THE COOL EARLY EARTH AND THE TIDAL CAPTURE MODEL: THERMAL AND TECTONIC EFFECTS ON EARTH AND MOON
We have done a series of co-planar three-body numerical simulations of capture of a lunar-sized planetoid by an earth-mass planet using a fourth-order Runge-Kutta integration procedure described in Malcuit et al. (1992). The planet is in a circular orbit at 1.0 AU and the planetoid is in a slightly smaller heliocentric orbit (1.5% eccentricity and semi-major axis of 0.972 AU). The important body parameters for the interacting bodies are the displacement Love number (h) and the specific dissipation factor (Q) for each body. Using reasonable h and Q values for the planet and planetoid, we find that well over 90% of the energy for capture must be dissipated in the planetoid. The equilibrium rock tides for the capture encounter are about 20 km for the planet and over 300 km for the planetoid. Thus during any capture scenario, the captured planetoid is severely heated and deformed while the planet is only mildly thermally effected and tidally disturbed only in the equatorial zone.
Crustal zircon crystals could be completely destroyed in the equatorial zone by deep subduction but there would be a transition in a poleward direction to where very little subduction occurs. At some intermediate latitude, subduction would be shallow enough for the zircon crystals to survive and these zircons could record a Cool Early Earth.