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首页> 外文期刊>Icarus: International Journal of Solar System Studies >An analysis of Pluto occultation light curves using an atmospheric radiative-conductive model
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An analysis of Pluto occultation light curves using an atmospheric radiative-conductive model

机译:利用大气辐射传导模型分析冥王星掩星光曲线

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We use a radiative-conductive model to least-squares fit Pluto stellar occultation light curve data. This model predicts atmospheric temperature based on surface temperature, surface pressure, surface radius, and CH4 and CO mixing ratios, from which model light curves are to be calculated. The model improves upon previous techniques for deriving Pluto's atmospheric thermal structure from stellar occultation light curves by calculating temperature (as a function of height) caused by heating and cooling by species in Pluto's atmosphere, instead of a general assumption that temperature follows a power law with height or some other idealized function. We are able to fit for model surface radius, surface pressure, and CH4 mixing ratio with one of the 2006 datasets and for surface pressure and CH4 mixing ratio for other datasets from the years 1988, 2002, 2006, and 2008. It was not possible to fit for CO mixing ratio and surface temperature because the light curves are not sensitive to these parameters. We determine that the model surface radius, under the assumption of a stratosphere only (i.e. no troposphere) model in radiative-conductive balance, is 1180-10+20km. The CH4 mixing ratio results are more scattered with time and are in the range of 1.8-9.4×10-3. The surface pressure results show an increasing trend from 1988 to 2002, although it is not as dramatic as the factor of 2 from previous studies.
机译:我们使用辐射传导模型对Pluto恒星掩星光曲线数据进行最小二乘拟合。该模型根据表面温度,表面压力,表面半径以及CH4和CO的混合比预测大气温度,并据此计算模型光曲线。该模型对以前的技术进行了改进,该技术通过计算由冥王星大气中的物质加热和冷却引起的温度(作为高度的函数)从恒星掩星光曲线得出冥王星大气热结构的方法,而不是一般假定温度遵循幂定律高度或其他理想功能。我们能够用2006年的一个数据集拟合模型的表面半径,表面压力和CH4混合比,并拟合1988、2002、2006和2008年其他数据集的表面压力和CH4混合比。这是不可能的因为光曲线对这些参数不敏感,因此适合CO混合比和表面温度。我们确定仅在辐射传导平衡的平流层(即无对流层)模型的假设下,模型表面半径为1180-10 + 20km。 CH4混合比结果随时间散布更多,范围为1.8-9.4×10-3。从1988年到2002年,表面压力结果显示出增加的趋势,尽管它没有以前研究的2倍那么显着。

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