New constraints on pluto's sputnik planitia ice sheet from a coupled reorientation-climate model
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Johnson_2021_Planet._Sci._J._2 ...
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Lunar and Planetary Laboratory, University of ArizonaIssue Date
2021
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Johnson, P. E., Keane, J. T., Young, L. A., & Matsuyama, I. (2021). New constraints on pluto’s sputnik planitia ice sheet from a coupled reorientation-climate model. Planetary Science Journal, 2(5).Journal
Planetary Science JournalRights
Copyright © 2021. The Author(s). Published by the American Astronomical Society. Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
We present a coupled reorientation and climate model, to understand how true polar wander (TPW) and atmospheric condensation worked together to create the Sputnik Planitia (SP) ice sheet and reorient it to its presentday location on Pluto. SP is located at 18°N, 178°E, very close to the anti-Charon point, and it has been previously shown that this location can be explained by TPW reorientation of an impact basin as it fills with N2 ice. We readdress that hypothesis while including a more accurate treatment of Pluto's climate and orbital obliquity cycle. Our model again finds that TPW is a viable mechanism for the formation and present-day location of SP. We find that the initial impact basin could have been located north of the present-day location, at latitudes between 35°N and 50°N. The empty basin is constrained to be 2.5-3 km deep, with enough N2 available to form at most a 1-2 km thick ice sheet. Larger N2 inventories reorient too close to the anti-Charon point. After reaching the final location, the ice sheet undergoes short periods of sublimation and recondensation on the order of 10 m of ice, due to Pluto's variable obliquity cycle, which drives short periods of reorientation of a few kilometers. The obliquity cycle also has a role in the onset of infilling; some initial basin locations are only able to begin accumulating N2 ice at certain points during the obliquity cycle. We also explore the sensitivity of the coupled model to albedo, initial obliquity, and Pluto's orbit. © 2021. The Author(s).Note
Open access journalISSN
2632-3338Version
Final published versionae974a485f413a2113503eed53cd6c53
10.3847/PSJ/ac1d42
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Except where otherwise noted, this item's license is described as Copyright © 2021. The Author(s). Published by the American Astronomical Society. Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence.

