Astronomy and Astrophysics – Astronomy
Scientific paper
Apr 2012
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2012apj...748..143k&link_type=abstract
The Astrophysical Journal, Volume 748, Issue 2, article id. 143 (2012).
Astronomy and Astrophysics
Astronomy
Gravitation, Hydrodynamics, Planets And Satellites: General, Planets And Satellites: Individual: Jupiter, Planets And Satellites: Interiors
Scientific paper
Rapidly rotating giant planets are usually marked by the existence of strong zonal flows at the cloud level. If the zonal flow is sufficiently deep and strong, it can produce hydrostatic-related gravitational anomalies through distortion of the planet's shape. This paper determines the zonal gravity coefficients, J 2n , n = 1, 2, 3, ..., via an analytical method taking into account rotation-induced shape changes by assuming that a planet has an effective uniform density and that the zonal flows arise from deep convection and extend along cylinders parallel to the rotation axis. Two different but related hydrostatic models are considered. When a giant planet is in rigid-body rotation, the exact solution of the problem using oblate spheroidal coordinates is derived, allowing us to compute the value of its zonal gravity coefficients \bar{J}_{2n}, n=1,2,3, \dots, without making any approximation. When the deep zonal flow is sufficiently strong, we develop a general perturbation theory for estimating the variation of the zonal gravity coefficients, \Delta {J}_{2n}={J}_{2n}-\bar{J}_{2n}, n=1,2,3, \dots, caused by the effect of the deep zonal flows for an arbitrarily rapidly rotating planet. Applying the general theory to Jupiter, we find that the deep zonal flow could contribute up to 0.3% of the J 2 coefficient and 0.7% of J 4. It is also found that the shape-driven harmonics at the 10th zonal gravity coefficient become dominant, i.e., \Delta {J}_{2n} \,{\ge}\, \bar{J}_{2n} for n >= 5.
Kong Dali
Schubert Gerald
Zhang Keke
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