Hills cloud

For the gravitational sphere of astronomical bodies, see Hill sphere.
Artist's view of the Oort cloud, Hills cloud, and Kuiper belt (inset)

In astronomy, the Hills cloud (also called the inner Oort cloud[1] and inner cloud[2]) is a vast theoretical circumstellar disc, interior to the Oort cloud, whose outer border would be located at around 20,000 to 30,000 astronomical units (AU) from the Sun, and whose inner border, less well defined, is hypothetically located at 100-3,000 AU, well beyond planet and Kuiper-belt object orbits, but distances might be much greater. If it exists, the Hills cloud contains roughly 5 times as many comets as the Oort cloud.[3]

Oort cloud comets are continually perturbed by their environment. A non-negligible fraction leaves the Solar System or goes in the inner system. Hence it should have depleted itself long ago, but it has not. The Hills cloud theory addresses the longevity of the Oort cloud by postulating a densely populated inner Oort region. Objects ejected from the Hills cloud are likely to end up in the classical Oort cloud region, maintaining the Oort cloud.[4] It is likely that the Hills cloud is the largest concentration of comets in the whole Solar System.

The existence of the Hills cloud is plausible, since many bodies have been found already. It would be denser than the Oort cloud,[5][6] but much smaller. Gravitational interaction with the closest stars and tidal effects from the galaxy have given circular orbits to the comets in the Oort cloud, which must not be the case for the comets in the Hills cloud. The Hills cloud's total mass is unknown; some scientists think it would be more massive than the Oort cloud.

History

Original Oort cloud model

Ernst Öpik

Between 1932 and 1981, astronomers believed that the Oort cloud (theorized by Ernst Öpik and Jan Oort) and the Kuiper belt were the only comet reserves in the Solar System.

In 1932, Estonian astronomer Ernst Öpik hypothesized that comets were rooted in a cloud orbiting the outer boundary of the Solar System.[7] In 1950, this idea was revived independently by Dutch astronomer Jan Oort to explain an apparent contradiction: comets are destroyed after several passes through the inner Solar System, so if any had existed for several billion years (since the beginning of the Solar System), no more could be observed now.[8]

Oort selected 46 comets for his study that were best observed between 1850 and 1952. The distribution of the inverse of the semi-major axes showed a maximum frequency which suggested the existence of a reservoir of comets between 40,000 and 150,000 AU (0.6 and 2.4 ly) away. This reservoir, located at the limits of the Sun's sphere of influence, would be subject to stellar disturbances, likely to expel cloud comets outwards or inwards.

New model

Jack G. Hills, the astronomer who first proposed the Hills cloud

In the 1980s, astronomers realized that the main cloud could have an internal section that would start at about 3,000 AU from the Sun and continue up to the classic cloud at 20,000 AU. Most estimates place the population of the Hills cloud at about 20 trillion (about five to ten times that of the outer cloud), although the number could be ten times greater than that.[9]

The main model of an "inner cloud" was proposed in 1981 by the astronomer J.G. Hills, from the Los Alamos Laboratory, who gave the region its name. He highlighted that cloud when calculated that the passage of a star near the Solar System could have caused extinctions on Earth, triggering a "comet rain". Indeed, his research suggested that the orbits of most cloud comets have a semi-major axis of 10,000 AU, much closer to the Sun than the proposed distance of the Oort cloud.[5] Moreover, the influence of the surrounding stars and that of the galactic tide should have sent the Oort cloud comets either closer to the Sun or outside of the Solar System. To account for these issues, he proposed the presence of an inner cloud, which would have tens or hundreds of times as many cometary nuclei as the outer halo.[5] Thus, it would be a possible source of new comets to resupply the tenuous outer cloud.

In the following years other astronomers searched for the Hills cloud and studied long-period comets. This was the case with Sidney van den Bergh and Mark E. Bailey, who each suggested the Hills cloud's structure in 1982 and 1983 respectively.[10] In 1986, Bailey stated that the majority of comets in the Solar System were located not in the Oort cloud area, but closer and in an internal cloud, with an orbit with a semi-major axis of 5,000 AU.[11] The research was further expanded upon by studies of Victor Clube and Bill Napier in 1987 and those of 1988 RB Stothers.[10]

However, the Hills cloud regained major interest in 1991,[12] when scientists resumed Hills' theory (excluding documents written by Martin Duncan, Thomas Quinn and Scott Tremaine in 1987, which included Hills' theory and contained additional research).

Characteristics

Structure and composition

Interior and exterior Oort cloud

Oort cloud comets are constantly disturbed by their surroundings and distant objects. A significant number either leave the Solar System or go much closer to the Sun. The Oort cloud should therefore have broken apart long ago, but it still remains intact. The Hills cloud theory could provide an explanation; JG Hills and other scientists suggest that it could replenish the comets in the outer Oort cloud.[13]

It is also likely that the Hills cloud is the largest concentration of comets across the Solar System.[10] The Hills cloud is much denser than the outer Oort cloud; it is somewhere between 5,000 and 20,000 AU in size. In contrast, the Oort cloud is be 20,000 and 50,000 AU (0.3 and 0.8 ly) in size.[14]

The mass of the Hills cloud is not known. Some scientists believe it could be five times more massive than the Oort cloud.[15] Mark E. Bailey estimates the mass of the Hills cloud to be 13.8 Earth masses, if the majority of the bodies are located at 10,000 AU.[11]

If the analyzes of comets are representative of the whole, the vast majority of Hills cloud objects consists of various windows, such as water, methane, ethane, carbon monoxide and hydrogen cyanide.[16] However, the discovery of the object 1996 PW, an asteroid on a typical orbit of a long-period comet, suggests that the cloud may also contain rocky objects.[17]

The carbon analysis and isotopic ratios of nitrogen firstly in the comets of the families of the Oort cloud and the other in the body of the Jupiter area shows little difference between the two, despite their distinctly remote areas. This suggests that both come from a protoplanetary disk,[18] a conclusion also supported by studies of comet cloud sizes and the recent impact study of Comet Tempel 1.[19]

Formation

Many scientists think that the Hills cloud formed from a close (800 AU) encounter between the Sun and another star within the first 800 million years of the Solar System, which could explain the eccentric orbit of 90377 Sedna, which should not be where it is, being neither influenced by Jupiter nor Neptune, nor tidal effects.[20] It is then possible that the Hills cloud would be "younger" than the Oort cloud, which probably formed earlier. Only Sedna bears those irregularities; for 2000 OO67 and 2006 SQ372 this theory is not necessary, because both orbit close to the Solar System's gas giants.

Possible Hills cloud objects

Name Diameter
(km) 		Perihelion
(AU) 		Aphelion
(AU) 		Discovery
V774104 500 to 1000 50 ~1000 2015
2012 VP113 315 to 640 80.5 445 2012
Sedna 995 to 1,060 76.1 935 2003
2000 OO67 28 to 87 20.8 1,014.2 2000
2006 SQ372 50 to 100 24.17 2,005.38 2006

Bodies in the Hills cloud are made mostly of water ice, methane and ammonia. Astronomers suspect many long-period comets originate from the Hills cloud, such as Comet Hyakutake.

In their article announcing the discovery of Sedna, Mike Brown and his colleagues asserted that they observed the first Oort cloud object. They observed that, unlike scattered disc objects like Eris, Sedna's perihelion (76 AU) was too remote for the gravitational influence of Neptune to have played a role in its evolution.[21] The authors regarded Sedna as an "inner Oort cloud object", located on the disk placed between the Kuiper belt and the spherical part of the cloud.[22][23] However, Sedna is much closer to the Sun than expected for objects in the Hills cloud and its inclination is close to that of the planets and the Kuiper belt.

Considerable mystery surrounds 2008 KV42, with its retrograde orbit that could make it originate from the Hills cloud or perhaps the Oort cloud.[24] The same goes for damocloids, whose origins are doubtful, such as the namesake for this category, 5335 Damocles.

Comets

Comet McNaught

Astronomers suspect that several comets come from the same region as the Hills cloud; in particular, they focus on those with aphelia greater than 1,000 AU (which are thus from a farther region than the Kuiper belt), but less than 10,000 AU (or they would otherwise be too close to the outer Oort cloud).

Some famous comets reach great distances and are candidates for Hills cloud objects. For example, Comet Lovejoy, discovered on 15 March 2007 by Australian astronomer Terry Lovejoy, reached an aphelion distance of 2,850 AU.[25] Comet Hyakutake, discovered in 1996 by amateur astronomer Yuji Hyakutake, has an aphelion of 3,410 AU. The Machholz comet, discovered on 27 August 2004 by amateur astronomer Donald Machholz Edward, goes even further, to 4,787 AU.

Comet McNaught, discovered on 7 August 2006 in Australia by Robert H. McNaught, became one of the brightest comets of recent decades, with an aphelion of 4,100 AU. Finally, one of the farthest-known comets is Comet West, discovered by Danish astronomer Richard Martin West at the La Silla Observatory in Chile on 10 August 1975; it reaches 13,560 AU.

Sedna, the first major candidate

Animation of Sedna's orbit (in red) with the Hills cloud (in blue)
Artist's impression of Sedna

Sedna is a minor planet discovered by Michael E. Brown, Chad Trujillo and David L. Rabinowitz on 14 November 2003. It is difficult to determine its shape because of its distance. Spectroscopic measures show that its surface composition is similar to that of other trans-Neptunian objects: it is mainly composed of a mixture of water ices, methane and nitrogen with Tholin. Its surface is one of the reddest in the Solar System.

This is likely the first detection of a Hills cloud object. The area of the Hills cloud is defined as any objects with orbits measuring between 2,000 and 15,000 AU.

Sedna is however much closer to the internal system than the supposed distance of the Hills cloud. The planetoid discovered at a distance of about 13 billion kilometers (90 AU) from the Sun, travels in an elliptical orbit that brings it every 12,260 years only 75 AU from the Sun during its closest approach (the next to be held in 2076), and leads to the more than 987 AU at its farthest point. Unlike comets, this body was not discovered during a stay in the internal system. With a larger diameter than the dwarf planet Ceres, Sedna is also greater than the usual comets.

However, Sedna cannot be considered a Kuiper belt object because its path does not bring it into the region of the Kuiper belt. It is one of those bodies not belonging to any model, which is called a detached object. Most of these objects are also in resonance with Neptune. Sedna never approaches closer than 75 AU and does not resonate with the gaseous planet. Therefore, consider Sedna as an object of the inner Oort cloud may be a possibility.

VP113: cloud confirmation

The discovery of the trans-Neptunian object 2012 VP113 announced on March 26, 2014 changes the vision of trans-Neptunian objects. This comet of 450 km in diameter, unlike the dwarf planets, is not part of the Kuiper belt. Its more distant orbit lies between 80 and 400 AU from the Sun. This discovery allowed to find three, not two reservoirs of comets in the Kuiper belt: the Hills cloud objects and the classic Oort cloud objects. The Hills cloud contains about a thousand bodies of about 1000 km in diameter. Unlike how the Kuiper belt is subjected to the force of Neptune and how the classic Oort cloud is influenced by tidal forces of the Milky Way, the Hills cloud is not subject to any force and is frozen completely.

References

  1. ↑ see Oort cloud
  2. ↑ astronomie, astéroïdes et comètes
  3. ↑ "The Formation and Extent of the Solar System Comet Cloud". SAO/NASA. 1987. Retrieved December 19, 2008.
  4. ↑ J. A. Fernandez (1997). "The Formation of the Oort cloud and the Primitive Galactic Environment". Icarus. Vol. 129 no. 1. pp. 106–119. Bibcode:1997Icar..129..106F. doi:10.1006/icar.1997.5754.
  5. 1 2 3 Jack G. Hills (1981). "Comet showers and the steady-state infall of comets from the Oort Cloud". Astronomical Journal 86: 1730–1740. Bibcode:1981AJ.....86.1730H. doi:10.1086/113058.
  6. ↑ "Planetary Sciences: American and Soviet Research, Proceedings from the U.S.-U.S.S.R. Workshop on Planetary Sciences, p. 251". 1991. Retrieved November 7, 2007.
  7. ↑ Ernst Öpik (1932). "Note on Stellar Perturbations of Nearby Parabolic Orbits". Proceedings of the American Academy of Arts and Sciences 67. pp. 169–182.
  8. ↑ Jan Oort (1950). "The Structure of the Cloud of Comets Surrounding the Solar System and a Hypothesis Concerning its Origin" (pdf). Bull. Astron. Inst. Neth. 11. pp. 91–110.
  9. ↑ Dave E. Matson (May 2012). "Young Earth Evidence - Short-period Comets". Young Earth Creationism.
  10. 1 2 3 Cratering constraints on the inner Oort cloud - Steady-state models, Bailey, M. E. & Stagg, C. R, 1888, page 2
  11. 1 2 Cratering constraints on the inner Oort cloud - Steady-state models, Bailey, M. E. & Stagg, C. R, 1888, page 3
  12. ↑ Loloch.free
  13. ↑ J. A. Fernandez (September 1997). "The Formation of the Oort Cloud and the Primitive Galactic Environment". Icarus 129 (1). pp. 106–119. doi:10.1006/icar.1997.5754.
  14. ↑ Matt Williams (10 August 2015). "What is the Oort Cloud?". Universe Today. Retrieved February 20, 2016.
  15. ↑ The Formation and Extent of the Solar System Comet Cloud
  16. ↑ E. L. Gibb, M. J. Mumma, N. Dello Russo, M. A. DiSanti and K. Magee-Sauer (2003). "Methane in Oort Cloud comets".
  17. ↑ P. R. Weissman; H. F. Levison (October 1997). "Origin and Evolution of the Unusual Object 1996 PW: Asteroids from the Oort Cloud?". Astrophysical Journal Letters 488. pp. L133. doi:10.1086/310940.
  18. ↑ D. Hutsemekers, J. Manfroid, E. Jehin, C. Arpigny, A. Cochran, R. Schulz, J.A. Stüwe, and J.M. Zucconi (2005). "Isotopic abundances of carbon and nitrogen in Jupiter-family and Oort Cloud comets".
  19. ↑ Michael J. Mumma, Michael A. DiSanti, Karen Magee-Sauer et al. (2005). "Parent Volatiles in Comet 9P/Tempel 1: Before and After Impact". Science Express 310 (5746): 270–274.
  20. ↑ Ciel et espace, January 2006
  21. ↑ Mike Brown; David Rabinowitz; Chad Trujillo (2004). "Discovery of a Candidate Inner Oort Cloud Planetoid". Astrophysical Journal 617 (1). pp. 645–649. Bibcode:2004ApJ...617..645B. doi:10.1086/422095.
  22. ↑ David Jewitt; Alessandro Morbidelli; Heike Rauer (2007). Berlin: Springer, ed. Trans-Neptunian Objects and Comets: Saas-Fee Advanced Course 35. Swiss Society for Astrophysics and Astronomy. Berlin. p. 86. ISBN 978-3-540-71957-1. LCCN 2007934029.
  23. ↑ Patryk Sofia Lykawka; Mukai Tadashi (2007). "Dynamical Classification of Trans-Neptunian Objects: Probing their Origin, Evolution, and Interrelation". Icarus 189 (1). pp. 213–232. Bibcode:2007Icar..189..213L. doi:10.1016/j.icarus.2007.01.001.
  24. ↑ Actualité > 2008 KV42, l'astéroïde qui tourne à l'envers
  25. ↑ JPL Small-Body Database Browser C/2007 E2 (Lovejoy)

Further reading

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