高超声速稀薄流中横向喷流干扰特性实验研究
EXPERIMENTAL STUDY ON THE CHARACTERIZATION OF TRANSVERSE JET INTERACTION IN HYPERSONIC RAREFIED FLOW
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摘要:喷流干扰是高超声速飞行高精度控制的一种有效手段, 研究者们以往大部分都主要集中于连续流条件下喷流干扰效应的机理研究, 并给出了喷流干扰流场的典型结构, 而稀薄流条件下喷流干扰特性的实验数据还十分匮乏. 本文利用JFX爆轰激波风洞产生高超声速稀薄自由流, 基于平板模型开展不同喷流压力和自由来流参数对横向喷流干扰特性影响的实验研究, 采用高速纹影成像及图像处理技术, 获得稀薄流条件下喷流干扰流场演化过程及流场结构的变化规律. 相比于无喷流条件形成的流场, 横向喷流与稀薄自由流相互作用形成的流场结构更为复杂, 喷流压力由于受到稀薄来流的扰动, 斜激波会短暂穿透喷流干扰流场并延伸至楔形体上部. 喷流干扰流场内桶状激波的影响范围随着喷流压力的升高而逐渐变宽, 位于三波点上游的斜激波空间位置不会随喷流压力的变化而改变, 而位于三波点下游的弓形激波则向上游移动, 当喷流压力过低时, 桶状激波不会与其他两种激波交汇形成三波点. 高超声速稀薄来流压力的降低同样会使桶状激波的影响范围变宽, 弓形激波同样也会向上游移动, 但基本不会对斜激波空间位置产生任何影响.Abstract:Jet interaction is an effective approach for hypersonic flight controls with higher agility and improved maneuverability. Previous researches are mainly focused on the mechanisms of jet interaction effects in continuous region, classical flowfield structures of jet interaction based on different models have been proposed theoretically, on the other hand, scarce experimental data on characterizations of jet interaction in rarefied region exist. Therefore, the objective of this work aims to experimentally investigate the effects of jet pressure and hypersonic rarefied flow condition on the characterizations of transverse jet interaction based on a flat plate model, whereas hypersonic rarefied flows are generated in a JFX detonation shock tunnel. Evolution and typical structure of transverse jet interaction in hypersonic rarefied flow are recorded using high-speed schlieren imaging approach, and variations of spatial positions of different shock waves are analyzed using imaging process technique. Compared to the flowfield without the presence of jet flow, the interaction between jet flow and hypersonic rarefied flow makes the flowfield much more complex. Oblique shock could instantaneously penetrate through the flowfield of jet interaction due to the pressure fluctuation of jet flow caused by the incoming flow. With increasing the jet pressure, the affecting region of the barrel shock gradually becomes broader. The spatial position of the oblique shock wave in the upstream of the triple point barely changes with an increase in the jet pressure, while in the downstream of the triple point, the bow shock moves upstream with increasing pressure. The spatial position of the barrel shock would not overlap with the other two when the jet pressure is low. The pressure reduction of the incoming hypersonic rarefied flow can broaden the affecting region of the barrel shock and thus move the bow shock upstream as well, but it has little influence on the spatial position of the oblique shock wave.