Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger
This article presents the development of some case studies on shell and tube heat exchangers using a graphical interface developed in MATLAB®. Through the case studies, the variation in the performance of the equipment was determined by means of the heat transfer coefficient in function of some para...
- Autores:
-
Delgado Ruiz, Leonardo
Acevedo Peñaloza, Carlos Humberto
Valencia Ochoa, Guillermo
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2018
- Institución:
- Universidad Francisco de Paula Santander
- Repositorio:
- Repositorio Digital UFPS
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.ufps.edu.co:ufps/1113
- Acceso en línea:
- http://repositorio.ufps.edu.co/handle/ufps/1113
- Palabra clave:
- Heat Exchanger
- Rights
- openAccess
- License
- © Research India Publications.
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| dc.title.eng.fl_str_mv |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| title |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| spellingShingle |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger Heat Exchanger |
| title_short |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| title_full |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| title_fullStr |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| title_full_unstemmed |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| title_sort |
Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger |
| dc.creator.fl_str_mv |
Delgado Ruiz, Leonardo Acevedo Peñaloza, Carlos Humberto Valencia Ochoa, Guillermo |
| dc.contributor.author.none.fl_str_mv |
Delgado Ruiz, Leonardo Acevedo Peñaloza, Carlos Humberto Valencia Ochoa, Guillermo |
| dc.subject.proposal.eng.fl_str_mv |
Heat Exchanger |
| topic |
Heat Exchanger |
| description |
This article presents the development of some case studies on shell and tube heat exchangers using a graphical interface developed in MATLAB®. Through the case studies, the variation in the performance of the equipment was determined by means of the heat transfer coefficient in function of some parameters such as mass flow and tube arrangements, establishing initial conditions for each run that were established in the software. Likewise, the article shows in detail the methodology with which the study was developed, the fundamental equations used to calculate these results and the graphs obtained. Through this study, it was verified that the variables studied had such an influence on the parameters evaluated, with the objective of establishing selection and operation criteria when designing a shell and tube heat exchanger. |
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2018 |
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2018 |
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2021-11-18T23:38:35Z |
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2021-11-18T23:38:35Z |
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Artículo de revista |
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Text |
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0973-4562 |
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http://repositorio.ufps.edu.co/handle/ufps/1113 |
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0973-4562 |
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eng |
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eng |
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International Journal of Applied Engineering Research |
| dc.relation.citationedition.spa.fl_str_mv |
Vol.13 No.14.(2018) |
| dc.relation.citationendpage.spa.fl_str_mv |
11391 |
| dc.relation.citationissue.spa.fl_str_mv |
14(2018) |
| dc.relation.citationstartpage.spa.fl_str_mv |
11387 |
| dc.relation.citationvolume.spa.fl_str_mv |
13 |
| dc.relation.cites.none.fl_str_mv |
Ruiz, L. D., Peñaloza, C. A., & Ochoa, G. V. (2018). Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger. International Journal of Applied Engineering Research, 13(14), 11387-11391. |
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International Journal of Applied Engineering Research |
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© Research India Publications. |
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http://purl.org/coar/access_right/c_abf2 |
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info:eu-repo/semantics/openAccess |
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Atribución-NoComercial 4.0 Internacional (CC BY-NC 4.0) |
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© Research India Publications. Atribución-NoComercial 4.0 Internacional (CC BY-NC 4.0) http://purl.org/coar/access_right/c_abf2 |
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openAccess |
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05 páginas |
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application/pdf |
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International Journal of Applied Engineering Research |
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India |
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http://www.ripublication.com/Volume/ijaerv13n14.htm |
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Universidad Francisco de Paula Santander |
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Delgado Ruiz, Leonardo08fd6ad6a925e0807edc4acebacc4564Acevedo Peñaloza, Carlos Humberto1f12a99f8d5bcc67d1eb10c7c07c76a3600Valencia Ochoa, Guillermo7b9fd01ee22f884965a5cd038e2d734d2021-11-18T23:38:35Z2021-11-18T23:38:35Z20180973-4562http://repositorio.ufps.edu.co/handle/ufps/1113This article presents the development of some case studies on shell and tube heat exchangers using a graphical interface developed in MATLAB®. Through the case studies, the variation in the performance of the equipment was determined by means of the heat transfer coefficient in function of some parameters such as mass flow and tube arrangements, establishing initial conditions for each run that were established in the software. Likewise, the article shows in detail the methodology with which the study was developed, the fundamental equations used to calculate these results and the graphs obtained. Through this study, it was verified that the variables studied had such an influence on the parameters evaluated, with the objective of establishing selection and operation criteria when designing a shell and tube heat exchanger.05 páginasapplication/pdfengInternational Journal of Applied Engineering ResearchIndiaInternational Journal of Applied Engineering ResearchVol.13 No.14.(2018)1139114(2018)1138713Ruiz, L. D., Peñaloza, C. A., & Ochoa, G. V. (2018). Effect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger. International Journal of Applied Engineering Research, 13(14), 11387-11391.International Journal of Applied Engineering Research© Research India Publications.info:eu-repo/semantics/openAccessAtribución-NoComercial 4.0 Internacional (CC BY-NC 4.0)http://purl.org/coar/access_right/c_abf2http://www.ripublication.com/Volume/ijaerv13n14.htmEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchangerArtículo de revistahttp://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/version/c_970fb48d4fbd8a85Heat ExchangerV. I. & V. O. & A. Sukomel., TRANSMISION DEL CALOR. 1979.W. H. McAdams, TRANSMISION DE CALOR. Madrid, 1964.T. M. Yusof, H. Ibrahim, W. H. Azmi, and M. R. M. Rejab, “The thermal characteristics and performance of a ground heat exchanger for tropical climates,” Renew. Energy, vol. 121, pp. 528–538, 2018.V. Pandiyarajan, M. Chinna Pandian, E. Malan, R. Velraj, and R. V. Seeniraj, “Experimental investigation on heat recovery from diesel engine exhaust using finned shell and tube heat exchanger and thermal storage system,” Appl. Energy, vol. 88, no. 1, pp. 77–87, 2011.M. Medrano, M. O. Yilmaz, M. Nogués, I. Martorell, J. Roca, and L. F. Cabeza, “Experimental evaluation of commercial heat exchangers for use as PCM thermal storage systems,” Appl. Energy, vol. 86, no. 10, pp. 2047–2055, 2009.Y. Cengel and B. Michael, Thermodinámica, 7th ed. 2012.ORIGINALEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger.pdfEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger.pdfapplication/pdf673470https://repositorio.ufps.edu.co/bitstream/ufps/1113/1/Effect%20of%20the%20mass%20flow%20rate%20on%20the%20heat%20transfer%20phenomena%20in%20a%20shell%20and%20tube%20heat%20exchanger.pdfd83852185985112fe42536a77d7b3f09MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstream/ufps/1113/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTEXTEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger.pdf.txtEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger.pdf.txtExtracted texttext/plain16183https://repositorio.ufps.edu.co/bitstream/ufps/1113/3/Effect%20of%20the%20mass%20flow%20rate%20on%20the%20heat%20transfer%20phenomena%20in%20a%20shell%20and%20tube%20heat%20exchanger.pdf.txt119909e41b0c446402dc28a6c8e7ad60MD53open accessTHUMBNAILEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger.pdf.jpgEffect of the mass flow rate on the heat transfer phenomena in a shell and tube heat exchanger.pdf.jpgGenerated Thumbnailimage/jpeg16646https://repositorio.ufps.edu.co/bitstream/ufps/1113/4/Effect%20of%20the%20mass%20flow%20rate%20on%20the%20heat%20transfer%20phenomena%20in%20a%20shell%20and%20tube%20heat%20exchanger.pdf.jpgd8832873e565577e7c16dc52d042d78aMD54open accessufps/1113oai:repositorio.ufps.edu.co:ufps/11132022-05-23 10:54:48.793open accessRepositorio Universidad Francisco de Paula 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 incorporada en las Obras Colectivas.

b.	Distribuir copias o fonogramas de las Obras, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública, incluyéndolas como incorporadas en Obras Colectivas, según corresponda.

c.	Distribuir copias de las Obras Derivadas que se generen, exhibirlas públicamente, ejecutarlas públicamente y/o ponerlas a disposición pública.
Los derechos mencionados anteriormente pueden ser ejercidos en todos los medios y formatos, actualmente conocidos o que se inventen en el futuro. Los derechos antes mencionados incluyen el derecho a realizar dichas modificaciones en la medida que sean técnicamente necesarias para ejercer los derechos en otro medio o formatos, pero de otra manera usted no está autorizado para realizar obras derivadas. Todos los derechos no otorgados expresamente por el Licenciante quedan por este medio reservados, incluyendo pero sin limitarse a aquellos que se mencionan en las secciones 4(d) y 4(e).

4. Restricciones.
La licencia otorgada en la anterior Sección 3 está expresamente sujeta y limitada por las siguientes restricciones:

a.	Usted puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra sólo bajo las condiciones de esta Licencia, y Usted debe incluir una copia de esta licencia o del Identificador Universal de Recursos de la misma con cada copia de la Obra que distribuya, exhiba públicamente, ejecute públicamente o ponga a disposición pública. No es posible ofrecer o imponer ninguna condición sobre la Obra que altere o limite las condiciones de esta Licencia o el ejercicio de los derechos de los destinatarios otorgados en este documento. No es posible sublicenciar la Obra. Usted debe mantener intactos todos los avisos que hagan referencia a esta Licencia y a la cláusula de limitación de garantías. Usted no puede distribuir, exhibir públicamente, ejecutar públicamente, o poner a disposición pública la Obra con alguna medida tecnológica que controle el acceso o la utilización de ella de una forma que sea inconsistente con las condiciones de esta Licencia. Lo anterior se aplica a la Obra incorporada a una Obra Colectiva, pero esto no exige que la Obra Colectiva aparte de la obra misma quede sujeta a las condiciones de esta Licencia. Si Usted crea una Obra Colectiva, previo aviso de cualquier Licenciante debe, en la medida de lo posible, eliminar de la Obra Colectiva cualquier referencia a dicho Licenciante o al Autor Original, según lo solicitado por el Licenciante y conforme lo exige la cláusula 4(c).

b.	Usted no puede ejercer ninguno de los derechos que le han sido otorgados en la Sección 3 precedente de modo que estén principalmente destinados o directamente dirigidos a conseguir un provecho comercial o una compensación monetaria privada. El intercambio de la Obra por otras obras protegidas por derechos de autor, ya sea a través de un sistema para compartir archivos digitales (digital file-sharing) o de cualquier otra manera no será considerado como estar destinado principalmente o dirigido directamente a conseguir un provecho comercial o una compensación monetaria privada, siempre que no se realice un pago mediante una compensación monetaria en relación con el intercambio de obras protegidas por el derecho de autor.

c.	Si usted distribuye, exhibe públicamente, ejecuta públicamente o ejecuta públicamente en forma digital la Obra o cualquier Obra Derivada u Obra Colectiva, Usted debe mantener intacta toda la información de derecho de autor de la Obra y proporcionar, de forma razonable según el medio o manera que Usted esté utilizando: (i) el nombre del Autor Original si está provisto (o seudónimo, si fuere aplicable), y/o (ii) el nombre de la parte o las partes que el Autor Original y/o el Licenciante hubieren designado para la atribución (v.g., un instituto patrocinador, editorial, publicación) en la información de los derechos de autor del Licenciante, términos de servicios o de otras formas razonables; el título de la Obra si está provisto; en la medida de lo razonablemente factible y, si está provisto, el Identificador Uniforme de Recursos (Uniform Resource Identifier) que el Licenciante especifica para ser asociado con la Obra, salvo que tal URI no se refiera a la nota sobre los derechos de autor o a la información sobre el licenciamiento de la Obra; y en el caso de una Obra Derivada, atribuir el crédito identificando el uso de la Obra en la Obra Derivada (v.g., "Traducción Francesa de la Obra del Autor Original," o "Guión Cinematográfico basado en la Obra original del Autor Original"). Tal crédito puede ser implementado de cualquier forma razonable; en el caso, sin embargo, de Obras Derivadas u Obras Colectivas, tal crédito aparecerá, como mínimo, donde aparece el crédito de cualquier otro autor comparable y de una manera, al menos, tan destacada como el crédito de otro autor comparable.

d.	Para evitar toda confusión, el Licenciante aclara que, cuando la obra es una composición musical:

i.	Regalías por interpretación y ejecución bajo licencias generales. El Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública o la ejecución pública digital de la obra y de recolectar, sea individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, SAYCO), las regalías por la ejecución pública o por la ejecución pública digital de la obra (por ejemplo Webcast) licenciada bajo licencias generales, si la interpretación o ejecución de la obra está primordialmente orientada por o dirigida a la obtención de una ventaja comercial o una compensación monetaria privada.

ii.	Regalías por Fonogramas. El Licenciante se reserva el derecho exclusivo de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, los consagrados por la SAYCO), una agencia de derechos musicales o algún agente designado, las regalías por cualquier fonograma que Usted cree a partir de la obra (“versión cover”) y distribuya, en los términos del régimen de derechos de autor, si la creación o distribución de esa versión cover está primordialmente destinada o dirigida a obtener una ventaja comercial o una compensación monetaria privada.

e.	Gestión de Derechos de Autor sobre Interpretaciones y Ejecuciones Digitales (WebCasting). Para evitar toda confusión, el Licenciante aclara que, cuando la obra sea un fonograma, el Licenciante se reserva el derecho exclusivo de autorizar la ejecución pública digital de la obra (por ejemplo, webcast) y de recolectar, individualmente o a través de una sociedad de gestión colectiva de derechos de autor y derechos conexos (por ejemplo, ACINPRO), las regalías por la ejecución pública digital de la obra (por ejemplo, webcast), sujeta a las disposiciones aplicables del régimen de Derecho de Autor, si esta ejecución pública digital está primordialmente dirigida a obtener una ventaja comercial o una compensación monetaria privada.

5. Representaciones, Garantías y Limitaciones de Responsabilidad.
A MENOS QUE LAS PARTES LO ACORDARAN DE OTRA FORMA POR ESCRITO, EL LICENCIANTE OFRECE LA OBRA (EN EL ESTADO EN EL QUE SE ENCUENTRA) “TAL CUAL”, SIN BRINDAR GARANTÍAS DE CLASE ALGUNA RESPECTO DE LA OBRA, YA SEA EXPRESA, IMPLÍCITA, LEGAL O CUALQUIERA OTRA, INCLUYENDO, SIN LIMITARSE A ELLAS, GARANTÍAS DE TITULARIDAD, COMERCIABILIDAD, ADAPTABILIDAD O ADECUACIÓN A PROPÓSITO DETERMINADO, AUSENCIA DE INFRACCIÓN, DE AUSENCIA DE DEFECTOS LATENTES O DE OTRO TIPO, O LA PRESENCIA O AUSENCIA DE ERRORES, SEAN O NO DESCUBRIBLES (PUEDAN O NO SER ESTOS DESCUBIERTOS). ALGUNAS JURISDICCIONES NO PERMITEN LA EXCLUSIÓN DE GARANTÍAS IMPLÍCITAS, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.

6. Limitación de responsabilidad.
A MENOS QUE LO EXIJA EXPRESAMENTE LA LEY APLICABLE, EL LICENCIANTE NO SERÁ RESPONSABLE ANTE USTED POR DAÑO ALGUNO, SEA POR RESPONSABILIDAD EXTRACONTRACTUAL, PRECONTRACTUAL O CONTRACTUAL, OBJETIVA O SUBJETIVA, SE TRATE DE DAÑOS MORALES O PATRIMONIALES, DIRECTOS O INDIRECTOS, PREVISTOS O IMPREVISTOS PRODUCIDOS POR EL USO DE ESTA LICENCIA O DE LA OBRA, AUN CUANDO EL LICENCIANTE HAYA SIDO ADVERTIDO DE LA POSIBILIDAD DE DICHOS DAÑOS. ALGUNAS LEYES NO PERMITEN LA EXCLUSIÓN DE CIERTA RESPONSABILIDAD, EN CUYO CASO ESTA EXCLUSIÓN PUEDE NO APLICARSE A USTED.

7. Término.

a.	Esta Licencia y los derechos otorgados en virtud de ella terminarán automáticamente si Usted infringe alguna condición establecida en ella. Sin embargo, los individuos o entidades que han recibido Obras Derivadas o Colectivas de Usted de conformidad con esta Licencia, no verán terminadas sus licencias, siempre que estos individuos o entidades sigan cumpliendo íntegramente las condiciones de estas licencias. Las Secciones 1, 2, 5, 6, 7, y 8 subsistirán a cualquier terminación de esta Licencia.

b.	Sujeta a las condiciones y términos anteriores, la licencia otorgada aquí es perpetua (durante el período de vigencia de los derechos de autor de la obra). No obstante lo anterior, el Licenciante se reserva el derecho a publicar y/o estrenar la Obra bajo condiciones de licencia diferentes o a dejar de distribuirla en los términos de esta Licencia en cualquier momento; en el entendido, sin embargo, que esa elección no servirá para revocar esta licencia o que deba ser otorgada , bajo los términos de esta licencia), y esta licencia continuará en pleno vigor y efecto a menos que sea terminada como se expresa atrás. La Licencia revocada continuará siendo plenamente vigente y efectiva si no se le da término en las condiciones indicadas anteriormente.

8. Varios.

a.	Cada vez que Usted distribuya o ponga a disposición pública la Obra o una Obra Colectiva, el Licenciante ofrecerá al destinatario una licencia en los mismos términos y condiciones que la licencia otorgada a Usted bajo esta Licencia.

b.	Si alguna disposición de esta Licencia resulta invalidada o no exigible, según la legislación vigente, esto no afectará ni la validez ni la aplicabilidad del resto de condiciones de esta Licencia y, sin acción adicional por parte de los sujetos de este acuerdo, aquélla se entenderá reformada lo mínimo necesario para hacer que dicha disposición sea válida y exigible.

c.	Ningún término o disposición de esta Licencia se estimará renunciada y ninguna violación de ella será consentida a menos que esa renuncia o consentimiento sea otorgado por escrito y firmado por la parte que renuncie o consienta.

d.	Esta Licencia refleja el acuerdo pleno entre las partes respecto a la Obra aquí licenciada. No hay arreglos, acuerdos o declaraciones respecto a la Obra que no estén especificados en este documento. El Licenciante no se verá limitado por ninguna disposición adicional que pueda surgir en alguna comunicación emanada de Usted. Esta Licencia no puede ser modificada sin el consentimiento mutuo por escrito del Licenciante y Usted.
0000-0002-5049-87541f12a99f8d5bcc67d1eb10c7c07c76a3600 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