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高超声速风洞来流扰动测量及数据后处理技术研究

余涛 王俊鹏 刘向宏 赵家权 吴杰

余涛, 王俊鹏, 刘向宏, 等. 高超声速风洞来流扰动测量及数据后处理技术研究[J]. 实验流体力学, 2019, 33(5): 49-56. doi: 10.11729/syltlx20180142
引用本文: 余涛, 王俊鹏, 刘向宏, 等. 高超声速风洞来流扰动测量及数据后处理技术研究[J]. 实验流体力学, 2019, 33(5): 49-56. doi: 10.11729/syltlx20180142
Yu Tao, Wang Junpeng, Liu Xianghong, et al. Measurements and data processing technology of freestream fluctuations in hypersonic wind tunnel[J]. Journal of Experiments in Fluid Mechanics, 2019, 33(5): 49-56. doi: 10.11729/syltlx20180142
Citation: Yu Tao, Wang Junpeng, Liu Xianghong, et al. Measurements and data processing technology of freestream fluctuations in hypersonic wind tunnel[J]. Journal of Experiments in Fluid Mechanics, 2019, 33(5): 49-56. doi: 10.11729/syltlx20180142

高超声速风洞来流扰动测量及数据后处理技术研究

doi: 10.11729/syltlx20180142
基金项目: 

国家自然基金青年科学基金项目 11702106

装备预先研究项目 41406020901

详细信息
    作者简介:

    余涛(1995-), 男, 湖北襄阳人, 硕士研究生。研究方向:高超声速流场测量。通信地址:湖北省武汉市洪山区关山街道珞喻路1037号华中科技大学航空航天学院(430074)。E-mail:yu_tao@hust.edu.cn

    通讯作者:

    吴杰,E-mail: jiewu@hust.edu.cn

  • 中图分类号: V211.74

Measurements and data processing technology of freestream fluctuations in hypersonic wind tunnel

  • 摘要: 来流扰动对高超声速风洞中开展的实验研究,如层/湍流边界层的不稳定性与转捩实验,有直接影响。为加深对高超声速风洞中边界层转捩实验的认识,需对高超声速风洞的来流扰动进行定性与定量的测量与分析。提出一种高超声速风洞扰动模态校测方法,使用热线风速仪和皮托管压力探头对高超声速风洞自由来流进行测量。在小扰动假设前提下通过模态离解分析,并结合直接数值模拟结果,获得风洞自由来流各扰动模态的幅值。运用德国不伦瑞克工业大学马赫数6 Ludwieg式高超声速风洞对该方法进行检验。实验结果显示:该风洞为典型噪声风洞,其来流扰动中声波模态高达扰动总模态的69%,涡波模态和熵波模态约各占15%。该扰动模态校测方法为高超声速风洞的流场扰动测量提供了一个思路,为基于高超声速风洞开展的实验提供了借鉴和参考。
  • 图  1  高超声速风洞自由来流的扰动[16]

    Figure  1.  Freestream fluctuation in hypersonic wind tunnel [16]

    图  2  德国不伦瑞克工业大学马赫数6 Ludwieg式高超声速风洞[35]

    Figure  2.  Mach 6 Ludwieg wind tunnel at Technical University of Braunschweig in Germany[35]

    图  3  热线风速仪系统

    Figure  3.  hot-wire anemometer system

    图  4  皮托压力探头

    Figure  4.  Pressure pitot probe

    图  5  热线仪校核曲线

    Figure  5.  Calibration curve of hot-wire

    图  6  热线仪流量与总温敏感系数比较

    Figure  6.  Sensitivity coefficients ratio of hot-wire

    图  7  自由来流中皮托管压力脉动

    Figure  7.  Pressure fluctuation of pitot tube in freestream

    图  8  皮托总压与马赫数6自由来流压力脉动传递函数(声波迎角为120°)[44]

    Figure  8.  Transfer function between pitot total pressure and Mach 6 freestream pressure disturbance (sonic attack angle is 120°) [44]

    图  9  马赫数6自由来流流量和总温脉动

    Figure  9.  Flow and total temperature fluctuation of Mach 6 freestream

    图  10  自由来流扰动子模态分析

    Figure  10.  Freestream fluctuation modal analysis

    图  11  热线仪输出电压与敏感系数线性拟合

    Figure  11.  Linear fitting of output voltage and sensitivity coefficient of hot-wire

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出版历程
  • 收稿日期:  2018-10-15
  • 修回日期:  2019-03-25
  • 刊出日期:  2019-10-25

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