非圆形毛细管中半月板形状和马兰戈尼流动的研究

Aiqiang Chen, Haoyan Zhang, Jianfei Song, Bin Liu, Chensi Zhang, P. Theodorakis
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摘要

汽液界面是提高换热器换热效率的关键。在本文中,我们报告了乙醇在不同内部横截面的毛细管中蒸发的实验结果,因为所选择的条件允许由于毛细管力的存在而沿着管的内角形成液体膜。为了实现我们的目标,我们使用3D视频显微镜来监测半月板在蒸发过程中的行为,并计算了三个不同横截面形状的通道的毛细管压力,即圆形、正方形和等边三角形横截面,三个固液接触角,即30°、60°和90°。同时,我们将红外热成像技术与粒子成像测速(PIV)可视化技术相结合,对夹角处的剧烈马兰戈尼对流进行了分析。为此,利用红外摄像机和PIV分别测量了马兰戈尼对流在不同视角下的界面温度分布和流态。对于具有夹角的毛细管,半月板处的温度梯度在夹角处达到最大。此外,含角液膜中同时存在温度梯度和对流梯度。当毛细管的角度越小,毛细管效应就会增大,导致形成较厚的膜。我们的研究构成了毛细管角落马兰戈尼流动的“极端”实验。由于毛细力的作用,液体膜可以在多角形管的角部上升到管的入口。此外,乙醇在三角形管角度处的润湿力比在方形管角度处的润湿力大得多。最后,Marangoni涡旋从液体中心相对高温的区域向夹角方向流动,在夹角处蒸发更快,物质和能量的补给更集中。我们期望我们的研究能够揭示不同形状横截面毛细管的半月板形状和马兰戈尼流,这对于各种应用,特别是微流体系统具有重要的基础意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the Meniscus Shape and Marangoni Flow in Capillary Tubes with Noncircular Cross-Section Shapes
The liquid–vapor interface remains a key point for improving the heat transfer efficiency of heat exchangers. In this paper, we report experimental results on the evaporation of ethanol in capillary tubes of different internal cross-sections as the bulk meniscus recedes inside the tube, since the chosen conditions allow for the development of a liquid film along tube's internal corners due to the presence of capillary forces. To achieve our aims, we used 3D video microscopy to monitor the behavior of the meniscus during evaporation and, also, calculated the capillary pressures for three channels with different cross-sectional shapes each, namely circular, square and equilateral triangle cross-sections, for three solid–liquid contact angles, i.e., 30°, 60°, and 90°. At the same time, we have combined infrared thermal imaging technology with particle imaging velocimetry (PIV) visualization technology to analyze the severe Marangoni convection at the included angle. To this end, the interfacial temperature distribution of Marangoni convection was measured by means of an infrared camera and the flow pattern by means of PIV, respectively, through the plane in various views. For capillary tubes with included angle, the temperature gradient at the meniscus reaches its maximum at the included angle. Moreover, both temperature and convective gradients exist in the liquid film with included angle. When the angle of the capillary tube is smaller, the capillary effect will increase, leading to the formation of a thicker film. Our investigation constitutes an "extreme" experiment of Marangoni flow at the corners of the capillary tube. Due to the capillary forces, liquid films can rise in the corners of polygonal tubes up to the entrance of the tubes. Furthermore, the wetting force of ethanol at the angle of the triangle tube is much larger than that in the case of the square tube. Finally, the Marangoni vortex flows from the relatively high-temperature region in the center of the liquid towards the included angle, where evaporation is faster and the recharge of material and energy is more concentrated. We anticipate that our study sheds light into the meniscus shape and Marangoni flow in capillary tubes of with cross-sections of different shapes, which is of fundamental importance for various applications and in particular microfluidic systems.
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