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The Role of Boundary-Layer Thickness on Cylinder- Generated Shock-Wave/Turbulent Boundary-Layer Interactions, Part I: Computations

机译:边界层厚度在圆柱产生的冲击波/湍流边界层相互作用中的作用,第一部分:计算

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Scaling parameters of a shock-wave/turbulent boundary-layer interaction generated by a semi-infinite standing cylinder were explored using steady-state RANS simulations. The simulations were performed in collaboration with an experimental study (see Part II) conducted at Mach 2.0. By maintaining constant Mach and Reynolds numbers, only the primary variable d, the cylinder diameter, and the secondary variable S, the boundary-layer thickness, were varied. The ratio of d/δ was varied from 0.125-16 via a constant set of d and δ to provide a broad range of values. A power law dependence on d/δ was observed for separation distance and triple-point height, which was verified by the experimental study and aligned with data from the literature. The impact of viscous effects on the shock orientation and interaction strength was found to increase in importance as the shock generator approached the scale of the boundary-layer thickness; conversely, for values of d/δ ≥ 6, the curvature and strength of the lambda-shock structure became seemingly independent of d/δ. Additionally, the viscous impact was observed for separation distance and triple-point height, where it correlated with a larger interaction scale, as well as a reduced peak pressure ratio on the floor upstream of the cylinder. The peak pressure ratio on the cylinder leading edge, however, only exhibited a dependence on d/δ for values less than 0.5. All cases exhibited a trough pressure ratio on the cylinder leading edge at y/d = 0.3, corresponding to a separation line of a secondary vortex. It appeared that this parameter was not a function of S.
机译:利用稳态RANS模拟,探索了由半无限立柱产生的激波/湍流边界层相互作用的尺度参数。与在2.0马赫数下进行的实验研究(参见第二部分)合作进行了仿真。通过保持恒定的马赫数和雷诺数,只有主要变量d(圆柱直径)和次要变量S(边界层厚度)发生变化。 d /δ之比通过恒定的d和δ值在0.125-16之间变化,以提供宽范围的值。观察到分离距离和三点高度的幂定律依赖于d /δ,这已通过实验研究得到验证,并与文献数据相符。随着冲击发生器接近边界层厚度的尺度,发现粘性效应对冲击取向和相互作用强度的影响越来越重要。相反,对于d /δ≥6的值,λ冲击结构的曲率和强度似乎与d /δ无关。此外,在分离距离和三点高度处观察到了粘性冲击,这与较大的相互作用尺度以及气缸上游底板上的峰值压力比降低相关。然而,气缸前缘上的峰值压力比仅对d /δ表示小于0.5的值。在所有情况下,气缸前缘处的谷底压力比为y / d = 0.3,与次级涡旋的分离线相对应。看来此参数不是S的函数。

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