首页> 外文会议>International conference on computational and experimental methods in multiphase and complex flow >EXPANSION PROCESSES AND STRUCTURES OF TWO-PHASE FLOWS IN AERATED-LIQUID JETS DISCHARGED INTO A QUIESCENT ENVIRONMENT
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EXPANSION PROCESSES AND STRUCTURES OF TWO-PHASE FLOWS IN AERATED-LIQUID JETS DISCHARGED INTO A QUIESCENT ENVIRONMENT

机译:排放到环境中的充气液体射流中两相流的扩展过程和结构

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Expansion processes and near-field structures in the two-phase flow within an aerated-liquid jet injected into a quiescent environment were experimentally explored with the confocal x-ray fluorescence technique available at Argonne National Laboratory. Quantitative time-averaged liquid and gas density distributions within the aerated-liquid jet were spatially resolved simultaneously. For the present injection condition, the observation of a dome-shaped gas plume head and a high gas density gradient within a short distance from the nozzle exit clearly indicates that the initial gas expansion processes across the nozzle exit are highly similar to those within a typical under-expanded gaseous jet. With the assistance of compressible gas expansion near the nozzle exit, the liquid plume exhibits a plume width larger than that of the aerating gas plume, leading to a separation between liquid and gas plumes at the downstream location. Expansion of the gas plume creates a region of low gas density, followed by a region of gas density recovery in the near field. The low gas density region resembles the region with over-expanded gas in front of a Mach disk inside a typical under-expanded gaseous jet. The density variation within the low density region, however, is small, indicating a low level of over expansion and a weak Mach disk. The present analysis of Mach disk location within the discharged aerating gas plume shows that, while the location can be generally identified from gas density measurements, the use of correlations for location identification may be unreasonable, due to the lack of direct measurement data on characteristic pressures.
机译:使用可从Argonne国家实验室获得的共聚焦X射线荧光技术,对注入静态环境的充气液体射流中两相流中的膨胀过程和近场结构进行了实验研究。充气液体射流中的时间平均定量液体和气体密度分布在空间上同时得到解析。对于当前的喷射条件,在距喷嘴出口很近的距离内观察到圆顶状的气体羽状喷头和高气体密度梯度,清楚地表明,整个喷嘴出口处的初始气体膨胀过程与典型的气体膨胀过程高度相似。膨胀不足的气体射流。借助于在喷嘴出口附近的可压缩气体膨胀,液体羽流的羽流宽度大于充气的气体羽流的羽流宽度,从而导致下游位置的液体羽流和气体羽流分离。气体羽流的膨胀产生了低气体密度的区域,随后是近场中的气体密度恢复的区域。低气体密度区域类似于典型的膨胀不足的气态射流内部马赫盘前面的膨胀气体过多的区域。然而,在低密度区域内的密度变化很小,表明低水平的过度膨胀和较弱的马赫盘。目前对排出的充气气体羽流中马赫盘位置的分析表明,尽管通常可以通过气体密度测量来确定位置,但由于缺乏有关特征压力的直接测量数据,因此使用相关性进行位置识别可能是不合理的。

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