Write and use the torque balance from part (ii) to eliminate the resonant argument. The resonant contribution is
Adding the Poynting–Robertson drag contribution gives the dissipative resonant eccentricity equilibrium equation
where
For , integrating with gives
Here is the fixed resonant semi-major axis and the expression describes averaged evolution, neglecting the small resonant-argument libration. The physical bound-orbit interpretation also requires ; a quantitatively controlled second-order calculation needs .

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