Condensation Droplet Distribution Affected by Electrowetting Approach

Run-gang Yan, Chung-Lung Chen
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Abstract

This paper presents a visualization of condensation droplet distribution affected by the electrowetting-on-dielectric (EWOD) approach. A single-side double-layer-electrode design (grid wire, thin wire, and thick wire) and coplanar-electrode design (zigzag) are discussed. Side-by-side experiments with applied 40V DC electric potential are carried out to compare droplet distribution between charged and uncharged devices with the identical design. The uncharged devices show a random droplet distribution, whereas charged devices have a regulated distribution based on the designed patterns. As droplets on the electrode boundaries become larger, they are likely to slide away and stay in electrode-free regions. The droplets ‘sit’ inside the grid wires and distribute vertically along thin and thick wires. On the coplanar-electrode zigzag device, droplets cover the electrode gaps and are distributed vertically. The charged surfaces lead to a faster droplet growth rate, resulting in larger droplet size and more dispersed droplet distribution. This phenomenon accelerates droplets’ shedding frequency and frees up more condensing areas for small droplets to nucleate and grow. The first shedding moment of the charged surfaces occurs earlier than the uncharged ones for all types of EWOD devices. The detected droplet shedding diameter ranges from 1.2 mm to 2 mm in this study. The work presented in this paper introduces a novel approach to actively influence droplet distribution on microfabricated condensing surfaces and indicates great potential for improving condensation heat transfer rate via EWOD.
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电润湿方法对冷凝液滴分布的影响
本文给出了电介质电润湿(EWOD)方法对冷凝液滴分布影响的可视化图。讨论了单面双层电极设计(网格线、细线和粗线)和共面电极设计(锯齿形)。在外加40V直流电势的情况下,对相同设计的带电和不带电器件的液滴分布进行了对比实验。未带电器件的液滴分布是随机的,而带电器件的液滴分布是基于设计的模式而调节的。当电极边界上的液滴变大时,它们很可能会滑动并停留在无电极区域。液滴“坐在”网格线内,沿着细线和粗线垂直分布。在共面电极之字形装置上,液滴覆盖在电极间隙上并垂直分布。带电表面导致液滴生长速度加快,液滴尺寸增大,液滴分布更加分散。这种现象加速了液滴的脱落频率,并释放出更多的冷凝区域,供小液滴成核和生长。在所有类型的EWOD器件中,带电表面的第一次脱落时刻比不带电表面的第一次脱落时刻发生得早。本研究检测到的液滴脱落直径范围为1.2 ~ 2mm。本文介绍了一种主动影响微加工冷凝表面液滴分布的新方法,表明了通过EWOD提高冷凝换热率的巨大潜力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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