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首页> 外文期刊>The Astrophysical journal >PLUTO’s ATMOSPHERE FROM STELLAR OCCULTATIONS IN 2012 AND 2013*
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PLUTO’s ATMOSPHERE FROM STELLAR OCCULTATIONS IN 2012 AND 2013*

机译:PLUTO在2012年和2013年的星空活动中的氛围*

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We analyze two multi-chord stellar occultations by Pluto that were observed on 2012 July 18th and 2013 May 4th, and respectively monitored from five and six sites. They provide a total of fifteen light curves, 12 of which were used for a simultaneous fit that uses a unique temperature profile, assuming a clear (no haze) and pure N2 atmosphere, but allowing for a possible pressure variation between the two dates. We find a solution that satisfactorily fits (i.e., within the noise level) all of the 12 light curves, providing atmospheric constraints between ~1190 km (pressure ~11 μbar) and ~1450 km (pressure ~0.1 μbar) from Pluto's center. Our main results are: (1) the best-fitting temperature profile shows a stratosphere with a strong positive gradient between 1190 km (at 36 K, 11 μbar) and r = 1215 km (6.0 μbar), where a temperature maximum of 110 K is reached; above it is a mesosphere with a negative thermal gradient of ?0.2 K km?1 up to ~1390 km (0.25 μbar), where the mesosphere connects itself to a more isothermal upper branch around 81 K; (2) the pressure shows a small (6%) but significant increase (6σ level) between the two dates; (3) without a troposphere, Pluto's radius is found to be 5 km. Allowing for a troposphere, RP is constrained to lie between 1168 and 1195 km; and (4) the currently measured CO abundance is too small to explain the mesospheric negative thermal gradient. Cooling by HCN is possible, but only if this species is largely saturated. Alternative explanations like zonal winds or vertical compositional variations of the atmosphere are unable to explain the observed mesospheric negative thermal gradient.
机译:我们分析了冥王星在2012年7月18日和2013年5月4日观测到的两个多弦恒星掩星,分别从五个和六个站点进行了监测。它们提供了总共15条光曲线,其中12条用于同时拟合,使用了独特的温度曲线,并假设有清晰(无雾)和纯净的N2气氛,但允许两个日期之间可能存在压力变化。我们找到了一种可以令人满意地拟合(即在噪声水平之内)所有12条光曲线的解决方案,在距冥王星中心约1190 km(压力〜11μbar)和〜1450 km(压力〜0.1μbar)之间提供了大气限制。我们的主要结果是:(1)最合适的温度曲线显示平流层在1190 km(在36 K,11μbar)和r = 1215 km(6.0μbar)之间具有强正梯度,其中最高温度为110 K到达了;在它上面是一个中球层,负温度梯度为?0.2 K km?1,最高可达〜1390 km(0.25μbar),其中中球层将自身连接到一个约81 K的等温上部分支。 (2)两个日期之间的压力显示很小(6%)但显着增加(6σ水平); (3)在没有对流层的情况下,冥王星的半径为5 km。考虑到对流层,RP被限制在1168至1195 km之间。 (4)目前测得的CO丰度太小,无法解释中层负热梯度。可以通过HCN进行冷却,但前提是该物种已大大饱和。纬向风或大气的垂直成分变化等其他解释也无法解释观测到的中层负热梯度。
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