微灌鱼雷网式过滤器全流场数值模拟
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  • 英文篇名:Numerical simulation on flow field of screen filter with torpedo in micro-irrigation
  • 作者:阿力甫江·阿不里米提 ; 虎胆·吐马尔白 ; 木拉提·玉赛音 ; 木克然·阿娃
  • 英文作者:Alifujiang·Abulimiti;Hudan·Tumaerbai;Mulati·Yusaiyin;Mukeran·Awa;College of Water Conservancy and Civil Engineering, Xinjiang Agricultural University;Xinjiang College of Water Resources and Hydropower Engineering;Xinjiang Xinshui Modern Water Resources Engineering Co., Ltd.;
  • 关键词:流场 ; 流速 ; 压力 ; 鱼雷网式过滤器 ; 数值模拟 ; 湍流模型
  • 英文关键词:flow fields;;flow velocity;;pressure;;torpedo screen filter;;numerical simulation;;turbulence model
  • 中文刊名:NYGU
  • 英文刊名:Transactions of the Chinese Society of Agricultural Engineering
  • 机构:新疆农业大学水利与土木工程学院;新疆水利水电学校;新疆鑫水现代水利工程有限公司;
  • 出版日期:2017-02-08
  • 出版单位:农业工程学报
  • 年:2017
  • 期:v.33;No.305
  • 基金:国家自然科学基金资助项目“大规模滴灌条件下棉田土壤盐分积累过程与排盐模式研究”(51469033)(2015-2018)
  • 语种:中文;
  • 页:NYGU201703014
  • 页数:6
  • CN:03
  • ISSN:11-2047/S
  • 分类号:115-120
摘要
为了充分了解鱼雷网式过滤器内部流场分布规律,该文应用雷诺时均(Reynolds-Averaged Navier-Stokes,RANS)方程及RNG k-ε湍流模型,对过滤器内部全流场进行全流场数值模拟。结果表明:鱼雷部件和出水口边界条件对该过滤器的速度流场和压力场分布规律影响很大,鱼雷部件的影响是尤为突出;滤网及其内、外侧的水流流速沿X轴的变化规律分流速迅速增加、流速迅速减小和流速缓慢减小3个阶段;滤网内外压力分布有很大的的差异,滤网内侧压力沿X轴分布从迅速增加到缓慢减小、最后趋于稳定。而滤网外侧压力分布沿X轴的变化很大,特别是在出水口处压力迅速减少,压力沿X轴的波动幅度较大。滤网内侧压力比外侧的大,两者的压力差沿X轴越来越小,最大压力差为23 k Pa左右,最小压力差为0.5 k Pa。研究结果认为整个滤网堵塞不均匀,滤网堵塞呈现从尾部开始向出水口方向发展的趋势,对后续滤网的冲洗排污产生重要影响。该文建议在设定最佳排污压差时需要慎重考虑。
        In order to deeply understand the flow distribution of the torpedo screen filter,the Reynolds-averaged Navier-Stokes(RANS)equation and Re-Normalization Group(RNG)k-εturbulence closure model were used to simulate the flow field of this filter system.To ensure the reliability of the numerical simulation,the physical experiment results were compared to the numerical simulation results,and the result showed that the maximum relative error between the head loss in the physical experiment and the numerical simulation was 5.99%when the filtering system was operated at a maximum flow rate of 360m3/h,indicating reliability of the simulation method.The simulation results showed that the torpedo components and the boundary conditions of the outlet notably affected the distribution rules of both the velocity and the pressure fields for the filter,especially for the torpedo components.The distributions of the flow velocities of inside and outside of the screen along the X-axis were not uniform during the filtering process.And the flow velocity distributions inside and outside of the filter screen along the X-axis were divided into 3 stages:1)a rapid increase;2)a rapid decrease;and 3)a gradual decrease.The maximum velocities inside and outside of the screen and their spatial locations along the X-axis were different.For the upper part of the screen,the inside flow velocity increased in a larger amplitude than did the outside flow velocity,and the flow velocity achieved its maximum(5.53 m/s)at the X value of 0.29 m.The outside water flow velocity of the upper part of the screen achieved its maximum value(3.9 m/s)at the X value of 0.33 m.When the X value ranged from 0.2 to 0.6 m,the inside flow velocity of the upper part of the screen was larger than that of the outside;however,the difference in the flow velocity along the X-axis continually decreased from the maximum difference of 4.1 m/s.For the lower part of the screen,the maximum flow velocity and its position of lower part of the screen was 5.4 m/s and 0.42 m,respectively.When the X value was 0.41-0.51 m,the flow velocity of the water in the outside area of the lower part of the screen was larger than that of water in the inside area.Nonetheless,the flow velocities of water in the other inside of lower screen were higher than those of water in the outside,and the maximum difference in the flow velocity was 2.28 m/s.There was a notable difference in the pressure distributions along the inside and outside of the screen.The pressure of the inside along the X-axis first rapidly increased,then gradually decreased,and finally stabilized.In contrast,the pressure of the outside along the X-axis exhibited a greater variation;for example,the pressure rapidly decreases at the outlet,and the fluctuations along the X-axis are relatively large.The pressure of the inside of the screen was larger than that of the outside;however,the pressure differences along the X-axis continually decreased,and the maximum and minimum pressure differences between the two were approximately 23 and 0.5 k Pa,respectively.This indicated that the screen clogging was not evenly distributed,and the screen clogging began at the downstream end of the screen and developed progressively upstream towards the outlet.This phenomenon significantly affected the cleaning process of the filter.Therefore,it is strongly suggested that in a practical application the optimum drainage differential pressure must be circumspectly considered.
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