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Large-eddy simulation of underexpanded round jets impinging on a flat plate 4 to 9 radii downstream from the nozzle

机译:扩管后的圆形射流撞击喷嘴下游4至9半径的大涡模拟

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Supersonic round jets have been computed by compressible Large Eddy Simulation (LES) using low-dispersion and low-dissipation schemes. The jets are underexpanded, and are characterized by a Nozzle Pressure Ratio of NPR = P_r/P_(amb) = 4.03, where P_r is the stagnation pressure and P_(amb) is the ambient pressure. They have a fully expanded Mach number of M_j = 1.56, an exit Mach number of M_e = 1, and a Reynolds number of Re_j = u_jD/v = 5 × 10~4, where u_e and D are the jet exit velocity and the nozzle diameter, respectively. A free jet is first considered. Four jets impinging on a flat plate normally are then examined. The distance L between the nozzle lip and the flat plate varies from L = 4.16r_0 up to L = 9.32r_0 where r_0 = D/2, for the impinging jets. The effects of the plate on the aerodynamic and acoustic properties of the jets are thus studied. For the free jet, snapshots of density, pressure and vorticity are presented. Mean velocity fields are displayed, they are in good agreement with experimental data. The near pressure field of the jet is investigated using Fourier decomposition. A screech tone component is found, at a frequency comparing well with experimental data and theoretical models. For the four impinging jets, similarly, flow snapshots and mean flow fields are shown. The results obtained are similar to the corresponding measurements. The convection velocity of large-scale structures in the jet shear layers is then evaluated and an expression giving the average convection velocity between the nozzle lips and the flat plate is proposed. The near pressure fields are then explored, and the main properties of the aeroacoustic feedback mechanism occurring between the nozzle lip and the flat plate are presented. The results are consistent with theoretical models and experimental data.
机译:超音速圆形射流已经通过可压缩的大涡模拟(LES)使用低分散和低耗散方案进行了计算。射流未充分膨胀,其特征是喷嘴压力比NPR = P_r / P_(amb)= 4.03,其中P_r是停滞压力,P_(amb)是环境压力。它们具有完全扩展的马赫数M_j = 1.56,出口马赫数M_e = 1和雷诺数Re_j = u_jD / v = 5×10〜4,其中u_e和D是射流出口速度和喷嘴直径分别。首先考虑免费喷气式飞机。然后检查通常撞击在平板上的四个喷嘴。喷嘴唇和平板之间的距离L从L = 4.16r_0到L = 9.32r_0,其中r_0 = D / 2(对于撞击射流)不等。因此,研究了板对射流的空气动力学和声学特性的影响。对于自由射流,给出了密度,压力和涡度的快照。显示了平均速度场,它们与实验数据非常吻合。使用傅里叶分解研究射流的近压力场。发现刺耳的音调成分,其频率与实验数据和理论模型很好地比较。对于四个撞击射流,类似地显示了流量快照和平均流场。获得的结果与相应的测量结果相似。然后评估射流剪切层中大型结构的对流速度,并提出了给出喷嘴唇口和平板之间平均对流速度的表达式。然后探索附近​​的压力场,并给出了在喷嘴唇和平板之间出现的空气声反馈机制的主要特性。结果与理论模型和实验数据一致。

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