In:
ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2018-01, No. 30 ( 2018-04-13), p. 1721-1721
Kurzfassung:
The independence from Platinum-Group-Metal (PGM) is one of the major goals towards the commercialization of Proton Exchange Membrane Fuel Cells (PEMFCs), due to the limited availability of PGM and their considerable loading on the Oxygen-Reduction-Reaction (ORR), increasing their cost contribution to the overall system. On the other hand, the challenges for PGM-free ORR catalysts are an activity approaching that of Pt and a long-term operational stability in the strong acidic environment of a PEMFC. Low-cost FeNC catalysts fulfill the high activity requirement, but they still face fast degradation in acidic environment [1, 2]. On the contrary, pure valve-metal oxides as non-PGM ORR catalysts need a significant improvement in ORR activity and H 2 O yield but they are very promising in terms of stability during PEMFC operation [3, 4]. The aim of this contribution is to combine the intrinsic high ORR activity of Fe with the stability of valve-metal oxides, via partial substitution of Zr 4+ with Fe 3+ in the ZrO 2 structure [5]. The formation of a solid solution of oxides of the two aliovalent-metals should also provide oxygen vacancies or uncoordinated metal sites at the oxide surface, hypothesized to be correlated to an increased ORR activity of valve-metal oxides [6, 7] . In this study, to obtain Fe-substituted ZrO 2 we used a homogeneous mixture of the two metals at the molecular level, by employing two soluble organometallic precursors, i. e., zirconium (IV) tetra-tert-butyl dichloro phthalocyanine (ZrCl 2 Pc(tBu) 4 ) and iron(II) tetra-tert-butyl phthalocyanine (FePc(tBu) 4 ). Graphitized Ketjen-Black carbon is first impregnated with the precursors and then heat-treated as described in [8, 9]. XRD and TEM characterization show that our catalysts consist of ZrO 2 particles of about 3 nm (Fe-substituted) and 7 nm (pure ZrO 2 ). Mössbauer spectroscopy reveals that the Fe moieties are isolated and in Fe 3+ electronic configuration at high spin, typical of an oxidic environment. This is confirmed by soft XAS data at the Fe L-edge and XPS data, pointing to the desired Fe x Zr 1-x O 2-δ phase. We already published an evaluation of the ORR mass activity of Fe x Zr 1-x O 2-δ in comparison to Fe-only and ZrO 2 -only catalysts, using a thin-film rotating (ring) disk electrode (RRDE) setup [9]. Using the preferred catalyst Fe 0.07 Zr 0.93 O 2-δ , the variation of its mass activity and selectivity as a function of the loading is further discussed, with a H 2 O 2 yield even lower in comparison to an FeNC catalyst [10]. The catalyst mass activity and its Arrhenius analysis in a single PEMFC at ≈0.4 mg cat /cm² is compared to the RDE results (Figure 1) [11]. The Arrhenius analysis resulted in an ORR activation energy of 16 kJ/mol (RDE) and 18 kJ/mol (PEMFC) at 0.4 V RHE , significantly lower than our best pure-ZrO 2 catalyst reported (21 kJ/mol from RDE and 29 kJ/mol from PEMFC data) [4]. Stability tests and loading optimization of nanometric Fe x Zr 1-x O 2-δ will be the future outlook. Acknowledgements: This work was supported by the Bayerische Forschungsstiftung (Project ForOxiE², AZ 1143-14). References: [1] M. Lefèvre, J. P. Dodelet, ECS Transactions 2012 , 45(2) , 35-44. [2] B. Piela, T. S. Olson, P. Atanassov, P. Zelenay, Electrochimica Acta 2010 , 55 , 7615-7621. [3] A. Ishihara, S. Yin, K. Suito, N. Uehara, Y. Okada, Y. Kohno, K. Matsuzawa, S. Mitsushima, M. Chisaka, Y. Ohgi, M. Matsumoto, H. Imai, K. Ota, ECS Transactions 2013 , 58 , 1495-1500. [4] T. Mittermeier, P. Madkikar, X. Wang, H. A. Gasteiger and M. Piana, J. Electrochem. Soc. 2016 , 163 , F1543-F1552. [5] D. Sangalli, A. Lamperti, E. Cianci, R. Ciprian, M. Perego, A. Debernardi, Phys. Rev. B 2013 , 87 , 085206. [6] A. Ishihara, M. Tamura, Y. Ohgi, M. Matsumoto, K. Matsuzawa, S. Mitsushima, H. Imai, K.-i. Ota, J. Phys. Chem. C , 2013 , 117 , 18837–18844. [7] Y. Ohgi, A. Ishihara, K. Matsuzawa, S. Mitsushima, K.-i. Ota, M. Matsumoto, H. Imai, J. Electrochem. Soc. 2013 , 160 , F162-F167. [8] P. Madkikar, X. Wang, T. Mittermeier, A. H. A. Monteverde Videla, C. Denk, S. Specchia, H. A. Gasteiger, M. Piana, J. Nanostruct. Chem. 2017 , 7 , 133-147. [9] P. Madkikar, T. Mittermeier, H. A. Gasteiger, M. Piana, J. Electrochem. Soc. 2017 , 164(7) , F831-F833. [10] A. Bonakdarpour, M. Lefevre, R. Yang, F. Jaouen, T. Dahn, J.-P. Dodelet, J. R. Dahn, Electrochem. Solid-State Lett. 2008 , 11(6) , B105-B108. [11] P. Madkikar, D. Menga, G. Harzer, T. Mittermeier, F. E. Wagner, M. Merz, S. Schuppler, P. Nagel, A. Siebel, H. A. Gasteiger, M. Piana, manuscript in preparation . Figure 1
Materialart:
Online-Ressource
ISSN:
2151-2043
DOI:
10.1149/MA2018-01/30/1721
Sprache:
Unbekannt
Verlag:
The Electrochemical Society
Publikationsdatum:
2018
ZDB Id:
2438749-6
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