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Simulation of Shock/Boundary-Layer Interactions with Bleed Using Immersed-Boundary Methods

机译:使用浸入边界方法模拟渗流与冲击/边界层的相互作用

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This work uses an immersed-boundary method to simulate the effects of arrays of discrete bleed holes in controlling shock-wave/turbulent-boundary-layer interactions. Both Reynolds-averaged Navier-Stokes and hybrid large-eddy/Reynolds-averaged Navier-Stokes turbulence closures are used with the immersed-boundary technique. The approach is validated by conducting simulations of Mach 2.5 flow over a perforated plate containing 18 individual bleed holes. Computed values of discharge coefficient as a function of bleed plenum pressure are compared to experimental data. Simulations of an impinging-oblique-shock/boundary-layer interaction at Mach 2.45 with and without bleed control are also performed. For the studies with bleed, two different bleed rates are employed. The 68 hole bleed plate is rendered as an immersed object in the computational domain. Wall pressure predictions show that, in general, the large-eddy/Reynolds-averaged Navier-Stokes technique underestimates the upstream extent of axial separation that occurs in the absence of bleed. Good agreement with pitot pressure surveys throughout the interaction region is obtained, however. Flow control at the maximum-bleed rate completely removes the separation region and induces local disturbances in the wall pressure distributions that are associated with the expansion of the boundary-layer fluid into the bleed port and its subsequent recompression. Computed pitot pressure distributions are in good agreement with experiment for the cases with bleed. Swirl-strength probability density distributions are used to estimate the evolution of turbulent length scales throughout the interaction. These, along with Reynolds-stress predictions, indicate that an effect of strong bleed rates is to accelerate the recovery of the boundary layer toward a new equilibrium state downstream of the interaction region.
机译:这项工作使用沉浸边界方法来模拟离散泄放孔阵列在控制冲击波/湍流边界层相互作用中的作用。雷诺平均纳维-斯托克斯和混合大涡/雷诺平均纳维-斯托克斯湍流闭塞都与沉浸边界技术一起使用。该方法通过在包含18个单独排放孔的多孔板上进行的2.5马赫流动仿真得到验证。将排放系数作为放气压力的函数的计算值与实验数据进行比较。还对在有和没有渗出控制的情况下在2.45马赫时的撞击斜向冲击/边界层相互作用进行了模拟。对于有出血的研究,采用两种不同的出血速率。 68孔放气板在计算域中被渲染为沉浸对象。壁面压力预测表明,通常,大涡流/雷诺平均Navier-Stokes技术会低估在没有渗漏的情况下发生的轴向分离的上游程度。但是,在整个交互作用区域都获得了皮托管压力测量的良好一致性。以最大排放速率进行流量控制会完全去除分离区域,并在壁压力分布中引起局部扰动,这些扰动与边界层流体向排出口的膨胀及其随后的再压缩有关。计算的皮托管压力分布与出血病例的实验结果非常吻合。旋流强度概率密度分布用于估计整个相互作用过程中湍流长度尺度的演变。这些以及雷诺应力预测表明,强渗出率的作用是促进边界层向相互作用区域下游的新平衡态恢复。

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