List of gravitationally rounded objects of the Solar System explained
This is a list of most likely gravitationally rounded objects (GRO) of the Solar System, which are objects that have a rounded, ellipsoidal shape due to their own gravity (but are not necessarily in hydrostatic equilibrium). Apart from the Sun itself, these objects qualify as planets according to common geophysical definitions of that term. The radii of these objects range over three orders of magnitude, from planetary-mass objects like dwarf planets and some moons to the planets and the Sun. This list does not include small Solar System bodies, but it does include a sample of possible planetary-mass objects whose shapes have yet to be determined. The Sun's orbital characteristics are listed in relation to the Galactic Center, while all other objects are listed in order of their distance from the Sun.
Star
See main article: Sun.
The Sun is a G-type main-sequence star. It contains almost 99.9% of all the mass in the Solar System.[1]
| Sun[2] [3] |
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| |
Symbol (image) | |
Symbol (Unicode) | ☉ |
Discovery year | Prehistoric |
Mean distance from the Galactic Center | km light years | ≈ 2.5 ≈ 26,000 |
Mean radius | km :E | 695,508 109.3 |
Surface area | km2 :E | 6.0877 11,990 |
Volume | km3 :E | 1.4122 1,300,000 |
Mass | kg :E | 1.9855 332,978.9 |
Gravitational parameter | m3/s2 | 1.327×1020 |
Density | g/cm3 | 1.409 |
Equatorial gravity | m/s2 g | 274.0 27.94 |
Escape velocity | km/s | 617.7 |
Rotation period | days | 25.38 |
Orbital period about Galactic Center[4] | million years | 225–250 |
Mean orbital speed | km/s | ≈ 220 |
Axial tilt to the ecliptic | deg. | 7.25 |
Axial tilt to the galactic plane | deg. | 67.23 |
Mean surface temperature | K | 5,778 |
Mean coronal temperature[5] | K | 1–2 |
Photospheric composition | H, He, O, C, Fe, S | |
Planets
See main article: Planet.
In 2006, the International Astronomical Union (IAU) defined a planet as a body in orbit around the Sun that was large enough to have achieved hydrostatic equilibrium and to have "cleared the neighbourhood around its orbit".[6] The practical meaning of "cleared the neighborhood" is that a planet is comparatively massive enough for its gravitation to control the orbits of all objects in its vicinity. In practice, the term "hydrostatic equilibrium" is interpreted loosely. Mercury is round but not actually in hydrostatic equilibrium, but it is universally regarded as a planet nonetheless.[7]
According to the IAU's explicit count, there are eight planets in the Solar System; four terrestrial planets (Mercury, Venus, Earth, and Mars) and four giant planets, which can be divided further into two gas giants (Jupiter and Saturn) and two ice giants (Uranus and Neptune). When excluding the Sun, the four giant planets account for more than 99% of the mass of the Solar System.
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|
|
|
| °Jupiter[17] [18] | °Saturn[19] [20] | ×Uranus[21] [22] | ×Neptune[23] [24] |
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| | | | | | | |
Symbol | | | | | | | or | |
Symbol (Unicode) | ☿ | ♀ | | ♂ | ♃ | ♄ | ⛢ or ♅ | ♆ |
Discovery year | Prehistoric | Prehistoric | Prehistoric | Prehistoric | Prehistoric | Prehistoric | 1781 | 1846 |
Mean distance from the Sun | km AU | 57,909,175 0.38709893 | 108,208,930 0.72333199 | 149,597,890 1.00000011 | 227,936,640 1.52366231 | 778,412,010 5.20336301 | 1,426,725,400 9.53707032 | 2,870,972,200 19.19126393 | 4,498,252,900 30.06896348 |
Equatorial radius | km :E | 2,440.53 0.3826 | 6,051.8 0.9488 | 6,378.1366 1 | 3,396.19 0.53247 | 71,492 11.209 | 60,268 9.449 | 25,559 4.007 | 24,764 3.883 |
Surface area | km2 :E | 75,000,000 0.1471 | 460,000,000 0.9020 | 510,000,000 1 | 140,000,000 0.2745 | 64,000,000,000 125.5 | 44,000,000,000 86.27 | 8,100,000,000 15.88 | 7,700,000,000 15.10 |
Volume | km3 :E | 6.083 0.056 | 9.28 0.857 | 1.083 1 | 1.6318 0.151 | 1.431 1,321.3 | 8.27 763.62 | 6.834 63.102 | 6.254 57.747 |
Mass | kg :E | 3.302 0.055 | 4.8690 0.815 | 5.972 1 | 6.4191 0.107 | 1.8987 318 | 5.6851 95 | 8.6849 14.5 | 1.0244 17 |
Gravitational parameter | m3/s2 | 2.203×1013 | 3.249×1014 | 3.986×1014 | 4.283×1013 | 1.267×1017 | 3.793×1016 | 5.794×1015 | 6.837×1015 |
Density | g/cm3 | 5.43 | 5.24 | 5.52 | 3.940 | 1.33 | 0.70 | 1.30 | 1.76 |
Equatorial gravity | m/s2 g | 3.70 0.377 | 8.87 0.904 | 9.8 1.00 | 3.71 0.378 | 24.79 2.528 | 10.44 1.065 | 8.87 0.904 | 11.15 1.137 |
Escape velocity | km/s | 4.25 | 10.36 | 11.18 | 5.02 | 59.54 | 35.49 | 21.29 | 23.71 |
Rotation period | days | 58.646225 | 243.0187 | 0.99726968 | 1.02595675 | 0.41354 | 0.44401 | 0.71833 | 0.67125 |
Orbital period | days years | 87.969 0.2408467 | 224.701 0.61519726 | 365.256363 1.0000174 | 686.971 1.8808476 | 4,332.59 11.862615 | 10,759.22 29.447498 | 30,688.5 84.016846 | 60,182 164.79132 |
Mean orbital speed | km/s | 47.8725 | 35.0214 | 29.7859 | 24.1309 | 13.0697 | 9.6724 | 6.8352 | 5.4778 |
Eccentricity | 0.20563069 | 0.00677323 | 0.01671022 | 0.09341233 | 0.04839266 | 0.05415060 | 0.04716771 | 0.00858587 |
Inclination | deg. | 7.00 | 3.39 | 0 | 1.85 | 1.31 | 2.48 | 0.76 | 1.77 |
Axial tilt | deg. | 0.0 | 177.3 | 23.44 | 25.19 | 3.12 | 26.73 | 97.86 | 28.32 |
Mean surface temperature | K | 440–100 | 730 | 287 | 227 | 152 | 134 | 76 | 73 |
Mean air temperature | K | | | 288 | | 165 | 135 | 76 | 73 |
Atmospheric composition | He, Na+ K+ | CO2, N2, SO2 | N2, O2, Ar, CO2 | CO2, N2 Ar | H2, He | H2, He | H2, He CH4 | H2, He CH4 |
Number of known moons | 0 | 0 | 1 | 2 | 95 | 146 | 28 | 16 |
Rings? | No | No | No | No | Yes | Yes | Yes | Yes |
Planetary discriminant | 9.1 | 1.35 | 1.7 | 1.8 | 6.25 | 1.9 | 2.9 | 2.4 | |
Dwarf planets
See main article: Dwarf planet.
See also: List of possible dwarf planets.
Dwarf planets are bodies orbiting the Sun that are massive and warm enough to have achieved hydrostatic equilibrium, but have not cleared their neighbourhoods of similar objects. Since 2008, there have been five dwarf planets recognized by the IAU, although only Pluto has actually been confirmed to be in hydrostatic equilibrium[25] (Ceres is close to equilibrium, though some anomalies remain unexplained).[26] Ceres orbits in the asteroid belt, between Mars and Jupiter. The others all orbit beyond Neptune.
| †[27] | ‡[28] [29] | ‡[30] [31] [32] | ‡[33] [34] | §[35] |
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| | | | | |
Symbol | | or | | | |
Symbol (Unicode) | ⚳ | ♇ or ⯓ | | | ⯰ |
Minor planet number | 1 | 134340 | 136108 | 136472 | 136199 |
Discovery year | 1801 | 1930 | 2004 | 2005 | 2005 |
Mean distance from the Sun | km AU | 413,700,000 2.766 | 5,906,380,000 39.482 | 6,484,000,000 43.335 | 6,850,000,000 45.792 | 10,210,000,000 67.668 |
Mean radius | km :E | 473 0.0742 | 1,188.3 0.186 | 816 0.13[36] [37] | 715 0.11[38] | 1,163 0.18[39] |
Volume | km3 :E | 4.21 0.00039 | 6.99 0.0065 | 1.98 0.0018 | 1.7 0.0016 | 6.59 0.0061 |
Surface area | km2 :E | 2,770,000 0.0054 | 17,700,000 0.035 | 8,140,000 0.016 | 6,900,000 0.0135 | 17,000,000 0.0333 |
Mass | kg :E | 9.39 0.00016 | 1.30 0.0022 | 4.01 ± 0.04 0.0007[40] | ≈ 3.1 0.0005 | 1.65 0.0028 |
Gravitational parameter | m3/s2 | 6.263 × 1010 | 8.710 × 1011 | 2.674 × 1011 | 2.069 × 1011 | 1.108 × 1012 |
Density | g/cm3 | 2.16 | 1.87 | 2.02 | 2.03 | 2.43 |
Equatorial gravity | m/s2 g | 0.27 0.028 | 0.62 0.063 | 0.63 0.064 | 0.40 0.041 | 0.82 0.084 |
Escape velocity | km/s | 0.51 | 1.21 | 0.91 | 0.54 | 1.37 |
Rotation period | days | 0.3781 | 6.3872 | 0.1631 | 0.9511 | 15.7859 |
Orbital period | years | 4.599 | 247.9 | 283.8 | 306.2 | 559 |
Mean orbital speed | km/s | 17.882 | 4.75 | 4.48 | 4.40 | 3.44 |
Eccentricity | 0.080 | 0.249 | 0.195 | 0.161 | 0.436 |
Inclination | deg. | 10.59 | 17.14 | 28.21 | 28.98 | 44.04 |
Axial tilt | deg. | 4 | 119.6 | ≈ 126 | ? | ≈ 78 |
Mean surface temperature | K | 167[41] | 40[42] | <50[43] | 30 | 30 |
Atmospheric composition | H2O | N2, CH4, CO | ? | N2, CH4[44] | N2, CH4[45] |
Number of known moons | 0 | 5 | 2[46] | 1[47] | 1[48] |
Rings? | No | No | Yes | ? | ? |
Planetary discriminant | 0.33 | 0.077 | 0.023 | 0.02 | 0.10 | |
Astronomers usually refer to solid bodies such as Ceres as dwarf planets, even if they are not strictly in hydrostatic equilibrium. They generally agree that several other trans-Neptunian objects (TNOs) may be large enough to be dwarf planets, given current uncertainties. However, there has been disagreement on the required size. Early speculations were based on the small moons of the giant planets, which attain roundness around a threshold of 200 km radius.[49] However, these moons are at higher temperatures than TNOs and are icier than TNOs are likely to be. Estimates from an IAU question-and-answer press release from 2006, giving 800 km radius and mass as cut-offs that normally would be enough for hydrostatic equilibrium, while stating that observation would be needed to determine the status of borderline cases.[50] Many TNOs in the 200–500 km radius range are dark and low-density bodies, which suggests that they retain internal porosity from their formation, and hence are not planetary bodies (as planetary bodies have sufficient gravitation to collapse out such porosity).
In 2023, Emery et al. wrote that near-infrared spectroscopy by the James Webb Space Telescope (JWST) in 2022 suggests that Sedna, Gonggong, and Quaoar underwent internal melting, differentiation, and chemical evolution, like the larger dwarf planets Pluto, Eris, Haumea, and Makemake, but unlike "all smaller KBOs". This is because light hydrocarbons are present on their surfaces (e.g. ethane, acetylene, and ethylene), which implies that methane is continuously being resupplied, and that methane would likely come from internal geochemistry. On the other hand, the surfaces of Sedna, Gonggong, and Quaoar have low abundances of CO and CO2, similar to Pluto, Eris, and Makemake, but in contrast to smaller bodies. This suggests that the threshold for dwarf planethood in the trans-Neptunian region is around 500 km radius.[51]
In 2024, Kiss et al. found that Quaoar has an ellipsoidal shape incompatible with hydrostatic equilibrium for its current spin. They hypothesised that Quaoar originally had a rapid rotation and was in hydrostatic equilibrium, but that its shape became "frozen in" and did not change as it spun down due to tidal forces from its moon Weywot.[52] If so, this would resemble the situation of Saturn's moon Iapetus, which is too oblate for its current spin.[53] [54] Iapetus is generally still considered a planetary-mass moon nonetheless, though not always.[55]
The table below gives Orcus, Quaoar, Gonggong, and Sedna as additional consensus dwarf planets; slightly smaller Salacia, which is larger than 400 km radius, has been included as a borderline case for comparison, (and is therefore italicized).
| ‡Orcus[56] | ‡Salacia[57] | ‡Quaoar[58] | §Gonggong[59] | ×Sedna[60] |
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| | | | | |
Symbol | | | | | |
Symbol (Unicode) | | | | | ⯲ |
Minor-planet number | 90482 | 120347 | 50000 | 225088 | 90377 |
Discovery year | 2004 | 2004 | 2002 | 2007 | 2003 |
Semi-major axis | km AU | 5,896,946,000 39.419 | 6,310,600,000 42.18 | 6,535,930,000 43.69 | 10,072,433,340 67.33 | 78,668,000,000 525.86 |
Mean radius | km :E | 458.5[61] 0.0720 | 423[62] 0.0664 | 555[63] 0.0871 | 615 0.0982 | 497.5[64] 0.0780 |
Surface area | km2 :E | 2,641,700 0.005179 | 2,248,500 0.004408 | 3,870,800 0.007589 | 4,932,300 0.009671 | 3,110,200 0.006098 |
Volume | km3 :E | 403,744,500 0.000373 | 317,036,800 0.000396 | 716,089,900 0.000661 | 1,030,034,600 0.000951 | 515,784,000 0.000476 |
Mass | kg :E | 5.48< | --mass of Orcus' system minus mass of Vanth-->[65] 0.0001 | 4.9 0.0001 | 1.20 0.0002 | 1.75 0.0003 | ? |
---|
Density | g/cm3 | | | ≈ | | ? |
Equatorial gravity | m/s2 g | 0.017 | 0.018 | 0.025 | 0.029 | ? |
Escape velocity | km/s | | | | | ? |
Rotation period | days | 9.54? | ? | 0.7367[66] | 0.9333 | 0.4280[67] |
Orbital period | years | 247.49 | 273.98 | 287.97 | 552.52 | 12,059 |
Mean orbital speed | km/s | 4.68 | 4.57 | 4.52 | 3.63 | 1.04 |
Eccentricity | 0.226 | 0.106 | 0.038 | 0.506 | 0.855 |
Inclination | deg. | 20.59 | 23.92 | 7.99 | 30.74 | 11.93 |
Axial tilt | deg. | ? | ? | 13.6[68] or 14.0[69] | ? | ? |
Mean surface temperature | K | ≈ 42 | ≈ 43 | ≈ 41 | ≈ 30 | ≈ 12 |
Number of known moons | 1[70] | 1 | 1[71] | 1 | 0 |
Rings? | ? | ? | Yes | ? | ? |
Planetary discriminant | 0.003 | <0.1 | 0.0015 | <0.1 | ? |
Absolute magnitude (H) | 2.3 | 4.1 | 2.71 | 1.8 | 1.5 | |
As for objects in the asteroid belt, none are generally agreed as dwarf planets today among astronomers other than Ceres. The second- through fifth-largest asteroids have been discussed as candidates. Vesta (radius), the second-largest asteroid, appears to have a differentiated interior and therefore likely was once a dwarf planet, but it is no longer very round today.[72] Pallas (radius), the third-largest asteroid, appears never to have completed differentiation and likewise has an irregular shape. Vesta and Pallas are nonetheless sometimes considered small terrestrial planets anyway by sources preferring a geophysical definition, because they do share similarities to the rocky planets of the inner solar system.[73] The fourth-largest asteroid, Hygiea (radius), is icy. The question remains open if it is currently in hydrostatic equilibrium: while Hygiea is round today, it was probably previously catastrophically disrupted and today might be just a gravitational aggregate of the pieces.[74] The fifth-largest asteroid, Interamnia (radius), is icy and has a shape consistent with hydrostatic equilibrium for a slightly shorter rotation period than it now has.[75]
Satellites
See main article: Planetary-mass moon.
There are at least 19 natural satellites in the Solar System that are known to be massive enough to be close to hydrostatic equilibrium: seven of Saturn, five of Uranus, four of Jupiter, and one each of Earth, Neptune, and Pluto. Alan Stern calls these satellite planets, although the term major moon is more common. The smallest natural satellite that is gravitationally rounded is Saturn I Mimas (radius). This is smaller than the largest natural satellite that is known not to be gravitationally rounded, Neptune VIII Proteus (radius).
Several of these were once in equilibrium but are no longer: these include Earth's moon[76] and all of the moons listed for Saturn apart from Titan and Rhea.[54] The status of Callisto, Titan, and Rhea is uncertain, as is that of the moons of Uranus, Pluto[25] and Eris.[77] The other large moons (Io, Europa, Ganymede, and Triton) are generally believed to still be in equilibrium today. Other moons that were once in equilibrium but are no longer very round, such as Saturn IX Phoebe (radius), are not included. In addition to not being in equilibrium, Mimas and Tethys have very low densities and it has been suggested that they may have non-negligible internal porosity,[78] [79] in which case they would not be satellite planets.
The moons of the trans-Neptunian objects (other than Charon) have not been included, because they appear to follow the normal situation for TNOs rather than the moons of Saturn and Uranus, and become solid at a larger size (900–1000 km diameter, rather than 400 km as for the moons of Saturn and Uranus). Eris I Dysnomia and Orcus I Vanth, though larger than Mimas, are dark bodies in the size range that should allow for internal porosity, and in the case of Dysnomia a low density is known.
Satellites are listed first in order from the Sun, and second in order from their parent body. For the round moons, this mostly matches the Roman numeral designations, with the exceptions of Iapetus and the Uranian system. This is because the Roman numeral designations originally reflected distance from the parent planet and were updated for each new discovery until 1851, but by 1892, the numbering system for the then-known satellites had become "frozen" and from then on followed order of discovery. Thus Miranda (discovered 1948) is Uranus V despite being the innermost of Uranus' five round satellites. The missing Saturn VII is Hyperion, which is not large enough to be round (mean radius).
| Moon[80] | ♃Io[81] | ♃Europa[82] | ♃Ganymede[83] | ♃Callisto[84] | ♄Mimas | ♄Enceladus | ♄Tethys | ♄Dione | ♄Rhea |
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| | | | | | | | | | |
Roman numeral designation | Earth I | Jupiter I | Jupiter II | Jupiter III | Jupiter IV | Saturn I | Saturn II | Saturn III | Saturn IV | Saturn V |
Symbol | | JI | JII | JIII | JIV | SI | SII | SIII | SIV | SV |
Symbol (Unicode) | ☾ | | | | | | | | | |
Discovery year | Prehistoric | 1610 | 1610 | 1610 | 1610 | 1789 | 1789 | 1684 | 1684 | 1672 |
Mean distance from primary | km | 384,399 | 421,600 | 670,900 | 1,070,400 | 1,882,700 | 185,520 | 237,948 | 294,619 | 377,396 | 527,108 |
Mean radius | km :E | 1,737.1 0.272 | 1,815 0.285 | 1,569 0.246 | 2,634.1 0.413 | 2,410.3 0.378 | 198.30 0.031 | 252.1 0.04 | 533 0.084 | 561.7 0.088 | 764.3 0.12 |
Surface area | 1 km2 | 37.93 | 41.910 | 30.9 | 87.0 | 73 | 0.49 | 0.799 | 3.57 | 3.965 | 7.337 |
Volume | 1 km3 | 22 | 25.3 | 15.9 | 76 | 59 | 0.033 | 0.067 | 0.63 | 0.8 | 1.9 |
Mass | 1 kg | 7.3477 | 8.94 | 4.80 | 14.819 | 10.758 | 0.00375 | 0.0108 | 0.06174 | 0.1095 | 0.2306 |
Density | g/cm3 | 3.3464 | 3.528 | 3.01 | 1.936 | 1.83 | 1.15 | 1.61 | 0.98 | 1.48 | 1.23 |
Equatorial gravity | m/s2 g | 1.622 0.1654 | 1.796 0.1831 | 1.314 0.1340 | 1.428 0.1456 | 1.235 0.1259 | 0.0636 0.00649 | 0.111 0.0113 | 0.145 0.0148 | 0.231 0.0236 | 0.264 0.0269 |
Escape velocity | km/s | 2.38 | 2.56 | 2.025 | 2.741 | 2.440 | 0.159 | 0.239 | 0.393 | 0.510 | 0.635 |
Rotation period | days | 27.321582 (sync) | 1.7691378 (sync) | 3.551181 (sync) | 7.154553 (sync) | 16.68902 (sync) | 0.942422 (sync) | 1.370218 (sync) | 1.887802 (sync) | 2.736915 (sync) | 4.518212 (sync) |
Orbital period about primary | days | 27.32158 | 1.769138 | 3.551181 | 7.154553 | 16.68902 | 0.942422 | 1.370218 | 1.887802 | 2.736915 | 4.518212 |
Mean orbital speed | km/s | 1.022 | 17.34 | 13.740 | 10.880 | 8.204 | 14.32 | 12.63 | 11.35 | 10.03 | 8.48 |
Eccentricity | 0.0549 | 0.0041 | 0.009 | 0.0013 | 0.0074 | 0.0202 | 0.0047 | 0.02 | 0.002 | 0.001 |
Inclination to primary's equator | deg. | 18.29–28.58 | 0.04 | 0.47 | 1.85 | 0.2 | 1.51 | 0.02 | 1.51 | 0.019 | 0.345 |
Axial tilt | deg. | 6.68 | 0.000405 ± 0.00076 | 0.0965 ± 0.0069 | 0.155 ± 0.065[85] | ≈ 0–2 | ≈ 0 | ≈ 0 | ≈ 0 | ≈ 0 | ≈ 0 |
Mean surface temperature | K | 220 | 130 | 102 | 110[86] | 134 | 64 | 75 | 64 | 87 | 76 |
Atmospheric composition | Ar, He Na, K, H | SO2[87] | O2[88] | O2[89] | O2, CO2[90] | | H2O, N2 CO2, CH4[91] | | | | |
| ♄Titan | ♄Iapetus | ⛢Miranda | ⛢Ariel | ⛢Umbriel | ⛢Titania | ⛢Oberon | ♆Triton[92] | ♇Charon |
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| | | | | | | | | |
Roman numeral designation | Saturn VI | Saturn VIII< | --NOT A TYPO; Saturn VII (7) IS HYPERION, WHICH IS NOT ROUND--> | Uranus V< | --ALSO NOT A TYPO: Miranda was discovered well after the other four--> | Uranus I | Uranus II | Uranus III | Uranus IV | Neptune I | Pluto I |
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Symbol | SVI | SVIII | UV | UI | UII | UIII | UIV | NI | PI |
Discovery year | 1655 | 1671 | 1948 | 1851 | 1851 | 1787 | 1787 | 1846 | 1978 |
Mean distance from primary | km | 1,221,870 | 3,560,820 | 129,390 | 190,900 | 266,000 | 436,300 | 583,519 | 354,759 | 17,536 |
Mean radius | km :E | 2,576 0.404 | 735.60 0.115 | 235.8 0.037 | 578.9 0.091 | 584.7 0.092 | 788.9 0.124 | 761.4 0.119 | 1,353.4 0.212 | 603.5 0.095 |
Surface area | 1 km2 | 83.0 | 6.7 | 0.70 | 4.211 | 4.296 | 7.82 | 7.285 | 23.018 | 4.580 |
Volume | 1 km3 | 71.6 | 1.67 | 0.055 | 0.81 | 0.84 | 2.06 | 1.85 | 10 | 0.92 |
Mass | 1 kg | 13.452 | 0.18053 | 0.00659 | 0.135 | 0.12 | 0.35 | 0.3014 | 2.14 | 0.152 |
Density | g/cm3 | 1.88 | 1.08 | 1.20 | 1.67 | 1.40 | 1.72 | 1.63 | 2.061 | 1.65 |
Equatorial gravity | m/s2 g | 1.35 0.138 | 0.22 0.022 | 0.08 0.008 | 0.27 0.028 | 0.23 0.023 | 0.39 0.040 | 0.35 0.036 | 0.78 0.080 | 0.28 0.029 |
Escape velocity | km/s | 2.64 | 0.57 | 0.19 | 0.56 | 0.52 | 0.77 | 0.73 | 1.46 | 0.58 |
Rotation period | days | 15.945 (sync) | 79.322 (sync) | 1.414 (sync) | 2.52 (sync) | 4.144 (sync) | 8.706 (sync) | 13.46 (sync) | 5.877 (sync) | 6.387 (sync) |
Orbital period about primary | days | 15.945 | 79.322 | 1.4135 | 2.520 | 4.144 | 8.706 | 13.46 | 5.877 | 6.387 |
Mean orbital speed | km/s | 5.57 | 3.265 | 6.657 | 5.50898 | 4.66797 | 3.644 | 3.152 | 4.39 | 0.2 |
Eccentricity | 0.0288 | 0.0286 | 0.0013 | 0.0012 | 0.005 | 0.0011 | 0.0014 | 0.00002 | 0.0022 |
Inclination to primary's equator | deg. | 0.33 | 14.72 | 4.22 | 0.31 | 0.36 | 0.14 | 0.10 | 157 | 0.001 |
Axial tilt | deg. | ≈ 0.3[93] | ≈ 0 | ≈ 0 | ≈ 0 | ≈ 0 | ≈ 0 | ≈ 0 | ≈ 0.7[94] | ≈ 0 |
Mean surface temperature | K | 93.7[95] | 130 | 59 | 58 | 61 | 60 | 61 | 38[96] | 53 |
Atmospheric composition | N2, CH4[97] | | | | | | | N2, CH4[98] | | |
See also
Notes
Other notes
Notes and References
- Michael Mark . Woolfson . Michael Woolfson . The Origin and Evolution of the Solar System . 10.1046/j.1468-4004.2000.00012.x . 2000 . Astronomy & Geophysics . 41 . 1 . 1.12–1.19 . 2000A&G....41a..12W . free.
- http://solarsystem.nasa.gov/planets/profile.cfm?Object=Sun&Display=Facts&System=Metric NASA Solar System exploration Sun factsheet
- Web site: By the Numbers Sun - NASA Solar System Exploration. NASA. 16 June 2021. 23 May 2019. https://web.archive.org/web/20190523230455/https://solarsystem.nasa.gov/solar-system/sun/by-the-numbers/. live.
- Web site: Period of the Sun's Orbit around the Galaxy (Cosmic Year) . The Physics Factbook (self-published) . Stacy . Leong . Glenn . Elert . 2002 . 2008-06-26 . 7 January 2019 . https://web.archive.org/web/20190107010909/https://hypertextbook.com/facts/2002/StacyLeong.shtml . live .
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