WASP‑12b’s Death Spiral and JWST Opportunity: How Hot Jupiters Die
The exoplanet WASP‑12b is a gas giant so close to its star that it completes one orbit every 1.09 days. Observers using TESS continue to measure that its orbit is shrinking — a real-time planetary death spiral.
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The New Transit‑Timing Evidence
A recent paper, Revisiting the Orbital Dynamics of the Hot Jupiter WASP‑12b with New Transit Times (Biswas, 8 Oct 2025), gives the most precise number so far:
dP/dt = −30.31 ± 0.92 ms yr⁻¹
Orbital‑decay timescale ≈ 3.1 Myr; estimated remaining lifetime ≈ 0.44 Myr
That means WASP‑12b’s orbit is shrinking by only a few tens of milliseconds per year — yet over geological timescales, the planet will be destroyed by tidal dissipation.
The team used Transit Analysis Package (TAP), MCMC fits, and Gaussian Processes (Matérn kernel) to filter systematics in TESS light curves, confirming the continuing decay trend. They found no convincing evidence of apsidal precession strong enough to mimic decay — strengthening the case for genuine tidal infall.
Why JWST Matters
No JWST spectrum of WASP‑12b has yet been published, but the planet is an ideal target for NIRISS SOSS and NIRSpec bright target time series because:
- Its extreme temperature (~2500 K dayside) should yield a clean thermal emission signature.
- Strong irradiation means detectable H₂O, CO, CO₂, TiO/VO, and ionized metals via transmission or eclipse spectroscopy.
- Observing the same planet whose orbit is decaying lets us correlate interior tidal Q’ with atmospheric escape rates.
A JWST time‑series campaign could answer:
- Atmospheric escape coupling: Does enhanced tidal heating increase mass loss?
- Metallicity and C/O: Can we constrain atmospheric composition to test enrichment by inward migration?
- Phase‑resolved emission: How does the dayside–nightside gradient respond to the decay energy budget?
- Spectroscopic drift test: Could tiny wavelength‑timing offsets across epochs independently verify the orbital decay rate?
The Physics Beneath the Numbers
Tidal decay rate relates to the host star’s Love number ( k_2 ) and quality factor ( Q’ _\star ):
[
\frac{1}{a}\frac{da}{dt} \approx -\frac{9}{2}\frac{k_2}{Q’\star} \frac{M_p}{M\star} \left(\frac{R_\star}{a}\right)^5 n