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dc.creatorFoncubierta Blázquez, Juan Luises
dc.creatorRodríguez Maestre, Ismaeles
dc.creatorGonzález Gallero, Francisco Javieres
dc.creatorPérez-Lombard, Luises
dc.creatorBottarelli, Michelees
dc.date.accessioned2023-03-27T13:51:46Z
dc.date.available2023-03-27T13:51:46Z
dc.date.issued2023-01
dc.identifier.citationFoncubierta Blázquez, J.L., Rodríguez Maestre, I., González Gallero, F.J., Pérez-Lombard, L. y Bottarelli, M. (2023). Experimental adjustment of the turbulent Schmidt number to model the evaporation rate of swimming pools in CFD programmes. Case Studies in Thermal Engineering, 41, 102665. https://doi.org/10.1016/j.csite.2022.102665.
dc.identifier.issn2214-157Xes
dc.identifier.urihttps://hdl.handle.net/11441/143594
dc.descriptionThis is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).es
dc.description.abstractWater evaporation rate is among the most significant parameters to design and select air con- ditioning systems in buildings with indoor swimming pools. Experimental correlations are today widely used to estimate water evaporation rate, although discrepancies of up to 80% among existing correlations have been shown. An alternative to these empirical methods is the calcu- lation of evaporation rate through computer fluid dynamics techniques. One of the most signif- icant parameters to solve the mass transfer at the air-water interface in these models is the value of the turbulent Schmidt number. Although this value depends on air and water conditions (i.e., temperatures, velocities, and vapour pressure, among others), commercial computer fluid dy- namics programmes set a fixed value by default. This study presents a new value through an experimental adjustment. A total of 40 experimental tests have been performed in a wind tunnel under typical conditions in indoor swimming pools. Afterwards, the adjustment was validated with data from 145 experimental tests reported in the scientific literature. The mean relative error in the evaporation rate using the turbulent Schmidt number was 7%, as against 25% using the value by default. The maximum error was reduced from 35% to 15% in forced convection regime.es
dc.formatapplication/pdfes
dc.format.extent9 p.es
dc.language.isoenges
dc.publisherElsevieres
dc.relation.ispartofCase Studies in Thermal Engineering, 41, 102665.
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.titleExperimental adjustment of the turbulent Schmidt number to model the evaporation rate of swimming pools in CFD programmeses
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.contributor.affiliationUniversidad de Sevilla. Departamento de Ingeniería Energéticaes
dc.relation.publisherversionhttps://www.sciencedirect.com/science/article/pii/S2214157X22009029es
dc.identifier.doi10.1016/j.csite.2022.102665es
dc.contributor.groupUniversidad de Sevilla. TEP143: Termotecnia.es
dc.journaltitleCase Studies in Thermal Engineeringes
dc.publication.volumen41es
dc.publication.initialPage102665es

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