Numerical study on dynamic behaviours of a micro-droplet impacting on a vertical wall in PEMFC

被引:8
|
作者
Zhang, Zhen [1 ]
Zhao, Juan [1 ]
Ling, Xiang [1 ]
Ma, Jie [1 ]
机构
[1] Nanjing Tech Univ, Sch Mech & Power Engn, 30 PuZhu South Rd, Nanjing 211816, Peoples R China
关键词
PEMFC; Micro-droplet impact; Vertical wall; Numerical simulation; Dynamic behaviour; Transition from spreading to; rebound; GAS-DIFFUSION LAYER; WATER DROPLET; HEAT-TRANSFER; LEVEL SET; SIMULATIONS;
D O I
10.1016/j.ijhydene.2021.03.006
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The droplet/wall interaction in the gas channel (GC) of proton exchange membrane fuel cells (PEMFCs) has significant influence on water management, which may affect the performance and durability of the cell. In this paper, a coupled level-set and volume-of fluid (CLSVOF) method is used to simulate the dynamic behaviours of a micro-droplet impacting on a vertical wall in the GC. The effects of impact velocity (expressed by the Weber number, We), and impact angle on the spreading dynamics are evaluated. Next, the critical conditions for the transition from spreading to rebound are further discussed. For 0 < We <80, only the spreading, retracting, and rebound are observed, and the phenomenon of air bubble entrapment is captured on different wettable walls. With an increment of We, the maximum total spreading factor l* tot and corresponding normalised time t* will increase, as well as the normalised time difference DT2 between the maximum spreading length and minimum height. Moreover, when increasing the impact angle, the maximum front spreading factor depending on the tangential velocity component will decrease, while the absolute value of maximum back spreading factor squeezed by the normal velocity component will increase. For the oblique downward impact, the front liquid led by the tangential velocity component plays a more important role in dominating the spreading process. The results also indicate that both the wall wettability and We can affect the transition threshold. When the static contact angle is between 90 degrees and 150 degrees, the effect of We on the rebound is inversely proportional to the hydrophobicity of the wall. (C) 2021 Hydrogen Energy Publications LLC. Published by Elsevier Ltd. All rights reserved.
引用
收藏
页码:18557 / 18570
页数:14
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