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dc.contributor.authorBanerjee, Ayan Kumar
dc.date.accessioned2024-04-24T22:29:38Z
dc.date.available2024-04-24T22:29:38Z
dc.date.copyright3/28/2024 12:00:00 AM
dc.date.issued2024
dc.identifier.issn2832-8450
dc.identifier.otherht_146_07_071802.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4295323
dc.description.abstractThe instantaneous and time-averaged dynamics of turbulent pulsating convective pipe flow is investigated experimentally over Strouhal number, St=3.3×10−4−0.12 that falls in the quasi-steady and low-frequency regimes, pulsation amplitude, βb=0.05−0.2, and bulk Reynolds numbers, Reb=7528−10,920. The analytical expressions for pulsation amplitudes of centerline velocity, bulk velocity, and Nusselt number are derived. The time series of oscillating components of centerline velocity (Uc˜), cross-sectionally averaged bulk velocity (Ub˜), and Nusselt number (Nu˜) depicts that the phase differences between Uc˜, and Ub˜, and between Ub˜, and Nu˜ increase with St nonmonotonically with near zero phase difference at St→0. The time-averaged pulsating Nusselt number Nu¯ is invariant of St for St > 0.01. Nu¯ depends marginally on βb. The relative mean Nusselt number, Nur=Nu¯/Nus<1 for Reb≥8885 and Nur>1 for Reb = 7528. The general observations from this study is that, in the quasi-steady and low-frequency regimes, turbulent pulsating flows leads to marginal changes in the time-averaged Nusselt number Nu¯ compared to the time-averaged Nusselt number Nus in steady flow condition at any Reb.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleTurbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes
dc.typeJournal Paper
dc.journal.volume146
dc.journal.issue7
dc.journal.titleASME Journal of Heat and Mass Transfer
dc.identifier.doi10.1115/1.4064977
dc.journal.fristpage71802-1
dc.journal.lastpage71802-14
dc.page14
dc.treeASME Journal of Heat and Mass Transfer:;2024:;volume( 146 ):;issue: 007
dc.contenttypeFulltext


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