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    Turbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes

    Source: ASME Journal of Heat and Mass Transfer:;2024:;volume( 146 ):;issue: 007::page 71802-1
    Author:
    Banerjee, Ayan Kumar
    DOI: 10.1115/1.4064977
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The 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.
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      Turbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes

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    contributor authorBanerjee, Ayan Kumar
    date accessioned2024-04-24T22:29:38Z
    date available2024-04-24T22:29:38Z
    date copyright3/28/2024 12:00:00 AM
    date issued2024
    identifier issn2832-8450
    identifier otherht_146_07_071802.pdf
    identifier urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4295323
    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.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleTurbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes
    typeJournal Paper
    journal volume146
    journal issue7
    journal titleASME Journal of Heat and Mass Transfer
    identifier doi10.1115/1.4064977
    journal fristpage71802-1
    journal lastpage71802-14
    page14
    treeASME Journal of Heat and Mass Transfer:;2024:;volume( 146 ):;issue: 007
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
    yabeshDSpacePersian