i + is = i0 (1 – θ) exp(αnFη/RT) [1]
Here, i, is and i0 are, respectively, the measured, shorting, and ORR exchange current densities, (1 – θ) is the fraction of active sites available for ORR, and ηc is the ORR kinetic overpontential.9 As seen in Fig. 1a, the availability of active sites has a sigmoidal dependence on the cathode potential, with the largest increase in site availability occurring between 0.7 and 0.8 V. This finding will be discussed in the context of the potential window, over which the Fe3+/Fe2+ transition occurs.4,10–12 When the potential dependence of the PGM-free active site availability is incorporated into the electrochemical model, it results in an excellent fit of the experimental data, depicted in Fig. 1b. The results from this experimental/model approach not only offer guidance for means to improve the performance of (AD)Fe-N-C catalysts, but also increase our understanding of the kinetic limitations of other PGM-free ORR electrocatalysts systems.
Figure 1. a) Potential-dependent availability of ORR active sites. b) Fitting of the modeling results with experimental data from polarization curves taken at different O2 partial pressures for PEMFC fabricated with the LANL PGM-free catalysts at the cathode (80oC, 100% RH, 300/300 sccm H2/O2, 3.5 mgcat/cm2elec).
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