Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/97548
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dc.contributorDepartment of Building and Real Estateen_US
dc.creatorXia, Len_US
dc.creatorNi, Men_US
dc.creatorHe, Qen_US
dc.creatorXu, Qen_US
dc.creatorCheng, Cen_US
dc.date.accessioned2023-03-06T01:20:01Z-
dc.date.available2023-03-06T01:20:01Z-
dc.identifier.issn0306-2619en_US
dc.identifier.urihttp://hdl.handle.net/10397/97548-
dc.language.isoenen_US
dc.publisherPergamon Pressen_US
dc.rights© 2021 Elsevier Ltd. All rights reserved.en_US
dc.rights© 2021. This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/.en_US
dc.rightsThe following publication Xia, L., et al. (2021). "Optimization of gas diffusion layer in high temperature PEMFC with the focuses on thickness and porosity." Applied Energy 300: 117357 is available at https://dx.doi.org/10.1016/j.apenergy.2021.117357.en_US
dc.subjectFlow uniformityen_US
dc.subjectGas diffusion layeren_US
dc.subjectGeometric optimizationen_US
dc.subjectHT-PEMFCen_US
dc.subjectPorosityen_US
dc.titleOptimization of gas diffusion layer in high temperature PEMFC with the focuses on thickness and porosityen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume300en_US
dc.identifier.doi10.1016/j.apenergy.2021.117357en_US
dcterms.abstractWide ranges of thickness (e.g. 100–400 μm) and porosity (e.g. 30–70%) of gas diffusion layer (GDL) in a high temperature proton exchange membrane fuel cell (HT-PEMFC) are available in the literature. However, the effects of GDL porosity and thickness on electron conduction and gas distribution uniformity (under the rib and under the channel) are unclear. In this study, a numerical non-isothermal 3D model was developed. After model validation, parametric analyses were performed to investigate the effects of thickness and porosity on flow uniformity (under the rib and under the channel), diffusion flux and ohmic resistance. It is found that both the flow uniformity and ohmic resistance increase with increasing thickness and porosity. However, the thickness and porosity have opposite influence on diffusion flux, which decreases with increasing GDL thickness but increases with increasing porosity. Unlike the previous research suggesting thin GDL with high porosity, optimal GDL thickness and porosity are found in the present study. The appropriate GDL thicknesses for anode and cathode are 80–120 μm and 140–170 μm respectively while the optimal value for GDL porosity is 35–45%. This study clearly demonstrates that we can further achieve a performance increment of 7.7% by carefully controlling the thickness and porosity of GDL.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationApplied energy, 15 Oct. 2021, v. 300, 117357en_US
dcterms.isPartOfApplied energyen_US
dcterms.issued2021-10-15-
dc.identifier.scopus2-s2.0-85110216191-
dc.identifier.eissn1872-9118en_US
dc.identifier.artn117357en_US
dc.description.validate202303 bcwwen_US
dc.description.oaAccepted Manuscripten_US
dc.identifier.FolderNumberBRE-0033-
dc.description.fundingSourceRGCen_US
dc.description.pubStatusPublisheden_US
dc.identifier.OPUS53885485-
dc.description.oaCategoryGreen (AAM)en_US
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