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Cassini Ion and Neutral Mass Spectrometer data in Titan's upper atmosphere and exosphere: Observation of a suprathermal corona

机译:泰坦高层大气和大气层中的卡西尼离子和中性质谱仪数据:超热电晕的观测

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摘要

The neutral nitrogen and methane measurements made by Ion and Neutral Mass Spectrometer during Cassini flybys T A , T B , and T 5 in Titan's upper atmosphere and exosphere are presented. Large horizontal variations are observed in the total density, recorded to be twice as large during T A as during T 5. Comparison between the atmospheric and exospheric data show evidence for the presence of a significant population of suprathermal molecules. Using a diffusion model to simultaneously fit the N2 and CH4 density profiles below 1500 km, the atmospheric structure parameters are determined, taking into account recent changes in the calibration parameters. The best fits are obtained for isothermal profiles with values 152.8 ± 4.6 K for T A , 149.0 ± 9.2 K for T B , and 157.4 ± 4.9 K for T 5, suggesting a temperature ≃5 K warmer at night than at dusk, a trend opposite to that determined by solar-driven models. Using standard exospheric theory and a Maxwellian exobase distribution, a temperature of 20 to 70 K higher would be necessary to fit the T A , T B , and egress-T 5 data above 1500 km. The suprathermal component of the corona was fit with various exobase energy distributions, using a method based on the Liouville theorem. This gave a density of suprathermals at the exobase of 4.4 ± 5.1 × 105 cm−3 and 1.1 ± 0.9 × 105 cm−3, and an energy deposition rate at the exobase of 1.1 ± 0.9 × 102 eV cm−3 s−1 and 3.9 ± 3.5 × 101 eV cm−3 s−1 for the hot N2 and CH4 populations, respectively. The energy deposition rate allowed us to roughly estimate escape rates for nitrogen of ≃7.7 ± 7.1 × 107 N cm−2 s−1 and for methane of ≃2.8 ± 2.1 × 107 CH4 cm−2 s−1. Interestingly, no suprathermal component was observed in the ingress-T 5 data.
机译:给出了离子和中性质谱仪在卡西尼号飞越塔A,T B和T 5在泰坦的高层大气和大气层中进行的中性氮和甲烷测量。在总密度中观察到较大的水平变化,记录的变化是在T A期间是T 5期间的两倍。大气和大气外数据的比较表明存在大量的超热分子。使用扩散模型同时拟合1500 km以下的N2和CH4密度曲线,并考虑到校准参数的最新变化来确定大气结构参数。等温曲线的最佳拟合是TA的值为152.8±4.6 K,TB的值为149.0±9.2 K,T 5的值为157.4±4.9 K,表明夜间的温度比黄昏的温度高≃5K,这一趋势与之相反由太阳能驱动的模型确定。使用标准的大气外层理论和Maxwellian大气外层分布,需要高出20至70 K的温度才能拟合1500 km以上的T A,T B和egress-T 5数据。使用基于Liouville定理的方法,将电晕的超热成分与各种exobase能量分布拟合。这样在外底的超热密度为4.4±5.1×105 cm-3和1.1±0.9×105 cm-3,在外底的能量沉积速率为1.1±0.9×102 eV cm-3 s-1和对于热的N2和CH4族群,分别为3.9±3.5×101 eV cm-3 s-1。能量沉积速率使我们能够粗略估计for7.7±7.1×107 N cm−2 s-1的氮气和≃2.8±2.1×107 CH4 cm−2 s-1的甲烷的逸出速率。有趣的是,在入口T 5数据中未观察到超热成分。

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