典型机动飞行状态下轴承-转子系统非线性刚度及动态特性分析

Nonlinear stiffness and dynamic characteristics analysis of bearing-rotor system under typical maneuvering flight conditions

  • 摘要: 飞机进行机动飞行时产生的附加载荷使得航空发动机主轴承刚度发生变化,影响着航空发动机转子系统动态特性。考虑滚动体与内/外圈之间相互作用与相对位置关系,建立滚动轴承拟静力学模型,并与转子有限元模型进行耦合,建立考虑典型盘旋机动载荷作用的滚动轴承-转子系统动力学模型;利用Newmark-β积分法对系统动力学方程进行求解,揭示机动载荷作用下轴承刚度特性变化规律;基于轴承刚度分析结果,分析不同的机动飞行状态下转子系统动态特性变化规律。结果表明:机动载荷会使轴承刚度发生非线性变化,附加离心力、附加陀螺力矩作用下轴承刚度变化趋势相反;不同半径盘旋机动飞行状态下,轴承刚度变化趋势分别受附加离心力或附加陀螺力矩主导;机动载荷会使转子一阶临界转速增加,对整个系统产生刚度增强效应;附加离心力和附加陀螺力矩使轮盘中心的轴心轨迹发生不同方向的偏移,而机动载荷下轴承刚度非线变化会改变偏移量大小。

     

    Abstract: The additional loads generated when the aircraft carries out maneuvering flight make the main bearing stiffness of the aero-engine change, which affects the dynamic characteristics of the aero-engine rotor system. Considering the interaction and relative position relationship between rolling body and inner and outer rings, the quasi-static model of rolling bearing is established, and coupled with the rotor finite element model, the dynamic model of rolling bearing-rotor system is established to consider the role of typical hovering maneuvering load; the system dynamic equations are solved by using the Newmark-β integration method to reveal the changing law of the bearing stiffness characteristics under the action of maneuvering load; based on the results of bearing stiffness analysis, the dynamic characteristics of the rotor system under different maneuvering flight conditions are analyzed. The results show that: the maneuvering load will make the bearing stiffness change nonlinearly, and the bearing stiffness change trend is opposite under the action of additional centrifugal force and additional gyroscopic moment; under the maneuvering flight condition of different radii, the bearing stiffness change trend is dominated by the additional centrifugal force or the additional gyroscopic moment, respectively; the maneuvering load makes the first-order critical speed of rotor increase, and the stiffness enhancement effect is produced for the whole system; the additional centrifugal force and additional gyroscopic moment make the axis trajectory of the wheel center offset in different directions, and the nonlinear change of bearing stiffness under maneuvering load will change the offset.

     

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