Planetary chaotic zone clearing: destinations and timescales
arXiv:1411.1378 · doi:10.1088/0004-637X/799/1/41
Abstract
We investigate the orbital evolution of particles in a planet's chaotic zone to determine their final destinations and their timescales of clearing. There are four possible final states of chaotic particles: collision with the planet, collision with the star, escape, or bounded but non-collision orbits. In our investigations, within the framework of the planar circular restricted three body problem for planet-star mass ratio in the range to , we find no particles hitting the star. The relative frequencies of escape and collision with the planet are not scale-free, as they depend upon the size of the planet. For planet radius where is the planet's Hill radius, we find that most chaotic zone particles collide with the planet for ; particle scattering to large distances is significant only for higher mass planets. For fixed ratio , the particle clearing timescale, , has a broken power-law dependence on . A shallower power-law, , prevails at small where particles are cleared primarily by collisions with the planet; a steeper power law, , prevails at larger where scattering dominates the particle loss. In the limit of vanishing planet radius, we find . The interior and exterior boundaries of the annular zone in which chaotic particles are cleared are increasingly asymmetric about the planet's orbit for larger planet masses; the inner boundary coincides well with the classical first order resonance overlap zone, ; the outer boundary is better described by , where is the planet-star separation.
20 pages, 7 figures; accepted for publication in ApJ
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