| Extrasolar planet | List of extrasolar planets | |
|---|---|---|
| Parent star | ||
| Star | Gliese 581 | |
| Constellation | Libra | |
| Right ascension | (α) | 15h 19m 26s |
| Declination | (δ) | −07° 43′ 20″ |
| Apparent magnitude | (mV) | 10.55 |
| Distance | 20.3 ± 0.3 ly (6.2 ± 0.1 pc) |
|
| Spectral type | M3V | |
| Mass | (m) | 0.31 M☉ |
| Radius | (r) | 0.29 R☉ |
| Temperature | (T) | 3480 ± 48 K |
| Metallicity | [Fe/H] | -0.33 ± 0.12 |
| Age | 7 – 11 Gyr | |
| Orbital elements Epoch JD 2451409.762[1] |
||
| Semimajor axis | (a) | 0.072993 ± 0.000022[1] AU |
| Eccentricity | (e) | 0[1] |
| Orbital period | (P) | 12.9191 ± 0.0058[1] d (0.03537 y) |
| (310.06 h) | ||
| Mean anomaly | (M) | 33 ± 19[1]° |
| Semi-amplitude | (K) | 3.30 ± 0.19[1] m/s |
| Physical characteristics | ||
| Minimum mass | (m sin i) | 5.6 ± 0.3[1] M⊕ |
| Discovery information | ||
| Discovery date | April 4, 2007 April 24, 2007 (announced) |
|
| Discoverer(s) | Stéphane Udry et al. | |
| Detection method | Radial velocity | |
| Discovery site | La Silla Observatory | |
| Discovery status | Published | |
| Database references | ||
| Extrasolar Planets Encyclopaedia |
data | |
| SIMBAD | data | |
Gliese 581 c ( /ˈɡliːzə/) or Gl 581 c is a planet orbiting the red dwarf star Gliese 581.[2] It is the second planet discovered in the system and the third in order from the star. With a mass at least 5.6 times that of the Earth,[1] it is classified as a super-Earth (a planet of 1 to 10 Earth masses).[3] Assuming that the planet's mass is close to the lower limit determined by radial velocity measurements (the true mass is unknown), it was the smallest known extrasolar planet around a main sequence star, but on April 21, 2009, another planet orbiting Gliese 581, Gliese 581 e, was announced with an approximate mass of 1.9 Earth masses, which is now the smallest known extrasolar planet around a main sequence star.[4]
Gliese 581 c initially generated interest because it was originally reported to be the first potentially Earth-like planet in the habitable zone of its star, with a temperature right for liquid water on its surface, and by extension, potentially capable of supporting extremophile forms of Earth-like life.[2][5] However, further research on the potential effects of the planetary atmosphere casts doubt upon the habitability of Gliese 581 c and indicates that the fourth planet in the system, Gliese 581 g, is a better candidate for habitability.[1] In astronomical terms, the Gliese 581 system is relatively close to Earth, at 20.3 light years (192 trillion km or 119 trillion miles) in the direction of the constellation of Libra.[6][7] This distance, along with the declination and right ascension coordinates, give its exact location in our galaxy. It is identified as Gliese 581 by its number in the Gliese Catalogue of Nearby Stars; it is the 87th closest known star system to the Sun.[8]
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The team released a paper of their findings dated April 27, 2007, published in the July, 2007 journal Astronomy and Astrophysics.[9] In the paper they also announced the discovery of another planet in the system, Gliese 581 d, with a minimum mass of 7.7 Earth masses and a semi-major axis of 0.25 astronomical units. (A reanalysis of the radial velocity data has since reduced the minimum possible mass of Gliese 581 d to 5.6 Earth masses.)[10]
The existence of Gliese 581 c and its mass have been measured by the radial velocity method of detecting extrasolar planets. The mass of a planet is calculated by the small periodic movements around a common centre of mass between the host star Gliese 581 and its planets. When all six planets are fit with a Keplerian solution, the minimum mass of the planet is determined to be 5.6 Earth masses.[1] The radial velocity method cannot by itself determine the true mass, but it cannot be very much larger than this or the system would be dynamically unstable.[9] Dynamical simulations of the Gliese 581 system which assume the orbits of the planets are coplanar indicate that the planets cannot exceed approximately 1.6 – 2 times their minimum masses or the planetary system becomes unstable (this is primarily due to the interaction between planets e and b). For Gliese 581 c, the upper bound is 10.4 Earth masses.[11]
Since Gliese 581 c has not been detected directly, there are no measurements of its radius. Furthermore, the radial velocity method used to detect it only puts a lower limit on the planet's mass, which means theoretical models of planetary radius and structure can only be of limited use. However, assuming a random orientation of the planet's orbit, the true mass is likely to be close to the measured minimum mass.
Assuming that the true mass is the minimum mass, the radius may be calculated using various models. For example, if Gliese 581 c is a rocky planet with a large iron core, it should have a radius approximately 50% larger than that of Earth, according to Udry's team.[9][12] Gravity on such a planet's surface would be approximately 2.24 times as strong as on Earth. However, if Gliese 581 c is an icy and/or watery planet, its radius would be less than 2 times that of Earth, even with a very large outer hydrosphere, according to density models compiled by Diana Valencia and her team for Gliese 876 d.[3] Gravity on the surface of such an icy and/or watery planet would be at least 1.25 times as strong as on Earth. They claim the real value of the radius may be anything between the two extremes calculated by density models outlined above.[13]
Other scientists' views differ. Sara Seager at MIT has speculated that Gliese 581 c and other five-Earth-mass planets could be:[14]
If the planet transits the star as seen from our direction, the radius should be measurable, albeit with some uncertainty. Unfortunately, measurements made with the Canadian-built MOST space telescope indicate that transits do not occur.[15]
For comparison, the smallest confirmed diameter of a planet around a main-sequence star is that of COROT-7b, which is about 70% larger than Earth.
Gliese 581 c has an orbital period ("year") of 13 Earth days[6] and its orbital radius is only about 7% that of the Earth, about 11 million km,[16] while the Earth is 150 million kilometres from the Sun.[17] Since the host star is smaller and colder than the Sun—and thus less luminous—this distance places the planet on the "warm" edge of the habitable zone around the star according to Udry's team.[9][12] Note that in astrophysics, the "habitable zone" is defined as the range of distances from the star at which a planet could support liquid water on its surface: it should not be taken to mean that the planet's environment would be suitable for humans, a situation which requires a more restrictive range of parameters. A typical radius for an M0 star of Gliese 581's age and metallicity is 0.00128 AU,[18] against the sun's 0.00465 AU. This proximity means that the primary star should appear 3.75 times wider and 14 times larger in area for an observer on the planet's surface looking at the sky than the Sun appears to be from Earth's surface.
Because of its small separation from Gliese 581, the planet has been generally considered to always have one hemisphere facing the star (only day), and the other always facing away (only night), or in other words being tidally locked.[19][20] Although a recent orbital fit to the Gliese 581 system uses a circular orbit for Gliese 581 c,[1] older fits use an eccentricity between 0.10 and 0.22. If the orbit of the planet were eccentric, it would undergo violent tidal flexing.[21] Because tidal forces are stronger when the planet is close to the star, eccentric planets are expected to have a rotation period which is shorter than its orbital period, also called pseudo-synchronization.[22] An example of this effect is seen in Mercury, which is tidally locked in a 3:2 resonance, completing three rotations every two orbits. In any case, even in the case of 1:1 tidal lock, the planet would undergo libration and the terminator would be alternatively lit and darkened during libration.[23]
Models of the evolution of the planet's orbit over time suggest that heating resulting from this tidal locking may play a major role in the planet's geology. Models proposed by scientists predict that tidal heating could yield a surface heat flux about three times greater than the Jupiter's moon Io's, which could result in major geological activity such as volcanoes and plate tectonics.[24]
The study of Gliese 581 c by the von Bloh et al. team has been quoted as concluding "The super-Earth Gl 581c is clearly outside the habitable zone, since it is too close to the star."[25] The study by Selsis et al. claims even "a planet in the habitable zone is not necessarily habitable" itself, and this planet "is outside what can be considered the conservative habitable zone" of the parent star, and further that if there was any water there then it was lost when the red dwarf was a strong X-ray and EUV emitter, it could have surface temperatures ranging from 700 K to 1000 K (430 to 730 °C), like Venus today.[26] Temperature speculations by other scientists were based on the temperature of (and heat from) the parent star Gliese 581 and have been calculated without factoring in the margin of error (96 °C/K) for the star's temperature of 3432 K to 3528 K, which leads to a large irradiance range for the planet, even before eccentricity is considered.[27]
Using the measured stellar luminosity of Gliese 581 of 0.013 times that of our Sun, it is possible to calculate Gliese 581 c's effective temperature a.k.a. black body temperature. (note: this probably differs from its surface temperature). According to Udry's team, the effective temperature for Gliese 581 c, assuming an albedo (reflectivity) such as Venus' (0.64), would be −3 °C (27 °F), and assuming an Earth-like albedo (0.296), then it would be 40 °C (104 °F),[6][9] a range of temperatures which overlaps with the range that water would be liquid at a pressure of 1 atmosphere. However, the effective temperature and actual surface temperature can be very different due to the greenhouse properties of the planetary atmosphere: for example, Venus has an effective temperature of 34.25 °C (307.40 K; 93.65 °F), but a surface temperature of 463.85 °C (737.00 K; 866.93 °F) (mainly due to a 96.5% carbon dioxide atmosphere), a difference of about 430 °C (770 °F).[28] Studies of the habitability (i.e. liquid water for extremophile forms of life)[29] conclude that Gliese 581 c is likely to suffer from a runaway greenhouse effect similar to that found on Venus, as such, is highly unlikely to be habitable. Nevertheless, this runaway greenhouse effect could be prevented by the presence of sufficient reflective cloud cover on the planet's day side.[30] Alternatively, if the surface were covered in ice, it would have a high albedo (reflectivity), and thus could reflect enough of the incident sunlight back into space to render the planet too cold for habitability, although this situation is expected to be very unstable except for very high albedos greater than about 0.95 (i.e. ice): release of carbon dioxide by volcanic activity or of water vapor due to heating at the substellar point would trigger a runaway greenhouse effect.[31]
Gliese 581 c is likely to lie outside the habitable zone.[25][32] No direct evidence has been found for water to be present, and it is probably not present in the liquid state. Techniques like the one used to measure the extrasolar planet HD 209458 b may in the future be used to determine the presence of water in the form of vapor in the planet's atmosphere, but only in the rare case of a planet with an orbit aligned so as to transit its star, which Gliese 581 c is not known to do.
Theoretical models predict that volatile compounds such as water and carbon dioxide, if present, might evaporate in the scorching heat of the sunward side, migrate to the cooler night side, and condense to form ice caps. Over time, the entire atmosphere might freeze into ice caps on the night side of the planet. However, it remains unknown if water and/or carbon dioxide are even present on the surface of Gliese 581c. Alternatively, an atmosphere large enough to be stable would circulate the heat more evenly, allowing for a wider habitable area on the surface.[33] For example, although Venus has a small axial inclination, very little sunlight reaches the surface at the poles. A slow rotation rate approximately 117 times slower than Earth's produces prolonged days and nights. Despite the uneven distribution of sunlight cast on Venus at any given time, polar areas and the night side of Venus are kept almost as hot as on the day side by globally circulating winds.[34]
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Coordinates: 15h 19m 26s, −07° 43′ 20″