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Adhesion and friction in hard and soft contacts: theory and experiment

机译:粘附和摩擦在硬和软接触中:理论与实验

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This paper is devoted to an analytical, numerical, and experimental analysis of adhesive contacts subjected to tangential motion. In particular, it addresses the phenomenon of instable, jerky movement of the boundary of the adhesive contact zone and its dependence on the surface roughness. We argue that the “adhesion instabilities” with instable movements of the contact boundary cause energy dissipation similarly to the elastic instabilities mechanism. This leads to different effective works of adhesion when the contact area expands and contracts. This effect is interpreted in terms of “friction” to the movement of the contact boundary. We consider two main contributions to friction: (a) boundary line contribution and (b) area contribution. In normal and rolling contacts, the only contribution is due to the boundary friction, while in sliding both contributions may be present. The boundary contribution prevails in very small, smooth, and hard contacts (as e.g., diamond-like-carbon (DLC) coatings), while the area contribution is prevailing in large soft contacts. Simulations suggest that the friction due to adhesion instabilities is governed by “Johnson parameter”. Experiments suggest that for soft bodies like rubber, the stresses in the contact area can be characterized by a constant critical value. Experiments were carried out using a setup allowing for observing the contact area with a camera placed under a soft transparent rubber layer. Soft contacts show a great variety of instabilities when sliding with low velocity — depending on the indentation depth and the shape of the contacting bodies. These instabilities can be classified as “microscopic” caused by the roughness or chemical inhomogeneity of the surfaces and “macroscopic” which appear also in smooth contacts. The latter may be related to interface waves which are observed in large contacts or at small indentation depths. Numerical simulations were performed using the Boundary Element Method (BEM).
机译:本文致力于对切向运动的粘合触点的分析,数值和实验分析。特别地,它解决了粘合接触区的边界的不稳定,生涩运动的现象及其对表面粗糙度的依赖性。我们认为,“粘合不稳定性”与接触边界的不稳定运动导致能量耗散与弹性不稳定性机制类似。当接触面积膨胀和收缩时,这导致不同的有效粘合作品。这种效果在“摩擦”对接触边界的运动方面解释。我们考虑了摩擦的两个主要贡献:(a)边界线贡献和(b)区域贡献。在正常和滚动的触点中,唯一的贡献是由于边界摩擦,而在滑动中,也可以存在两个贡献。边界贡献在非常小,光滑和硬触点(例如,金刚石 - 碳(DLC)涂层)中占上去,而该面积贡献在大型软触点中是普遍存在的。模拟表明,由于粘附不稳定性导致的摩擦受“约翰逊参数”的管辖。实验表明,对于橡胶等软体,接触面积中的应力可以通过恒定的临界值表征。使用设置进行实验,允许使用放置在软透明橡胶层下的相机观察接触区域。软触点以低速滑动时显示出各种各样的不稳定性 - 取决于缩进深度和接触体的形状。这些不稳定性可以被归类为由表面的粗糙度或化学不均匀性和“宏观”的“显微镜”分类,以及在平滑触点中出现的“宏观”。后者与在大触点或小凹口深度中观察到的界面波有关。使用边界元法(BEM)进行数值模拟。

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