Write and use the torque balance from part (ii) to eliminate the resonant argument. The resonant contribution isAdding the Poynting–Robertson drag contribution gives the dissipative resonant eccentricity equilibrium equationwhereFor , integrating with givesHere 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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