粗糙表面的加卸载分形接触解析模型

陈建江 1; 原园 1; 徐颖强 2

doi:10.7652/xjtuxb201803014

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粗糙表面的加卸载分形接触解析模型

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- 粗糙表面的加卸载分形接触解析模型
- An Analytical Model of Loading-Unloading Contact Between Rough Surfaces Based on Fractal Theory
- 西安交通大学学报 2018年52卷第3期页码：98-110
- 作者机构：
  
  西安理工大学机械与精密仪器工程学院,西安,710048
- 作者简介：
- 基金信息：
  
  : 2017-08-09。作者简介: 陈建江(1992—),男,硕士生;原园(通信作者),男,副教授。基金项目: 国家自然科学基金资助项目(51105304,51475364);中国博士后科学基金资助项目(2014M552467)
- DOI：10.7652/xjtuxb201803014
  中图分类号： TH117
- 网络首发：2018-03-10，
  
  纸质出版：2018
- 稿件说明：
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陈建江 1, 原园 1, 徐颖强 2. 粗糙表面的加卸载分形接触解析模型[J]. 西安交通大学学报, 2018,52(3):98-110.

An Analytical Model of Loading-Unloading Contact Between Rough Surfaces Based on Fractal Theory[J]. 2018, 52(3): 98-110.
陈建江 1, 原园 1, 徐颖强 2. 粗糙表面的加卸载分形接触解析模型[J]. 西安交通大学学报, 2018,52(3):98-110. DOI： 10.7652/xjtuxb201803014.

An Analytical Model of Loading-Unloading Contact Between Rough Surfaces Based on Fractal Theory[J]. 2018, 52(3): 98-110. DOI： 10.7652/xjtuxb201803014.

摘要

基于分形理论

建立了粗糙表面加卸载接触力学模型

推导出了单个微凸体弹性、弹塑性以及塑性变形的存在条件

获得了对应条件下微凸体加、卸载的力学表达式。根据加载终点与卸载起点真实接触面积和总接触载荷不变规则

对传统的微凸体面积密度分布函数进行变换

分别给出了加、卸载接触过程中不同频率指数微凸体的面积密度分布函数

最终得到了加、卸载接触过程中粗糙表面真实接触面积与总接触载荷之间的关系。结果表明:在一个加、卸载接触循环内

粗糙表面加、卸载接触的力学性质取决于微凸体频率指数的范围; 当微凸体的最小频率指数n

min

与临界弹性频率指数n

的关系满足n

min

+5≤n

时

粗糙表面在整个加卸载接触过程中呈现弹性性质; 当n

min

、接触下压量大于微凸体自身临界下压量发生弹塑性变形时

在相同的总接触载荷条件下

卸载过程中的量纲一真实接触面积大于加载过程中的量纲一真实接触面积

且两者的差值与下压量成正比

最大量纲一差值范围为0～0.085 8。

Abstract

Based on fractal theory

a loading-unloading contact mechanics model of rough surfaces is established. The existence conditions of elastic deformation

elastoplastic deformation and fully plastic deformation of single asperity are deduced. And the mechanical expressions of single asperity under loading and unloading are obtained for different deformation conditions. The traditional area density distribution function of asperities is modified according to a rule that the real contact area and total contact load at the end of loading equal the real contact area and total contact load in the inception of unloading. And the

area and density distribution function of asperity's frequency index is deduced under loading and unloading conditions. Eventually

the relationship between total contact load and real contact area is obtained. The results show that the contact mechanical properties of the rough surface depend on the asperity's frequency index in a loading-unloading cycle. When asperity's frequency index n

min

+5 is less than critical elastic frequency index n

the rough surface shows an elastic deformation behavior in a loading-unloading cycle. When the asperity's frequency index n

min

is greater than the critical elastic frequency index and the deformation is greater than the critical deformation

and the real contact area in unloading process is greater than that in loading process. As the deformation increases

the non-dimensional difference between the real areas of loading and unloading is proportional to the deformation

whose range is from 0 to 0.085 8.

关键词

Keywords

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