Abstract
Vibration generated by engine and its accessories deteriorates product performance. At present, lacking global model, mounting design of engine and accessories are separate, not conductive to solving the vibration of engine, belt, and accessories as a whole. In this article, three problems of the typical structure are analyzed, that is, the belt tension is unstable, static preloading makes engine mount design deviate, and the belt is prone to lateral vibration. Then, a rigid constraint rod is proposed to fix the center distance. The vibrational motion equation is established. By matrix analysis, the accessory mount along the rod is canceled. Then, engine and accessories can be analyzed as independent systems. Among them, the vibration isolation of the engine tends to be good, and for accessories and belts, the influences of the accessory mount stiffness on the force and torque transmission rate and belt vibration response were comprehensively evaluated, and that the infinite stiffness is presented. The innovative design of five-rod structure mainly composed of two connecting rods is obtained which does not transfer vibration perpendicular to rod and the vibration of engine, belt, and accessories are all well controlled. This experiment proves the five-link structure as a useful solution.
Highlights
Engine–accessory system is a common configuration of many mechanical products
Analysis of the accessory subsystem transfer rate and belt vibration response For the rod connection effect, the accessory subsystem is attached to the engine subsystem and vibrates with it in the xa direction, and the xaÀdof in this direction of the accessory subsystem need not be studied
The vibration isolation performance is satisfied, we found the lateral vibration of the belt is still serious
Summary
Engine–accessory system is a common configuration of many mechanical products. Engine and accessories are vibration excitation sources to belt, and belt is excited to resonance. According to the above analysis, the generalized force matrix of the motion equation is shown in equation (5), where m0 and n0 are the horizontal and vertical distances between the input wheel center of the accessory subsystem and the compressor belt pulley center, respectively p1ðtÞ
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