Showing posts with label New Horizons Probe. Show all posts
Showing posts with label New Horizons Probe. Show all posts

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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Wednesday, 9 March 2016

Sputnik Planum: An apparently young feature on the surface of Pluto.

Pluto was the first known and is one of the largest bodies in the Kuiper Belt, a field of Dwarf Planets and smaller bodies beyond Neptune which are thought to have been beyond the zone of true-planet formation, and therefore to reflect the nature of the early Solar System. In July 2015 the New Horizons spacecraft flew past Pluto, making a detailed survey of the surface of the body, the first such study of any Kuiper Belt object. This survey revealed, amongst other features, an area which has been informally named Sputnik Planum, a field of nitrogen ice covering apparently 2.5% of Pluto's surface, which is devoid of impact craters visible at observed resolutions. This is surprising as Pluto sweeps through an area of the Kuiper Belt where it is predicted to encounter many smaller objects which impact on its surface, creating a pattern of craters seen on other parts of the Dwarf Planet. The absence of craters on Sputnik Planum sugests that this area must be relatively young, as no known phenomenon can cause impact events to preferentially avoid one area on the surface of a body.

In a paper published on the online arXiv database at Cornell University Library on 12 January 2016 and in the journal PLoS One on 20 January 2016, David Trilling of the Department of Physics and Astronomy at Northern Arizona University and the Lowell Observatory discuses the nature of Sputnik Planum and attempts to assess how this area could be resurfaced to remove craters.

The entire surface of Sputnik Planum has been imaged at a resolution of 400 m/pixel, at which level of detail it ought to be possible to detect a crater 2 km in diameter, which would be caused by an impactor of roughly 400 m. About 20% of Sputnik Planum has been imaged at the higher resolution of 125 m/pixel, at which resolution it should be possible to detect a crater 625 m in diameter, which would be caused by an impactor approximately 90 m across. No craters were detected on the surface of Sputnik Planum at either resolution.

Low resolution image of the surface of Pluto. Sputnik Planum is the white area at the center of the image. New Horizons.

Trilling estimates that at the predicted gravity of Pluto nitrogen ice with a density of 1000 kg/m2, a crater 2 km across should be removed by viscous relaxation (although a solid ice does flow very slowly) within 10 million years, which he calculates to be the upper age of Sputnik Planum. He also notes that two other possible surface processes could potentially be speeding up this crater removal; active convective overturn, in which the nitrogen ice is being heated from below by some heat-source within Pluto rather than simply by the Sun, of cryovolcanism, in which melted nitrogen is reaching the surface from a buried reservoir, which would also require a heat-source within Pluto.

Trilling also notes that these figures are based uppon current estimates of the number and density of objects within the Kuiper Belt, figures which have a wide margin of error. Potentially the number of objects could be ten times lower, in which case the number of impacts would be ten times lower and Sputnik Planum could have a surface age of about 100 million years, allowing for much slower surface reworking, or ten times as high, in which case the number of impacts would also be ten times as high, and the surface of Sputnik Planum might only be a million years old, strongly suggesting reworking by a process other than viscous relaxation.

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http://sciencythoughts.blogspot.co.uk/2015/04/assessing-composition-of-ices-on.htmlAssessing the composition of ices on the surface of Makemake.                                  The Dwarf Planet Makemake is one of the three largest Trans-Neptunian Objects, with a diameter of about 1400 km, along with Pluto and Eris (2370 km 2330 km respectively). Makemake is thought to have a...
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Tuesday, 9 September 2014

Observations of New Horizons candidate bodies with the Hubble Space Telescope.

The New Horizons Spacecraft was launched in January 2006, and is due to pass through the Pluto System (Pluto is now recognized to be a cluster of at least six objects rather than a single large body) in July 2015. After this it is hoped that New Horizons will be able to adjust its path in order to visit one of the smaller bodies of the Kuiper Belt, possibly the only such body that will be visited by a probe in the lifetime of anyone currently alive. As well as hopefully visiting a small Kuiper Belt object, New Horizons will pass within 0.3 AU (30% of the distance of the Earth and the Sun) of a larger number of bodies, providing the opportunity to provide clearer observations than possible from any Earth-based telescope, or space telescope in a near-Earth orbit.

Attempts to locate Kuiper Belt objects that would be within range of New Horizons observation began in 2004, though the wide area of space that required surveying in order to detect bodies that would be close to the New Horizons path in 2015/16, combined with the smallness of the telescopes available at the time, prevented the production of useful results. By 2011 the area of space that needed to be searched had shrunk considerably, and it was possible to use larger telescopes in the search for target bodies, notably the 8.4-m Subaru Telescope and 6.5-m Magellan Telescopes. As yet no object has been located that would be within range of a a New Horizons flyby, but a number of candidate objects for longer range observation have been identified.

In a paper published on the arXiv database at Cornell University Library on 28 May 2014, and accepted for publication in the journal Icarus, Susan Benecchi of the Planetary Science Institute and the Department of Terrestrial Magnetism at the Carnegie Institution of Washington, Keith Noll of the Goddard Space Flight Center, Harold Weaver of the Space Department at the Applied Physics Laboratory at Johns Hopkins University, John Spencer, Alan Stern and Marc Buie of the Southwest Research Institute and Alex Parker of the Department of Astronomy at the University of California, Berkeley describe the results of follow-up observations of four objects discovered by the ground based survey with the Hubble Space Telescope.

One of the objects found by the Earth-based survey could not be recovered by the Hubble Space Telescope. 2011 JW31 was discovered on 4 May 2011 (the name 2011 JW31 implies the 797th object discovered in the first half of May 2011), and is thought to have a 306 year orbital period and an elliptical orbit titled at an angle of 1.9° to the plane of the Solar System that takes it from 42.9 AU from the Sun (i.e. 42.9 times as far from the Sun as the Earth) to 47.9 AU from the Sun (47.9 times as far as the Earth). However it was the faintest of the objects included in the study, and was predicted to be in front of a cluster of faint stars at the time of observation, making it hard to observe and poorly understood.

The Calculated orbit 2011 JW31. JPL Small Body Database Browser.

2011 JY31 was discovered on 4 May 2011 (the name 2011 JY31 implies the 799th object discovered in the first half of May 2011), and re-observed 6, 34, 65 and 365 days after its initial discovery, so its parameters were reasonably well understood. Hubble Was able to observe it 510 days after its initial discovery, on 18 September 2012, within 0.4 arcseconds of its predicted position (the sky is a sphere split into 360 degrees by astronomers, each degree is subdivided into 60 arcminutes, and each arcminute into 60 arcseconds), which corresponds to about 14 000 km at a distance of 44 AU (44 times the average distance between the Earth and the Sun). 

Hubble Space Telescope image of 2011 JY31. Benecchi et al. (2014).

2013 JW31 appears to be a single body; Hubble was unable to observe any potential companion object within 0.02 arcseconds (700 km at 44 AU). It has a 291 year orbital period and an elliptical orbit tilted at an angle of 2.6° to the plane of the Solar System that takes it from 41.5-46.3 AU from the Sun (41.5-46.3 times as far as Earth), and will have its closest encounter with New Horizons on 27 September 2018, when it will be 0.16 AU (23 940 000 km) from the spacecraft.

The calculated orbit of 2011 JW31. JPL Small Body Database Browser.

2011 HZ102 was discovered on 28 April 2011 (the name 2011 HZ means the 2575th asteroid discovered in the second half of April 2011). It was re-observed by Hubble 17 September 2012.

Hubble Space Telescope image of 2011 HZ102. Benecchi et al. (2014).

2011 HZ102 also appears to be a single body; Hubble was again unable to observe any potential companion object within 0.02 arcseconds (700 km at 44 AU). It has a 283 year orbital period and an elliptical orbit tilted at an angle of 2.4° to the plane of the Solar System that takes it from 42.6-43.6 AU from the Sun (42.6-43.6 times as far as Earth), and will have its closest encounter with New Horizons on 16 December 2018, when it will be 0.15-0.16 AU (22 400 000-23 940 000 km) from the spacecraft.

The calculated orbit of 2011 HZ102. JPL Small Body Database Browser.

2013 LU35 was discovered on 5 June 2013 (the name 2013 LU35 implies the 895th asteroid discovered in the first half of June 2013). It was reobserved by Hubble on 27 September 2013.

Hubble Space Telescope image of 2013 LU35. Benecchi et al. (2014).

2013 LU35 also appears to be a single body; Hubble was again unable to observe any potential companion object within 0.02 arcseconds (700 km at 44 AU). It has a 288 year orbital period, and an eccentric orbit tilted at an angle of 3° to the plane of the Solar System that takes it from 41.3-45.9 AU from the Sun (41.3-45.9 times as far as Earth), and will have its closest encounter with New Horizons between 4 February and 12 October 2019, when it will be 0.30-0.38 AU (44 880 000-56 850 000 km) from the spacecraft.

The calculated orbit of 2013 LU35. JPL Small Body Database Browser.

A fifth body, 2011 HJ103, will also come within long range observation distance of New Horizons, though this was not observed by Hubble. 2011 HJ103 was discovered on 28 April 2011 (the name 2011 HJ103 implies the 2585th asteroid discovered in the second half of April 2011). It is calculated to have a 314 year orbital period, and an eccentric orbit tilted at an angle of 5.3° to the plane of the Solar System that takes it from 40.3-52.2 AU from the Sun (40.3-52.2 times as far as Earth). It is predicted to be at its closest to New Horizons between 24 February 2017 and 10 January 2018, when it will be 0.19-0.43 AU (28 420 000-64 330 000 km) from the spacecraft.

The calculated orbit of 2011 HJ103. JPL Small Body Database Browser.

See also…


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