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Passing Through Resonance: The Excitation and Dissipation of the Lunar Free Libration in Longitude

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Interactions Between Physics and Dynamics of Solar System Bodies

Abstract

The acceleration of the mean lunar longitude has a small effect on the periods of most terms in a Fourier expansion of the longitude. There are several planetary perturbation terms that have small amplitudes, but whose periods are close to the resonant period of the lunar libration in longitude. Some of these terms are moving toward resonance, some are moving away from resonance, and the periods of those terms that do not include the Delaunay variables in their arguments are not moving. Because of its acceleration of longitude, the Moon is receding from the Earth, so the magnitude of the restoring torque that the Earth exerts on the rotating Moon is gradually attenuating; thus resonance itself is moving, but at a much slower rate than the periods of the accelerating planetary perturbations. There are five planetary perturbation terms from the ELP-2000 Ephemeris (with amplitudes of 0”.00001 or greater) that have passed through resonance in the past two million years. One of them is of special interest because it appears to be the excitation source of a supposed free libration in longitude that has been detected by the lunar laser ranging experiment. The amplitude of the term is only 0”.00021 but it could be the source of the ~ 1” amplitude free libration term if the viscoelastic properties of the Moon are similar to those of the Earth.

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© 1993 Springer Science+Business Media Dordrecht

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Eckhardt, D.H. (1993). Passing Through Resonance: The Excitation and Dissipation of the Lunar Free Libration in Longitude. In: Bois, E., Oberti, P., Henrard, J. (eds) Interactions Between Physics and Dynamics of Solar System Bodies. Springer, Dordrecht. https://doi.org/10.1007/978-94-011-1902-3_25

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  • DOI: https://doi.org/10.1007/978-94-011-1902-3_25

  • Publisher Name: Springer, Dordrecht

  • Print ISBN: 978-94-010-4840-8

  • Online ISBN: 978-94-011-1902-3

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