The differential equation of motion of a nonlinear viscoelastic beam i
s established and is based on a novel and sophisticated stress-strain
law for polymers. Applying this equation we examine a periodically for
ced oscillation of such a simply supported beam and search for possibl
e chaotic responses. To this purpose we establish the Holmes-Melnikov
boundary for the system. All further investigations are developed by m
eans of a computer simulation. In this connection the authors examine
critically the Poincare mapping and the Lyapunov exponent techniques a
nd distinguish in this way between chaotic and regular motion. A set o
f control parameters of the equation is found, for which either a chao
tic or a regular motion can be generated, depending on the initial con
ditions and the corresponding basins of attraction. Thus, in this part
icular case two attractors of completely different nature-regular and
chaotic, respectively-coexist in the phase space. The basins of attrac
tion of the two attractors for a fixed instant of time are plotted, an
d appear to possess a very complex fractal geometry.