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Discussion of 'Effect of jet aeration on hydrodynamic forces on plunge pool floors'

机译:讨论“射流曝气对跳水池底部水动力的影响”

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The Discussers congratulate the Authors for their interesting work in the field of hydrodynamic forces on plunge pool floors. The Authors present the effect of jet aeration on mean dynamic pressures at pool floors, based on both analytical computations and small-scale laboratory measurements. Based on air sucked into low-velocity water jets (V = 3.53 m/s), they obtained air concentrations close to the stagnation point of the developed jet at the pool floor of max. 30 percent. The exact pool depth is not provided by the Authors, but has been estimated by the Discussers at roughly 0.70 m, for a jet thickness at impact of roughly 0.70/11.5-0.06 m (h/b = 11.5, being the diffusion length). The corresponding mean dynamic pressure head at jet issuance is thus about 0.65 m. Superposition with the static water head of 0.70 m provides a total relative head of about 1.35 m at the pool floor. The Discussers measured mean air concentrations in plunge pools at the Laboratory of Hydraulic Constructions of the Ecole Polytechnique Federale de Lausanne, Switzerland for high velocity plunging jets (Manso 2006; Manso et al. 2006). The experiments document void fractions at singular points in plunge pools with a flat bottom. Air was entrained naturally in the pool at the jet plunging section. Rough turbulent water jets with very high velocities (up to 30 m/s) were used to replicate prototype pool aeration conditions typically found at large dam spillways. This allows creating air entrainment conditions exempt of significant scale effects in terms of Weber, Reynolds, and Froude numbers.
机译:讨论者对作者在水池池底水动力方面的有趣工作表示祝贺。作者基于分析计算和小规模实验室测量,介绍了射流曝气对池底平均动压的影响。根据吸入低速水射流(V = 3.53 m / s)中的空气,他们获得的空气浓度接近最大池池底部发达水射流的停滞点。 30%。作者没有提供确切的池深度,但是讨论者估计池深度约为0.70 m,撞击时的射流厚度约为0.70 / 11.5-0.06 m(h / b = 11.5,即扩散长度)。因此,射流发出时相应的平均动压头约为0.65 m。静态水头高度为0.70 m时的叠加可在池底提供约1.35 m的总相对水头。讨论者在瑞士洛桑联邦理工学院水力建筑实验室测量了高速冲刺射流的平均水含量(Manso 2006; Manso et al。2006)。实验记录了具有平坦底部的切入池中奇异点处的空隙率。空气自然流进了射流切入段的水池中。使用具有很高速度(高达30 m / s)的湍流湍流水射流来复制通常在大型水坝溢洪道上发现的原型水池曝气条件。这样就可以创建免除韦伯,雷诺兹和弗洛德数的明显规模效应的引气条件。

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