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...
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Published in | Nature Vol. 450; no. 7171; pp. 845 - 848 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
London
Nature Publishing Group UK
06.12.2007
Nature Publishing Nature Publishing Group |
Subjects | |
Online Access | Get full text |
ISSN | 0028-0836 1476-4687 1476-4687 1476-4679 |
DOI | 10.1038/nature06378 |
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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. |
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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 |