Abstract

A circular silicone sheet as a masker was used to cover a glass slide, and then the super-hydrophobic coating was sprayed on the glass slide free of silicone sheet masker, thus a round hydrophilic area surrounded by a super-hydrophobic coating is obtained. The PS colloidal droplets are confined in the hydrophilic area, and the droplet volume can be changed within a large range. Variation of the droplet volume influences the initial apparent contact angle. We investigate the particle deposition behavior of the confined colloidal droplet for a hydrophobic apparent contact angle in evaporation process by using an in situ optical observation system. In the whole evaporation process the contact-line of the confined droplet is pinned at the junction between the hydrophilic area and hydrophobic area. In the particle deposition process the main driving flow is different, and the final deposition pattern is controlled by three flow behaviors. In the early stage, the main flow is the Marangoni flow, which drives the particle clusters float on the droplet surfaces, part of them accumulated at the boundaries. As the evaporation proceeds, when the apparent contact angle decreases (<60°), the evaporation flux becomes singular near the contact line, Capillary flow towards the contact inside the drop as a compensation to the solvent loss at the drop boundary, which drives the particles in the droplet to rapidly accumulate at the contact-line. In the last evaporation stage, the thickness of the film in the hydrophilic area becomes very thin, and there is only one layer of particles in this thin film, the thin liquid film instability triggers the particles in the middle area to rapidly aggregate and then form a kind of network pattern, due to the decrease of distances between the particles. Capillary force between particles also takes part in this aggregate process.

Highlights

  • Hydrophobic /hydrophilic confined substrate. (a) A glass slide with confined area treated by superhydrophobic coating, the white part is the coating and the centre is the confined hydrophilic area; (b) measurement of the super-hydrophobic contact angle; (c) SEM image of the cross section of substrate with coating

  • 此外, 液滴蒸发过程中 Marangoni 效应, 毛细补偿流, 薄液层失稳这些作 用的独立及耦合作用机理的深入研究将会有助于 我们实现对胶体晶体生长过程的控制

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Summary

Introduction

在干燥的最后阶段, 亲水区域内的液层变得很薄, 只有一单层粒子存在于这一薄液层 中, 蒸发继续进行时, 薄液层发生失稳使得粒子迅速聚集而形成网络化图案, 由于粒子间距变小, 球间的液桥 毛细力也会参与到这一聚集过程中. 同时 Deegan 等通过在溶液中添加表 面活性剂来改变蒸发过程中溶液表面张力梯度, 来 研究表面活性剂浓度变化导致的 Marangoni 效应 Hu 和 Xu 等 [24−27] 关于液滴 蒸发中 Marangoni 对流的报道进一步补充了颗粒 蒸发自组装机理.

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