Please use this identifier to cite or link to this item: http://cmuir.cmu.ac.th/jspui/handle/6653943832/62974
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dc.contributor.authorSudarat Srichanen_US
dc.contributor.authorWannarat Rakpakdeeen_US
dc.contributor.authorTanongkiat Kiatsiriroaten_US
dc.contributor.authorWeerachai Chaiworapueken_US
dc.date.accessioned2018-12-14T03:56:52Z-
dc.date.available2018-12-14T03:56:52Z-
dc.date.issued2018-01-01en_US
dc.identifier.issn15210480en_US
dc.identifier.issn08916152en_US
dc.identifier.other2-s2.0-85057347683en_US
dc.identifier.other10.1080/08916152.2018.1545806en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85057347683&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/62974-
dc.description.abstract© 2018, © 2018 Taylor & Francis. This study presents the thermal behavior of two young turbulent spots merging into a longitudinal direction on an isothermal flat plate for the local Reynolds number between 6.1 × 104 and 1.3 × 105 in a low freestream turbulence water tunnel having a turbulent intensity of 1.16%. The two turbulent spots are generated by water injection through a 1-mm-diameter hole in the perpendicular direction of the mainstream flow with a dimensionless separating time (Δτ) of 42.08, 84.16, and 126.24. Thermochromic liquid crystals are utilized mutually with an image processing technique to extract the spot characteristics qualitatively and quantitatively. The results demonstrate that the following turbulent spot directly causes an increase in the local Nusselt number and heat rate within the footprint of the merging spots. The relatively highest increase in this study occurs when Δτ = 84.16. The average Nusselt number and effectiveness characterize differently in the intersection zone, non-intersection zone of the leading spot, and non-intersection zone of the following spot. The results confirm that turbulent spots under the boundary layer transition augment the heat transfer rate to the level of full turbulence by not only their spot maturity but also the merging mechanism. Finally, the heat transfer mechanism is discussed and the predictive formulas for the Nusselt number and heat flux of the longitudinal merging of turbulent spots for Δτ from 0 to 126.24 are provided.en_US
dc.subjectEngineeringen_US
dc.subjectPhysics and Astronomyen_US
dc.titleThermal characterization of longitudinal merging of turbulent spotsen_US
dc.typeJournalen_US
article.title.sourcetitleExperimental Heat Transferen_US
article.stream.affiliationsKasetsart Universityen_US
article.stream.affiliationsChiang Mai Universityen_US
Appears in Collections:CMUL: Journal Articles

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