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首页> 外文期刊>Journal of Fluid Science and Technology >Laminar-Turbulent Transition of an Inlet Boundary Layer in a Circular Pipe Induced by Periodic Injection (Shape of Isolated Turbulent Patches and Their Growth)
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Laminar-Turbulent Transition of an Inlet Boundary Layer in a Circular Pipe Induced by Periodic Injection (Shape of Isolated Turbulent Patches and Their Growth)

机译:周期性注入引起的圆形管道入口边界层的层流湍流过渡(孤立的湍流斑块的形状及其生长)

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The laminar-turbulent transition of a boundary layer induced by a jet injection in the inlet region of a circular pipe was experimentally investigated. The jet was periodically injected radially from a small hole in the inlet region into the pipe flow. Axial velocity was measured by a hot-wire anemometer. The turbulence induced by the jet within the boundary layer developed into turbulent patches which then grew in the axial, circumferential and radial directions downstream. The shape of the patches shown by the intermittency factor in the diametrical plane was similar to the turbulent spot in the flat plate boundary layer at first, then became similar to the turbulent slug in the pipe flow developed downstream. The turbulent patches protruded from the boundary layer after they grew and reached the circumferential opposite side, although they stayed within the boundary layer as long as the shape was turbulent spot-like in the diametrical plane. The propagation velocity at the leading edge became faster than the cross-sectional velocity, though it turned slower at the trailing edge. Therefore, the growth rate of its axial length varied downstream. The growth rate of the patches' circumferential length was smaller than that in the turbulent spot under zero pressure gradient and was almost the same as the spot under favorable pressure gradient.
机译:实验研究了在圆形管的入口区域中由喷射注入引起的边界层的层流湍流转变。射流从进口区域的一个小孔周期性地径向注入到管道流中。轴向速度通过热线风速仪测量。由边界层内的射流引起的湍流发展成湍流斑块,然后在下游的轴向,周向和径向方向上增长。在径向平面上,由间断因子显示的斑块的形状首先类似于平板边界层中的湍流点,然后类似于下游形成的管道流中的湍流塞。湍流斑块生长并到达周向相对侧后,便从边界层突出,尽管它们停留在边界层之内,只要形状在直径平面上呈湍流点状即可。前缘处的传播速度变得比横截面速度快,尽管在后缘处的传播速度变慢。因此,其轴向长度的增长率在下游变化。在零压力梯度下,斑块圆周长度的生长速率要小于湍流斑的生长速率,而在有利的压力梯度下,斑块的圆周长度的生长速率几乎与斑点相同。

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