Please use this identifier to cite or link to this item: http://hdl.handle.net/11452/23835
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dc.date.accessioned2022-01-04T07:20:52Z-
dc.date.available2022-01-04T07:20:52Z-
dc.date.issued2006-11-
dc.identifier.citationUmur, H. ve Özalp, A. A. (2006). ''Fluid flow and heat transfer in transitional boundary layers: Effects of surface curvature and free stream velocity''. Heat and Mass Transfer, 43(1), 7-15.en_US
dc.identifier.issn0947-7411-
dc.identifier.urihttps://doi.org/10.1007/s00231-005-0080-8-
dc.identifier.urihttps://link.springer.com/article/10.1007%2Fs00231-005-0080-8-
dc.identifier.urihttp://hdl.handle.net/11452/23835-
dc.description.abstractVelocity and wall temperature measurements, over flat plate, concave and convex walls, were experimentally investigated in a low-speed wind tunnel with inlet velocities of 4 and 12 m/s encompassing the transitional region with streamwise distance Reynolds numbers from 3.15x10(5) to 1.04x10(6). As the velocity profiles, recorded by a semi-circular pitot tube and a digital constant-temperature hot-wire anemometer, were compared to exact Blasius profile and (1/7)th power law, experimental local Stanton numbers to analytical flat plate solution and turbulent correlation formula. Intermittency factors, derived from velocities and local Stanton numbers, were presented both in streamwise and pitchwise directions. It was found that the convex curvature delayed transition up to Re (x) =1.04x10(6), with a mean intermittency value of 0.61 and a shape factor of 1.81, where the similar intermittency and shape factors were determined at Re (x) of 8.33x10(5) and 4.25x10(5) for the flat plate and concave wall, indicating the enhancing role of concave curvature on the transition mechanism. The thinner boundary layers of the concave surface resulted in higher intermittency values, corresponding to higher skin friction and Stanton numbers; moreover the lowest gap between the measured and derived Stanton numbers were also obtained over the concave surface. Destabilising role of the concave wall caused Stanton numbers to increase up to 22%, whereas the convex wall, due to its stabilising character, produced lower Stanton numbers by 12% with respect to those of the flat plate.en_US
dc.language.isoenen_US
dc.publisherSpringeren_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectThermodynamicsen_US
dc.subjectMechanicsen_US
dc.subjectStraighten_US
dc.subjectLaminaren_US
dc.subjectTurbulenceen_US
dc.subjectIntermittencyen_US
dc.subjectThermal structuresen_US
dc.subjectTransfer enhancementen_US
dc.subjectWind tunnelsen_US
dc.subjectThermal effectsen_US
dc.subjectStream flowen_US
dc.subjectReynolds numberen_US
dc.subjectHeat transferen_US
dc.subjectFlow of fluidsen_US
dc.subjectTurbulent correlation formulaen_US
dc.subjectTransitional boundary layersen_US
dc.subjectPower lawen_US
dc.subjectPitot tubesen_US
dc.subjectBoundary layersen_US
dc.titleFluid flow and heat transfer in transitional boundary layers: Effects of surface curvature and free stream velocityen_US
dc.typeArticleen_US
dc.identifier.wos000240803600002tr_TR
dc.identifier.scopus2-s2.0-33749248854tr_TR
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergitr_TR
dc.contributor.departmentUludağ Üniversitesi/Mühendislik Mimarlık Fakültesi/Makine Mühendisliği Bölümü.tr_TR
dc.contributor.orcid0000-0002-4976-9027tr_TR
dc.identifier.startpage7tr_TR
dc.identifier.endpage15tr_TR
dc.identifier.volume43tr_TR
dc.identifier.issue1tr_TR
dc.relation.journalHeat and Mass Transferen_US
dc.contributor.buuauthorUmur, H.-
dc.contributor.buuauthorÖzalp, A. Alper-
dc.contributor.researcheridABI-6888-2020tr_TR
dc.subject.wosThermodynamicsen_US
dc.subject.wosMechanicsen_US
dc.indexed.wosSCIEen_US
dc.indexed.scopusScopusen_US
dc.wos.quartileQ4en_US
dc.contributor.scopusid6602945164tr_TR
dc.contributor.scopusid6506131689tr_TR
dc.subject.scopusBoundary Layer Transition; Transition Model; Cascade Wind Tunnelsen_US
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