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Hydraulic Characteristics of Chute Block-Trapezoidal Block Joint Dissipator
ZHAO Qian, MU Zhen-wei, ZHOU Kai, GAO Shang, ZHANG Hong-hong
Journal of Changjiang River Scientific Research Institute ›› 2025, Vol. 42 ›› Issue (1) : 120-128.
PDF(4090 KB)
PDF(4090 KB)
Hydraulic Characteristics of Chute Block-Trapezoidal Block Joint Dissipator
This study aims to address the turbulent flow patterns and significant water surface fluctuations in the original stilling basin, which lead to the formation of repelled downstream hydraulic jumps and subsequent scouring damage to the apron slab. To mitigate these problems, a combined chute block and trapezoidal block energy dissipator is employed, and the hydraulic characteristics of this dissipator are investigated. Physical model testing and numerical simulation techniques are combined to study the energy dissipation behavior under various flow rates. The energy conversion processes within the flow are analyzed, and flow velocity reduction ratios are calculated to assess the effectiveness of the dissipator. Findings indicate that, for the chute block-trapezoidal block joint dissipator with double rows of trapezoidal blocks arranged in a staggered manner, the velocity reduction ratios at three different flow rates are 60.00%, 75.34%, and 73.75%, respectively. Compared to the original stilling basin, this arrangement reduces the length of the hydraulic jump by 11.29%, 14.17%, and 10.22% across the respective flow rates. The energy dissipation mechanism is categorized into four distinct zones: the flow contraction and diversion area, the hydraulic jump swirl area, the vortex areas on both sides, and the post-jump mainstream area. The findings provide a valuable reference for the design of joint dissipators and the optimization of stilling basins.
stilling basin / hydraulic characteristics / hydraulic jump / chute block - trapezoidal block / energy dissipation
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According to the definition of frictional head loss, the theoretical relations of frictional head loss with coefficient of bed resistance, conjugate depth ratio of hydraulic jump, ratio of width to height of initial section, and initial depth are deduced. The theoretical calculation equations of frictional head loss coefficient and the local head loss coefficient of free hydraulic jump in rectangular open channel are given, and the simple fitting formulas of frictional, local, and total head loss coefficients are put forward. It is shown that frictional head loss grows with the rise of the initial depth of hydraulic jump and the coefficient of bed resistance; but declines with the increase of the conjugate depth ratio and the ratio of width to height of initial section. Local head loss coefficient augments with the increasing of the Froude number of initial section. The proportion of local head loss in the total head loss becomes larger with the increase of Froude number. When Froude number is 3, the proportion of local head loss is 90%, and when Froude number is 6, the proportion of local head loss is over 95%. The research results could improve and enrich the theoretical system of hydraulic jump.
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The differences in hydraulic characteristics between two energy dissipation approaches, combination of diversion pier and suspended grid and single suspended grid, were investigated by tracking the nonlinear free surface using the VOF method based on the Navier-Stokes equation. The large-scale turbulence and intensive air entrainment in the hydraulic jump were simulated. On this basis, the detained flow structure and wall pressure in the stilling pool were obtained for analyzing the turbulence and pressure distribution. Results illustrated that the joint energy dissipator significantly increased the turbulent intensity and fluctuating scale of water body in the paraboloid of stilling basin. The turbulence intensity, which decayed remarkably along the flow direction, was highly improved compared with the control scheme (single suspended grid) for relative depth h* in the range from 0.4 to 0.8. Hydrodynamic pressure on the base slab of stilling pool fluctuated notably, and the average pressure reduced slightly compared with that in the control scheme. The peak of pressure fluctuation is located nearby 0.3<xp<0.4(xp is the relative location), and the dynamic pressure coefficient is 2.0~2.4 times of the maximum value on the base slab of the pool.
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