Current, concentration and overpotential distributions on columnar structured electrodes in a 2 D PEMFC model
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.
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 |
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Inglés | |
Agencia Nacional de Investigación e Innovación | |
REDI | |
https://hdl.handle.net/20.500.12381/636
http://dx.doi.org/10.1002/celc.202200146 |
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Acceso abierto | |
Dedicación de Dominio Público 1.0 Universal. (CC0) |
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---|---|
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 |