Sarkar Jayati, Sharma Ashutosh, Shenoy Vijay
Department of Chemical Engineering, Indian Institute of Technology Kanpur, UP 208 016, India.
Langmuir. 2005 Feb 15;21(4):1457-69. doi: 10.1021/la048061o.
We study the phenomenon of debonding in a thin soft elastic film sandwiched between two rigid plates as one of the plates is brought into intimate contact and then pulled away from contact proximity by application of a normal force. Nonlinear simulations based on minimization of total energy (composed of stabilizing elastic strain energy and destabilizing adhesive interaction energy) are employed to address the problems of contact hysteresis, cavitation, crack morphology, variation of contact area, snap-off distance, pull-off force, work done, and energy loss. Below a critical distance (d(c)) upon approach, simulations show the formation of columnar structures and nonrandom, regularly arranged nanocavities at the soft interface at a length scale of approximately 3h (h being the thickness of the film). The persistence of such instability upon withdrawal (distance >>d(c)) indicates a contact hysteresis, which is caused by an energy barrier that separates the metastable states of the patterned configuration and the global minimum state of the flat film. The energy and the pull-off force are found to be nonequilibrium and nonunique properties depending on the initial contact, defects, noise, etc. Three broad pathways of debonding leading to adhesive failure of the interface, depending on the stiffness of the film, step size of withdrawal, and the imposed noise, are identified: a catastrophic column collapse mode, a peeling mode involving a continuous decrease in the contact area, and a column splitting mode. The first two modes are caused by a very high stress concentration near the cavity edges. These metastable patterned configurations engender pull-off forces that are orders of magnitude smaller than that required to separate two flat surfaces from contact.
我们研究夹在两个刚性板之间的薄软弹性膜中的脱粘现象,其中一个板与另一个板紧密接触,然后通过施加法向力将其从接触附近拉开。基于总能量(由稳定的弹性应变能和不稳定的粘附相互作用能组成)最小化的非线性模拟被用于解决接触滞后、空化、裂纹形态、接触面积变化、脱开距离、拉脱力、做功以及能量损失等问题。在接近时低于临界距离(d(c)),模拟显示在软界面处形成柱状结构和非随机、规则排列的纳米空洞,长度尺度约为3h(h为膜的厚度)。在撤回时(距离>>d(c))这种不稳定性的持续表明存在接触滞后,这是由将图案化构型的亚稳态和平坦膜的全局最小态分开的能量势垒引起的。发现能量和拉脱力是非平衡且不唯一的特性,这取决于初始接触、缺陷、噪声等。根据膜的刚度、撤回步长和施加的噪声,确定了导致界面粘附失效的三种主要脱粘途径:灾难性的柱体坍塌模式、涉及接触面积持续减小的剥离模式以及柱体分裂模式。前两种模式是由空洞边缘附近非常高的应力集中引起的。这些亚稳态的图案化构型产生的拉脱力比将两个平坦表面从接触中分离所需的力小几个数量级。