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Indentation of a rigid sphere into an elastic substrate with surface tension and adhesion

机译:通过表面张力和附着力将硬球压入弹性基材

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摘要

The surface tension of compliant materials such as gels provides resistance to deformation in addition to and sometimes surpassing that owing to elasticity. This paper studies how surface tension changes the contact mechanics of a small hard sphere indenting a soft elastic substrate. Previous studies have examined the special case where the external load is zero, so contact is driven by adhesion alone. Here, we tackle the much more complicated problem where, in addition to adhesion, deformation is driven by an indentation force. We present an exact solution based on small strain theory. The relation between indentation force (displacement) and contact radius is found to depend on a single dimensionless parameter: ω=σ(μR)−2/3((9π/4)Wad)−1/3, where σ and μ are the surface tension and shear modulus of the substrate, R is the sphere radius and Wad is the interfacial work of adhesion. Our theory reduces to the Johnson–Kendall–Roberts (JKR) theory and Young–Dupre equation in the limits of small and large ω, respectively, and compares well with existing experimental data. Our results show that, although surface tension can significantly affect the indentation force, the magnitude of the pull-off load in the partial wetting liquid-like limit is reduced only by one-third compared with the JKR limit and the pull-off behaviour is completely determined by ω.
机译:诸如凝胶之类的顺应性材料的表面张力除了弹性而且有时甚至超过弹性,还提供了抗变形的能力。本文研究了表面张力如何改变压入软弹性基材的小硬球的接触力学。先前的研究已经检查了外部负载为零的特殊情况,因此接触仅由粘附力驱动。在这里,我们解决了更为复杂的问题,其中除了粘附力之外,变形还由压入力驱动。我们提出基于小应变理论的精确解决方案。发现压入力(位移)和接触半径之间的关系取决于单个无量纲参数:ω=σ(μR) −2/3 ((9π/ 4)Wad)- 1/3 ,其中σ和μ是基底的表面张力和剪切模量,R是球体半径,Wad是粘附的界面功。我们的理论分别在小和大ω的范围内简化为Johnson-Kendall-Roberts(JKR)理论和Young-Dupre方程,并与现有实验数据进行了比较。我们的结果表明,尽管表面张力会显着影响压痕力,但与JKR极限相比,部分润湿液体状极限中的拉力载荷大小仅降低了三分之一,并且拉力行为为完全由ω决定。

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