The single cell performances of polymer electrolyte fuel cells (PEFCs) using Pt catalyst supported on Nb-SnO 2 (Pt/Nb-SnO 2 ) with/without graphitized carbon black (GCB) were compared with that of a cell using Pt/GCB. The Pt-mass specific power of the Pt/Nb-SnO 2 cathode under low humidity conditions was superior to that of the Pt/GCB cathode, because the hydrophilic SnO 2 support helped to increase the proton conductivity of the ionomer, which led to high Pt effectiveness. The addition of GCB to the Pt/Nb-SnO 2 cathode improved the cell performance under high humidity, and the Pt-mass specific power value reached more than 10 kW g Pt −1. The improvement conditions was attributed to the formation of gas diffusion paths by adding the hydrophobic GCB. The Pt/Nb-SnO 2 cathodes, with/without GCB, had greater durability than that of the Pt/GCB cathode during the startup / shutdown potential sweep evaluation. The migration of Pt particles on the Nb-SnO 2 support was suppressed by the high stability of Nb-SnO 2 and strong orientation between Pt and Nb-SnO 2 support. The degradation of GCB in the Pt/Nb-SnO 2 cathode was smaller than that in the Pt/GCB cathode because of the absence of Pt on the added GCB. Therefore, the added GCB was still able to provide gas diffusion paths even after extensive cycling.
We measured highly accurate ohmic resistances of single cells at high frequency (HF) using Pt/Nb-SnO2 cathodes under several different conditions, including various cathode potentials and various atmospheres, in order to study the relationships between the ohmic resistances of single cells and the electrical conductivity of the Pt/Nb-SnO2 catalyst for polymer electrolyte fuel cells (PEFCs). The ohmic resistance of a cell using Pt/Nb-SnO2 increased with increasing cathode potential, in the range of typical cathode operation (0.4 V to 1.0 V vs. the reversible hydrogen electrode). The increase of Pt loading on the Nb-SnO2 support from 9 wt% to 17 wt% was effective in decreasing the ohmic resistance and in improving the cell performance. We propose that Pt oxidation might impede the effect of shrinking the depletion layer of the Nb-SnO2 surface. The addition of graphitized carbon black (GCB) to the Pt/Nb-SnO2 cathode was able to improve the cell performance by constructing both electronic pathways and gas diffusion pathways in the catalyst layer, under low and high current density operation, respectively. The performance of the Pt/Nb-SnO2 + GCB cathode was superior to that of the Pt/GCB cathode due to these effects.
Platinum catalysts supported on carbon black (Pt/CB) have been widely applied as the cathode catalysts for PEFCs. It is well known that the CB degrades under high potential operating conditions. In order to improve the durability of the support, SnO2 have been proposed as an alternative to carbon.1 The enhancement of the electrical conductivity of SnO2 by doping of aliovalent cations (e.g., Sb5+) was shown to be accompanied by an improvement of the ORR activity.2 We also reported that the electrical conductivity of Nb-doped SnO2 nanoparticles improved by the fused aggregation of particles with nearest-neighbors and by construction of a CB-like randomly branched structure (fused aggregate structure).3 Moreover, the single cell performance using a Pt cathode catalyst supported on the Nb-SnO2 (Pt/Nb-SnO2) was reported to be higher than that using commercial Pt/CB.4-6 In this research, we evaluated the cell resistance using a Pt/Nb-SnO2 cathode catalyst layer as a function of cell potential, current density and AC frequency, and investigated the reason for the unique electrically conducting behavior of the catalyst layers. The Nb-SnO2 supports with fused aggregate structure were synthesized by the flame combustion method and were loaded with nanometer-sized Pt catalysts by the colloidal method (Pt loading; 16.5 wt% and 9.6 wt%). The catalyst inks for cathodes were prepared with the Pt/Nb-SnO2, Nafion® binder, ethanol and pure water, and were sprayed onto the Nafion membrane by the pulse-swirl-spray technique. The Pt loading amounts on the cathode catalyst layers were 0.16 mg cm-2 (16.5 wt%) and 0.08 mg cm-2 (9.6 wt%), which meant that the Nb-SnO2 loading amounts were almost the same (1.0 ± 0.1 mg-support cm-2). The Japan Automobile Research Institute (JARI) standard cell (active geometric area 29.2 cm2) was used for the electrochemical measurements. The impedance spectra were potentiostatically measured under steady-state operation, with hydrogen and oxygen/air at 80◦C under ambient pressure. The utilizations of the reactant gases were 70% for H2, 40% for O2 and 40% for air. Each cell resistance was estimated from the intercept of the x-axis of the Nyquist plots. Figure 1 showed the cell potentials and ohmic resistances obtained by impedance spectra at 80 oC, 100% RH. In general, the cell ohmic resistance derives mainly from the proton conductivity of the membrane and is maintained stable value at 100% RH, as indicated in the cell resistance using heat-treated Pt catalyst supported on graphitized CB (Pt/GCB-HT). In contrast, the cell ohmic resistances using both Pt/Nb-SnO2 cathodes decreased with increasing current density. The resistance of the cell using 16.5 wt% Pt/Nb-SnO2 at 150 mA/cm2 was approximately the same as that using the Pt/GCB-HT cathode. The resistance using the 16.5 wt% Pt/Nb-SnO2 cathode was less than half of that using the 9.6 wt% Pt/Nb-SnO2 cathode. Figure 2 showed the Nyquist plots for these cells at 0.65 V. The intercept of x-axis of each Nyquist plot appeared at different frequency. In addition, we found that the ohmic resistances of the cell using Pt/Nb-SnO2 cathodes were strongly dependent on the cell potential, as shown in Fig. 3. In our previous research, we reported that the electrical conductivities of Nb-SnO2 supports were dependent on the atmospheric condition, and increased with increasing amounts of loaded metallic Pt. The conductivity of the catalyst reached the values more than three orders of magnitude larger than that of the bare support.3 Such phenomena should strongly be related to the thickness of the depletion layer of the Nb-SnO2 supports.3 which should not pertain to the GCB support, in principle. The cell potential dependence of the resistance using the Pt/Nb-SnO2 cathode indicated that the electrically conductive paths in the Pt/Nb-SnO2 catalyst layers should be improved with decreasing cell potential due to reduction of Pt oxide to metallic Pt. Acknowledgement This research was supported by funds for the “Research on Nanotechnology for High Performance Fuel Cells” (HiPer-FC) project from the New Energy and Industrial Technology Development Organization (NEDO) of Japan. References A. Masao et al., Electrochem. Solid-State Lett., 12, B119 (2009). F. Takasaki et al., J. Electrochem. Soc., 158, B1270 (2011) Y. Senoo et al., RSC Adv., 4, 32180 (2014). K. Kakinuma, et al., Electrochim. Acta, 110, 316 (2013). Y. Senoo et al., Electrochem. Commun., 51, 37 (2015). Y.Chino et al., J. Electrochem. Soc., 162, F736 (2015). Figure 1
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