2021
DOI: 10.1021/acs.energyfuels.1c02023
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Effects of the Structure, Wettability, and Rib-Channel Width Ratio on Liquid Water Transport in Gas Diffusion Layer Using the Lattice Boltzmann Method

Abstract: The gas diffusion layer (GDL) plays a key role in water management. The effects of the structure, wettability, and rib-channel width ratio on liquid water transport in GDL are studied using a multiphase lattice Boltzmann method (LBM) model. It is found that the liquid water in GDL shows capillary fingering behavior. With the increase of carbon fiber diameter or porosity, the water saturation in GDL increases, and the time for liquid water to break through GDL decreases. The porosity has a significant effect on… Show more

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Cited by 18 publications
(5 citation statements)
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“…This is probably due to the water saturation level under ribs of the flow field (Figure b). Since the GDL under cold ribs had a large liquid water saturation level at low temperatures, , oxygen diffusion was hindered, resulting in increased R GDL . When GDLs were stacked in the cell, R GDL had little influence on the cell temperature (Figure c) because the thick GDL layer harvested the uniform gas supply to the CL, even if liquid water accumulated under cold ribs (Figure c).…”
Section: Resultsmentioning
confidence: 99%
“…This is probably due to the water saturation level under ribs of the flow field (Figure b). Since the GDL under cold ribs had a large liquid water saturation level at low temperatures, , oxygen diffusion was hindered, resulting in increased R GDL . When GDLs were stacked in the cell, R GDL had little influence on the cell temperature (Figure c) because the thick GDL layer harvested the uniform gas supply to the CL, even if liquid water accumulated under cold ribs (Figure c).…”
Section: Resultsmentioning
confidence: 99%
“…A droplet of radius R is placed in the center of a 100 × 100 lu 2 square computational domain and the rest of the domain is filled with gas. The initial density is set as follows: the droplet region is set to ρ ai r = 1 × 10 −5 , ρ water = 2; the gas region is set to ρ water = 1 × 10 −5 , ρ air = 2 [ 50 , 51 ]. From the Young–Laplace law, it follows that the droplet will remain a steady circle under surface tension when the system reaches force equilibrium and that the pressure difference between the inside and outside of the droplet at a steady state satisfies the following relationship: …”
Section: Numerical Approachmentioning
confidence: 99%
“…According to Laplace’s law, the pressure difference between the inside and outside of a bubble and its radius of curvature satisfy the following relationship where Δ P is the pressure difference between the inside and outside of the bubble, R is the bubble radius, and σ denotes the surface tension coefficient. The pressure difference as a function of 1/ R is shown in Figure b.…”
Section: Numerical Approachmentioning
confidence: 99%