fbpx
Wikipedia

Mercury (planet)

Mercury is the smallest planet in the Solar System and the closest to the Sun. Its orbit around the Sun takes 87.97 Earth days, the shortest of all the Sun's planets. It is named after the Roman god Mercurius (Mercury), god of commerce, messenger of the gods, and mediator between gods and mortals, corresponding to the Greek god Hermes (Ἑρμῆς). Like Venus, Mercury orbits the Sun within Earth's orbit as an inferior planet; its apparent distance from the Sun as viewed from Earth never exceeds 28°. This proximity to the Sun means the planet can only be seen near the western horizon after sunset or the eastern horizon before sunrise, usually in twilight. At this time, it may appear as a bright star-like object, but is more difficult to observe than Venus. From Earth, the planet telescopically displays the complete range of phases, similar to Venus and the Moon, which recurs over its synodic period of approximately 116 days. Due to its synodic proximity to Earth, Mercury is most often the closest planet to Earth, with Venus periodically taking this role.[18][19]

Mercury
Mercury in true color (by MESSENGER in 2008)
Designations
Pronunciation/ˈmɜːrkjʊri/ (listen)
AdjectivesMercurian /mərˈkjʊəriən/,[1]
Mercurial /mərˈkjʊəriəl/[2]
Orbital characteristics[5]
Epoch J2000
Aphelion
  • 0.466697 AU
  • 69,816,900 km
Perihelion
  • 0.307499 AU
  • 46,001,200 km
  • 0.387098 AU
  • 57,909,050 km
Eccentricity0.205630[3]
115.88 d[3]
47.36 km/s[3]
174.796°
Inclination
48.331°
29.124°
SatellitesNone
Physical characteristics
Mean diameter
4880 km
Mean radius
  • 2,439.7±1.0 km[6][7]
  • 0.3829 Earths
Flattening0.0009[3]
  • 7.48×107 km2[6]
  • 0.147 Earths
Volume
  • 6.083×1010 km3[6]
  • 0.056 Earths
Mass
  • 3.3011×1023 kg[8]
  • 0.055 Earths
Mean density
5.427 g/cm3[6]
0.346±0.014[9]
4.25 km/s[6]
176 d[10]
  • 58.646 d
  • 1407.5 h[6]
Equatorial rotation velocity
10.892 km/h (3.026 m/s)
2.04 ± 0.08 (to orbit)[9]
(0.034°)[3]
North pole right ascension
  • 18h 44m 2s
  • 281.01°[3]
North pole declination
61.45°[3]
Albedo
Temperature437 K (164 °C) (blackbody temperature)[13]
Surface temp. min mean max
0°N, 0°W [14] -173 °C 67 °C 427 °C
85°N, 0°W[14] -193 °C -73 °C 106.85 °C
−2.48 to +7.25[15]
4.5–13″[3]
Atmosphere[3][16][17]
Surface pressure
trace (≲ 0.5 nPa)
Composition by volume

Mercury rotates in a way that is unique in the Solar System. It is tidally locked with the Sun in a 3:2 spin–orbit resonance,[20] meaning that relative to the fixed stars, it rotates on its axis exactly three times for every two revolutions it makes around the Sun.[a][21] As seen from the Sun, in a frame of reference that rotates with the orbital motion, it appears to rotate only once every two Mercurian years. An observer on Mercury would therefore see only one day every two Mercurian years.

Mercury's axis has the smallest tilt of any of the Solar System's planets (about 130 degree). Its orbital eccentricity is the largest of all known planets in the Solar System;[b] at perihelion, Mercury's distance from the Sun is only about two-thirds (or 66%) of its distance at aphelion. Mercury's surface appears heavily cratered and is similar in appearance to the Moon's, indicating that it has been geologically inactive for billions of years. Having almost no atmosphere to retain heat, it has surface temperatures that vary diurnally more than on any other planet in the Solar System, ranging from 100 K (−173 °C; −280 °F) at night to 700 K (427 °C; 800 °F) during the day across the equatorial regions.[22] The polar regions are constantly below 180 K (−93 °C; −136 °F). The planet has no natural satellites.

Two spacecraft have visited Mercury: Mariner 10 flew by in 1974 and 1975; and MESSENGER, launched in 2004, orbited Mercury over 4,000 times in four years before exhausting its fuel and crashing into the planet's surface on April 30, 2015.[23][24][25] The BepiColombo spacecraft is planned to arrive at Mercury in 2025.

Nomenclature

The ancients knew Mercury by different names depending on whether it was an evening star or a morning star. By about 350 BC, the ancient Greeks had realized the two stars were one.[26] They knew the planet as Στίλβων Stilbōn, meaning "twinkling", and Ἑρμής Hermēs, for its fleeting motion,[27] a name that is retained in modern Greek (Ερμής Ermis).[28] The Romans named the planet after the swift-footed Roman messenger god, Mercury (Latin Mercurius), which they equated with the Greek Hermes, because it moves across the sky faster than any other planet.[26][29] The astronomical symbol for Mercury is a stylized version of Hermes' caduceus; a Christian cross was added in the 16th century:  .[30][31]

Physical characteristics

Mercury is one of four terrestrial planets in the Solar System, and is a rocky body like Earth. It is the smallest planet in the Solar System, with an equatorial radius of 2,439.7 kilometres (1,516.0 mi).[3] Mercury is also smaller—albeit more massive—than the largest natural satellites in the Solar System, Ganymede and Titan. Mercury consists of approximately 70% metallic and 30% silicate material.[32]

Internal structure

 
Mercury's internal structure and magnetic field

Mercury appears to have a solid silicate crust and mantle overlying a solid, iron sulfide outer core layer, a deeper liquid core layer, and a solid inner core.[33][34] The planet's density is the second highest in the Solar System at 5.427 g/cm3, only slightly less than Earth's density of 5.515 g/cm3.[3] If the effect of gravitational compression were to be factored out from both planets, the materials of which Mercury is made would be denser than those of Earth, with an uncompressed density of 5.3 g/cm3 versus Earth's 4.4 g/cm3.[35] Mercury's density can be used to infer details of its inner structure. Although Earth's high density results appreciably from gravitational compression, particularly at the core, Mercury is much smaller and its inner regions are not as compressed. Therefore, for it to have such a high density, its core must be large and rich in iron.[36]

The radius of Mercury's core is estimated to be 2,020 ± 30 km (1,255 ± 19 mi), based on interior models constrained to be consistent with the value of the moment of inertia factor given in the infobox.[9][37] Hence, Mercury's core occupies about 57% of its volume; for Earth this proportion is 17%. Research published in 2007 suggests that Mercury has a molten core.[38][39] Surrounding the core is a 500–700 km (310–430 mi) mantle consisting of silicates.[40][41] Based on data from the Mariner 10 and MESSENGER missions, in addition to Earth-based observation, Mercury's crust is estimated to be 35 km (22 mi) thick.[42][43] However, this model may be an overestimate and the crust could be 26 ± 11 km (16.2 ± 6.8 mi) thick based on an Airy isostacy model.[44] One distinctive feature of Mercury's surface is the presence of numerous narrow ridges, extending up to several hundred kilometers in length. It is thought that these were formed as Mercury's core and mantle cooled and contracted at a time when the crust had already solidified.[45][46][47]

Mercury's core has a higher iron content than that of any other major planet in the Solar System, and several theories have been proposed to explain this. The most widely accepted theory is that Mercury originally had a metal–silicate ratio similar to common chondrite meteorites, thought to be typical of the Solar System's rocky matter, and a mass approximately 2.25 times its current mass.[48] Early in the Solar System's history, Mercury may have been struck by a planetesimal of approximately 1/6 Mercury's mass and several thousand kilometers across.[48] The impact would have stripped away much of the original crust and mantle, leaving the core behind as a relatively major component.[48] A similar process, known as the giant impact hypothesis, has been proposed to explain the formation of the Moon.[48]

Alternatively, Mercury may have formed from the solar nebula before the Sun's energy output had stabilized. It would initially have had twice its present mass, but as the protosun contracted, temperatures near Mercury could have been between 2,500 and 3,500 K and possibly even as high as 10,000 K.[49] Much of Mercury's surface rock could have been vaporized at such temperatures, forming an atmosphere of "rock vapor" that could have been carried away by the solar wind.[49] A third hypothesis proposes that the solar nebula caused drag on the particles from which Mercury was accreting, which meant that lighter particles were lost from the accreting material and not gathered by Mercury.[50]

Each hypothesis predicts a different surface composition, and two space missions have been tasked with making observations of this composition. The first MESSENGER, which ended in 2015, found higher-than-expected potassium and sulfur levels on the surface, suggesting that the giant impact hypothesis and vaporization of the crust and mantle did not occur because said potassium and sulfur would have been driven off by the extreme heat of these events.[51] BepiColombo, which will arrive at Mercury in 2025, will make observations to test these hypotheses.[52] The findings so far would seem to favor the third hypothesis; however, further analysis of the data is needed.[53]

Surface geology

Mercury's surface is similar in appearance to that of the Moon, showing extensive mare-like plains and heavy cratering, indicating that it has been geologically inactive for billions of years. It is more heterogeneous than the surface of Mars or the Moon, both of which contain significant stretches of similar geology, such as maria and plateaus.[54] Albedo features are areas of markedly different reflectivity, which include impact craters, the resulting ejecta, and ray systems. Larger albedo features correspond to higher reflectivity plains.[55] Mercury has dorsa (also called "wrinkle-ridges"), Moon-like highlands, montes (mountains), planitiae (plains), rupes (escarpments), and valles (valleys).[56][57]

 
MASCS spectrum scan of Mercury's surface by MESSENGER

The planet's mantle is chemically heterogeneous, suggesting the planet went through a magma ocean phase early in its history. Crystallization of minerals and convective overturn resulted in layered, chemically heterogeneous crust with large-scale variations in chemical composition observed on the surface. The crust is low in iron but high in sulfur, resulting from the stronger early chemically reducing conditions than is found in the other terrestrial planets. The surface is dominated by iron-poor pyroxene and olivine, as represented by enstatite and forsterite, respectively, along with sodium-rich plagioclase and minerals of mixed magnesium, calcium, and iron-sulfide. The less reflective regions of the crust are high in carbon, most likely in the form of graphite.[58]

Names for features on Mercury come from a variety of sources. Names coming from people are limited to the deceased. Craters are named for artists, musicians, painters, and authors who have made outstanding or fundamental contributions to their field. Ridges, or dorsa, are named for scientists who have contributed to the study of Mercury. Depressions or fossae are named for works of architecture. Montes are named for the word "hot" in a variety of languages. Plains or planitiae are named for Mercury in various languages. Escarpments or rupēs are named for ships of scientific expeditions. Valleys or valles are named for abandoned cities, towns, or settlements of antiquity.[59]

Impact basins and craters

 
Enhanced-color image of craters Munch (left), Sander (center) and Poe (right) amid volcanic plains (orange) near Caloris Basin

Mercury was heavily bombarded by comets and asteroids during and shortly following its formation 4.6 billion years ago, as well as during a possibly separate subsequent episode called the Late Heavy Bombardment that ended 3.8 billion years ago.[60] Mercury received impacts over its entire surface during this period of intense crater formation,[57] facilitated by the lack of any atmosphere to slow impactors down.[61] During this time Mercury was volcanically active; basins were filled by magma, producing smooth plains similar to the maria found on the Moon.[62][63] One of the most unusual craters is Apollodorus, or "the Spider", which hosts a serious of radiating troughs extending outwards from its impact site.[64]

Craters on Mercury range in diameter from small bowl-shaped cavities to multi-ringed impact basins hundreds of kilometers across. They appear in all states of degradation, from relatively fresh rayed craters to highly degraded crater remnants. Mercurian craters differ subtly from lunar craters in that the area blanketed by their ejecta is much smaller, a consequence of Mercury's stronger surface gravity.[65] According to International Astronomical Union rules, each new crater must be named after an artist who was famous for more than fifty years, and dead for more than three years, before the date the crater is named.[66]

 
Overhead view of Caloris Basin
 
Perspective view of Caloris Basin – high (red); low (blue)

The largest known crater is Caloris Planitia, or Caloris Basin, with a diameter of 1,550 km.[67] The impact that created the Caloris Basin was so powerful that it caused lava eruptions and left a concentric mountainous ring ~2 km tall surrounding the impact crater. The floor of the Caloris Basin is filled by a geologically distinct flat plain, broken up by ridges and fractures in a roughly polygonal pattern. It is not clear whether they are volcanic lava flows induced by the impact or a large sheet of impact melt.[65]

At the antipode of the Caloris Basin is a large region of unusual, hilly terrain known as the "Weird Terrain". One hypothesis for its origin is that shock waves generated during the Caloris impact traveled around Mercury, converging at the basin's antipode (180 degrees away). The resulting high stresses fractured the surface.[68] Alternatively, it has been suggested that this terrain formed as a result of the convergence of ejecta at this basin's antipode.[69]

 
Tolstoj basin is along the bottom of this image of Mercury's limb

Overall, 46 impact basins have been identified.[70] A notable basin is the 400 km wide, multi-ring Tolstoj Basin that has an ejecta blanket extending up to 500 km from its rim and a floor that has been filled by smooth plains materials. Beethoven Basin has a similar-sized ejecta blanket and a 625 km diameter rim.[65] Like the Moon, the surface of Mercury has likely incurred the effects of space weathering processes, including solar wind and micrometeorite impacts.[71]

Plains

There are two geologically distinct plains regions on Mercury.[65][72] Gently rolling, hilly plains in the regions between craters are Mercury's oldest visible surfaces,[65] predating the heavily cratered terrain. These inter-crater plains appear to have obliterated many earlier craters, and show a general paucity of smaller craters below about 30 km in diameter.[72]

Smooth plains are widespread flat areas that fill depressions of various sizes and bear a strong resemblance to the lunar maria. Unlike lunar maria, the smooth plains of Mercury have the same albedo as the older inter-crater plains. Despite a lack of unequivocally volcanic characteristics, the localisation and rounded, lobate shape of these plains strongly support volcanic origins.[65] All the smooth plains of Mercury formed significantly later than the Caloris basin, as evidenced by appreciably smaller crater densities than on the Caloris ejecta blanket.[65]

Compressional features

One unusual feature of Mercury's surface is the numerous compression folds, or rupes, that crisscross the plains. These also exist on the moon, but are much more prominent on Mercury.[73] As Mercury's interior cooled, it contracted and its surface began to deform, creating wrinkle ridges and lobate scarps associated with thrust faults. The scarps can reach lengths of 1000 km and heights of 3 km.[74] These compressional features can be seen on top of other features, such as craters and smooth plains, indicating they are more recent.[75] Mapping of the features has suggested a total shrinkage of Mercury's radius in the range of ~1 to 7 km.[76] Most activity along the major thrust systems probably ended about 3.6–3.7 billion years ago.[77] Small-scale thrust fault scarps have been found, tens of meters in height and with lengths in the range of a few km, that appear to be less than 50 million years old, indicating that compression of the interior and consequent surface geological activity continue to the present.[74][76]

Volcanism

 
Picasso crater — the large arc-shaped pit located on the eastern side of its floor are postulated to have formed when subsurface magma subsided or drained, causing the surface to collapse into the resulting void.

There is evidence for pyroclastic flows on Mercury from low-profile shield volcanoes.[78][79][80] 51 pyroclastic deposits have been identified,[81] where 90% of them are found within impact craters.[81] A study of the degradation state of the impact craters that host pyroclastic deposits suggests that pyroclastic activity occurred on Mercury over a prolonged interval.[81]

A "rimless depression" inside the southwest rim of the Caloris Basin consists of at least nine overlapping volcanic vents, each individually up to 8 km in diameter. It is thus a "compound volcano".[82] The vent floors are at least 1 km below their brinks and they bear a closer resemblance to volcanic craters sculpted by explosive eruptions or modified by collapse into void spaces created by magma withdrawal back down into a conduit.[82] Scientists could not quantify the age of the volcanic complex system but reported that it could be on the order of a billion years.[82]

Surface conditions and exosphere

 
Composite of the north pole of Mercury, where NASA confirmed the discovery of a large volume of water ice, in permanently dark craters that are found there.[83]

The surface temperature of Mercury ranges from 100 to 700 K (−173 to 427 °C; −280 to 800 °F)[22] at the most extreme places: 0°N, 0°W, or 180°W. It never rises above 180 K at the poles,[14] due to the absence of an atmosphere and a steep temperature gradient between the equator and the poles. The subsolar point reaches about 700 K during perihelion (0°W or 180°W), but only 550 K at aphelion (90° or 270°W).[84] On the dark side of the planet, temperatures average 110 K.[14][85] The intensity of sunlight on Mercury's surface ranges between 4.59 and 10.61 times the solar constant (1,370 W·m−2).[86]

Although the daylight temperature at the surface of Mercury is generally extremely high, observations strongly suggest that ice (frozen water) exists on Mercury. The floors of deep craters at the poles are never exposed to direct sunlight, and temperatures there remain below 102 K, far lower than the global average.[87] This creates a cold trap where ice can accumulate. Water ice strongly reflects radar, and observations by the 70-meter Goldstone Solar System Radar and the VLA in the early 1990s revealed that there are patches of high radar reflection near the poles.[88] Although ice was not the only possible cause of these reflective regions, astronomers think it was the most likely.[89]

The icy regions are estimated to contain about 1014–1015 kg of ice,[90] and may be covered by a layer of regolith that inhibits sublimation.[91] By comparison, the Antarctic ice sheet on Earth has a mass of about 4×1018 kg, and Mars's south polar cap contains about 1016 kg of water.[90] The origin of the ice on Mercury is not yet known, but the two most likely sources are from outgassing of water from the planet's interior or deposition by impacts of comets.[90]

Mercury is too small and hot for its gravity to retain any significant atmosphere over long periods of time; it does have a tenuous surface-bounded exosphere[92] containing hydrogen, helium, oxygen, sodium, calcium, potassium and others[16][17] at a surface pressure of less than approximately 0.5 nPa (0.005 picobars).[3] This exosphere is not stable—atoms are continuously lost and replenished from a variety of sources. Hydrogen atoms and helium atoms probably come from the solar wind, diffusing into Mercury's magnetosphere before later escaping back into space. Radioactive decay of elements within Mercury's crust is another source of helium, as well as sodium and potassium. MESSENGER found high proportions of calcium, helium, hydroxide, magnesium, oxygen, potassium, silicon and sodium. Water vapor is present, released by a combination of processes such as: comets striking its surface, sputtering creating water out of hydrogen from the solar wind and oxygen from rock, and sublimation from reservoirs of water ice in the permanently shadowed polar craters. The detection of high amounts of water-related ions like O+, OH, and H3O+ was a surprise.[93][94] Because of the quantities of these ions that were detected in Mercury's space environment, scientists surmise that these molecules were blasted from the surface or exosphere by the solar wind.[95][96]

Sodium, potassium and calcium were discovered in the atmosphere during the 1980–1990s, and are thought to result primarily from the vaporization of surface rock struck by micrometeorite impacts[97] including presently from Comet Encke.[98] In 2008, magnesium was discovered by MESSENGER.[99] Studies indicate that, at times, sodium emissions are localized at points that correspond to the planet's magnetic poles. This would indicate an interaction between the magnetosphere and the planet's surface.[100]

On November 29, 2012, NASA confirmed that images from MESSENGER had detected that craters at the north pole contained water ice. MESSENGER's principal investigator Sean Solomon is quoted in The New York Times estimating the volume of the ice to be large enough to "encase Washington, D.C., in a frozen block two and a half miles deep".[83]

According to NASA, Mercury is not a suitable planet for Earth-like life. It has a surface boundary exosphere instead of a layered atmosphere, extreme temperatures, and high solar radiation. It is unlikely that any living beings can withstand those conditions.[101] Some parts of the subsurface of Mercury may have been habitable, and perhaps life forms, albeit likely primitive microorganisms, may have existed on the planet.[102][103][104]

Magnetic field and magnetosphere

 
Graph showing relative strength of Mercury's magnetic field

Despite its small size and slow 59-day-long rotation, Mercury has a significant, and apparently global, magnetic field. According to measurements taken by Mariner 10, it is about 1.1% the strength of Earth's. The magnetic-field strength at Mercury's equator is about 300 nT.[105][106] Like that of Earth, Mercury's magnetic field is dipolar.[100] Unlike Earth's, Mercury's poles are nearly aligned with the planet's spin axis.[107] Measurements from both the Mariner 10 and MESSENGER space probes have indicated that the strength and shape of the magnetic field are stable.[107]

It is likely that this magnetic field is generated by a dynamo effect, in a manner similar to the magnetic field of Earth.[108][109] This dynamo effect would result from the circulation of the planet's iron-rich liquid core. Particularly strong tidal heating effects caused by the planet's high orbital eccentricity would serve to keep part of the core in the liquid state necessary for this dynamo effect.[40][110]

Mercury's magnetic field is strong enough to deflect the solar wind around the planet, creating a magnetosphere. The planet's magnetosphere, though small enough to fit within Earth,[100] is strong enough to trap solar wind plasma. This contributes to the space weathering of the planet's surface.[107] Observations taken by the Mariner 10 spacecraft detected this low energy plasma in the magnetosphere of the planet's nightside. Bursts of energetic particles in the planet's magnetotail indicate a dynamic quality to the planet's magnetosphere.[100]

During its second flyby of the planet on October 6, 2008, MESSENGER discovered that Mercury's magnetic field can be extremely "leaky". The spacecraft encountered magnetic "tornadoes" – twisted bundles of magnetic fields connecting the planetary magnetic field to interplanetary space – that were up to 800 km wide or a third of the radius of the planet. These twisted magnetic flux tubes, technically known as flux transfer events, form open windows in the planet's magnetic shield through which the solar wind may enter and directly impact Mercury's surface via magnetic reconnection[111] This also occurs in Earth's magnetic field. The MESSENGER observations showed the reconnection rate is ten times higher at Mercury, but its proximity to the Sun only accounts for about a third of the reconnection rate observed by MESSENGER.[111]

Orbit, rotation, and longitude

 
Orbit of Mercury (2006)
 
Animation of Mercury's and Earth's revolution around the Sun

Mercury has the most eccentric orbit of all the planets in the Solar System; its eccentricity is 0.21 with its distance from the Sun ranging from 46,000,000 to 70,000,000 km (29,000,000 to 43,000,000 mi). It takes 87.969 Earth days to complete an orbit. The diagram illustrates the effects of the eccentricity, showing Mercury's orbit overlaid with a circular orbit having the same semi-major axis. Mercury's higher velocity when it is near perihelion is clear from the greater distance it covers in each 5-day interval. In the diagram, the varying distance of Mercury to the Sun is represented by the size of the planet, which is inversely proportional to Mercury's distance from the Sun. This varying distance to the Sun leads to Mercury's surface being flexed by tidal bulges raised by the Sun that are about 17 times stronger than the Moon's on Earth.[112] Combined with a 3:2 spin–orbit resonance of the planet's rotation around its axis, it also results in complex variations of the surface temperature.[32] The resonance makes a single solar day (the length between two meridian transits of the Sun) on Mercury last exactly two Mercury years, or about 176 Earth days.[113]

Mercury's orbit is inclined by 7 degrees to the plane of Earth's orbit (the ecliptic), the largest of all eight known solar planets.[114] As a result, transits of Mercury across the face of the Sun can only occur when the planet is crossing the plane of the ecliptic at the time it lies between Earth and the Sun, which is in May or November. This occurs about every seven years on average.[115]

Mercury's axial tilt is almost zero,[116] with the best measured value as low as 0.027 degrees.[117] This is significantly smaller than that of Jupiter, which has the second smallest axial tilt of all planets at 3.1 degrees. This means that to an observer at Mercury's poles, the center of the Sun never rises more than 2.1 arcminutes above the horizon.[117]

At certain points on Mercury's surface, an observer would be able to see the Sun peek up a little more than two-thirds of the way over the horizon, then reverse and set before rising again, all within the same Mercurian day.[c] This is because approximately four Earth days before perihelion, Mercury's angular orbital velocity equals its angular rotational velocity so that the Sun's apparent motion ceases; closer to perihelion, Mercury's angular orbital velocity then exceeds the angular rotational velocity. Thus, to a hypothetical observer on Mercury, the Sun appears to move in a retrograde direction. Four Earth days after perihelion, the Sun's normal apparent motion resumes.[32] A similar effect would have occurred if Mercury had been in synchronous rotation: the alternating gain and loss of rotation over revolution would have caused a libration of 23.65° in longitude.[118]

For the same reason, there are two points on Mercury's equator, 180 degrees apart in longitude, at either of which, around perihelion in alternate Mercurian years (once a Mercurian day), the Sun passes overhead, then reverses its apparent motion and passes overhead again, then reverses a second time and passes overhead a third time, taking a total of about 16 Earth-days for this entire process. In the other alternate Mercurian years, the same thing happens at the other of these two points. The amplitude of the retrograde motion is small, so the overall effect is that, for two or three weeks, the Sun is almost stationary overhead, and is at its most brilliant because Mercury is at perihelion, its closest to the Sun. This prolonged exposure to the Sun at its brightest makes these two points the hottest places on Mercury. Maximum temperature occurs when the Sun is at an angle of about 25 degrees past noon due to diurnal temperature lag, at 0.4 Mercury days and 0.8 Mercury years past sunrise.[119] Conversely, there are two other points on the equator, 90 degrees of longitude apart from the first ones, where the Sun passes overhead only when the planet is at aphelion in alternate years, when the apparent motion of the Sun in Mercury's sky is relatively rapid. These points, which are the ones on the equator where the apparent retrograde motion of the Sun happens when it is crossing the horizon as described in the preceding paragraph, receive much less solar heat than the first ones described above.[120]

Mercury attains inferior conjunction (nearest approach to Earth) every 116 Earth days on average,[3] but this interval can range from 105 days to 129 days due to the planet's eccentric orbit. Mercury can come as near as 82,200,000 km (0.549 astronomical units; 51.1 million miles) to Earth, and that is slowly declining: The next approach to within 82,100,000 km (51 million mi) is in 2679, and to within 82,000,000 km (51 million mi) in 4487, but it will not be closer to Earth than 80,000,000 km (50 million mi) until 28,622.[121] Its period of retrograde motion as seen from Earth can vary from 8 to 15 days on either side of inferior conjunction. This large range arises from the planet's high orbital eccentricity.[32] Essentially because Mercury is closest to the Sun, when taking an average over time, Mercury is most often the closest planet to the Earth,[18][19] and—in that measure—it is the closest planet to each of the other planets in the Solar System.[122][123][124][d]

Longitude convention

The longitude convention for Mercury puts the zero of longitude at one of the two hottest points on the surface, as described above. However, when this area was first visited, by Mariner 10, this zero meridian was in darkness, so it was impossible to select a feature on the surface to define the exact position of the meridian. Therefore, a small crater further west was chosen, called Hun Kal, which provides the exact reference point for measuring longitude.[125][126] The center of Hun Kal defines the 20° west meridian. A 1970 International Astronomical Union resolution suggests that longitudes be measured positively in the westerly direction on Mercury.[127] The two hottest places on the equator are therefore at longitudes 0° W and 180° W, and the coolest points on the equator are at longitudes 90° W and 270° W. However, the MESSENGER project uses an east-positive convention.[128]

Spin-orbit resonance

 
After one orbit, Mercury has rotated 1.5 times, so after two complete orbits the same hemisphere is again illuminated.

For many years it was thought that Mercury was synchronously tidally locked with the Sun, rotating once for each orbit and always keeping the same face directed towards the Sun, in the same way that the same side of the Moon always faces Earth. Radar observations in 1965 proved that the planet has a 3:2 spin-orbit resonance, rotating three times for every two revolutions around the Sun. The eccentricity of Mercury's orbit makes this resonance stable—at perihelion, when the solar tide is strongest, the Sun is nearly still in Mercury's sky.[129]

The rare 3:2 resonant tidal locking is stabilized by the variance of the tidal force along Mercury's eccentric orbit, acting on a permanent dipole component of Mercury's mass distribution.[130] In a circular orbit there is no such variance, so the only resonance stabilized in such an orbit is at 1:1 (e.g., Earth–Moon), when the tidal force, stretching a body along the "center-body" line, exerts a torque that aligns the body's axis of least inertia (the "longest" axis, and the axis of the aforementioned dipole) to point always at the center. However, with noticeable eccentricity, like that of Mercury's orbit, the tidal force has a maximum at perihelion and therefore stabilizes resonances, like 3:2, ensuring that the planet points its axis of least inertia roughly at the Sun when passing through perihelion.[130]

The original reason astronomers thought it was synchronously locked was that, whenever Mercury was best placed for observation, it was always nearly at the same point in its 3:2 resonance, hence showing the same face. This is because, coincidentally, Mercury's rotation period is almost exactly half of its synodic period with respect to Earth. Due to Mercury's 3:2 spin-orbit resonance, a solar day lasts about 176 Earth days.[32] A sidereal day (the period of rotation) lasts about 58.7 Earth days.[32]

Simulations indicate that the orbital eccentricity of Mercury varies chaotically from nearly zero (circular) to more than 0.45 over millions of years due to perturbations from the other planets.[32][131] This was thought to explain Mercury's 3:2 spin-orbit resonance (rather than the more usual 1:1), because this state is more likely to arise during a period of high eccentricity.[132] However, accurate modeling based on a realistic model of tidal response has demonstrated that Mercury was captured into the 3:2 spin-orbit state at a very early stage of its history, within 20 (more likely, 10) million years after its formation.[133]

Numerical simulations show that a future secular orbital resonant perihelion interaction with Jupiter may cause the eccentricity of Mercury's orbit to increase to the point where there is a 1% chance that the orbit will be destabilized in the next five billion years. If this happens, Mercury may fall into the Sun, collide with Venus, be ejected from the Solar System, or even disrupt the rest of the inner Solar System.[134][135]

Advance of perihelion

In 1859, the French mathematician and astronomer Urbain Le Verrier reported that the slow precession of Mercury's orbit around the Sun could not be completely explained by Newtonian mechanics and perturbations by the known planets. He suggested, among possible explanations, that another planet (or perhaps instead a series of smaller "corpuscules") might exist in an orbit even closer to the Sun than that of Mercury, to account for this perturbation.[136] (Other explanations considered included a slight oblateness of the Sun.) The success of the search for Neptune based on its perturbations of the orbit of Uranus led astronomers to place faith in this possible explanation, and the hypothetical planet was named Vulcan, but no such planet was ever found.[137]

The observed perihelion precession of Mercury is 5,600 arcseconds (1.5556°) per century relative to Earth, or 574.10±0.65 arcseconds per century[138] relative to the inertial ICRF. Newtonian mechanics, taking into account all the effects from the other planets (included 0.0254 arcsecond per century due to the "flatteness" of the Sun), predicts a precession of 5,557 arcseconds (1.5436°) per century relative to Earth, or 531.63±0.69 arcseconds per century relative to ICRF.[138] In the early 20th century, Albert Einstein's general theory of relativity provided the explanation for the observed precession, by formalizing gravitation as being mediated by the curvature of spacetime. The effect is small: just 42.98 arcseconds per century (or 0.43 arcsecond per year, or 0.1038 arcsecond per orbital period) for Mercury; it therefore requires a little over twelve million orbits, or 2.8 million years, for a full excess turn. Similar, but much smaller, effects exist for other Solar System bodies: 8.62 arcseconds per century for Venus, 3.84 for Earth, 1.35 for Mars, and 10.05 for 1566 Icarus.[139][140]

Observation

 
Image mosaic by Mariner 10, 1974

Mercury's apparent magnitude is calculated to vary between −2.48 (brighter than Sirius) around superior conjunction and +7.25 (below the limit of naked-eye visibility) around inferior conjunction.[15] The mean apparent magnitude is 0.23 while the standard deviation of 1.78 is the largest of any planet. The mean apparent magnitude at superior conjunction is −1.89 while that at inferior conjunction is +5.93.[15] Observation of Mercury is complicated by its proximity to the Sun, as it is lost in the Sun's glare for much of the time. Mercury can be observed for only a brief period during either morning or evening twilight.[141]

But in some cases Mercury can better be observed in daylight with a telescope when the position is known because it is higher in the sky and less atmospheric effects affect the view of the planet. When proper safety precautions are taken to prevent inadvertently pointing the telescope at the Sun (and thus blinding the user), Mercury can be viewed as close as 4° to the Sun when near superior conjunction when it is almost at its brightest.

Mercury can, like several other planets and the brightest stars, be seen during a total solar eclipse.[142]

Like the Moon and Venus, Mercury exhibits phases as seen from Earth. It is "new" at inferior conjunction and "full" at superior conjunction. The planet is rendered invisible from Earth on both of these occasions because of its being obscured by the Sun,[141] except its new phase during a transit.

Mercury is technically brightest as seen from Earth when it is at a full phase. Although Mercury is farthest from Earth when it is full, the greater illuminated area that is visible and the opposition brightness surge more than compensates for the distance.[143] The opposite is true for Venus, which appears brightest when it is a crescent, because it is much closer to Earth than when gibbous.[143][144]

 
False-color map showing the maximum temperatures of the north polar region

Nonetheless, the brightest (full phase) appearance of Mercury is an essentially impossible time for practical observation, because of the extreme proximity of the Sun. Mercury is best observed at the first and last quarter, although they are phases of lesser brightness. The first and last quarter phases occur at greatest elongation east and west of the Sun, respectively. At both of these times Mercury's separation from the Sun ranges anywhere from 17.9° at perihelion to 27.8° at aphelion.[145][146] At greatest western elongation, Mercury rises at its earliest before sunrise, and at greatest eastern elongation, it sets at its latest after sunset.[147]

 
False-color image of Carnegie Rupes, a tectonic landform—high terrain (red); low (blue).

Mercury is more often and easily visible from the Southern Hemisphere than from the Northern. This is because Mercury's maximum western elongation occurs only during early autumn in the Southern Hemisphere, whereas its greatest eastern elongation happens only during late winter in the Southern Hemisphere.[147] In both of these cases, the angle at which the planet's orbit intersects the horizon is maximized, allowing it to rise several hours before sunrise in the former instance and not set until several hours after sundown in the latter from southern mid-latitudes, such as Argentina and South Africa.[147]

An alternate method for viewing Mercury involves observing the planet during daylight hours when conditions are clear, ideally when it is at its greatest elongation. This allows the planet to be found easily, even when using telescopes with 8 cm (3.1 in) apertures. However, great care must be taken to obstruct the Sun from sight because of the extreme risk for eye damage.[148] This method bypasses the limitation of twilight observing when the ecliptic is located at a low elevation (e.g. on autumn evenings).

Ground-based telescope observations of Mercury reveal only an illuminated partial disk with limited detail. The first of two spacecraft to visit the planet was Mariner 10, which mapped about 45% of its surface from 1974 to 1975. The second is the MESSENGER spacecraft, which after three Mercury flybys between 2008 and 2009, attained orbit around Mercury on March 17, 2011,[149] to study and map the rest of the planet.[150]

The Hubble Space Telescope cannot observe Mercury at all, due to safety procedures that prevent its pointing too close to the Sun.[151]

Because the shift of 0.15 revolutions in a year makes up a seven-year cycle (0.15 × 7 ≈ 1.0), in the seventh year Mercury follows almost exactly (earlier by 7 days) the sequence of phenomena it showed seven years before.[145]

Observation history

Ancient astronomers

 
Mercury, from Liber astronomiae, 1550

The earliest known recorded observations of Mercury are from the MUL.APIN tablets. These observations were most likely made by an Assyrian astronomer around the 14th century BC.[152] The cuneiform name used to designate Mercury on the MUL.APIN tablets is transcribed as UDU.IDIM.GU\U4.UD ("the jumping planet").[e][153] Babylonian records of Mercury date back to the 1st millennium BC. The Babylonians called the planet Nabu after the messenger to the gods in their mythology.[154]

The Greco-Egyptian[155] astronomer Ptolemy wrote about the possibility of planetary transits across the face of the Sun in his work Planetary Hypotheses. He suggested that no transits had been observed either because planets such as Mercury were too small to see, or because the transits were too infrequent.[156]

 
Ibn al-Shatir's model for the appearances of Mercury, showing the multiplication of epicycles using the Tusi couple, thus eliminating the Ptolemaic eccentrics and equant.

In ancient China, Mercury was known as "the Hour Star" (Chen-xing 辰星). It was associated with the direction north and the phase of water in the Five Phases system of metaphysics.[157] Modern Chinese, Korean, Japanese and Vietnamese cultures refer to the planet literally as the "water star" (水星), based on the Five elements.[158][159][160] Hindu mythology used the name Budha for Mercury, and this god was thought to preside over Wednesday.[161] The god Odin (or Woden) of Germanic paganism was associated with the planet Mercury and Wednesday.[162] The Maya may have represented Mercury as an owl (or possibly four owls; two for the morning aspect and two for the evening) that served as a messenger to the underworld.[163]

In medieval Islamic astronomy, the Andalusian astronomer Abū Ishāq Ibrāhīm al-Zarqālī in the 11th century described the deferent of Mercury's geocentric orbit as being oval, like an egg or a pignon, although this insight did not influence his astronomical theory or his astronomical calculations.[164][165] In the 12th century, Ibn Bajjah observed "two planets as black spots on the face of the Sun", which was later suggested as the transit of Mercury and/or Venus by the Maragha astronomer Qotb al-Din Shirazi in the 13th century.[166] (Note that most such medieval reports of transits were later taken as observations of sunspots.[167])

In India, the Kerala school astronomer Nilakantha Somayaji in the 15th century developed a partially heliocentric planetary model in which Mercury orbits the Sun, which in turn orbits Earth, similar to the Tychonic system later proposed by Tycho Brahe in the late 16th century.[168]

Ground-based telescopic research

 
Transit of Mercury. Mercury is visible as a black dot below and to the left of center. The dark area above the center of the solar disk is a sunspot.
 
Elongation is the angle between the Sun and the planet, with Earth as the reference point. Mercury appears close to the Sun.

The first telescopic observations of Mercury were made by Thomas Harriot and Galileo from 1610. In 1612, Simon Marius observed the brightness of Mercury varied with the planet's orbital position and concluded it had phases "in the same way as Venus and the Moon".[169] In 1631, Pierre Gassendi made the first telescopic observations of the transit of a planet across the Sun when he saw a transit of Mercury predicted by Johannes Kepler. In 1639, Giovanni Zupi used a telescope to discover that the planet had orbital phases similar to Venus and the Moon. The observation demonstrated conclusively that Mercury orbited around the Sun.[32]

A rare event in astronomy is the passage of one planet in front of another (occultation), as seen from Earth. Mercury and Venus occult each other every few centuries, and the event of May 28, 1737 is the only one historically observed, having been seen by John Bevis at the Royal Greenwich Observatory.[170] The next occultation of Mercury by Venus will be on December 3, 2133.[171]

The difficulties inherent in observing Mercury mean that it was far less studied than the other planets. In 1800, Johann Schröter made observations of surface features, claiming to have observed 20-kilometre-high (12 mi) mountains. Friedrich Bessel used Schröter's drawings to erroneously estimate the rotation period as 24 hours and an axial tilt of 70°.[172] In the 1880s, Giovanni Schiaparelli mapped the planet more accurately, and suggested that Mercury's rotational period was 88 days, the same as its orbital period due to tidal locking.[173] This phenomenon is known as synchronous rotation. The effort to map the surface of Mercury was continued by Eugenios Antoniadi, who published a book in 1934 that included both maps and his own observations.[100] Many of the planet's surface features, particularly the albedo features, take their names from Antoniadi's map.[174]

In June 1962, Soviet scientists at the Institute of Radio-engineering and Electronics of the USSR Academy of Sciences, led by Vladimir Kotelnikov, became the first to bounce a radar signal off Mercury and receive it, starting radar observations of the planet.[175][176][177] Three years later, radar observations by Americans Gordon H. Pettengill and Rolf B. Dyce, using the 300-meter Arecibo radio telescope in Puerto Rico, showed conclusively that the planet's rotational period was about 59 days.[178][179] The theory that Mercury's rotation was synchronous had become widely held, and it was a surprise to astronomers when these radio observations were announced. If Mercury were tidally locked, its dark face would be extremely cold, but measurements of radio emission revealed that it was much hotter than expected. Astronomers were reluctant to drop the synchronous rotation theory and proposed alternative mechanisms such as powerful heat-distributing winds to explain the observations.[180]

 
Water ice (yellow) at Mercury's north polar region

Italian astronomer Giuseppe Colombo noted that the rotation value was about two-thirds of Mercury's orbital period, and proposed that the planet's orbital and rotational periods were locked into a 3:2 rather than a 1:1 resonance.[181] Data from Mariner 10 subsequently confirmed this view.[182] This means that Schiaparelli's and Antoniadi's maps were not "wrong". Instead, the astronomers saw the same features during every second orbit and recorded them, but disregarded those seen in the meantime, when Mercury's other face was toward the Sun, because the orbital geometry meant that these observations were made under poor viewing conditions.[172]

Ground-based optical observations did not shed much further light on Mercury, but radio astronomers using interferometry at microwave wavelengths, a technique that enables removal of the solar radiation, were able to discern physical and chemical characteristics of the subsurface layers to a depth of several meters.[183][184] Not until the first space probe flew past Mercury did many of its most fundamental morphological properties become known. Moreover, recent technological advances have led to improved ground-based observations. In 2000, high-resolution lucky imaging observations were conducted by the Mount Wilson Observatory 1.5 meter Hale telescope. They provided the first views that resolved surface features on the parts of Mercury that were not imaged in the Mariner 10 mission.[185] Most of the planet has been mapped by the Arecibo radar telescope, with 5 km (3.1 mi) resolution, including polar deposits in shadowed craters of what may be water ice.[186]

Research with space probes

 
MESSENGER being prepared for launch
 
Mercury transiting the Sun as viewed by the Mars rover Curiosity (June 3, 2014).[187]

Reaching Mercury from Earth poses significant technical challenges, because it orbits so much closer to the Sun than Earth. A Mercury-bound spacecraft launched from Earth must travel over 91 million kilometres (57 million miles) into the Sun's gravitational potential well. Mercury has an orbital speed of 47.4 km/s (29.5 mi/s), whereas Earth's orbital speed is 29.8 km/s (18.5 mi/s).[114] Therefore, the spacecraft must make a large change in velocity (delta-v) to get to Mercury and then enter orbit,[188] as compared to the delta-v required for, say, Mars planetary missions.

The potential energy liberated by moving down the Sun's potential well becomes kinetic energy, requiring a delta-v change to do anything other than pass by Mercury. Some portion of this delta-v budget can be provided from a gravity assist during one or more fly-bys of Venus.[189] To land safely or enter a stable orbit the spacecraft would rely entirely on rocket motors. Aerobraking is ruled out because Mercury has a negligible atmosphere. A trip to Mercury requires more rocket fuel than that required to escape the Solar System completely. As a result, only three space probes have visited it so far.[190] A proposed alternative approach would use a solar sail to attain a Mercury-synchronous orbit around the Sun.[191]

Mariner 10

 
Mariner 10, the first probe to visit Mercury

The first spacecraft to visit Mercury was NASA's Mariner 10 (1974–1975).[26] The spacecraft used the gravity of Venus to adjust its orbital velocity so that it could approach Mercury, making it both the first spacecraft to use this gravitational "slingshot" effect and the first NASA mission to visit multiple planets.[192] Mariner 10 provided the first close-up images of Mercury's surface, which immediately showed its heavily cratered nature, and revealed many other types of geological features, such as the giant scarps that were later ascribed to the effect of the planet shrinking slightly as its iron core cools.[193] Unfortunately, the same face of the planet was lit at each of Mariner 10's close approaches. This made close observation of both sides of the planet impossible,[194] and resulted in the mapping of less than 45% of the planet's surface.[195]

The spacecraft made three close approaches to Mercury, the closest of which took it to within 327 km (203 mi) of the surface.[196] At the first close approach, instruments detected a magnetic field, to the great surprise of planetary geologists—Mercury's rotation was expected to be much too slow to generate a significant dynamo effect. The second close approach was primarily used for imaging, but at the third approach, extensive magnetic data were obtained. The data revealed that the planet's magnetic field is much like Earth's, which deflects the solar wind around the planet. For many years after the Mariner 10 encounters, the origin of Mercury's magnetic field remained the subject of several competing theories.[197][198]

On March 24, 1975, just eight days after its final close approach, Mariner 10 ran out of fuel. Because its orbit could no longer be accurately controlled, mission controllers instructed the probe to shut down.[199] Mariner 10 is thought to be still orbiting the Sun, passing close to Mercury every few months.[200]

MESSENGER

 
Estimated details of the impact of MESSENGER on April 30, 2015

A second NASA mission to Mercury, named MESSENGER (MErcury Surface, Space ENvironment, GEochemistry, and Ranging), was launched on August 3, 2004. It made a fly-by of Earth in August 2005, and of Venus in October 2006 and June 2007 to place it onto the correct trajectory to reach an orbit around Mercury.[201] A first fly-by of Mercury occurred on January 14, 2008, a second on October 6, 2008,[202] and a third on September 29, 2009.[203] Most of the hemisphere not imaged by Mariner 10 was mapped during these fly-bys. The probe successfully entered an elliptical orbit around the planet on March 18, 2011. The first orbital image of Mercury was obtained on March 29, 2011. The probe finished a one-year mapping mission,[202] and then entered a one-year extended mission into 2013. In addition to continued observations and mapping of Mercury, MESSENGER observed the 2012 solar maximum.[204]

The mission was designed to clear up six key issues: Mercury's high density, its geological history, the nature of its magnetic field, the structure of its core, whether it has ice at its poles, and where its tenuous atmosphere comes from. To this end, the probe carried imaging devices that gathered much-higher-resolution images of much more of Mercury than Mariner 10, assorted spectrometers to determine abundances of elements in the crust, and magnetometers and devices to measure velocities of charged particles. Measurements of changes in the probe's orbital velocity were expected to be used to infer details of the planet's interior structure.[205] MESSENGER's final maneuver was on April 24, 2015, and it crashed into Mercury's surface on April 30, 2015.[206][207][208] The spacecraft's impact with Mercury occurred near 3:26 pm EDT on April 30, 2015, leaving a crater estimated to be 16 m (52 ft) in diameter.[209]

BepiColombo

The European Space Agency and the Japanese Space Agency developed and launched a joint mission called BepiColombo, which will orbit Mercury with two probes: one to map the planet and the other to study its magnetosphere.[210] Launched on October 20, 2018, BepiColombo is expected to reach Mercury in 2025.[211] It will release a magnetometer probe into an elliptical orbit, then chemical rockets will fire to deposit the mapper probe into a circular orbit. Both probes will operate for one terrestrial year.[210] The mapper probe carries an array of spectrometers similar to those on MESSENGER, and will study the planet at many different wavelengths including infrared, ultraviolet, X-ray and gamma ray.[212] BepiColombo conducted the first of its six planned Mercury flybys on October 1, 2021.[213]

See also

Notes

  1. ^ In astronomy, the words "rotation" and "revolution" have different meanings. "Rotation" is the turning of a body about an axis that passes through the body, as in "Earth rotates once a day." "Revolution" is motion around a centre that is external to the body, usually in orbit, as in "Earth takes a year for each revolution around the Sun." The verbs "rotate" and "revolve" mean doing rotation and revolution, respectively.
  2. ^ Pluto was considered a planet from its discovery in 1930 to 2006, but after that it has been reclassified as a dwarf planet. Pluto's orbital eccentricity is greater than Mercury's. Pluto is also smaller than Mercury, but was thought to be larger until 1976.
  3. ^ The Sun's total angular displacement during its apparent retrograde motion as seen from the surface of Mercury is ~1.23°, while the Sun's angular diameter when the apparent retrograde motion begins and ends is ~1.71°, increasing to ~1.73° at perihelion (midway through the retrograde motion).
  4. ^ It is important to be clear about the meaning of "closeness". In the astronomical literature, the term "closest planets" often means "the two planets that approach each other most closely". In other words, the orbits of the two planets approach each other most closely. However, this does not mean that the two planets are closest over time. For example, essentially because Mercury is closer to the Sun than Venus, Mercury spends more time in proximity to Earth; it could, therefore, be said that Mercury is the planet that is "closest to Earth when averaged over time". However, using this time-average definition of 'closeness'—as noted above—it turns out that Mercury is the closest planet to all other planets in the solar system. For that reason, arguably, the proximity-definition is not particularly helpful. An episode of the BBC Radio 4 programme "More or Less" explains the different notions of proximity well.[19]
  5. ^ Some sources precede the cuneiform transcription with "MUL". "MUL" is a cuneiform sign that was used in the Sumerian language to designate a star or planet, but it is not considered part of the actual name. The "4" is a reference number in the Sumero–Akkadian transliteration system to designate which of several syllables a certain cuneiform sign is most likely designating.

References

  1. ^ . Lexico UK English Dictionary. Oxford University Press. Archived from the original on March 27, 2020.
  2. ^ . Lexico UK English Dictionary UK English Dictionary. Oxford University Press. Archived from the original on December 22, 2019.
  3. ^ a b c d e f g h i j k l m Williams, David R. (November 25, 2020). "Mercury Fact Sheet". NASA. Retrieved April 19, 2021.
  4. ^ Souami, D.; Souchay, J. (July 2012). "The solar system's invariable plane". Astronomy & Astrophysics. 543: 11. Bibcode:2012A&A...543A.133S. doi:10.1051/0004-6361/201219011. A133.
  5. ^ Yeomans, Donald K. (April 7, 2008). "HORIZONS Web-Interface for Mercury Major Body". JPL Horizons On-Line Ephemeris System. Retrieved April 7, 2008. – Select "Ephemeris Type: Orbital Elements", "Time Span: 2000-01-01 12:00 to 2000-01-02". ("Target Body: Mercury" and "Center: Sun" should be defaulted to.) Results are instantaneous osculating values at the precise J2000 epoch.
  6. ^ a b c d e f g Davis, Phillips; Barnett, Amanda (February 15, 2021). "Mercury". Solar System Exploration. NASA Jet Propulsion Laboratory. Retrieved April 21, 2021.
  7. ^ Seidelmann, P. Kenneth; Archinal, Brent A.; A'Hearn, Michael F.; et al. (2007). "Report of the IAU/IAG Working Group on cartographic coordinates and rotational elements: 2006". Celestial Mechanics and Dynamical Astronomy. 98 (3): 155–180. Bibcode:2007CeMDA..98..155S. doi:10.1007/s10569-007-9072-y. S2CID 122772353.
  8. ^ Mazarico, Erwan; Genova, Antonio; Goossens, Sander; Lemoine, Frank G.; Neumann, Gregory A.; Zuber, Maria T.; Smith, David E.; Solomon, Sean C. (2014). "The gravity field, orientation, and ephemeris of Mercury from MESSENGER observations after three years in orbit" (PDF). Journal of Geophysical Research: Planets. 119 (12): 2417–2436. Bibcode:2014JGRE..119.2417M. doi:10.1002/2014JE004675. hdl:1721.1/97927. ISSN 2169-9097. S2CID 42430050.
  9. ^ a b c Margot, Jean-Luc; Peale, Stanton J.; Solomon, Sean C.; Hauck, Steven A.; Ghigo, Frank D.; Jurgens, Raymond F.; Yseboodt, Marie; Giorgini, Jon D.; Padovan, Sebastiano; Campbell, Donald B. (2012). "Mercury's moment of inertia from spin and gravity data". Journal of Geophysical Research: Planets. 117 (E12): n/a. Bibcode:2012JGRE..117.0L09M. CiteSeerX 10.1.1.676.5383. doi:10.1029/2012JE004161. ISSN 0148-0227. S2CID 22408219.
  10. ^ "ESO". ESO. Retrieved June 3, 2021.
  11. ^ Mallama, Anthony (2017). "The spherical bolometric albedo for planet Mercury". arXiv:1703.02670 [astro-ph.EP].
  12. ^ Mallama, Anthony; Wang, Dennis; Howard, Russell A. (2002). "Photometry of Mercury from SOHO/LASCO and Earth". Icarus. 155 (2): 253–264. Bibcode:2002Icar..155..253M. doi:10.1006/icar.2001.6723.
  13. ^ "Atmospheres and Planetary Temperatures". American Chemical Society. July 18, 2013. Retrieved January 3, 2023.
  14. ^ a b c d Vasavada, Ashwin R.; Paige, David A.; Wood, Stephen E. (February 19, 1999). "Near-Surface Temperatures on Mercury and the Moon and the Stability of Polar Ice Deposits" (PDF). Icarus. 141 (2): 179–193. Bibcode:1999Icar..141..179V. doi:10.1006/icar.1999.6175. Figure 3 with the "TWO model"; Figure 5 for pole.
  15. ^ a b c Mallama, Anthony; Hilton, James L. (October 2018). "Computing apparent planetary magnitudes for The Astronomical Almanac". Astronomy and Computing. 25: 10–24. arXiv:1808.01973. Bibcode:2018A&C....25...10M. doi:10.1016/j.ascom.2018.08.002. S2CID 69912809.
  16. ^ a b Milillo, A.; Wurz, P.; Orsini, S.; Delcourt, D.; Kallio, E.; Killen, R. M.; Lammer, H.; Massetti, S.; Mura, A.; Barabash, S.; Cremonese, G.; Daglis, I. A.; Angelis, E.; Lellis, A. M.; Livi, S.; Mangano, V.; Torkar, K. (April 2005). "Surface-Exosphere-Magnetosphere System Of Mercury". Space Science Reviews. 117 (3–4): 397–443. Bibcode:2005SSRv..117..397M. doi:10.1007/s11214-005-3593-z. S2CID 122285073.
  17. ^ a b Berezhnoy, Alexey A. (January 2018). "Chemistry of impact events on Mercury". Icarus. 300: 210–222. Bibcode:2018Icar..300..210B. doi:10.1016/j.icarus.2017.08.034.
  18. ^ a b "Venus is not Earth's closest neighbor". Physics Today. AIP Publishing. March 12, 2019. doi:10.1063/pt.6.3.20190312a. ISSN 1945-0699. S2CID 241077611.
  19. ^ a b c Harford, Tim (January 11, 2019). "BBC Radio 4 – More or Less, Sugar, Outdoors Play and Planets". BBC. Oliver Hawkins, more or less alumnus and statistical legend, wrote some code for us, which calculated which planet was closest to the Earth on each day for the past 50 years, and then sent the results to David A. Rothery, professor of planetary geosciences at the Open University.
  20. ^ Elkins-Tanton, Linda T. (2006). Uranus, Neptune, Pluto, and the Outer Solar System. Infobase Publishing. p. 51. ISBN 978-1-4381-0729-5. Extract of page 51
  21. ^ "Animated clip of orbit and rotation of Mercury". Sciencenetlinks.com.
  22. ^ a b Prockter, Louise (2005). Ice in the Solar System (PDF). Vol. 26. Johns Hopkins APL Technical Digest. Retrieved July 27, 2009.
  23. ^ . Archived from the original on May 3, 2015. Retrieved April 30, 2015.
  24. ^ "From Mercury orbit, MESSENGER watches a lunar eclipse". Planetary Society. October 10, 2014. Retrieved January 23, 2015.
  25. ^ "Innovative use of pressurant extends MESSENGER's Mercury mission". Astronomy.com. December 29, 2014. Retrieved January 22, 2015.
  26. ^ a b c Dunne, James A.; Burgess, Eric (1978). "Chapter One". The Voyage of Mariner 10 – Mission to Venus and Mercury. NASA History Office.
  27. ^ Στίλβων, Ἑρμῆς. Liddell, Henry George; Scott, Robert; A Greek–English Lexicon at the Perseus Project.
  28. ^ "Greek Names of the Planets". April 25, 2010. Retrieved July 14, 2012. Ermis is the Greek name of the planet Mercury, which is the closest planet to the Sun. It is named after the Greek God of commerce, Ermis or Hermes, who was also the messenger of the Ancient Greek gods. See also the Greek article about the planet.
  29. ^ Antoniadi, Eugène Michel (1974). The Planet Mercury. Translated from French by Moore, Patrick. Shaldon, Devon: Keith Reid Ltd. pp. 9–11. ISBN 978-0-904094-02-2.
  30. ^ Duncan, John Charles (1946). Astronomy: A Textbook. Harper & Brothers. p. 125. The symbol for Mercury represents the Caduceus, a wand with two serpents twined around it, which was carried by the messenger of the gods.
  31. ^ Jones, Alexander (1999). Astronomical papyri from Oxyrhynchus. pp. 62–63. ISBN 9780871692337. It is now possible to trace the medieval symbols for at least four of the five planets to forms that occur in some of the latest papyrus horoscopes ([ P.Oxy. ] 4272, 4274, 4275 [...]). Mercury's is a stylized caduceus.
  32. ^ a b c d e f g h Strom, Robert G.; Sprague, Ann L. (2003). Exploring Mercury: the iron planet. Springer. ISBN 978-1-85233-731-5.
  33. ^ Talbert, Tricia, ed. (March 21, 2012). "MESSENGER Provides New Look at Mercury's Surprising Core and Landscape Curiosities". NASA.
  34. ^ "Scientists find evidence Mercury has a solid inner core". AGU Newsroom. Retrieved April 17, 2019.
  35. ^ . US Geological Survey. May 8, 2003. Archived from the original on September 29, 2006. Retrieved November 26, 2006.
  36. ^ Lyttleton, Raymond A. (1969). "On the Internal Structures of Mercury and Venus". Astrophysics and Space Science. 5 (1): 18–35. Bibcode:1969Ap&SS...5...18L. doi:10.1007/BF00653933. S2CID 122572625.
  37. ^ Hauck, Steven A.; Margot, Jean-Luc; Solomon, Sean C.; Phillips, Roger J.; Johnson, Catherine L.; Lemoine, Frank G.; Mazarico, Erwan; McCoy, Timothy J.; Padovan, Sebastiano; Peale, Stanton J.; Perry, Mark E.; Smith, David E.; Zuber, Maria T. (2013). "The curious case of Mercury's internal structure". Journal of Geophysical Research: Planets. 118 (6): 1204–1220. Bibcode:2013JGRE..118.1204H. doi:10.1002/jgre.20091. hdl:1721.1/85633. S2CID 17668886.
  38. ^ Gold, Lauren (May 3, 2007). "Mercury has molten core, Cornell researcher shows". Chronicle. Cornell University. Retrieved May 12, 2008.
  39. ^ Finley, Dave (May 3, 2007). "Mercury's Core Molten, Radar Study Shows". National Radio Astronomy Observatory. Retrieved May 12, 2008.
  40. ^ a b Spohn, Tilman; Sohl, Frank; Wieczerkowski, Karin; Conzelmann, Vera (2001). "The interior structure of Mercury: what we know, what we expect from BepiColombo". Planetary and Space Science. 49 (14–15): 1561–1570. Bibcode:2001P&SS...49.1561S. doi:10.1016/S0032-0633(01)00093-9.
  41. ^ Gallant, Roy A. (1986). The National Geographic Picture Atlas of Our Universe (2nd ed.). National Geographic Society. ISBN 9780870446443.
  42. ^ Padovan, Sebastiano; Wieczorek, Mark A.; Margot, Jean-Luc; Tosi, Nicola; Solomon, Sean C. (2015). "Thickness of the crust of Mercury from geoid-to-topography ratios". Geophysical Research Letters. 42 (4): 1029. Bibcode:2015GeoRL..42.1029P. doi:10.1002/2014GL062487. S2CID 31442257.
  43. ^ Solomon, Sean C.; Nittler, Larry R.; Anderson, Brian J. (December 20, 2018). Mercury: The View after MESSENGER. Cambridge University Press. p. 534. ISBN 978-1-107-15445-2.
  44. ^ Sori, Michael M. (May 2018). "A thin, dense crust for Mercury". Earth and Planetary Science Letters. 489: 92–99. Bibcode:2018E&PSL.489...92S. doi:10.1016/j.epsl.2018.02.033.
  45. ^ Schenk, Paul M.; Melosh, H. Jay (March 1994). "Lobate Thrust Scarps and the Thickness of Mercury's Lithosphere". Abstracts of the 25th Lunar and Planetary Science Conference. 1994: 1994LPI....25.1203S. Bibcode:1994LPI....25.1203S.
  46. ^ Watters, T. R.; Nimmo, F.; Robinson, M. S. (2004). Chronology of Lobate Scarp Thrust Faults and the Mechanical Structure of Mercury's Lithosphere. Lunar and Planetary Science Conference. p. 1886. Bibcode:2004LPI....35.1886W.
  47. ^ Watters, Thomas R.; Robinson, Mark S.; Cook, Anthony C. (November 1998). "Topography of lobate scarps on Mercury; new constraints on the planet's contraction". Geology. 26 (11): 991–994. Bibcode:1998Geo....26..991W. doi:10.1130/0091-7613(1998)026<0991:TOLSOM>2.3.CO;2.
  48. ^ a b c d Benz, W.; Slattery, W. L.; Cameron, Alastair G. W. (1988). "Collisional stripping of Mercury's mantle". Icarus. 74 (3): 516–528. Bibcode:1988Icar...74..516B. doi:10.1016/0019-1035(88)90118-2.
  49. ^ a b Cameron, Alastair G. W. (1985). "The partial volatilization of Mercury". Icarus. 64 (2): 285–294. Bibcode:1985Icar...64..285C. doi:10.1016/0019-1035(85)90091-0.
  50. ^ Weidenschilling, Stuart J. (1987). "Iron/silicate fractionation and the origin of Mercury". Icarus. 35 (1): 99–111. Bibcode:1978Icar...35...99W. doi:10.1016/0019-1035(78)90064-7.
  51. ^ Sappenfield, Mark (September 29, 2011). "Messenger's message from Mercury: Time to rewrite the textbooks". The Christian Science Monitor. Retrieved August 21, 2017.
  52. ^ "BepiColombo". Science & Technology. European Space Agency. Retrieved April 7, 2008.
  53. ^ Cartwright, Jon (September 30, 2011). "Messenger sheds light on Mercury's formation". Chemistry World. Retrieved August 21, 2017.
  54. ^ Morris, Jefferson (November 10, 2008). "Laser Altimetry". Aviation Week & Space Technology. 169 (18): 18. Mercury's crust is more analogous to a marbled cake than a layered cake.
  55. ^ Hughes, E. T.; Vaughan, W. M. (March 2012). Albedo Features of Mercury. 43rd Lunar and Planetary Science Conference, held March 19–23, 2012 at The Woodlands, Texas. Vol. 1659. Bibcode:2012LPI....43.2151H. 2151.
  56. ^ Blue, Jennifer (April 11, 2008). "Gazetteer of Planetary Nomenclature". US Geological Survey. Retrieved April 11, 2008.
  57. ^ a b Dunne, James A.; Burgess, Eric (1978). "Chapter Seven". The Voyage of Mariner 10 – Mission to Venus and Mercury. NASA History Office. Retrieved May 28, 2008.
  58. ^ Nittler, Larry R.; Weider, Shoshana Z. (2019). "The Surface Composition of Mercury". Elements. 15 (1): 33–38. doi:10.2138/gselements.15.1.33. S2CID 135051680.
  59. ^ "Categories for Naming Features on Planets and Satellites". US Geological Survey. Retrieved August 20, 2011.
  60. ^ Strom, Robert G. (1979). "Mercury: a post-Mariner assessment". Space Science Reviews. 24 (1): 3–70. Bibcode:1979SSRv...24....3S. doi:10.1007/BF00221842. S2CID 122563809.
  61. ^ Broadfoot, A. Lyle; Kumar, Shailendra; Belton, Michael J. S.; McElroy, Michael B. (July 12, 1974). "Mercury's Atmosphere from Mariner 10: Preliminary Results". Science. 185 (4146): 166–169. Bibcode:1974Sci...185..166B. doi:10.1126/science.185.4146.166. PMID 17810510. S2CID 7790470.
  62. ^ Geology of the solar system. IMAP 2596. U.S. Geological Survey. 1997. doi:10.3133/i2596.
  63. ^ Head, James W.; Solomon, Sean C. (1981). (PDF). Science. 213 (4503): 62–76. Bibcode:1981Sci...213...62H. CiteSeerX 10.1.1.715.4402. doi:10.1126/science.213.4503.62. hdl:2060/20020090713. PMID 17741171. Archived from the original (PDF) on July 21, 2018. Retrieved October 25, 2017.
  64. ^ "Scientists see Mercury in a new light". Science Daily. February 28, 2008. Retrieved April 7, 2008.
  65. ^ a b c d e f g Spudis, Paul D. (2001). "The Geological History of Mercury". Workshop on Mercury: Space Environment, Surface, and Interior, Chicago (1097): 100. Bibcode:2001mses.conf..100S.
  66. ^ Ritzel, Rebecca (December 20, 2012). "Ballet isn't rocket science, but the two aren't mutually exclusive, either". The Washington Post. Washington, D.C., United States. Retrieved December 22, 2012.
  67. ^ Shiga, David (January 30, 2008). "Bizarre spider scar found on Mercury's surface". NewScientist.com news service.
  68. ^ Schultz, Peter H.; Gault, Donald E. (1975). "Seismic effects from major basin formations on the moon and Mercury". Earth, Moon, and Planets. 12 (2): 159–175. Bibcode:1975Moon...12..159S. doi:10.1007/BF00577875. S2CID 121225801.
  69. ^ Wieczorek, Mark A.; Zuber, Maria T. (2001). "A Serenitatis origin for the Imbrian grooves and South Pole-Aitken thorium anomaly". Journal of Geophysical Research. 106 (E11): 27853–27864. Bibcode:2001JGR...10627853W. doi:10.1029/2000JE001384. Retrieved May 12, 2008.
  70. ^ Fassett, Caleb I.; Head, James W.; Baker, David M. H.; Zuber, Maria T.; Smith, David E.; Neumann, Gregory A.; Solomon, Sean C.; Klimczak, Christian; Strom, Robert G.; Chapman, Clark R.; Prockter, Louise M.; Phillips, Roger J.; Oberst, Jürgen; Preusker, Frank (October 2012). "Large impact basins on Mercury: Global distribution, characteristics, and modification history from MESSENGER orbital data". Journal of Geophysical Research. 117. 15 pp. Bibcode:2012JGRE..117.0L08F. doi:10.1029/2012JE004154. E00L08.
  71. ^ Denevi, Brett W.; Robinson, Mark S. (2008). "Albedo of Immature Mercurian Crustal Materials: Evidence for the Presence of Ferrous Iron". Lunar and Planetary Science. 39 (1391): 1750. Bibcode:2008LPI....39.1750D.
  72. ^ a b Wagner, Roland J.; Wolf, Ursula; Ivanov, Boris A.; Neukum, Gerhard (October 4–5, 2001). Application of an Updated Impact Cratering Chronology Model to Mercury' s Time-Stratigraphic System. Workshop on Mercury: Space Environment, Surface, and Interior. Proceedings of a workshop held at The Field Museum. Chicago, IL: Lunar and Planetary Science Institute. p. 106. Bibcode:2001mses.conf..106W.
  73. ^ Schleicher, Lisa S.; Watters, Thomas R.; Martin, Aaron J.; Banks, Maria E. (October 2019). "Wrinkle ridges on Mercury and the Moon within and outside of mascons". Icarus. 331: 226–237. Bibcode:2019Icar..331..226S. doi:10.1016/j.icarus.2019.04.013. S2CID 150072193.
  74. ^ a b Choi, Charles Q. (September 26, 2016). "Mercuryquakes May Currently Shake Up the Tiny Planet". Space.com. Retrieved September 28, 2016.
  75. ^ Dzurisin, Daniel (October 10, 1978). "The tectonic and volcanic history of Mercury as inferred from studies of scarps, ridges, troughs, and other lineaments". Journal of Geophysical Research. 83 (B10): 4883–4906. Bibcode:1978JGR....83.4883D. doi:10.1029/JB083iB10p04883.
  76. ^ a b Watters, Thomas R.; Daud, Katie; Banks, Maria E.; Selvans, Michelle M.; Chapman, Clark R.; Ernst, Carolyn M. (September 26, 2016). "Recent tectonic activity on Mercury revealed by small thrust fault scarps". Nature Geoscience. 9 (10): 743–747. Bibcode:2016NatGe...9..743W. doi:10.1038/ngeo2814.
  77. ^ Giacomini, L.; Massironi, M.; Galluzzi, V.; Ferrari, S.; Palumbo, P. (May 2020). "Dating long thrust systems on Mercury: New clues on the thermal evolution of the planet". Geoscience Frontiers. 11 (3): 855–870. doi:10.1016/j.gsf.2019.09.005. S2CID 210298205.
  78. ^ Kerber, Laura; Head, James W.; Solomon, Sean C.; Murchie, Scott L.; Blewett, David T. (August 15, 2009). "Explosive volcanic eruptions on Mercury: Eruption conditions, magma volatile content, and implications for interior volatile abundances". Earth and Planetary Science Letters. 285 (3–4): 263–271. Bibcode:2009E&PSL.285..263K. doi:10.1016/j.epsl.2009.04.037.
  79. ^ Head, James W.; Chapman, Clark R.; Strom, Robert G.; Fassett, Caleb I.; Denevi, Brett W. (September 30, 2011). "Flood Volcanism in the Northern High Latitudes of Mercury Revealed by MESSENGER" (PDF). Science. 333 (6051): 1853–1856. Bibcode:2011Sci...333.1853H. doi:10.1126/science.1211997. PMID 21960625. S2CID 7651992.
  80. ^ Thomas, Rebecca J.; Rothery, David A.; Conway, Susan J.; Anand, Mahesh (September 16, 2014). "Long-lived explosive volcanism on Mercury". Geophysical Research Letters. 41 (17): 6084–6092. Bibcode:2014GeoRL..41.6084T. doi:10.1002/2014GL061224. S2CID 54683272.
  81. ^ a b c Groudge, Timothy A.; Head, James W. (March 2014). "Global inventory and characterization of pyroclastic deposits on Mercury: New insights into pyroclastic activity from MESSENGER orbital data" (PDF). Journal of Geophysical Research. 119 (3): 635–658. Bibcode:2014JGRE..119..635G. doi:10.1002/2013JE004480. S2CID 14393394.
  82. ^ a b c Rothery, David A.; Thomas, Rebeca J.; Kerber, Laura (January 1, 2014). "Prolonged eruptive history of a compound volcano on Mercury: Volcanic and tectonic implications" (PDF). Earth and Planetary Science Letters. 385: 59–67. Bibcode:2014E&PSL.385...59R. doi:10.1016/j.epsl.2013.10.023.
  83. ^ a b Chang, Kenneth (November 29, 2012). "On Closest Planet to the Sun, NASA Finds Lots of Ice". The New York Times. p. A3. from the original on November 29, 2012. Sean C. Solomon, the principal investigator for MESSENGER, said there was enough ice there to encase Washington, D.C., in a frozen block two and a half miles deep.
  84. ^ Lewis, John S. (2004). Physics and Chemistry of the Solar System (2nd ed.). Academic Press. p. 463. ISBN 978-0-12-446744-6.
  85. ^ Murdock, Thomas L.; Ney, Edward P. (1970). "Mercury: The Dark-Side Temperature". Science. 170 (3957): 535–537. Bibcode:1970Sci...170..535M. doi:10.1126/science.170.3957.535. PMID 17799708. S2CID 38824994.
  86. ^ Lewis, John S. (2004). Physics and Chemistry of the Solar System. Academic Press. ISBN 978-0-12-446744-6. Retrieved June 3, 2008.
  87. ^ Ingersoll, Andrew P.; Svitek, Tomas; Murray, Bruce C. (1992). "Stability of polar frosts in spherical bowl-shaped craters on the Moon, Mercury, and Mars". Icarus. 100 (1): 40–47. Bibcode:1992Icar..100...40I. doi:10.1016/0019-1035(92)90016-Z.
  88. ^ Slade, Martin A.; Butler, Bryan J.; Muhleman, Duane O. (1992). "Mercury radar imaging – Evidence for polar ice". Science. 258 (5082): 635–640. Bibcode:1992Sci...258..635S. doi:10.1126/science.258.5082.635. PMID 17748898. S2CID 34009087.
  89. ^ Williams, David R. (June 2, 2005). "Ice on Mercury". NASA Goddard Space Flight Center. Retrieved May 23, 2008.
  90. ^ a b c Rawlins, Katherine; Moses, Julianne I.; Zahnle, Kevin J. (1995). "Exogenic Sources of Water for Mercury's Polar Ice". Bulletin of the American Astronomical Society. 27: 1117. Bibcode:1995DPS....27.2112R.
  91. ^ Harmon, John K.; Perillat, Phil J.; Slade, Martin A. (2001). "High-Resolution Radar Imaging of Mercury's North Pole". Icarus. 149 (1): 1–15. Bibcode:2001Icar..149....1H. doi:10.1006/icar.2000.6544.
  92. ^ Domingue DL, Koehn PL, et al. (2009). "Mercury's Atmosphere: A Surface-Bounded Exosphere". Space Science Reviews. 131 (1–4): 161–186. Bibcode:2007SSRv..131..161D. doi:10.1007/s11214-007-9260-9. S2CID 121301247.
  93. ^ Hunten, Donald M.; Shemansky, Donald Eugene; Morgan, Thomas Hunt (1988). "The Mercury atmosphere". In Vilas, Faith; Chapman, Clark R.; Shapley Matthews, Mildred (eds.). Mercury. University of Arizona Press. ISBN 978-0-8165-1085-6.
  94. ^ Lakdawalla, Emily (July 3, 2008). "MESSENGER Scientists "Astonished" to Find Water in Mercury's Thin Atmosphere". The Planetary Society. Retrieved May 18, 2009.
  95. ^ Zurbuchen TH, Raines JM, et al. (2008). "MESSENGER Observations of the Composition of Mercury's Ionized Exosphere and Plasma Environment". Science. 321 (5885): 90–92. Bibcode:2008Sci...321...90Z. doi:10.1126/science.1159314. PMID 18599777. S2CID 206513512.
  96. ^ "Instrument Shows What Planet Mercury Is Made Of". University of Michigan. June 30, 2008. Retrieved May 18, 2009.
  97. ^ Killen, Rosemary; Cremonese, Gabrielle; et al. (2007). "Processes that Promote and Deplete the Exosphere of Mercury". Space Science Reviews. 132 (2–4): 433–509. Bibcode:2007SSRv..132..433K. doi:10.1007/s11214-007-9232-0. S2CID 121944553.
  98. ^ Killen, Rosemary M.; Hahn, Joseph M. (December 10, 2014). "Impact Vaporization as a Possible Source of Mercury's Calcium Exosphere". Icarus. 250: 230–237. Bibcode:2015Icar..250..230K. doi:10.1016/j.icarus.2014.11.035. hdl:2060/20150010116.
  99. ^ McClintock, William E.; Vervack, Ronald J.; et al. (2009). "MESSENGER Observations of Mercury's Exosphere: Detection of Magnesium and Distribution of Constituents". Science. 324 (5927): 610–613. Bibcode:2009Sci...324..610M. doi:10.1126/science.1172525. PMID 19407195. S2CID 5578520.
  100. ^ a b c d e Beatty, J. Kelly; Petersen, Carolyn Collins; Chaikin, Andrew (1999). The New Solar System. Cambridge University Press. ISBN 978-0-521-64587-4.
  101. ^ "Mercury". NASA. October 19, 2021. Retrieved July 4, 2022.
  102. ^ Hall, Shannon (March 24, 2020). "Life on the Planet Mercury? 'It's Not Completely Nuts' – A new explanation for the rocky world's jumbled landscape opens a possibility that it could have had ingredients for habitability". The New York Times. from the original on March 24, 2020. Retrieved March 26, 2020.
  103. ^ Rodriguez, J. Alexis P.; Leonard, Gregory J.; Kargel, Jeffrey S.; Domingue, Deborah; Berman, Daniel C.; Banks, Maria; Zarroca, Mario; Linares, Rogelio; Marchi, Simone; Baker, Victor R.; Webster, Kevin D.; Sykes, Mark (March 16, 2020). "The Chaotic Terrains of Mercury Reveal a History of Planetary Volatile Retention and Loss in the Innermost Solar System". Scientific Reports. 10 (4737): 4737. Bibcode:2020NatSR..10.4737R. doi:10.1038/s41598-020-59885-5. PMC 7075900. PMID 32179758.
  104. ^ "Vast Collapsed Terrains on Mercury Might be Windows Into Ancient – Possibly Habitable – Volatile-Rich Materials". Planetary Science Institute. March 16, 2020. Retrieved August 27, 2022.
  105. ^ Seeds, Michael A. (2004). Astronomy: The Solar System and Beyond (4th ed.). Brooks Cole. ISBN 978-0-534-42111-3.
  106. ^ Williams, David R. (January 6, 2005). "Planetary Fact Sheets". NASA National Space Science Data Center. Retrieved August 10, 2006.
  107. ^ a b c "Mercury's Internal Magnetic Field". NASA. January 30, 2008. Retrieved April 21, 2021.
  108. ^ Gold, Lauren (May 3, 2007). "Mercury has molten core, Cornell researcher shows". Cornell University. Retrieved April 7, 2008.
  109. ^ Christensen, Ulrich R. (2006). "A deep dynamo generating Mercury's magnetic field". Nature. 444 (7122): 1056–1058. Bibcode:2006Natur.444.1056C. doi:10.1038/nature05342. PMID 17183319. S2CID 4342216.
  110. ^ Padovan, Sebastiano; Margot, Jean-Luc; Hauck, Steven A.; Moore, William B.; Solomon, Sean C. (April 2014). "The tides of Mercury and possible implications for its interior structure". Journal of Geophysical Research: Planets. 119 (4): 850–866. Bibcode:2014JGRE..119..850P. doi:10.1002/2013JE004459. S2CID 56282397.
  111. ^ a b Steigerwald, Bill (June 2, 2009). "Magnetic Tornadoes Could Liberate Mercury's Tenuous Atmosphere". NASA Goddard Space Flight Center. Retrieved July 18, 2009.
  112. ^ Van Hoolst, Tim; Jacobs, Carla (2003). "Mercury's tides and interior structure". Journal of Geophysical Research. 108 (E11): 7. Bibcode:2003JGRE..108.5121V. doi:10.1029/2003JE002126.
  113. ^ . Planetary Society. Archived from the original on July 28, 2011. Retrieved April 12, 2007.
  114. ^ a b Williams, David R. (October 21, 2019). "Planetary Fact Sheet – Metric". NASA. Retrieved April 20, 2021.
  115. ^ Espenak, Fred (April 21, 2005). "Transits of Mercury". NASA/Goddard Space Flight Center. Retrieved May 20, 2008.
  116. ^ Biswas, Sukumar (2000). Cosmic Perspectives in Space Physics. Astrophysics and Space Science Library. Springer. p. 176. ISBN 978-0-7923-5813-8.
  117. ^ a b Margot, J. L.; Peale, S. J.; Jurgens, R. F.; Slade, M. A.; et al. (2007). "Large Longitude Libration of Mercury Reveals a Molten Core". Science. 316 (5825): 710–714. Bibcode:2007Sci...316..710M. doi:10.1126/science.1140514. PMID 17478713. S2CID 8863681.
  118. ^ Popular Astronomy: A Review of Astronomy and Allied Sciences. Goodsell Observatory of Carleton College. 1896. although in the case of Venus the libration in longitude due to the eccentricity of the orbit amounts to only 47' on either side of the mean position, in the case of Mercury it amounts to 23° 39'
  119. ^ Seligman, C. "The Rotation of Mercury". cseligman.com. NASA Flash animation. Retrieved July 31, 2019.
  120. ^ van Hemerlrijck, E. (August 1983). "On the Variations in the Insolation at Mercury Resulting from Oscillations of the Orbital Eccentricity". The Moon and the Planets. 29 (1): 83–93. Bibcode:1983M&P....29...83V. doi:10.1007/BF00928377. S2CID 122761699.
  121. ^ Mercury Closest Approaches to Earth generated with:
    1. Solex 10  December 20, 2008, at the Wayback Machine (Text Output file March 9, 2012, at the Wayback Machine)
    2. Gravity Simulator charts September 12, 2014, at the Wayback Machine
    3. JPL Horizons 1950–2200  November 6, 2015, at the Wayback Machine
    (3 sources are provided to address original research concerns and to support general long-term trends)
  122. ^ Stockman, Tom; Monroe, Gabriel; Cordner, Samuel (March 12, 2019). "Venus is not Earth's closest neighbor". Physics Today. doi:10.1063/PT.6.3.20190312a. S2CID 241077611.
  123. ^ Stockman, Tom (March 7, 2019). Mercury is the closest planet to all seven other planets (video). Archived from the original on October 28, 2021. Retrieved May 29, 2019 – via YouTube.
  124. ^ 🌍 Which Planet is the Closest?, archived from the original on October 28, 2021, retrieved July 22, 2021
  125. ^ Davies, M. E. (June 10, 1975). "Surface Coordinates and Cartography of Mercury". Journal of Geophysical Research. 80 (B17): 2417–2430. Bibcode:1975JGR....80.2417D. doi:10.1029/JB080i017p02417.
  126. ^ Davies, M. E.; Dwornik, S. E.; Gault, D. E.; Strom, R. G. (1978). NASA Atlas of Mercury. NASA Scientific and Technical Information Office.
  127. ^ . Archived from the original on October 24, 2011. Retrieved October 22, 2009.
  128. ^ Archinal, Brent A.; A'Hearn, Michael F.; Bowell, Edward L.; Conrad, Albert R.; et al. (2010). "Report of the IAU Working Group on Cartographic Coordinates and Rotational Elements: 2009". Celestial Mechanics and Dynamical Astronomy. 109 (2): 101–135. Bibcode:2011CeMDA.109..101A. doi:10.1007/s10569-010-9320-4. ISSN 0923-2958. S2CID 189842666.
  129. ^ Liu, Han-Shou; O'Keefe, John A. (1965). "Theory of Rotation for the Planet Mercury". Science. 150 (3704): 1717. Bibcode:1965Sci...150.1717L. doi:10.1126/science.150.3704.1717. PMID 17768871. S2CID 45608770.
  130. ^ a b Colombo, Giuseppe; Shapiro, Irwin I. (1966). "The rotation of the planet Mercury". Astrophysical Journal. 145: 296. Bibcode:1966ApJ...145..296C. doi:10.1086/148762.
  131. ^ Correia, Alexandre C. M.; Laskar, Jacques (2009). "Mercury's capture into the 3/2 spin-orbit resonance including the effect of core–mantle friction". Icarus. 201 (1): 1–11. arXiv:0901.1843. Bibcode:2009Icar..201....1C. doi:10.1016/j.icarus.2008.12.034. S2CID 14778204.
  132. ^ Correia, Alexandre C. M.; Laskar, Jacques (2004). "Mercury's capture into the 3/2 spin-orbit resonance as a result of its chaotic dynamics". Nature. 429 (6994): 848–850. Bibcode:2004Natur.429..848C. doi:10.1038/nature02609. PMID 15215857. S2CID 9289925.
  133. ^ Noyelles, B.; Frouard, J.; Makarov, V. V. & Efroimsky, M. (2014). "Spin-orbit evolution of Mercury revisited". Icarus. 241 (2014): 26–44. arXiv:1307.0136. Bibcode:2014Icar..241...26N. doi:10.1016/j.icarus.2014.05.045. S2CID 53690707.
  134. ^ Laskar, Jacques (March 18, 2008). "Chaotic diffusion in the Solar System". Icarus. 196 (1): 1–15. arXiv:0802.3371. Bibcode:2008Icar..196....1L. doi:10.1016/j.icarus.2008.02.017. S2CID 11586168.
  135. ^ Laskar, Jacques; Gastineau, Mickaël (June 11, 2009). "Existence of collisional trajectories of Mercury, Mars and Venus with the Earth". Nature. 459 (7248): 817–819. Bibcode:2009Natur.459..817L. doi:10.1038/nature08096. PMID 19516336. S2CID 4416436.
  136. ^ Le Verrier, Urbain (1859). "Lettre de M. Le Verrier à M. Faye sur la théorie de Mercure et sur le mouvement du périhélie de cette planète". Comptes rendus hebdomadaires des séances de l'Académie des sciences (in French). Paris. 49: 379–383. (At p. 383 in the same volume Le Verrier's report is followed by another, from Faye, enthusiastically recommending to astronomers to search for a previously undetected intra-mercurial object.)
  137. ^ Baum, Richard; Sheehan, William (1997). In Search of Planet Vulcan, The Ghost in Newton's Clockwork Machine. New York: Plenum Press. ISBN 978-0-306-45567-4.
  138. ^ a b Clemence, Gerald M. (1947). "The Relativity Effect in Planetary Motions". Reviews of Modern Physics. 19 (4): 361–364. Bibcode:1947RvMP...19..361C. doi:10.1103/RevModPhys.19.361.
  139. ^ Gilvarry, John J. (1953). "Relativity Precession of the Asteroid Icarus". Physical Review. 89 (5): 1046. Bibcode:1953PhRv...89.1046G. doi:10.1103/PhysRev.89.1046.
  140. ^ Brown, Kevin. "6.2 Anomalous Precession". Reflections on Relativity. MathPages. Retrieved May 22, 2008.
  141. ^ a b Menzel, Donald H. (1964). A Field Guide to the Stars and Planets. The Peterson Field Guide Series. Boston: Houghton Mifflin Co. pp. 292–293.
  142. ^ Tezel, Tunç (January 22, 2003). "Total Solar Eclipse of 2006 March 29". Department of Physics at Fizik Bolumu in Turkey. Retrieved May 24, 2008.
  143. ^ a b Mallama, Anthony (2011). "Planetary magnitudes". Sky and Telescope. 121 (1): 51–56.
  144. ^ Espenak, Fred (1996). "NASA Reference Publication 1349; Venus: Twelve year planetary ephemeris, 1995–2006". Twelve Year Planetary Ephemeris Directory. NASA. Retrieved May 24, 2008.
  145. ^ a b Walker, John. "Mercury Chaser's Calculator". Fourmilab Switzerland. Retrieved May 29, 2008. (look at 1964 and 2013)
  146. ^ . Archived from the original on May 11, 2013. Retrieved May 30, 2008. – Numbers generated using the Solar System Dynamics Group, Horizons On-Line Ephemeris System
  147. ^ a b c Kelly, Patrick, ed. (2007). Observer's Handbook 2007. Royal Astronomical Society of Canada. ISBN 978-0-9738109-3-6.
  148. ^ Curtis, A. C. (October 1972). "Finding Venus or Mercury in daylight". Journal of the British Astronomical Association. 82: 438–439. Bibcode:1972JBAA...82..438C.
  149. ^ Alers, Paul E. (March 17, 2011). "Celebrating Mercury Orbit". NASA Multimedia. Retrieved March 18, 2011.
  150. ^ "NASA spacecraft now circling Mercury – a first". NBC News. March 17, 2011. Retrieved March 24, 2011.
  151. ^ Baumgardner, Jeffrey; Mendillo, Michael; Wilson, Jody K. (2000). "A Digital High-Definition Imaging System for Spectral Studies of Extended Planetary Atmospheres. I. Initial Results in White Light Showing Features on the Hemisphere of Mercury Unimaged by Mariner 10". The Astronomical Journal. 119 (5): 2458–2464. Bibcode:2000AJ....119.2458B. doi:10.1086/301323. S2CID 17361371.
  152. ^ Schaefer, Bradley E. (2007). "The Latitude and Epoch for the Origin of the Astronomical Lore in MUL.APIN". American Astronomical Society Meeting 210, #42.05. 38: 157. Bibcode:2007AAS...210.4205S.
  153. ^ Hunger, Hermann; Pingree, David (1989). "MUL.APIN: An Astronomical Compendium in Cuneiform". Archiv für Orientforschung. 24: 146.
  154. ^ "MESSENGER: Mercury and Ancient Cultures". NASA JPL. 2008. Retrieved April 7, 2008.
  155. ^ Heath, Sir Thomas (1921). A History of Greek Mathematics. Vol. II. Oxford: Clarendon Press. pp. vii, 273.
  156. ^ Goldstein, Bernard R. (1996). "The Pre-telescopic Treatment of the Phases and Apparent Size of Venus". Journal for the History of Astronomy. 27: 1. Bibcode:1996JHA....27....1G. doi:10.1177/002182869602700101. S2CID 117218196.
  157. ^ Kelley, David H.; Milone, E. F.; Aveni, Anthony F. (2004). Exploring Ancient Skies: An Encyclopedic Survey of Archaeoastronomy. Birkhäuser. ISBN 978-0-387-95310-6.
  158. ^ De Groot, Jan Jakob Maria (1912). Religion in China: universism. a key to the study of Taoism and Confucianism. American lectures on the history of religions. Vol. 10. G. P. Putnam's Sons. p. 300. Retrieved January 8, 2010.
  159. ^ Crump, Thomas (1992). The Japanese numbers game: the use and understanding of numbers in modern Japan. Nissan Institute/Routledge Japanese studies series. Routledge. pp. 39–40. ISBN 978-0-415-05609-0.
  160. ^ Hulbert, Homer Bezaleel (1909). The passing of Korea. Doubleday, Page & company. p. 426. Retrieved January 8, 2010.
  161. ^ Pujari, R. M.; Kolhe, Pradeep; Kumar, N. R. (2006). Pride of India: A Glimpse Into India's Scientific Heritage. Samskrita Bharati. ISBN 978-81-87276-27-2.
  162. ^ Bakich, Michael E. (2000). The Cambridge Planetary Handbook. Cambridge University Press. ISBN 978-0-521-63280-5.
  163. ^ Milbrath, Susan (1999). Star Gods of the Maya: Astronomy in Art, Folklore and Calendars. University of Texas Press. ISBN 978-0-292-75226-9.
  164. ^ Samsó, Julio; Mielgo, Honorino (1994). "Ibn al-Zarqālluh on Mercury". Journal for the History of Astronomy. 25 (4): 289–96 [292]. Bibcode:1994JHA....25..289S. doi:10.1177/002182869402500403. S2CID 118108131.
  165. ^ Hartner, Willy (1955). "The Mercury Horoscope of Marcantonio Michiel of Venice". Vistas in Astronomy. 1 (1): 84–138. Bibcode:1955VA......1...84H. doi:10.1016/0083-6656(55)90016-7. at pp. 118–122.
  166. ^ Ansari, S. M. Razaullah (2002). History of oriental astronomy: proceedings of the joint discussion-17 at the 23rd General Assembly of the International Astronomical Union, organised by the Commission 41 (History of Astronomy), held in Kyoto, August 25–26, 1997. Springer Science+Business Media. p. 137. ISBN 1-4020-0657-8.
  167. ^ Goldstein, Bernard R. (1969). "Some Medieval Reports of Venus and Mercury Transits". Centaurus. 14 (1): 49–59. Bibcode:1969Cent...14...49G. doi:10.1111/j.1600-0498.1969.tb00135.x.
  168. ^ Ramasubramanian, K.; Srinivas, M. S.; Sriram, M. S. (1994). (PDF). Current Science. 66: 784–790. Archived from the original (PDF) on December 23, 2010. Retrieved April 23, 2010.
  169. ^ Gaab, Hans (2018). Simon Marius and His Research. Springer. p. 256. ISBN 978-3-319-92620-9. Marius noted in the dedication from June 30, 1612, in the Prognosticon auf 1613 "that Mercury is illuminated by the Sun in the same way as the Venus and the Moon" and reports his observations of the brightness.
  170. ^ Sinnott, Roger W.; Meeus, Jean (1986). "John Bevis and a Rare Occultation". Sky and Telescope. 72: 220. Bibcode:1986S&T....72..220S.
  171. ^ Ferris, Timothy (2003). Seeing in the Dark: How Amateur Astronomers. Simon and Schuster. ISBN 978-0-684-86580-5.
  172. ^ a b Colombo, Giuseppe; Shapiro, Irwin I. (November 1965). "The Rotation of the Planet Mercury". SAO Special Report #188R. 188: 188. Bibcode:1965SAOSR.188.....C.
  173. ^ Holden, Edward S. (1890). "Announcement of the Discovery of the Rotation Period of Mercury [by Professor Schiaparelli]". Publications of the Astronomical Society of the Pacific. 2 (7): 79. Bibcode:1890PASP....2...79H. doi:10.1086/120099. S2CID 122095054.
  174. ^ Davies, Merton E.; Dwornik, Stephen E.; Gault, Donald E.; Strom, Robert G. (1978). "Surface Mapping". Atlas of Mercury. NASA Office of Space Sciences. Retrieved May 28, 2008.
  175. ^ Evans, John V.; Brockelman, Richard A.; Henry, John C.; Hyde, Gerald M.; Kraft, Leon G.; Reid, Wyatt A.; Smith, W. W. (1965). "Radio Echo Observations of Venus and Mercury at 23 cm Wavelength". Astronomical Journal. 70: 487–500. Bibcode:1965AJ.....70..486E. doi:10.1086/109772.
  176. ^ Moore, Patrick (2000). The Data Book of Astronomy. New York: CRC Press. p. 483. ISBN 978-0-7503-0620-1.
  177. ^ Butrica, Andrew J. (1996). "Chapter 5". To See the Unseen: A History of Planetary Radar Astronomy. NASA History Office, Washington D.C. ISBN 978-0-16-048578-7.
  178. ^ Pettengill, Gordon H.; Dyce, Rolf B. (1965). "A Radar Determination of the Rotation of the Planet Mercury". Nature. 206 (1240): 451–2. Bibcode:1965Natur.206Q1240P. doi:10.1038/2061240a0. S2CID 31525579.
  179. ^ "Mercury". Eric Weisstein's World of Astronomy. Wolfram Research. Retrieved April 18, 2021.
  180. ^ Murray, Bruce C.; Burgess, Eric (1977). Flight to Mercury. Columbia University Press. ISBN 978-0-231-03996-3.
  181. ^ Colombo, Giuseppe (1965). "Rotational Period of the Planet Mercury". Nature. 208 (5010): 575. Bibcode:1965Natur.208..575C. doi:10.1038/208575a0. S2CID 4213296.
  182. ^ Davies, Merton E.; et al. (1976). "Mariner 10 Mission and Spacecraft". SP-423 Atlas of Mercury. NASA JPL. Retrieved April 7, 2008.
  183. ^ Golden, Leslie M. (1977). A Microwave Interferometric Study of the Subsurface of the Planet Mercury (Thesis). University of California, Berkeley. Bibcode:1977PhDT.........9G.
  184. ^ Mitchell, David L.; De Pater, Imke (1994). "Microwave Imaging of Mercury's Thermal Emission at Wavelengths from 0.3 to 20.5 cm (1994)". Icarus. 110 (1): 2–32. Bibcode:1994Icar..110....2M. doi:10.1006/icar.1994.1105.
  185. ^ Dantowitz, Ronald F.; Teare, Scott W.; Kozubal, Marek J. (2000). "Ground-based High-Resolution Imaging of Mercury". Astronomical Journal. 119 (4): 2455–2457. Bibcode:2000AJ....119.2455D. doi:10.1086/301328. S2CID 121483006.
  186. ^ Harmon, John K.; Slade, Martin A.; Butler, Bryan J.; Head III, James W.; Rice, Melissa S.; Campbell, Donald B. (2007). "Mercury: Radar images of the equatorial and midlatitude zones". Icarus. 187 (2): 374–405. Bibcode:2007Icar..187..374H. doi:10.1016/j.icarus.2006.09.026.
  187. ^ Webster, Guy (June 10, 2014). "Mercury Passes in Front of the Sun, as Seen From Mars". NASA. Retrieved June 10, 2014.
  188. ^ Zacny, Kris (July 2, 2015). Inner Solar System: Prospective Energy and Material Resources. Springer International Publishing. p. 154. ISBN 9783319195698.
  189. ^ Wagner, Sam; Wie, Bong (November 2015). "Hybrid Algorithm for Multiple Gravity-Assist and Impulsive Delta-V Maneuvers". Journal of Guidance, Control, and Dynamics. 38 (11): 2096–2107. Bibcode:2015JGCD...38.2096W. doi:10.2514/1.G000874.
  190. ^ "Mercury" (PDF). NASA Jet Propulsion Laboratory. May 5, 2008. Retrieved April 26, 2021.
  191. ^ Leipold, Manfred E.; Seboldt, W.; Lingner, Stephan; Borg, Erik; Herrmann, Axel Siegfried; Pabsch, Arno; Wagner, O.; Brückner, Johannes (1996). "Mercury sun-synchronous polar orbiter with a solar sail". Acta Astronautica. 39 (1): 143–151. Bibcode:1996AcAau..39..143L. doi:10.1016/S0094-5765(96)00131-2.
  192. ^ Dunne, James A. & Burgess, Eric (1978). "Chapter Four". The Voyage of Mariner 10 – Mission to Venus and Mercury. NASA History Office. Retrieved May 28, 2008.
  193. ^ Phillips, Tony (October 1976). "NASA 2006 Transit of Mercury". SP-423 Atlas of Mercury. NASA. Retrieved April 7, 2008.
  194. ^ "BepiColumbo – Background Science". European Space Agency. Retrieved June 18, 2017.
  195. ^ Malik, Tariq (August 16, 2004). "MESSENGER to test theory of shrinking Mercury". USA Today. Retrieved May 23, 2008.
  196. ^ Davies ME, et al. (1978). "Mariner 10 Mission and Spacecraft". Atlas of Mercury. NASA Office of Space Sciences. Retrieved May 30, 2008.
  197. ^ Ness, Norman F. (1978). "Mercury – Magnetic field and interior". Space Science Reviews. 21 (5): 527–553. Bibcode:1978SSRv...21..527N. doi:10.1007/BF00240907. S2CID 120025983.
  198. ^ Aharonson, Oded; Zuber, Maria T; Solomon, Sean C (2004). "Crustal remanence in an internally magnetized non-uniform shell: a possible source for Mercury's magnetic field?". Earth and Planetary Science Letters. 218 (3–4): 261–268. Bibcode:2004E&PSL.218..261A. doi:10.1016/S0012-821X(03)00682-4.
  199. ^ Dunne, James A. & Burgess, Eric (1978). "Chapter Eight". The Voyage of Mariner 10 – Mission to Venus and Mercury. NASA History Office.
  200. ^ Grayzeck, Ed (April 2, 2008). "Mariner 10". NSSDC Master Catalog. NASA. Retrieved April 7, 2008.
  201. ^ "MESSENGER Engine Burn Puts Spacecraft on Track for Venus". SpaceRef.com. 2005. Retrieved March 2, 2006.
  202. ^ a b . Johns Hopkins University Applied Physics Laboratory. January 14, 2008. Archived from the original on May 13, 2013. Retrieved May 30, 2008.
  203. ^ . MESSENGER Mission News. September 30, 2009. Archived from the original on May 10, 2013. Retrieved September 30, 2009.
  204. ^ "NASA extends spacecraft's Mercury mission". United Press International. November 15, 2011. Retrieved November 16, 2011.
  205. ^ "MESSENGER: Fact Sheet" (PDF). Applied Physics Laboratory. February 2011. Retrieved August 21, 2017.
  206. ^ Wall, Mike (March 29, 2015). "NASA Mercury Probe Trying to Survive for Another Month". Space.com. Retrieved April 4, 2015.
  207. ^ Chang, Kenneth (April 27, 2015). "NASA's Messenger Mission Is Set to Crash Into Mercury". The New York Times. from the original on April 29, 2015. Retrieved April 27, 2015.
  208. ^ Corum, Jonathan (April 30, 2015). "Messenger's Collision Course With Mercury". The New York Times. Retrieved April 30, 2015.
  209. ^ "Best Determination of MESSENGER's Impact Location". MESSENGER Featured Images. Johns Hopkins – Applied Physics Lab. June 3, 2015. Retrieved April 29, 2015.
  210. ^ a b "ESA gives go-ahead to build BepiColombo". European Space Agency. February 26, 2007. Retrieved May 29, 2008.
  211. ^ "BepiColombo Fact Sheet". European Space Agency. December 1, 2016. Retrieved December 19, 2016.
  212. ^ "Objectives". European Space Agency. February 21, 2006. Retrieved May 29, 2008.
  213. ^ Warren, Haygen (October 24, 2021). "BepiColombo completes first Mercury flyby, science provides insight into planet's unique environment". NASA Spaceflight. Retrieved October 8, 2022.

External links

Listen to this article (41 minutes)
 
This audio file was created from a revision of this article dated 16 January 2008 (2008-01-16), and does not reflect subsequent edits.
  • Atlas of Mercury. NASA. 1978. SP-423.
  • Mercury nomenclature and from the USGS/IAU Gazetteer of Planetary Nomenclature
  • Equirectangular map of Mercury by Applied Coherent Technology Corp
  • 3D globe of Mercury by Google
  • Mercury at Solarviews.com
  • Mercury by Astronomy Cast
  • MESSENGER mission web site
  • BepiColombo mission web site

mercury, planet, first, planet, redirects, here, other, systems, numbering, planets, planet, history, mercury, smallest, planet, solar, system, closest, orbit, around, takes, earth, days, shortest, planets, named, after, roman, mercurius, code, promoted, code,. First planet redirects here For other systems of numbering planets see Planet History Mercury is the smallest planet in the Solar System and the closest to the Sun Its orbit around the Sun takes 87 97 Earth days the shortest of all the Sun s planets It is named after the Roman god Mercurius code lat promoted to code la Mercury god of commerce messenger of the gods and mediator between gods and mortals corresponding to the Greek god Hermes Ἑrmῆs code ell promoted to code el Like Venus Mercury orbits the Sun within Earth s orbit as an inferior planet its apparent distance from the Sun as viewed from Earth never exceeds 28 This proximity to the Sun means the planet can only be seen near the western horizon after sunset or the eastern horizon before sunrise usually in twilight At this time it may appear as a bright star like object but is more difficult to observe than Venus From Earth the planet telescopically displays the complete range of phases similar to Venus and the Moon which recurs over its synodic period of approximately 116 days Due to its synodic proximity to Earth Mercury is most often the closest planet to Earth with Venus periodically taking this role 18 19 MercuryMercury in true color by MESSENGER in 2008 DesignationsPronunciation ˈ m ɜːr k j ʊr i listen AdjectivesMercurian m er ˈ k jʊer i e n 1 Mercurial m er ˈ k jʊer i e l 2 Orbital characteristics 5 Epoch J2000Aphelion0 466697 AU 69 816 900 kmPerihelion0 307499 AU 46 001 200 kmSemi major axis0 387098 AU 57 909 050 kmEccentricity0 205630 3 Orbital period sidereal 87 9691 d 0 240846 yr 0 5 Mercury synodic dayOrbital period synodic 115 88 d 3 Average orbital speed47 36 km s 3 Mean anomaly174 796 Inclination7 005 to ecliptic 3 38 to Sun s equator 6 35 to invariable plane 4 Longitude of ascending node48 331 Argument of perihelion29 124 SatellitesNonePhysical characteristicsMean diameter4880 kmMean radius2 439 7 1 0 km 6 7 0 3829 EarthsFlattening0 0009 3 Surface area7 48 107 km2 6 0 147 EarthsVolume6 083 1010 km3 6 0 056 EarthsMass3 3011 1023 kg 8 0 055 EarthsMean density5 427 g cm3 6 Surface gravity3 7 m s2 0 38 g 6 Moment of inertia factor0 346 0 014 9 Escape velocity4 25 km s 6 Synodic rotation period176 d 10 Sidereal rotation period58 646 d 1407 5 h 6 Equatorial rotation velocity10 892 km h 3 026 m s Axial tilt2 04 0 08 to orbit 9 0 034 3 North pole right ascension18h 44m 2s 281 01 3 North pole declination61 45 3 Albedo0 088 Bond 11 0 142 geom 12 Temperature437 K 164 C blackbody temperature 13 Surface temp min mean max0 N 0 W 14 173 C 67 C 427 C85 N 0 W 14 193 C 73 C 106 85 CApparent magnitude 2 48 to 7 25 15 Angular diameter4 5 13 3 Atmosphere 3 16 17 Surface pressuretrace 0 5 nPa Composition by volumeatomic oxygen sodium magnesium atomic hydrogen potassium calcium helium Trace amounts of iron aluminium argon dinitrogen dioxygen carbon dioxide water vapor xenon krypton and neonMercury rotates in a way that is unique in the Solar System It is tidally locked with the Sun in a 3 2 spin orbit resonance 20 meaning that relative to the fixed stars it rotates on its axis exactly three times for every two revolutions it makes around the Sun a 21 As seen from the Sun in a frame of reference that rotates with the orbital motion it appears to rotate only once every two Mercurian years An observer on Mercury would therefore see only one day every two Mercurian years Mercury s axis has the smallest tilt of any of the Solar System s planets about 1 30 degree Its orbital eccentricity is the largest of all known planets in the Solar System b at perihelion Mercury s distance from the Sun is only about two thirds or 66 of its distance at aphelion Mercury s surface appears heavily cratered and is similar in appearance to the Moon s indicating that it has been geologically inactive for billions of years Having almost no atmosphere to retain heat it has surface temperatures that vary diurnally more than on any other planet in the Solar System ranging from 100 K 173 C 280 F at night to 700 K 427 C 800 F during the day across the equatorial regions 22 The polar regions are constantly below 180 K 93 C 136 F The planet has no natural satellites Two spacecraft have visited Mercury Mariner 10 flew by in 1974 and 1975 and MESSENGER launched in 2004 orbited Mercury over 4 000 times in four years before exhausting its fuel and crashing into the planet s surface on April 30 2015 23 24 25 The BepiColombo spacecraft is planned to arrive at Mercury in 2025 Contents 1 Nomenclature 2 Physical characteristics 2 1 Internal structure 2 2 Surface geology 2 2 1 Impact basins and craters 2 2 2 Plains 2 2 3 Compressional features 2 2 4 Volcanism 2 3 Surface conditions and exosphere 2 4 Magnetic field and magnetosphere 3 Orbit rotation and longitude 3 1 Longitude convention 3 2 Spin orbit resonance 3 3 Advance of perihelion 4 Observation 5 Observation history 5 1 Ancient astronomers 5 2 Ground based telescopic research 5 3 Research with space probes 5 3 1 Mariner 10 5 3 2 MESSENGER 5 3 3 BepiColombo 6 See also 7 Notes 8 References 9 External linksNomenclatureThe ancients knew Mercury by different names depending on whether it was an evening star or a morning star By about 350 BC the ancient Greeks had realized the two stars were one 26 They knew the planet as Stilbwn Stilbōn meaning twinkling and Ἑrmhs Hermes for its fleeting motion 27 a name that is retained in modern Greek Ermhs Ermis 28 The Romans named the planet after the swift footed Roman messenger god Mercury Latin Mercurius which they equated with the Greek Hermes because it moves across the sky faster than any other planet 26 29 The astronomical symbol for Mercury is a stylized version of Hermes caduceus a Christian cross was added in the 16th century 30 31 Physical characteristicsMercury is one of four terrestrial planets in the Solar System and is a rocky body like Earth It is the smallest planet in the Solar System with an equatorial radius of 2 439 7 kilometres 1 516 0 mi 3 Mercury is also smaller albeit more massive than the largest natural satellites in the Solar System Ganymede and Titan Mercury consists of approximately 70 metallic and 30 silicate material 32 Internal structure Mercury s internal structure and magnetic field Mercury appears to have a solid silicate crust and mantle overlying a solid iron sulfide outer core layer a deeper liquid core layer and a solid inner core 33 34 The planet s density is the second highest in the Solar System at 5 427 g cm3 only slightly less than Earth s density of 5 515 g cm3 3 If the effect of gravitational compression were to be factored out from both planets the materials of which Mercury is made would be denser than those of Earth with an uncompressed density of 5 3 g cm3 versus Earth s 4 4 g cm3 35 Mercury s density can be used to infer details of its inner structure Although Earth s high density results appreciably from gravitational compression particularly at the core Mercury is much smaller and its inner regions are not as compressed Therefore for it to have such a high density its core must be large and rich in iron 36 The radius of Mercury s core is estimated to be 2 020 30 km 1 255 19 mi based on interior models constrained to be consistent with the value of the moment of inertia factor given in the infobox 9 37 Hence Mercury s core occupies about 57 of its volume for Earth this proportion is 17 Research published in 2007 suggests that Mercury has a molten core 38 39 Surrounding the core is a 500 700 km 310 430 mi mantle consisting of silicates 40 41 Based on data from the Mariner 10 and MESSENGER missions in addition to Earth based observation Mercury s crust is estimated to be 35 km 22 mi thick 42 43 However this model may be an overestimate and the crust could be 26 11 km 16 2 6 8 mi thick based on an Airy isostacy model 44 One distinctive feature of Mercury s surface is the presence of numerous narrow ridges extending up to several hundred kilometers in length It is thought that these were formed as Mercury s core and mantle cooled and contracted at a time when the crust had already solidified 45 46 47 Mercury s core has a higher iron content than that of any other major planet in the Solar System and several theories have been proposed to explain this The most widely accepted theory is that Mercury originally had a metal silicate ratio similar to common chondrite meteorites thought to be typical of the Solar System s rocky matter and a mass approximately 2 25 times its current mass 48 Early in the Solar System s history Mercury may have been struck by a planetesimal of approximately 1 6 Mercury s mass and several thousand kilometers across 48 The impact would have stripped away much of the original crust and mantle leaving the core behind as a relatively major component 48 A similar process known as the giant impact hypothesis has been proposed to explain the formation of the Moon 48 Alternatively Mercury may have formed from the solar nebula before the Sun s energy output had stabilized It would initially have had twice its present mass but as the protosun contracted temperatures near Mercury could have been between 2 500 and 3 500 K and possibly even as high as 10 000 K 49 Much of Mercury s surface rock could have been vaporized at such temperatures forming an atmosphere of rock vapor that could have been carried away by the solar wind 49 A third hypothesis proposes that the solar nebula caused drag on the particles from which Mercury was accreting which meant that lighter particles were lost from the accreting material and not gathered by Mercury 50 Each hypothesis predicts a different surface composition and two space missions have been tasked with making observations of this composition The first MESSENGER which ended in 2015 found higher than expected potassium and sulfur levels on the surface suggesting that the giant impact hypothesis and vaporization of the crust and mantle did not occur because said potassium and sulfur would have been driven off by the extreme heat of these events 51 BepiColombo which will arrive at Mercury in 2025 will make observations to test these hypotheses 52 The findings so far would seem to favor the third hypothesis however further analysis of the data is needed 53 Surface geology Main article Geology of Mercury Mercury s surface is similar in appearance to that of the Moon showing extensive mare like plains and heavy cratering indicating that it has been geologically inactive for billions of years It is more heterogeneous than the surface of Mars or the Moon both of which contain significant stretches of similar geology such as maria and plateaus 54 Albedo features are areas of markedly different reflectivity which include impact craters the resulting ejecta and ray systems Larger albedo features correspond to higher reflectivity plains 55 Mercury has dorsa also called wrinkle ridges Moon like highlands montes mountains planitiae plains rupes escarpments and valles valleys 56 57 MASCS spectrum scan of Mercury s surface by MESSENGER The planet s mantle is chemically heterogeneous suggesting the planet went through a magma ocean phase early in its history Crystallization of minerals and convective overturn resulted in layered chemically heterogeneous crust with large scale variations in chemical composition observed on the surface The crust is low in iron but high in sulfur resulting from the stronger early chemically reducing conditions than is found in the other terrestrial planets The surface is dominated by iron poor pyroxene and olivine as represented by enstatite and forsterite respectively along with sodium rich plagioclase and minerals of mixed magnesium calcium and iron sulfide The less reflective regions of the crust are high in carbon most likely in the form of graphite 58 Names for features on Mercury come from a variety of sources Names coming from people are limited to the deceased Craters are named for artists musicians painters and authors who have made outstanding or fundamental contributions to their field Ridges or dorsa are named for scientists who have contributed to the study of Mercury Depressions or fossae are named for works of architecture Montes are named for the word hot in a variety of languages Plains or planitiae are named for Mercury in various languages Escarpments or rupes are named for ships of scientific expeditions Valleys or valles are named for abandoned cities towns or settlements of antiquity 59 Impact basins and craters Enhanced color image of craters Munch left Sander center and Poe right amid volcanic plains orange near Caloris Basin Mercury was heavily bombarded by comets and asteroids during and shortly following its formation 4 6 billion years ago as well as during a possibly separate subsequent episode called the Late Heavy Bombardment that ended 3 8 billion years ago 60 Mercury received impacts over its entire surface during this period of intense crater formation 57 facilitated by the lack of any atmosphere to slow impactors down 61 During this time Mercury was volcanically active basins were filled by magma producing smooth plains similar to the maria found on the Moon 62 63 One of the most unusual craters is Apollodorus or the Spider which hosts a serious of radiating troughs extending outwards from its impact site 64 Craters on Mercury range in diameter from small bowl shaped cavities to multi ringed impact basins hundreds of kilometers across They appear in all states of degradation from relatively fresh rayed craters to highly degraded crater remnants Mercurian craters differ subtly from lunar craters in that the area blanketed by their ejecta is much smaller a consequence of Mercury s stronger surface gravity 65 According to International Astronomical Union rules each new crater must be named after an artist who was famous for more than fifty years and dead for more than three years before the date the crater is named 66 Overhead view of Caloris Basin Perspective view of Caloris Basin high red low blue The largest known crater is Caloris Planitia or Caloris Basin with a diameter of 1 550 km 67 The impact that created the Caloris Basin was so powerful that it caused lava eruptions and left a concentric mountainous ring 2 km tall surrounding the impact crater The floor of the Caloris Basin is filled by a geologically distinct flat plain broken up by ridges and fractures in a roughly polygonal pattern It is not clear whether they are volcanic lava flows induced by the impact or a large sheet of impact melt 65 At the antipode of the Caloris Basin is a large region of unusual hilly terrain known as the Weird Terrain One hypothesis for its origin is that shock waves generated during the Caloris impact traveled around Mercury converging at the basin s antipode 180 degrees away The resulting high stresses fractured the surface 68 Alternatively it has been suggested that this terrain formed as a result of the convergence of ejecta at this basin s antipode 69 Tolstoj basin is along the bottom of this image of Mercury s limb Overall 46 impact basins have been identified 70 A notable basin is the 400 km wide multi ring Tolstoj Basin that has an ejecta blanket extending up to 500 km from its rim and a floor that has been filled by smooth plains materials Beethoven Basin has a similar sized ejecta blanket and a 625 km diameter rim 65 Like the Moon the surface of Mercury has likely incurred the effects of space weathering processes including solar wind and micrometeorite impacts 71 Plains There are two geologically distinct plains regions on Mercury 65 72 Gently rolling hilly plains in the regions between craters are Mercury s oldest visible surfaces 65 predating the heavily cratered terrain These inter crater plains appear to have obliterated many earlier craters and show a general paucity of smaller craters below about 30 km in diameter 72 Smooth plains are widespread flat areas that fill depressions of various sizes and bear a strong resemblance to the lunar maria Unlike lunar maria the smooth plains of Mercury have the same albedo as the older inter crater plains Despite a lack of unequivocally volcanic characteristics the localisation and rounded lobate shape of these plains strongly support volcanic origins 65 All the smooth plains of Mercury formed significantly later than the Caloris basin as evidenced by appreciably smaller crater densities than on the Caloris ejecta blanket 65 Compressional features One unusual feature of Mercury s surface is the numerous compression folds or rupes that crisscross the plains These also exist on the moon but are much more prominent on Mercury 73 As Mercury s interior cooled it contracted and its surface began to deform creating wrinkle ridges and lobate scarps associated with thrust faults The scarps can reach lengths of 1000 km and heights of 3 km 74 These compressional features can be seen on top of other features such as craters and smooth plains indicating they are more recent 75 Mapping of the features has suggested a total shrinkage of Mercury s radius in the range of 1 to 7 km 76 Most activity along the major thrust systems probably ended about 3 6 3 7 billion years ago 77 Small scale thrust fault scarps have been found tens of meters in height and with lengths in the range of a few km that appear to be less than 50 million years old indicating that compression of the interior and consequent surface geological activity continue to the present 74 76 Volcanism Picasso crater the large arc shaped pit located on the eastern side of its floor are postulated to have formed when subsurface magma subsided or drained causing the surface to collapse into the resulting void There is evidence for pyroclastic flows on Mercury from low profile shield volcanoes 78 79 80 51 pyroclastic deposits have been identified 81 where 90 of them are found within impact craters 81 A study of the degradation state of the impact craters that host pyroclastic deposits suggests that pyroclastic activity occurred on Mercury over a prolonged interval 81 A rimless depression inside the southwest rim of the Caloris Basin consists of at least nine overlapping volcanic vents each individually up to 8 km in diameter It is thus a compound volcano 82 The vent floors are at least 1 km below their brinks and they bear a closer resemblance to volcanic craters sculpted by explosive eruptions or modified by collapse into void spaces created by magma withdrawal back down into a conduit 82 Scientists could not quantify the age of the volcanic complex system but reported that it could be on the order of a billion years 82 Surface conditions and exosphere Main article Atmosphere of Mercury Composite of the north pole of Mercury where NASA confirmed the discovery of a large volume of water ice in permanently dark craters that are found there 83 The surface temperature of Mercury ranges from 100 to 700 K 173 to 427 C 280 to 800 F 22 at the most extreme places 0 N 0 W or 180 W It never rises above 180 K at the poles 14 due to the absence of an atmosphere and a steep temperature gradient between the equator and the poles The subsolar point reaches about 700 K during perihelion 0 W or 180 W but only 550 K at aphelion 90 or 270 W 84 On the dark side of the planet temperatures average 110 K 14 85 The intensity of sunlight on Mercury s surface ranges between 4 59 and 10 61 times the solar constant 1 370 W m 2 86 Although the daylight temperature at the surface of Mercury is generally extremely high observations strongly suggest that ice frozen water exists on Mercury The floors of deep craters at the poles are never exposed to direct sunlight and temperatures there remain below 102 K far lower than the global average 87 This creates a cold trap where ice can accumulate Water ice strongly reflects radar and observations by the 70 meter Goldstone Solar System Radar and the VLA in the early 1990s revealed that there are patches of high radar reflection near the poles 88 Although ice was not the only possible cause of these reflective regions astronomers think it was the most likely 89 The icy regions are estimated to contain about 1014 1015 kg of ice 90 and may be covered by a layer of regolith that inhibits sublimation 91 By comparison the Antarctic ice sheet on Earth has a mass of about 4 1018 kg and Mars s south polar cap contains about 1016 kg of water 90 The origin of the ice on Mercury is not yet known but the two most likely sources are from outgassing of water from the planet s interior or deposition by impacts of comets 90 Mercury is too small and hot for its gravity to retain any significant atmosphere over long periods of time it does have a tenuous surface bounded exosphere 92 containing hydrogen helium oxygen sodium calcium potassium and others 16 17 at a surface pressure of less than approximately 0 5 nPa 0 005 picobars 3 This exosphere is not stable atoms are continuously lost and replenished from a variety of sources Hydrogen atoms and helium atoms probably come from the solar wind diffusing into Mercury s magnetosphere before later escaping back into space Radioactive decay of elements within Mercury s crust is another source of helium as well as sodium and potassium MESSENGER found high proportions of calcium helium hydroxide magnesium oxygen potassium silicon and sodium Water vapor is present released by a combination of processes such as comets striking its surface sputtering creating water out of hydrogen from the solar wind and oxygen from rock and sublimation from reservoirs of water ice in the permanently shadowed polar craters The detection of high amounts of water related ions like O OH and H3O was a surprise 93 94 Because of the quantities of these ions that were detected in Mercury s space environment scientists surmise that these molecules were blasted from the surface or exosphere by the solar wind 95 96 Sodium potassium and calcium were discovered in the atmosphere during the 1980 1990s and are thought to result primarily from the vaporization of surface rock struck by micrometeorite impacts 97 including presently from Comet Encke 98 In 2008 magnesium was discovered by MESSENGER 99 Studies indicate that at times sodium emissions are localized at points that correspond to the planet s magnetic poles This would indicate an interaction between the magnetosphere and the planet s surface 100 On November 29 2012 NASA confirmed that images from MESSENGER had detected that craters at the north pole contained water ice MESSENGER s principal investigator Sean Solomon is quoted in The New York Times estimating the volume of the ice to be large enough to encase Washington D C in a frozen block two and a half miles deep 83 According to NASA Mercury is not a suitable planet for Earth like life It has a surface boundary exosphere instead of a layered atmosphere extreme temperatures and high solar radiation It is unlikely that any living beings can withstand those conditions 101 Some parts of the subsurface of Mercury may have been habitable and perhaps life forms albeit likely primitive microorganisms may have existed on the planet 102 103 104 Magnetic field and magnetosphere Main article Mercury s magnetic field Graph showing relative strength of Mercury s magnetic field Despite its small size and slow 59 day long rotation Mercury has a significant and apparently global magnetic field According to measurements taken by Mariner 10 it is about 1 1 the strength of Earth s The magnetic field strength at Mercury s equator is about 300 nT 105 106 Like that of Earth Mercury s magnetic field is dipolar 100 Unlike Earth s Mercury s poles are nearly aligned with the planet s spin axis 107 Measurements from both the Mariner 10 and MESSENGER space probes have indicated that the strength and shape of the magnetic field are stable 107 It is likely that this magnetic field is generated by a dynamo effect in a manner similar to the magnetic field of Earth 108 109 This dynamo effect would result from the circulation of the planet s iron rich liquid core Particularly strong tidal heating effects caused by the planet s high orbital eccentricity would serve to keep part of the core in the liquid state necessary for this dynamo effect 40 110 Mercury s magnetic field is strong enough to deflect the solar wind around the planet creating a magnetosphere The planet s magnetosphere though small enough to fit within Earth 100 is strong enough to trap solar wind plasma This contributes to the space weathering of the planet s surface 107 Observations taken by the Mariner 10 spacecraft detected this low energy plasma in the magnetosphere of the planet s nightside Bursts of energetic particles in the planet s magnetotail indicate a dynamic quality to the planet s magnetosphere 100 During its second flyby of the planet on October 6 2008 MESSENGER discovered that Mercury s magnetic field can be extremely leaky The spacecraft encountered magnetic tornadoes twisted bundles of magnetic fields connecting the planetary magnetic field to interplanetary space that were up to 800 km wide or a third of the radius of the planet These twisted magnetic flux tubes technically known as flux transfer events form open windows in the planet s magnetic shield through which the solar wind may enter and directly impact Mercury s surface via magnetic reconnection 111 This also occurs in Earth s magnetic field The MESSENGER observations showed the reconnection rate is ten times higher at Mercury but its proximity to the Sun only accounts for about a third of the reconnection rate observed by MESSENGER 111 Orbit rotation and longitude Orbit of Mercury 2006 Animation of Mercury s and Earth s revolution around the Sun Mercury has the most eccentric orbit of all the planets in the Solar System its eccentricity is 0 21 with its distance from the Sun ranging from 46 000 000 to 70 000 000 km 29 000 000 to 43 000 000 mi It takes 87 969 Earth days to complete an orbit The diagram illustrates the effects of the eccentricity showing Mercury s orbit overlaid with a circular orbit having the same semi major axis Mercury s higher velocity when it is near perihelion is clear from the greater distance it covers in each 5 day interval In the diagram the varying distance of Mercury to the Sun is represented by the size of the planet which is inversely proportional to Mercury s distance from the Sun This varying distance to the Sun leads to Mercury s surface being flexed by tidal bulges raised by the Sun that are about 17 times stronger than the Moon s on Earth 112 Combined with a 3 2 spin orbit resonance of the planet s rotation around its axis it also results in complex variations of the surface temperature 32 The resonance makes a single solar day the length between two meridian transits of the Sun on Mercury last exactly two Mercury years or about 176 Earth days 113 Mercury s orbit is inclined by 7 degrees to the plane of Earth s orbit the ecliptic the largest of all eight known solar planets 114 As a result transits of Mercury across the face of the Sun can only occur when the planet is crossing the plane of the ecliptic at the time it lies between Earth and the Sun which is in May or November This occurs about every seven years on average 115 Mercury s axial tilt is almost zero 116 with the best measured value as low as 0 027 degrees 117 This is significantly smaller than that of Jupiter which has the second smallest axial tilt of all planets at 3 1 degrees This means that to an observer at Mercury s poles the center of the Sun never rises more than 2 1 arcminutes above the horizon 117 At certain points on Mercury s surface an observer would be able to see the Sun peek up a little more than two thirds of the way over the horizon then reverse and set before rising again all within the same Mercurian day c This is because approximately four Earth days before perihelion Mercury s angular orbital velocity equals its angular rotational velocity so that the Sun s apparent motion ceases closer to perihelion Mercury s angular orbital velocity then exceeds the angular rotational velocity Thus to a hypothetical observer on Mercury the Sun appears to move in a retrograde direction Four Earth days after perihelion the Sun s normal apparent motion resumes 32 A similar effect would have occurred if Mercury had been in synchronous rotation the alternating gain and loss of rotation over revolution would have caused a libration of 23 65 in longitude 118 For the same reason there are two points on Mercury s equator 180 degrees apart in longitude at either of which around perihelion in alternate Mercurian years once a Mercurian day the Sun passes overhead then reverses its apparent motion and passes overhead again then reverses a second time and passes overhead a third time taking a total of about 16 Earth days for this entire process In the other alternate Mercurian years the same thing happens at the other of these two points The amplitude of the retrograde motion is small so the overall effect is that for two or three weeks the Sun is almost stationary overhead and is at its most brilliant because Mercury is at perihelion its closest to the Sun This prolonged exposure to the Sun at its brightest makes these two points the hottest places on Mercury Maximum temperature occurs when the Sun is at an angle of about 25 degrees past noon due to diurnal temperature lag at 0 4 Mercury days and 0 8 Mercury years past sunrise 119 Conversely there are two other points on the equator 90 degrees of longitude apart from the first ones where the Sun passes overhead only when the planet is at aphelion in alternate years when the apparent motion of the Sun in Mercury s sky is relatively rapid These points which are the ones on the equator where the apparent retrograde motion of the Sun happens when it is crossing the horizon as described in the preceding paragraph receive much less solar heat than the first ones described above 120 Mercury attains inferior conjunction nearest approach to Earth every 116 Earth days on average 3 but this interval can range from 105 days to 129 days due to the planet s eccentric orbit Mercury can come as near as 82 200 000 km 0 549 astronomical units 51 1 million miles to Earth and that is slowly declining The next approach to within 82 100 000 km 51 million mi is in 2679 and to within 82 000 000 km 51 million mi in 4487 but it will not be closer to Earth than 80 000 000 km 50 million mi until 28 622 121 Its period of retrograde motion as seen from Earth can vary from 8 to 15 days on either side of inferior conjunction This large range arises from the planet s high orbital eccentricity 32 Essentially because Mercury is closest to the Sun when taking an average over time Mercury is most often the closest planet to the Earth 18 19 and in that measure it is the closest planet to each of the other planets in the Solar System 122 123 124 d Longitude convention The longitude convention for Mercury puts the zero of longitude at one of the two hottest points on the surface as described above However when this area was first visited by Mariner 10 this zero meridian was in darkness so it was impossible to select a feature on the surface to define the exact position of the meridian Therefore a small crater further west was chosen called Hun Kal which provides the exact reference point for measuring longitude 125 126 The center of Hun Kal defines the 20 west meridian A 1970 International Astronomical Union resolution suggests that longitudes be measured positively in the westerly direction on Mercury 127 The two hottest places on the equator are therefore at longitudes 0 W and 180 W and the coolest points on the equator are at longitudes 90 W and 270 W However the MESSENGER project uses an east positive convention 128 Spin orbit resonance After one orbit Mercury has rotated 1 5 times so after two complete orbits the same hemisphere is again illuminated For many years it was thought that Mercury was synchronously tidally locked with the Sun rotating once for each orbit and always keeping the same face directed towards the Sun in the same way that the same side of the Moon always faces Earth Radar observations in 1965 proved that the planet has a 3 2 spin orbit resonance rotating three times for every two revolutions around the Sun The eccentricity of Mercury s orbit makes this resonance stable at perihelion when the solar tide is strongest the Sun is nearly still in Mercury s sky 129 The rare 3 2 resonant tidal locking is stabilized by the variance of the tidal force along Mercury s eccentric orbit acting on a permanent dipole component of Mercury s mass distribution 130 In a circular orbit there is no such variance so the only resonance stabilized in such an orbit is at 1 1 e g Earth Moon when the tidal force stretching a body along the center body line exerts a torque that aligns the body s axis of least inertia the longest axis and the axis of the aforementioned dipole to point always at the center However with noticeable eccentricity like that of Mercury s orbit the tidal force has a maximum at perihelion and therefore stabilizes resonances like 3 2 ensuring that the planet points its axis of least inertia roughly at the Sun when passing through perihelion 130 The original reason astronomers thought it was synchronously locked was that whenever Mercury was best placed for observation it was always nearly at the same point in its 3 2 resonance hence showing the same face This is because coincidentally Mercury s rotation period is almost exactly half of its synodic period with respect to Earth Due to Mercury s 3 2 spin orbit resonance a solar day lasts about 176 Earth days 32 A sidereal day the period of rotation lasts about 58 7 Earth days 32 Simulations indicate that the orbital eccentricity of Mercury varies chaotically from nearly zero circular to more than 0 45 over millions of years due to perturbations from the other planets 32 131 This was thought to explain Mercury s 3 2 spin orbit resonance rather than the more usual 1 1 because this state is more likely to arise during a period of high eccentricity 132 However accurate modeling based on a realistic model of tidal response has demonstrated that Mercury was captured into the 3 2 spin orbit state at a very early stage of its history within 20 more likely 10 million years after its formation 133 Numerical simulations show that a future secular orbital resonant perihelion interaction with Jupiter may cause the eccentricity of Mercury s orbit to increase to the point where there is a 1 chance that the orbit will be destabilized in the next five billion years If this happens Mercury may fall into the Sun collide with Venus be ejected from the Solar System or even disrupt the rest of the inner Solar System 134 135 Advance of perihelion Main article Perihelion precession of Mercury In 1859 the French mathematician and astronomer Urbain Le Verrier reported that the slow precession of Mercury s orbit around the Sun could not be completely explained by Newtonian mechanics and perturbations by the known planets He suggested among possible explanations that another planet or perhaps instead a series of smaller corpuscules might exist in an orbit even closer to the Sun than that of Mercury to account for this perturbation 136 Other explanations considered included a slight oblateness of the Sun The success of the search for Neptune based on its perturbations of the orbit of Uranus led astronomers to place faith in this possible explanation and the hypothetical planet was named Vulcan but no such planet was ever found 137 The observed perihelion precession of Mercury is 5 600 arcseconds 1 5556 per century relative to Earth or 574 10 0 65 arcseconds per century 138 relative to the inertial ICRF Newtonian mechanics taking into account all the effects from the other planets included 0 0254 arcsecond per century due to the flatteness of the Sun predicts a precession of 5 557 arcseconds 1 5436 per century relative to Earth or 531 63 0 69 arcseconds per century relative to ICRF 138 In the early 20th century Albert Einstein s general theory of relativity provided the explanation for the observed precession by formalizing gravitation as being mediated by the curvature of spacetime The effect is small just 42 98 arcseconds per century or 0 43 arcsecond per year or 0 1038 arcsecond per orbital period for Mercury it therefore requires a little over twelve million orbits or 2 8 million years for a full excess turn Similar but much smaller effects exist for other Solar System bodies 8 62 arcseconds per century for Venus 3 84 for Earth 1 35 for Mars and 10 05 for 1566 Icarus 139 140 Observation Image mosaic by Mariner 10 1974 Mercury s apparent magnitude is calculated to vary between 2 48 brighter than Sirius around superior conjunction and 7 25 below the limit of naked eye visibility around inferior conjunction 15 The mean apparent magnitude is 0 23 while the standard deviation of 1 78 is the largest of any planet The mean apparent magnitude at superior conjunction is 1 89 while that at inferior conjunction is 5 93 15 Observation of Mercury is complicated by its proximity to the Sun as it is lost in the Sun s glare for much of the time Mercury can be observed for only a brief period during either morning or evening twilight 141 But in some cases Mercury can better be observed in daylight with a telescope when the position is known because it is higher in the sky and less atmospheric effects affect the view of the planet When proper safety precautions are taken to prevent inadvertently pointing the telescope at the Sun and thus blinding the user Mercury can be viewed as close as 4 to the Sun when near superior conjunction when it is almost at its brightest Mercury can like several other planets and the brightest stars be seen during a total solar eclipse 142 Like the Moon and Venus Mercury exhibits phases as seen from Earth It is new at inferior conjunction and full at superior conjunction The planet is rendered invisible from Earth on both of these occasions because of its being obscured by the Sun 141 except its new phase during a transit Mercury is technically brightest as seen from Earth when it is at a full phase Although Mercury is farthest from Earth when it is full the greater illuminated area that is visible and the opposition brightness surge more than compensates for the distance 143 The opposite is true for Venus which appears brightest when it is a crescent because it is much closer to Earth than when gibbous 143 144 False color map showing the maximum temperatures of the north polar region Nonetheless the brightest full phase appearance of Mercury is an essentially impossible time for practical observation because of the extreme proximity of the Sun Mercury is best observed at the first and last quarter although they are phases of lesser brightness The first and last quarter phases occur at greatest elongation east and west of the Sun respectively At both of these times Mercury s separation from the Sun ranges anywhere from 17 9 at perihelion to 27 8 at aphelion 145 146 At greatest western elongation Mercury rises at its earliest before sunrise and at greatest eastern elongation it sets at its latest after sunset 147 False color image of Carnegie Rupes a tectonic landform high terrain red low blue Mercury is more often and easily visible from the Southern Hemisphere than from the Northern This is because Mercury s maximum western elongation occurs only during early autumn in the Southern Hemisphere whereas its greatest eastern elongation happens only during late winter in the Southern Hemisphere 147 In both of these cases the angle at which the planet s orbit intersects the horizon is maximized allowing it to rise several hours before sunrise in the former instance and not set until several hours after sundown in the latter from southern mid latitudes such as Argentina and South Africa 147 An alternate method for viewing Mercury involves observing the planet during daylight hours when conditions are clear ideally when it is at its greatest elongation This allows the planet to be found easily even when using telescopes with 8 cm 3 1 in apertures However great care must be taken to obstruct the Sun from sight because of the extreme risk for eye damage 148 This method bypasses the limitation of twilight observing when the ecliptic is located at a low elevation e g on autumn evenings Ground based telescope observations of Mercury reveal only an illuminated partial disk with limited detail The first of two spacecraft to visit the planet was Mariner 10 which mapped about 45 of its surface from 1974 to 1975 The second is the MESSENGER spacecraft which after three Mercury flybys between 2008 and 2009 attained orbit around Mercury on March 17 2011 149 to study and map the rest of the planet 150 The Hubble Space Telescope cannot observe Mercury at all due to safety procedures that prevent its pointing too close to the Sun 151 Because the shift of 0 15 revolutions in a year makes up a seven year cycle 0 15 7 1 0 in the seventh year Mercury follows almost exactly earlier by 7 days the sequence of phenomena it showed seven years before 145 Observation historyAncient astronomers Mercury from Liber astronomiae 1550 The earliest known recorded observations of Mercury are from the MUL APIN tablets These observations were most likely made by an Assyrian astronomer around the 14th century BC 152 The cuneiform name used to designate Mercury on the MUL APIN tablets is transcribed as UDU IDIM GU U4 UD the jumping planet e 153 Babylonian records of Mercury date back to the 1st millennium BC The Babylonians called the planet Nabu after the messenger to the gods in their mythology 154 The Greco Egyptian 155 astronomer Ptolemy wrote about the possibility of planetary transits across the face of the Sun in his work Planetary Hypotheses He suggested that no transits had been observed either because planets such as Mercury were too small to see or because the transits were too infrequent 156 Ibn al Shatir s model for the appearances of Mercury showing the multiplication of epicycles using the Tusi couple thus eliminating the Ptolemaic eccentrics and equant In ancient China Mercury was known as the Hour Star Chen xing 辰星 It was associated with the direction north and the phase of water in the Five Phases system of metaphysics 157 Modern Chinese Korean Japanese and Vietnamese cultures refer to the planet literally as the water star 水星 based on the Five elements 158 159 160 Hindu mythology used the name Budha for Mercury and this god was thought to preside over Wednesday 161 The god Odin or Woden of Germanic paganism was associated with the planet Mercury and Wednesday 162 The Maya may have represented Mercury as an owl or possibly four owls two for the morning aspect and two for the evening that served as a messenger to the underworld 163 In medieval Islamic astronomy the Andalusian astronomer Abu Ishaq Ibrahim al Zarqali in the 11th century described the deferent of Mercury s geocentric orbit as being oval like an egg or a pignon although this insight did not influence his astronomical theory or his astronomical calculations 164 165 In the 12th century Ibn Bajjah observed two planets as black spots on the face of the Sun which was later suggested as the transit of Mercury and or Venus by the Maragha astronomer Qotb al Din Shirazi in the 13th century 166 Note that most such medieval reports of transits were later taken as observations of sunspots 167 In India the Kerala school astronomer Nilakantha Somayaji in the 15th century developed a partially heliocentric planetary model in which Mercury orbits the Sun which in turn orbits Earth similar to the Tychonic system later proposed by Tycho Brahe in the late 16th century 168 Ground based telescopic research Transit of Mercury Mercury is visible as a black dot below and to the left of center The dark area above the center of the solar disk is a sunspot Elongation is the angle between the Sun and the planet with Earth as the reference point Mercury appears close to the Sun The first telescopic observations of Mercury were made by Thomas Harriot and Galileo from 1610 In 1612 Simon Marius observed the brightness of Mercury varied with the planet s orbital position and concluded it had phases in the same way as Venus and the Moon 169 In 1631 Pierre Gassendi made the first telescopic observations of the transit of a planet across the Sun when he saw a transit of Mercury predicted by Johannes Kepler In 1639 Giovanni Zupi used a telescope to discover that the planet had orbital phases similar to Venus and the Moon The observation demonstrated conclusively that Mercury orbited around the Sun 32 A rare event in astronomy is the passage of one planet in front of another occultation as seen from Earth Mercury and Venus occult each other every few centuries and the event of May 28 1737 is the only one historically observed having been seen by John Bevis at the Royal Greenwich Observatory 170 The next occultation of Mercury by Venus will be on December 3 2133 171 The difficulties inherent in observing Mercury mean that it was far less studied than the other planets In 1800 Johann Schroter made observations of surface features claiming to have observed 20 kilometre high 12 mi mountains Friedrich Bessel used Schroter s drawings to erroneously estimate the rotation period as 24 hours and an axial tilt of 70 172 In the 1880s Giovanni Schiaparelli mapped the planet more accurately and suggested that Mercury s rotational period was 88 days the same as its orbital period due to tidal locking 173 This phenomenon is known as synchronous rotation The effort to map the surface of Mercury was continued by Eugenios Antoniadi who published a book in 1934 that included both maps and his own observations 100 Many of the planet s surface features particularly the albedo features take their names from Antoniadi s map 174 In June 1962 Soviet scientists at the Institute of Radio engineering and Electronics of the USSR Academy of Sciences led by Vladimir Kotelnikov became the first to bounce a radar signal off Mercury and receive it starting radar observations of the planet 175 176 177 Three years later radar observations by Americans Gordon H Pettengill and Rolf B Dyce using the 300 meter Arecibo radio telescope in Puerto Rico showed conclusively that the planet s rotational period was about 59 days 178 179 The theory that Mercury s rotation was synchronous had become widely held and it was a surprise to astronomers when these radio observations were announced If Mercury were tidally locked its dark face would be extremely cold but measurements of radio emission revealed that it was much hotter than expected Astronomers were reluctant to drop the synchronous rotation theory and proposed alternative mechanisms such as powerful heat distributing winds to explain the observations 180 Water ice yellow at Mercury s north polar region Italian astronomer Giuseppe Colombo noted that the rotation value was about two thirds of Mercury s orbital period and proposed that the planet s orbital and rotational periods were locked into a 3 2 rather than a 1 1 resonance 181 Data from Mariner 10 subsequently confirmed this view 182 This means that Schiaparelli s and Antoniadi s maps were not wrong Instead the astronomers saw the same features during every second orbit and recorded them but disregarded those seen in the meantime when Mercury s other face was toward the Sun because the orbital geometry meant that these observations were made under poor viewing conditions 172 Ground based optical observations did not shed much further light on Mercury but radio astronomers using interferometry at microwave wavelengths a technique that enables removal of the solar radiation were able to discern physical and chemical characteristics of the subsurface layers to a depth of several meters 183 184 Not until the first space probe flew past Mercury did many of its most fundamental morphological properties become known Moreover recent technological advances have led to improved ground based observations In 2000 high resolution lucky imaging observations were conducted by the Mount Wilson Observatory 1 5 meter Hale telescope They provided the first views that resolved surface features on the parts of Mercury that were not imaged in the Mariner 10 mission 185 Most of the planet has been mapped by the Arecibo radar telescope with 5 km 3 1 mi resolution including polar deposits in shadowed craters of what may be water ice 186 Research with space probes Main article Exploration of Mercury MESSENGER being prepared for launch Mercury transiting the Sun as viewed by the Mars rover Curiosity June 3 2014 187 Reaching Mercury from Earth poses significant technical challenges because it orbits so much closer to the Sun than Earth A Mercury bound spacecraft launched from Earth must travel over 91 million kilometres 57 million miles into the Sun s gravitational potential well Mercury has an orbital speed of 47 4 km s 29 5 mi s whereas Earth s orbital speed is 29 8 km s 18 5 mi s 114 Therefore the spacecraft must make a large change in velocity delta v to get to Mercury and then enter orbit 188 as compared to the delta v required for say Mars planetary missions The potential energy liberated by moving down the Sun s potential well becomes kinetic energy requiring a delta v change to do anything other than pass by Mercury Some portion of this delta v budget can be provided from a gravity assist during one or more fly bys of Venus 189 To land safely or enter a stable orbit the spacecraft would rely entirely on rocket motors Aerobraking is ruled out because Mercury has a negligible atmosphere A trip to Mercury requires more rocket fuel than that required to escape the Solar System completely As a result only three space probes have visited it so far 190 A proposed alternative approach would use a solar sail to attain a Mercury synchronous orbit around the Sun 191 Mariner 10 Main article Mariner 10 Mariner 10 the first probe to visit Mercury The first spacecraft to visit Mercury was NASA s Mariner 10 1974 1975 26 The spacecraft used the gravity of Venus to adjust its orbital velocity so that it could approach Mercury making it both the first spacecraft to use this gravitational slingshot effect and the first NASA mission to visit multiple planets 192 Mariner 10 provided the first close up images of Mercury s surface which immediately showed its heavily cratered nature and revealed many other types of geological features such as the giant scarps that were later ascribed to the effect of the planet shrinking slightly as its iron core cools 193 Unfortunately the same face of the planet was lit at each of Mariner 10 s close approaches This made close observation of both sides of the planet impossible 194 and resulted in the mapping of less than 45 of the planet s surface 195 The spacecraft made three close approaches to Mercury the closest of which took it to within 327 km 203 mi of the surface 196 At the first close approach instruments detected a magnetic field to the great surprise of planetary geologists Mercury s rotation was expected to be much too slow to generate a significant dynamo effect The second close approach was primarily used for imaging but at the third approach extensive magnetic data were obtained The data revealed that the planet s magnetic field is much like Earth s which deflects the solar wind around the planet For many years after the Mariner 10 encounters the origin of Mercury s magnetic field remained the subject of several competing theories 197 198 On March 24 1975 just eight days after its final close approach Mariner 10 ran out of fuel Because its orbit could no longer be accurately controlled mission controllers instructed the probe to shut down 199 Mariner 10 is thought to be still orbiting the Sun passing close to Mercury every few months 200 MESSENGER Main article MESSENGER Estimated details of the impact of MESSENGER on April 30 2015 A second NASA mission to Mercury named MESSENGER MErcury Surface Space ENvironment GEochemistry and Ranging was launched on August 3 2004 It made a fly by of Earth in August 2005 and of Venus in October 2006 and June 2007 to place it onto the correct trajectory to reach an orbit around Mercury 201 A first fly by of Mercury occurred on January 14 2008 a second on October 6 2008 202 and a third on September 29 2009 203 Most of the hemisphere not imaged by Mariner 10 was mapped during these fly bys The probe successfully entered an elliptical orbit around the planet on March 18 2011 The first orbital image of Mercury was obtained on March 29 2011 The probe finished a one year mapping mission 202 and then entered a one year extended mission into 2013 In addition to continued observations and mapping of Mercury MESSENGER observed the 2012 solar maximum 204 The mission was designed to clear up six key issues Mercury s high density its geological history the nature of its magnetic field the structure of its core whether it has ice at its poles and where its tenuous atmosphere comes from To this end the probe carried imaging devices that gathered much higher resolution images of much more of Mercury than Mariner 10 assorted spectrometers to determine abundances of elements in the crust and magnetometers and devices to measure velocities of charged particles Measurements of changes in the probe s orbital velocity were expected to be used to infer details of the planet s interior structure 205 MESSENGER s final maneuver was on April 24 2015 and it crashed into Mercury s surface on April 30 2015 206 207 208 The spacecraft s impact with Mercury occurred near 3 26 pm EDT on April 30 2015 leaving a crater estimated to be 16 m 52 ft in diameter 209 BepiColombo Main article BepiColombo The European Space Agency and the Japanese Space Agency developed and launched a joint mission called BepiColombo which will orbit Mercury with two probes one to map the planet and the other to study its magnetosphere 210 Launched on October 20 2018 BepiColombo is expected to reach Mercury in 2025 211 It will release a magnetometer probe into an elliptical orbit then chemical rockets will fire to deposit the mapper probe into a circular orbit Both probes will operate for one terrestrial year 210 The mapper probe carries an array of spectrometers similar to those on MESSENGER and will study the planet at many different wavelengths including infrared ultraviolet X ray and gamma ray 212 BepiColombo conducted the first of its six planned Mercury flybys on October 1 2021 213 See also Solar System portal Outer space portal Astronomy portalOutline of Mercury planet Budha a deity identified with the planet in Hindu astrology Colonization of Mercury Mercury in astrology Mercury in fictionNotes In astronomy the words rotation and revolution have different meanings Rotation is the turning of a body about an axis that passes through the body as in Earth rotates once a day Revolution is motion around a centre that is external to the body usually in orbit as in Earth takes a year for each revolution around the Sun The verbs rotate and revolve mean doing rotation and revolution respectively Pluto was considered a planet from its discovery in 1930 to 2006 but after that it has been reclassified as a dwarf planet Pluto s orbital eccentricity is greater than Mercury s Pluto is also smaller than Mercury but was thought to be larger until 1976 The Sun s total angular displacement during its apparent retrograde motion as seen from the surface of Mercury is 1 23 while the Sun s angular diameter when the apparent retrograde motion begins and ends is 1 71 increasing to 1 73 at perihelion midway through the retrograde motion It is important to be clear about the meaning of closeness In the astronomical literature the term closest planets often means the two planets that approach each other most closely In other words the orbits of the two planets approach each other most closely However this does not mean that the two planets are closest over time For example essentially because Mercury is closer to the Sun than Venus Mercury spends more time in proximity to Earth it could therefore be said that Mercury is the planet that is closest to Earth when averaged over time However using this time average definition of closeness as noted above it turns out that Mercury is the closest planet to all other planets in the solar system For that reason arguably the proximity definition is not particularly helpful An episode of the BBC Radio 4 programme More or Less explains the different notions of proximity well 19 Some sources precede the cuneiform transcription with MUL MUL is a cuneiform sign that was used in the Sumerian language to designate a star or planet but it is not considered part of the actual name The 4 is a reference number in the Sumero Akkadian transliteration system to designate which of several syllables a certain cuneiform sign is most likely designating References Mercurian Lexico UK English Dictionary Oxford University Press Archived from the original on March 27 2020 Mercurial Lexico UK English Dictionary UK English Dictionary Oxford University Press Archived from the original on December 22 2019 a b c d e f g h i j k l m Williams David R November 25 2020 Mercury Fact Sheet NASA Retrieved April 19 2021 Souami D Souchay J July 2012 The solar system s invariable plane Astronomy amp Astrophysics 543 11 Bibcode 2012A amp A 543A 133S doi 10 1051 0004 6361 201219011 A133 Yeomans Donald K April 7 2008 HORIZONS Web Interface for Mercury Major Body JPL Horizons On Line Ephemeris System Retrieved April 7 2008 Select Ephemeris Type Orbital Elements Time Span 2000 01 01 12 00 to 2000 01 02 Target Body Mercury and Center Sun should be defaulted to Results are instantaneous osculating values at the precise J2000 epoch a b c d e f g Davis Phillips Barnett Amanda February 15 2021 Mercury Solar System Exploration NASA Jet Propulsion Laboratory Retrieved April 21 2021 Seidelmann P Kenneth Archinal Brent A A Hearn Michael F et al 2007 Report of the IAU IAG Working Group on cartographic coordinates and rotational elements 2006 Celestial Mechanics and Dynamical Astronomy 98 3 155 180 Bibcode 2007CeMDA 98 155S doi 10 1007 s10569 007 9072 y S2CID 122772353 Mazarico Erwan Genova Antonio Goossens Sander Lemoine Frank G Neumann Gregory A Zuber Maria T Smith David E Solomon Sean C 2014 The gravity field orientation and ephemeris of Mercury from MESSENGER observations after three years in orbit PDF Journal of Geophysical Research Planets 119 12 2417 2436 Bibcode 2014JGRE 119 2417M doi 10 1002 2014JE004675 hdl 1721 1 97927 ISSN 2169 9097 S2CID 42430050 a b c Margot Jean Luc Peale Stanton J Solomon Sean C Hauck Steven A Ghigo Frank D Jurgens Raymond F Yseboodt Marie Giorgini Jon D Padovan Sebastiano Campbell Donald B 2012 Mercury s moment of inertia from spin and gravity data Journal of Geophysical Research Planets 117 E12 n a Bibcode 2012JGRE 117 0L09M CiteSeerX 10 1 1 676 5383 doi 10 1029 2012JE004161 ISSN 0148 0227 S2CID 22408219 ESO ESO Retrieved June 3 2021 Mallama Anthony 2017 The spherical bolometric albedo for planet Mercury arXiv 1703 02670 astro ph EP Mallama Anthony Wang Dennis Howard Russell A 2002 Photometry of Mercury from SOHO LASCO and Earth Icarus 155 2 253 264 Bibcode 2002Icar 155 253M doi 10 1006 icar 2001 6723 Atmospheres and Planetary Temperatures American Chemical Society July 18 2013 Retrieved January 3 2023 a b c d Vasavada Ashwin R Paige David A Wood Stephen E February 19 1999 Near Surface Temperatures on Mercury and the Moon and the Stability of Polar Ice Deposits PDF Icarus 141 2 179 193 Bibcode 1999Icar 141 179V doi 10 1006 icar 1999 6175 Figure 3 with the TWO model Figure 5 for pole a b c Mallama Anthony Hilton James L October 2018 Computing apparent planetary magnitudes for The Astronomical Almanac Astronomy and Computing 25 10 24 arXiv 1808 01973 Bibcode 2018A amp C 25 10M doi 10 1016 j ascom 2018 08 002 S2CID 69912809 a b Milillo A Wurz P Orsini S Delcourt D Kallio E Killen R M Lammer H Massetti S Mura A Barabash S Cremonese G Daglis I A Angelis E Lellis A M Livi S Mangano V Torkar K April 2005 Surface Exosphere Magnetosphere System Of Mercury Space Science Reviews 117 3 4 397 443 Bibcode 2005SSRv 117 397M doi 10 1007 s11214 005 3593 z S2CID 122285073 a b Berezhnoy Alexey A January 2018 Chemistry of impact events on Mercury Icarus 300 210 222 Bibcode 2018Icar 300 210B doi 10 1016 j icarus 2017 08 034 a b Venus is not Earth s closest neighbor Physics Today AIP Publishing March 12 2019 doi 10 1063 pt 6 3 20190312a ISSN 1945 0699 S2CID 241077611 a b c Harford Tim January 11 2019 BBC Radio 4 More or Less Sugar Outdoors Play and Planets BBC Oliver Hawkins more or less alumnus and statistical legend wrote some code for us which calculated which planet was closest to the Earth on each day for the past 50 years and then sent the results to David A Rothery professor of planetary geosciences at the Open University Elkins Tanton Linda T 2006 Uranus Neptune Pluto and the Outer Solar System Infobase Publishing p 51 ISBN 978 1 4381 0729 5 Extract of page 51 Animated clip of orbit and rotation of Mercury Sciencenetlinks com a b Prockter Louise 2005 Ice in the Solar System PDF Vol 26 Johns Hopkins APL Technical Digest Retrieved July 27 2009 NASA Completes MESSENGER Mission with Expected Impact on Mercury s Surface Archived from the original on May 3 2015 Retrieved April 30 2015 From Mercury orbit MESSENGER watches a lunar eclipse Planetary Society October 10 2014 Retrieved January 23 2015 Innovative use of pressurant extends MESSENGER s Mercury mission Astronomy com December 29 2014 Retrieved January 22 2015 a b c Dunne James A Burgess Eric 1978 Chapter One The Voyage of Mariner 10 Mission to Venus and Mercury NASA History Office Stilbwn Ἑrmῆs Liddell Henry George Scott Robert A Greek English Lexicon at the Perseus Project Greek Names of the Planets April 25 2010 Retrieved July 14 2012 Ermis is the Greek name of the planet Mercury which is the closest planet to the Sun It is named after the Greek God of commerce Ermis or Hermes who was also the messenger of the Ancient Greek gods See also the Greek article about the planet Antoniadi Eugene Michel 1974 The Planet Mercury Translated from French by Moore Patrick Shaldon Devon Keith Reid Ltd pp 9 11 ISBN 978 0 904094 02 2 Duncan John Charles 1946 Astronomy A Textbook Harper amp Brothers p 125 The symbol for Mercury represents the Caduceus a wand with two serpents twined around it which was carried by the messenger of the gods Jones Alexander 1999 Astronomical papyri from Oxyrhynchus pp 62 63 ISBN 9780871692337 It is now possible to trace the medieval symbols for at least four of the five planets to forms that occur in some of the latest papyrus horoscopes P Oxy 4272 4274 4275 Mercury s is a stylized caduceus a b c d e f g h Strom Robert G Sprague Ann L 2003 Exploring Mercury the iron planet Springer ISBN 978 1 85233 731 5 Talbert Tricia ed March 21 2012 MESSENGER Provides New Look at Mercury s Surprising Core and Landscape Curiosities NASA Scientists find evidence Mercury has a solid inner core AGU Newsroom Retrieved April 17 2019 Mercury US Geological Survey May 8 2003 Archived from the original on September 29 2006 Retrieved November 26 2006 Lyttleton Raymond A 1969 On the Internal Structures of Mercury and Venus Astrophysics and Space Science 5 1 18 35 Bibcode 1969Ap amp SS 5 18L doi 10 1007 BF00653933 S2CID 122572625 Hauck Steven A Margot Jean Luc Solomon Sean C Phillips Roger J Johnson Catherine L Lemoine Frank G Mazarico Erwan McCoy Timothy J Padovan Sebastiano Peale Stanton J Perry Mark E Smith David E Zuber Maria T 2013 The curious case of Mercury s internal structure Journal of Geophysical Research Planets 118 6 1204 1220 Bibcode 2013JGRE 118 1204H doi 10 1002 jgre 20091 hdl 1721 1 85633 S2CID 17668886 Gold Lauren May 3 2007 Mercury has molten core Cornell researcher shows Chronicle Cornell University Retrieved May 12 2008 Finley Dave May 3 2007 Mercury s Core Molten Radar Study Shows National Radio Astronomy Observatory Retrieved May 12 2008 a b Spohn Tilman Sohl Frank Wieczerkowski Karin Conzelmann Vera 2001 The interior structure of Mercury what we know what we expect from BepiColombo Planetary and Space Science 49 14 15 1561 1570 Bibcode 2001P amp SS 49 1561S doi 10 1016 S0032 0633 01 00093 9 Gallant Roy A 1986 The National Geographic Picture Atlas of Our Universe 2nd ed National Geographic Society ISBN 9780870446443 Padovan Sebastiano Wieczorek Mark A Margot Jean Luc Tosi Nicola Solomon Sean C 2015 Thickness of the crust of Mercury from geoid to topography ratios Geophysical Research Letters 42 4 1029 Bibcode 2015GeoRL 42 1029P doi 10 1002 2014GL062487 S2CID 31442257 Solomon Sean C Nittler Larry R Anderson Brian J December 20 2018 Mercury The View after MESSENGER Cambridge University Press p 534 ISBN 978 1 107 15445 2 Sori Michael M May 2018 A thin dense crust for Mercury Earth and Planetary Science Letters 489 92 99 Bibcode 2018E amp PSL 489 92S doi 10 1016 j epsl 2018 02 033 Schenk Paul M Melosh H Jay March 1994 Lobate Thrust Scarps and the Thickness of Mercury s Lithosphere Abstracts of the 25th Lunar and Planetary Science Conference 1994 1994LPI 25 1203S Bibcode 1994LPI 25 1203S Watters T R Nimmo F Robinson M S 2004 Chronology of Lobate Scarp Thrust Faults and the Mechanical Structure of Mercury s Lithosphere Lunar and Planetary Science Conference p 1886 Bibcode 2004LPI 35 1886W Watters Thomas R Robinson Mark S Cook Anthony C November 1998 Topography of lobate scarps on Mercury new constraints on the planet s contraction Geology 26 11 991 994 Bibcode 1998Geo 26 991W doi 10 1130 0091 7613 1998 026 lt 0991 TOLSOM gt 2 3 CO 2 a b c d Benz W Slattery W L Cameron Alastair G W 1988 Collisional stripping of Mercury s mantle Icarus 74 3 516 528 Bibcode 1988Icar 74 516B doi 10 1016 0019 1035 88 90118 2 a b Cameron Alastair G W 1985 The partial volatilization of Mercury Icarus 64 2 285 294 Bibcode 1985Icar 64 285C doi 10 1016 0019 1035 85 90091 0 Weidenschilling Stuart J 1987 Iron silicate fractionation and the origin of Mercury Icarus 35 1 99 111 Bibcode 1978Icar 35 99W doi 10 1016 0019 1035 78 90064 7 Sappenfield Mark September 29 2011 Messenger s message from Mercury Time to rewrite the textbooks The Christian Science Monitor Retrieved August 21 2017 BepiColombo Science amp Technology European Space Agency Retrieved April 7 2008 Cartwright Jon September 30 2011 Messenger sheds light on Mercury s formation Chemistry World Retrieved August 21 2017 Morris Jefferson November 10 2008 Laser Altimetry Aviation Week amp Space Technology 169 18 18 Mercury s crust is more analogous to a marbled cake than a layered cake Hughes E T Vaughan W M March 2012 Albedo Features of Mercury 43rd Lunar and Planetary Science Conference held March 19 23 2012 at The Woodlands Texas Vol 1659 Bibcode 2012LPI 43 2151H 2151 Blue Jennifer April 11 2008 Gazetteer of Planetary Nomenclature US Geological Survey Retrieved April 11 2008 a b Dunne James A Burgess Eric 1978 Chapter Seven The Voyage of Mariner 10 Mission to Venus and Mercury NASA History Office Retrieved May 28 2008 Nittler Larry R Weider Shoshana Z 2019 The Surface Composition of Mercury Elements 15 1 33 38 doi 10 2138 gselements 15 1 33 S2CID 135051680 Categories for Naming Features on Planets and Satellites US Geological Survey Retrieved August 20 2011 Strom Robert G 1979 Mercury a post Mariner assessment Space Science Reviews 24 1 3 70 Bibcode 1979SSRv 24 3S doi 10 1007 BF00221842 S2CID 122563809 Broadfoot A Lyle Kumar Shailendra Belton Michael J S McElroy Michael B July 12 1974 Mercury s Atmosphere from Mariner 10 Preliminary Results Science 185 4146 166 169 Bibcode 1974Sci 185 166B doi 10 1126 science 185 4146 166 PMID 17810510 S2CID 7790470 Geology of the solar system IMAP 2596 U S Geological Survey 1997 doi 10 3133 i2596 Head James W Solomon Sean C 1981 Tectonic Evolution of the Terrestrial Planets PDF Science 213 4503 62 76 Bibcode 1981Sci 213 62H CiteSeerX 10 1 1 715 4402 doi 10 1126 science 213 4503 62 hdl 2060 20020090713 PMID 17741171 Archived from the original PDF on July 21 2018 Retrieved October 25 2017 Scientists see Mercury in a new light Science Daily February 28 2008 Retrieved April 7 2008 a b c d e f g Spudis Paul D 2001 The Geological History of Mercury Workshop on Mercury Space Environment Surface and Interior Chicago 1097 100 Bibcode 2001mses conf 100S Ritzel Rebecca December 20 2012 Ballet isn t rocket science but the two aren t mutually exclusive either The Washington Post Washington D C United States Retrieved December 22 2012 Shiga David January 30 2008 Bizarre spider scar found on Mercury s surface NewScientist com news service Schultz Peter H Gault Donald E 1975 Seismic effects from major basin formations on the moon and Mercury Earth Moon and Planets 12 2 159 175 Bibcode 1975Moon 12 159S doi 10 1007 BF00577875 S2CID 121225801 Wieczorek Mark A Zuber Maria T 2001 A Serenitatis origin for the Imbrian grooves and South Pole Aitken thorium anomaly Journal of Geophysical Research 106 E11 27853 27864 Bibcode 2001JGR 10627853W doi 10 1029 2000JE001384 Retrieved May 12 2008 Fassett Caleb I Head James W Baker David M H Zuber Maria T Smith David E Neumann Gregory A Solomon Sean C Klimczak Christian Strom Robert G Chapman Clark R Prockter Louise M Phillips Roger J Oberst Jurgen Preusker Frank October 2012 Large impact basins on Mercury Global distribution characteristics and modification history from MESSENGER orbital data Journal of Geophysical Research 117 15 pp Bibcode 2012JGRE 117 0L08F doi 10 1029 2012JE004154 E00L08 Denevi Brett W Robinson Mark S 2008 Albedo of Immature Mercurian Crustal Materials Evidence for the Presence of Ferrous Iron Lunar and Planetary Science 39 1391 1750 Bibcode 2008LPI 39 1750D a b Wagner Roland J Wolf Ursula Ivanov Boris A Neukum Gerhard October 4 5 2001 Application of an Updated Impact Cratering Chronology Model to Mercury s Time Stratigraphic System Workshop on Mercury Space Environment Surface and Interior Proceedings of a workshop held at The Field Museum Chicago IL Lunar and Planetary Science Institute p 106 Bibcode 2001mses conf 106W Schleicher Lisa S Watters Thomas R Martin Aaron J Banks Maria E October 2019 Wrinkle ridges on Mercury and the Moon within and outside of mascons Icarus 331 226 237 Bibcode 2019Icar 331 226S doi 10 1016 j icarus 2019 04 013 S2CID 150072193 a b Choi Charles Q September 26 2016 Mercuryquakes May Currently Shake Up the Tiny Planet Space com Retrieved September 28 2016 Dzurisin Daniel October 10 1978 The tectonic and volcanic history of Mercury as inferred from studies of scarps ridges troughs and other lineaments Journal of Geophysical Research 83 B10 4883 4906 Bibcode 1978JGR 83 4883D doi 10 1029 JB083iB10p04883 a b Watters Thomas R Daud Katie Banks Maria E Selvans Michelle M Chapman Clark R Ernst Carolyn M September 26 2016 Recent tectonic activity on Mercury revealed by small thrust fault scarps Nature Geoscience 9 10 743 747 Bibcode 2016NatGe 9 743W doi 10 1038 ngeo2814 Giacomini L Massironi M Galluzzi V Ferrari S Palumbo P May 2020 Dating long thrust systems on Mercury New clues on the thermal evolution of the planet Geoscience Frontiers 11 3 855 870 doi 10 1016 j gsf 2019 09 005 S2CID 210298205 Kerber Laura Head James W Solomon Sean C Murchie Scott L Blewett David T August 15 2009 Explosive volcanic eruptions on Mercury Eruption conditions magma volatile content and implications for interior volatile abundances Earth and Planetary Science Letters 285 3 4 263 271 Bibcode 2009E amp PSL 285 263K doi 10 1016 j epsl 2009 04 037 Head James W Chapman Clark R Strom Robert G Fassett Caleb I Denevi Brett W September 30 2011 Flood Volcanism in the Northern High Latitudes of Mercury Revealed by MESSENGER PDF Science 333 6051 1853 1856 Bibcode 2011Sci 333 1853H doi 10 1126 science 1211997 PMID 21960625 S2CID 7651992 Thomas Rebecca J Rothery David A Conway Susan J Anand Mahesh September 16 2014 Long lived explosive volcanism on Mercury Geophysical Research Letters 41 17 6084 6092 Bibcode 2014GeoRL 41 6084T doi 10 1002 2014GL061224 S2CID 54683272 a b c Groudge Timothy A Head James W March 2014 Global inventory and characterization of pyroclastic deposits on Mercury New insights into pyroclastic activity from MESSENGER orbital data PDF Journal of Geophysical Research 119 3 635 658 Bibcode 2014JGRE 119 635G doi 10 1002 2013JE004480 S2CID 14393394 a b c Rothery David A Thomas Rebeca J Kerber Laura January 1 2014 Prolonged eruptive history of a compound volcano on Mercury Volcanic and tectonic implications PDF Earth and Planetary Science Letters 385 59 67 Bibcode 2014E amp PSL 385 59R doi 10 1016 j epsl 2013 10 023 a b Chang Kenneth November 29 2012 On Closest Planet to the Sun NASA Finds Lots of Ice The New York Times p A3 Archived from the original on November 29 2012 Sean C Solomon the principal investigator for MESSENGER said there was enough ice there to encase Washington D C in a frozen block two and a half miles deep Lewis John S 2004 Physics and Chemistry of the Solar System 2nd ed Academic Press p 463 ISBN 978 0 12 446744 6 Murdock Thomas L Ney Edward P 1970 Mercury The Dark Side Temperature Science 170 3957 535 537 Bibcode 1970Sci 170 535M doi 10 1126 science 170 3957 535 PMID 17799708 S2CID 38824994 Lewis John S 2004 Physics and Chemistry of the Solar System Academic Press ISBN 978 0 12 446744 6 Retrieved June 3 2008 Ingersoll Andrew P Svitek Tomas Murray Bruce C 1992 Stability of polar frosts in spherical bowl shaped craters on the Moon Mercury and Mars Icarus 100 1 40 47 Bibcode 1992Icar 100 40I doi 10 1016 0019 1035 92 90016 Z Slade Martin A Butler Bryan J Muhleman Duane O 1992 Mercury radar imaging Evidence for polar ice Science 258 5082 635 640 Bibcode 1992Sci 258 635S doi 10 1126 science 258 5082 635 PMID 17748898 S2CID 34009087 Williams David R June 2 2005 Ice on Mercury NASA Goddard Space Flight Center Retrieved May 23 2008 a b c Rawlins Katherine Moses Julianne I Zahnle Kevin J 1995 Exogenic Sources of Water for Mercury s Polar Ice Bulletin of the American Astronomical Society 27 1117 Bibcode 1995DPS 27 2112R Harmon John K Perillat Phil J Slade Martin A 2001 High Resolution Radar Imaging of Mercury s North Pole Icarus 149 1 1 15 Bibcode 2001Icar 149 1H doi 10 1006 icar 2000 6544 Domingue DL Koehn PL et al 2009 Mercury s Atmosphere A Surface Bounded Exosphere Space Science Reviews 131 1 4 161 186 Bibcode 2007SSRv 131 161D doi 10 1007 s11214 007 9260 9 S2CID 121301247 Hunten Donald M Shemansky Donald Eugene Morgan Thomas Hunt 1988 The Mercury atmosphere In Vilas Faith Chapman Clark R Shapley Matthews Mildred eds Mercury University of Arizona Press ISBN 978 0 8165 1085 6 Lakdawalla Emily July 3 2008 MESSENGER Scientists Astonished to Find Water in Mercury s Thin Atmosphere The Planetary Society Retrieved May 18 2009 Zurbuchen TH Raines JM et al 2008 MESSENGER Observations of the Composition of Mercury s Ionized Exosphere and Plasma Environment Science 321 5885 90 92 Bibcode 2008Sci 321 90Z doi 10 1126 science 1159314 PMID 18599777 S2CID 206513512 Instrument Shows What Planet Mercury Is Made Of University of Michigan June 30 2008 Retrieved May 18 2009 Killen Rosemary Cremonese Gabrielle et al 2007 Processes that Promote and Deplete the Exosphere of Mercury Space Science Reviews 132 2 4 433 509 Bibcode 2007SSRv 132 433K doi 10 1007 s11214 007 9232 0 S2CID 121944553 Killen Rosemary M Hahn Joseph M December 10 2014 Impact Vaporization as a Possible Source of Mercury s Calcium Exosphere Icarus 250 230 237 Bibcode 2015Icar 250 230K doi 10 1016 j icarus 2014 11 035 hdl 2060 20150010116 McClintock William E Vervack Ronald J et al 2009 MESSENGER Observations of Mercury s Exosphere Detection of Magnesium and Distribution of Constituents Science 324 5927 610 613 Bibcode 2009Sci 324 610M doi 10 1126 science 1172525 PMID 19407195 S2CID 5578520 a b c d e Beatty J Kelly Petersen Carolyn Collins Chaikin Andrew 1999 The New Solar System Cambridge University Press ISBN 978 0 521 64587 4 Mercury NASA October 19 2021 Retrieved July 4 2022 Hall Shannon March 24 2020 Life on the Planet Mercury It s Not Completely Nuts A new explanation for the rocky world s jumbled landscape opens a possibility that it could have had ingredients for habitability The New York Times Archived from the original on March 24 2020 Retrieved March 26 2020 Rodriguez J Alexis P Leonard Gregory J Kargel Jeffrey S Domingue Deborah Berman Daniel C Banks Maria Zarroca Mario Linares Rogelio Marchi Simone Baker Victor R Webster Kevin D Sykes Mark March 16 2020 The Chaotic Terrains of Mercury Reveal a History of Planetary Volatile Retention and Loss in the Innermost Solar System Scientific Reports 10 4737 4737 Bibcode 2020NatSR 10 4737R doi 10 1038 s41598 020 59885 5 PMC 7075900 PMID 32179758 Vast Collapsed Terrains on Mercury Might be Windows Into Ancient Possibly Habitable Volatile Rich Materials Planetary Science Institute March 16 2020 Retrieved August 27 2022 Seeds Michael A 2004 Astronomy The Solar System and Beyond 4th ed Brooks Cole ISBN 978 0 534 42111 3 Williams David R January 6 2005 Planetary Fact Sheets NASA National Space Science Data Center Retrieved August 10 2006 a b c Mercury s Internal Magnetic Field NASA January 30 2008 Retrieved April 21 2021 Gold Lauren May 3 2007 Mercury has molten core Cornell researcher shows Cornell University Retrieved April 7 2008 Christensen Ulrich R 2006 A deep dynamo generating Mercury s magnetic field Nature 444 7122 1056 1058 Bibcode 2006Natur 444 1056C doi 10 1038 nature05342 PMID 17183319 S2CID 4342216 Padovan Sebastiano Margot Jean Luc Hauck Steven A Moore William B Solomon Sean C April 2014 The tides of Mercury and possible implications for its interior structure Journal of Geophysical Research Planets 119 4 850 866 Bibcode 2014JGRE 119 850P doi 10 1002 2013JE004459 S2CID 56282397 a b Steigerwald Bill June 2 2009 Magnetic Tornadoes Could Liberate Mercury s Tenuous Atmosphere NASA Goddard Space Flight Center Retrieved July 18 2009 Van Hoolst Tim Jacobs Carla 2003 Mercury s tides and interior structure Journal of Geophysical Research 108 E11 7 Bibcode 2003JGRE 108 5121V doi 10 1029 2003JE002126 Space Topics Compare the Planets Mercury Venus Earth The Moon and Mars Planetary Society Archived from the original on July 28 2011 Retrieved April 12 2007 a b Williams David R October 21 2019 Planetary Fact Sheet Metric NASA Retrieved April 20 2021 Espenak Fred April 21 2005 Transits of Mercury NASA Goddard Space Flight Center Retrieved May 20 2008 Biswas Sukumar 2000 Cosmic Perspectives in Space Physics Astrophysics and Space Science Library Springer p 176 ISBN 978 0 7923 5813 8 a b Margot J L Peale S J Jurgens R F Slade M A et al 2007 Large Longitude Libration of Mercury Reveals a Molten Core Science 316 5825 710 714 Bibcode 2007Sci 316 710M doi 10 1126 science 1140514 PMID 17478713 S2CID 8863681 Popular Astronomy A Review of Astronomy and Allied Sciences Goodsell Observatory of Carleton College 1896 although in the case of Venus the libration in longitude due to the eccentricity of the orbit amounts to only 47 on either side of the mean position in the case of Mercury it amounts to 23 39 Seligman C The Rotation of Mercury cseligman com NASA Flash animation Retrieved July 31 2019 van Hemerlrijck E August 1983 On the Variations in the Insolation at Mercury Resulting from Oscillations of the Orbital Eccentricity The Moon and the Planets 29 1 83 93 Bibcode 1983M amp P 29 83V doi 10 1007 BF00928377 S2CID 122761699 Mercury Closest Approaches to Earth generated with 1 Solex 10 Archived December 20 2008 at the Wayback Machine Text Output file Archived March 9 2012 at the Wayback Machine 2 Gravity Simulator charts Archived September 12 2014 at the Wayback Machine 3 JPL Horizons 1950 2200 Archived November 6 2015 at the Wayback Machine 3 sources are provided to address original research concerns and to support general long term trends Stockman Tom Monroe Gabriel Cordner Samuel March 12 2019 Venus is not Earth s closest neighbor Physics Today doi 10 1063 PT 6 3 20190312a S2CID 241077611 Stockman Tom March 7 2019 Mercury is the closest planet to all seven other planets video Archived from the original on October 28 2021 Retrieved May 29 2019 via YouTube Which Planet is the Closest archived from the original on October 28 2021 retrieved July 22 2021 Davies M E June 10 1975 Surface Coordinates and Cartography of Mercury Journal of Geophysical Research 80 B17 2417 2430 Bibcode 1975JGR 80 2417D doi 10 1029 JB080i017p02417 Davies M E Dwornik S E Gault D E Strom R G 1978 NASA Atlas of Mercury NASA Scientific and Technical Information Office USGS Astrogeology Rotation and pole position for the Sun and planets IAU WGCCRE Archived from the original on October 24 2011 Retrieved October 22 2009 Archinal Brent A A Hearn Michael F Bowell Edward L Conrad Albert R et al 2010 Report of the IAU Working Group on Cartographic Coordinates and Rotational Elements 2009 Celestial Mechanics and Dynamical Astronomy 109 2 101 135 Bibcode 2011CeMDA 109 101A doi 10 1007 s10569 010 9320 4 ISSN 0923 2958 S2CID 189842666 Liu Han Shou O Keefe John A 1965 Theory of Rotation for the Planet Mercury Science 150 3704 1717 Bibcode 1965Sci 150 1717L doi 10 1126 science 150 3704 1717 PMID 17768871 S2CID 45608770 a b Colombo Giuseppe Shapiro Irwin I 1966 The rotation of the planet Mercury Astrophysical Journal 145 296 Bibcode 1966ApJ 145 296C doi 10 1086 148762 Correia Alexandre C M Laskar Jacques 2009 Mercury s capture into the 3 2 spin orbit resonance including the effect of core mantle friction Icarus 201 1 1 11 arXiv 0901 1843 Bibcode 2009Icar 201 1C doi 10 1016 j icarus 2008 12 034 S2CID 14778204 Correia Alexandre C M Laskar Jacques 2004 Mercury s capture into the 3 2 spin orbit resonance as a result of its chaotic dynamics Nature 429 6994 848 850 Bibcode 2004Natur 429 848C doi 10 1038 nature02609 PMID 15215857 S2CID 9289925 Noyelles B Frouard J Makarov V V amp Efroimsky M 2014 Spin orbit evolution of Mercury revisited Icarus 241 2014 26 44 arXiv 1307 0136 Bibcode 2014Icar 241 26N doi 10 1016 j icarus 2014 05 045 S2CID 53690707 Laskar Jacques March 18 2008 Chaotic diffusion in the Solar System Icarus 196 1 1 15 arXiv 0802 3371 Bibcode 2008Icar 196 1L doi 10 1016 j icarus 2008 02 017 S2CID 11586168 Laskar Jacques Gastineau Mickael June 11 2009 Existence of collisional trajectories of Mercury Mars and Venus with the Earth Nature 459 7248 817 819 Bibcode 2009Natur 459 817L doi 10 1038 nature08096 PMID 19516336 S2CID 4416436 Le Verrier Urbain 1859 Lettre de M Le Verrier a M Faye sur la theorie de Mercure et sur le mouvement du perihelie de cette planete Comptes rendus hebdomadaires des seances de l Academie des sciences in French Paris 49 379 383 At p 383 in the same volume Le Verrier s report is followed by another from Faye enthusiastically recommending to astronomers to search for a previously undetected intra mercurial object Baum Richard Sheehan William 1997 In Search of Planet Vulcan The Ghost in Newton s Clockwork Machine New York Plenum Press ISBN 978 0 306 45567 4 a b Clemence Gerald M 1947 The Relativity Effect in Planetary Motions Reviews of Modern Physics 19 4 361 364 Bibcode 1947RvMP 19 361C doi 10 1103 RevModPhys 19 361 Gilvarry John J 1953 Relativity Precession of the Asteroid Icarus Physical Review 89 5 1046 Bibcode 1953PhRv 89 1046G doi 10 1103 PhysRev 89 1046 Brown Kevin 6 2 Anomalous Precession Reflections on Relativity MathPages Retrieved May 22 2008 a b Menzel Donald H 1964 A Field Guide to the Stars and Planets The Peterson Field Guide Series Boston Houghton Mifflin Co pp 292 293 Tezel Tunc January 22 2003 Total Solar Eclipse of 2006 March 29 Department of Physics at Fizik Bolumu in Turkey Retrieved May 24 2008 a b Mallama Anthony 2011 Planetary magnitudes Sky and Telescope 121 1 51 56 Espenak Fred 1996 NASA Reference Publication 1349 Venus Twelve year planetary ephemeris 1995 2006 Twelve Year Planetary Ephemeris Directory NASA Retrieved May 24 2008 a b Walker John Mercury Chaser s Calculator Fourmilab Switzerland Retrieved May 29 2008 look at 1964 and 2013 Mercury Elongation and Distance Archived from the original on May 11 2013 Retrieved May 30 2008 Numbers generated using the Solar System Dynamics Group Horizons On Line Ephemeris System a b c Kelly Patrick ed 2007 Observer s Handbook 2007 Royal Astronomical Society of Canada ISBN 978 0 9738109 3 6 Curtis A C October 1972 Finding Venus or Mercury in daylight Journal of the British Astronomical Association 82 438 439 Bibcode 1972JBAA 82 438C Alers Paul E March 17 2011 Celebrating Mercury Orbit NASA Multimedia Retrieved March 18 2011 NASA spacecraft now circling Mercury a first NBC News March 17 2011 Retrieved March 24 2011 Baumgardner Jeffrey Mendillo Michael Wilson Jody K 2000 A Digital High Definition Imaging System for Spectral Studies of Extended Planetary Atmospheres I Initial Results in White Light Showing Features on the Hemisphere of Mercury Unimaged by Mariner 10 The Astronomical Journal 119 5 2458 2464 Bibcode 2000AJ 119 2458B doi 10 1086 301323 S2CID 17361371 Schaefer Bradley E 2007 The Latitude and Epoch for the Origin of the Astronomical Lore in MUL APIN American Astronomical Society Meeting 210 42 05 38 157 Bibcode 2007AAS 210 4205S Hunger Hermann Pingree David 1989 MUL APIN An Astronomical Compendium in Cuneiform Archiv fur Orientforschung 24 146 MESSENGER Mercury and Ancient Cultures NASA JPL 2008 Retrieved April 7 2008 Heath Sir Thomas 1921 A History of Greek Mathematics Vol II Oxford Clarendon Press pp vii 273 Goldstein Bernard R 1996 The Pre telescopic Treatment of the Phases and Apparent Size of Venus Journal for the History of Astronomy 27 1 Bibcode 1996JHA 27 1G doi 10 1177 002182869602700101 S2CID 117218196 Kelley David H Milone E F Aveni Anthony F 2004 Exploring Ancient Skies An Encyclopedic Survey of Archaeoastronomy Birkhauser ISBN 978 0 387 95310 6 De Groot Jan Jakob Maria 1912 Religion in China universism a key to the study of Taoism and Confucianism American lectures on the history of religions Vol 10 G P Putnam s Sons p 300 Retrieved January 8 2010 Crump Thomas 1992 The Japanese numbers game the use and understanding of numbers in modern Japan Nissan Institute Routledge Japanese studies series Routledge pp 39 40 ISBN 978 0 415 05609 0 Hulbert Homer Bezaleel 1909 The passing of Korea Doubleday Page amp company p 426 Retrieved January 8 2010 Pujari R M Kolhe Pradeep Kumar N R 2006 Pride of India A Glimpse Into India s Scientific Heritage Samskrita Bharati ISBN 978 81 87276 27 2 Bakich Michael E 2000 The Cambridge Planetary Handbook Cambridge University Press ISBN 978 0 521 63280 5 Milbrath Susan 1999 Star Gods of the Maya Astronomy in Art Folklore and Calendars University of Texas Press ISBN 978 0 292 75226 9 Samso Julio Mielgo Honorino 1994 Ibn al Zarqalluh on Mercury Journal for the History of Astronomy 25 4 289 96 292 Bibcode 1994JHA 25 289S doi 10 1177 002182869402500403 S2CID 118108131 Hartner Willy 1955 The Mercury Horoscope of Marcantonio Michiel of Venice Vistas in Astronomy 1 1 84 138 Bibcode 1955VA 1 84H doi 10 1016 0083 6656 55 90016 7 at pp 118 122 Ansari S M Razaullah 2002 History of oriental astronomy proceedings of the joint discussion 17 at the 23rd General Assembly of the International Astronomical Union organised by the Commission 41 History of Astronomy held in Kyoto August 25 26 1997 Springer Science Business Media p 137 ISBN 1 4020 0657 8 Goldstein Bernard R 1969 Some Medieval Reports of Venus and Mercury Transits Centaurus 14 1 49 59 Bibcode 1969Cent 14 49G doi 10 1111 j 1600 0498 1969 tb00135 x Ramasubramanian K Srinivas M S Sriram M S 1994 Modification of the Earlier Indian Planetary Theory by the Kerala Astronomers c 1500 AD and the Implied Heliocentric Picture of Planetary Motion PDF Current Science 66 784 790 Archived from the original PDF on December 23 2010 Retrieved April 23 2010 Gaab Hans 2018 Simon Marius and His Research Springer p 256 ISBN 978 3 319 92620 9 Marius noted in the dedication from June 30 1612 in the Prognosticon auf 1613 that Mercury is illuminated by the Sun in the same way as the Venus and the Moon and reports his observations of the brightness Sinnott Roger W Meeus Jean 1986 John Bevis and a Rare Occultation Sky and Telescope 72 220 Bibcode 1986S amp T 72 220S Ferris Timothy 2003 Seeing in the Dark How Amateur Astronomers Simon and Schuster ISBN 978 0 684 86580 5 a b Colombo Giuseppe Shapiro Irwin I November 1965 The Rotation of the Planet Mercury SAO Special Report 188R 188 188 Bibcode 1965SAOSR 188 C Holden Edward S 1890 Announcement of the Discovery of the Rotation Period of Mercury by Professor Schiaparelli Publications of the Astronomical Society of the Pacific 2 7 79 Bibcode 1890PASP 2 79H doi 10 1086 120099 S2CID 122095054 Davies Merton E Dwornik Stephen E Gault Donald E Strom Robert G 1978 Surface Mapping Atlas of Mercury NASA Office of Space Sciences Retrieved May 28 2008 Evans John V Brockelman Richard A Henry John C Hyde Gerald M Kraft Leon G Reid Wyatt A Smith W W 1965 Radio Echo Observations of Venus and Mercury at 23 cm Wavelength Astronomical Journal 70 487 500 Bibcode 1965AJ 70 486E doi 10 1086 109772 Moore Patrick 2000 The Data Book of Astronomy New York CRC Press p 483 ISBN 978 0 7503 0620 1 Butrica Andrew J 1996 Chapter 5 To See the Unseen A History of Planetary Radar Astronomy NASA History Office Washington D C ISBN 978 0 16 048578 7 Pettengill Gordon H Dyce Rolf B 1965 A Radar Determination of the Rotation of the Planet Mercury Nature 206 1240 451 2 Bibcode 1965Natur 206Q1240P doi 10 1038 2061240a0 S2CID 31525579 Mercury Eric Weisstein s World of Astronomy Wolfram Research Retrieved April 18 2021 Murray Bruce C Burgess Eric 1977 Flight to Mercury Columbia University Press ISBN 978 0 231 03996 3 Colombo Giuseppe 1965 Rotational Period of the Planet Mercury Nature 208 5010 575 Bibcode 1965Natur 208 575C doi 10 1038 208575a0 S2CID 4213296 Davies Merton E et al 1976 Mariner 10 Mission and Spacecraft SP 423 Atlas of Mercury NASA JPL Retrieved April 7 2008 Golden Leslie M 1977 A Microwave Interferometric Study of the Subsurface of the Planet Mercury Thesis University of California Berkeley Bibcode 1977PhDT 9G Mitchell David L De Pater Imke 1994 Microwave Imaging of Mercury s Thermal Emission at Wavelengths from 0 3 to 20 5 cm 1994 Icarus 110 1 2 32 Bibcode 1994Icar 110 2M doi 10 1006 icar 1994 1105 Dantowitz Ronald F Teare Scott W Kozubal Marek J 2000 Ground based High Resolution Imaging of Mercury Astronomical Journal 119 4 2455 2457 Bibcode 2000AJ 119 2455D doi 10 1086 301328 S2CID 121483006 Harmon John K Slade Martin A Butler Bryan J Head III James W Rice Melissa S Campbell Donald B 2007 Mercury Radar images of the equatorial and midlatitude zones Icarus 187 2 374 405 Bibcode 2007Icar 187 374H doi 10 1016 j icarus 2006 09 026 Webster Guy June 10 2014 Mercury Passes in Front of the Sun as Seen From Mars NASA Retrieved June 10 2014 Zacny Kris July 2 2015 Inner Solar System Prospective Energy and Material Resources Springer International Publishing p 154 ISBN 9783319195698 Wagner Sam Wie Bong November 2015 Hybrid Algorithm for Multiple Gravity Assist and Impulsive Delta V Maneuvers Journal of Guidance Control and Dynamics 38 11 2096 2107 Bibcode 2015JGCD 38 2096W doi 10 2514 1 G000874 Mercury PDF NASA Jet Propulsion Laboratory May 5 2008 Retrieved April 26 2021 Leipold Manfred E Seboldt W Lingner Stephan Borg Erik Herrmann Axel Siegfried Pabsch Arno Wagner O Bruckner Johannes 1996 Mercury sun synchronous polar orbiter with a solar sail Acta Astronautica 39 1 143 151 Bibcode 1996AcAau 39 143L doi 10 1016 S0094 5765 96 00131 2 Dunne James A amp Burgess Eric 1978 Chapter Four The Voyage of Mariner 10 Mission to Venus and Mercury NASA History Office Retrieved May 28 2008 Phillips Tony October 1976 NASA 2006 Transit of Mercury SP 423 Atlas of Mercury NASA Retrieved April 7 2008 BepiColumbo Background Science European Space Agency Retrieved June 18 2017 Malik Tariq August 16 2004 MESSENGER to test theory of shrinking Mercury USA Today Retrieved May 23 2008 Davies ME et al 1978 Mariner 10 Mission and Spacecraft Atlas of Mercury NASA Office of Space Sciences Retrieved May 30 2008 Ness Norman F 1978 Mercury Magnetic field and interior Space Science Reviews 21 5 527 553 Bibcode 1978SSRv 21 527N doi 10 1007 BF00240907 S2CID 120025983 Aharonson Oded Zuber Maria T Solomon Sean C 2004 Crustal remanence in an internally magnetized non uniform shell a possible source for Mercury s magnetic field Earth and Planetary Science Letters 218 3 4 261 268 Bibcode 2004E amp PSL 218 261A doi 10 1016 S0012 821X 03 00682 4 Dunne James A amp Burgess Eric 1978 Chapter Eight The Voyage of Mariner 10 Mission to Venus and Mercury NASA History Office Grayzeck Ed April 2 2008 Mariner 10 NSSDC Master Catalog NASA Retrieved April 7 2008 MESSENGER Engine Burn Puts Spacecraft on Track for Venus SpaceRef com 2005 Retrieved March 2 2006 a b Countdown to MESSENGER s Closest Approach with Mercury Johns Hopkins University Applied Physics Laboratory January 14 2008 Archived from the original on May 13 2013 Retrieved May 30 2008 MESSENGER Gains Critical Gravity Assist for Mercury Orbital Observations MESSENGER Mission News September 30 2009 Archived from the original on May 10 2013 Retrieved September 30 2009 NASA extends spacecraft s Mercury mission United Press International November 15 2011 Retrieved November 16 2011 MESSENGER Fact Sheet PDF Applied Physics Laboratory February 2011 Retrieved August 21 2017 Wall Mike March 29 2015 NASA Mercury Probe Trying to Survive for Another Month Space com Retrieved April 4 2015 Chang Kenneth April 27 2015 NASA s Messenger Mission Is Set to Crash Into Mercury The New York Times Archived from the original on April 29 2015 Retrieved April 27 2015 Corum Jonathan April 30 2015 Messenger s Collision Course With Mercury The New York Times Retrieved April 30 2015 Best Determination of MESSENGER s Impact Location MESSENGER Featured Images Johns Hopkins Applied Physics Lab June 3 2015 Retrieved April 29 2015 a b ESA gives go ahead to build BepiColombo European Space Agency February 26 2007 Retrieved May 29 2008 BepiColombo Fact Sheet European Space Agency December 1 2016 Retrieved December 19 2016 Objectives European Space Agency February 21 2006 Retrieved May 29 2008 Warren Haygen October 24 2021 BepiColombo completes first Mercury flyby science provides insight into planet s unique environment NASA Spaceflight Retrieved October 8 2022 External linksListen to this article 41 minutes source source track This audio file was created from a revision of this article dated 16 January 2008 2008 01 16 and does not reflect subsequent edits Audio help More spoken articles Mercury at Wikipedia s sister projects Definitions from Wiktionary Media from Commons Quotations from Wikiquote Texts from Wikisource Textbooks from Wikibooks Resources from Wikiversity Data from Wikidata Atlas of Mercury NASA 1978 SP 423 Mercury nomenclature and map with feature names from the USGS IAU Gazetteer of Planetary Nomenclature Equirectangular map of Mercury by Applied Coherent Technology Corp 3D globe of Mercury by Google Mercury at Solarviews com Mercury by Astronomy Cast MESSENGER mission web site BepiColombo mission web site Portals Astronomy Stars Spaceflight Outer space Solar system Retrieved from https en wikipedia org w index php title Mercury planet amp oldid 1135550469, wikipedia, wiki, book, books, library,

article

, read, download, free, free download, mp3, video, mp4, 3gp, jpg, jpeg, gif, png, picture, music, song, movie, book, game, games.