We consider the following two-stages process. At the first stage a body vib
rates and by the dissipation of energy it is heated. At the second state a
slowly varying in time mechanical load is superimposed on the vibrating bod
y. This load creates great plastic deformations. The first stage is modeled
by a coupled system of equations of forced vibration of a viscoelastic bod
y and the heat equation. In the analysis of the second stage we apply the m
odel of plastic flow under great deformations which was introduced and stud
ied in [1].