Skip to content
Pax Abyssi

Planet class · GGC, GGT, GGH · G1-C, G3-T, G2-H

Gas giant

ObservedMeasured or catalogued in the real sky, with its source cited.ModelPublished physics or a published model, applied as written.SimWhat the simulation generates or renders; it may depart from reality and says where.This page mixes measured in the real sky, published physics applied as written and what the simulation does, with its departures marked.How we decide
Old revisionYou are reading revision 136, saved 27 Sept 2026, 18:42 UTC by Pax Abyssi Science Deskbotstaff. Read the current page.
ContentsShow

A gas giant is a planet made mostly of hydrogen and helium, the two lightest elements, with no solid surface to stand on. Jupiter and Saturn are the Solar System's gas giants; Uranus and Neptune, which are mostly heavier material, are classed separately as ice giants. Gas giants range from about a tenth of Jupiter's mass up to about 13 Jupiter masses, where objects become massive enough to fuse deuterium and are called brown dwarfs. They were the first planets found around Sun-like stars, and they shape the systems they live in: their gravity steers asteroids and comets, and their migration can clear or scatter everything nearby.

What makes a gas giant

A gas giant has roughly the composition of the gas its star formed from. Jupiter's upper atmosphere is about 90% molecular hydrogen and 10% helium by volume, with methane, ammonia, water and hydrogen sulfide as trace gases 1. The heavier elements are enriched relative to the Sun: the Galileo probe, which fell into Jupiter in 1995, measured carbon, nitrogen and sulfur at about three times the solar proportion 2. That enrichment is a clue to how the planet formed, since it means Jupiter swallowed solids as well as gas.

The name is slightly misleading. Only the outer few per cent of a gas giant's radius behaves like a gas. Deeper, the pressure squeezes hydrogen into a dense fluid, and beyond about a million times the pressure at Earth's surface the hydrogen's electrons break free and it conducts electricity like a liquid metal. Currents in this metallic hydrogen generate the planet's magnetic field 3.

Gas giants are also oddly uniform in size. Adding mass to a giant squeezes its interior harder, and above about half a Jupiter mass the extra compression nearly cancels the extra material. An old, cool giant of 0.5 Jupiter masses and one of 10 both have radii close to Jupiter's own, and the curve stays nearly flat into the brown dwarf range 4 5. Saturn, at 0.30 Jupiter masses, is on the rising part of the curve at 0.84 Jupiter radii, and its mean density of 0.687 g/cm³ is lower than that of water 6. The main exceptions are the hot Jupiters, many of which are inflated well beyond Jupiter's size by their stars' heat.

Inside a gas giant

NASA's Juno spacecraft, orbiting Jupiter since 2016, has mapped the planet's gravity field closely enough to test models of its interior. The result was unexpected: Jupiter's heavy elements are not packed into a small, dense core but spread through a large "dilute core" that blends into the hydrogen envelope around it 7 8. Saturn has a similar diffuse core, revealed by the way oscillations inside the planet disturb the waves in its rings 9.

Helium is separating out of both planets. At the pressures and temperatures deep in a cooling giant, helium stops mixing with metallic hydrogen and condenses into droplets that sink, a process called helium rain. The Galileo probe found Jupiter's upper atmosphere depleted in helium, with a mass fraction of 0.234 against about 0.27 in the gas the Sun formed from 10. Neon, which dissolves into the helium droplets and is carried down with them, is depleted about tenfold, the signature helium rain predicts 11. Saturn, smaller and colder, has taken the process further 12.

Figure 1Diagram: inside Jupiter and Saturn, as Juno's gravity data and Saturn's ring seismology now picture them.

Gas giants also shine by their own heat. Jupiter radiates 7.5 watts per square metre from its interior on top of the sunlight it re-emits, so it gives off slightly more than twice the energy it absorbs from the Sun 13. The heat is left over from the planet's formation and is released as the planet slowly cools and contracts; helium rain adds to it. Internal heat drives the convection that stirs the atmosphere and powers the magnetic field.

Clouds, colours and temperature

Rapid rotation (Jupiter turns in 9.93 hours 1) organises a gas giant's weather into bands of alternating east and west winds: the familiar belts and zones, with long-lived storms like the Great Red Spot riding between them. Which clouds form, and so what colour the bands are, depends on temperature. A cold giant like Jupiter has ammonia ice clouds on top; a warmer one would have water clouds; warmer still, no clouds form high in the atmosphere at all; and the hottest have clouds of rock and metal. The Sudarsky classification turns that sequence into five classes.

Astronomers usually sort giant exoplanets by orbital period or equilibrium temperature. Hot Jupiters have periods of a few days; warm Jupiters orbit in roughly 10 to 200 days; cold Jupiters orbit beyond about 1 AU, the region where giants are most common. The sim uses equilibrium temperature for the same split, with three types: cold (below 150 K), temperate (150 to 800 K) and hot (above 800 K).

Jupiter in true colour, cream zones and brown belts, the Great Red Spot in the southern hemisphere
Figure 2Observation: Jupiter in true colour, assembled from Cassini images taken on 29 December 2000. Credit: NASA/JPL/Space Science Institute.
PD-NASA

Formation

Two ideas compete to explain how gas giants form. In core accretion, the favoured model for most giants, a core of rock and ice grows in the disc around a young star until, at about ten Earth masses, its gravity can pull in the surrounding gas faster and faster. The planet must finish before the disc disperses, within a few million years, which favours the region just beyond the snow line, where ice adds to the solid material available 14. In disc instability, a massive, cold disc fragments directly into giant planets under its own gravity, far faster than a core can grow 15; this route may explain some massive giants on very wide orbits.

Giants need not stay where they form. Interactions with the gas disc, with other planets or with a distant companion star can move them inward, and a giant pushed close to its star becomes a hot Jupiter 16.

Core accretion predicts that stars richer in heavy elements should form giants more easily, and they do. The chance that a Sun-like star has a giant planet rises roughly with the square of its iron abundance, so a star with twice the Sun's iron is about four times as likely to host one 17.

How common are they?

Radial-velocity surveys, which detect the wobble a planet induces in its star, find about 14 giant planets per 100 Sun-like stars with orbits of 2 to 8 AU, and about 9 per 100 at 8 to 32 AU. Giants are about four times more common beyond 1 AU than inside it 18. Hot Jupiters are rare: they orbit about 0.4% of the stars Kepler watched 19 and about 1.2% of nearby Sun-like stars in radial-velocity surveys 20. They were found first because they are the easiest planets to detect.

How we know

  • Spacecraft have visited all four giants of the Solar System. The Galileo probe sampled Jupiter's atmosphere directly in 1995; Cassini measured Saturn's gravity, rings and heat balance and refined Jupiter's 13; Juno is mapping Jupiter's gravity and magnetic field.
  • Radial velocities found the first gas giant around a Sun-like star, 51 Pegasi b, in 1995 21.
  • Transits give radii and, combined with radial velocities, densities; HD 209458 b in 1999 was the first planet seen to transit 22.
  • Spectroscopy during transits and eclipses reads the atmospheres. JWST made the first clear detection of carbon dioxide in an exoplanet, the Saturn-mass WASP-39 b, in 2022 23.
  • Direct imaging separates the light of young or wide-orbit giants from their stars' glare 24 25.

Notable examples

PlanetMassRadiusOrbitNotes
Jupiter1 M_Jup (317.8 Earth masses)71,492 km5.20 AU, 11.9 yearsLargest planet in the Solar System 1
Saturn0.30 M_Jup (95.2 Earth masses)60,268 km9.6 AU, 29.4 yearsMean density below water's 6
51 Pegasi bat least about 0.5 M_Jupunknown4.23 daysFirst gas giant found around a Sun-like star 21
HD 209458 b0.69 M_Jup1.27 R_Jup3.5 daysFirst planet seen to transit 26 22
KELT-9 babout 2.9 M_Jupabout 1.9 R_Jup1.5 daysDayside near 4,600 K, one of the hottest planets known 27
epsilon Indi Ababout 6 M_Jupabout 200 yearsCold giant 12 light years away, imaged by JWST; effective temperature about 275 K 25 28
HR 8799 b, c, d, eseveral M_Jup eachabout 15 to 70 AUFour young giants imaged around one star 24 29

See also

References

  1. 1NASA Space Science Data Coordinated Archive. Jupiter Fact Sheet. nssdc.gsfc.nasa.gov/planetary/factsheet/jupiterfact.html
  2. 2Atreya, S. K. et al. (1999). A comparison of the atmospheres of Jupiter and Saturn: deep atmospheric composition, cloud structure, vertical mixing, and origin. Planetary and Space Science 47, 1243-1262. doi:10.1016/S0032-0633(99)00047-1
  3. 3Stevenson, D. J. (2020). Jupiter's Interior as Revealed by Juno. Annual Review of Earth and Planetary Sciences 48, 465-489. doi:10.1146/annurev-earth-081619-052855
  4. 4Fortney, J. J., Marley, M. S. and Barnes, J. W. (2007). Planetary Radii across Five Orders of Magnitude in Mass and Stellar Insolation: Application to Transits. The Astrophysical Journal 659, 1661-1672. doi:10.1086/512120
  5. 5Chen, J. and Kipping, D. (2017). Probabilistic Forecasting of the Masses and Radii of Other Worlds. The Astrophysical Journal 834, 17. doi:10.3847/1538-4357/834/1/17
  6. 6NASA Space Science Data Coordinated Archive. Saturn Fact Sheet. nssdc.gsfc.nasa.gov/planetary/factsheet/saturnfact.html
  7. 7Wahl, S. M. et al. (2017). Comparing Jupiter interior structure models to Juno gravity measurements and the role of a dilute core. Geophysical Research Letters 44, 4649-4659. doi:10.1002/2017GL073160
  8. 8Militzer, B. et al. (2022). Juno Spacecraft Measurements of Jupiter's Gravity Imply a Dilute Core. The Planetary Science Journal 3, 185. doi:10.3847/PSJ/ac7ec8
  9. 9Mankovich, C. R. and Fuller, J. (2021). A diffuse core in Saturn revealed by ring seismology. Nature Astronomy 5, 1103-1109. doi:10.1038/s41550-021-01448-3
  10. 10von Zahn, U., Hunten, D. M. and Lehmacher, G. (1998). Helium in Jupiter's atmosphere: Results from the Galileo probe Helium Interferometer Experiment. Journal of Geophysical Research: Planets 103, 22815-22829. doi:10.1029/98JE00695
  11. 11Wilson, H. F. and Militzer, B. (2010). Sequestration of Noble Gases in Giant Planet Interiors. Physical Review Letters 104, 121101. doi:10.1103/PhysRevLett.104.121101
  12. 12Mankovich, C. R. and Fortney, J. J. (2020). Evidence for a Dichotomy in the Interior Structures of Jupiter and Saturn from Helium Phase Separation. The Astrophysical Journal 889, 51. doi:10.3847/1538-4357/ab6210
  13. 13Li, L. et al. (2018). Less absorbed solar energy and more internal heat for Jupiter. Nature Communications 9, 3709. doi:10.1038/s41467-018-06107-2
  14. 14Pollack, J. B. et al. (1996). Formation of the Giant Planets by Concurrent Accretion of Solids and Gas. Icarus 124, 62-85. doi:10.1006/icar.1996.0190
  15. 15Boss, A. P. (1997). Giant Planet Formation by Gravitational Instability. Science 276, 1836-1839. doi:10.1126/science.276.5320.1836
  16. 16Dawson, R. I. and Johnson, J. A. (2018). Origins of Hot Jupiters. Annual Review of Astronomy and Astrophysics 56, 175-221. doi:10.1146/annurev-astro-081817-051853
  17. 17Fischer, D. A. and Valenti, J. (2005). The Planet-Metallicity Correlation. The Astrophysical Journal 622, 1102-1117. doi:10.1086/428383
  18. 18Fulton, B. J. et al. (2021). California Legacy Survey. II. Occurrence of Giant Planets beyond the Ice Line. The Astrophysical Journal Supplement Series 255, 14. doi:10.3847/1538-4365/abfcc1
  19. 19Fressin, F. et al. (2013). The False Positive Rate of Kepler and the Occurrence of Planets. The Astrophysical Journal 766, 81. doi:10.1088/0004-637X/766/2/81
  20. 20Wright, J. T. et al. (2012). The Frequency of Hot Jupiters Orbiting Nearby Solar-type Stars. The Astrophysical Journal 753, 160. doi:10.1088/0004-637X/753/2/160
  21. 21Mayor, M. and Queloz, D. (1995). A Jupiter-mass companion to a solar-type star. Nature 378, 355-359. doi:10.1038/378355a0
  22. 22Charbonneau, D. et al. (2000). Detection of Planetary Transits Across a Sun-like Star. The Astrophysical Journal 529, L45-L48. doi:10.1086/312457
  23. 23JWST Transiting Exoplanet Community Early Release Science Team et al. (2023). Identification of carbon dioxide in an exoplanet atmosphere. Nature 614, 649-652. doi:10.1038/s41586-022-05269-w
  24. 24Marois, C. et al. (2008). Direct Imaging of Multiple Planets Orbiting the Star HR 8799. Science 322, 1348-1352. doi:10.1126/science.1166585
  25. 25Matthews, E. C. et al. (2024). A temperate super-Jupiter imaged with JWST in the mid-infrared. Nature 633, 789-792. doi:10.1038/s41586-024-07837-8
  26. 26Mazeh, T. et al. (2000). The Spectroscopic Orbit of the Planetary Companion Transiting HD 209458. The Astrophysical Journal 532, L55-L58. doi:10.1086/312558
  27. 27Gaudi, B. S. et al. (2017). A giant planet undergoing extreme-ultraviolet irradiation by its hot massive-star host. Nature 546, 514-518. doi:10.1038/nature22392
  28. 28Max Planck Society (2024). Webb images nearest super-Jupiter, opening a new window to exoplanet research. www.mpg.de/22154949/0702-astr-2024-jwst-eps-ind-150980-x
  29. 29Marois, C. et al. (2010). Images of a fourth planet orbiting HR 8799. Nature 468, 1080-1083. doi:10.1038/nature09684