论文标题

arokoth的近表面温度模型

A Near Surface Temperature Model of Arrokoth

论文作者

Umurhan, O. M., Grundy, W. M., Bird, M. K., Beyer, R., Keane, J. T., Linscott, I. R., Birch, S., Bierson, C., Young, L. A., Stern, S. A., Lisse, C. M., Howett, C. J. A., Protopapa, S., Spencer, J. R., Binzel, R. P., Mckinnon, W. B., Lauer, T. R., Weaver, H. A., Olkin, C. B., Singer, K. N., Verbiscer, A. J., Parker, A. H.

论文摘要

基于最近发布的$ 10^5 $方面模型,开发了ARROKOTH的近表面热模型。该热溶液考虑了Arrokoth的表面重新放置回到自身。该解决方案方法利用了Arrokoth的周期性轨道特性,使用时间激素溶液方法进行热响应,该方法涉及热方程的傅立叶变换溶液,这是其他人最近使用的方法。我们将显示详细的热解决方案,假设Arrokoth的近地面材料的热惯性$ {\ cal i} = $ 2.5 w/m $^{ - 2} $ k $^{ - 1} $ s $ s $^{1/2} $。我们预测,在New Horizo​​ns与Arrokoth的相遇时,其相遇的半球表面温度为$ \ sim $ 57-59 K,其赤道区域为30-40 K,其冬季半球为11-13 K。 ARROKOTH的轨道平均温度约为其极性区域的30-35 K,近距离赤道区域接近40 K。从周围表面的热辐射量不到总能量预算的5%,而在一个轨道上通过热传导将Arrokoth内部挖出的总能量约为总能量预算的0.5%。作为这种热建模的广义应用以及其他KBO起源考虑因素,我们赞成这样的解释:New Horizo​​ns的Rex仪器的$ 29 \ pm 5 $ k亮度温度测量与Arrokoth的近表面材料是由近距离的MM大小的Tholin涂层的1.1的tholin coperation coperations i clocoth的表面材料一致。 w/m $^{ - 2} $ k $^{ - 1} $ s $^{1/2} $ $ <{\ cal i} <$ 10-20 w/m $^{ - 2} $ k $^{ - 1} $ s $ s $ s $ s $^{1/2} $,以及由X-Band emissivity n.9 and and and and and and and and and and 1.9和1.9。

A near surface thermal model for Arrokoth is developed based on the recently released $10^5$ facet model of the body. This thermal solution takes into account Arrokoth's surface re-radiation back onto itself. The solution method exploits Arrokoth's periodic orbital character to develop a thermal response using a time-asymptotic solution method, which involves a Fourier transform solution of the heat equation, an approach recently used by others. We display detailed thermal solutions assuming that Arrokoth's near surface material's thermal inertia ${\cal I} = $ 2.5 W/m$^{-2}$K$^{-1}$s$^{1/2}$. We predict that at New Horizons' encounter with Arrokoth its encounter hemisphere surface temperatures were $\sim$ 57-59 K in its polar regions, 30-40 K on its equatorial zones, and 11-13 K for its winter hemisphere. Arrokoth's orbitally averaged temperatures are around 30-35 K in its polar regions, and closer to 40 K near its equatorial zones. Thermal reradiation from the surrounding surface amounts to less than 5\% of the total energy budget, while the total energy ensconced into and exhumed out Arrokoth's interior via thermal conduction over one orbit is about 0.5\% of the total energy budget. As a generalized application of this thermal modeling together with other KBO origins considerations, we favor the interpretation that New Horizons' REX instrument's $29 \pm 5$K brightness temperature measurement is consistent with Arrokoth's near surface material's being made of sub-to-few mm sized tholin-coated amorphous \water ice grains with 1 W/m$^{-2}$K$^{-1}$s$^{1/2}$ $< {\cal I} < $10-20 W/m$^{-2}$K$^{-1}$s$^{1/2}$, and which are characterized by an X-band emissivity in the range 0.9 and 1.

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