Abstract
Numerical experiments of fictitious small bodies with initial eccentricities e=0.1 have been performed in the overlapping region of the 3/1 mean motion resonance and of thev 6 secular resonance 2.48≤a≤2.52AU for different values of the initial inclination 16°≤i≤20°. An analysis for thev 6 secular resonance shows that the topology is different from the one found outside the overlapping region: the critical argument for thev 6 resonance in the overlapping region rotates in opposite direction as compared to the purev 6 region. In the 3/1 resonance region the secular resonancev 5 is dominant, and some secondary secular resonances asv 6 −v 16 andv 5 +v 6 are present.
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References
Henrard, J. and Lemaître, A.: 1983, ‘A second fundamental model for resonance’,Celest. Mech.,30, 197–218.
Krogh, F. T.: 1970,JPL Technical Utilization Document, No.CP-38.
Morbidelli, A. (1991a) ‘Topological methods for the qualitative analysis of a numerical simulation close to a resonance’ inInterrelations entre la Physique et la Dynamique des Petits Corps du Système Solaire, Goutelas 1991, D. Benest and Cl. Froeschlé eds., in press.
Morbidelli, A. (1991b) ‘Perturbations methods and asteroids dynamics’,PhD Thesis University of Namur, 205–216.
Morbidelli, A. and Henrard, J. (1991) ‘The main secular resonancesv 6,v 5 andv 16 in the asteroid belt’,Celest. Mech.,51, 169–197.
Yoshikawa, M.: 1987, ‘A simple analytical model for thev 6 resonance.’,Celest. Mech.,40, 233–272.
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Froeschlé, C., Scholl, H. Numerical experiments in the 3/1 andv 6 overlapping resonance region. Celestial Mech Dyn Astr 56, 163–176 (1993). https://doi.org/10.1007/BF00699729
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DOI: https://doi.org/10.1007/BF00699729