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Length scale for the estimation of buzz frequency in the limit of high mechanical blockage in mixed-compression intakes

机译:混合压缩摄入量高机械堵塞极限估计嗡嗡声估计的长度

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Oscillatory flow features are common in the unstart of hypersonic mixed-compression intakes and can be classified as low-amplitude or high-amplitude oscillatory unstarted flows. The low-amplitude oscillatory unstarted flow is driven by the shear layer from shock interactions ahead of the cowl, while the high-amplitude oscillatory unstarted flow is driven by the separation caused by shock-boundary-layer interaction on the ramp. While previous studies have observed these flow features and reported their associated frequency, there is no simple criterion available for predicting which mode will occur, and there is a lack of consensus on the appropriate frequency scaling parameter. We study a mixed-compression hypersonic intake in a hypersonic wind tunnel by varying the internal contraction ratio and the throttling ratio to observe various kinds of unstart regimes. Two significant conclusions emerge from considering the results for high-throttling-ratio conditions (TR > 0.55) from the current as well as previous studies. Firstly, the actual shock-on-lip condition at the cowl corresponding to the unthrottled condition, as observed from schlieren images, demarcates the boundary between the two modes of oscillatory unstart flows upon throttling. Secondly, a suitable length scale (l*), defined as the extent of the subsonic region in the unstarted flow (as observed from the experimental schlieren images), gives the appropriate frequency scaling parameter (f * = a(0)/4l* where a(0) is the stagnation acoustic speed).
机译:振荡流动特征在高超声速混合压缩进气道的非起动中很常见,可分为低振幅或高振幅振荡非起动流动。低振幅振荡未启动流由前罩激波相互作用产生的剪切层驱动,而高振幅振荡未启动流由斜坡激波边界层相互作用产生的分离驱动。虽然之前的研究已经观察到了这些流动特征,并报告了它们的相关频率,但没有简单的标准可用于预测将出现哪种模式,并且对适当的频率标度参数缺乏共识。在高超声速风洞中,我们通过改变内部收缩比和节流比来研究混合压缩高超声速进气道,以观察各种非起动状态。从当前和以前的研究中,考虑到高节流比条件(TR>0.55)的结果,得出了两个重要结论。首先,根据纹影图像观察到的与无节流条件对应的整流罩唇部条件下的实际冲击,划分了节流时两种振荡非起动流动模式之间的边界。其次,一个合适的长度标度(l*)定义为未开始流动中亚音速区域的范围(从实验纹影图像中观察到),给出了合适的频率标度参数(f*=a(0)/4l*,其中a(0)是停滞声速)。

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