Effective interfacial area in agitated liquid–liquid continuous reactors

Detalhes bibliográficos
Autor(a) principal: Quadros, Paulo A.
Data de Publicação: 2003
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)
Texto Completo: http://hdl.handle.net/10316/7411
https://doi.org/10.1016/S0009-2509(03)00302-6
Resumo: A chemical method has been used to quantify the e ective interfacial area in a ba4ed continuous stirred liquid–liquid reactor. Two and four straight paddle impellers were used in the experimental runs, at 34◦C, with hold-up fractions of dispersed organic phase between 0.061 and 0.166 and stirring speed ranging from 360 to 1500 rpm. In:uence of the residence time on the formation of the interfacial area generated in this system was not registered; however, di erences were reported between continuous and batch mode operations. The interfacial area was correlated to hold-up fraction and Weber number by a new empirical model proposed in this work. This model allows to use only one equation to calculate the interfacial area in this continuous stirred reactor in the wide range of operating conditions tested (490¡We¡9600), which include di erent :ow regimes. This is a relevant contribution as previous studies in this =eld only contemplate turbulent :ow. In the transitional regime the mean drop size diameter decreases abruptly with Weber number, but this pattern changes in the higher range ofWeber where the dispersed drops become smaller very smoothly. This pattern does not depend on the agitator used or hold-up fraction. The mean drop size diameter is smaller for the four paddle impeller and increases with hold-up fraction. The model developed may be applicable to dispersions in aromatic nitration reactors, improving its operation and design.
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spelling Effective interfacial area in agitated liquid–liquid continuous reactorsMultiphase reactorsInterfacial areaLiquid–liquidDrop sizeModelDispersionA chemical method has been used to quantify the e ective interfacial area in a ba4ed continuous stirred liquid–liquid reactor. Two and four straight paddle impellers were used in the experimental runs, at 34◦C, with hold-up fractions of dispersed organic phase between 0.061 and 0.166 and stirring speed ranging from 360 to 1500 rpm. In:uence of the residence time on the formation of the interfacial area generated in this system was not registered; however, di erences were reported between continuous and batch mode operations. The interfacial area was correlated to hold-up fraction and Weber number by a new empirical model proposed in this work. This model allows to use only one equation to calculate the interfacial area in this continuous stirred reactor in the wide range of operating conditions tested (490¡We¡9600), which include di erent :ow regimes. This is a relevant contribution as previous studies in this =eld only contemplate turbulent :ow. In the transitional regime the mean drop size diameter decreases abruptly with Weber number, but this pattern changes in the higher range ofWeber where the dispersed drops become smaller very smoothly. This pattern does not depend on the agitator used or hold-up fraction. The mean drop size diameter is smaller for the four paddle impeller and increases with hold-up fraction. The model developed may be applicable to dispersions in aromatic nitration reactors, improving its operation and design.2003-09info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://hdl.handle.net/10316/7411http://hdl.handle.net/10316/7411https://doi.org/10.1016/S0009-2509(03)00302-6engChemical Engineering Science. 58:17 (2003) 3935-3945Quadros, Paulo A.info:eu-repo/semantics/openAccessreponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãoinstacron:RCAAP2020-11-06T16:59:28Zoai:estudogeral.uc.pt:10316/7411Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireopendoar:71602024-03-19T20:59:17.409838Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) - Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãofalse
dc.title.none.fl_str_mv Effective interfacial area in agitated liquid–liquid continuous reactors
title Effective interfacial area in agitated liquid–liquid continuous reactors
spellingShingle Effective interfacial area in agitated liquid–liquid continuous reactors
Quadros, Paulo A.
Multiphase reactors
Interfacial area
Liquid–liquid
Drop size
Model
Dispersion
title_short Effective interfacial area in agitated liquid–liquid continuous reactors
title_full Effective interfacial area in agitated liquid–liquid continuous reactors
title_fullStr Effective interfacial area in agitated liquid–liquid continuous reactors
title_full_unstemmed Effective interfacial area in agitated liquid–liquid continuous reactors
title_sort Effective interfacial area in agitated liquid–liquid continuous reactors
author Quadros, Paulo A.
author_facet Quadros, Paulo A.
author_role author
dc.contributor.author.fl_str_mv Quadros, Paulo A.
dc.subject.por.fl_str_mv Multiphase reactors
Interfacial area
Liquid–liquid
Drop size
Model
Dispersion
topic Multiphase reactors
Interfacial area
Liquid–liquid
Drop size
Model
Dispersion
description A chemical method has been used to quantify the e ective interfacial area in a ba4ed continuous stirred liquid–liquid reactor. Two and four straight paddle impellers were used in the experimental runs, at 34◦C, with hold-up fractions of dispersed organic phase between 0.061 and 0.166 and stirring speed ranging from 360 to 1500 rpm. In:uence of the residence time on the formation of the interfacial area generated in this system was not registered; however, di erences were reported between continuous and batch mode operations. The interfacial area was correlated to hold-up fraction and Weber number by a new empirical model proposed in this work. This model allows to use only one equation to calculate the interfacial area in this continuous stirred reactor in the wide range of operating conditions tested (490¡We¡9600), which include di erent :ow regimes. This is a relevant contribution as previous studies in this =eld only contemplate turbulent :ow. In the transitional regime the mean drop size diameter decreases abruptly with Weber number, but this pattern changes in the higher range ofWeber where the dispersed drops become smaller very smoothly. This pattern does not depend on the agitator used or hold-up fraction. The mean drop size diameter is smaller for the four paddle impeller and increases with hold-up fraction. The model developed may be applicable to dispersions in aromatic nitration reactors, improving its operation and design.
publishDate 2003
dc.date.none.fl_str_mv 2003-09
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
format article
status_str publishedVersion
dc.identifier.uri.fl_str_mv http://hdl.handle.net/10316/7411
http://hdl.handle.net/10316/7411
https://doi.org/10.1016/S0009-2509(03)00302-6
url http://hdl.handle.net/10316/7411
https://doi.org/10.1016/S0009-2509(03)00302-6
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Chemical Engineering Science. 58:17 (2003) 3935-3945
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eu_rights_str_mv openAccess
dc.source.none.fl_str_mv reponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)
instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informação
instacron:RCAAP
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reponame_str Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)
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