L10 From Planetesimals to protoplanets
L10 From Planetesimals to protoplanets
L10 From Planetesimals to protoplanets
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Orderly growth<br />
Once the gaseous nebula is dispersed (after ~10 Myrs), and all planetesimals have been<br />
accreted in<strong>to</strong> oligarchs, no mechanisms (gas damping, viscous friction) exist any more <strong>to</strong><br />
damp the random velocities of the big bodies. Gravitational scattering then increases the<br />
random velocities <strong>to</strong> v~vesc. This means that the gravitational focussing fac<strong>to</strong>r Fg becomes ~1.<br />
The collisional cross section is thus reduced <strong>to</strong> the geometrical cross section. Growth in this<br />
regime is very slow. Growth of velocity dispersion in the disk is dominated by the<br />
pro<strong>to</strong>planets, and gravitational focusing is weak.<br />
With Fg =1, the master equation becomes<br />
or in relative terms<br />
This means that the growth rate decreases with increasing mass. Bigger bodies grow slower.<br />
This is the same as in the oligarchic regime. However, Fg is much larger in the oligarchic<br />
regime than in the orderly growth regime.<br />
Orderly growth is the final regime for planet growth, at least in the inner solar system.