Lin Ji, Lin Yuan, Qian Jin
Department of Engineering Mechanics, Soft Matter Research Center, Zhejiang University , Hangzhou, Zhejiang 310027, China.
Langmuir. 2014 Jun 3;30(21):6089-94. doi: 10.1021/la404153t. Epub 2013 Dec 19.
It is widely known in adhesive contact mechanics that a spherical particle will not detach from an elastic half-space unless a critical level of pulling force is reached, as already revealed by JKR- or DMT-type deterministic models. This article focuses on the scenario of particle-substrate adhesion where the size of particles is down to the nanometer scale. A consequence of particle size reduction to this range is that the energy scale confining the state of system equilibrium becomes comparable to the unit of thermal energy, leading to statistical particle detachment even below the critical pull-off force. We describe the process by Kramers' theory as a thermally activated escape from an energy well and develop a Smoluchowski partial differential equation that governs the spatial-temporal evolution of the adhesion state in probabilistic terms. These results show that the forced or spontaneous separation of nanometer-sized particles from compliant substrates occurs diffusively and statistically rather than ballistically and deterministically as assumed in existing models.
在粘着接触力学领域广为人知的是,除非达到临界拉力水平,球形颗粒不会从弹性半空间脱离,这一点已由JKR型或DMT型确定性模型揭示。本文聚焦于颗粒尺寸降至纳米尺度的颗粒 - 基底粘附情况。颗粒尺寸减小到这个范围的一个结果是,限制系统平衡状态的能量尺度变得与热能单位相当,导致即使在临界脱附力以下也会发生统计性的颗粒脱离。我们用克莱默斯理论将这个过程描述为从能量阱的热激活逃逸,并推导了一个斯莫卢霍夫斯基偏微分方程,该方程从概率角度描述了粘附状态的时空演化。这些结果表明,纳米级颗粒从柔性基底上的强制或自发分离是以扩散和统计的方式发生的,而不是像现有模型所假设的那样以弹道和确定性的方式发生。