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Astron. Astrophys. 329, 1145-1151 (1998) 2. Dynamical analysisThe three observed objects have been integrated a first time with the same code used to build the First General Page of the Atlas of Dynamical Evolution of Short-Period Comets (Carusi et al., 1995). Initial orbital parameters of these objects have been derived from the Bowell (1996) catalogue of asteroid orbital data. The integration of the orbits, over a time interval of 821.4 years centered on 1996 (1585-2406), has been performed using the Everhart's routine RADAU to the 15th order (Everhart, 1985), taking into account the gravitational influence of the Sun and all planets. All passages of minor bodies within a sphere of a given radius d around each planet have been recorded as described in Carusi and Dotto (1996) and in Carusi et al. (1985a,b). Tables 1, 2 and 3 summarize, for each object, the results
obtained by the Atlas orbital integration. These Tables contain:
i) the listing of the orbital parameters at the starting point
of the integration (first line) and every 50 000 days, from JD
2 300 000.5 to JD 2 600 000.5. The Epoch and the time of
perihelion passage T are given, according to the Gregorian
Calendar, in year, month and day. The other columns report the
semi-major axis of the orbit a (in AU), its eccentricity
e, the argument of perihelion Table 1. Dynamical evolution over a time span of 821.4 years of (6042) 1990 WW2 : (top) orbital parameters at the starting point of the integration (first line) and every 50 000 days, from JD 2 300 000.5 to JD 2 600 000.5; (middle) close encounters with planets; (bottom) possible librations about mean motion resonances with the giant planets. Table 2. Dynamical evolution over a time span of 821.4 years of (6144) 1994 EQ3 : (top) orbital parameters at the starting point of the integration (first line) and every 50 000 days, from JD 2 300 000.5 to JD 2 600 000.5; (middle) close encounters with planets; (bottom) possible librations about mean-motion resonances with the giant planets. Table 3. Dynamical evolution over a time span of 821.4 years of 1995 QY2 : (top) orbital parameters at the starting point of the integration (first line) and every 50 000 days, from JD 2 300 000.5 to JD 2 600 000.5; (middle) close encounters with planets; (bottom) possible librations about mean-motion resonances with the giant planets. Figs. 1, 2 and 3 show, for each object, the obtained evolution of
dynamical parameters, as in the Second General Page of the Atlas of
Dynamical Evolution of Short-Period Comets (Carusi et al., 1995).
Plots have the time in abscissa from 1 500 to 2 500 AD and represent:
i) the energy diagram, since the ordinate
(6042) 1990 WW2 has an high inclination orbit, which seems to have a typical asteroidal behavior with very small variations of the semi-major axis and of the aphelion and perihelion distances; (6144) 1994 EQ3 is on a Jupiter-crossing orbit and, as a consequence, the semimajor axis varies chaotically due to repeated close encounters with Jupiter, while 1995 QY2 is a Mars crosser and librates about the 15/7 resonance with Jupiter. To investigate in more detail the dynamical evolution of the last two objects [(6144) 1994 EQ3 and 1995 QY2 ], we have integrated for a long-time span a sample of 15 "clone" orbits for each object. The clones were obtained by changing the last digit of the current orbital elements. The orbital integration, performed with the Everhart's routine RADAU, includes all planets. The clones of (6144) 1994 EQ3 have been
integrated backwards for 1 The 15 clones of 1995 QY2 have been integrated
forwards in time for 1.2
© European Southern Observatory (ESO) 1998 Online publication: December 16, 1997 ![]() |