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Local current density and water management in PEMFCs

机译:PEMFC中的局部电流密度和水管理

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We have used computational fluid dynamics analysis to investigate the local current density distribution at the membrane-gas diffusion layer (GDL) interface at average current densities ranging from 0.1 to 2.4 A/cm~2. A three-dimensional, non-isothermal model was used with a single straight channel geometry. Both anode and cathode humidification were included in the model. In addition, phase transportation was included in the model to predict the distributions of water vapor and liquid water and the related water management for systems operating at different current densities. The dependency of local current density on total water and thermal management of the fuel cell and its other related linkage with physical parameters were investigated. The simulation results showed that at low average current density, the local current density does not vary along the width but gradually decreases along the cell length. However, the opposite trend starts to emerge as the average current density is increased. The anode water activity was found to play a significant role in determining the membrane conductivity and the local current density variation in the cell. Moreover, at high average current density, the local current density in the downstream end of the channel is dominated by the cathode water rather than the membrane conductivity. Specifically, the cathode water accumulates in the shoulder area and congests the pores of the GDL, thereby blocking the passage of oxygen to the reacting area. The resulting scarcity of oxygen in the shoulder area causes a dramatic reduction in the local current density in this region. Simulations using different cathode stoichiometric rates showed that increasing the cathode stoichiometric rate led to better oxygen transportation to the GDL at the shoulder area, and hence improved to smooth the local current density distribution. The model was validated by comparison with the polarization curve (Ⅰ-Ⅴ characteristics) in the literature.
机译:我们已经使用计算流体动力学分析来研究膜-气体扩散层(GDL)界面处的平均电流密度分布,其平均电流密度为0.1到2.4 A / cm〜2。使用具有单一直通道几何形状的三维非等温模型。该模型同时包括阳极和阴极加湿。此外,模型中还包括相转移,以预测在不同电流密度下运行的系统中水蒸气和液态水的分布以及相关的水管理。研究了局部电流密度对燃料电池总水和热管理的依赖性以及与物理参数的其他相关联系。仿真结果表明,在低平均电流密度下,局部电流密度沿宽度不变,而沿电池长度逐渐减小。但是,随着平均电流密度的增加,相反的趋势开始出现。发现阳极水活度在确定电池中的膜电导率和局部电流密度变化中起重要作用。此外,在高平均电流密度下,通道下游端的局部电流密度由阴极水而不是膜电导率控制。具体地,阴极水积聚在肩部区域中并堵塞了GDL的孔,从而阻止了氧气通过到反应区域。肩部区域氧气的稀缺导致该区域局部电流密度的显着降低。使用不同阴极化学计量比的模拟表明,增加阴极化学计量比可导致更好的氧气向肩部区域的GDL传输,因此可以改善以平滑局部电流密度分布。通过与文献中的极化曲线(Ⅰ-Ⅴ特性)比较来验证该模型。

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