Himalia (Moon)
Himalia is the largest irregular satellite of Jupiter and the principal member of the prograde Himalia collisional family, exhibiting a dark carbonaceous spectrum consistent with a captured outer main-belt or Trojan asteroid.
Himalia (designated Jupiter VI) is the largest irregular satellite of Jupiter and the sixth largest Jovian moon overall after the four Galilean satellites and only slightly smaller in longest dimension than inner Amalthea, though possessing a greater total mass and volume. Orbiting on a moderately eccentric, highly inclined prograde path at a mean distance of approximately 11.45 million km from Jupiter, Himalia serves as the archetype and dominant parent body of the Himalia groupโa tightly clustered dynamical family of prograde outer moons created by the ancient collisional breakup of a captured carbonaceous asteroid. In modern planetary astronomy, Himalia provides a key laboratory for studying heliocentric capture mechanisms in the early giant-planet subnebula and the collisional evolution of outer satellite swarms.
Discovery and Observational History
Unlike the four Galilean moons discovered visually by Galileo Galilei in 1610 and inner Amalthea spotted visually by Edward Emerson Barnard in 1892, Himalia was the first Jovian satellite discovered via astrophotography. On December 3, 1904, Charles Dillon Perrine detected the 14.6-magnitude satellite on glass photographic plates exposed with the 36-inch Crossley Reflector at Lick Observatory in California. Because orbital determinations swiftly revealed that the object traveled at more than six times the distance of Callisto on an orbit inclined by roughly 28ยฐ to Jupiter's equator, Perrine's discovery established the existence of a distinct population of distant, captured irregular satellites around Jupiter.
For seventy years, the satellite was known simply as Jupiter VI (or occasionally Hestia in informal literature) until October 1975, when the International Astronomical Union formally approved the name Himalia, after the nymph of Rhodes in Greek mythology who bore three sons to Zeus. Following IAU naming conventions for Jovian irregular satellites, members of the prograde Himalia group receive names ending in the letter -a (such as Elara, Lysithea, Leda, Dia, Pandia, and Ersa), whereas outer retrograde satellites receive names ending in -e.
In December 2000, the Cassini spacecraft acquired the first disk-resolved images of Himalia from a distance of 4.4 million km during its gravitational-assist flyby of Jupiter en route to Saturn. Six years later, in February 2007, the New Horizons spacecraft imaged Himalia with its Long Range Reconnaissance Imager (LORRI) from distances between 4.7 and 8.0 million km, constraining its phase curve, rotational light curve, and irregular silhouette.
Orbital Mechanics and the Himalia Collisional Family
Himalia revolves around Jupiter in a prograde direction with a mean semi-major axis of 11,451,970 km (approximately 160 Jovian radii, or roughly 21.5% of Jupiter's Hill sphere radius of ~53 million km), completing one orbit every 250.23 Earth days (~8.2 months). Because of its substantial distance from the planet, solar gravitational perturbations induce strong secular and periodic variations in its orbital mechanics. Over multi-century integrations, Himalia's orbital eccentricity oscillates between 0.11 and 0.25 (around a mean of ~0.160), while its inclination relative to the ecliptic fluctuates between 25.8ยฐ and 30.8ยฐ (averaging ~27.5ยฐ).
| Parameter | Value |
|---|---|
| Designation | Jupiter VI (Himalia) |
| Cassini/Ground Dimensions (km) | ~206 ร 141 ร 120 (mean diameter ~140โ170 km) |
| Estimated Mass (kg) | (4.2 ยฑ 0.6) ร 1018 |
| Estimated Bulk Density (g/cm3) | 1.63โ2.60 (from asteroid perturbations) |
| Mean Semi-Major Axis (km) | 11,451,971 |
| Mean Orbital Period (days) | 250.23 |
| Mean Eccentricity | 0.1598 |
| Mean Inclination to Ecliptic | 27.50ยฐ |
| Rotation Period (hours) | 7.7819 ยฑ 0.0005 |
| Visual Geometric Albedo | 0.04โ0.057 |
Unlike tidally locked inner moons that rotate synchronously with their orbital periods, Himalia lies far beyond the regime of planetary tidal despinning and rotates rapidly on its axis once every 7.7819 hours, producing a photometric light-curve amplitude of ~0.12โ0.20 magnitudes due to its elongated shape.
Himalia contains more than 85% of the total mass of the Himalia group, a cluster of at least seven confirmed prograde satellitesโHimalia, Elara (~80 km diameter), Lysithea (~42 km), Leda (~21 km), Dia (~4 km), Pandia (~3 km), and Ersa (~3 km)โthat share semi-major axes between 11.15 and 11.75 million km, inclinations between 26.6ยฐ and 28.6ยฐ, and eccentricities between 0.11 and 0.21. The velocity dispersion among these moons is approximately 50 to 150 m/s, matching the expected velocity distribution of fragments ejected from the hypervelocity disruption of a single progenitor asteroid roughly 180โ200 km in diameter.
Furthermore, Galileo and Cassini impact-dust observations, combined with orbital integrations of the 4-km fragment Dia, suggest that ongoing secondary collisions within the Himalia swarm generate a tenuous, transient dust ring around Jupiter at 11.4 million kmโan outer-system analogue to how Neptune's Nereid and the Irregular Moons of Uranus (Sycorax and Caliban) record early outer solar system bombardment.
Mass Estimation via Mutual Satellite Perturbations
Because no spacecraft has ever executed a close flyby of Himalia within a few thousand kilometers, its mass cannot be measured directly from spacecraft Doppler tracking. Instead, astronomers have determined Himalia's gravitational parameter (GM) by analyzing the long-term astrometric perturbations that Himalia exerts on the other members of its collisional family (particularly Elara and Lysithea) over more than a century of photographic and CCD observations.
In 2005, Nikolay Emelyanov analyzed 100 years of astrometric observations of Elara and Lysithea during close approaches to Himalia, deriving GM = 0.28 ยฑ 0.04 km3/s2, corresponding to a mass of (4.2 ยฑ 0.6) ร 1018 kg. Subsequent astrometric solutions incorporating Gaia stellar reference catalogs and close encounters with seven other irregular Jovian moons have yielded values in the range GM โ 0.21โ0.28 km3/s2. Depending on whether one adopts the larger radiometric diameter (~170 km) or the smaller stellar occultation and shape-model effective diameter (~139.6 km measured during the May 2018 stellar occultation across the United States), Himalia's bulk density falls between 1.63 and 2.60 g/cm3, consistent with a hydrated C-type carbonaceous asteroid with moderate internal porosity.
Surface Composition and Capture Origin
Visible and near-infrared reflectance spectroscopy from ground-based telescopes and the Cassini Visual and Infrared Mapping Spectrometer (VIMS) show that Himalia is exceedingly dark, with a visual geometric albedo between 0.040 and 0.057, and displays a neutral-to-slightly-bluish visible continuum slope matching C-type or B-type carbonaceous asteroids of the outer main belt (specifically the 24 Themis or 10 Hygiea asteroid families).
High-sensitivity ground-based spectra across the 0.7 ฮผm and 3.0 ฮผm wavelength bands reveal a distinct absorption band centered near 0.7 ฮผmโdiagnostic of Fe2+ โ Fe3+ intervalence charge transfer in oxidized iron-bearing phyllosilicates (hydrated clay minerals)โalongside a broad 3.0 ฮผm hydration band produced by structural OH groups and interlayer H2O in aqueous-altered silicates. Unlike icy regular satellites, Himalia shows no clean crystalline water-ice absorption bands at 1.5 and 2.0 ฮผm.
These spectral signatures confirm that Himalia's progenitor did not accrete in situ within a circum-Jovian disk (which would have placed it on a circular, equatorial orbit like Ganymede and Callisto), nor did it originate in the ultra-red trans-Neptunian belt. Instead, the Himalia parent body formed as a volatile-rich carbonaceous planetesimal near the outer asteroid belt or Hilda/Trojan zones (3.2โ5.2 AU), underwent mild internal heating that melted pore ice and drove aqueous alteration of anhydrous silicates into phyllosilicates, and was subsequently captured into a bound circum-Jovian orbit beyond the planetary Roche limit. Viable capture mechanisms include hydrodynamic gas drag as the asteroid passed through the extended envelope of the proto-Jovian gas nebula, rapid mass growth ("pull-down" capture) as Jupiter accreted its gaseous envelope, or three-body gravitational scattering during early giant-planet migration.
Frequently Asked Questions
How could Jupiter capture an asteroid into a permanent orbit?
Under pure two-body gravitational mechanics, a heliocentric asteroid approaching Jupiter on a hyperbolic trajectory will simply swing past the planet and escape back into solar orbit unless it loses kinetic energy inside Jupiter's Hill sphere. In the early solar system, energy dissipation occurred either through aerodynamic gas drag within Jupiter's extended protoplanetary subnebula, through a rapid increase in Jupiter's mass during runaway gas accretion, or via three-body gravitational interactions involving another planetesimal or giant planet.
Why are several moons clustered in almost the exact same orbit as Himalia?
The seven confirmed members of the Himalia group (Himalia, Elara, Lysithea, Leda, Dia, Pandia, and Ersa) share nearly identical orbital distances (~11.4 million km), inclinations (~27.5ยฐ), and dark carbonaceous colors because they are fragments of a single captured asteroid (~180โ200 km across) that was shattered by a high-speed collision after being captured by Jupiter. Himalia is the largest surviving remnant of that parent body.
Is Himalia larger than Amalthea?
While Amalthea has a slightly longer single axis (250 km long, compared to ~206 km for Himalia's longest dimension), Amalthea is much narrower across its other two axes (146 ร 128 km) and has a very low porous density (0.857 g/cm3). Himalia has a larger mean volumetric diameter (~140โ170 km vs. ~167 km for Amalthea) and more than twice Amalthea's total mass (~4.2 ร 1018 kg vs. ~2.08 ร 1018 kg), making Himalia the fifth most massive moon of Jupiter.
References
- Porco, C. C., West, R. A., McEwen, A., Del Genio, A. D., Ingersoll, A. P., Thomas, P., Squyres, S., Dones, L., Murray, C. D., Johnson, T. V., Burns, J. A., Brahic, A., Neukum, G., Veverka, J., Barbara, J. M., Denk, T., Evans, M., Ferrier, J. J., Geissler, P., ... & Vasavada, A. R. (2003). Cassini imaging of Jupiter's atmosphere, satellites, and rings. Science, 299(5612), 1541โ1547. https://doi.org/10.1126/science.1079462
- Emelyanov, N. V. (2005). The mass of Himalia from the perturbations on other satellites. Astronomy & Astrophysics, 438(3), L33โL36. https://doi.org/10.1051/0004-6361:200500143
- Chamberlain, M. A., & Brown, R. H. (2004). Near-infrared spectroscopy of Himalia. Icarus, 172(1), 163โ169. https://doi.org/10.1016/j.icarus.2003.12.016
- Nesvornรฝ, D., Alvarellos, J. L. A., Dones, L., & Levison, H. F. (2003). Orbital and collisional evolution of the irregular satellites. The Astronomical Journal, 126(1), 398โ429. https://doi.org/10.1086/375461
- Brown, M. E., & Rhoden, A. R. (2014). The 3 ฮผm spectrum of Jupiter's irregular satellite Himalia. The Astrophysical Journal Letters, 793(2), L44. https://doi.org/10.1088/2041-8205/793/2/L44