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Characterization of reactant gases, water and heat distributions in proton-exchange-membrane fuel cells.

机译:质子交换膜燃料电池中反应气体,水和热分布的特征。

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Proper reactant gas distribution and water and heat management are essential for obtaining high-power-density performance at high energy efficiency for proton-exchange-membrane (PEM) fuel cells. An along-the-channel model has been developed to evaluate the effects of various design and operating parameters on the performance of PEM fuel cells. The model accounts for water transport across membrane by electro-osmosis, diffusion, and convection, temperature distribution in the solid phase along the flow channel, and heat removal by natural convection and coflow and counterflow heat exchanger. Results from the model show that the performance of a PEM fuel cell could be improved by anode humidification and positive differential pressure between the cathode and anode to increase the back transport rate of water across the membrane. Results also show that effective heat removal is necessary for preventing excessive temperatures, which could lead to local membrane dehydration. For optimal heat removal and distribution, the counterflow heat exchanger is most effective.; A gas-diffusion model was developed to study the effect of the design parameters of the gas distributor plates. Laplace's equation with boundary conditions that account for the shoulder area design was used to describe the gas transport through the cathode electrode layer. From the results, it was found that the current generated in the cathode side can be limited as much as 45% when compared with a gas distributor design which has no shoulder area.; To improve the mass transport rates of the reactants from the flow channels to the catalysts of the porous electrode, an interdigitated gas distributor design has been developed. This design reduces the electrode-flooding problem in the cathode. To understand how these effects contribute to the cell performance, experiments were performed. Simultaneously, two mathematical models for the cathode electrode were also developed. The first model, a multi-component, single-phase cathode model, describes the two-dimensional flow patterns and the distributions of the gaseous species in the porous electrode and predicts the current density generated at the reaction interface as a function of various operating conditions and design parameters. Results from the model show that the flow-through conditions created by the interdigitated gas distributor greatly reduces the diffusion layer in the electrode. This model has been expanded to a two-phase cathode model which includes the presence of liquid water in the electrode. The flow of the liquid water in the electrode is described as convection due to the gas flow and capillary diffusion due to the difference of capillary pressures of liquid water. The modeling results showed that a higher differential pressure between the inlet and outlet channels is favored. Moreover, more channels and thinner shoulder width are preferred in designing the interdigitated gas distributor. Results also show that the electrode thickness needs to be optimized to get optimal performance because a thinner electrode results in reduced reactant flow rates, and a thicker electrode results in an increased diffusion layer thickness.
机译:适当的反应气体分布以及水和热量管理对于质子交换膜(PEM)燃料电池以高能效获得高功率密度性能至关重要。已开发出一种沿通道模型来评估各种设计和运行参数对PEM燃料电池性能的影响。该模型考虑了电渗透,扩散和对流,沿流道的固相温度分布以及自然对流,同流和逆流换热器进行除热的过程,从而跨膜传输水。该模型的结果表明,通过阳极加湿和阴极与阳极之间的正压差可以提高PEM燃料电池的性能,以提高水跨膜的反传输速率。结果还表明,有效的除热对于防止温度过高是必要的,因为温度过高可能会导致局部膜脱水。为了达到最佳的散热和分配效果,逆流热交换器是最有效的。建立了气体扩散模型以研究气体分配板设计参数的影响。带有肩部区域设计的边界条件的拉普拉斯方程用于描述气体通过阴极电极层的传输。从结果可以发现,与没有肩部区域的气体分配器设计相比,在阴极侧产生的电流可以被限制在45%之内。为了提高反应物从流动通道到多孔电极的催化剂的质量传输速率,已经开发了一种叉指式气体分配器设计。这种设计减少了阴极中的电极溢流问题。为了了解这些效应如何促进细胞性能,进行了实验。同时,还开发了两个用于阴极的数学模型。第一个模型是多组分单相阴极模型,描述了二维流动模式和多​​孔电极中气态物质的分布,并预测了在各种操作条件下在反应界面产生的电流密度和设计参数。该模型的结果表明,由叉指状气体分配器产生的流通条件大大减少了电极中的扩散层。该模型已扩展为两相阴极模型,其中包括电极中存在液态水。电极中的液态水的流动被描述为由于气体流动而产生的对流,以及由于液态水的毛细管压力的差异而引起的毛细管扩散。建模结果表明,入口和出口通道之间的压差较高。此外,在设计叉指式气体分配器时,优选更多的通道和更薄的肩宽。结果还表明,需要优化电极厚度以获得最佳性能,因为较薄的电极会导致反应物流速降低,而较厚的电极会导致扩散层厚度增加。

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