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PROGRESS
Venus as a more Earth-like planet
Ha
˚
kan Svedhem
1
, Dmitry V. Titov
2,3
, Fredric W. Taylor
4
& Olivier Witasse
1
Venus is Earth’s near twin in mass and radius, and our nearest planetary neighbour, yet conditions there are very different in
many respects. Its atmosphere, mostly compos ed of carbon dioxide, has a surface temperature and pressure far higher than
those of Earth. Only traces of water are found, although it is likely that there was much more present in the past, possibly
forming Earth-like oceans. Here we discuss how the first year of observations by Venus Express brings into focus the
evolutionary paths by which the climates of two similar planets diverged from common beginnings to such extremes. These
include a CO
2
-driven greenhouse effect, erosion of the atmosphere by solar particles and radiation, surface
–
atmosphere
interactions, and atmospheric circulation regimes defined by differing planetary rotation rates.
V
enus, Earth and Mars—the three terrestrial planets with
atmospheres, grouped close together in the inner solar
system—have many features in common. Earth and
Venus, in particular, are nearly the same size and seem
to have been quite similar in the epoch when they formed and cooled,
probably with large inventories of CO
2
in Earth’s atmosphere and
liquid water oceans on the surfaces of Venus (and Mars). Today they
have very different conditions on their surface as a result of evolu-
tionary processes that we try to understand by measuring and
modelling the common processes, aided by data from space missions
designed to probe the planets and their environments. Earth and
Venus have roughly the same amount of CO
2
; on Earth it is bound
in carbonates in the crust, whereas on Venus it exists mostly as gas.
The extreme climate at the surface of Venus, driven by this excess of
CO
2
in the atmosphere, reminds us of pressing problems caused by
similar physics on Earth.
More than 30 spacecraft have made the trip to Venus since the
Americans sent Mariner 2 in 1962—the first successful man-made mis-
sion to another planet. The Soviet Venera and Vega and the American
Pioneer Venus missions in 1967–92 were particularly influential in
establishing a basic description of the physical and chemical conditions
prevailing in the atmosphere. They showed the venusian atmosphere to
be filled with corrosive gases and thick clouds, extraordinarily active,
with high winds and complex cloud formations sculpted by meteoro-
logical systems that seemed to defy categorization by terrestrial analogy,
and a vast double-eyed vortex over each pole. Now the European Space
Agency has sent its first mission to our nearest planetary neighbour, to
investigate how the global atmospheric circ ulation, the cloud chemis try,
surface–atmosphere physical and chemical interactions including vol-
canism, atmospheric escape processes and the global energy balance and
the ‘greenhouse’ effect at the surface all act together to produce a climate
apparently defiantly different from Earth’s
1
.
Venus Express
The Venus Express design is based on the successful Mars Express
spacecraft—a 600-kg, three-axis-stabilized platform with a body-
fixed communications antenna
2
. It was launched by the Russian
Soyuz-Fregat launcher from Baikonur, Kazakhstan, on 9 November
2005 and is the first mission dedicated to atmospheric and plasma
investigations of Venus since NASA launched its Pioneer Venus
orbiter and probes more than a quarter of a century ago. It arrived
at Venus on 11 April 2006 and became fully operational in June of
that year, deploying a new generation of instrumentation
2
and using
new modes of observation
3
. The core of the payload is composed of
optical instruments including spectrometers and spectro-imagers
(Fig. 1 and Table 1), which make the first systematic use of the
spectral windows between 1 and 3 mm for three-dimensional imaging
of the atmosphere all the way down to the surface
4
. Solar, stellar and
Earth radio occultation is used for vertical profiling of atmospheric
properties. The highly elliptical polar orbit combines global nadir
observations of extended duration of the southern hemisphere with
close-up snapshots of the equatorial and northern latitudes
3
.
Middle and lower atmosphere
These first observations covering a range of depths in Venus’s
atmosphere at high spatial resolution have revealed, in addition to
1
ESA/ESTEC, PB 299, 2200AG Noordwijk, The Netherlands.
2
Max Planck Institute for Solar System Research, Max-Planck-Strasse 2, 37191 Katlenburg-Lindau, Germany.
3
Space
Research Institute (IKI), Profsojuznaja ul. 84/32, 117997 Moscow, Russia.
4
Department of Atmospheric, Oceanic and Planetary Physics, University of Oxford, Oxford OX1 3PU, UK.
MAG
VMC
VeRa
ASPERA
VIRTIS
PFS
SPICAV/
SOIR
Figure 1
|
The Venus Express spacecraft. The inset shows the positions of the
seven scientific instruments in a semi-transparent view. The optical
instruments for remote sensing are mounted below the upper platform; all
apertures are aligned with the 1z axis (pointing towards the top of the image).
The magnetometer (MAG) on its 1-m-long boom can be seen on the upper
platform, while the two ASPERA sensors are mounted on the bottom platform
(only one can be seen in this view). PFS, Planetary Fourier Spectrometer;
VeRa, Venus Radio Science Experiment; VMC, Venus Monitoring Camera.
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localized ‘weather’ phenomena, the overall organization of the atmo-
spheric circulation. Three broad regimes are clearly present in the
middle and lower atmosphere, with convective and wave-dominated
meteorology in the lower latitudes and an abrupt transition to
smoother, banded flow at middle to high latitudes
5
. The latter ter-
minates at about 30u from the pole, where the cold polar collar dis-
covered by earlier missions lies. This encloses a vast vortex-type
structure several thousand kilometres across with a complex double
‘eye’ that rotates every 2.5–2.8 Earth days. Simultaneous observations
in the ultraviolet and thermal infrared spectral ranges show corre-
lated patterns, indicating that the contrasts at both wavelengths,
although representing different atmospheric levels, are driven by
the same circumpolar dynamical regime
5,6
. Spectroscopic observa-
tions indicate marked changes in the temperature and cloud struc-
ture in the vortex, with the cloud top in the polar collar located at an
altitude of 70–72 km, about 5 km or one scale height higher than in
the eye. Night-side observations in the transparent spectral windows
showed that the vortex structure and circulation exist at as least as
great a depth as the lower cloud deck at 50–55 km, although its
‘dipole’ appearance seems to be confined to the cloud-top region
6
.
The edge of the polar collar at 50–60u latitude apparently marks the
poleward limit of the Hadley circulation, the planet-wide overturn-
ing of the atmosphere in response to the concentration of solar heat-
ing in the equatorial zones (Fig. 2a). Indirect evidence of such
meridional circulation is provided by monitoring of the latitude
distribution of minor constituents, especially carbon monoxide, as
dynamical tracers in the lower atmosphere.
The mesopause on Venus at 100–120 km altitude marks another
transition between different global circulation regimes, this time in
the vertical. The predominance of zonal super-rotation in the lower
atmosphere below the mesopause is replaced by solar to antisolar
flow in the thermosphere above, as revealed by non-LTE (non-local
thermodynamic equilibrium) emission in the spectral band of O
2
at
1.27 mm that originates from the recombination of oxygen atoms in
descending flow on the night side (Fig. 2b). The observed emission
patterns are highly variable, with the maximum at about the anti-
solar point and the peak altitude at about the mesopause
7
. A meso-
spheric temperature maximum is observed on the night side
8
,
produced by adiabatic heating in the subsiding branch of the thermo-
spheric solar to anti-solar circulation.
Sequences of ultraviolet and infrared images have been used to
measure the wind speeds at different altitudes by tracking the
motions of contrast features in the clouds. Zonal winds at the cloud
tops (,70 km) derived from the ultraviolet imaging are in the range
100 6 10 m s
21
at latitudes below 50u (ref. 5), in good agreement with
the earlier observations
9,10
. The new data, which penetrate the bright
upper haze obscuring the main cloud at middle latitudes, find that
the cloud-top winds quickly decline poleward of 50u. The infrared
observations
6
sound the dynamics in the main cloud deck at , 50 km
altitude on the night side, finding strong vertical wind shear of about
3ms
21
km
21
below 50u, and no shear poleward of this latitude, when
compared with the higher-altitude ultraviolet-derived winds. The
wind velocity profiles on Venus are found to be roughly, although
not exactly, in agreement with those predicted by the cyclostrophic
Table 1
|
The scientific payload of Venus Express
Name (acronym) Description Measured parameters
ASPERA-4 Detection and characterization of neutral and charged particles Electrons 1 eV
–
20 keV; ions0.01
–
36 keV/q; neutral particles0.1
–
60 keV
MAG Dual sensor fluxgate magnetometer, one sensor on a 1-m-long boom B field 8 pT
–
262 nT at 128 Hz
PFS Planetary Fourier Spectrometer (currently not operating) Wavelength 0.9
–
45 mm; spectral resolving power about 1,200
SPICAV/SOIR Ultraviolet and infrared spectrometer for stellar and solar occultation
measurements and nadir observations
Wavelengths 110
–
320 nm, 0.7
–
1.65 mmand2.2
–
4.4 mm; spectral
resolving power up to 20,000
VeRa Radio Science investigation for radio-occultation and bi-static radar measurements X- and S-band Doppler shift, polarization and amplitude variations
VIRTIS Ultraviolet
–
visible
–
infrared imaging spectrometer and high-resolution infrared
spectrometer
Wavelength 0.25
–
5 mm for the imaging spectrometer and 2
–
5 mm for
the high-resolution channel; resolving power about 2,000
VMC Venus Monitoring Camera for wide-field imaging Four parallel channels at 365, 513, 965 and 1010 nm
These instruments are expected to produce more than 2 terabits of data during the design lifetime of four Venus sidereal days (about 1,000 Earth days). Venus Express is operating in an elliptical
polar orbit with a period of 24 h and an apocentre altitude of 66,000 km. The pericentre altitude is maintained between 250 and 400 km approximately over the north pole. q is elementary charge.
Polar vortex
Sub-solar to
anti-solar cell
Hadley cell
Cold
Cold
Warm Warm
Polar collar
Solar heating
EUV flux
Recombination
of O atoms
into O
2
(∆)
Night-side
airglow
CO
2
photodissociation
a
b
Figure 2
|
Schematic view of the general circulation of Venus’s atmosphere.
a
, The main featureis a convectively driven Hadley cell, which extends fromthe
equatorial region up to about 60u of latitude in each hemisphere. The trend is
polewards at all levels that can be observed by tracking the winds (at about
50–65 km altitude above the surface), so the return branchof thecell must be in
the atmospherebelowthe clouds.A cold‘polarcollar’ is foundaroundeach pole
at about 70u latitude; the Hadley circulation evidently feeds a mid-latitude jet at
its poleward extreme, inside which there is a circumpolar belt characterized by
remarkably low temperatures and dense, high clouds. Inside the collar a
thinning of the upper cloud layer forms a complex and highly variable feature,
called the ‘polar dipole’ in earlier literature describing poorly resolved
observations, which appears bright in the thermal infrared
6
. Because in general
terms thinner-than-average or lower-than-average cloud is often associated
with a descending air mass, and vice versa, the vortex may represent a second,
high-latitude circulation cell, resembling winter hemisphere behaviour on
Earth.
b, Above about 100 km altitude the circulation regime on Venus changes
completely to a sub-solar to anti-solar pattern. Oxygen airglow emission at
1.27 mm reveals the recombination of oxygen atoms into molecular oxygen
while descendingto lower altitudes in theanti-solar region.Additional evidence
ofthiscirculationis givenby theupper-atmospheretemperatureprofiles,which
show a pronounced temperature maximum on the night side that is due to
compressional heating in the downward branch of the circulation cell
8
.
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approximation
9
, which postulates a balance of pressure gradient
and centrifugal force in a purely zonal flow. This is, as expected, in
contrast with Earth, where so-called geostrophic balance generally
applies, dominated by the Coriolis forces produced by the relatively
rapid rotation of Earth.
Figure 3 summarizes the results so far of composition measure-
ments by Venus Express
8
. In the deep atmosphere, the most remark-
able result is the distribution of CO, which shows a larger systematic
latitudinal variability than the other minor species observed, includ-
ing water vapour. With a large source high in the atmosphere from
the photolysis of CO
2
and sinks in the clouds and near the surface,
and a lifetime measured in weeks, CO turns out to be an excellent
tracer of the general circulation. VIRTIS (Visible and Infrared
Thermal Imaging Spectrometer) global maps show a well-defined
maximum in the abundance of CO at a latitude of about 60u, near
the outer edge of the cold collar, which probably marks the poleward
extent of the Hadley cell (Fig. 2a). The other species seem to be much
more uniformly distributed over the globe in the deep atmosphere
but may be variable at the #10% level. The clouds show tremendous
variability, with a variety of meteorological systems in several differ-
ent layers, and distinct regions in which different mean particle sizes
predominate. There are, for instance, distinctly larger particle sizes in
the clouds in the polar region, although no definite departure from
the composition of sulphuric acid and water has been detected.
Upper atmosphere and plasma environment
The absence of an internal magnetic field for Venus means that the
solar wind interacts directly with the upper atmosphere, leading to a
different distribution of the energies and densities of electrons, ions
and energetic neutral atoms from that around Earth
11,12
(Fig. 4).
Venus Express measurements are taken at solar minimum, thus com-
plementing the Pioneer Venus plasma studies that were acquired
during solar maximum. Photoelectrons with a typical energy of
22–28 eV are measured in situ when the satellite dips into the iono-
sphere while passing the pericentre at 250–350 km. Below this alti-
tude the vertical distribution of electron density is sounded by radio
occultation
13
, suggesting a stable bottom of the ionosphere at 120 km.
The electron density peaks at about 4 3 10
5
cm
23
at about 140 km
altitude, and a very dynamic topside ionosphere is observed.
Simultaneous measurements of the vertical profiles of hydrogen-
bearing species in the upper atmosphere and plasma in situ monitor-
ing have begun to characterize the escape processes that have been
responsible for the depletion of water on Venus over the planet’s
history. Earlier measurements established a D/H ratio ,150 times
the terrestrial value in the lower atmosphere
14
, which is consistent
with the long-term loss of much larger amounts of hydrogen—
presumably from water—from Venus compared with Earth. Still
higher values of D/H, up to twofold higher, are now being found
above the clouds by SPICAV/SOIR (Spectroscopy for Investigation
of Characteristics of the Atmosphere of Venus/Solar Occultation
at Infrared), which has also uncovered strong variability in both
H
2
O and HDO content
8
. This unexpected behaviour has been
0.001 0.01 0.1 1.0 10 100 1,000
Mixin
g
ratio (p.p.m. by volume)
Altitude (km)
100
HF
HDO
HCl
HCl
H
2
O
H
2
O
SO
2
H
2
O
CO
CO
COS
80
60
40
20
0
Clouds
Figure 3
|
Atmospheric composition from the Venus Express observations.
The colours mark different trace gases. The vertical profiles of H
2
O, HDO,
CO, HCl and HF above the clouds have been derived from SPICAV/SOIR
solar occultation measurements
8
; the abundances of H
2
O, CO, SO
2
and COS
below the clouds are derived from VIRTIS spectra. The error bars in mixing
ratios indicate the minimum and maximum detections over all latitudes, and
the error bars in altitudes for the lower atmosphere indicate the width of the
weighting functions used for deriving the altitude. The bars with arrows in
the lower atmosphere show the expected sensitivity of the Venus Express
measurements for which data analysis is still in progress.
Solar wind
Escaping ions
H
+
, O
+
, He
+
Induced magnetopause
Bow shock
H
+
He
2+
B
sw
B
ps
B
t
0
1
2
3
0
–1
1
2
3–2
–3
Distance to Venus–Sun line (R
V
)
Venus–Sun line, x (R
V
)
Figure 4
|
The plasma environment of Venus as determined by Venus
Express.
All parametersnoted in the figure are measured on a regular basis by
the magnetometer and the ASPERA instrument, in three distinctly different
regions: the unperturbed solar wind (sw), the plasma sheath (ps) and the
induced magnetosphere/tail (t). The boundaries determined by the two
instruments are shown approximately to scale. Oxygen ions are observed at
high concentrations around the terminator and at lower concentrations well
into the tail, indicating escape from a specific source region. He
1
shows
similar behaviour, whereas H
1
is observed much more evenly distributed
around the planet
11
. The figure shows cylindrical coordinates; the x axis is
aligned with the Venus–Sun line. R
V
, radius of Venus.
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tentatively explained by a combination of fractionation in the con-
densation of ice particles and atmospheric transport, which would
imply that species bearing hydrogen and deuterium are already frac-
tionated in the mesosphere right beneath the region from which
escape occurs.
ASPERA-4 (Analyser of Space Plasmas and Energetic Atoms 4) has
established for the first time the composition of the escaping plan-
etary ions, finding that, after H
1
, the main escaping ion is O
1
. This is
in contrast with Mars, where the escaping plasma consists of approxi-
mately equal amounts of O
1
,O
2
1
and CO
2
1
, and it results from the
higher gravitational acceleration at Venus, which tends to retain
heavier components such as CO
2
1
. High fluxes of escaping He
1
are also detected
11
. Oxygen and hydrogen ions are formed by the
dissociation of neutral atmospheric species, including water, by solar
ultraviolet radiation, which are then blown away towards the outer
reaches of the Solar System (Fig. 4). This happens at a faster rate on
Venus than on Earth, not just because Venus is closer to the Sun but
also because it lacks the magnetic field that protects Earth from the
flux of energetic charged particles from the Sun. These loss processes
must have removed large amounts of water from Venus during the
first billion years or so after the formation of the Solar System. A
detailed quantification of the loss rates enables a more accurate
estimate of how much water Venus has lost over its entire history,
and by the end of the mission we should know better whether the
planet once had an ocean as extensive and deep as Earth’s.
Lightning
For a long time the existence of lightning on Venus has been contro-
versial. Whistler-mode waves, which can be considered reliable evid-
ence of lightning, were detected by the Venus Express magnetometer
during more than 10% of the pericentre passes
15
. This corresponds to
a lightning rate at least half that of Earth. Frequent lightning repre-
sents a significant energy input that has important implications for
the chemistry in the lower and middle atmosphere on Earth, and this
now seems likely to be true for Venus also.
Venus is more Earth-like
The overall sense of the results from the first year of operation of
Venus Express is that the differences, particularly in climate, between
Venus and Earth are much less mysterious than previously thought
after the early phase of spacecraft exploration. They are consistent
with theoretical ideas and interpretations suggesting that the two
planets had similar surface environments in the past and that they
evolved differently, with Earth’s oceans converting most of its atmo-
spheric CO
2
to carbonate rocks, and Venus losing most of its water to
space. Both processes can now be seen to be still going on. The high
zonal winds and near-equatorial turbulence on Venus, as well of
course as the high surface temperatures, result from the depth of
the atmosphere and huge inventory of greenhouse gas retained by
Venus. The slow rotation of Venus, as well as possibly being respon-
sible for the lack of magnetic field that makes erosion of the atmo-
sphere by the solar wind so effective, permits the Earth-like Hadley
cell component of the atmospheric circulation to extend closer to the
poles, where it breaks down in spectacular fashion to form mid-
latitude jets and polar vortices that are larger and more energetic
than Earth’s but are in many respects quite similar.
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Acknowledgements We thank R. Hueso and J. Bailey for the provision of graphics
and data for Fig. 2b, and E. Marcq, C. Tsang, P. Drossart and J.-L. Bertaux for
providing data for Fig. 3.
Author Information Reprints and permissions information is available at
www.nature.com/reprints. Correspondence should be addressed to H.S.
(h.svedhem@esa.int).
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