Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction

Reaction mechanisms between catalyst (Pt) and one of the fuels (H2) are found by means of DFT-B3LYP calculation, which represents a bridge bond between the theoretical calculations and the processes of fuel transformation in the fuel cells. All the closed shell energies involved in the process are obtained, starting when the platinum and the hydrogen are completely separated and ending until the hydrogen atoms separate and stay bound to the platinum, forming a new product. The equilibrium geometry of the latter system is reached with a broken H-H bond at an HPtH angle of about 90°. The latter was obtained using the DFT-B3LYP method. The confidence in all of these results is based on the fact that the potential energy well of the Pt-H2 interaction calculated using the DFT-B3LYP method is located between those calculated using Moller-Plesset and PSHONDO-IJKL-FOCK-CIPSI ab initio methods.

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Main Authors: Pacheco,J.H., Zaragoza,I.P., García,L.A., Bravo,A., Castillo,S., Novaro,O.
Format: Digital revista
Language:English
Published: Sociedad Mexicana de Física 2006
Online Access:http://www.scielo.org.mx/scielo.php?script=sci_arttext&pid=S0035-001X2006000200013
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spelling oai:scielo:S0035-001X20060002000132009-04-20Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interactionPacheco,J.H.Zaragoza,I.P.García,L.A.Bravo,A.Castillo,S.Novaro,O. Potential energy surfaces fuel cells platinum hydrgen interaction Reaction mechanisms between catalyst (Pt) and one of the fuels (H2) are found by means of DFT-B3LYP calculation, which represents a bridge bond between the theoretical calculations and the processes of fuel transformation in the fuel cells. All the closed shell energies involved in the process are obtained, starting when the platinum and the hydrogen are completely separated and ending until the hydrogen atoms separate and stay bound to the platinum, forming a new product. The equilibrium geometry of the latter system is reached with a broken H-H bond at an HPtH angle of about 90°. The latter was obtained using the DFT-B3LYP method. The confidence in all of these results is based on the fact that the potential energy well of the Pt-H2 interaction calculated using the DFT-B3LYP method is located between those calculated using Moller-Plesset and PSHONDO-IJKL-FOCK-CIPSI ab initio methods.info:eu-repo/semantics/openAccessSociedad Mexicana de FísicaRevista mexicana de física v.52 n.2 20062006-04-01info:eu-repo/semantics/articletext/htmlhttp://www.scielo.org.mx/scielo.php?script=sci_arttext&pid=S0035-001X2006000200013en
institution SCIELO
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country México
countrycode MX
component Revista
access En linea
databasecode rev-scielo-mx
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region America del Norte
libraryname SciELO
language English
format Digital
author Pacheco,J.H.
Zaragoza,I.P.
García,L.A.
Bravo,A.
Castillo,S.
Novaro,O.
spellingShingle Pacheco,J.H.
Zaragoza,I.P.
García,L.A.
Bravo,A.
Castillo,S.
Novaro,O.
Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction
author_facet Pacheco,J.H.
Zaragoza,I.P.
García,L.A.
Bravo,A.
Castillo,S.
Novaro,O.
author_sort Pacheco,J.H.
title Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction
title_short Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction
title_full Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction
title_fullStr Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction
title_full_unstemmed Bridge bond between potential energy surfaces and fuel cells on Pt-H2 interaction
title_sort bridge bond between potential energy surfaces and fuel cells on pt-h2 interaction
description Reaction mechanisms between catalyst (Pt) and one of the fuels (H2) are found by means of DFT-B3LYP calculation, which represents a bridge bond between the theoretical calculations and the processes of fuel transformation in the fuel cells. All the closed shell energies involved in the process are obtained, starting when the platinum and the hydrogen are completely separated and ending until the hydrogen atoms separate and stay bound to the platinum, forming a new product. The equilibrium geometry of the latter system is reached with a broken H-H bond at an HPtH angle of about 90°. The latter was obtained using the DFT-B3LYP method. The confidence in all of these results is based on the fact that the potential energy well of the Pt-H2 interaction calculated using the DFT-B3LYP method is located between those calculated using Moller-Plesset and PSHONDO-IJKL-FOCK-CIPSI ab initio methods.
publisher Sociedad Mexicana de Física
publishDate 2006
url http://www.scielo.org.mx/scielo.php?script=sci_arttext&pid=S0035-001X2006000200013
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