In this study, we characterize the τ/ε-ratio for two GDL substrates (without the addition of an MPL), one from Toray and one from Freudenberg, using limiting current measurements in an operating fuel cell. The τ/ε-ratio describes the deviation of the effective diffusivity compared to ideal molecular diffusion. However, depending of the range of pore diameters in the gas diffusion medium, a mixture of molecular diffusion and Knudsen diffusion has to be taken into account. Fig. 1 shows the theoretical contribution ratio of Knudsen diffusion and molecular diffusion (left y‑axis) versus the relevant range of pore diameters for different pressures. The graphic illustrates that Knudsen diffusion dominates at lower pore sizes, while molecular diffusion is mostly present at larger pore sizes. An increase in pressure shifts the regime of molecular diffusion to smaller pores. In addition to the theoretical contribution ratio, Fig. 1 depicts the pore size distribution of a Toray and a Freudenberg GDL substrate determined by mercury intrusion porosimetry (MIP). While the Toray paper has a narrow pore size distribution at pores of 30-50 µm, where only molecular diffusion occurs, the Freudenberg GDL contains a broader range of larger pores at 10-40 µm (molecular diffusion) together with the presence of small pores at ca. 70-80 nm that derive from the addition of carbon black and that present a medium where Knudsen and molecular diffusion occur.
After the validation of the principle, the method is transferred to determine the τ/ε-number of a microporous layer based on vapor-grown carbon-fibers (VGCF), whose transport properties in a PEMFC have been described previously.[5]
References
[1] O. Gröger, H. A. Gasteiger, J.-P. Suchsland, J. Electrochem. Soc. 2015, 162, A2605-A2622.
[2] D. R. Baker, D. A. Caulk, K. C. Neyerlin, M. W. Murphy, J. Electrochem. Soc. 2009, 156, B991.
[3] D. Kramer, S. A. Freunberger, R. Flückiger, I. A. Schneider, A. Wokaun, F. N. Büchi, G. G. Scherer, Journal of Electroanalytical Chemistry 2008, 612, 63-77.
[4] K.-D. Wagner, A. Bock, K. Salama, A. Weller, Vol. US 2010/0219069 A1, Carl Freudenberg KG 2010.
[5] C. Simon, J. Endres, B. Nefzger-Loders, F. Wilhelm, H. A. Gasteiger, J. Electrochem. Soc. 2019, 166, F1022-F1035.
Acknowledgements
We gratefully acknowledge funding from the Swiss National Foundation under the funding scheme Sinergia (project grant number 180335). We also thank Michael Striednig and Christoph Simon for initial work on the topic.
Figure 1: Left y-axis: theoretical contribution ratio of Knudsen (green) and molecular diffusion (orange) versus pore diameter for different absolute pressures of 115 kPaabs (solid lines), 150 kPaabs (dashed lines), 200 kPaabs (dotted lines), and 300 kPaabs (dash-dotted lines). With smaller pores and lower pressures, more contributions from Knudsen diffusion can be expected. Right y-axis: log. differential intrusion measured by MIP analysis for the Toray (blue) and the Freudenberg (grey) GDL substrates, whereby the Freudenberg GDL shows pores at ~70-80 nm that are caused by the addition of carbon black.