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arXiv 1608.07928physics.flu-dyn
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轴对称边界层的整体稳定性分析

Global stability analysis of axisymmetric boundary layers

N. Vinod, Ramesh Bhoraniya

摘要:

本文对不可压圆柱轴对称边界层的线性整体稳定性进行了分析。在入口处,底部流动平行于圆柱的轴线。沿流向的压力梯度为零。基本流速剖面在性质上是完全不平行和不相似的。边界层在空间方向上连续增长。在圆柱极坐标系下,推导了扰动流量的线性化Navier-Stokes(LNS)方程。LNS方程与齐次边界条件一起构成广义特征值问题。由于基流是轴对称的,扰动在方位角方向上是周期性的。用Chebyshev谱配置法和Arnoldi迭代法求解一般特征值问题。计算了雷诺数范围和不同方位波数下的全球时间模式。计算的本征模的最大虚部是负的,因此流动是暂时稳定的。本征模的空间结构表明,流动是对流不稳定的,因为扰动振幅的大小和幅度增长时,向下游移动。在低雷诺数下,轴对称边界层的整体模态比二维平板边界层的整体模态稳定。然而,在高雷诺数下,它们接近于二维平板边界层。因此,在低雷诺数下,横向曲率的阻尼效应是显著的。的波动性质的扰动被发现最不稳定的本征模。

英文摘要:

This paper presents the linear global stability analysis of the incompressible axisymmetric boundary layer on a circular cylinder. The base flow is parallel to the axis of the cylinder at inlet. The pressure gradient is zero in the streamwise direction. The base flow velocity profile is fully non-parallel and non-similar in nature. The boundary layer grows continuously in the spatial directions. Linearized Navier-Stokes(LNS) equations are derived for the disturbance flow quantities in the cylindrical polar coordinates. The LNS equations along with homogeneous boundary conditions forms a generalized eigenvalues problem. Since the base flow is axisymmetric, the disturbances are periodic in azimuthal direction. Chebyshev spectral collocation method and Arnoldi's iterative algorithm is used for the solution of the general eigenvalues problem. The global temporal modes are computed for the range of Reynolds numbers and different azimuthal wave numbers. The largest imaginary part of the computed eigenmodes are negative and hence the flow is temporally stable. The spatial structure of the eigenmodes shows that the flow is convectively unstable because the disturbance amplitudes grow in size and magnitude when moving towards downstream. The global modes of axisymmetric boundary layer are more stable than that of 2D flat plate boundary layer at low Reynolds number. However, at high Reynolds number they approaches to 2D flat plate boundary layer. Thus, the damping effect of transverse curvature is significant at low Reynolds number. The wave-like nature of the disturbances is found for most unstable eigenmodes.

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