|Atmosphere of Venus|
Cloud structure in Venus' atmosphere,
|Average surface pressure||(92 bar or) 9.2 MPa|
|Mass||4.8 × 1020 kg|
|Carbon dioxide||96.5 %|
|Sulfur dioxide||150 ppm|
|Water vapor||20 ppm|
|Carbon monoxide||17 ppm|
|Hydrogen chloride||0.1–0.6 ppm|
|Hydrogen fluoride||0.001–0.005 ppm|
In 1761, Russian polymath Mikhail Lomonosov discovered that Venus has an atmosphere. Its atmosphere is much denser and hotter than that of Earth. The temperature and pressure at the surface are 740 K (467°C, 872°F) and 93 bar, respectively. The Venusian atmosphere supports opaque clouds made of sulfuric acid, making optical observation of the surface impossible. Information about the topography of Venus has been obtained exclusively by radar imaging. The main atmospheric gases on Venus are carbon dioxide and nitrogen. Other chemical compounds are present only in trace amounts.
The atmosphere of Venus is in a state of vigorous circulation and super-rotation. The whole atmosphere circles the planet in just four Earth days, much faster than Venus' sideral day of 243 days. The winds supporting super-rotation blow as fast as 100 m/s (~220 mph). Near the poles are anticyclonic structures called polar vortexes. Each vortex is double-eyed and shows a characteristic S-shaped pattern of clouds.
Unlike Earth, Venus lacks a magnetic field. Its ionosphere separates the atmosphere from outer space and the solar wind. This ionized layer excludes the solar magnetic field, giving Venus a distinct magnetic environment. This is considered Venus' induced magnetosphere. Lighter gases, including water vapor, are continuously blown away by the solar wind through the induced magnetotail. It is currently thought that the atmosphere of Venus up to around 4 billion years ago was more like that of the Earth with liquid water on the surface. The runaway greenhouse effect may have been caused by the evaporation of the surface water and subsequent rise of the levels of other greenhouse gases.
Despite the harsh conditions on the surface, the atmospheric pressure and temperature at about 50 km to 65 km above the surface of the planet is nearly the same as that of the Earth, making its upper atmosphere the most Earth-like area in the Solar System, even more so than the surface of Mars. Due to the similarity in pressure and temperature and the fact that breathable air (21% oxygen, 78% nitrogen) is a lifting gas on Venus in the same way that helium is a lifting gas on Earth, the upper atmosphere has been proposed as a location for both exploration and colonization.
Structure and compositionEdit
The atmosphere of Venus is composed mainly of carbon dioxide, along with a small amount of nitrogen and other trace elements. The amount of nitrogen in the atmosphere is relatively small compared to the amount of carbon dioxide, but as the atmosphere is so much thicker than that on Earth, its total nitrogen content is roughly four times higher than Earth's, even though on Earth nitrogen makes up about 78% of the atmosphere.
The atmosphere contains a range of interesting compounds in small quantities, including some based on hydrogen, such as hydrogen chloride (HCl) and hydrogen fluoride (HF). There are carbon monoxide, water vapor and molecular oxygen as well. A large amount of the planet's hydrogen is theorised to have been lost to space, with the remainder being mostly bound up in sulfuric acid (H2SO4) and hydrogen sulfide. Subsequently, hydrogen is in relatively short supply in the Venusian atmosphere. The loss of significant amounts of hydrogen is proved by a very high D/H ratio measured in the Venusian atmosphere. The ratio is about 0.025, which is much higher than the terrestrial value of 1.6×10−4. In addition, in the upper atmosphere of Venus D/H ratio is 1.5 higher than in the bulk atmosphere.
The atmosphere is divided into a number of sections depending on altitude. The densest part of the atmosphere, the troposphere, begins at the surface and extends upwards to 65 km. At the furnace-like surface the winds are slow, but at the top of the troposphere the temperature and pressure reaches Earth-like levels and clouds pick up speed to 100 m/s.
The atmospheric pressure at the surface of Venus is about 92 times that of the Earth, similar to the pressure found 910 metres below the surface of the ocean. The atmosphere has a mass of 4.8×1020 kg, about 93 times the mass of the Earth's total atmosphere. The pressure found on Venus's surface is high enough that the carbon dioxide is technically no longer a gas, but a supercritical fluid. The density of the air at the surface is 67 kg/m3, which is 6.5% that of liquid water on Earth.
The large amount of CO2 in the atmosphere together with water vapor and sulfur dioxide create a strong greenhouse effect, trapping solar energy and raising the surface temperature to around 740 K (467°C), hotter than any other planet in the solar system, even that of Mercury despite being located further out from the Sun and receiving only 25% of the solar energy Mercury does. The average temperature on the surface is above the melting points of lead 600 K (327°C), tin 505 K (232°C), and zinc 693 K (420°C). The thick troposphere also makes the difference in temperature between the day and night side small, even though the slow retrograde rotation of the planet causes a single solar day to last 116.5 days on Earth. The surface of Venus spends 58.3 days of darkness before the sun rises again behind the clouds.
The troposphere on Venus contains 99% of the atmosphere by mass. Ninety percent of the atmosphere of Venus is within 28 km of the surface, by comparison, ninety percent of the atmosphere of Earth is within 10 km of the surface. At a height of 50 km the atmospheric pressure is approximately equal to that at the surface of Earth. On the night side of Venus clouds can still be found at 80 km above the surface.
The area of the troposphere most similar to Earth is near the tropopause—the boundary between troposphere and mesosphere. It is located slightly above 50 km. According to measurements by the Magellan and Venus Express probes, the area from 52.5 to 54 km has a temperature between 293 K (20 °C) and 310 K (37°C), and the area at 49.5 km above the surface is where the pressure becomes the same as Earth at sea level. As manned ships sent to Venus would be able to compensate for differences in temperature to a certain extent, anywhere from about 50 to 54 km or so above the surface would be the easiest area in which to base an exploration or colony, where the temperature would be in the crucial "liquid water" range of 273 K (0°C) to 323 K (50°C) and the air pressure the same as habitable regions of Earth.
The circulation in Venus's troposphere follows the so-called cyclostrophic approximation. Its windspeeds are roughly determined by the balance of the pressure gradient and centrifugal forces in almost purely zonal flow. In contrast, the circulation in the Earth's atmosphere is governed by the geostrophic balance. Venus's windspeeds can be directly measured only in the upper troposphere (tropopause), between 60–70 km, altitude, which corresponds to the upper cloud deck. The cloud motion is usually observed in the ultraviolet part of the spectrum, where the contrast between clouds is the highest. The linear wind speeds at this level are about 100 ± 10 m/s at lower than 50° latitude. They are retrograde in the sense that they blow in the direction of the retrograde rotation of the planet. The winds quickly decrease towards the higher latitudes, eventually reaching zero at the poles. Such strong cloud-top winds cause a phenomenon known as the super-rotation of the atmosphere. In other words, these high-speed winds circle the whole planet faster than the planet itself rotates. The super-rotation on Venus is differential, which means that the equatorial troposphere super-rotates more slowly than the troposphere at the midlatitudes. The winds also have a strong vertical gradient. They decline deep in the troposphere with the rate of 3 m/s per km. The winds near the surface of Venus are much slower than that on Earth. They actually move at only a few kilometers per hour (generally less than 2 m/s and with an average of 0.3 to 1.0 m/s), but due to the high density of the atmosphere at the surface, this is still enough to transport dust and small stones across the surface, much like a slow-moving current of water.
All winds on Venus are ultimately driven by convection. Hot air rises in the equatorial zone, where solar heating is concentrated, and flows to the poles. Such an almost-planetwide overturning of the troposphere is called Hadley circulation. However, the meridional air motions are much slower than zonal winds. The poleward limit of the planet wide Hadley cell on Venus is near ±60° latitudes. Here air starts to descend and returns to the equator below the clouds. This interpretation is supported by the distribution of the carbon monoxide, which is also concentrated in the vicinity of ±60° latitudes. Poleward of the Hadley cell a different pattern of circulation is observed. In the latitude range 60°–70° cold polar collars exist. They are characterised by temperatures about 30–40 K lower than in the upper troposphere at nearby latitudes. The lower temperature is probably caused by the upwelling of the air in them and by the resulting adiabatic cooling. Such an interpretation is supported by the denser and higher clouds in the collars. The clouds lie at 70–72 km altitude in the collars—about 5 km higher than at the poles and low latitudes. A connection may exist between the cold collars and high speed midlatitude jets in which winds blow as fast as 140 m/s. Such jets are a natural consequence of the Hadley–type circulation and should exist on Venus between 55–60° latitude.
Odd structures known as polar vortices lie within the cold polar collars. They are giant hurricane-like storms four times larger than their terrestrial analogs. Each vortex has two "eyes"—the centers of rotation, which are connected by distinct S-shaped cloud structures. Such double eyed structures are also called polar dipoles. Vortexes rotate with the period of about 3 days in the direction of general super-rotation of the atmosphere. The linear wind speeds are 35–50 m/s near their outer edges and zero at the poles. The temperature at the cloud-tops in the polar vortexes are much higher than in the nearby polar collars reaching 250 K (−23°C). The conventional interpretation of the polar vortexes is that they are anticyclones with downwelling in the center and upwelling in the cold polar collars. This type of circulation resembles the winter polar anticyclonic vortexes on Earth, especially the one found over Antarctica. The observations in the various infrared atmospheric windows indicate that the anticyclonic circulation observed near the poles may penetrate as deep as to 50 km altitude, i.e. to the base of the clouds. The polar upper troposphere and mesosphere are extremely dynamic; large bright clouds may appear and disappear over the space of a few hours. One such event was observed by Venus Express between 9 and 13 January 2007, when the south polar region became brighter by 30%. This event was probably caused by an injection of sulfur dioxide into the mesosphere, which then condensed forming a bright haze. The two eyes in the vortexes have yet to be explained.
The first vortex on Venus was discovered at the north pole by the Pioneer Venus mission in 1978. A discovery of the second large 'double-eyed' vortex at the south pole of Venus was made in the summer of 2006 by Venus Express, which came with no surprise.
Upper atmosphere and ionosphereEdit
The mesosphere of Venus extends from 65 km to 120 km in height, and the thermosphere begins at around 120, eventually reaching the upper limit of the atmosphere (exosphere) at about 220 to 350 km. The exosphere is the altitude at which the atmosphere becomes collisonless.
The mesosphere of Venus can be divided into two layers: the lower one between 62–73 km and the upper one between 73–95 km. In the first layer the temperature is nearly constant at 230 K (−43°C). This layer coincides with the upper cloud deck. In the second layer temperature starts to decrease again reaching about 165 K (−108°C) at the altitude of 95 km, where mesopause begins. It is the coldest part of the Venusian dayside atmosphere. In the dayside mesopause, which serves as a boundary between the mesophere and thermosphere and is located between 95–120 km, temperature grows up to a constant—about 300–400 K (27–127°C)—value prevalent in the thermosphere. In contrast the nightside Venusian thermosphere is the coldest place on Venus with temperature as low as 100 K (−173°C). It is even called a cryosphere.
The circulation patterns in the upper mesosphere and thermosphere of Venus are completely different from those in the lower atmosphere. At altitudes 90–150 km the Venusian air moves from the dayside to nightside of the planet, with upwelling over sunlit hemisphere and downwelling over dark hemisphere. The downwelling over the nightside causes adiabatic heating of the air, which forms a warm layer in the nightside mesosphere at the altitudes 90–120 km. The temperature of this layer—230 K (−43°C) is far higher than the typical temperature found in the nightside thermosphere—100 K (−173°C). The air circulated from the dayside also carries oxygen atoms, which after recombination form excited molecules of oxygen in the long lived singlet state (1Δg), which then relax and emit infrared radiation at the wavelength 1.27 μm. This radiation from the altitude range 90–100 km is often observed from the ground and spacecraft. The nightside upper mesosphere and thermosphere of Venus is also the source of non-LTE (non-local thermodynamic equilibrium) emissions of CO2 and NO molecules, which are responsible for the low temperature of the nightside thermosphere.
The Venus Express probe has shown through stellar occultation that the atmospheric haze extends much further up on the night side than the day side. On the day side the cloud deck has a thickness of 20 km and extends up to about 65 km, whereas on the night side the cloud deck in the form of a thick haze reaches up to 90 km in altitude—well into mesosphere, continuing even further to 105 km as a more transparent haze.
Venus has an extended ionosphere located at altitudes 120–300 km. The ionosphere almost coincides with the thermosphere. The high levels of the ionisation are maintained only over the dayside of the planet. Over the nightside the concentration of the electrons is almost zero. The ionosphere of Venus consists of three layers: v1 between 120–130 km, v2 between 140–160 km and v3 between 200–250 km. There may be an additional layer near 180 km. The maximum electron volume density (number of electrons in a unit of volume) 3×1011 m−3 is reached in the v2 layer near the subsolar point. The upper boundary of the ionosphere—ionopause is located at altitudes 220–375 km and separates the plasma of the planetary origin from that of the induced magnetosphere. The main ionic species in the v1 and v2 layers is O2+ ion, whereas the v3 layer consists of O+ ions.
Venus is known not to have a magnetic field. The reason for its absence is not clear, but is probably related to the planet's slow rotation or the lack of convection in the mantle. Venus only has an induced magnetosphere formed by the Sun's magnetic field carried by the solar wind. This process can be understood as the field lines wrapping around an obstacle—Venus in this case. The induced magnetosphere of Venus has a bow shock, magnetosheath, magnetopause and magnetotail with the current sheet.
At the subsolar point the bow shock stands 1900 km (0.3 Rv, where Rv is the radius of Venus) above the surface of Venus. This distance was measured in 2007 near the solar activity minimum. Near the solar activity maximum it can be several times further from the planet. The magnetopause is located at the altitude of 300 km. The upper boundary of the ionosphere (ionopause) is near 250 km. Between the magnetopause and ionopause there exists a magnetic barrier—a local enhancement of the magnetic field, which prevents solar plasma from penetrating deeper into the Venusian atmosphere, at least near solar activity minimum. The magnetic field in the barrier reaches up to 40 nT. The magnetotail continues up to ten radiuses from the planet. It is the most active part of the Venusian magnetosphere. There are reconnection events and particle acceleration in the tail. The energies of electrons and ions in the magnetotail are around 100 ev and 1000 ev respectively.
Due to the lack of the intrinsic magnetic field on Venus, the solar wind penetrates relatively deep into the planetary exosphere and causes substantial atmosphere loss. The loss happens mainly via the magnetotail. Currently the main ion types being lost are O+, H+ and He+. The ratio of hydrogen to oxygen losses is around 2 (i.e. almost stoichometric) indicating the ongoing loss of water.
Venusian clouds are thick and are composed of sulfur dioxide and droplets of sulfuric acid. These clouds reflect about 75% of the sunlight that falls on them, which is what obscures the surface of Venus from regular imaging. The reflectivity of the clouds causes the amount of light reflected upward to be nearly the same as that coming in from above, and a probe exploring the cloud tops could harness solar energy almost as well from below as above, enabling solar cells to be fitted just about anywhere.
The cloud cover is such that very little sunlight can penetrate down to the surface, and the light level is only around 5,000–10,000 lux with a visibility of three kilometres. At this level little to no solar energy could conceivably be collected by a probe. Humidity at this level is less than 0.1%. In fact, due to the thick, highly reflective cloud cover the total solar energy received by the planet is less than that of the Earth.
Sulfuric acid is produced in the upper atmosphere by the sun's photochemical action on carbon dioxide, sulfur dioxide, and water vapor. Ultraviolet photons of wavelengths less than 169 nm can photodissociate carbon dioxide into carbon monoxide and atomic oxygen. Atomic oxygen is highly reactive; when it reacts with sulfur dioxide, a trace component of the Venusian atmosphere, the result is sulfur trioxide, which can combine with water vapor, another trace component of Venus' atmosphere, to yield sulfuric acid.
Venus's sulfuric acid rain never reaches the ground, but is evaporated by the heat before reaching the surface in a phenomenon known as virga. It is theorized that early volcanic activity released sulfur into the atmosphere and the high temperatures prevented it from being trapped into solid compounds on the surface as it was on the Earth.
The clouds of Venus are capable of producing lightning much like the clouds on Earth. The existence of lightning had been controversial since the first suspected bursts were detected by the Soviet Venera probes. However in 2006–2007 Venus Express was reported to detect whistler mode waves, which were attributed to lightning. Their intermittent appearance indicates a pattern associated with weather activity. The lightning rate is at least half of that on Earth.
In 2009 a prominent bright spot in the atmosphere was noted by an amateur astronomer and photographed by Venus Express. Its cause is currently unknown, with surface vulcanism advanced as a possible explanation.
Possibility of lifeEdit
Due to the harsh conditions on the surface, little of the planet has been explored; in addition to the fact that life as currently understood may not necessarily be the same in other parts of the universe, the extent of the tenacity of life on Earth itself has not yet been shown. Creatures known as extremophiles exist on Earth, preferring extreme habitats. Thermophiles and hyperthermophiles thrive at temperatures reaching above the boiling point of water, acidophiles thrive at a pH level of 3 or below, polyextremophiles can survive a varied number of extreme conditions, and many other types of extremophiles exist on Earth.
However, life could also exist outside of the extremophile range in the cloudtops, and in the same way that bacteria have been found living and reproducing in clouds on Earth, it has been proposed that life could exist in the same area on Venus. Microbes in the thick, cloudy atmosphere could be protected from solar radiation by the sulfur compounds in the air.
The Venusian atmosphere has been found to be sufficiently out of equilibrium as to require further investigation. Analysis of data from the Venera, Pioneer and Magellan missions has found the chemicals hydrogen sulfide (H2S) and sulfur dioxide (SO2) together in the upper atmosphere, as well as carbonyl sulfide (OCS). The first two gases react with each other, implying that something must produce them. In addition, carbonyl sulfide is noteworthy for being exceptionally difficult to produce through inorganic means. Were it on Earth, this compound would be considered an "unambiguous indicator of life". Further, it is an often overlooked fact that one of the early Venera probes detected large amounts of chlorine just below the Venusian cloud deck.
It has been proposed that microbes at this level could be soaking up ultraviolet light from the sun as a source of energy, which could be a possible explanation for dark patches seen on UV images of the planet. Large, non-spherical cloud particles have also been detected in the cloud decks. Their composition is still unknown.
Through studies of the present cloud structure and geology of the surface combined with the fact that the luminosity of the Sun has increased by 25% since around 3.8 billion years ago, it is thought that the atmosphere of Venus up to around 4 billion years ago was more like that of Planet Earth with liquid water on the surface. The runaway greenhouse effect may have been caused by the evaporation of the surface water and the rise of the levels of greenhouse gases that followed. Venus' atmosphere has therefore received a great deal of attention from those studying climate change on Earth.
There are no geologic forms on the planet to suggest the presence of water over the past billion years. However there is no reason to suppose that Venus was an exception to the processes that formed Earth and gave it its water during its early history, possibly from the original rocks that formed the planet or later on from comets. The common view among research scientists is that water would have existed for about 600 million years on the surface before evaporating, though some such as David Grinspoon believe that up to 2 billion years could also be plausible.
Observations and measurement from EarthEdit
The upper atmosphere of Venus can be measured from Earth when the planet crosses the sun in a rare event known as a solar transit. The last solar transit of Venus occurred in 2004. Using quantitative astronomical spectroscopy, scientists were able to analyze sunlight that passed through the planet's atmosphere to reveal chemicals within it. As the technique to analyze light to discover information about a planet's atmosphere only first showed results in 2001, this was the first opportunity to gain conclusive results in this way on the atmosphere of Venus since observation of solar transits began. This solar transit was a rare opportunity considering the lack of information on the atmosphere between 65 and 85 km. The solar transit in 2004 enabled astronomers to gather a large amount of data useful not only in determining the composition of the upper atmosphere of Venus, but also in refining techniques used in searching for extrasolar planets. The atmosphere of mostly CO2, absorbs near-infrared radiation, making it easy to observe. During the 2004 transit, the absorption in the atmosphere as a function of wavelength revealed the properties of the gases at that altitude. The Doppler shift of the gases also enabled wind patterns to be measured.
A solar transit of Venus is an extremely rare event, and the last solar transit of the planet before 2004 was in 1882. The next solar transit is in 2012. However, after the solar transit in 2012, another one will not occur for 105 years.
The Venus Express spacecraft is now in orbit around the planet, probing deeper into the atmosphere using infrared imaging spectroscopy in the 1–5 µm spectral range. the JAXA probe PLANET-C to be launched in 2010 will study the planet for a period of two years, including the structure and activity of the atmosphere. One of its five cameras known as the "IR2" will be able to measure the atmosphere of the planet underneath its thick clouds, in addition to its movement and distribution of trace components. With a varied orbit from 300 to 60,000 km, it will be able to take close-up photographs of the planet, and should also confirm the presence of both active volcanoes as well as lightning.
The Venus In-Situ Explorer, proposed by NASA's New Frontiers program is a proposed probe which would aid in understanding the processes on the planet that led to climate change, as well as paving the way towards a later sample return mission.
Another craft called the Venus Mobile Explorer has been proposed by the Venus Exploration Analysis Group (VEXAG) to study the composition and isotopic measurements of the surface and the atmosphere, for about 90 days. A launch date has not yet been set.
After missions discovered the reality of the harsh nature of the planet's surface, attention shifted towards other targets such as Mars. There have been a number of proposed missions recently however, and many of these involve the little-known upper atmosphere. The Soviet Vega program in 1985 dropped two balloons into the atmosphere, but these were battery-powered and lasted for only about two Earth days each before running out of power and since then there has been no exploration of the upper atmosphere. In 2002 the NASA contractor Global Aerospace proposed a balloon that would be capable of staying in the upper atmosphere for hundreds of Earth days as opposed to two.
A solar flyer has also been proposed by Geoffrey A. Landis in place of a balloon, and the idea has been featured from time to time since the early 2000s. Venus has a high albedo, and reflects most of the sunlight that shines on it making the surface quite dark, the upper atmosphere at 60 km has an upward solar intensity of 90%, meaning that solar panels on both the top and the bottom of a craft could be used with nearly equal efficiency. In addition to this, the slightly lower gravity, high air pressure and slow rotation allowing for perpetual solar power make this part of the planet ideal for exploration. The proposed flyer would operate best at an altitude where sunlight, air pressure and wind speed would enable it to remain in the air perpetually, with slight dips down to lower altitudes for a few hours at a time before returning to higher altitudes. As sulfuric acid in the clouds at this height is not a threat for a properly-shielded craft, this so-called "solar flyer" would be able to measure the area in between 45 km and 60 km indefinitely, as long as mechanical error or unforeseen problems do not cause it to fail. Landis also proposed that rovers similar to Spirit and Opportunity could possibly explore the surface, with the difference being that Venus surface rovers would be "dumb" rovers controlled by radio signals from computers located in the flyer above, only requiring parts such as motors and transistors to withstand the surface pressure, but not weaker parts involved in microelectronics that could not be made resistant to the heat, pressure and acidic conditions.
- ↑ 1.00 1.01 1.02 1.03 1.04 1.05 1.06 1.07 1.08 1.09 1.10 1.11 Basilevsky, Alexandr T.; Head, James W. (2003). "The surface of Venus" (abstract page). Rep. Prog. Phys. 66: 1699–1734. doi:10.1088/0034-4885/66/10/R04, http://www.iop.org/EJ/abstract/0034-4885/66/10/R04/.
- ↑ 2.0 2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 2.9 Bertaux, Jean-Loup; Vandaele, Ann-Carine; Korablev, Oleg; et al. (2007). "A warm layer in Venus’ cryosphere and high-altitude measurements of HF, HCl, H2O and HDO". Nature 450: 646–649. doi:10.1038/nature05974, http://adsabs.harvard.edu/abs/2007Natur.450..646B.
- ↑ Marov, Mikhail Ya. (2004). "Mikhail Lomonosov and the discovery of the atmosphere of Venus during the 1761 transit". Proceedings of the International Astronomical Union (Cambridge University Press) 2004 (IAUC196): 209–219. doi:10.1017/S1743921305001390, http://adsabs.harvard.edu/abs/2005tvnv.conf..209M.
- ↑ Britannica online encyclopedia: Mikhail Vasilyevich Lomonosov
- ↑ 5.00 5.01 5.02 5.03 5.04 5.05 5.06 5.07 5.08 5.09 5.10 5.11 5.12 5.13 5.14 5.15 5.16 5.17 5.18 Svedhem, Hakan; Titov, Dmitry V.; Taylor, Fredric V.; Witasse, Oliver (2007). "Venus as a more Earth-like planet". Nature 450: 629–632. doi:10.1038/nature06432, http://adsabs.harvard.edu/abs/2007Natur.450..629S.
- ↑ 6.0 6.1 6.2 6.3 6.4 6.5 6.6 6.7 6.8 Piccioni, G.; Drossart, P.; Sanchez-Lavega, A.; et al. (2007). "South-polar features on Venus similar to those near the north pole". Nature 450: 637–640. doi:10.1038/nature06209, http://adsabs.harvard.edu/abs/2007Natur.450..637P.
- ↑ 7.0 7.1 Kasting, J (1988). "Runaway and moist greenhouse atmospheres and the evolution of Earth and Venus". Icarus 74: 472–494. doi:10.1016/0019-1035(88)90116-9, http://adsabs.harvard.edu/abs/1988Icar...74..472K.
- ↑ 8.0 8.1 Landis, Geoffrey A. (2003). "Colonization of Venus". AIP Conf. Proc. 654 (1): 1193–1198. doi:10.1063/1.1541418, http://link.aip.org/link/?APCPCS/654/1193/1.
- ↑ 9.0 9.1 "Clouds and atmosphere of Venus". Institut de mécanique céleste et de calcul des éphémérides. Retrieved on 2008-01-22.
- ↑ Lovelock, James (1979). Gaia: A New Look at Life on Earth, Oxford University Press. ISBN 0-19-286218-9.
- ↑ 11.00 11.01 11.02 11.03 11.04 11.05 11.06 11.07 11.08 11.09 11.10 Patzold, M.; Hausler, B.; Bird, M.K.; et al. (2007). "The structure of Venus’ middle atmosphere and ionosphere". Nature 450: 657–660. doi:10.1038/nature06239, http://adsabs.harvard.edu/abs/2007Natur.450..657P.
- ↑ 13.0 13.1 "Flying over the cloudy world – science updates from Venus Express". Venus Today (2006-07-12). Retrieved on 2007-01-17.
- ↑ "Venus Atmosphere Temperature and Pressure Profiles". Shade Tree Physics. Retrieved on 2008-01-23.
- ↑ 15.0 15.1 15.2 Landis, Geoffrey A.; Colozza, Anthony; and LaMarre, Christopher M. "Atmospheric Flight on Venus" (PDF) in 40th Aerospace Sciences Meeting and Exhibit sponsored by the American Institute of Aeronautics and Astronautics. Proceedings: IAC–02–Q.4.2.03, AIAA-2002-0819, AIAA0.
- ↑ 16.0 16.1 16.2 16.3 16.4 16.5 16.6 Markiewicz, W.J.; Titov, D.V.; Limaye, S.S.; et al. (2007). "Morphology and dynamics of the upper cloud layer of Venus". Nature 450: 633–636. doi:10.1038/nature06320, http://adsabs.harvard.edu/abs/2007Natur.450..633M.
- ↑ Moshkin, B.E.; Ekonomov, A.P., Golovin Iu.M. (1979). "Dust on the surface of Venus". Kosmicheskie Issledovaniia (Cosmic Research) 17: 280–285, http://adsabs.harvard.edu/abs/1979KosIs..17..280M.
- ↑ 18.0 18.1 "Double vortex at Venus South Pole unveiled!". European Space Agency (2006-06-27). Retrieved on 2008-01-17.
- ↑ Emily Lakdawalla (2006-04-14). "First Venus Express VIRTIS Images Peel Away the Planet's Clouds". Archived from the original on 2006-04-21. Retrieved on 2008-01-17.
- ↑ This thickness correspond to the polar latitudes. It is narrower near the equator—65–67 km.
- ↑ 21.0 21.1 Drossart, P.; Piccioni, G.; Gerard, G.C.; et al. (2007). "A dynamic upper atmosphere of Venus as revealed by VIRTIS on Venus Express". Nature 450: 641–645. doi:10.1038/nature06140, http://adsabs.harvard.edu/abs/2007Natur.450..641D.
- ↑ 22.0 22.1 22.2 22.3 22.4 Russell, C.T. (1993). "Planetary Magnetospheres". Rep. Prog. Phys. 56: 687–732. doi:10.1088/0034-4885/56/6/001, http://adsabs.harvard.edu/abs/1993RPPh...56..687R.
- ↑ 23.0 23.1 23.2 23.3 23.4 23.5 Zhang, T.L.; Delva, M.; Baumjohann, W.; et al. (2007). "Little or no solar wind enters Venus’ atmosphere at solar minimum". Nature 450: 654–656. doi:10.1038/nature06026, http://adsabs.harvard.edu/abs/2007Natur.450..654Z.
- ↑ 24.0 24.1 Barabash, S.; Fedorov, A.; Sauvaud, J.J.; et al. (2007). "The loss of ions from Venus through the plasma wake". Nature 450: 650–653. doi:10.1038/nature06434, http://adsabs.harvard.edu/abs/2007Natur.450..650B.
- ↑ 2004 Venus Transit information page, Venus Earth and Mars, NASA
- ↑ Krasnopolsky, V.A.; Parshev V.A. (1981). "Chemical composition of the atmosphere of Venus". Nature 292: 610–613. doi:10.1038/292610a0, http://adsabs.harvard.edu/abs/1981Natur.292..610K.
- ↑ This is the spherical albedo. The geometrical albedo is 85%.
- ↑ 28.0 28.1 Landis, Geoffrey A. (2001). "Exploring Venus by Solar Airplane". AIP Conference Proceedings (American Institute of Physics) 522: 16–18. doi:10.1063/1.1357898, http://adsabs.harvard.edu/abs/2001AIPC..552...16L.
- ↑ Koehler, H. W. (1982). "Results of the Venus sondes Venera 13 and 14". Sterne und Weltraum 21: 282, http://adsabs.harvard.edu/abs/1982S&W....21..282K.
- ↑ "Planet Venus: Earth's 'evil twin'", BBC News (7 November 2005).
- ↑ http://hyperphysics.phy-astr.gsu.edu/HBASE/Solar/venusenv.html
- ↑ 32.0 32.1 Russell, C.T.; Zhang, T.L.; Delva, M.; et al. (2007). "Lightning on Venus inferred from whistler-mode waves in the ionosphere". Nature 450: 661–662. doi:10.1038/nature05930, http://adsabs.harvard.edu/abs/2007Natur.450..661R.
- ↑ "Experts puzzled by spot on Venus", BBC News (1 August 2009).
- ↑ 34.0 34.1 34.2 34.3 Cockell, Charles S (1999). "Life on Venus". Plan.Space Sci. 47: 1487–1501. doi:10.1016/S0032-0633(99)00036-7, http://adsabs.harvard.edu/abs/1999P%26SS...47.1487C.
- ↑ Landis, Geoffrey A. (2003). "Astrobiology: the Case for Venus". J. of the British Interplanetary Society 56 (7/8): 250–254, http://gltrs.grc.nasa.gov/citations/all/tm-2003-212310.html.
- ↑ Grinspoon, David (1998). Venus Revealed: A New Look Below the Clouds of Our Mysterious Twin Planet. Reading, Mass.: Addison-Wesley Pub.. ISBN 978-0201328394.
- ↑ "Venus could be a haven for life", ABC News (2002-09-28).
- ↑ Newman, M.J.; Rood, R. T. (1977). "Implications of solar evolution for the Earth’s early atmosphere". Science 198 (4321): 1035–1037. doi:10.1126/science.198.4321.1035. PMID 17779689, http://adsabs.harvard.edu/abs/1977Sci...198.1035N.
- ↑ Henry Bortman (2004-08-26). "Was Venus Alive? The Signs are Probably There". Astrobiology Magazine. Retrieved on 2008-01-17.
- ↑ Robert Roy Britt (2001-11-27). "First Detection Made of an Extrasolar Planet's Atmosphere". Space.com. Archived from the original on 2001-11-28. Retrieved on 2008-01-17.
- ↑ 41.0 41.1 "Venus' Atmosphere to be Probed During Rare Solar Transit". Space.com (2004-06-07). Archived from the original on 2004-06-08. Retrieved on 2008-01-17.
- ↑ 42.0 42.1 "NCAR Scientist to View Venus's Atmosphere during Transit, Search for Water Vapor on Distant Planet]". National Center for Atmospheric Research and UCAR Office of Programs (2004-06-03). Retrieved on 2008-01-17.
- ↑ "Venus Exploration Mission PLANET-C". Japan Aerospace Exploration Agency (2006-05-17). Retrieved on 2008-01-17.
- ↑ "New Frontiers Program - Program Description". NASA. Retrieved on 2008-01-17.
- ↑ "Venus Mobile Explorer -Description". NASA. Retrieved on 2008-12-23.
- ↑ Myers, Robert (2002-11-13). "Robotic Balloon Probe Could Pierce Venus's Deadly Clouds", SPACE.com. Retrieved on 17 January 2008. Archived from the original on 6 December 2002.
- ↑ Landis, Geoffrey A. (2006). "Robotic Exploration of the Surface and Atmosphere of Venus". Acta Astronautica 59: 570–579. doi:10.1016/j.actaastro.2006.04.011.
- ↑ Paul Marks (2005-05-08). "To conquer Venus, try a plane with a brain". NewScientist.com. Retrieved on 2008-01-17.