dc.creatorIsmail, KAR
dc.creatorde Sousa, LM
dc.creatorLino, FAM
dc.date2012
dc.dateMAR
dc.date2014-07-30T18:43:10Z
dc.date2015-11-26T17:43:40Z
dc.date2014-07-30T18:43:10Z
dc.date2015-11-26T17:43:40Z
dc.date.accessioned2018-03-29T00:25:44Z
dc.date.available2018-03-29T00:25:44Z
dc.identifierInternational Journal Of Heat And Mass Transfer. Pergamon-elsevier Science Ltd, v. 55, n. 41858, n. 1823, n. 1835, 2012.
dc.identifier0017-9310
dc.identifierWOS:000300967600002
dc.identifier10.1016/j.ijheatmasstransfer.2011.11.031
dc.identifierhttp://www.repositorio.unicamp.br/jspui/handle/REPOSIP/71796
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/71796
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1287652
dc.descriptionConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)
dc.descriptionThis paper presents the results of an experimental and numerical investigation on the solidification of PCM around a curved cold tube to determine the effects of the Dean number, cooling fluid flow rate and its temperature on the interface velocity, the time for complete solidification and the solidified mass. To formulate the solidification process around a curved tube a conduction model was used together with the immobilization technique and the Landau transform. The energy equation and the associated boundary conditions were discretized by the finite control volumes method. The computational program was optimized by numerical experiments and the optimized form was used to validate the model. Comparisons of the numerical predictions and experiments to investigate the effects the Dean number on the solidified mass showed agreement within 1% while the interface velocity and the time for complete solidification showed agreements of about 8% and less than 6%, respectively. The effects of the flow rate of the working fluid could be predicted within less than 8% for the solidified mass and to less than 4% for both the interface velocity and the time for complete solidification. The effects of the temperature of the working fluid are predictable to within less than 8% for the time for complete solidification and the interface velocity. (C) 2011 Elsevier Ltd. All rights reserved.
dc.description55
dc.description41858
dc.description1823
dc.description1835
dc.descriptionConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)
dc.descriptionFAPEMA
dc.descriptionConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)
dc.languageen
dc.publisherPergamon-elsevier Science Ltd
dc.publisherOxford
dc.publisherInglaterra
dc.relationInternational Journal Of Heat And Mass Transfer
dc.relationInt. J. Heat Mass Transf.
dc.rightsfechado
dc.rightshttp://www.elsevier.com/about/open-access/open-access-policies/article-posting-policy
dc.sourceWeb of Science
dc.subjectPCM
dc.subjectSolidification
dc.subjectPhase change
dc.subjectCurved tube
dc.subjectModeling of thermal storage
dc.subjectStream-line Motion
dc.subjectHeat-transfer
dc.subjectIce Formation
dc.subjectPipe
dc.subjectFlow
dc.subjectFluid
dc.titleSolidification of PCM around a curved tube
dc.typeArtículos de revistas


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