Abstract
Our purpose is to build a model of rotation for a rigid Mercury, involving the planetary perturbations and the non-spherical shape of the planet. The approach is purely analytical, based on Hamiltonian formalism; we start with a first-order basic averaged resonant potential (including J 2 and C 22, and the first powers of the eccentricity and the inclination of Mercury). With this kernel model, we identify the present equilibrium of Mercury; we introduce local canonical variables, describing the motion around this 3:2 resonance. We perform a canonical untangling transformation, to generate three sets of action-angle variables, and identify the three basic frequencies associated to this motion. We show how to reintroduce the short-periodic terms, lost in the averaging process, thanks to the Lie generator; we also comment about the damping effects and the planetary perturbations. At any point of the development, we use the model SONYR to compare and check our calculations.
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Lemaitre, A., D’Hoedt, S., Rambaux, N. (2006). The 3:2 spin-orbit resonant motion of Mercury. In: Celletti, A., Ferraz-Mello, S. (eds) Periodic, Quasi-Periodic and Chaotic Motions in Celestial Mechanics: Theory and Applications. Springer, Dordrecht. https://doi.org/10.1007/978-1-4020-5325-2_12
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DOI: https://doi.org/10.1007/978-1-4020-5325-2_12
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