Abstract
The D’Alembert model for the spin/orbit problem in celestial mechanics is considered. Using a Hamiltonian formalism, it is shown that in a small neighborhood of a p : q spin/orbit resonance with (p, q) different from (1, 1) and (2, 1) the ‘effective’ D’Alembert Hamiltonian is a completely integrable system with phase space foliated by maximal invariant curves; instead, in a small neighborhood of a p : q spin/orbit resonance with (p, q) equal to (1, 1) or (2, 1) the ‘effective’ D’Alembert Hamiltonian has a phase portrait similar to that of the standard pendulum (elliptic and hyperbolic equilibria, separatrices, invariant curves of different homotopy). A fast averaging with respect to the ‘mean anomaly’ is also performed (by means of Nekhoroshev techniques) showing that, up to exponentially small terms, the resonant D’Alembert Hamiltonian is described by a twodegrees-of-freedom, properly degenerate Hamiltonian having the lowest order terms corresponding to the ‘effective’ Hamiltonian mentioned above.
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Biasco, L., Chierchia, L. (2002). Effective Hamiltonian for the D’Alembert Planetary Model near a Spin/Orbit Resonance. In: Celletti, A., Ferraz-Mello, S., Henrard, J. (eds) Modern Celestial Mechanics: From Theory to Applications. Springer, Dordrecht. https://doi.org/10.1007/978-94-017-2304-6_14
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DOI: https://doi.org/10.1007/978-94-017-2304-6_14
Publisher Name: Springer, Dordrecht
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