NEBULAR GAS DRAG AND PLANETARY ACCRETION .2. PLANET ON AN ECCENTRIC ORBIT

Citation
Dm. Kary et Jj. Lissauer, NEBULAR GAS DRAG AND PLANETARY ACCRETION .2. PLANET ON AN ECCENTRIC ORBIT, Icarus, 117(1), 1995, pp. 1-24
Citations number
30
Categorie Soggetti
Astronomy & Astrophysics
Journal title
IcarusACNP
ISSN journal
00191035
Volume
117
Issue
1
Year of publication
1995
Pages
1 - 24
Database
ISI
SICI code
0019-1035(1995)117:1<1:NGDAPA>2.0.ZU;2-W
Abstract
We study the trajectories of planetesimals whose orbits decay starward as a result of gas drag and are perturbed by the gravity of a massive planet on an eccentric orbit. Each planetesimal ultimately suffers on e of three possible fates: (1) trapping in a mean motion resonance wit h the planet, (2) accretion by the planet, or (3) passage by the plane t and continued orbital decay. At moderate to large planetary eccentri city, numerical 3-body integrations of the motion of a planetesimal in the solar nebula demonstrate that migrating planetesimals can become trapped in the 1/1 resonance. These bodies initially have large librat ion amplitudes (approaching 2 pi) which decay down to 0 at the trailin g Lagrange point. With some combinations of drag rate and planetary ec centricity, over 15% of the planetesimals which encounter the planet a re trapped in the 1/1 resonance. Bodies trapped in the this way could be the precursors of the Trojan asteroids. Migrating planetesimals can be caught in both pure Lindblad and combined Lindblad/corotation reso nances exterior to the planet's orbit. Trapping has been found in seve ral j/(j + k) resonances with k's ranging from 1 to 4. As one consider s larger planetary eccentricities, corotation resonances become more i mportant than Lindblad resonances, and (for a given drag rate) trappin g can occur at higher k's and farther from the planet. At large planet ary eccentricities, planetesimals can also be caught in (j + 1)/j Lind blad/corotation resonances interior to the planet. Interior trapping, which is dynamically forbidden in the case of a planet on a circular o rbit, requires planetary eccentricity to increase both the planetesima l's semimajor axis and its eccentricity near conjunction to counter ga s drag. Provided the planetesimal's and planet's apoapses are roughly aligned, and conjunction occurs while both bodies are approaching apoa pse, then the planetesimal can become trapped in an interior resonance . The probability of a planetesimal avoiding accretion while migrating past the planet can be described as the probability of not being accr eted in a single conjunction to the power of the number of conjunction s that a planetesimal has with the planet while passing through its fe eding zone. In the nongravitating planet limit (which is valid for a l ow mean density planet on a highly eccentric orbit), the accretion pro bability increases with planetary eccentricity due to the growth of th e planet's feeding zone. When the planet's gravity is considered using the 2+2-body approximation (which is valid for a dense planet on a mo derately eccentric orbit), the accretion rate is nearly independent of planetary eccentricity. Numerical simulations show that at small plan etary eccentricities, the 2+2-body approximation breaks down, and the accretion probability gradually increases with decreasing eccentricity in this regime. (C) 1995 Academic Press, Inc.