论文标题

从胶体液体桥的蒸发中的可延展图案:咖啡环到扇贝壳

Malleable patterns from the evaporation of colloidal liquid bridge: coffee ring to the scallop shell

论文作者

Chattopadhyay, Ankur, S, Srinivas Rao, Hegde, Omkar, Basu, Saptarshi

论文摘要

本文强调了一种从液体桥配置中的干液滴产生对比模式的方法,与众所周知的咖啡环不同。降低限制距离(固体表面之间的间隙)导致系统化的纳米粒子聚集的屈服,类似于发言的模式,类似于在扇贝壳上而不是圆周边缘沉积。限制长度的改变调节曲率需要跨液体蒸气界面的蒸发通量变化。因此,不同液体桥(LB)内部的流动在不同的限制长度方面有很大变化。较小的限制长度导致挤压液体桥的粘粘运动。相反,拉伸的LBS表现出固定的接触线。我们破译了一个主张,即在三相接触线附近脱水过程中存在的干燥液薄膜是负责颗粒的排列沉积。限制距离决定了这种薄膜的高度,其理论估计是使用反射干涉法对实验观察结果进行验证的,进一步表现出良好的一致性(按数量级)。调节粒径不会显着影响沉淀模式。但是,颗粒浓度可以基本影响沉积模式。沉积模式的差异归因于蒸发通量梯度的复杂相互作用引起的接触线运动与脱水过程中薄液膜的干燥结合使用。

The present article highlights an approach to generate contrasting patterns from drying droplets in a liquid bridge configuration, different from well-known coffee rings. Reduction of the confinement distance (the gap between the solid surfaces) leads to systematized nano-particle agglomeration yielding to spokes-like patterns similar to those found on scallop shells instead of circumferential edge deposition. Alteration of the confinement length modulates the curvature that entails variations in the evaporation flux across the liquid-vapor interface. Consequently, flow inside different liquid bridges (LBs) varies significantly for different confinement lengths. Small confinement lengths result in the stick-slip motion of squeezed liquid bridges. On the contrary, the stretched LBs exhibit pinned contact lines. We decipher a proposition that a drying liquid thin film present during dewetting near the three-phase contact line is responsible for the aligned deposition of particles. The confinement distance determines the height of this thin film, and its theoretical estimations are validated against the experimental observations using reflection interferometry, further exhibiting good agreement (in order of magnitude). Modulating the particle size does not significantly influence the precipitate patterns; however, particle concentration can substantially affect the deposition patterns. The differences in deposition patterns are attributed to the complex interplay of the gradient of evaporation flux induced motion of contact line in combination with the drying of thin liquid film during dewetting.

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