Turbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency RegimesSource: ASME Journal of Heat and Mass Transfer:;2024:;volume( 146 ):;issue: 007::page 71802-1Author:Banerjee, Ayan Kumar
DOI: 10.1115/1.4064977Publisher: 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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contributor author | Banerjee, Ayan Kumar | |
date accessioned | 2024-04-24T22:29:38Z | |
date available | 2024-04-24T22:29:38Z | |
date copyright | 3/28/2024 12:00:00 AM | |
date issued | 2024 | |
identifier issn | 2832-8450 | |
identifier other | ht_146_07_071802.pdf | |
identifier uri | http://yetl.yabesh.ir/yetl1/handle/yetl/4295323 | |
description 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. | |
publisher | The American Society of Mechanical Engineers (ASME) | |
title | Turbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes | |
type | Journal Paper | |
journal volume | 146 | |
journal issue | 7 | |
journal title | ASME Journal of Heat and Mass Transfer | |
identifier doi | 10.1115/1.4064977 | |
journal fristpage | 71802-1 | |
journal lastpage | 71802-14 | |
page | 14 | |
tree | ASME Journal of Heat and Mass Transfer:;2024:;volume( 146 ):;issue: 007 | |
contenttype | Fulltext |