EXPANSION PROCESSES AND STRUCTURES OF TWO-PHASE FLOWS IN AERATED-LIQUID JETS DISCHARGED INTO A QUIESCENT ENVIRONMENT

Kuo-Cheng Lin, A. Kastengren, C. Carter
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Abstract

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.
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静态环境下加气液体射流中两相流的膨胀过程和结构
利用阿贡国家实验室的共聚焦x射线荧光技术,对注入静息环境的加气液体射流内两相流的膨胀过程和近场结构进行了实验探索。同时对加气液体射流内定量的时间平均液气密度分布进行了空间解析。在目前的喷射条件下,在喷管出口近距离内观察到的圆顶状气体羽头和高气体密度梯度清楚地表明,喷管出口的初始气体膨胀过程与典型的欠膨胀气体射流中的初始气体膨胀过程非常相似。在喷嘴出口处可压缩气体膨胀的帮助下,液体羽流的羽流宽度大于充气气体羽流,导致下游位置的液、气羽分离。气体羽流的膨胀产生了一个低气体密度区域,随后在近场产生了一个气体密度恢复区域。低气体密度区域类似于典型的欠膨胀气体射流中马赫数盘前的过度膨胀气体区域。而低密度区内的密度变化较小,表明过膨胀程度较低,马赫盘较弱。本文对排气气羽内马赫盘位置的分析表明,虽然可以通过气体密度测量来确定位置,但由于缺乏特征压力的直接测量数据,使用相关性进行位置识别可能是不合理的。
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