弹塑性轴对称正弦表面凹凸接触

S. Saha, R. Jackson
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引用次数: 5

摘要

弹塑性球面接触和正弦接触的封闭有限元经验解是可行的。然而,其中一些模型没有考虑与相邻凸起的相互作用的影响,或者因为它们采用全三维模型而需要大量的数值资源。本文在建模时考虑了这些因素。目前的有限元模型(FEM)是一个接触刚性平面的轴对称弹塑性正弦波表面,它具有广泛的材料特性和不同的振幅与波长比值。数值结果与现有弹塑性球面接触模型进行了比较。导出了两个表面达到完全接触的临界压力的经验方程。当两个接触面之间没有间隙时,就会发生完全接触。还建立了从初始接触到完全接触将发生完全弹性变形的正弦粗糙度振幅临界值的方程。目前的研究发现,对于振幅低于临界值且具有弹性性质的情况,可以使用先前发表的完全弹性模型。结果适用于几乎所有种类的金属材料。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Elastic-plastic axisymmetric sinusoidal surface asperity contact
Closed-form finite-element empirical solutions are available for elastic-plastic spherical and sinusoidal contact. However, some of these models do not consider the effect of interaction with adjacent asperities or require extensive numerical resources because they employ a full 3-D model. The present work has considered these factors during modeling. The current finite element model (FEM) represents an axisymmetric elastic-plastic sinusoidal surface in contact with a rigid flat for a wide range of material properties and different values of the amplitude to wavelength ratio. The numerical results are compared with the existing elastic-plastic spherical contact model. Empirical equations are derived for the critical pressure at which two surface will reach complete contact. Complete contact occurs when there is no gap remaining between two contacting surfaces. An equation for the critical value of the amplitude of the sinusoidal asperity below which it will deform completely elastically from initial to complete contact is also established. The current study finds that for the cases which have amplitudes that fall below the critical value, and are elastic in nature, that the previously published perfectly elastic model can be used. The results are applicable for almost all kinds of metallic materials.
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