A stability limit for the atmospheres of giant extrasolar planets

Close companions The extrasolar 'hot Jupiter' HD209458b is orbiting close to a solar-type star and is subject to intense heating as a result. It is surrounded by an expanded atmosphere of atomic hydrogen that is escaping from the planet. Such escape is theoretically possible at least insid...

Full description

Saved in:
Bibliographic Details
Published inNature Vol. 450; no. 7171; pp. 845 - 848
Main Authors Koskinen, Tommi T., Aylward, Alan D., Miller, Steve
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 06.12.2007
Nature Publishing
Nature Publishing Group
Subjects
Online AccessGet full text
ISSN0028-0836
1476-4687
1476-4687
1476-4679
DOI10.1038/nature06378

Cover

Loading…
More Information
Summary:Close companions The extrasolar 'hot Jupiter' HD209458b is orbiting close to a solar-type star and is subject to intense heating as a result. It is surrounded by an expanded atmosphere of atomic hydrogen that is escaping from the planet. Such escape is theoretically possible at least inside an orbit of 0.1 AU (one AU is the distance between Earth and the Sun). But at 5 AU from the Sun, Jupiter has a stable atmosphere. So somewhere between those extremes there must be a crossover between stability and instability. Numerical modelling now suggests that crossover occurs between 0.14 and 0.16 AU for a Jupiter-like planet. Recent observations of the planet HD209458b indicate that it is surrounded by an expanded atmosphere of atomic hydrogen that is escaping hydrodynamically 1 , 2 , 3 . Theoretically, it has been shown that such escape is possible at least inside an orbit of 0.1  au (refs 4 and 5 ), and also that H 3 + ions play a crucial role in cooling the upper atmosphere 5 , 6 . Jupiter’s atmosphere is stable 7 , so somewhere between 5 and 0.1  au there must be a crossover between stability and instability. Here we show that there is a sharp breakdown in atmospheric stability between 0.14 and 0.16  au for a Jupiter-like planet orbiting a solar-type star. These results are in contrast to earlier modelling 4 , 8 that implied much higher thermospheric temperatures and more significant evaporation farther from the star. (We use a three-dimensional, time-dependent coupled thermosphere–ionosphere model 6 and properly include cooling by H 3 + ions, allowing us to model globally the redistribution of heat and changes in molecular composition.) Between 0.2 and 0.16  au cooling by H 3 + ions balances heating by the star, but inside 0.16  au molecular hydrogen dissociates thermally, suppressing the formation of H 3 + and effectively shutting down that mode of cooling.
Bibliography:ObjectType-Article-1
SourceType-Scholarly Journals-1
ObjectType-Feature-2
content type line 14
content type line 23
ObjectType-Article-2
ObjectType-Feature-1
ISSN:0028-0836
1476-4687
1476-4687
1476-4679
DOI:10.1038/nature06378