Frost Formation on Aluminum and Hydrophobic Surfaces

M. R. Haque, A. Betz
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引用次数: 3

Abstract

Ice and frost formation on the surfaces of car windshield, airplanes, air-conditioning duct, transportation, refrigeration and other structures is of great interest due to its negative impact in the efficiency and reliability of the system. Frost formation is a complex and fascinating phenomenon. Frequent defrosting are required to remove the ice that causes economic losses. In order to delay the freezing phenomenon, hydrophobic surfaces (Al-H) were prepared using a very simple and low cost method by dip coating of Aluminum in Teflon© and FC - 40 solution at a ratio of 2:10. Later, the samples were placed on a freezing stage in a computer controlled environmental chamber. The freezing stage was held at a constant temperature of 265 ± 0.5 K. The environmental temperature was set to 295 ± 0.5 K and the relative humidity (RH) was set to 40% and 60% respectively. The samples were observed via optical microscopy from the top and videos of the freezing dynamics were captured. The time required for the whole surface to freeze was named as ‘Freezing time’ and is determined by investigating the consecutive images. The inter-droplet freezing wave propagation was accelerated via a frozen droplet/area and then propagates through the surface very quickly. Ice bridging was also seen for the frost propagation. However, the maximum freezing front propagation velocity was found for Al surfaces at 60% RH. At 40% RH, the Al surface required approximately 10 ± 1 minutes to freeze while the Al-H surface delay freezing until 15 ± 1 minutes. This is due to a slow rate of nucleation and also increased rate of coalescence. At 60% RH, both surface froze faster than 40% RH. The Al surface required 6.5 ± 1 minutes and the Al-H surface froze after 10 ± 1 minutes. The change in freezing kinetics, freezing time, the size of droplets at freezing, and the surface area covered at freezing are all related to the rate of coalescence of droplets. Again, the added thermal resistance of the coating and less water-surface contact area of the droplet to the cooled hydrophobic surface inhibited the growth rate resulting the freezing delay.
铝和疏水表面结霜
汽车挡风玻璃、飞机、空调风管、交通运输、制冷等结构表面的冰和霜的形成对系统的效率和可靠性产生了负面影响,因此引起了人们的极大兴趣。霜的形成是一种复杂而迷人的现象。需要经常解冻,以清除造成经济损失的冰。为了延缓冻结现象,将铝以2:10的比例浸涂在Teflon©和FC - 40溶液中,采用一种非常简单、低成本的方法制备了疏水表面Al-H。之后,这些样品被放置在计算机控制的环境室的冷冻阶段。冻结阶段保持在265±0.5 K恒温。环境温度设定为295±0.5 K,相对湿度(RH)分别设定为40%和60%。通过光学显微镜从顶部观察样品,并捕获冻结动力学的视频。整个表面冻结所需的时间被称为“冻结时间”,并通过调查连续图像来确定。液滴间冻结波通过冻结液滴/区域加速传播,然后在表面快速传播。在霜的传播过程中也观察到冰桥现象。而在60%相对湿度下,Al表面的冻结锋传播速度最大。在40% RH条件下,Al表面需要大约10±1分钟冻结,而Al- h表面延迟冻结至15±1分钟。这是由于成核速率缓慢,同时也增加了聚结速率。在60% RH时,两个表面冻结的速度都快于40% RH。Al表面需要6.5±1分钟,Al- h表面在10±1分钟后冻结。冻结动力学、冻结时间、冻结时液滴大小、冻结时覆盖表面积的变化都与液滴的聚并速率有关。同样,涂层热阻的增加和液滴与冷却的疏水表面接触面积的减少抑制了生长速度,导致冻结延迟。
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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