4.7 Article

Hydrodynamic simulations of unevenly irradiated Jovian planets

Journal

ASTROPHYSICAL JOURNAL
Volume 674, Issue 2, Pages 1106-1116

Publisher

IOP PUBLISHING LTD
DOI: 10.1086/523957

Keywords

planetary systems; planets and satellites : individual (HD 80606b, HD 37605b, HD 108147b, HAT-P-2b, HD 118203b, HD 185269b)

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We employ a two-dimensional, grid-based hydrodynamic model to simulate upper atmospheric dynamics on extra-solar giant planets. The hydrodynamic equations of motion are integrated on a rotating, irradiated sphere using a pseudo-spectral algorithm. We use a two-frequency, two-stream approximation of radiative transfer to model the temperature forcing. This model is well suited to simulate the dynamics of the atmospheres of planets with high orbital eccentricity, which are subject to widely varying irradiation conditions. We identify six such planets, with eccentricities between e = 0.28 and e = 0.93 and semimajor axes from a = 0.0508 AU to a = 0.432 AU, as particularly interesting. For each, we determine the temperature profile and resulting infrared light curves in the 8 mu m Spitzer band. Especially notable are the results for HD 80606b, which has the largest eccentricity (e = 0.9321) of any known planet, and HAT-P-2b, which transits its parent star, so that its physical properties are well constrained. Despite the varied orbital parameters, the atmospheric dynamics of these planets display a number of interesting common properties. In all cases, the atmospheric response is primarily driven by the intense irradiation at periastron. The resulting expansion of heated air produces high-velocity turbulent flow, including long-lived circumpolar vortices. In addition, a superrotating acoustic front develops on some planets; the strength of this disturbance depends on both the eccentricity and the temperature gradient from uneven heating. The specifics of the resulting infrared light curves depend strongly on the orbital geometry. We show, however, that the variations on HD 80606b and HAT-P-2b should be readily detectable at 4.5 and 8 mu m using Spitzer. These two objects present the most attractive observational targets of all known high-e exoplanets.

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