Wave-drift damping results from low-frequency oscillatory motions of a
floating body, in the presence of an incident wave field. Previous wo
rks have analysed this effect in a quasi-steady manner. based on the r
ate of change of the added resistance in waves, with respect to a smal
l steady forward velocity. In this paper the wave-drift damping coeffi
cient is derived more directly, from a perturbation analysis where the
low-frequency body oscillations are superposed on the diffraction fie
ld. Unlike the case of body oscillations in calm water, where the damp
ing due to wave radiation is asymptotically small for low frequencies,
the superposition of oscillatory motions on the diffraction field res
ults in an order-one damping coefficient. All three degrees of freedom
are considered in the horizontal plane. The resulting matrix of dampi
ng coefficients is derived from pressure integration on the body. and
transformed in special cases to a far-field control surface.