Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors

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“The purpose of this study is to numerically investigate the performance of a solar physical surface absorption cooling system, in which activated carbon/methanol is used as a working pair, which is placed inside a parabolic-shaped solar collector. The governing mathematical model of this issue is b...

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Detalles Bibliográficos
Autores: Albaker, Abdullah, Cuba Carbajal, Nestor, Fernandez Atho, Manuel Octavio, Nunez Fernandez, Anderson, Delgado Laime, Maria Del Carmen, Borda Echavarria, Ani Mary, Alayi, Reza, Aladdin, Morteza
Formato: artículo
Fecha de Publicación:2023
Institución:Universidad Privada Norbert Wiener
Repositorio:UWIENER-Institucional
Lenguaje:inglés
OAI Identifier:oai:repositorio.uwiener.edu.pe:20.500.13053/9589
Enlace del recurso:https://hdl.handle.net/20.500.13053/9589
Nivel de acceso:acceso abierto
Materia:Thermodynamic analysis, The governing mathematical
3.03.00 -- Ciencias de la salud
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dc.title.es_PE.fl_str_mv Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
title Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
spellingShingle Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
Albaker, Abdullah
Thermodynamic analysis, The governing mathematical
3.03.00 -- Ciencias de la salud
title_short Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
title_full Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
title_fullStr Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
title_full_unstemmed Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
title_sort Thermodynamic analysis of absorption refrigeration cycles by parabolic trough collectors
author Albaker, Abdullah
author_facet Albaker, Abdullah
Cuba Carbajal, Nestor
Fernandez Atho, Manuel Octavio
Nunez Fernandez, Anderson
Delgado Laime, Maria Del Carmen
Borda Echavarria, Ani Mary
Alayi, Reza
Aladdin, Morteza
author_role author
author2 Cuba Carbajal, Nestor
Fernandez Atho, Manuel Octavio
Nunez Fernandez, Anderson
Delgado Laime, Maria Del Carmen
Borda Echavarria, Ani Mary
Alayi, Reza
Aladdin, Morteza
author2_role author
author
author
author
author
author
author
dc.contributor.author.fl_str_mv Albaker, Abdullah
Cuba Carbajal, Nestor
Fernandez Atho, Manuel Octavio
Nunez Fernandez, Anderson
Delgado Laime, Maria Del Carmen
Borda Echavarria, Ani Mary
Alayi, Reza
Aladdin, Morteza
dc.subject.es_PE.fl_str_mv Thermodynamic analysis, The governing mathematical
topic Thermodynamic analysis, The governing mathematical
3.03.00 -- Ciencias de la salud
dc.subject.ocde.es_PE.fl_str_mv 3.03.00 -- Ciencias de la salud
description “The purpose of this study is to numerically investigate the performance of a solar physical surface absorption cooling system, in which activated carbon/methanol is used as a working pair, which is placed inside a parabolic-shaped solar collector. The governing mathematical model of this issue is based on the equations of conservation of mass, conservation of energy, and thermodynamics of the physical surface absorption process. The equations are discretized using the fully implicit finite difference method, and the Fortran computer program was simulated. A comparison with the results of previous laboratory and numerical studies validated this model. At each point in the bed, the temperature, pressure, and mass of the refrigerant absorbed during the physical surface absorption/discharge process were calculated. In addition, the effects of the bed diameter, amount of solar radiation, source temperature, temperature, and pressure of the evaporator and condenser were investigated on the solar performance coefficient and the specific cooling power of the system. According to the built laboratory model and the working conditions of the system, the solar performance coefficient and the specific cooling capacity of the system are equal to 0.12 and 45.6 W/kg, respectively.“
publishDate 2023
dc.date.accessioned.none.fl_str_mv 2023-10-18T20:32:08Z
dc.date.available.none.fl_str_mv 2023-10-18T20:32:08Z
dc.date.issued.fl_str_mv 2023-06-13
dc.type.es_PE.fl_str_mv info:eu-repo/semantics/article
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dc.identifier.uri.none.fl_str_mv https://hdl.handle.net/20.500.13053/9589
dc.identifier.doi.none.fl_str_mv 10.1063/5.0153839
url https://hdl.handle.net/20.500.13053/9589
identifier_str_mv 10.1063/5.0153839
dc.language.iso.es_PE.fl_str_mv eng
language eng
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dc.format.es_PE.fl_str_mv application/pdf
dc.publisher.es_PE.fl_str_mv American Institute of Physics Inc
dc.publisher.country.es_PE.fl_str_mv USA
dc.source.none.fl_str_mv reponame:UWIENER-Institucional
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spelling Albaker, AbdullahCuba Carbajal, NestorFernandez Atho, Manuel OctavioNunez Fernandez, AndersonDelgado Laime, Maria Del CarmenBorda Echavarria, Ani MaryAlayi, RezaAladdin, Morteza2023-10-18T20:32:08Z2023-10-18T20:32:08Z2023-06-13https://hdl.handle.net/20.500.13053/958910.1063/5.0153839“The purpose of this study is to numerically investigate the performance of a solar physical surface absorption cooling system, in which activated carbon/methanol is used as a working pair, which is placed inside a parabolic-shaped solar collector. The governing mathematical model of this issue is based on the equations of conservation of mass, conservation of energy, and thermodynamics of the physical surface absorption process. The equations are discretized using the fully implicit finite difference method, and the Fortran computer program was simulated. A comparison with the results of previous laboratory and numerical studies validated this model. At each point in the bed, the temperature, pressure, and mass of the refrigerant absorbed during the physical surface absorption/discharge process were calculated. In addition, the effects of the bed diameter, amount of solar radiation, source temperature, temperature, and pressure of the evaporator and condenser were investigated on the solar performance coefficient and the specific cooling power of the system. According to the built laboratory model and the working conditions of the system, the solar performance coefficient and the specific cooling capacity of the system are equal to 0.12 and 45.6 W/kg, respectively.“application/pdfengAmerican Institute of Physics IncUSAinfo:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by/4.0/Thermodynamic analysis, The governing mathematical3.03.00 -- Ciencias de la saludThermodynamic analysis of absorption refrigeration cycles by parabolic trough collectorsinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionreponame:UWIENER-Institucionalinstname:Universidad Privada Norbert Wienerinstacron:UWIENERPublicationORIGINALPhysicsofFluids.pdfPhysicsofFluids.pdfapplication/pdf2322294https://dspace-uwiener.metabuscador.org/bitstreams/f4eac9ed-ad22-4b29-9aed-58029d6c0ee2/download920c0929229bafa9536df192755b8d93MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://dspace-uwiener.metabuscador.org/bitstreams/4a1dfb23-3542-4c64-b9e5-fb5752493b03/download8a4605be74aa9ea9d79846c1fba20a33MD52TEXTPhysicsofFluids.pdf.txtPhysicsofFluids.pdf.txtExtracted texttext/plain41688https://dspace-uwiener.metabuscador.org/bitstreams/b1237bf7-dd9f-4470-8680-ba72785b8541/download0f60ee405dc4cdc64b15d9be36102aa6MD53THUMBNAILPhysicsofFluids.pdf.jpgPhysicsofFluids.pdf.jpgGenerated Thumbnailimage/jpeg4496https://dspace-uwiener.metabuscador.org/bitstreams/66d2a4a8-e6db-42ef-985d-ff2182c2490e/download730249ff8ac2e08f8f37f6f5a7f942f3MD5420.500.13053/9589oai:dspace-uwiener.metabuscador.org:20.500.13053/95892024-12-13 12:09:10.098https://creativecommons.org/licenses/by/4.0/info:eu-repo/semantics/openAccessopen.accesshttps://dspace-uwiener.metabuscador.orgRepositorio Institucional de la Universidad de Wienerbdigital@metabiblioteca.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