Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field

In this study, we report the thermophysical properties (at room temperature) and the morphology of a composite with a polyester resin matrix and magnetite filler powders (Fe3O4), conformed in three configurations: randomly dispersed particles, particles oriented parallel to a constant 300 mT magneti...

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Autores:
LARA GONZÁLEZ, LUIS ÁNGEL
Peña Rodriguez, Gabriel
Pineda Triana, Yaneth
Tipo de recurso:
Article of journal
Fecha de publicación:
2019
Institución:
Universidad Francisco de Paula Santander
Repositorio:
Repositorio Digital UFPS
Idioma:
eng
OAI Identifier:
oai:repositorio.ufps.edu.co:ufps/1442
Acceso en línea:
http://repositorio.ufps.edu.co/handle/ufps/1442
Palabra clave:
resin-magnetite composites
thermophysical properties
morphology
morphology
Hashin and Shtrikman model
Rights
openAccess
License
Atribución 4.0 Internacional (CC BY 4.0)
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dc.title.eng.fl_str_mv Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
title Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
spellingShingle Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
resin-magnetite composites
thermophysical properties
morphology
morphology
Hashin and Shtrikman model
title_short Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
title_full Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
title_fullStr Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
title_full_unstemmed Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
title_sort Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field
dc.creator.fl_str_mv LARA GONZÁLEZ, LUIS ÁNGEL
Peña Rodriguez, Gabriel
Pineda Triana, Yaneth
dc.contributor.author.none.fl_str_mv LARA GONZÁLEZ, LUIS ÁNGEL
Peña Rodriguez, Gabriel
Pineda Triana, Yaneth
dc.subject.proposal.eng.fl_str_mv resin-magnetite composites
thermophysical properties
morphology
morphology
Hashin and Shtrikman model
topic resin-magnetite composites
thermophysical properties
morphology
morphology
Hashin and Shtrikman model
description In this study, we report the thermophysical properties (at room temperature) and the morphology of a composite with a polyester resin matrix and magnetite filler powders (Fe3O4), conformed in three configurations: randomly dispersed particles, particles oriented parallel to a constant 300 mT magnetic field, and particles oriented perpendicular to a constant 300 mT magnetic field. Samples were formed by hand lay-up with weight percentages of 10, 20 and 30%, where the highest concentration corresponds to the resin. The thermophysical properties were determined using the KD2 Pro® system, which uses the physical principle of linear transient heat flow, for which the dual sensor SH-1 was used. The morphology and microanalysis were studied using a scanning electron microscope (SEM, FEI Quanta 650 FEG). It was observed from the morphology that the magnetite particles are oriented in the direction of the magnetic field lines during the process of resin curing. It was also perceived that the values of the thermophysical properties found experimentally are within the limits (upper and lower) of Hashin and Shtrikman and that those values increase when the magnetite concentration increases in the sample. No significant difference was observed in the thermal properties because of the magnetic field applied.
publishDate 2019
dc.date.issued.none.fl_str_mv 2019-07-02
dc.date.accessioned.none.fl_str_mv 2021-11-26T13:47:22Z
dc.date.available.none.fl_str_mv 2021-11-26T13:47:22Z
dc.type.spa.fl_str_mv Artículo de revista
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dc.identifier.uri.none.fl_str_mv http://repositorio.ufps.edu.co/handle/ufps/1442
dc.identifier.doi.none.fl_str_mv 10.3934/matersci.2019.4.549
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dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartof.none.fl_str_mv AIMS Materials Science
dc.relation.citationedition.spa.fl_str_mv Vol.6 No.4.(2019)
dc.relation.citationendpage.spa.fl_str_mv 558
dc.relation.citationissue.spa.fl_str_mv 4 (2019)
dc.relation.citationstartpage.spa.fl_str_mv 549
dc.relation.citationvolume.spa.fl_str_mv 6
dc.relation.cites.none.fl_str_mv González, L. Á. L., Peña-Rodríguez, G., & Triana, Y. P. (2019). Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field. AIMS Materials Science, 6(4), 549-558.
dc.relation.ispartofjournal.spa.fl_str_mv AIMS Materials Science
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dc.rights.creativecommons.spa.fl_str_mv Atribución 4.0 Internacional (CC BY 4.0)
eu_rights_str_mv openAccess
rights_invalid_str_mv Atribución 4.0 Internacional (CC BY 4.0)
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dc.format.mimetype.spa.fl_str_mv application/pdf
dc.publisher.spa.fl_str_mv AIMS Materials Science
dc.publisher.place.spa.fl_str_mv Washintong D.C , Estados Unidos
dc.source.spa.fl_str_mv http://www.aimspress.com/article/id/3915
institution Universidad Francisco de Paula Santander
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spelling LARA GONZÁLEZ, LUIS ÁNGELe01cd1156f74ce64a1d9bc54b6bb029e600Peña Rodriguez, Gabriel4eaba0408a3f49f82929dc957fa8eee1600Pineda Triana, Yaneth89985e3f38e9b2c2d6ddac81a69c32cf6002021-11-26T13:47:22Z2021-11-26T13:47:22Z2019-07-02http://repositorio.ufps.edu.co/handle/ufps/144210.3934/matersci.2019.4.549In this study, we report the thermophysical properties (at room temperature) and the morphology of a composite with a polyester resin matrix and magnetite filler powders (Fe3O4), conformed in three configurations: randomly dispersed particles, particles oriented parallel to a constant 300 mT magnetic field, and particles oriented perpendicular to a constant 300 mT magnetic field. Samples were formed by hand lay-up with weight percentages of 10, 20 and 30%, where the highest concentration corresponds to the resin. The thermophysical properties were determined using the KD2 Pro® system, which uses the physical principle of linear transient heat flow, for which the dual sensor SH-1 was used. The morphology and microanalysis were studied using a scanning electron microscope (SEM, FEI Quanta 650 FEG). It was observed from the morphology that the magnetite particles are oriented in the direction of the magnetic field lines during the process of resin curing. It was also perceived that the values of the thermophysical properties found experimentally are within the limits (upper and lower) of Hashin and Shtrikman and that those values increase when the magnetite concentration increases in the sample. No significant difference was observed in the thermal properties because of the magnetic field applied.application/pdfengAIMS Materials ScienceWashintong D.C , Estados UnidosAIMS Materials ScienceVol.6 No.4.(2019)5584 (2019)5496González, L. Á. L., Peña-Rodríguez, G., & Triana, Y. P. (2019). Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field. AIMS Materials Science, 6(4), 549-558.AIMS Materials Science© 2019 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)info:eu-repo/semantics/openAccessAtribución 4.0 Internacional (CC BY 4.0)http://purl.org/coar/access_right/c_abf2http://www.aimspress.com/article/id/3915Effective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic fieldArtículo 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_970fb48d4fbd8a85resin-magnetite compositesthermophysical propertiesmorphologymorphologyHashin and Shtrikman modelNgo I, Jeon S, Byon C (2016) Thermal conductivity of transparent and flexible polymers containing fillers: a literature review. Int J Heat Mass Tran 98: 219–226Hussain ARJ, Alahyari AA, Eastman S, et al. 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Mater Today 17: 163–174Burgen N, Laachachi A, Ferriol M, et al. (2016) Review of thermal conductivity in composites: mechanisms, parameters and theory. Prog Polym Sci 61: 1–28Weidenfeller B, Hofer M, Schilling F (2002) Thermal and electrical properties of magnetite filled polymers. Compos Part A-Appl S 33: 1041–1053Younes H, Christensen G, Liu M, et al. (2014) Alignment of carbon nanofibers in water and epoxy by wxternal magnetic field. J Nanofluids 3: 33–37.. Horton M, Hong H, Li C, et al. (2010). Magnetic alignment of Ni-coated single wall carbon nanotubes in heat transfer nanofluids. J Appl Phys 107: 1–4.Liu M, Younes H, Hong H, et al. (2019) Polymer nanocomposites with improved mechanical and thermal properties by magnetically aligned carbon nanotubes. Polymer 166: 81–87Younes H, Christensen G, Luan X, et al. (2012) Effects of alignment, pH, surfactant, and solvent on heat transfer nanofluids containing Fe2O3 and CuO nanoparticles. J Appl Phys 111: 064308Ku J, Valdez-Grijalva MA, Deng R, et al. (2019) Modelling external magnetic fields of magnetite particles: from micro- to macro-scale. Geosciences 9: 133Vargas Z, Filipcsei G, Zrinyi M (2006) Magnetic field sensitive functional elastomers with tuneable elastic modulus. Polymer 47: 227–233Boon MS, Mariatti M (2014) Optimization of magnetic and dielectric properties of surface-treated magnetite-filled epoxy composites by factorial design. J Magn Magn Mater 355: 319–324Pedroso AG, Rosa DS, Atvars TDZ (2002) Manufacture of sheets using post-consumer unsaturated polyester resin/glass fibre composites. Prog Rubber Plast Re 18: 111–125Oladunjove M, Sanuade OA (2012) Thermal diffusivity, thermal effusivity and specific heat in soils in Olurungo Powerplan, soutwestern Nigeria. IJRRAS 13: 502–521Ma X, Omer S, Zhang W, et al. (2008) Thermal conductivity measurement of two microencapsulated phase change slurries. Int J Low-Carbon Tec 3: 245–253Gustavsson M, Karawaracki E, Gustafsson SE (1994) Thermal conductivity, thermal diffusivity, and specific heat of thin samples from transient measurements with hot disk sensors. Rev Sci Instrum 65: 3856–3859Maldonado LM, Rodríguez GP (2014) Effect of ceramic dental waste in thermo-physical properties of materials composed with polyester resins. Ingeniería Investigación y Desarrollo 14: 2–5. Available from: https://doi.org/10.19053/1900771X.3442.Schilling F, Weidenfeller B, Ho M (2002) Thermal and electrical properties of magnetite filled polymers. Compos Part A-Appl S 33: 1041–1053Hashin Z, Shtrikman S (1962) A variational approach to the theory of the effective magnetic permeability of multiphase materials. J Appl Phys 33: 3125–3131.Razzaq MY, Anhlt M, Fromann L, et al. (2007) Thermal, electrical and magnetic studies of magnetite filled polyurethane shape memory polymers. Mat Sci Eng A-Struct 444: 227– 235Gong L, Wang Y, Cheng X, et al. (2014) International journal of heat and mass transfer a novel effective medium theory for modelling the thermal conductivity of porous materials. Int J Heat Mass Tran 68: 295–298Pena-Rodríguez G, Rivera-Suarez PA, Gónzalez-Gómez CH, et al. (2018) Effect of the concentration of magnetite on the structure, electrical and magnetic properties of a polyester resin-based composite. TecnoLogicas 21: 13–27ORIGINALEffective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field.pdfEffective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field.pdfapplication/pdf600763https://repositorio.ufps.edu.co/bitstream/ufps/1442/1/Effective%20thermal%20properties%20of%20a%20magnetite-polyester%20composite%20conformed%20in%20the%20presence%20of%20a%20constant%20magnetic%20field.pdfd416719f7b58cf6336b8a7e497256927MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-814828https://repositorio.ufps.edu.co/bitstream/ufps/1442/2/license.txt2f9959eaf5b71fae44bbf9ec84150c7aMD52open accessTEXTEffective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field.pdf.txtEffective thermal properties of a magnetite-polyester composite conformed in the presence of a constant magnetic field.pdf.txtExtracted 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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, GA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