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In the paper the problem of stability of a journal bearing system with divided and movable shell controlled by piezoelectric elements is considered. The shell consists of three segments - two fixed and the middle one driven by a piezoelectric actuator. This way the actuator affects the size of the oil gap - one of the most important parameters responsible for the stability threshold of the system. The paper presents the concept and provides one with theoretical fundamentals. Considerations are based on a simplified Reynolds equation. Nonlinear behaviour and its sensitivity to the applied method of stabilisation is examined in the direct neighbourhood of the critical threshold. A bifurcating, near-critical solution is introduced and analysed for this purpose. Results of numerical simulations prove that the method is effective and brings considerable growth of the critical speed. It is found however, that this effect is associated with increase of Floquet's exponent, which physically means that the system can exhibit subcritical bifurcation (hard self-excitation). A compromise is then required in obtaining an optimal control.
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