In a previous paper, the authors considered the free rotation of an earth m
odel composed of a rigid mantle and a liquid core in the presence of dissip
ation and under the Hamiltonian formalism, obtaining analytical expressions
for the free nutation modes.
In this paper we treat the forced motion. Approximate analytical solutions
are worked out by means of Hori's perturbation method, the free solutions o
btained in the former paper playing the role of the unperturbed solutions r
equired in the application of the method. These solutions are consistent in
the sense that, with the usual terminology, the rigid body solutions and t
he complex transfer functions are calculated with the same parameters.
Besides in-phase terms, the dissipation at the core-mantle boundary studied
in this paper gives rise to out-of-phase terms. From a qualitative perspec
tive, we discuss the issue of the resonance in this context. The presence o
f dissipation changes dramatically the character of the FCN wobble; that is
, it is no longer a regular oscillation but a damped one. A strict resonanc
e phenomenon cannot take place thereby, since the forcing perturbations are
oscillations with a real (non-complex) frequency.