H
O and CO
in the Upper Atmospheres of the Giant Planets
E. Lellouch (Obs. Meudon), H. Feuchtgruber (MPI Garching), Th. de Graauw (SRON Groningen), B. Bézard, Th. Encrenaz (Obs. Meudon), M. Griffin (QMWC London)
Observations with the Short Wavelength Spectrometer (SWS) of the Infrared
Space Observatory (ISO) have allowed the detection of a series of
emissions due to the rotational lines of water vapor between
28 and 45
m in the spectrum of Saturn, Uranus and Neptune. These
emissions originate
from the sub-millibar region and the implied H
O column densities
are about 1.5
10
, 9
10
and 3
10
molec. cm
, respectively. The CO
band at 14.98
m was
also detected in emission on Saturn and Neptune but not on Uranus.
The CO
column density is about 8
10
molec. cm
for both
planets (assuming uniform mixing at p
10 mbar in Saturn's case).
Because of the tropopause cold trap, the detection of H
O at stratospheric
levels implies an external origin. Similarly, CO
must be deposited
or formed locally in Neptune's stratosphere. On Saturn, another
possibility if updraft of CO
from the deep interior. Sources of
water include interplanetary dust, infall of asteroidal/cometary objects
and material sputtered from rings and satellites. Using a simple model,
in which water is deposited in the 0.1-3
bar range by meteoritic ablation
and the main loss is assumed to be vertical transport, external fluxes
in the range 10
to 10
H
O molec. cm
s
are required
to explain the observed H
O amounts.
The presence of CO
in Saturn and Neptune may result from similar ablation
of CO
ice contained in infalling meteorites, or, perhaps more likely
given its non-detection at Uranus, secondary production from CO + OH.
Preliminary calculations suggest that this mechanism is quantitatively
viable at least for Neptune.
The existence of external sources of water in Giant Planets has also implications for the energy budget, photochemistry and ionospheric properties of these atmospheres. Elucidating the interplanetary vs. ring/satellite origin of water may also provide constraints on cometary activity at large heliocentric distances.