The conditions that give rise to non-periodic motions of a Jeffcott ro
tor in the presence of non-linear elastic restoring forces are examine
d. It is well known that non-periodic behaviours that characterise the
dynamics of a rotor are fundamentally a consequence of two aspects: t
he non-linearity of the hydrodynamic forces in the lubricated bearings
of the supports and the non-linearity that affects the elastic restor
ing forces in the shaft of the rotor. In the present research the anal
ysis was restricted to the influence of the non-linearity that charact
erises the elastic restoring forces in the shaft, adopting a system th
at was selected the simplest as possible. This system was represented
by a Jeffcott rotor with a shaft of mass that was negligible respect t
o the one of the disk, and supported with ball bearings. In order to c
heck in a straightforward manner the non-linearity of the system and t
o confirm the results obtained through theoretical analysis, an invest
igation was carried out using an experimental model consisting of a ro
tating disk fitted in the middle of a piano wire pulled taut at its en
ds but leaving the tension adjustable. The adopted length/diameter rat
io was high enough to assume the wire itself was perfectly flexible wh
ile its mass was negligible compared to that of the disk. Under such h
ypotheses the motion of the disk centre can be expressed by means of t
wo ordinary, non-linear and coupled differential equations. The condit
ions that make the above motion non-periodic or chaotic were found thr
ough numerical integration of the equations of motion. A number of num
erical trials were carried out using a 4th order Runge-Kutta routine w
ith adaptive stepsize control. This procedure made it possible to plot
the trajectories of the disk centre and the phase diagrams of the com
ponent motions, taken along two orthogonal coordinate axes, with their
projections of the Poincare sections. On the basis of the theoretical
results obtained, the conditions that give rise to non-periodic motio
ns of the experimental rotor were identified.