液态金属非稳定分层混合对流的湍流输运研究
STUDY ON TURBULENT TRANSPORT IN MIXED CONVECTION WITH UNSTABLE STRATIFICATION FOR LIQUID METALS
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摘要: 液态金属低普朗特数流体的强热扩散性质使传统雷诺比拟理论失效, 依据常规工质流体得出的湍流流动传热模型将不能直接应用于液态金属的湍流输运研究. 流体密度差与重力引起的浮升力效应使得液态金属在湍流动量与能量输运方面具有更加复杂的现象与机理. 本研究基于高阶谱元法开展液态金属在水平槽道内湍流非稳定分层混合对流的隐式大涡模拟研究. 计算对象是普朗特数为Pr = 0.025的液态金属工质. 计算工况的最高名义摩擦雷诺数为Re_\tau ,N = 1020以满足工程应用需求, 理查德森数范围在Ri = 0\sim 10以覆盖强迫对流及强浮升力混合对流工况. 研究结果表明浮升力诱导的大尺度准流向涡卷结构对液态金属非稳定分层混合对流的湍流动量与能量输运起主导作用, 该大尺度结构使近壁瞬时流场出现明显的聚并与间歇行为. 一维流向协谱表明强浮升力非稳定分层混合对流的近壁湍流动量与能量在低波数区间分别呈现 - 1 \mathord\left/ \vphantom - 1 5 \right. 5与 - 1 \mathord\left/ \vphantom - 1 2 \right. 2幂律标度, 而湍流能量在槽道中心呈现明显的 - 7 \mathord\left/ \vphantom - 7 3 \right. 3幂律标度. 相比于强迫对流, 浮升力增强了近壁湍流各向异性并加快了槽道中心不同尺度间湍流能量的输运过程. 雷诺切应力与壁面法向湍流热流密度守恒输运方程的结果表明, 强浮升力条件下压力脉动相关项主导近壁湍流动量的生成与损失, 湍流能量的脉动输运与温度-压力梯度关联输运在湍流外区受浮升力影响而显著增强. 湍流非稳定分层混合对流工况下, 湍流外区湍流普朗特数和全局平均湍流普朗特数主要受理查德森数影响. 依据计算数据, 新提出两种实用的湍流普朗特数唯象模型并标定了经验参数. 湍流普朗特数的逐项预乘谱分析结果表明浮升力诱导的大尺度准流向涡卷结构对湍流动量与能量输运的典型流向波长为8h, 其中h为槽道半高度. 非稳定分层混合对流工况下湍流普朗特数分子项预乘谱在流向波长为8h的负峰值表明湍流普朗特数在湍流外区的降低不仅与湍流传热作用增强有关, 还有浮升力诱导大尺度湍流结构对湍流动量输运的调制作用.Abstract: The strong thermal diffusivity of low Prandtl number liquid metals makes traditional Reynolds analogy invalidity, and the models concluded from regular fluids are not directly applicable to turbulent transport of liquid metals. The buoyant effect induced by density difference and gravity makes more complex behaviors and mechanisms of turbulent momentum and energy transfer for liquid metals. In this study we conduct the implicit large-eddy simulation of mixed convection with unstable stratification in a horizontal channel for liquid metals based on high-order spectral element method. The Prandtl number is fixed at Pr = 0.025. The nominal friction Reynolds number is up to Re_\tau ,N = 1020 for engineering practical use, and the range of Richardson number is Ri = 0\sim 10 to cover the forced convection and mixed convection with strong buoyancy. The results indicate that buoyancy induced large-scale quasi-streamwise rollers play the dominant role on turbulent momentum and energy transports in mixed convection for liquid metals, and the large-scale structures make the instantaneous flow fields in near wall region show obvious coalescence and intermittency. The one-dimensional streamwise co-spectra show that under mixed convection condition, the turbulent momentum and energy transfer in low wavenumber range are observed with - 1 \mathord\left/ \vphantom - 1 5 \right. 5 and - 1 \mathord\left/ \vphantom - 1 2 \right. 2 power-law scaling at wall vicinity, respectively. The turbulent energy transfer at channel center is observed with - 7 \mathord\left/ \vphantom - 7 3 \right. 3 power-law scaling in mixed convection. Compare to forced convection, buoyancy enhances turbulence anisotropy at wall vicinity and accelerates the turbulent energy transfer rates between different turbulence scales at channel center. The transport equations of Reynolds shear stress and wall-normal turbulent heat flux show that under strong buoyancy conditions, the pressure-related terms dominate the gain and loss of turbulent momentum in near wall region, while the turbulence transport and temperature-pressure gradient terms are remarkably enhanced by buoyancy in turbulence outer region. The turbulent Prandtl number in turbulence outer region and global average turbulent Prandtl number are mainly controlled by Richardson number in mixed convection with unstable stratification. New phenomenological models for turbulent Prandtl number are proposed and the empirical constants are calibrated. The spectral analysis of each term in turbulent Prandtl number shows that the typical wavelength of buoyancy induced large-scale quasi-streamwise rollers for turbulent momentum and energy is 8h, where h is channel half-height. The negative peak at streamwise wavelength 8h in premultiplied spectra of numerator term means that the decrease of turbulent Prandtl number in outer region not only caused by enhancement of turbulent heat transfer, but also worked by the modulation of turbulent momentum transport by buoyancy induced large-scale structures.
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