陶洪飞, 杨海华, 马英杰, 戚印鑫, 耿凡坤, 滕晓静, 刘亚丽. 流量对河水滴灌重力沉沙过滤池内流速分布的影响[J]. 农业工程学报, 2017, 33(1): 131-137. DOI: 10.11975/j.issn.1002-6819.2017.01.018
    引用本文: 陶洪飞, 杨海华, 马英杰, 戚印鑫, 耿凡坤, 滕晓静, 刘亚丽. 流量对河水滴灌重力沉沙过滤池内流速分布的影响[J]. 农业工程学报, 2017, 33(1): 131-137. DOI: 10.11975/j.issn.1002-6819.2017.01.018
    Tao Hongfei, Yang Haihua, Ma Yingjie, Qi Yinxin, Geng Fankun, Teng Xiaojing, Liu Yali. Influence of flow rate on flow velocity distribution in gravity sinking and filter tank for drip irrigation with river water[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2017, 33(1): 131-137. DOI: 10.11975/j.issn.1002-6819.2017.01.018
    Citation: Tao Hongfei, Yang Haihua, Ma Yingjie, Qi Yinxin, Geng Fankun, Teng Xiaojing, Liu Yali. Influence of flow rate on flow velocity distribution in gravity sinking and filter tank for drip irrigation with river water[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2017, 33(1): 131-137. DOI: 10.11975/j.issn.1002-6819.2017.01.018

    流量对河水滴灌重力沉沙过滤池内流速分布的影响

    Influence of flow rate on flow velocity distribution in gravity sinking and filter tank for drip irrigation with river water

    • 摘要: 为研究流量对河水滴灌重力沉沙过滤池流速分布规律的影响,该文对5种不同流量下的水沙两相流流场进行了数值模拟。通过对不同流量下流速沿程分布规律、流速沿水深方向分布规律及水沙分离效率的对比与分析,可知河水滴灌重力沉沙过滤池的适宜流量范围为0.05~0.2 m3/s,进水流量越小,流速变化幅度也就越小,越有利于泥沙沉降,水沙分离效率不小于72.5%。不同流量下沉淀池中流速沿程变化规律可分成3个阶段:流速迅速增加阶段、流速缓慢减小阶段和流速迅速减小阶段。清水池中流速方向与沉淀池的相反,流速沿程减小。受进水口、出水口和固体边界,以及侧向溢流堰的影响,不同流量下河水滴灌重力沉沙过滤池中的流速沿水深方向分布规律有差别。当流量为0.05和0.1 m3/s时,远离进水口、出水口及侧向溢流堰的位置,流速沿水深方向的分布规律包含流速迅速增加、流速缓慢减小和流速恒定3个阶段,而清水池则只包括流速迅速增加和流速恒定阶段。研究可对大首部的应用提供参考。

       

      Abstract: Abstract: Filters have high energy consumption, high cost and high water consumption and other shortcomings. In order to solve this problem, gravity sinking and filter tank for drip irrigation with river water (GSFTDIRW) is proposed, which consists of sedimentation tank, clear water tank and sewage tank. The flow is the key factor influencing the separation efficiency of water-sediment and the flow field of wate-sediment. This study investigated the influence of flow rate on the GSFTDIRW. A physical experiment was carried out in the hydraulic experiment hall of Xinjiang Institute of Water Resources and Hydropower Research. The parameters such as water depth, flow velocity and sediment concentration in the GSFTDIRW under flow rate of 0.05 m3/s were measured. The model was set up according to the model size used in the physical experiment in the gambit drawing software. Meanwhile, the boundary conditions were set in the gambit drawing software. Then the parameters were set in the Fluent software. Simulated values were processed by tecplot software. By comparing the experimental values and simulated values, it was shown that the porous media model was reliable in simulating the filter mesh. It was feasible to simulate the internal flow field in GSFTDIRW using the standard k-ε two-equation model and the mixture model. Based on these, the flow field of water-sediment two-phase flow was simulated in the GSFTDIRW under 4 different flow rates. By comparing the distribution of flow velocity along the length, the distribution of water velocity along water depth and the separation efficiency of water-sediment, it was found that the appropriate flow rate was in a range of 0.05-0.2 m3/s when the sedimentation tank was 25 m in length, 1.5 m in width, 0.80 m in height, slope 1%, and lateral overflow weir 5 m. At the same time, the average flow velocity of sedimentation tank is 0.053-0.19 m/s. The smaller the influent flow was, the smaller the velocity variation was. This was more conducive to sedimentation. The sediment concentration was less than or equal to 1.65 kg/m3 in the clear water tank, and the total water-sediment separation efficiency was not less than 72.5%. Under the different flow rates, the flow velocity change along the sedimentation tank could be divided into 3 stages: increasing rapidly, decreasing slowly and decreasing rapidly. The velocity of flow in the clear water tank was opposite to that of the sedimentation tank, and the flow velocity decreased along the path. Under the influence of inlet, outlet and solid boundary, and lateral overflow weir, the distribution of flow velocity along water depth was different under different flow rate in the GSFTDIRW: the distribution of velocity along the depth of water at the locations far away from the water inlet, outlet and lateral weir contained 3 stages when the flow rate was 0.05 and 0.1 m3/s: rapid increase, slow decrease and constant. However, the distribution of velocity only included the rapid increase and constant stage in clear water tank.

       

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