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雷诺数对不同展弦比下长平板绕流湍流特性影响的实验研究

刘宇陆 刘欣 丁旭 李家骅

刘宇陆,刘欣,丁旭,等. 雷诺数对不同展弦比下长平板绕流湍流特性影响的实验研究[J]. 应用技术学报,2024,24(1):1-8. doi:  10.3969/j.issn.2096-3424.2024.01.014
引用本文: 刘宇陆,刘欣,丁旭,等. 雷诺数对不同展弦比下长平板绕流湍流特性影响的实验研究[J]. 应用技术学报,2024,24(1):1-8. doi:  10.3969/j.issn.2096-3424.2024.01.014
LIU Yulu, LIU Xin, DING Xu, LI Jiahua. An experimental study on the effect of Reynolds number on the turbulent characteristics of a rectangular cylinder with different aspect ratio[J]. J. Technol, 2024, 24(1): 1-8. doi: 10.3969/j.issn.2096-3424.2024.01.014
Citation: LIU Yulu, LIU Xin, DING Xu, LI Jiahua. An experimental study on the effect of Reynolds number on the turbulent characteristics of a rectangular cylinder with different aspect ratio[J]. J. Technol, 2024, 24(1): 1-8. doi: 10.3969/j.issn.2096-3424.2024.01.014

雷诺数对不同展弦比下长平板绕流湍流特性影响的实验研究

doi: 10.3969/j.issn.2096-3424.2024.01.014
基金项目: 国家自然科学基金项目(12032016,12372277)资助
详细信息
    作者简介:

    刘宇陆(1959-),男,教授,博士,主要研究方向为湍流的理论与应用研究、环境流体力学等。E-mail: ylliu@sit.edu.cn

    通讯作者:

    李家骅(1982-),男,高级实验师,博士,主要研究方向为实验流体力学及应用等。E-mail:lijiahua@sit.edu.cn

  • 中图分类号: O351.2

An experimental study on the effect of Reynolds number on the turbulent characteristics of a rectangular cylinder with different aspect ratio

  • 摘要: 利用粒子图像测速(PIV)实验研究了不同展弦比下,雷诺数对长平板绕流的影响。雷诺数为:Re=500、800、1000,平板板长L与厚度D的比值为L/DL/D=3、6。实验结果表明,展弦比L/D=3时,流体从平板前缘分离后重新附着在平板尾缘处。展弦比L/D=3和6时,平板上方再附着长度及平板后的回流区长度会随着雷诺数的增大而增大,展弦比为6时,雷诺数对板上分离泡的影响较小。雷诺数和展弦比会影响流场的湍流特性。展弦比L/D=3时,雷诺数的增加会导致平板两侧的脉动强度增加,而板后的脉动强度减弱;随着展弦比L/D增加,流场的湍流脉动强度减小。同时随着雷诺数的增加,流场中的小尺度涡结构增加。
  • 图  1  实验模型示意图和视场图

    Figure  1.  The schematic diagram of experimental model and view of PIV region

    图  2  Re=1000时,展弦比L/D=3和6的St数分布

    Figure  2.  The distribution of Strouhal number(St) when Reynolds number is 1000 and aspect ratio is L/D=3 and 6

    图  3  时均流线分布

    Figure  3.  The distributions of time-averaged streamline

    图  4  L/D=3和6时,近壁区(y/D=0.58)的流向速度$ U/{U_\infty } $分布

    Figure  4.  The distribution of stream wise velocity at different positions along y/D=0.58 when aspect ratio is L/D=3 and 6

    图  5  平板上表面回流系数云图

    Figure  5.  Contours of reverse flow intermittency

    图  6  L/D=3和6时,近壁区(y/D=0.58)的回流系数分布

    Figure  6.  The distribution of reverse flow intermittency along y/D=0.58 when aspect ratio is L/D=3 and 6

    图  7  时均涡量场

    Figure  7.  Time-averaged vorticity fields

    图  8  流向速度脉动强度云图

    Figure  8.  Contour plot of streamwise velocity fluctuation

    图  9  前50阶POD模态能量分布及累积能量

    Figure  9.  Percentage of the total energy contributed by the first 50 POD modes and the corresponding cumulative energy

    图  10  前两阶模态分布

    Figure  10.  The distribution of the first two POD modes

    图  11  Re=1000,L/D=3时的相位平均λci场和流线的分布

    Figure  11.  Phase mean λci field and corresponding streamlines when Reynolds number is 1000 and aspect ratio is L/D=3

    图  12  Re=1000,L/D=6时的相位平均λci场和流线的分布

    Figure  12.  Phase mean λci field and corresponding streamlines when Reynolds number is 1000 and aspect ratio is L/D=6

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出版历程
  • 收稿日期:  2023-09-28
  • 网络出版日期:  2024-01-26
  • 刊出日期:  2024-03-30

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