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首页> 外文期刊>International Journal of Heat and Fluid Flow >The effect of the Reynolds number on the velocity and temperature distributions of a turbulent condensing jet
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The effect of the Reynolds number on the velocity and temperature distributions of a turbulent condensing jet

机译:雷诺数对湍流冷凝射流速度和温度分布的影响

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摘要

In this study, we investigated the effect of the Reynolds number (Re) on the velocity and temperature distributions of a turbulent condensing jet from a long pipe nozzle. The Re of the condensing jet ranged from 78,000 to 170,000. Jet velocity was measured using a Phase Doppler Particle Analyzer (PDPA) system and temperature was measured with a K-type thermocouple. We used the effective radius to investigate the effect of Re on the velocity and temperature distributions and compared our results with previous results on air (single phases) jet. From the experimental results, it was found that distributions of velocity and temperature show a self-similarity state in the far-field. The condensation more occurred at low Re. Thus, from momentum conservation, the velocity decay rate decreases by 18.2% as the Re increases from 78,000 to 170,000. Compared to air jet issuing from the pipe nozzle, velocity of condensing jet decays more rapidly due to the condensation of water vapor. The velocity spread rate also falls by 8.1% as the Re increases from 78,000 to 170,000. The temperature decay rate decreases by 11.1% and temperature spread rate increases by 7.4% as the Re increases from 78,000 to 170,000 since jet entrainment decreases at higher Re. The latent heat was released at the condensing jet by condensation of vapor. Thus, the temperature decay rate of condensing jet is smaller than that of air jet while the temperature half width of condensing jet is larger than that of air jet. (C) 2017 Elsevier Inc. All rights reserved.
机译:在这项研究中,我们研究了雷诺数(Re)对长管喷嘴的湍流冷凝射流的速度和温度分布的影响。冷凝喷嘴的Re范围为78,000至170,000。使用相多普勒粒子分析仪(PDPA)系统测量射流速度,并使用K型热电偶测量温度。我们使用有效半径来研究Re对速度和温度分布的影响,并将我们的结果与以前的空气(单相)射流结果进行比较。从实验结果发现,速度和温度的分布在远场中显示出自相似状态。在低Re下更多地发生冷凝。因此,从动量守恒来看,随着Re从78,000增加到170,000,速度衰减率降低了18.2%。与从喷嘴喷出的空气相比,由于水蒸气的凝结,凝结射流的速度衰减得更快。随着Re从78,000增加到170,000,速度扩展率也下降了8.1%。当Re从78,000增加到170,000时,温度衰减率降低11.1%,温度扩展率增加7.4%,这是因为在Re较高时射流夹带减少。潜热通过蒸气的冷凝在冷凝喷嘴处释放。因此,冷凝射流的温度衰减率小于空气射流的温度衰减率,而冷凝射流的温度一半宽度大于空气射流的温度衰减率。 (C)2017 Elsevier Inc.保留所有权利。

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