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arXiv 2010.08577physics.flu-dyn
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强压力梯度湍流边界层的直接数值模拟

Direct Numerical Simulation of a Turbulent Boundary Layer with Strong Pressure Gradients

Riccardo Balin, Kenneth E. Jansen

摘要:

采用不可压纳维-斯托克斯方程的直接数值模拟(DNS)方法,计算了高斯型凸块上的湍流边界层。二维的碰撞导致一系列快速连续交替的强压力梯度。在流入处,动量厚度雷诺数约为1,000,边界层厚度为凸起高度的1/8。DNS结果表明,强有利压力梯度(FPG)使边界层进入再层化过程。近壁湍流明显减弱,并成为间歇性的,但再层化没有完成。流向速度分布偏离标准对数律,雷诺切应力减小。强加速度也抑制壁面剪切归一化湍流动能产生率。在碰撞峰值,FPG切换到逆梯度(APG),近壁湍流突然增强,通过一个部分的再转变过程。这导致了新的高能量内层,其对强APG更具弹性,并且仅在下游侧产生初始流动分离。在强FPG和APG区域中,内层和外层在很大程度上变得彼此独立。近壁区域响应于压力梯度并确定表面摩擦。外层的行为类似于自由剪切层的压力梯度和平均流线曲率的影响。从RANS模拟的凸点的结果也进行了讨论,清楚地表明缺乏预测能力的近壁压力梯度的平均流量的影响。

英文摘要:

The turbulent boundary layer over a Gaussian shaped bump is computed by direct numerical simulation (DNS) of the incompressible Navier-Stokes equations. The two-dimensional bump causes a series of strong pressure gradients alternating in rapid succession. At the inflow, the momentum thickness Reynolds number is approximately 1,000 and the boundary layer thickness is 1/8 of the bump height. DNS results show that the strong favorable pressure gradient (FPG) causes the boundary layer to enter a relaminarization process. The near-wall turbulence is significantly weakened and becomes intermittent, however relaminarization does not complete. The streamwise velocity profiles deviate above the standard logarithmic law and the Reynolds shear stress is reduced. The strong acceleration also suppresses the wall-shear normalized turbulent kinetic energy production rate. At the bump peak, where the FPG switches to an adverse gradient (APG), the near-wall turbulence is suddenly enhanced through a partial retransition process. This results in a new highly energized internal layer which is more resilient to the strong APG and only produces incipient flow separation on the downstream side. In the strong FPG and APG regions, the inner and outer layers become largely independent of each other. The near-wall region responds to the pressure gradients and determines the skin friction. The outer layer behaves similarly to a free-shear layer subject to pressure gradients and mean streamline curvature effects. Results from a RANS simulation of the bump are also discussed and clearly show the lack of predictive capacity of the near-wall pressure gradient effects on the mean flow.

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