Tidal Swings of an Eccentric Jupiter ✛

Original: "Case Study of a Super-eccentric Warm Jupiter Migrating via Equilibrium and Dynamical Tides"
arXiv:2607.16406v1 · 2026-07-17 · CC BY 4.0 · 3 min
A planet with a record eccentricity of 0,94 rocks on a gravitational swing, and only equilibrium tides explain its present orbit.

Every 165 days, the giant planet dives toward its star, nearly grazing its fiery corona, then flies off into the icy void. This is TIC 241249530 b — an exoplanet with a record eccentricity of 0,94. Discovered through photometry by the TESS telescope and refined with spectroscopy, it showed a barely perceptible transit dimming but a huge amplitude in the star's radial velocity. Such behavior is a sure sign of a transit planet, whose orbit resembles a mad swing.

With such an eccentricity, the planet swings closer to the star than Mercury (0,04 AU), then soars out beyond Earth's orbit (1,2 AU) — like a pendulum hours of light long.

The culprit behind this sweeping dance is a distant companion star, whose gravity rocks the orbit through von Zeipel–Lidov–Kozai oscillations. This mechanism turns the orbit into a cosmic swing: under the influence of the foreign pull, the planet's eccentricity periodically soars to enormous values, and then might drop if not for tidal forces. It is they, like friction in a hinge, that gradually damp the swing and bring the planet closer to the star — that's how hot Jupiters are born. We have a rare chance to catch migration in the act.

Astrophysicists tested which type of tidal braking is responsible for the present orbit. In numerical simulations, they ran through thousands of variations, including general relativity effects and two competing scenarios. Equilibrium tides — where the planet behaves like a viscous ball: the tidal bulge lags behind the star's motion and brakes the planet. Chaotic dynamical tides — where nonlinear oscillations are excited inside the giant, dumping energy through stochastic kicks. Calculations with the MESA code, originally designed for stellar evolution, even accounted for heating and inflation of the planet from friction. The verdict was unambiguous.

To slow the swing, the tides needed an anomalous strength — 300 times greater than Jupiter's. Probably, inertial waves run inside the planet, akin to ocean waves on Earth.

Only equilibrium tides could reproduce the observed state. The chaotic scenario invariably sent the planet into too tight a pericenter: the key conserved quantity — the reduced angular momentum j² = a(1−e²) — would have dropped to 0,026 AU instead of the actual 0,074. This little formula — a constant of tidal evolution — ruled out chaos. Moreover, an analysis of all known eccentric giants showed that none violate this threshold. Cosmic swings are arranged so that chaos either never kicks in or quickly ends, leaving behind only hot Jupiters.

It seems equilibrium tides are the principal conductor of the migrating planet orchestra. The observational hunt for new 'swing systems' with distant companions will continue, and each discovery will shed light on the birth of the most unusual worlds.

With its current eccentricity of 0.94, TIC 241249530 b approaches the star to 0.04 AU, then recedes to 1.2 AU. If you placed this planet in the Solar System, it would 'swing' from Mercury's orbit to Earth's orbit every 165 days.

j^2 = a(1-e^2)
Reduced angular momentum, conserved during tidal evolution without external perturbations; the product of the semi-major axis and (1−e²) remains constant.
Scientists
Christian DopplerD. B. McLaughlinDidier QuelozMichel MayorR. A. RossiterDavid Charbonneau
Concepts
tidal migration hot jupiter tidal heating jupiter europa planetary migration North Equatorial Countercurrent eccentric orbit transit method gravitational wave eccentricity red dwarf planets transit terrestrial exoplanet Hadley cell exoplanets around red dwarfs starburst critical transition exoplanet trappist 1 hot jupiter atmospheres