Fig. 2

Secular normalized torques of zero-order |⟨T0(r2)⟩| (left column) and first-order |⟨T1(r2)⟩| (right column), computed on m2 due to the tidal deformation on m0 induced by m1, plotted as a function of the mean-motion ratio n1 ∕ n2. We considered m0 = 1, a1 = 1 and varied a2 to include orbits both interior and exterior to m1. Upper panels: circular orbits (e1 = e2 = 0). Lower panels: eccentric orbits with e1 = e2 = 0.1. Light brown vertical lines highlight the location of some important MMRs. We note that the first-order torques in the right panels are also normalized respect to the time-lag Δt0.
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