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Experimental and theoretical study of density jumps on smooth and rough beds

机译:光滑和粗糙床上密度跳跃的实验和理论研究

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Hydraulic jumps in density currents are technically referred to density jumps. These jumps significantly influence the dynamic and quality characteristics of the gravity currents. The density jump is studied theoretically and experimentally in this study by considering the bed roughness. Experiments were performed in a rectangular laboratory flume (0.4 m width; 0.9 m depth; 8.3 m length). Four rough beds comprised of closely packed gravel particles glued onto the horizontal part of the bed were examined. For both smooth and rough beds, a simple relationship was obtained for estimating the conjugate depth ratio as a function of the relative roughness and the upstream densimetric Froude number. The conjugate depth ratio was found to decrease with increasing relative roughness. The results also indicated that, if the entrainment ratio is specified, the minimum value of the upstream densimetric Froude number increases with increasing relative bed roughness. An equation for calculating the maximum possible value of the relative roughness was also determined. The spatial development of the density current for smooth beds was analysed in both super-critical and sub-critical flow regimes. Good similarity collapses of velocity and concentration profiles were obtained for the super-critical section just upstream of the jump. The concentration distributions located just downstream of the jump, however, exhibited a large scattering of measured data, especially near the bed. It was found that this scattering decreases with the distance from the end of the jump. The results of the experimental runs also indicated that, at a distance about nine times the post-jump current thickness from the end of the jump, the non-dimensional vertical profile of mean velocity has a shape similar to that at the pre-jump section. A new reliable relationship was also proposed for calculating the local velocity inside both the wall and jet regions.
机译:密度电流中的液压跃变在技术上称为密度跃变。这些跳跃极大地影响了重力流的动态和质量特性。通过考虑床的粗糙度,在理论上和实验上研究了密度跃变。实验是在长方形的实验室水槽(宽0.4 m;深0.9 m;长8.3 m)中进行的。检查了四个粗糙的床,这些床由紧密堆积的砾石颗粒粘合在床的水平部分上组成。对于光滑床和粗糙床,都获得了一个简单的关系,用于估计共轭深度比与相对粗糙度和上游密度弗洛德数的关系。发现共轭深度比随着相对粗糙度的增加而降低。结果还表明,如果指定了夹带率,则上游密度弗洛德数的最小值随相对床粗糙度的增加而增加。还确定了用于计算相对粗糙度的最大可能值的方程式。在超临界和亚临界流态下都分析了光滑床的密度流的空间发展。在跳跃的上游,超临界部分获得了速度和浓度分布的良好相似性崩溃。然而,浓度分布恰好位于跃变的下游,显示出大量的测量数据散射,尤其是在床附近。发现该散射随着距跳跃末端的距离而减小。实验运行的结果还表明,在距跳跃结束点约九倍的跳跃后电流厚度的距离处,平均速度的无量纲垂直轮廓具有与跳跃前截面相似的形状。 。还提出了一种新的可靠关系,用于计算壁区域和射流区域内部的局部速度。

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