Onset of oligarchic growth and implication for accretion histories of dwarf planets
arXiv:1608.00043 · doi:10.1016/j.icarus.2016.07.019
Abstract
We investigate planetary accretion that starts from equal-mass planetesimals using an analytic theory and numerical simulations. We particularly focus on how the planetary mass at the onset of oligarchic growth depends on the initial mass of a planetesimal. Oligarchic growth commences when the velocity dispersion relative to the Hill velocity of the protoplanet takes its minimum. We find that if is small enough, this normalized velocity dispersion becomes as low as unity during the intermediate stage between the runaway and oligarchic growth stages. In this case, is independent of . If is large, on the other hand, oligarchic growth commences directly after runaway growth, and . The planetary mass for the solid surface density of the Minimum Mass Solar Nebula is close to the masses of the dwarf planets in a reasonable range of . This indicates that they are likely to be the largest remnant planetesimals that failed to become planets. The power-law exponent of the differential mass distribution of remnant planetesimals is typically and to for small and large . The slope, , and the bump at g (or 50 km in radius) for the mass distribution of hot Kuiper belt objects are reproduced if is the bump mass. On the other hand, small initial planetesimals with g or less are favored to explain the slope of large asteroids, , while the bump at g can be reproduced by introducing a small number of asteroid seeds each with mass of g.
34 pages, 10 figures, accepted for publication in Icarus
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