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Understanding Abrupt Leading Edge Separation as a Mechanism for the Onset of Dynamic Stall

机译:了解突然的前沿分离是动态失速发生的一种机制

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Large-eddy simulations of the dynamic stall process on a pitching NACA 0012 airfoil at Re_c = 1.0 x 10~6 have been performed. Using a constant-rate pitch-up maneuver it is shown that the onset of dynamic stall occurs due to bursting of a very small laminar separation bubble located near the airfoil leading edge. This bursting is initiated by direct interaction with the upstream propagation of the trailing edge turbulent boundary layer separation. Two vortex structures develop, the first from the bursting separation bubble and the second from the roll-up of the turbulent separation. These two vortex structures interact and then merge to form the dynamic stall vortex. A parametric study of pitching parameters is used to better understand the sensitivity of these interactions to airfoil motion. It is shown that the timing of dynamic stall onset is entirely dependent on the rate at which turbulent separation propagates upstream and the timing of the roll-up of the turbulent shear layer. The computations highlight the significant role the laminar separation bubble plays in the process despite its small size. Computations are also performed on the NACA 0009 airfoil to contrast against a case of standard pressure-gradient induced laminar separation bubble bursting without the presence of turbulent separation.
机译:对俯仰NACA 0012机翼在Re_c = 1.0 x 10〜6时进行了动态失速过程的大涡模拟。使用恒定速率的俯仰操纵,表明动态失速的发生是由于位于翼型前缘附近的非常小的层状分离气泡的破裂而发生的。该爆发是通过与后缘湍流边界层分离的上游传播的直接相互作用而引发的。形成两个涡流结构,第一个涡流结构来自破裂的分离气泡,第二个涡流结构来自湍流分离的卷起。这两个涡旋结构相互作用,然后合并以形成动态失速涡旋。对俯仰参数进行参数研究可更好地了解这些相互作用对机翼运动的敏感性。结果表明,动态失速开始的时间完全取决于湍流分离向上游传播的速度和湍流剪切层卷起的时间。这些计算突显了层流分离气泡尽管尺寸很小,但在过程中仍发挥着重要作用。还对NACA 0009机翼进行了计算,以与标准压力梯度引起的层流分离气泡破裂而没有湍流分离的情况形成对比。

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