Irregular moon

This diagram shows the orbits of Saturn's irregular satellites. At the centre, the orbit of Titan, a regular satellite, is highlighted in red for comparison.

In astronomy, an irregular moon, irregular satellite or irregular natural satellite is a natural satellite following a distant, inclined, and often eccentric and retrograde orbit. They have been captured by their parent planet, unlike regular satellites, which formed in orbit around them.

Counting Triton, 115 irregular satellites have been discovered, orbiting all four of the giant planets (Jupiter, Saturn, Uranus and Neptune). The largest of each planet are Himalia of Jupiter, Phoebe of Saturn, Sycorax of Uranus, and Triton of Neptune. It is currently thought that the irregular satellites were captured from heliocentric orbits near their current locations, shortly after the formation of their parent planet. An alternative theory, that they originated further out in the Kuiper belt, is not supported by current observations.

Definition

Planet rH, 106 km[1] rmin, km[1] Number
Jupiter 55 1.5 61
Saturn 69 3 38
Uranus 73 7 9
Neptune 116 16 7 (including Triton)

There is no widely accepted precise definition of an irregular satellite. Informally, satellites are considered irregular if they are far enough from the planet that the precession of their orbital plane is primarily controlled by the Sun.

In practice, the satellite's semi-major axis is compared with the radius of the planet's Hill sphere (that is, the sphere of its gravitational influence), . Irregular satellites have semi-major axes greater than 0.05 with apoapses extending as far as to 0.65 .[1] The radius of the Hill sphere is given in the adjacent table.

Orbits

Current distribution

Irregular satellites of Jupiter (red), Saturn (yellow), Uranus (green) and Neptune (blue) (excluding Triton). The horizontal axis shows their distance from the planet (semi-major axis) expressed as a fraction of the planet’s Hill sphere's radius. The vertical axis shows their orbital inclination. Points or circles represent their relative sizes.

The orbits of the known irregular satellites are extremely diverse, but there are certain patterns. Retrograde orbits are far more common (83%) than prograde orbits. No satellites are known with orbital inclinations higher than 55° (or smaller than 130° for retrograde satellites). In addition, some groupings can be identified, in which one large satellite shares a similar orbit with a few smaller ones.

Given their distance from the planet, the orbits of the outer satellites are highly perturbed by the Sun and their orbital elements change widely over short intervals. The semi-major axis of Pasiphae, for example, changes as much as 1.5 Gm in two years (single orbit), the inclination around 10°, and the eccentricity as much as 0.4 in 24 years (twice Jupiter’s orbit period).[2] Consequently, mean orbital elements (averaged over time) are used to identify the groupings rather than osculating elements at the given date. (Similarly, the proper orbital elements are used to determine the families of asteroids.)

Origin

Irregular satellites have been captured from heliocentric orbits. (Indeed, it appears that the irregular moons of the giant planets, the Jovian and Neptunian trojans, and grey Kuiper belt objects have a similar origin.[3]) For this to occur, at least one of three things needs to have happened:

After the capture, some of the satellites could break up leading to groupings of smaller moons following similar orbits. Resonances could further modify the orbits making these groupings less recognizable.

Long-term stability

Phoebe, Saturn's largest irregular satellite

The current orbits of the irregular moons are stable, in spite of substantial perturbations near the apocenter.[5] The cause of this stability in a number of irregulars is the fact that they orbit with a secular or Kozai resonance.[6]

In addition, simulations indicate the following conclusions:

Increasing eccentricity results in smaller pericenters and large apocenters. The satellites enter the zone of the regular (larger) moons and are lost or ejected via collision and close encounters. Alternatively, the increasing perturbations by the Sun at the growing apocenters push them beyond the Hill sphere.

Retrograde satellites can be found further from the planet than prograde ones. Detailed numerical integrations have shown this asymmetry. The limits are a complicated function of the inclination and eccentricity, but in general, prograde orbits with semi-major axes up to 0.47 rH (Hill sphere radius) can be stable, whereas for retrograde orbits stability can extend out to 0.67 rH.

The boundary for the semimajor axis is surprisingly sharp for the prograde satellites. A satellite on a prograde, circular orbit (inclination=0°) placed at 0.5 rH would leave Jupiter in as little as forty years. The effect can be explained by so-called evection resonance. The apocenter of the satellite, where the planet’s grip on the moon is at its weakest, gets locked in resonance with the position of the Sun. The effects of the perturbation accumulate at each passage pushing the satellite even further outwards.[5]

The asymmetry between the prograde and retrograde satellites can be explained very intuitively by the Coriolis acceleration in the frame rotating with the planet. For the prograde satellites the acceleration points outward and for the retrograde it points inward, stabilising the satellite.[7]

Physical characteristics

Size

Illustration of the power law. The number of objects depends on their size.

Given their greater distance from Earth, the known irregular satellites of Uranus and Neptune are larger than those of Jupiter and Saturn; smaller ones probably exist but have not yet been observed. However, with this observational bias in mind, the size distribution is similar for all four giant planets.

Typically, the relation expressing the number of objects of the diameter smaller or equal to is approximated by a power law:

with q defining the slope.

A shallow power law (q~2) is observed for sizes 10 to 100 km but steeper (q~3.5) for objects smaller than 10 km .

For comparison, the distribution of Kuiper belt objects is much steeper (q~4), i.e. for one object of 1000 km there are a thousand objects with a diameter of 100 km. The size distribution provides insights into the possible origin (capture, collision/break-up or accretion).

For every object of 100 km, ten objects of 10 km can be found.
For one object of 10 km, some 140 objects of 1 km can be found.

Colours

This diagram illustrates the differences of colour in the irregular satellites of Jupiter (red labels), Saturn (yellow) and Uranus (green). Only irregulars with known colour indices are shown. For reference, the centaur Pholus and three classical Kuiper belt objects are also plotted (grey labels, size not to scale). For comparison, see also colours of centaurs and KBOs.

The colours of irregular satellites can be studied via colour indices: simple measures of differences of the apparent magnitude of an object through blue (B), visible i.e. green-yellow (V), and red (R) filters. The observed colours of the irregular satellites vary from neutral (greyish) to reddish (but not as red as the colours of some Kuiper belt objects).

albedo[8] neutral reddish red
low C 3–8% P 2–6% D 2–5%
medium M 10–18% A 13–35%
high E 25–60%

Each planet's system displays slightly different characteristics. Jupiter's irregulars are grey to slightly red, consistent with C, P and D-type asteroids.[9] Some groups of satellites are observed to display similar colours (see later sections). Saturn's irregulars are slightly redder than those of Jupiter.

The large Uranian irregular satellites (Sycorax and Caliban) are light red, whereas the smaller Prospero and Setebos are grey, as are the Neptunian satellites Nereid and Halimede.[10]

Spectra

With the current resolution, the visible and near-infrared spectra of most satellites appear featureless. So far, water ice has been inferred on Phoebe and Nereid and features attributed to aqueous alteration were found on Himalia.

Rotation

Regular satellites are usually tidally locked (that is, their orbit is synchronous with their rotation so that they only show one face toward their parent planet). In contrast, tidal forces on the irregular satellites are negligible given their distance from the planet, and rotation periods in the range of only ten hours have been measured for the biggest moons Himalia, Phoebe and Nereid (to compare with their orbital periods of hundreds of days). Such rotation rates are in the same range that is typical for asteroids.

Families with a common origin

Some irregular satellites appear to orbit in 'groups', in which several satellites share similar orbits. The leading theory is that these objects constitute collisional families, parts of a larger body that broke up.

Dynamic groupings

Simple collision models can be used to estimate the possible dispersion of the orbital parameters given a velocity impulse Δv. Applying these models to the known orbital parameters makes it possible to estimate the Δv necessary to create the observed dispersion. A Δv of tens of meters per seconds (5–50 m/s) could result from a break-up. Dynamical groupings of irregular satellites can be identified using these criteria and the likelihood of the common origin from a break-up evaluated.[11]

When the dispersion of the orbits is too wide (i.e. it would require Δv in the order of hundreds of m/s)

Colour groupings

When the colours and spectra of the satellites are known, the homogeneity of these data for all the members of a given grouping is a substantial argument for a common origin. However, lack of precision in the available data often makes it difficult to draw statistically significant conclusions. In addition, the observed colours are not necessarily representative of the bulk composition of the satellite.

Observed groupings

Irregular satellites of Jupiter

The orbits of Jupiter's irregular satellites, showing how they cluster into groups. Satellites are represented by circles that indicate their relative sizes. An object's position on the horizontal axis shows its distance from Jupiter. Its position on the vertical axis indicates its orbital inclination. The yellow lines indicate its orbital eccentricity (i.e. the extent to which its distance from Jupiter varies during its orbit).

Typically, the following groupings are listed (dynamically tight groups displaying homogenous colours are listed in bold)

Sinope, sometimes included into the Pasiphae group, is red and given the difference in inclination, it could be captured independently.[9][13] Pasiphae and Sinope are also trapped in secular resonances with Jupiter.[5][11]

Irregular satellites of Saturn

Irregular satellites of Saturn, showing how they cluster into groups. For explanation, see Jupiter diagram

The following groupings are commonly listed for Saturn's satellites:

Irregulars of Uranus and Neptune

Irregular satellites of Uranus (green) and Neptune (blue) (excluding Triton). For explanation, see Jupiter diagram
Planet rmin[1]
Jupiter 1.5 km
Saturn 3 km
Uranus 7 km
Neptune 16 km

According to current knowledge, the number of irregular satellites orbiting Uranus and Neptune is smaller than that of Jupiter and Saturn. However, it is thought that this is simply a result of observational difficulties due to the greater distance of Uranus and Neptune. The table at right shows the minimum radius (rmin) of satellites that can be detected with current technology, assuming an albedo of 0.04; thus, there are almost certainly small Uranian and Neptunian moons that cannot yet be seen.

Due to the smaller numbers, statistically significant conclusions about the groupings are difficult. A single origin for the retrograde irregulars of Uranus seems unlikely given a dispersion of the orbital parameters that would require high impulse (Δv ≈ 300 km), implying a large diameter of the impactor (395 km), which is incompatible in turn with the size distribution of the fragments. Instead, the existence of two groupings has been speculated:[9]

These two groups are distinct (with 3σ confidence) in their distance from Uranus and in their eccentricity.[14] However, these groupings are not directly supported by the observed colours: Caliban and Sycorax appear light red, whereas the smaller moons are grey.[10]

For Neptune, a possible common origin of Psamathe and Neso has been noted.[15] Given the similar (grey) colours, it was also suggested that Halimede could be a fragment of Nereid.[10] The two satellites have had a very high probability (41%) of collision over the age of the solar system.[16]

Exploration

Distant Cassini image of Himalia

To date, the only irregular satellites to have been visited by a spacecraft are Triton and Phoebe, the largest of Neptune's and Saturn's irregulars respectively. Triton was imaged by Voyager 2 in 1989 and Phoebe by the Cassini probe in 2004. Cassini also captured a distant, low-resolution image of Jupiter's Himalia in 2000. There are no spacecraft planned to visit any irregular satellites in the future.

References

  1. 1 2 3 4 Sheppard, S. S. (2006). "Outer irregular satellites of the planets and their relationship with asteroids, comets and Kuiper Belt objects". Proceedings of the International Astronomical Union. 1: 319. arXiv:astro-ph/0605041Freely accessible. doi:10.1017/S1743921305006824.
  2. 1 2 Carruba, V.; Burns, J. A.; Nicholson, P. D.; Gladman, B. J.; On the Inclination Distribution of the Jovian Irregular Satellites, Icarus, 158 (2002), pp. 434–449 (pdf)
  3. Sheppard, S. S.; Trujillo, C. A. (2006). "A Thick Cloud of Neptune Trojans and Their Colors" (PDF). Science. 313 (5786): 511–514. Bibcode:2006Sci...313..511S. PMID 16778021. doi:10.1126/science.1127173.
  4. Agnor, C. B. and Hamilton, D. P. (2006). "Neptune's capture of its moon Triton in a binary-planet gravitational encounter". Nature. 441 (7090): 192–4. Bibcode:2006Natur.441..192A. PMID 16688170. doi:10.1038/nature04792.
  5. 1 2 3 Nesvorný, D.; Alvarellos, J. L. A.; Dones, L.; and Levison, H. F.; Orbital and Collisional Evolution of the Irregular Satellites, The Astronomical Journal,126 (2003), pp. 398–429.
  6. Ćuk, M. and Burns, J. A.; A New Model for the Secular Behavior of the Irregular Satellites, American Astronomical Society, DDA meeting #35, #09.03; Bulletin of the American Astronomical Society, Vol. 36, p. 864 (preprint)
  7. Hamilton, D. P.; and Burns, J. A.; Orbital Stability Zones about Asteroids, Icarus 92 (1991), pp. 118–131D.
  8. Based on the definitions from Oxford Dictionary of Astronomy, ISBN 0-19-211596-0
  9. 1 2 3 Grav, T.; Holman, M. J.; Gladman, B. J.; and Aksnes, K.; Photometric survey of the irregular satellites, Icarus, 166 (2003), pp. 33–45 (preprint).
  10. 1 2 3 Grav, Tommy; Holman, Matthew J.; Fraser, Wesley C. (2004-09-20). "Photometry of Irregular Satellites of Uranus and Neptune". The Astrophysical Journal. 613 (1): L77–L80. Bibcode:2004ApJ...613L..77G. arXiv:astro-ph/0405605Freely accessible. doi:10.1086/424997.
  11. 1 2 Nesvorný, D.; Beaugé, C.; and Dones, L.; Collisional Origin of Families of Irregular Satellites, The Astronomical Journal, 127 (2004), pp. 1768–1783 (pdf)
  12. 1 2 Grav, T.; and Holman, M. J.; Near-Infrared Photometry of the Irregular Satellites of Jupiter and Saturn,The Astrophysical Journal, 605, (2004), pp. L141–L144 (preprint).
  13. Sheppard, S. S.; Jewitt, D. C. (2003). "An abundant population of small irregular satellites around Jupiter" (pdf). Nature. 423 (6937): 261–263. Bibcode:2003Natur.423..261S. PMID 12748634. doi:10.1038/nature01584.
  14. Sheppard, S. S.; Jewitt, D.; Kleyna, J. (2005). "An Ultradeep Survey for Irregular Satellites of Uranus: Limits to Completeness". The Astronomical Journal. 129: 518. Bibcode:2005AJ....129..518S. arXiv:astro-ph/0410059Freely accessible. doi:10.1086/426329.
  15. Sheppard, Scott S.; Jewitt, David C.; Kleyna, Jan (2006). "A Survey for "Normal" Irregular Satellites around Neptune: Limits to Completeness". The Astronomical Journal. 132: 171–176. Bibcode:2006AJ....132..171S. arXiv:astro-ph/0604552Freely accessible. doi:10.1086/504799.
  16. Holman, M. J.; Kavelaars, J. J.; Grav, T.; et al. (2004). "Discovery of five irregular moons of Neptune" (PDF). Nature. 430 (7002): 865–867. Bibcode:2004Natur.430..865H. PMID 15318214. doi:10.1038/nature02832. Retrieved 24 October 2011.
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