{"title":"准稳定和低频状态下的湍流脉动对流","authors":"Ayan Banerjee","doi":"10.1115/1.4064977","DOIUrl":null,"url":null,"abstract":"\n The instantaneous and time-averaged dynamics of turbulent pulsating convective pipe flow is investigated experimentally over Strohoul 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=7528−10920. Analytical expressions for pulsation amplitudes of centerline velocity, bulk velocity and Nusselt number are derived. The time series of fluctuating components of centerline velocity (Uc̃), cross-sectionally averaged bulk velocity (Ub̃) and Nusselt number (Nũ) depics that the phase differences between Uc̃, and Ub̃, and between Ub̃, and Nũ increase with St non-monotically 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.","PeriodicalId":505153,"journal":{"name":"ASME Journal of Heat and Mass Transfer","volume":" 593","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Turbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes\",\"authors\":\"Ayan Banerjee\",\"doi\":\"10.1115/1.4064977\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"\\n The instantaneous and time-averaged dynamics of turbulent pulsating convective pipe flow is investigated experimentally over Strohoul 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=7528−10920. Analytical expressions for pulsation amplitudes of centerline velocity, bulk velocity and Nusselt number are derived. The time series of fluctuating components of centerline velocity (Uc̃), cross-sectionally averaged bulk velocity (Ub̃) and Nusselt number (Nũ) depics that the phase differences between Uc̃, and Ub̃, and between Ub̃, and Nũ increase with St non-monotically 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.\",\"PeriodicalId\":505153,\"journal\":{\"name\":\"ASME Journal of Heat and Mass Transfer\",\"volume\":\" 593\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-03-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ASME Journal of Heat and Mass Transfer\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1115/1.4064977\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ASME Journal of Heat and Mass Transfer","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1115/1.4064977","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Turbulent Pulsating Convective Flow in the Quasi-Steady and Low-Frequency Regimes
The instantaneous and time-averaged dynamics of turbulent pulsating convective pipe flow is investigated experimentally over Strohoul 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=7528−10920. Analytical expressions for pulsation amplitudes of centerline velocity, bulk velocity and Nusselt number are derived. The time series of fluctuating components of centerline velocity (Uc̃), cross-sectionally averaged bulk velocity (Ub̃) and Nusselt number (Nũ) depics that the phase differences between Uc̃, and Ub̃, and between Ub̃, and Nũ increase with St non-monotically 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.