无接触粘附:弹流粘附

Vincent Bertin, Alexandros T. Oratis, Jacco H. Snoeijer
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引用次数: 0

摘要

干燥固体表面之间的粘附力通常由接触力决定,涉及表面力和弹性。对于浸入液体中的表面,由于液体间隙打开时的粘性阻力,会产生非接触粘附力。虽然干固体之间的粘附可以用经典的 JKR 理论来描述,但对于软固体的湿粘附却没有相应的框架。在这里,我们从理论上研究了球体与弹性基体分离过程中出现的粘性粘附力。固体之间的粘性薄膜内的吸力会引起显著的弹性位移。出乎意料的是,弹性基体紧跟球体运动,导致无接触粘连。初始动力学是用相似解来描述的,结果产生了一个非线性粘附力,该粘附力随时间 F ~ t^(2/3) 而增长。当弹性位移变得足够大时,就会出现另一种相似解,通过有限次奇异性导致粘着接触的剧烈断裂。观察到的现象与 JKR 理论非常相似,并且与涉及粘性粘附的广泛应用相关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Sticking without contact: Elastohydrodynamic adhesion
The adhesion between dry solid surfaces is typically governed by contact forces, involving surface forces and elasticity. For surfaces immersed in a fluid, out-of-contact adhesion arises due to the viscous resistance to the opening of the liquid gap. While the adhesion between dry solids is described by the classical JKR theory, there is no equivalent framework for the wet adhesion of soft solids. Here, we investigate theoretically the viscous adhesion emerging during the separation of a sphere from an elastic substrate. The suction pressure within the thin viscous film between the solids induces significant elastic displacements. Unexpectedly, the elastic substrate closely follows the motion of the sphere, leading to a sticking without contact. The initial dynamics is described using similarity solutions, resulting in a nonlinear adhesion force that grows in time as F ~ t^(2/3). When elastic displacements become large enough, another similarity solution emerges that leads to a violent snap-off of the adhesive contact through a finite-time singularity. The observed phenomenology bears a strong resemblance with JKR theory, and is relevant for a wide range of applications involving viscous adhesion.
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