Showing posts with label Kuiper Belt. Show all posts
Showing posts with label Kuiper Belt. Show all posts

Wednesday, 22 April 2026

Dwarf Planet 136108 Haumea approaches opposition.

The Dwarf Planet 136108 Haumea will reach opposition (i.e. be directly opposite the Sun seen from Earth) at 8.47 am GMT on Thursday 23 April 2026. This means that it will both be at its closest to the Earth this year, about 42.1 AU (42.1 times the average distance between the Earth and the Sun, or about 6 298 255 000 km), and completely illuminated by the Sun. While it is not visible to the naked eye observer, the planets have phases just like those of the Moon; being further from the Sun than the Earth, 136108 Haumea is 'full' when directly opposite the Sun. 

The orbit and position of 136108 Haumea and the planets of the Solar System at 9.00 am on Thursday 23 April 2026. JPL Small Body Database Browser.

At opposition, the Dwarf Planet will be in the constellation of Bootes and at its highest point in the sky at about midnight local time from anywhere on Earth (this is because the rising and setting of objects in the sky is caused by the Earth's rotation, not the movement of the object). (Even at it's very brightest 136108 Haumea will only have a Magnitude of 17.3, making it almost impossible to see with any but the largest of Earth-based telescopes, and where resolvable it will only be possible to see it as a point of light indistinguishable from a faint star.

136108 Haumea orbits the Sun on an eccentric orbit tilted at an angle of 28.2° to the plane of the Solar System, which takes it from 34.4 AU from the Sun (34.4 times the average distance at which the Earth orbits the Sun) to 51.5 AU from the Sun (51.5 times the average distance at which the Earth orbits the Sun). With an average distance of 43.0 AU, 136108 Haumea completes one orbit around the Sun every 282 years. This means that the planet is almost stationary compared to the faster moving Earth, so that it reaches Opposition only one day later each year than the year before, and reaches Solar Conjunction (when it is directly on the opposite side of the Sun to the Earth), roughly six months later.

136108 Haumea was discovered on 28 December 2004 by a team led by Mike Brown of the Palomar Observatory in California, in images taken by them on 28 May 2004; on 27 July 2005 a team led by José Luis Ortiz Moreno and his team at the Instituto de Astrofísica de Andalucía reported that they had also discovered the Dwarf Planet, in images taken between 7 and 10 March 2003. With a diameter of 2100 km it is considered to be the third largest dwarf planet in the Solar System (after 134340 Pluto and 136199 Eris) as well as the eighteenth largest body in the Solar System, excluding the Sun (several moons, including our own, are larger).

Haumea has been calculated to be rotating once every 3.9 hours, far more rapidly than any other large body in the Solar System. Curiously for such a fast rotating body, it has not adopted a oblate spheroid (flattened sphere) shape, but is instead a triaxial ellipsoid (elongate flattened sphere, or flattened egg-shape). This implies that, although its surface is comprised of ice, it has a core of fairly dense rocky material. 

The Dwarf Planet Haumea is believed to rotate in just under 4 hours. This rapid rotation causes the Dwarf Planet to be elongated in appearance. Stephanie Hoover/Wikimedia Commons.

Although Haumea is only about a quarter the size of Pluto, it is thought to be large enough that it should have reached hydrostatic equilibrium (i.e. become approximately spherical due to its own gravity). The elongate shape of Haumea is at odds with this, something which, in combination with its high rotational rate, has been suggested as evidence of a major collision in Haumea's past. This has been supported by the discovery in 2017 of a ring surrounding the dwarf planet with a radius of about 2285 km. This is well within the Roche limit for Haumea (the distance below which a ring or other orbiting body should be disrupted by the parent body's gravity and either fall onto it or be ejected), suggesting that this is a temporary structure caused by a relatively recent event (although still potentially billions of years ago, given the weak gravitational forces involved).

136108 Haumea rotating within its ring system. Tom Ruen/Wikimedia Commons.

136108 has two small moons, both of which were discovered in 2005 by Darin Ragozzine and Michael Brown, at that time working at the W. M. Keck Observatory in Hawai'i. The larger of these, Hi'iaka, is roughly 370 km in diameter (although, like its parent body, it has been calculated to have an elongate, non-spherical shape) and orbits at a distance of 49 400 km, completing one orbit every 49.5 days. The smaller, Namaka, has been calculated to be about 150 km in diameter with an irregular shape, and to orbit at a distance of approximately 25 500 km.

Both the rings of 136108 Haumea and the larger moon, Hi'iaka, follow orbital paths 1-3° offset from the equator of the dwarf planet, and are thought to be products of the same collision. The smaller moon, Namaka, has an orbit offset by 69° from the equator of Haumea. This moon is thought to have been formed in the same collision, but to have had it's orbit perturbed significantly by tidal interactions with the larger moon.

Dwarf Planet Haumea and its satellites, imaged by the Hubble Space Telescope's WFC2 camera from 12 May 2008 and 19 May 2008. The brighter dot orbiting Haumea is the larger outer moon Hi'iaka while the fainter dot is the smaller inner moon Namaka. This animation of the moons' orbits spans 7 days and the orbital plane of Namaka is oriented vertically. Hubble Space Telescope/Michael Brown/Wikimedia Commons.

136108 Haumea is thought to be a member of a collisional family of Kuiper Belt objects; the only collisional family identified from this part of the Solar System. This family has been named the Haumea, or Haumean, Family in reference to its largest known member. Collisional families are groups of bodies which appear to have been created in a single collision event, and whose orbital trajectories can in theory all be traced back to a single point of origin, although this is not the case for the Haumea Family, which are thought to have had their orbital paths modified over time by interactions with the gravitational field of Neptune. 

As well as 136108 Haumea and its ring and moons, this family is thought to include the Kuiper Belt Objects (19308) 1996 TO66, (24835) 1995 SM55, (55636) 2002 TX300, (86047) 1999 OY3, (120178) 2003 OP32, (145453) 2005 RR43, (202421) 2005 UQ513, (308193) 2005 CB79, (315530) 2008 AP129, (386723) 2009 YE7, (416400) 2003 UZ117, (523645) 2010 VK201, (543454) 2014 HZ199, (612620) 2003 SQ317, (653589) 2014 QW441, (671467) 2014 LO28, and (673087) 2015 AJ281, as well, presumably, as other as yet undiscovered bodies.

The orbits of the bodies of the Haumea Collisional Family (not all are shown). Tom Ruen/Wikimedia Commons.

As well as having similar orbital properties, the bodies of the Haumea Family all share a similar high albedo (with the exception of (202421) 2005 UQ513), which suggests a surface largely covered by reflective water ice, rather than the darker, reddish, tholins (frozen organic compounds) which cover the surface of most Kuiper Belt objects. (202421) 2005 UQ513 has a lower albedo and a reddish spectrum, suggesting that it has an outer surface covered with tholins, but is included within the Haumea Family due to the similarity of its orbit.

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Thursday, 28 March 2024

Dwarf planet 136472 Makemake reaches oposition.

The dwarf planet 136472 Makemake will reach opposition (i.e. be directly opposite the Sun seen from Earth) on Saturday 30 March 2022 at 8.28 pm GMT. This means that it will both be at its closest to the Earth this year, about 51.80 AU (51.80 times the average distance between the Earth and the Sun, or about 7 776 097 000 km), and completely illuminated by the Sun. While it is not visible to the naked eye observer, the planets have phases just like those of the Moon; being further from the Sun than the Earth, 136472 Makemake is 'full' when directly opposite the Sun. The planet will be in the constellation of Coma Berenices and at its highest point in the sky at about midnight local time from anywhere on Earth (this is because the rising and setting of objects in the sky is caused by the Earth's rotation, not the movement of the object). (Even at it's very brightest 136472 Makemake will only have a Magnitude of 17.1, making it almost impossible to see with any but the largest of Earth-based telescopes, and where resolvable it will only be possible to see it as a point of light indistinguishable from a faint star.

The orbit and position of 136472 Makemake (2005 FY9) at 10.00 pm on Monday 28 March 2022. JPL Small Body Database Browser.

136472 Makemake orbits the Sun on an eccentric orbit tilted at an angle of 29.0° to the plane of the Solar System, which takes it from 37.8 AU from the Sun (37.8 times the average distance at which the Earth orbits the Sun) to 52.8 AU from the Sun (52.8 times the average distance at which the Earth orbits the Sun. With an average distance of 45.3 AU, 136472 Makemake completes one orbit around the Sun every 305 years. This means that the planet is almost stationary compared to the faster moving Earth, so that it reaches Opposition only two days earlier each year than the year before, and reaches Solar Conjunction (when it is directly on the opposite side of the Sun to the Earth), roughly six months later.

Hubble Space Telescope image of 136472 Makemake. Mike Brown/NASA.

136472 Makemake was discovered on 31 Match 2005 by a team led by Mike Brown of the Palomar Observatory in California. With a diameter of 1430 km it is considered to be the fourth largest dwarf planet in the Solar System (after 134340 Pluto, 136199 Eris, and 136108 Haumea) as well as the twenty second largest body in the Solar System, excluding the Sun (several moons, including our own, are larger). Makemake is also the second-brightest Kuiper belt object, after Pluto.

The surface of 136472 Makemake appears reddish at visual wavelengths, and spectral analysis suggests that it's surface is covered primarily by methane ice, with large amounts of ethane and tholins as well as smaller amounts of ethylene, acetylene and high-mass alkanes. Notably, nitrogen, although present, is observed at much lower levels than on Pluto and Triton, where it is the most abundant ice. 136472 Makemake apparently lacks any form of atmosphere, although it does have a satellite, S/2015 (136472) 1, which is estimated to be 175 km in diameter and orbits at a distance of at least 25 000 km, with an orbital period of at least 12 days.

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Tuesday, 11 July 2023

A colour enhanced image of Charon.

NASA has released a colour image of Pluto's largest moon, Charon, taken by the New Horizons space probe on 14 July 2015. The image is a composite built up from images taken in the blue, red, and infrared parts of the spectrum by the Ralph Multispectral Visual Imaging Camera, processed to accentuate the surface features of the moon.

Composite image of Pluto's moon Charon, built up from images taken by the Ralph Multispectral Visual Imaging Camera on the New Horizons space probe on 14 July 2015. NASA.

Discovered in 1978, Charon is the largest moon of Pluto, with a diameter of 1212 km, and 12% of the mass of Pluto itself. This makes it the sixth largest known trans-Neptunian object, after Pluto itself, Eris, Haumea, Makemake and Gonggong, as well as the twelfth largest moon in the Solar System, after Ganymede and Titan (which are both larger than the planet Mercury), Calisto, Io, the Earth's Moon, Europa, Triton, Titania, Rhea, Oberon, and Iapetus.

Pluto and Charon are gravitationally locked, always keeping the same face towards one-another, and orbiting their mutual barycentre every 6.387 days. The two bodies are, on average, 19 591 km apart, although this orbit does vary slightly. 

The orbit of Pluto and Charon about their mutual barycentre. Tom Ruen/Wikimedia Commons.

Unlike Pluto, which has a surface largely covered by methane and nitrogen ices, the surface of Charon appears to be covered largely by water ice, with patches of tholins and other hydrocarbons around its north pole. Patches of ammonia and water ice crystals on the surface are thought to indicators of cryovolcanism. The surface of the moon also has a number of large canyons following a southwest-northeast direction.

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Monday, 18 April 2022

Dwarf Planet 136108 Haumea reaches oposition.

The Dwarf Planet 136108 Haumea will reach opposition (i.e. be directly opposite the Sun seen from Earth) on Tuesday 19 April 2022 at 8.18 pm GMT. This means that it will both be at its closest to the Earth this year, about 49.28 AU (19.28 times the average distance between the Earth and the Sun, or about 7 327 183 000 km), and completely illuminated by the Sun. While it is not visible to the naked eye observer, the planets have phases just like those of the Moon; being further from the Sun than the Earth, 136108 Haumea is 'full' when directly opposite the Sun. The Dwarf Planet will be in the constellation of Bootes and at its highest point in the sky at about 1.40 am local time from anywhere on Earth (this is because the rising and setting of objects in the sky is caused by the Earth's rotation, not the movement of the object). (Even at it's very brightest 136108 Haumea will only have a Magnitude of 17.3, making it almost impossible to see with any but the largest of Earth-based telescopes, and where resolvable it will only be possible to see it as a point of light indistinguishable from a faint star.

 
The orbit and position of 136108 Haumea (2003 EL61) at 8.00 pm on Tuesday 19 April 2022. JPL Small Body Database Browser.

136108 Haumea orbits the Sun on an eccentric orbit tilted at an angle of 28.2° to the plane of the Solar System, which takes it from 34.4 AU from the Sun (34.4 times the average distance at which the Earth orbits the Sun) to 51.5 AU from the Sun (51.5 times the average distance at which the Earth orbits the Sun). With an average distance of 43.0 AU, 136108 Haumea completes one orbit around the Sun every 282 years. This means that the planet is almost stationary compared to the faster moving Earth, so that it reaches Opposition only one day later each year than the year before, and reaches Solar Conjunction (when it is directly on the opposite side of the Sun to the Earth), roughly six months later.

 
The Dwarf Planet Haumea is believed to rotate in just under 4 hours. This rapid rotation causes the Dwarf Planet to be elongated in appearance. Stephanie Hoover/Wikimedia Commons.

136108 Haumea was discovered on 28 December 2004 by a team led by Mike Brown of the Palomar Observatory in California, in images taken by them on 28 May 2004; on 27 July 2005 a team led by José Luis Ortiz Moreno and his team at the Instituto de Astrofísica de Andalucía reported that they had also discovered the Dwarf Planet, in images taken between 7 and 10 March 2003. With a diameter of 2100 km it is considered to be the third largest dwarf planet in the Solar System (after 134340 Pluto and 136199 Eris) as well as the eighteenth largest body in the Solar System, excluding the Sun (several moons, including our own, are larger).

Haumea has been calculated to be rotating once every 3.9 hours, far more rapidly than any other large body in the Solar System. Curiously for such a fast rotating body, it has not adopted a oblate spheroid (flattened sphere) shape, but is instead a triaxial ellipsoid (elongate flattened sphere, or flattened egg-shape). This implies that, although its surface is comprised of ice, it has a core of fairly dense rocky material. The Dwarf Planet also appears to be surrounded by a ring of icy material, and at least two moons, which have been named Hiʻiaka and Namaka.

 
Dwarf Planet Haumea and its satellites, imaged by the Hubble Space Telescope's WFC2 camera from 12 May 2008 and 19 May 2008. The brighter dot orbiting Haumea is the larger outer moon Hi'iaka while the fainter dot is the smaller inner moon Namaka. This animation of the moons' orbits spans 7 days and the orbital plane of Namaka is oriented vertically. Hubble Space Telescope/Michael Brown/Wikimedia Commons.

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Sunday, 3 April 2022

Understanding the unexpected volcanoes of Pluto.

Pluto is the largest body in the Kuiper Belt, with a diameter of 2377 km and a density which suggests a structure comprising about 300 km of water-rich ice overlaying a rocky core. It is not predicted to have high levels of internal radiogenic heating, and, while it is thought that the moon Charon was formed in a collision event, any residual heating from this event, or subsequent tidal interactions, should have dissipated billions of years ago. Surface temperatures on Pluto range between 35 and 60K (between -238 and -213°C). The surface pressure on Pluto is about 10 μbar, precluding the existence of any form of liquid there. At the temperatures and pressures found on the surface of Pluto water should be an immobile bedrock. Adding sufficient amounts of ammonia to water can lower its freezing point by about 100 degrees, and other substances could conceivably lower it slightly further, but depressing the freezing point of water enough for it to retain any fluidity on the surface of Pluto is highly unlikely. Nevertheless, when the New Horizons space probe visited the dwarf planet in 2015, it found abundant signs of resurfacing, which are difficult to explain without the presence of liquid water beneath the surface of Pluto.

In a paper published in the journal Nature Communications on 29 March 2021, a team of scientists led by Kelsi Singer of the Southwest Research Institute discuss the possibility of cryovolcanism (ice volcanoes) as an explanation for the observed features on the surface of Pluto.

Singer et al. examine an area to the southwest of the Sputnik Planitia ice sheet (an ancient impact basin with a diameter of about 1000 km), which they view as a possible volcanic terrain. The most prominent features of this region are a series of large rises or mounds of material separated by broad depressions, the two largest of which form annular features with deep central depressions, and are named Wright Mons and Picard Mons. Wright Mons stands roughly 4-5 km high, and has a diameter of about 150 km, giving it a volume of roughly 24 000 km³, while Picard Mons appears to be about 7 km high, and to have a diameter of about 225 km.

 
Panchromatic basemap mosaic of the putative cryovolcanic terrains; dashed red curve indicates the transition from directly sunlit terrain to haze-lit terrain. Simple cylindrical projection. Image shown with north up, and the lighting direction is indicated here with the large arrow at the upper left. Singer et al. (2022).

Wright Mons is surrounded, and partially covered, by a hummocky terrain, which has a typical wavelength of 6-12 km, but reaches up to 20 km between hummocks in places. The hummocks are generally interconnected rather than singular, and have flattened or rounded tops. In the images the northern flank of Wright Mons, and the plain to the north of the mountain, appear to be smoother and less hummocky, but Singer et al. suggest that this is probably an artifact of the lighting direction. The hummocks appear to have no preferred direction with regard to the summit, and closer examination shows smaller structures, such as boulders, blocks, slabs, and ridges, with scales of 1-2 km, superimposed on top of the hummocks.

 
Features of Wright Mons and the surrounding terrain. (a) Wright Mons region with features labelled, (b) high-resolution topography for Wright Mons, (c) zoom of region with smaller dome named Coleman Mons (label 'D'), undulating, hummocky terrain on the flanks of Wright Mons and the superposed smaller-scale (1–2 km) ridges or boulders, (d) topographic profile of Wright Mons and adjacent rise as shown by the line A to A’ in panel (a). All images are from the New Horizons observations on a simple cylindrical projection. The large arrow in the upper left of panel a indicates the direction of incoming sunlight. Figure shown with north up. Singer et al. (2022).

The slopes of the flanks of Wright Mons average about 3-5°, but reach 10° in places. The mountain has a central depression roughly 40-50 km across and about 4 km deep (i.e. taking it down to the level of the surrounding terrain). The central depression of Picard Mons appears to be larger still, with a more u-shaped profile. The structure of these bodies is unlike anything seen in terrestrial or Martian volcanoes, with the central caldera(?) taking up a third of the structure's area and being as deep as the mountain is tall. The inner slopes of the crater appear to have the same hummocky profile as the outer slopes, with no collapse terraces, or similar structures, as might be expected on a volcano in the Inner Solar System. The northern and southern faces of Wright Mons, and the nearby ridge of the Medial Montes all appear to have similar profiles, with a steeper northern face and a more shallowly inclined southern face, both of which are covered by hummocks.

 If the interior depressions of Wright and Picard montes are collapse structures, formed within formerly dome-shaped structures, then they would represent a loss of about half the mountains' total masses, which seems highly implausible. 

 
Topographic profile comparison. (a) Mauna Loa (subaerial portion only) compared with Wright Mons (roughly N-S through the feature), upper panel is without vertical exaggeration, and lower panel is shown at 10× vertical exaggeration. Mauna Lau continues for approximately 6 km below the ocean surface. This figure illustrates how Wright Mons is very dissimilar to Mauna Loa and that if Wright was originally more similar to a shield volcano it would have had to have lost more than 50% of its volume from the central region in order to attain its current appearance. (b) Martian shield volcanos from the Tharsis region provide additional examples of large volcanos, some with more advanced caldera collapse. Several of these also show signs of later embayment, thus they also may not represent the full original height of the features. The more typical collapse terraces can be seen in the Martian calderas. Note that none of these examples are scaled for gravity, they are shown at their original scales. Singer et al. (2022).

A few other depressions of varying size are scattered across the area around Wright and Picard montes. These are generally not circular in shape, which rules out an impact origin. Some of these structures may be related to collapse at fault faces, while others might be depressions between areas of uplift.

No vents or fractures from which effusive material might escape can be seen in this landscape, not any sign of flow through which the presence of such structure might be inferred, although this might be an artefact of the resolution of the images (234–315 m per pixel), which prevents the detection of small structures. Nor are there any signs of explosive eruptions, such as fall deposit patterns (either radial or directional), or steeper cones. The extent of this terrain is unclear, as it continues southward until it disappears within a low-light haze. The absence of any cratering on or around Wright Mons gives it a maximum age of 1-2 billion years, and potentially considerably younger.

Methane, nitrogen, and water ice have all been observed on the surface of Pluto, in high-volume, concentrated deposits, so Singer et al. consider whether these might make up the structures of Wright and Picard montes, and the surrounding terrain. Data provided by the Linear Etalon Imaging Spectral Array instrument on New Horizons suggests that nitrogen- and methane-rich complexes of nitrogen, methane, and carbon monoxide cover much of the surface of Pluto. These are likely to sublimate and redeposit on a seasonal cycle (which on Pluto implies a 248 Earth year cycle), or a multi-million-year cycle determined by obliquity/precession cycles. In darker areas with low albedos these volatiles are either not being deposited, or not being retained, with the upshot that these areas are dominated by the non-volatile water ice 'bedrock'. Such areas include the dark equatorial band of Pluto, as well as the terrain around Wright and Picard montes. In this later area, deeper areas are dark, implying water ice, whereas higher elevations are more reddish, suggesting the presence of methane ice. This is probably a thin layer of snow, with the bulk of the structures composed of water ice. The area shows a very different topographic profile to the 'bladed terrain' found at high altitudes close to Pluto's equator, which is thought to be formed by the condensation and sublimation of thick methane deposits.

 
Comparison of Bladed Terrain and Wright Mons region. (a) The bladed terrain deposits form one of the highest elevation areas on Pluto (on the far eastern side of the hemisphere observed by New Horizons during closest approach) and are hypothesized to be a sprawling, concentrated deposit of methane ice, with the bladed texture forming due to sublimation of methane. It may also exist in large areas on the 'ar side' of Pluto that was only observed at low resolution by New Horizons. (b) Although Wright Mons has several different scales and styles of textures, it is not covered by the distinctive blades that characterize the bladed terrain. The longitude and latitude extents are as follows: panels (a) approximately 220–243°E and approximately 10–26°N; panel (b) approximately 165–175°E and approximately 19–26°S. The large arrows in the upper left indicate the approximate direction of the incoming light. Singer et al. (2022).

Patches of nitrogen ice can also be seen in the area around Wright and Picard montes, both in thin layers on the peaks, similar to the distribution of methane, and in depressions where it has apparently pooled. Although conditions on Pluto are cold enough to make water ice an immobile bedrock, nitrogen here is much closer to its melting point, and therefore likely to be capable of some sort of glacier-like plastic flow, which means that nitrogen ice is unlikely to be able to form tall topographic features.

 
Colour information for the Wright Mons region. Darker/lower albedo, redder patches exist primarily on north-facing slopes but there are also more subtle differences in albedo and redness across the region. The region labelled 'A' represents a redder unit transition to less red units at lower elevation (described in the text and methods). The longitude and latitude extents of the image are approximately 160–182°E and 13–31°S. Singer et al. (2022).

For these reasons, Singer et al. assume that the bulk of the Wright and Picard montes structures, and the surrounding topographic features, are composed of water ice, although these is a potential for other materials to have played a role in their formation and evolution. Notably, ammonia has been detected in areas in Pluto's Northern Hemisphere where cryofluids are thought to have erupted through extensional fractures. No ammonia has been detected in the study area, but its presence could potentially be masked by the presence of methane ice. There are also some darker areas on some north-facing slopes, which may indicate the presence of tholins (disordered and insoluble carbon-rich macromolecular materials).

The ices of the Wright Mons region have a slightly reddish tinge to them, indicating the presence of methane, while the terrain to the north is significantly redder, and that to the west is much less red. This may indicate that these regions are of different ages, having been emplaced at different times, from varying source reservoirs, although their precise age-relationship is impossible to determine.

Singer et al. note a number of features which they  believe indicate suggest the study area was not formed by the erosion of an older, elevated terrain. The area around Wright and Picard montes represents a large area of terrain lacking in craters, suggesting that the area was resurfaced in a single or series of events rather than as a consequence of gradual evolution. The distinct hummocky pattern seen in this terrain covers both the plains and the raised topographic features, and is unlike anything seen elsewhere on Pluto. The raised topographic features of the region are variable in elevation, whereas topographic features made from similar materials and exposed to the same conditions tend to erode down to similar heights.

Examination of the available data leads Singer et al. to conclude that Wright Mons, and probably also Picard Mons, formed by the merging of multiple separate rises into a single structure, and that it shares a structure essentially similar to the other topographic features of the area. They note that a smaller dome-like feature, named Coleman Mons, may provide an example of the emplacement of how such structures form. This dome is about 25 km in diameter and 1.5 km high, a structure which could be achieved by water or water-ammonia ice being deposited around a central vent, but would be beyond the ductile strength of softer ices such as nitrogen or methane.

Smaller dome-like feature named Coleman mons. (a) Topography overlain on base image of feature, (b) base image alone, (c) topography alone, (d) perspective view of dome and pit with no vertical exaggeration, (e) view inside the pit, (f) topographic profiles as shown in panels (a)-(c) with 3× vertical exaggeration. Singer et al. (2022).

The hummocky profile of the flanks of Wright Mons and the surrounding terrain suggests some form of viscous flow is occurring. Singer et al. suggest three different possibilities for the formation of these features, namely; the (1) creation of individual small volcanic domes, the (2) viscous extrusion of rapidly cooled lavas analogous to pillow lavas, or the (3) compression of viscous material with a frozen skin analogous to pahoehoe, viscous pressure ridges, or funiscular terrain on Enceladus.

The formation of ridges from pillow-lava like extrusions would require lava ice to be extruded at similar rates and for similar durations, both on the flanks of Wright Mons and on the surrounding plains. Such an even rate of extrusion across a varied terrain seems highly unlikely, and is at odds with observations of volcano behaviour both on Earth and elsewhere in the Solar System. It is possible that the hummocks were formed first, and then uplifted, but this would require an implausibly large mass of material being emplaced from below. Likewise, if the hummocks are contractional or compressional features, then this would imply a high-viscosity layer 8-13 km thick, which is in itself implausible, as well as a force capable of compressing such a layer, for which no obvious cause exists.

In addition, the extrusion of material to the surface to form any of these features would require a system of deep fractures through which the material could escape. Such structures have been seen elsewhere on the surface of Pluto, but not within the subject area, with the only possible fractures being along the large scarp which separates the Wright region from the plateau to the west, and another possible scarp further to the northwest, although other fractures could be hidden beneath extruded material on the surface.

None of the conventional models used to explain the emplacement of volcanic terrains on Earth and other Solar System bodies examined to date appears to fit well with the observed features on Pluto. Furthermore, the features of the area around Wright Mons appear to be quite different from anything seen elsewhere in the Solar System. No obvious vent regions can be seen, and though the surface does appear to be subject to viscous flow, no indication of directionality can be observed, making it difficult to explain the formation of the topology of the region. However, the constructs are compatible with a cryovolcanic origin, fuelled from multiple subsurface sources where the sources are below the constructs. 

The low surface temperature on Pluto, combined with the low predicted heat flux within the Dwarf Planet's interior, makes it very hard to account for the mobilization of subsurface fluid comprised largely of water, but the relative youth of the terrain suggests that a heat-source must be available. While in itself apparently unlikely, such an unexplained heat-source is would help to explain other areas of Pluto with young surfaces comprised of volatile ices, such as Sputnik Planitia.

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