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含叠加微凸体的三维粗糙表面接触模型

A FRACTAL MODEL OF CONTACT BETWEEN THREE-DIMENSIONAL ROUGH SURFACES WITH SUPERPOSED ASPERITIES

  • 摘要: 摘要 基于分形理论,建立了含叠加微凸体的粗糙表面接触力学模型。依据Weierstrass-Mandelbrot函数,构建了频率等级优先、脊数优先和曲率半径优先三种叠加微凸体几何轮廓,通过几何对比方式确定出脊数优先建立的叠加微凸体与粗糙表面轮廓较为符合。根据经典接触理论,给出了叠加微凸体中各层发生弹性、弹塑性及完全塑性变形的必要条件。结合微凸体面积分布密度函数,获得了粗糙表面总接触载荷和真实接触面积的内在关系。计算结果表明:叠加微凸体的力学性质取决于其各层微凸体的力学性质,粗糙表面的力学性质由叠加微凸体的力学性质决定。叠加微凸体由N层微凸体叠加而成,若每层微凸体仅能发生弹性变形,则粗糙表面在接触过程中呈现弹性变形状态;若第1至第N-1层微凸体仅能发生塑性变形,粗糙表面表现出完全塑性变形性质;若第1至第I1层微凸体发生弹性变形,第I1+1至第I2层微凸体发生弹塑性变形,第I2+1至第N-1层微凸体发生完全塑性变形,则粗糙表面在接触过程中呈现出完全塑性变形、弹塑性变形、弹性变形顺序的力学性质。本文模型与其他模型、实验的结果对比说明了该模型的合理性。

     

    Abstract: Abstract A fractal model of contact between three-dimensional rough surfaces with superposed asperities is developed based on fractal theory. The superposed asperity is established by prioritized frequency index, prioritized ridge and prioritized radius of single asperity, respectively. It is found that the profile of superposed asperity established by prioritized ridge method does coincide with profile simulated by Weierstrass-Mandelbrot function. The relations between contact area and contact load for each layer of a single superposed asperity in elastic, elastoplastic, fully plastic deformation are given, respectively. The relations between real contact area and total contact load for rough surface are obtained by asperity size distribution function. The results show that the mechanical properties of a single superposed asperity depend on that of each single layer asperity in superposed asperity. The mechanical properties of rough surface depend on that of a single superposed asperity. A superposed asperity which is overlapped by a lot of single asperities has N layers asperities. As only elastic deformation takes place in each layer asperity, the rough surface appears elastic characteristic. As only fully plastic deformation takes place in asperities ranging from the first to N-1th layer, the rough surface appears fully plastic characteristic. As only elastic deformation takes place in asperities ranging from the first to I1th layer, only elastoplastic deformation takes place in asperities ranging from the I1+1th to I2th layer, only fully plastic deformation takes place in asperities ranging from the I2+1th to N-1th layer, a transition from fully plastic, elastoplastic to elastic contact mode takes place in rough surface. A comparison of the present model with the other models is given to verify the rationality of the present model.

     

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