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Lateral Shear Layer and Its Velocity Distribution of Flow in Rectangular Open Channels

机译:矩形明渠横向剪切层及其流速分布

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The lateral velocity distribution of flow in the shear layer of open channel is required to many problems in river and eco-environment engineering, e.g. distribution of pollutant dispersion, sediment transport and bank erosion, and aquatic habitat. It is not well understood about how the velocity varies laterally in the wall boundary layer. This paper gives an analytical solution of lateral velocity distribution in a rectangular open channel based on the depth-averaged momentum equation proposed by Shiono & Knight. The obtained lateral velocity distributions in the wall shear layer are related to the two hydraulic parameters of lateral eddy viscosity (λ ) and depth-averaged secondary flow (Γ) for given roughened channels. Preliminary relationships between the above two parameters and the aspect ratio of channel, B /H , are obtained from two sets of experimental data. The lateral width (δ ) of the shear layer was investigated and found to relate to the λ and the bed friction factor (f ), as described by Equation (2 6 ). This study indicates that the lateral shear layer near the wall can be very wide (δ /H = 14.6) for the extreme case (λ = 0.6 and f = 0.01).
机译:河流和生态环境工程中的许多问题(例如河道工程)都需要明渠剪切层中水流的横向速度分布。污染物扩散的分布,沉积物的运输和河岸侵蚀以及水生生境。关于速度如何在壁边界层中横向变化还不是很了解。本文根据Shiono&Knight提出的深度平均动量方程,给出了矩形明渠横向速度分布的解析解。对于给定的粗糙通道,在壁面剪切层中获得的横向速度分布与横向涡流粘度()和深度平均二次流(Γ)的两个水力参数有关。从两组实验数据获得上述两个参数与通道的纵横比B / H的初步关系。如等式(2 6)所述,研究了剪切层的横向宽度(iδ),并且发现其与iλ和床摩擦系数(i f)有关。这项研究表明,在极端情况下(λ= 0.6,f = 0.01),壁附近的横向剪切层可能非常宽(δ/ H = 14.6)。

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