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Effects of initial shear-layer thickness on turbulent subsonic jets at moderate Reynolds numbers

机译:初始剪切层厚度对中等雷诺数湍流亚音速射流的影响

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Large-Eddy Simulations of isothermal round jets at a Mach number of 0.9 are performed in order to investigate the influence of the nozzle-exit boundary-layer thickness on initially highly disturbed subsonic jets at moderate Reynolds numbers. The jets are originating from a pipe nozzle of radius r_0, and exhibit, at the exit section, peak disturbance levels of 9 per cent of the jet velocity, and mean velocity profiles similar to laminar boundary-layer profiles of thickness δ_0 = 0.09r_0, 0.15r_0, 0.25r_0 or 0.42r_0, yielding momentum thicknesses δ_θ(0) between 0.012r_0 and 0.05r_0. Four jets at a diameter Reynolds number Re_d = 5 × 10~4, providing momentum-thickness Reynolds numbers Reg = 304, 486, 782 and 1288 depending on δ_0, are first considered. Four jets at Reynolds numbers Re_D = 8.3 × 10~4, 5 × 10~4, 3 × 10~4 and 1.8 × 10~4, with δ_0 = 0.09r_0, 0.15r_0, 0.25r_0 and 0.42r_0, respectively, giving Re_θ ~ 480 in all cases, are then examined. The effects of δ_0/r_0 and Re_θ on the jet flow and sound fields can thus be distinguished. At a constant Re_D, thickening the initial shear layers mainly results in lower turbulence intensities in the mixing layers and weaker sound levels at all emission angles due to the variations of Re_θ. Different trends are therefore obtained at a nearly identical Re_θ. Increasing the ratio δ_0/r_0 in this case leads to a shorter potential core, higher centerline velocity fluctuations, and stronger noise in the downstream direction.
机译:执行马赫数为0.9的等温圆形喷射的大涡流模拟,以便在中度雷诺数时研究喷嘴出口边界层厚度对最初高度受到的亚音速喷射的影响。喷气机源自半径R_0的管道喷嘴,并在出口部分上展示,峰值干扰水平为射流速度的9%,平均速度分布类似于厚度Δ_0= 0.09R_0的层边界层轮廓, 0.15r_0,0.25r_0或0.42r_0,产生动量厚度Δ_θ(0)在0.012r_0和0.05r_0之间。直径雷诺数Re_d = 5×10〜4的四个喷射,首先考虑根据Δ_0的血管厚度雷诺数Reg = 304,486,782和1288,首先考虑。在Reynolds号码re_d = 8.3×10〜4,5×10〜4,3×10〜4和1.8×10〜4的喷射器,分别具有Δ_0= 0.09r_0,0.15r_0,0.25r_0和0.42r_0,给出re_θ 〜480在所有情况下,然后检查。因此可以区分Δ_0/ r_0和re_θ对喷射流和声场的影响。在恒定的RE_D处,初始剪切层的增厚主要导致混合层中的较低湍流强度,并且由于RE_θ的变化,在所有发射角处的声音较弱。因此,在几乎相同的RE_θ获得不同的趋势。在这种情况下增加比率Δ_0/ r_0导致较短的潜在核心,更高的中心线速度波动,以及下游方向的更强的噪声。

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