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dc.contributor.authorEichner, Benedikt J.
dc.contributor.authorAmiri, Mahshid N.
dc.contributor.authorBurheim, Odne Stokke
dc.contributor.authorLamb, Jacob Joseph
dc.date.accessioned2024-09-05T09:02:42Z
dc.date.available2024-09-05T09:02:42Z
dc.date.created2024-08-27T09:58:47Z
dc.date.issued2024
dc.identifier.citationFrontiers in Chemical Engineering. 2024, 6, 1-13.en_US
dc.identifier.issn2673-2718
dc.identifier.urihttps://hdl.handle.net/11250/3150293
dc.description.abstractPolymer electrolyte membrane electrolyser cells (PEMEC) are recognized as highly suitable for large-scale green hydrogen production from variable renewable sources. To enhance production rates in PEMECs, current densities have gradually increased, resulting in elevated heat generation within the electrolysis cells. Consequently, the consideration of thermal gradients within individual cells within the stacks becomes increasingly crucial. This study presents a 2D thermal numerical steady-state model of an industrial-sized PEMEC stack, predicting thermal gradients within the cells in both stacking direction and along the channels of the flow fields. Through-plane thermal conductivities were measured ex-situ for the titanium felt porous transport layer (PTL), Tion5-W PFSA membrane, and PEMEC catalyst layers (CLs). At a compaction pressure of 16 bar, the wet PTL exhibited a thermal conductivity of 2.7 ± 0.2 W m−1 K−1, the wet membrane of 0.31 ± 0.01 W m−1 K−1, and the wet CLs of 0.19 ± 0.03 W m−1 K−1. When modelled, thermal gradients of 16.5 ± 0.6 K in parallel flow and 17.6 ± 0.5 K in counter-flow were predicted within cells with a 1 m2 cell area, operating at 2 A cm−2. The counter-flow arrangement demonstrated a 0.2% advantage in voltage efficiency. An increase in current density to 3 A cm−2 resulted in a 10 K rise in thermal differences in both parallel and counter-flow conditions. However, the use of a sintered PTL reduced thermal gradients by approximately 3.7 K at 2 A cm−2. The simulation indicated a 20%–40% increase in maximal thermal gradients within the stack compared to models using lumped properties within the cells, emphasizing the significance of considering in-cell thermal gradients at the stack level.en_US
dc.language.isoengen_US
dc.publisherFrontiers Mediaen_US
dc.rightsNavngivelse 4.0 Internasjonal*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/deed.no*
dc.title2D simulation of temperature distribution within large-scale PEM electrolysis stack based on thermal conductivity measurementsen_US
dc.title.alternative2D simulation of temperature distribution within large-scale PEM electrolysis stack based on thermal conductivity measurementsen_US
dc.typeJournal articleen_US
dc.typePeer revieweden_US
dc.description.versionpublishedVersionen_US
dc.source.pagenumber1-13en_US
dc.source.volume6en_US
dc.source.journalFrontiers in Chemical Engineeringen_US
dc.identifier.doi10.3389/fceng.2024.1384772
dc.identifier.cristin2289632
cristin.ispublishedfalse
cristin.fulltextoriginal
cristin.qualitycode1


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Navngivelse 4.0 Internasjonal
Except where otherwise noted, this item's license is described as Navngivelse 4.0 Internasjonal