The equations of motion of a two-degrees-of-freedom mass in a magnetic
bearing are non-linear in displacement, with geometric coupling of th
e magnetic bearing coupling the horizontal and vertical components of
rotor motion. The non-linear forced response is studied in two ways: (
1) using imbalance force; (2) using non-imbalance harmonic force. In t
he forced response, only periodic motion is investigated here. Stable
periodic motion is obtained by numerical integration and by the approx
imate method of trigonometric collocation. Where unstable motion coexi
sts with stable motion after a bifurcation of periodic motion, the uns
table motion is obtained by the collocation method. The periodic motio
ns local stability and bifurcation behavior are obtained by Floquet th
eory. The parameters i.e., rotor speed, imbalance eccentricity, forcin
g amplitude, rotor weight, and geometric coupling are investigated to
find regimes of non-linear behavior such as jumps and subharmonic moti
on. (C) 1998 Academic Press.