A trans-Neptunian object (TNO) is any object in the solar system that orbits the sun at a greater distance on average than Neptune. The Kuiper belt, Scattered disk, and Oort cloud are names for three divisions of this volume of space. Pluto and its moon Charon are trans-Neptunian objects, and if Pluto had been discovered today, it might not have been called a planet. (See the definition of planet.)
The orbit of each of the planets is affected by the gravitational influences of all the other planets. Discrepancies in the early 1900s between the observed and expected orbits of the known planets suggested that there were one or more additional planets beyond Neptune (see Planet X). The search for these led to the discovery of Pluto. Pluto is too small to explain the discrepancies, however, and revised estimates of Neptune's mass showed that the problem was spurious.
It took more than 60 years to discover another TNO (with only the discovery of Pluto’s moon Charon in between). Since 1992 however, more than 1000 objects have been discovered, differing in sizes, orbits and surface composition.
The scattered disk extends to the right, far beyond the diagram, with known objects at mean distances beyond 500 AU (Sedna) and aphelia beyond 1,000 AU ( ).
A fuller list of objects is being compiled in the List of trans-Neptunian objects.
1Included in extended scattered disk by Jewitt (see References).
Given the apparent magnitude (>20) of all but the biggest trans-Neptunian objects, the physical studies are limited to the following:
Studying colours and spectra provides insight into the objects' origin and a potential correlation with other classes of objects, namely centaurs and some satellites of giant planets (Triton, Phoebe), suspected to originate in the Kuiper Belt. However, the interpretations are typically ambiguous as the spectra can fit more than one model of the surface composition and depend on the unknown particle size. More significantly, the optical surfaces of small bodies are subject to modification by intense radiation, solar wind and micrometeorites. Consequently, the thin optical surface layer could be quite different from the regolith underneath , and not representative of the bulk composition of the body.
Colour indices are simple measures of the differences of the apparent magnitude of an object seen through blue (B), visible (V) i.e. green-yellow and red (R) filters. The diagram illustrates known colour indices for all but the biggest objects (in slightly enhanced colour). O. R. Hainaut & A. C. Delsanti (2002) Color of Minor Bodies in the Outer Solar System Astronomy & Astrophysics, 389, 641 datasource For reference, two moons: Triton and Phoebe, the centaur Pholus and planet Mars are plotted (yellow labels, size not to scale).
Correlations between the colours and the orbital characteristics have been studied, to confirm theories of different origin of the different dynamic classes.
Classical objects
Classical objects seem to be composed of two different colour populations: so called cold (inclination <5°) displaying only red colours and hot (higher inclination) population displaying the whole range of colours from blue to very red. A. Doressoundiram, N. Peixinho, C. de Bergh, S. Fornasier, Ph. Thébault, M. A. Barucci and C. Veillet The color distribution in the Edgeworth-Kuiper Belt The Astronomical Journal, 124, pp. 2279-2296. Preprint on arXiv
A recent analysis based on the data from Deep Ecliptic Survey confirms this difference of colours between low inclination objects (named Core) and high inclination (named Halo). Red colours of the Core objects together with their unperturbed orbits suggest that these objects could be a relic of the original population of the Belt. Gulbis, Amanda A. S.; Elliot, J. L.; Kane, Julia F. The color of the Kuiper belt Core Icarus, 183 (july 2006), Issue 1, p. 168-178.
Scattered disk objects
Scattered disk objects show colour resemblances with hot classical objects pointing to a common origin.
The biggest objects Characteristically, big (bright) objects are typically on inclined orbits, while the invariable plane re-groups mostly small and dim objects. With the exception of Sedna, all big TNOs: , , , Charon, and Orcus display neutral colour (infrared index V-I < 0.2), while the relatively dimmer bodies (50000 Quaoar, Ixion, , and Varuna), as well as the population as the whole, are reddish (V-I in 0.3 to 0.6 range). This distinction leads to suggestion that the surface of the largest bodies is covered with ices, hiding the redder, darker areas underneath.
The diagram illustrates the relative sizes, albedos and colours of the biggest TNOs. Also shown, are the known satellites and the exceptional shape of resulting from its rapid rotation. The arc around represents uncertainty given its unknown albedo. The size of follows Brown’s measure (2400 km) based on HST point spread model. The arc around it represents the thermal measure (3000 km) by Bertoldi (see the related section of the article for the references).
Typical models of the surface include water ice, amorphous carbon, silicates and organic macromolecules, named tholins, created by intense radiation. Four major tholins are used to fit the reddening slope:
For other large TNOs, diameters can be estimated by thermal measurements. The intensity of light illuminating the object is known (from its distance to the Sun), and one assumes that most of its surface is in thermal equilibrium (usually not a bad assumption for an airless body). For a known albedo, it is possible to estimate the surface temperature, and correspondingly the intensity of heat radiation. Further, if the size of the object is known, it is possible to predict both the amount of visible light and emitted heat radiation reaching the Earth. A simplifying factor is that the Sun emits almost all of its energy in visible light and at nearby freqencies, while at the cold temperatures of TNOs, the heat radiation is emitted at completely different wavelengths (the far infrared). Thus there are two unknowns (albedo and size), which can be determined by two independent measurements (of the amount of reflected light and emitted infrared heat radiation).
Unfortunately, TNOs are so far from the Sun that they are very cold, hence produce black-body radiation around 60 micrometres in wavelength. This wavelength of light is impossible to observe on the Earth's surface: astronomers thus observe the tail of the black-body radiation in the far infrared. This far infrared radiation is so dim that the thermal method is only applicable to the largest KBOs. For the majority of (small) objects, the diameter is estimated by assuming an albedo. However, the albedos found range from 0.50 down to 0.05 resulting, as example for magnitude of 1.0, in uncertainty from 1200 – 3700 km!*.
In July, 2005, the American scientists submitted a name for the "new planet" to the International Astronomical Union, re-igniting the debate about whether or not Pluto should be considered a planet at all.
The brightest known TNOs (with absolute magnitudes < 4.0), are:
| Permanent Designation | Provisional Designation | Absolute magnitude | Albedo | Equatorial diameter (km) | Semimajor axis (AU) | Class | Discovery date | Discoverer(s) | Diameter method |
|---|---|---|---|---|---|---|---|---|---|
| −1.2 | ~0.55 ± 0.15(thermal) | 3000 ± 400 | 67.7 | SDO | 2005 | M. Brown, C. Trujillo & D. Rabinowitz | thermal | ||
| Pluto | −1.0 | 0.49 to 0.66 | 2306 ± 20 | 39.4 | KBO | 1930 | C. Tombaugh | occultation | |
| −0.3 | 0.8 ± 0.2 (assumed) | 1800 ± 200 | 45.7 | KBO | 2005 | M. Brown, C. Trujillo & D. Rabinowitz | assumed albedo | ||
| 0.1 | 0.7 ± 0.1 | ~1500 | 43.3 | KBO | 2005 | M. Brown, C. Trujillo & D. Rabinowitz | density inferred from rotation & oblate shape | ||
| Charon | S/1978 P 1 | 1 | 0.36 to 0.39 | 1205 ± 2 | 39.4 | KBO satellite | 1978 | J. Christy | occultation |
| (90377) Sedna | 1.6 | >0.2 (assumed) | <1800, >1180 | 502.0 | SDO? | 2003 | M. Brown, C. Trujillo & D. Rabinowitz | thermal | |
| (90482) Orcus | 2004 DW | 2.3 | 0.1 (assumed) | ~1500 | 39.4 | KBO | 2004 | M. Brown, C. Trujillo & D. Rabinowitz | assumed albedo |
| (50000) Quaoar | 2.6 | 0.10 ± 0.03 | 1260 ± 190 | 43.5 | KBO | 2002 | C. Trujillo & M. Brown | disk resolved | |
| (28978) Ixion | 3.2 | 0.25 – 0.50 | 400 – 550 | 39.6 | KBO | 2001 | Deep Ecliptic Survey | thermal | |
| 55636 | 3.3 | > 0.19 | < 709 | 43.1 | KBO | 2002 | NEAT | thermal | |
| 55565 | 3.3 | 0.14 – 0.20 | 650 – 750 | 47.4 | KBO | 2002 | C. Trujillo, M. Brown, E. Helin, S. Pravdo, K. Lawrence & M. Hicks / Palomar Observatory | thermal | |
| 55637 | 3.6 | 0.08? | ~910 | 42.5 | KBO | 2002 | A. Descour / Spacewatch | assumed albedo | |
| (20000) Varuna | 3.7 | 0.12 – 0.30 | 1060 | 43.0 | KBO | 2000 | R. McMillan | thermal | |
| 3.8 | 0.1 (assumed) | 730? | 41.8 | KBO | assumed albedo | ||||
| 3.8 | 0.1 (assumed) | 730? | 45.5 | KBO | assumed albedo | ||||
| 3.9 | 0.1 (assumed) | 700? | 39.6 | KBO | assumed albedo | ||||
| 84522 | 3.9 | > 0.03 | < 1211 | 55.1 | SDO | 2002 | NEAT | thermal |
The list has been sorted by increasing absolute magnitude. Estimated diameter is greatly affected by surface albedo which has often been assumed, not measured. Some potentially large Kuiper belt objects have not been included.
Sources: Grundy et al. Diverse Albedos of Small Trans-Neptunian Objects Icarus Notes. Preprint on arXiv (pdf) Dale P. Cruikshank et al. Albedos, Diameters (and a Density) of Kuiper Belt and Centaur Objects from a session of the 37th meeting of the Division for Planetary Sciences of the American Astronomical Society and the Royal Astronomical Society (September 2005, Cambridge, UK) Abstract The original press release announcing the measuring of the albedo of 2003 UB313 by Bertoldi et al. MPC Circular 2006-A28 for 2003 MW12 data
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