流动的模型来描述甲烷在氮中的扩散;通过假定观测到的大气结构是由太阳和等离子体诱导的热粒子产生的,来模拟外逸层上方的日冕结构。在后者中,假设需要光化学或等离子体离子诱导加热产生的热反冲。在另外两个模型中,提取的向上流动是由下方的热传导驱动的,假定这种热传导在名义外逸层上方继续起作用,产生一种被称为“缓慢流体动力学”逃逸的过程。对这些模型及其得出的损失率进行了回顾和比较。指出在土卫六轨道处磁层等离子体成分的初步估计似乎与为重元素所提出的最大损失率不一致,并且在一维模型中提取的平均向上流动可能与通过其他机制造成的大气损失一致,或者与向土卫六大气其他区域的传输一致。