Circular Problems Douglas P. Hamilton Probably the most striking regularity observed in our Solar System is that the planets all follow nearly circular, nearly coplanar orbits about the Sun. This feature lends strong support to the theory that the planets accreted out of the solar nebula - a flattened disk of gas and dust that surrounded the young Sun. But do flattened disks of dust and gas inevitably lead to a few massive widely-spaced planets on circular uninclined orbits? In the case of the inner Solar System, results from recent numerical simulations* suggest that this may not be the case. The formation of the terrestrial planets - Mercury, Venus, Earth, and Mars - can be loosely divided into three consecutive stages. Initially, dust grains move slowly through the solar nebula, bumping into one another in low velocity "sticking" collisions that gradually build up kilometer-sized "planetesimals"(1). Next, gravity from the planetesimals begins to enhance the accretion rate; this second stage is characterized by a rapid period of "run-away growth" in which the largest planetesimals outcompete and ultimately absorb their smaller neighbors(2). During these first two stages of planetary formation, gas drag from the solar nebula removes energy from the orbits of solid bodies, and damps away their radial and vertical motions as well. Thus solid bodies are thought to follow circular uninclined orbits that gradually evolve inward toward the Sun. The inward migration brings planetesimals together, and their nearly circular orbits lead to low relative velocities and sticking collisions, rather than to energetic impacts that can shatter planetesimals. This simple picture is altered by the gravitational perturbations of Jupiter and Saturn, which are traditionally thought to have formed after 10^6-10^7 years(3) (roughly around the time that there are several dozen Mercury-sized "protoplanets" in the terrestrial region), but which alternate theories suggest may have formed as quickly as 100-1000 years due to nebular gas instability(4). Working under the assumption that the shorter timescale is correct, S. Kortenkamp and G. Wetherill (Carnegie Institute) perform numerical simulations of the second stage of planetary formation and find that when both gas drag and jovian perturbations are important, different-sized planetesimals follow slightly eccentric orbits which are out of phase with one another(5). Collisions between these objects are often energetic enough to prevent accretion, thus hindering the formation of protoplanets. The magnitude of the effect depends sensitively on the orbits of the giant planets; it is diminished by the fact that Jupiter probably formed further from the Sun than it is now, subsequently migrating inward over 10^7-10^8 years(6). Nevertheless, if Jupiter formed quickly, this mechanism slows the runaway growth timescales for the terrestrial planets, and significantly hinders the formation of large planetesimals in the asteroid belt. Additionally, it suggests that if large Jupiter-mass planets in other planetary systems formed quickly rather than slowly, then the zone in which Earth-like planets could form might be significantly reduced. At the beginning of the third and final stage of terrestrial planet formation the largest objects have attained sizes of small planets (~3000km). Several dozen to several hundred of these "protoplanets" perturb one another gravitationally and merge in giant collisions until ultimately only the four terrestrial planets and the Moon remain. New numerical simulations of this stage of planetary formation were reported by two teams: J. Chambers (Armagh Observatory)(7) and C. Agnor (U. Colorado), R. Canup, H. Levison (SWRI). These and other(8) groups follow ~50 protoplanets for ~10^8 years. With reasonable starting conditions, their models produce inner planetary systems with roughly the correct number, sizes, and orbital spacings of planets. All groups, however, find that Earth-sized objects have orbital eccentricities and inclinations that are 5-10 times larger than observed for the present-day Earth and Venus. The eccentricities and inclinations are pumped up early in the simulations, primarily by secular interactions between the orbits of the protoplanets(7). So how did Venus and Earth end up on nearly circular orbits? There are only a few possibilities. First, the simulations may not include some critical physics which damps orbital eccentricities and inclinations (e.g. dynamical friction with smaller objects or larger than expected nebular gas drag) which would cause planets on circular orbits to be formed more readily than the simulations suggest. Second, perhaps the inner planets in our solar system did form with initially large eccentricities and inclinations and these have been subsequently damped by some dissipative force (e.g. solar tides, although these are thought to be too weak) over 4.5 billion years of Solar System history. Finally, perhaps elliptical orbits, rather than circular ones, are indeed the natural product of planetary formation. Using the anthropic principal, J. Chambers points out that if nearly circular orbits are necessary for climatic stability and the development of intelligent life, then Earth's low eccentricity can be understood. This argument is somewhat unsatisfying, however, in that it explains neither the low inclinations of Venus and Earth, nor the low eccentricity of Venus. Douglas P. Hamilton is in the Department of Astronomy, University of Maryland, College Park, Maryland 20742, USA. ________________________________________________________________________ * Reported at the 30th annual DPS meeting, Madison, Wisconsin, Oct. 11-16, 1998. (1) Weidenschilling, S.J. & Cuzzi, J.N. Protostars and Planets III, pp. 1031-1060 (1993). (2) Wetherill, G.W. & Stewart, G.R. Icarus 106, 190-209 (1993). (3) Pollack, J.B., Hubickyj, O. & Greenzweig, Y. Icarus 124, 62-85 (1996). (4) Boss, A.P. Science, 276, 1836-1839 (1997). (5) Fernandez, J.A. & Ip, W.H. Plan. Spa. Sci. 44, 431-439 (1996). (6) Kortenkamp, S.J. & Wetherill, G.W. Icarus, Submitted (1998). (7) Chambers, J.E. & Wetherill, G.W. Icarus, Submitted (1998). (8) Ito, T. & Tanikawa, K. Icarus, Submitted (1998).