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arXiv 2006.11084cond-mat.softcond-mat.mtrl-sciphysics.app-ph
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粗糙金属表面的塑性形变

Plastic deformation of rough metallic surfaces

A. Tiwari, A. Almqvist, B. N. J. Persson

摘要:

我们目前的实验和理论结果的塑性变形金属(铝)块的表面形貌。当一个表面光滑的硬球体(这里是一个钢球、石英玻璃球或氮化硅球)压入一个表面平坦但仍然粗糙的金属块时,由于塑性流动,会产生一个球杯状的压痕。然而,凹进区域中的表面粗糙度并不完全平坦。粗糙度的长波长(宏观粗糙)含量是由原始(铝)表面上的粗糙度引起的,但是现在塑性变形。在塑性变形的宏观粗糙接触区,短尺度的粗糙度是由硬球表面的粗糙度和不均匀的塑性流动引起的。我们使用边界元法,结合一个简单的数值计算过程,考虑到塑性流动的接触力学模型。该理论可以半定量地描述塑性流动对粗糙度的修正。由于在大多数情况下,金属密封的流体泄漏是由长波长粗糙度,我们预测,泄漏可以估计的基础上,这里采用的弹塑性接触力学模型。某些玻璃态聚合物表面的塑性形变与我们观察到的铝表面的塑性变形有很大不同,我们将其归因于强的加工硬化和聚合物的不均匀塑性流动。因此,这里提出的计算塑性流动的数值方法不能应用于一般的玻璃态聚合物。

英文摘要:

We present experimental and theoretical results for the surface topography of a plastically deformed metallic (aluminum) block. When a hard spherical body (here a steel-, silica glass- or silicon nitride ball) with a smooth surface is indented in a metal block with a nominally flat, but still rough, surface, a spherical-cup-like indentation result due to plastic flow. The surface roughness in the indented region is, however, not entirely flattened. The long wavelength (macroasperity) content of the roughness result from the roughness on the original (aluminum) surface, but now plastically deformed. The roughness at short length scale, in the plastically deformed macroasperity contact regions, result from the roughness on the hard ball, and from inhomogeneous plastic flow. We model the contact mechanics using the boundary element method, combined with a simple numerical procedure to take into account the plastic flow. The theory can semi-quantitatively describe the modification of the roughness by the plastic flow. Since the fluid leakage of metallic seals in most cases is determined by the long wavelength roughness, we predict that the leakage can be estimated based on the elastoplastic contact mechanics model employed here. The plastic deformations of surfaces of some glassy polymers is very different from what we observed for aluminum, which we attribute to strong work-hardening and to inhomogeneous plastic flow for the polymers. Thus the numerical procedure to account for the plastic flow proposed here cannot be applied to glassy polymers in general.

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