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The atomistic origin of the extraordinary oxygen reduction activity of Pt(3)Ni(7) fuel cell catalysts
Recently Debe et al. reported that Pt(3)Ni(7) leads to extraordinary Oxygen Reduction Reaction (ORR) activity. However, several reports show that hardly any Ni remains in the layers of the catalysts close to the surface (“Pt-skin effect”). This paradox that Ni is essential to the high catalytic acti...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Royal Society of Chemistry
2015
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5707479/ https://www.ncbi.nlm.nih.gov/pubmed/29218162 http://dx.doi.org/10.1039/c5sc00840a |
Sumario: | Recently Debe et al. reported that Pt(3)Ni(7) leads to extraordinary Oxygen Reduction Reaction (ORR) activity. However, several reports show that hardly any Ni remains in the layers of the catalysts close to the surface (“Pt-skin effect”). This paradox that Ni is essential to the high catalytic activity with the peak ORR activity at Pt(3)Ni(7) while little or no Ni remains close to the surface is explained here using large-scale first-principles-based simulations. We make the radical assumption that processing Pt–Ni catalysts under ORR conditions would leach out all Ni accessible to the solvent. To simulate this process we use the ReaxFF reactive force field, starting with random alloy particles ranging from 50% Ni to 90% Ni and containing up to ∼300 000 atoms, deleting the Ni atoms, and equilibrating the resulting structures. We find that the Pt(3)Ni(7) case and a final particle radius around 7.5 nm lead to internal voids in communication with the exterior, doubling the external surface footprint, in fair agreement with experiment. Then we examine the surface character of these nanoporous systems and find that a prominent feature in the surface of the de-alloyed particles is a rhombic structure involving 4 surface atoms which is crystalline-like but under-coordinated. Using density-functional theory, we calculate the energy barriers of ORR steps on Pt nanoporous catalysts, focusing on the O(ad)-hydration reaction (O(ad) + H(2)O(ad) → OH(ad) + OH(ad)) but including the barriers of O(2) dissociation (O(2ad) → O(ad) + O(ad)) and water formation (OH(ad) + H(ad) → H(2)O(ad)). We find that the reaction barrier for the O(ad)-hydration rate-determining-step is reduced significantly on the de-alloyed surface sites compared to Pt(111). Moreover we find that these active sites are prevalent on the surface of particles de-alloyed from a Pt–Ni 30 : 70 initial composition. These simulations explain the peak in surface reactivity at Pt(3)Ni(7), and provide a rational guide to use for further optimization of improved catalytic and nanoporous materials. |
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