Home > Publications database > Why impedance of the gas diffusion layer in a PEM fuel cell differs from the Warburg finite-length impedance? > print |
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005 | 20240711101427.0 | ||
024 | 7 | _ | |a 10.1016/j.elecom.2017.09.014 |2 doi |
024 | 7 | _ | |a 1388-2481 |2 ISSN |
024 | 7 | _ | |a 1873-1902 |2 ISSN |
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100 | 1 | _ | |a Kulikovsky, Andrei |0 P:(DE-Juel1)129878 |b 0 |e Corresponding author |
245 | _ | _ | |a Why impedance of the gas diffusion layer in a PEM fuel cell differs from the Warburg finite-length impedance? |
260 | _ | _ | |a Amsterdam [u.a.] |c 2017 |b Elsevier Science |
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520 | _ | _ | |a We report a simple physics-based model leading to an analytical expression for impedance of the gas-diffusion layer (GDL) in a PEM fuel cell. We show that this expression differs from the classic Warburg finite-length impedance due to large double layer capacitance Cdl of a porous catalyst layer the GDL is attached to. It follows that the Warburg solution is obtained for the transport layer attached to a planar electrode with vanishingly small Cdl. |
536 | _ | _ | |a 135 - Fuel Cells (POF3-135) |0 G:(DE-HGF)POF3-135 |c POF3-135 |f POF III |x 0 |
588 | _ | _ | |a Dataset connected to CrossRef |
773 | _ | _ | |a 10.1016/j.elecom.2017.09.014 |g Vol. 84, p. 28 - 31 |0 PERI:(DE-600)2027290-X |p 28 - 31 |t Electrochemistry communications |v 84 |y 2017 |x 1388-2481 |
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913 | 1 | _ | |a DE-HGF |l Speicher und vernetzte Infrastrukturen |1 G:(DE-HGF)POF3-130 |0 G:(DE-HGF)POF3-135 |2 G:(DE-HGF)POF3-100 |v Fuel Cells |x 0 |4 G:(DE-HGF)POF |3 G:(DE-HGF)POF3 |b Energie |
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