利用计算机视觉测定微通道流动沸腾中空隙率

M. Schepperle, Shayan Junaid, A. Mandal, D. Selvam, P. Woias
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摘要

孔隙率是表征微尺度通道中两相流沸腾的最关键参数之一。一些重要的热水力参数,如两相粘度和两相密度,可以从孔隙率的知识推导出来。此外,它还被用于许多模型中,以预测微通道中的传热、压降和流动模式。在这种情况下,最常用的空隙率定义是横截面空隙率,它是气相占据的横截面积与通道中给定位置的总横截面积之比[1]。该空隙率通常通过使用麦克斯韦-加内特方程(Maxwell-Garnett equations)进行电阻抗测量来粗略确定,该方程将阻抗和空隙率[2]联系起来,或者通过对微通道中特定位置的光学研究来实现高精度。然而,由于缺乏合适的图像处理,使得光学测定空隙率非常耗时,因为它必须为每帧手动计算。在本研究中,应用计算机视觉实现了微通道中不同位置垂直于流体流动方向的横截面空隙率的自动精确计算。每个通道位置的空隙分数可以连接在一起,以提供整个通道的平均空隙分数的地图。因此,在水压直径分别为430µm和750µm、长度为65 mm的矩形不锈钢微通道中,以去离子水进行两相流沸腾实验。质量流量范围为1.5 ~ 5 g/min,热负荷施加于
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Determination of Void Fraction in Microchannel Flow Boiling Using Computer Vision
Extended Abstract The void fraction is one of the most critical parameters for characterizing two-phase flow boiling in microscale channels. Several important thermal-hydraulic parameters such as two-phase viscosity and two-phase density can be derived from the knowledge of the void fraction. In addition, it is used in numerous models to predict heat transfer, pressure drop and flow patterns in microchannels. The most commonly used definition of void fraction in this context is the cross-sectional void fraction, which is the ratio of the cross-sectional area occupied by the vapor phase to the total cross-sectional area at a given location in the channel [1]. This void fraction is often determined roughly by electrical impedance measurements using the Maxwell-Garnett equations, which relate impedance and void fraction [2], or with high precision by optical studies at specific locations in the microchannel. However, the lack of suitable image processing makes the optical determination of the void fraction very time-consuming, since it must be calculated manually for each frame. In this study, computer vision was applied to realize an automatic and accurate calculation of cross-sectional void fractions perpendicular to the fluid flow direction at different locations in microchannels. The void fractions of each channel location could be linked together to provide a map of the average void fraction of the entire channel. Therefore, two-phase flow boiling experiments were performed with DI water in rectangular stainless-steel microchannels with hydraulic diameters of 430 and 750 µm and lengths of 65 mm. The mass flow rate ranged from 1.5 to 5 g/min and the heat load applied to the
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