Department of Chemical Engineering, Waterloo Institute for Nanotechnology, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada.
Department of Mechanical & Mechatronics Engineering, Waterloo Institute for Nanotechnology, University of Waterloo, Waterloo, Ontario N2L 3G1, Canada.
J Colloid Interface Sci. 2022 Dec 15;628(Pt B):788-797. doi: 10.1016/j.jcis.2022.08.075. Epub 2022 Aug 17.
The conventional solid-solid contact is well studied in the literature. However, a number of practical applications, such as adhesive patches and biomimetic surfaces, require a much deeper understanding of soft contact where there is a distinct time-dependent adhesion behavior due to the dual-phase structure (solids and liquids). To understand this, currently existing solid-solid contact behavior is extrapolated to soft contact, wherein the size-effect of the gel film and the preload are typically neglected. When introducing the finite-size effect and preload, gels could experience distinctive long-term contact dynamics in contact with another material.
We reconstruct the evolving surface profile of the gel films intercalated between a glass sphere and glass slide using dual wavelength-reflection interference contrast microscopy. The macro-sized glass sphere compresses the gel. The indentation depth is comparable to the gel film thickness, wherein the conventional contact theories are inapplicable.
The gel surface experiences two deformation stages. The natural preload and elastic force develop the contact area in the early state. In the later state, the viscous free molecules of the gel develop the ridge. We discover that the residual surface stress relaxes over 85 hr. Our findings on the long-term gel deformation provide a new perspective on soft adhesion, from developing soft adhesives to understanding biological tissues.
传统的固-固接触在文献中已有很好的研究。然而,许多实际应用,如粘性贴片和仿生表面,需要更深入地了解软接触,因为双相结构(固体和液体)导致明显的时间依赖性粘附行为。为了理解这一点,目前存在的固-固接触行为被推断到软接触中,其中凝胶膜的尺寸效应和预载通常被忽略。当引入有限尺寸效应和预载时,凝胶在与另一种材料接触时可能会经历独特的长期接触动力学。
我们使用双波长反射干涉对比显微镜重建玻璃球和玻璃片之间夹层凝胶膜的表面轮廓。宏观尺寸的玻璃球压缩凝胶。压痕深度与凝胶膜厚度相当,此时传统的接触理论不适用。
凝胶表面经历两个变形阶段。在早期阶段,自然预载和弹性力会扩展接触面积。在后期阶段,凝胶的粘性自由分子会形成脊。我们发现,残余表面应力在 85 小时内得到释放。我们对长期凝胶变形的研究为软粘附提供了一个新的视角,从开发软粘附到理解生物组织。