This paper investigates the nonlinear dynamic behavior of a repulsive force actuator from the bifurcation perspective in the cases of primary and principal parametric resonances. The studied model consists of a specific configuration that produces out-of-plane repulsive (levitation) force. The governed equation of motion around static equilibrium is described in the form of a generalized forced Mathieu equation holding quadratic and cubic nonlinearities. While the particular system of interest is one with generated levitation force, the results can be applied to a wide class of MEMS in which the governing equation of motion is classified as the forced Mathieu equation. Coordinate transformation of the systems’ analytical solution from polar to Cartesian is done to preclude the singularity in origin. The frequency response is studied, and analytical expressions for equilibrium positions as fixed points are presented. Assessing the Jacobian matrix, the stability of each branch is examined, and the critical detuning values are defined in which the bifurcations occur. This criterion is then used to border the regions and illustrate the phase portraits of picked points within the regions. The results graphically show that inducing system by the initial conditions corresponding to the fixed points, triggers constant amplitude as well as angle, which ends up with periodic motion. Moreover, the outcome proves that perturbation analysis merely captures the periodic motions and fails to detect quasi-periodic motions. Our analysis provides a platform for further understanding of the repulsive electrostatic force, which is highly nonlinear. The results can be deployed in designing sensors with a wider detection range in which the amplitude jump is measured near the pitchfork bifurcation of principal parametric and cyclic fold bifurcation of primary resonances.
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