Heat flow characteristics of Titanium elliptical low rib groove tube with outer falling film evaporation

被引:0
|
作者
Peng D. [1 ]
Xie Y. [1 ]
Jiang W. [2 ]
Yu T. [3 ]
Wu S. [1 ]
Tan Z. [1 ]
Wang Z. [1 ]
机构
[1] School of Mechanical Engineering and Mechanics, Xiangtan University, Xiangtan
[2] Hunan Changxing Energy Environmental Protection Technology Company Limited, Changsha
[3] School of Mechanical Engineering, Hunan University of Technology, Zhuzhou
来源
Zhongguo Shiyou Daxue Xuebao (Ziran Kexue Ban)/Journal of China University of Petroleum (Edition of Natural Science) | 2024年 / 48卷 / 02期
关键词
ellipse coefficient; falling film evaporation; liquid film distribution; Titanium elliptical low rib transverse groove tube; vapor-holdup;
D O I
10.3969/j.issn.1673-5005.2024.02.019
中图分类号
学科分类号
摘要
In order to improve the heat transfer efficiency of the falling film evaporator with a titanium elliptical low rib transverse groove tube, the heat flow characteristics of the liquid film flow outside the tube were numerically simulated with the ellipse coefficient E being in the range of 1. 0 to 2. 0. The results show that, there are different degrees of the dry patches outside the tube. The liquid film is significantly thicker near the dry patches than in other areas, and the liquid film coverage is the highest when the value of E is 1. 2. The liquid film spreads slower in both of the axial and circumferential directions. The liquid film̍s velocity at the upper of the tube decreases abruptly between Z∗ = -0. 25 ~ -0. 375 and 0. 25 ~ 0. 375 when E is 1. 0 and 1. 8, and the changing trend of liquid film̍s thickness along the axial direction from the position directly below the spray nozzle to the far end of the spray nozzle decreases firstly and then increases. The maximum heat transfer coefficient increases with the increase of E. The tube wall has the highest heat transfer coefficient at the junction between the liquid film and the dry patches, and the average heat transfer coefficient increases and then decreases. Compared to the round tube, the average heat transfer coefficient increases by 34. 5% and 15. 7% when E is 1. 2 and 2. 0, respectively. The distribution of vapor-holdup in the tank is opposite to that of the liquid film. The overall vapor-holdup of the liquid film firstly increases and then decreases with the increase of E, and the difference between the average vapor-holdup inside and outside the tank increases with the increase of E. © 2024 University of Petroleum, China. All rights reserved.
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页码:170 / 178
页数:8
相关论文
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