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首页> 外文期刊>JSME International Journal. Series B, Fluids and Thermal Engineering >Spanwise Variation of Turbulent Flowfield for the Turbulent Boundary Layer Interacting with Controlled Longitudinal Vortex Arrays
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Spanwise Variation of Turbulent Flowfield for the Turbulent Boundary Layer Interacting with Controlled Longitudinal Vortex Arrays

机译:与受控纵向涡流阵列相互作用的湍流边界层的湍流场跨度变化

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摘要

A vortical structure within a turbulent boundary layer and spanwise variation of turbulent flowfield have been investigated for further understanding of the development of the turbulent boundary layer interacting with the spanwise periodic longitudinal vortex arrays which are artificially generated in a free stream. One of the parameters, spanwise periodicity of longitudinal vortices L/S (L denotes the spanwise distance between neighboring airfoils, S the airfoil span), rules both magnitude and streamwise path of secondary vortices caused within the turbulent boundary layer. As a result, whether the turbulent quantities show linear or nonlinear interaction significantly depends on the value of L/S. Therefore, in cases where L/S < 1, although the spanwise distortion of turbulent quantities in the outer region is not marked, those spanwise periods change in the streamwise direction due to the rapid vortex diffusion following corotating merging vortices. However, in cases where L/S approx>1, turbulent quantities show a noticeable spanwise periodic variation corresponding to the arrangement of airfoil elements, and these spanwise periods are strictly maintained. Comparing the spanwise variations of the turbulent flowfield with those of the mean flowfield, mechanisms of spanwise variation of the turbulent boundary layer are discussed.
机译:为了进一步理解湍流边界层与在自由流中人工产生的翼展方向周期性纵向涡流阵列相互作用的湍流边界层的发展,已经研究了湍流边界层内的涡流结构和湍流流场的展向变化。参数之一,纵向涡旋的翼展方向周期性L / S(L表示相邻翼型之间的翼展方向距离,S为翼型翼展),可控制在湍流边界层内引起的次级涡旋的大小和流向路径。结果,湍流量显示线性还是非线性相互作用很大程度上取决于L / S的值。因此,在L / S <1的情况下,虽然外部区域中的湍流量的翼展方向畸变没有被显着,但是由于在合并旋转的涡旋后伴随着快速的涡流扩散,翼展方向周期在流向变化。但是,在L / S大约> 1的情况下,湍流量显示出与翼型元件的布置相对应的明显的翼展方向周期性变化,并且严格保持了这些翼展方向周期。将湍流场的展向变化与平均流场进行比较,讨论了湍流边界层展向变化的机理。

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