Temporally and spatially resolved X-ray densitometry in a shock tube

被引:0
|
作者
Shaik, R.A. [1 ]
Kastengren, A.L. [2 ]
Tranter, R.S. [3 ]
Lynch, P.T. [1 ]
机构
[1] Shaik, R.A.
[2] Kastengren, A.L.
[3] Tranter, R.S.
[4] Lynch, P.T.
来源
Lynch, P.T. (ptlynch@uic.edu) | 1600年 / Elsevier Inc.卷 / 224期
基金
美国国家科学基金会;
关键词
Shock tubes - Transmissions - X ray absorption spectroscopy - Boundary layer flow - Image reconstruction - Density of gases - Signal to noise ratio;
D O I
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中图分类号
学科分类号
摘要
Gas densities were measured by x-ray absorption spectroscopy to examine spatial inhomogeneity in density behind incident and reflected shock waves in a miniature (12.7 mm bore) high repetition rate shock tube. Shock waves were generated in argon. The pressure and temperature behind the incident shock were P2 ~ 1.72 bar and T2 ~ 800 K, while those behind the reflected shock were P5 ~ 6.5 bar and T5 ~ 1480 K. Time-resolved line-of-sight transmission measurements using x-rays at 9 keV photon energy were made along various axial and transverse locations covering the entire shock tube cross section. The x-ray transmission at each location was converted to pathlength-integrated densities, which in some conditions could be further converted to pathlength-averaged densities. The measured gas densities were compared with those calculated by the normal shock wave relations, and good agreement was found in the pre-shock and immediately behind the incident shock regions. Similar agreement was found for reflected shock conditions very near the endwall. However, increasingly large differences between the measured and calculated gas densities were found as distance from the endwall increased. Reconstruction by Abel inversion allowed time and radially resolved densities to be obtained from the transverse measurements. While the profiles measured in this experiment are of insufficient signal-to noise level and resolution to definitively assign boundary layer thicknesses, future improvements may be able to do this. The radially resolved densities reveal growing sidewall thermal boundary layers in gases behind the reflected shock. These reconstructions were compared with a model of the thermal boundary layer and are consistent with values of the thermal boundary layer thickness being between 0.25 mm and 1 mm at 0.7 ms after shock reflection. © 2020
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页码:136 / 149
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