Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model

Zinola, Carlos F.

Resumen:

The complete optimization of fuel cell´s performance involves the prediction of its operation conditions and electrochemical characteristics for short and long-time periods. One of the topics not studied in detail is the change in the surface morphology of metallic catalytic layers as a time-dependent function of the fuel cell working conditions. For single platinum catalysts a columnar growth is demonstrated after 1 month of hydrogen/oxygen continuous operation at the plateau, where electrochemical distributions of smooth surfaces are not operative. Since they act as a completely dynamic system, numerical solutions are not useful as they permanently need parametric profile optimizations. The employ of exact analytical functions instead, reduces large computational times and assures this information only knowing the final structure morphology. In this sense we encouraged current, concentration and potential shapes for these columnar electrodes adapting mass balance differential equations with a parametric profile to model these columns (trochoid curvilinear contours). The analytical solutions were compared with those of a smooth surface (early uses of the fuel cell) and with experimental values obtained using a home-made hydrogen/oxygen polymeric membrane cell.


Detalles Bibliográficos
2022
Agencia Nacional de Investigación e Innovación
Columnar platinum
Current distribution
Cycloid surfaces
Fuel cells
Ciencias Naturales y Exactas
Ciencias Químicas
Físico-Química, Ciencia de los Polímeros, Electroquímica
Inglés
Agencia Nacional de Investigación e Innovación
REDI
https://hdl.handle.net/20.500.12381/636
http://dx.doi.org/10.1002/celc.202200146
Acceso abierto
Dedicación de Dominio Público 1.0 Universal. (CC0)
_version_ 1814959262336548864
author Zinola, Carlos F.
author_facet Zinola, Carlos F.
author_role author
bitstream.checksum.fl_str_mv 3c9d86d36485746409b4281a0893d729
bf17c95ae7d09a0f3282f9902f2d7f69
bitstream.checksumAlgorithm.fl_str_mv MD5
MD5
bitstream.url.fl_str_mv https://redi.anii.org.uy/jspui/bitstream/20.500.12381/636/2/license.txt
https://redi.anii.org.uy/jspui/bitstream/20.500.12381/636/1/manuscript%20chemelectrochem.pdf
collection REDI
dc.creator.none.fl_str_mv Zinola, Carlos F.
dc.date.accessioned.none.fl_str_mv 2022-09-23T17:26:19Z
dc.date.available.none.fl_str_mv 2022-09-23T17:26:19Z
dc.date.issued.none.fl_str_mv 2022-07-21
dc.description.abstract.none.fl_txt_mv The complete optimization of fuel cell´s performance involves the prediction of its operation conditions and electrochemical characteristics for short and long-time periods. One of the topics not studied in detail is the change in the surface morphology of metallic catalytic layers as a time-dependent function of the fuel cell working conditions. For single platinum catalysts a columnar growth is demonstrated after 1 month of hydrogen/oxygen continuous operation at the plateau, where electrochemical distributions of smooth surfaces are not operative. Since they act as a completely dynamic system, numerical solutions are not useful as they permanently need parametric profile optimizations. The employ of exact analytical functions instead, reduces large computational times and assures this information only knowing the final structure morphology. In this sense we encouraged current, concentration and potential shapes for these columnar electrodes adapting mass balance differential equations with a parametric profile to model these columns (trochoid curvilinear contours). The analytical solutions were compared with those of a smooth surface (early uses of the fuel cell) and with experimental values obtained using a home-made hydrogen/oxygen polymeric membrane cell.
dc.description.sponsorship.none.fl_txt_mv Agencia Nacional de Investigación e Innovación
dc.identifier.anii.es.fl_str_mv FSE_1_2019_1_159390
dc.identifier.doi.none.fl_str_mv http://dx.doi.org/10.1002/celc.202200146
dc.identifier.uri.none.fl_str_mv https://hdl.handle.net/20.500.12381/636
dc.language.iso.none.fl_str_mv eng
dc.publisher.es.fl_str_mv Wiley Interscience
dc.rights.es.fl_str_mv Acceso abierto
dc.rights.license.none.fl_str_mv Dedicación de Dominio Público 1.0 Universal. (CC0)
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
dc.source.es.fl_str_mv ChemElectroChem
dc.source.none.fl_str_mv reponame:REDI
instname:Agencia Nacional de Investigación e Innovación
instacron:Agencia Nacional de Investigación e Innovación
dc.subject.anii.none.fl_str_mv Ciencias Naturales y Exactas
Ciencias Químicas
Físico-Química, Ciencia de los Polímeros, Electroquímica
dc.subject.es.fl_str_mv Columnar platinum
Current distribution
Cycloid surfaces
Fuel cells
dc.title.none.fl_str_mv Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
dc.type.es.fl_str_mv Artículo
dc.type.none.fl_str_mv info:eu-repo/semantics/article
dc.type.version.es.fl_str_mv Enviado
dc.type.version.none.fl_str_mv info:eu-repo/semantics/submittedVersion
description The complete optimization of fuel cell´s performance involves the prediction of its operation conditions and electrochemical characteristics for short and long-time periods. One of the topics not studied in detail is the change in the surface morphology of metallic catalytic layers as a time-dependent function of the fuel cell working conditions. For single platinum catalysts a columnar growth is demonstrated after 1 month of hydrogen/oxygen continuous operation at the plateau, where electrochemical distributions of smooth surfaces are not operative. Since they act as a completely dynamic system, numerical solutions are not useful as they permanently need parametric profile optimizations. The employ of exact analytical functions instead, reduces large computational times and assures this information only knowing the final structure morphology. In this sense we encouraged current, concentration and potential shapes for these columnar electrodes adapting mass balance differential equations with a parametric profile to model these columns (trochoid curvilinear contours). The analytical solutions were compared with those of a smooth surface (early uses of the fuel cell) and with experimental values obtained using a home-made hydrogen/oxygen polymeric membrane cell.
eu_rights_str_mv openAccess
format article
id REDI_85aa707abaf8d7aca9ec9a3bc16fd7ae
identifier_str_mv FSE_1_2019_1_159390
instacron_str Agencia Nacional de Investigación e Innovación
institution Agencia Nacional de Investigación e Innovación
instname_str Agencia Nacional de Investigación e Innovación
language eng
network_acronym_str REDI
network_name_str REDI
oai_identifier_str oai:redi.anii.org.uy:20.500.12381/636
publishDate 2022
reponame_str REDI
repository.mail.fl_str_mv jmaldini@anii.org.uy
repository.name.fl_str_mv REDI - Agencia Nacional de Investigación e Innovación
repository_id_str 9421
rights_invalid_str_mv Dedicación de Dominio Público 1.0 Universal. (CC0)
Acceso abierto
spelling Dedicación de Dominio Público 1.0 Universal. (CC0)Acceso abiertoinfo:eu-repo/semantics/openAccess2022-09-23T17:26:19Z2022-09-23T17:26:19Z2022-07-21https://hdl.handle.net/20.500.12381/636FSE_1_2019_1_159390http://dx.doi.org/10.1002/celc.202200146The complete optimization of fuel cell´s performance involves the prediction of its operation conditions and electrochemical characteristics for short and long-time periods. One of the topics not studied in detail is the change in the surface morphology of metallic catalytic layers as a time-dependent function of the fuel cell working conditions. For single platinum catalysts a columnar growth is demonstrated after 1 month of hydrogen/oxygen continuous operation at the plateau, where electrochemical distributions of smooth surfaces are not operative. Since they act as a completely dynamic system, numerical solutions are not useful as they permanently need parametric profile optimizations. The employ of exact analytical functions instead, reduces large computational times and assures this information only knowing the final structure morphology. In this sense we encouraged current, concentration and potential shapes for these columnar electrodes adapting mass balance differential equations with a parametric profile to model these columns (trochoid curvilinear contours). The analytical solutions were compared with those of a smooth surface (early uses of the fuel cell) and with experimental values obtained using a home-made hydrogen/oxygen polymeric membrane cell.Agencia Nacional de Investigación e InnovaciónengWiley InterscienceChemElectroChemreponame:REDIinstname:Agencia Nacional de Investigación e Innovacióninstacron:Agencia Nacional de Investigación e InnovaciónColumnar platinumCurrent distributionCycloid surfacesFuel cellsCiencias Naturales y ExactasCiencias QuímicasFísico-Química, Ciencia de los Polímeros, ElectroquímicaCurrent, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC modelArtículoEnviadoinfo:eu-repo/semantics/submittedVersioninfo:eu-repo/semantics/articleUniversidad de la República. Facultad de Ciencias//Ciencias Naturales y Exactas/Ciencias Químicas/Físico-Química, Ciencia de los Polímeros, ElectroquímicaZinola, Carlos F.LICENSElicense.txtlicense.txttext/plain; charset=utf-84944https://redi.anii.org.uy/jspui/bitstream/20.500.12381/636/2/license.txt3c9d86d36485746409b4281a0893d729MD52ORIGINALmanuscript chemelectrochem.pdfmanuscript chemelectrochem.pdfapplication/pdf2397994https://redi.anii.org.uy/jspui/bitstream/20.500.12381/636/1/manuscript%20chemelectrochem.pdfbf17c95ae7d09a0f3282f9902f2d7f69MD5120.500.12381/6362022-09-23 14:26:21.266oai:redi.anii.org.uy:20.500.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://www.anii.org.uy/https://redi.anii.org.uy/oai/requestjmaldini@anii.org.uyUruguayopendoar:94212022-09-23T17:26:21REDI - Agencia Nacional de Investigación e Innovaciónfalse
spellingShingle Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
Zinola, Carlos F.
Columnar platinum
Current distribution
Cycloid surfaces
Fuel cells
Ciencias Naturales y Exactas
Ciencias Químicas
Físico-Química, Ciencia de los Polímeros, Electroquímica
status_str submittedVersion
title Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
title_full Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
title_fullStr Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
title_full_unstemmed Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
title_short Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
title_sort Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
topic Columnar platinum
Current distribution
Cycloid surfaces
Fuel cells
Ciencias Naturales y Exactas
Ciencias Químicas
Físico-Química, Ciencia de los Polímeros, Electroquímica
url https://hdl.handle.net/20.500.12381/636
http://dx.doi.org/10.1002/celc.202200146