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Energy dissipation, flow resistance and gas-liquid interfacial area in skimming flows on moderate-slope stepped spillways

机译:中坡阶梯溢洪道撇渣流的能量耗散,流阻和气液界面面积

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With the re-evaluation and revision of a number of design floods, several embankment overtopping protection systems have been developed and a common technique is the construction of a stepped spillway on the downstream slope. For such moderate slope stepped channels, detailed air–water flow measurements were performed in a large facility with a focus on the rate of energy dissipation, flow resistance, air–water interfacial areas and re-aeration rates. Past and present experimental results showed a significant aeration of the flow. The median dimensionless residual head was about 3 × dc for the 21.8° sloping chute and smaller than that for flatter slopes (θ = 3.4° and 15.9°). The flow resistance results yielded an equivalent Darcy friction factor of about 0.25 implying a larger flow resistance for the 21.8° slope angle than for smaller slope angles. The re-aeration rate was deduced from the integration of the mass transfer equation using measured air–water interfacial areas and air–water flow velocities. The results suggested an increasing re-aeration rate with increasing rate of energy dissipation. The stepped invert contributed to intense turbulence production, free-surface aeration and large interfacial areas. The experimental data showed however some distinctive seesaw pattern in the longitudinal distribution of air–water flow properties with a wave length of about two step cavities. While these may be caused by the interactions between successive adjacent step cavities and their interference with the free-surface, the existence of such “instabilities” implies that the traditional concept of normal flow might not exist in skimming flows above moderate-slope stepped spillways.
机译:随着对许多设计洪水的重新评估和修订,已经开发了几种堤防防溢系统,一种常见的技术是在下游边坡上建造阶梯式溢洪道。对于这种中等坡度的阶梯状通道,在大型设施中进行了详细的空气-水流量测量,重点是能量耗散率,流阻,空气-水界面面积和通气率。过去和现在的实验结果显示出明显的通气。 21.8°倾斜斜槽的中位无量纲残留水头约为3×dc ,小于平坡(θ= 3.4°和15.9°)。流动阻力结果产生的等效达西摩擦系数约为0.25,这意味着与较小的倾斜角相比,对于21.8°的倾斜角,流动阻力更大。再充气率是由传质方程式的积分得出的,使用的是测量的气水界面面积和气水流速。结果表明,随着耗散率的增加,通气率也随之增加。阶梯状倒置有助于产生强烈的湍流,自由表面通气和较大的界面面积。然而,实验数据表明,在空气-水流特性的纵向分布中,存在一些独特的跷跷板模式,其波长约为两个阶梯腔。尽管这些可能是由于相邻的连续阶梯腔之间的相互作用以及它们对自由表面的干扰引起的,但这种“不稳定性”的存在暗示着正常流量的传统概念可能不存在于中坡阶梯溢洪道上方的撇油流量中。

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