超疏水表面对微系统润湿的影响

W. Li, R. Mohamadi, A. Amirfazli
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引用次数: 0

摘要

为了开发高效节能的微流体系统,重要的是要尽量减少液体对系统表面的粘附。文献中提出的方法之一是使用超疏水表面,即接触角超过150度的表面(对于水)。然而,文献中普遍没有深入考虑的问题是接触角滞后的作用(前后接触角的差异)。换句话说,要实现高效的微流体液滴驱动系统,仅使用具有大接触角的表面是不够的,而且还应具有低接触角迟滞(CAH)。接触角滞后是润湿过程中常见的现象。从理论上研究CAR对微系统超疏水表面的优化设计是很重要但困难的。我们将提出一种基于微纹理表面的自由能分析来计算CAR的通用方法。采用具有代表性的二维模型代替三维模型,极大地简化了接触角的热力学状态和自由能垒的计算,使通用性损失最小。选择一个柱状表面结构作为典型的例子(见图1)。结果表明,该方法可以预测与Wenzel和Cassie方程预测一致的CAR和平衡接触角。该方法还可以提供非复合和复合结构之间过渡的标准(即液体在表面上的自由扩散或在通道中液滴和表面之间实现最小接触面积)。本文还将讨论超疏水表面润湿的最新实验结果。
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Effect of Superhydrophobic Surfaces for Wetting in Micro-Systems
To develop energy efficient microfluidic systems it is important to minimize the adhesion of the liquid to the surfaces in the system. One of the proposed methods in the literature is to use superhydrophobic surfaces, i.e. surfaces with contact angles above 150 degrees (for water). However, the issue that is not generally considered in depth in literature is the role of contact angle hysteresis (the difference between advancing and receding contact angles). In other words, to have an energy efficient droplet actuation system for microfluidics it is not sufficient to use surfaces that have large contact angles, but they also should have low contact angle hysteresis (CAH). Contact angle hysteresis is a common phenomenon in wetting. It is important but difficult to theoretically investigate CAR to optimally design superhydrophobic surfaces for micro-systems. We will present a universal approach to calculate CAR based on a free energy analysis for micro-textured surfaces. Thermodynamic status of contact angles and calculation of free the energy barrier are significantly simplified by using a representative 2D model instead of a 3D model with minimum loss of generality. A pillar surface structure is chosen as a typical example (see Figure 1). It is demonstrated that this approach can predict CAR and equilibrium contact angles that are consistent with predictions of Wenzel's and Cassie's equations. This approach can also provide a criterion for transition between noncomposite and composite structures (i.e. free spreading of liquids on a surface or achieving minimum contact area between a liquid drop and surfaces in a channel). Recent experimental results for wetting of superhydrophobic surfaces will also be discussed.
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