We prove that the exact non local equation derived by the present authors f
or the temporal linear evolution of the surface of a viscous incompressible
fluid reduces asymptotically for high viscosity to a second order Mathieu
type equation proposed recently by Cerda and Tirapegui. The equation descri
bes a strongly damped pendulum and the conditions of validity of the asympt
otic regime are given in terms of the relevant physical parameters.