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Mixing in the Intermediate Field of Dense Jets in Cross Currents

机译:交叉流在密集喷流的中间场混合

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This study presents an experimental and numerical study for an inclined (60 degrees to horizontal) dense jet discharged into a coflowing current. The mixing and transport of the density current arising from the jet impingement on a horizontal bottom boundary is investigated. A light attenuation technique is employed to measure the layer-averaged concentration field over a region that extends 20FrD downstream and 9FrD laterally (where F = jet densimetric Froude number, and D = jet diameter). A comprehensive characterization of the resulting buoyant spread in both steady and unsteady cases is obtained. The concentration field is also computed using a three-dimensional (3D) shallow water equation model via the distributed entrainment sink approach that incorporates a near-field Lagrangian integral jet model (JETLAG) into the 3D model for dynamic simulation of the near-far field transition. The results show the occurrence of bifurcation in the gravitational spreading layer when the impinging dense jet is bent over, characterized by a crossflow Froude number F = UrFr of around 0.8 (where U-r = ratio of ambient to jet velocity). The lateral concentration profiles are bimodal in shape; the concentration maximum is off-centered and 1.6-2 times the centerline value. The buoyant spreading is governed by buoyancy and inertia, and the spreading layer grows as x(2/3) with downstream distance. For F approximate to 0.4, the upstream intrusion of the buoyant layer past the source is arrested; lateral gradients of concentrations are small and the dilution becomes constant downstream. In the intermediate range F approximate to 0.4-0.8, the profiles evolve gradually from top-hat to bimodal. The numerical prediction of the salient flow features as well as the intermediate field dilutions and spreading layer thickness are in good agreement with data. (C) 2015 American Society of Civil Engineers.
机译:这项研究提出了一个实验和数值研究,该实验是将倾斜的(与水平方向成60度)密集喷流排放到同流电流中。研究了由射流撞击水平底部边界产生的密度电流的混合和传输。采用光衰减技术来测量在向下游延伸20FrD,向侧面延伸9FrD的区域上的平均层浓度场(其中F =射流密度弗洛德数,D =射流直径)。在稳态和非稳态情况下,均可对所产生的浮力扩散进行全面表征。还使用三维(3D)浅水方程模型,通过分布式夹带下沉方法计算浓度场,该方法将近场拉格朗日积分射流模型(JETLAG)合并到3D模型中,以进行近场动态模拟过渡。结果表明,当撞击的密集射流弯曲时,在重力扩展层中发生了分叉,其特征是错流弗洛德数F = UrFr约为0.8(其中U-r =环境与射流速度之比)。侧向浓度分布为双峰形。浓度最大值偏离中心并且是中心线值的1.6-2倍。浮力的扩散受浮力和惯性的控制,扩散层随着下游距离的增长而以x(2/3)的速度增长。当F大约为0.4时,阻止源上方的浮力层向上游侵入。浓度的横向梯度很小,下游的稀释度恒定。在大约0.4-0.8的中间范围F中,轮廓从礼帽逐渐演变为双峰。显着流动特征的数值预测以及中间场稀释度和铺展层厚度与数据非常吻合。 (C)2015年美国土木工程师学会。

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