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

Ayan Banerjee
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Abstract

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.
准稳定和低频状态下的湍流脉动对流
通过实验研究了湍流脉动对流管道流的瞬时和时间平均动力学特性,包括斯特罗霍尔数(St=3.3×10-4-0.12,处于准稳态和低频状态)、脉动振幅(βb=0.05-0.2)和体积雷诺数(Reb=7528-10920)。得出了中心线速度、体积速度和努塞尔特数的脉动振幅的分析表达式。中心线速度(Uc̃)、横截面平均体积速度(Ub̃)和努塞尔特数(Nũ)波动分量的时间序列表明,Uc̃和 Ub̃之间以及 Ub̃和 Nũ 之间的相位差随 St 的增加而非单调增加,在 St→0 时相位差接近零。当 St > 0.01 时,时均脉动努塞尔特数 Nu¯ 与 St 无关。Nu¯ 与 βb 关系不大。相对平均努塞尔特数 Nur=Nu¯/Nus1 为 Reb = 7528。本研究得出的一般结论是,在准稳态和低频状态下,湍流脉动流导致的时均努塞尔特数 Nu¯ 与任意 Reb 条件下稳定流状态下的时均努塞尔特数 Nus 相比变化很小。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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