Asteroid Synthetic Proper Elements

Z. Knezevic1 and A. Milani2
1 University of Belgrad, Yugoslavia
2 University of Pisa, Italy


Analytically computed proper elements in the low to moderate inclination and eccentricity region of the asteroid main belt are accurate to a level very close to the fundamental threshold of the accuracy of any analytical theory. This results from the fact that there is an infinite web of resonances and because of the occurence of chaotic motions (typical instability over 5 Myr in the proper e and sin I being ≤ 0.0015, and even better in the proper a; Milani and Knezevic, 1994, ( Icarus 107, 219). Still, there are some regions of the belt (e.g. near resonances) in which these proper elements are of degraded accuracy, thus preventing a reliable definition of asteroid families. We have, therefore, tried a different approach to compute the asteroid proper elements, with a goal to further improve their accuracy and thus enable the identification of families in the densely populated zones of large samples of asteroids, as well as the more refined analysis of their long-term dynamics. Following the approach employed in the case of major planets by Carpino et al. (1987, Astron. Astrophys. 181, 182), that is, applying purely numerical techniques, we produced the so-called ``synthetic'' proper elements for a sample of 10,256 asteroids. We have taken into account all the asteroids with osculating semimajor axes between 2.5 AU and 4.0 AU, with the exception of those for which the initial value of the quantity (e2 + sin2 I)1/2 > 0.3, and the perihelion distance q < 1.75 AU. The procedure consisted of simultaneous integration of asteroid orbits for 2 Myr, on-line filtering of the short-periodic perturbations, and computation of Lyapunov Characteristic Exponents to monitor the chaotic behaviors. The output of the integration was next spectrally resolved, and the principal harmonics (proper values) extracted from the time series. For each set of proper elements and associated fundamental frequencies the corresponding standard and maximum deviations are supplied too. For 1862 asteroids exhibiting large standard deviations of proper values due to the chaotic or secular resonant effects, we have extended the integrations to 10 Myr, and repeated the analysis. For only 9 asteroids we could not derive the proper elements in this way because of the hyperbolic divergence of their orbits. In 8009 cases we have determined the proper elements with an accuracy in terms of the standard deviations of proper eccentricity and sine of proper inclination better than 0.001, and that of the proper semimajor axis better than 0.0003 AU. Out of these, in 6387 cases the error in proper e was even less than 0.0003 and in proper sin I less than 0.0001. On the other hand, we have identified 913 asteroids with standard deviations of proper eccentricity or proper sine of inclination larger than 0.003, 497 strongly chaotic bodies (Lyapunov times shorter than 10,000 yr), 33 ``pathological'' cases for which the errors of computed elements and/or frequencies were, for different reasons, excessively large, etc.

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