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高超声速风洞连续变动压舵面颤振试验

季辰 赵玲 朱剑 刘子强 李锋

季辰, 赵玲, 朱剑, 刘子强, 李锋. 高超声速风洞连续变动压舵面颤振试验[J]. 机械工程学报, 2017, 31(6): 37-44. doi: 10.11729/syltlx20170088
引用本文: 季辰, 赵玲, 朱剑, 刘子强, 李锋. 高超声速风洞连续变动压舵面颤振试验[J]. 机械工程学报, 2017, 31(6): 37-44. doi: 10.11729/syltlx20170088
Ji Chen, Zhao Ling, Zhu Jian, Liu Ziqiang, Li Feng. Hypersonic wind tunnel flutter test research on rudder models by continuously varying dynamic pressure[J]. JOURNAL OF MECHANICAL ENGINEERING, 2017, 31(6): 37-44. doi: 10.11729/syltlx20170088
Citation: Ji Chen, Zhao Ling, Zhu Jian, Liu Ziqiang, Li Feng. Hypersonic wind tunnel flutter test research on rudder models by continuously varying dynamic pressure[J]. JOURNAL OF MECHANICAL ENGINEERING, 2017, 31(6): 37-44. doi: 10.11729/syltlx20170088

高超声速风洞连续变动压舵面颤振试验

doi: 10.11729/syltlx20170088
基金项目: 

国家自然科学基金项目 11702285

详细信息
    作者简介:

    季辰(1982-), 男, 江苏南通人, 高级工程师。研究方向:气动弹性试验。通信地址:北京市7201信箱16分箱(100074)。E-mail:jichen167@sina.com

    通讯作者:

    季辰, E-mail: jichen167@sina.com

  • 中图分类号: V211.74;V215.3+4

Hypersonic wind tunnel flutter test research on rudder models by continuously varying dynamic pressure

  • 摘要: 为了研究舵、翼面高超声速颤振特性,中国航天空气动力技术研究院建立了高超声速风洞连续变动压颤振试验技术。对具有相同结构动力学和气动特性的舵面模型进行颤振试验,试验马赫数为4.95和5.95。试验中缓慢连续增加试验动压直至颤振发生,并由此获得颤振临界参数;采用短时傅里叶变换时频域分析法研究了试验中模型频率随动压变化的耦合特性,分析表明该模型在试验条件下发生了经典弯扭耦合颤振。试验中还采用亚临界试验数据对颤振余度法和阻尼外推法2种颤振边界预测技术进行了研究,2种方法在高超声速颤振试验中都显示了良好的预测精度。研究还表明,动压增加的速率对颤振边界的预测精度影响较小。采用红外热成像技术对模型的气动加热进行了研究,温度场测量显示舵面最高温度出现在舵根部前缘位置,舵前缘和舵面斜面中后部温度也较高;舵轴裸露在流场中的部分由于反射板附面层的影响其气动加热问题并不严重。

     

  • 图  数据采集系统

    Figure  1.  Data acquisition system

    图  红外热像仪

    Figure  2.  Infrared thermal imager

    图  计算模态振型

    Figure  3.  Calculation mode shapes

    图  模型纹影图

    Figure  4.  Schlieren photograph of the model

    图  F5模型高超颤振试验(Ma=4.95)

    Figure  5.  F5 hypersonic flutter test (Ma=4.95)

    图  F6模型高超颤振试验(Ma=5.95)

    Figure  6.  F6 hypersonic flutter test (Ma=5.95)

    图  时频谱图(F5, Ma=4.95)

    Figure  7.  Time-frequency spectrum (F5, Ma=4.95)

    图  时频谱图(F6, Ma=5.95)

    Figure  8.  Time-frequency spectrum (F6, Ma=5.95)

    图  颤振余度法(F5模型,Ma=4.95)

    Figure  9.  Flutter margin method (F5, Ma=4.95)

    图  10  颤振余度法(F6模型,Ma=5.95)

    Figure  10.  Flutter margin method (F6, Ma=5.95)

    图  11  阻尼比外插颤振边界(F5模型,Ma=4.95)

    Figure  11.  Damping ratio extrapolation (F5, Ma=4.95)

    图  12  阻尼比外插颤振边界(F6模型,Ma=5.95)

    Figure  12.  Damping ratio extrapolation (F6, Ma=5.95)

    图  13  颤振发展速率

    Figure  13.  Rate of flutter development

    图  14  动压增加速率

    Figure  14.  Rate of dynamic pressure increase

    图  15  动压增速与颤振发展速率

    Figure  15.  KFM vs Kq plot

    图  16  F5模型表面温度分布(Ma=4.95)

    Figure  16.  Temperature distribution of model F5 (Ma=4.95)

    图  17  F6模型表面温度分布(Ma=5.95)

    Figure  17.  Temperature distribution of model F6 (Ma=5.95)

    图  18  F5模型表面温度随时间变化曲线

    Figure  18.  The surface temperature of model F5 versus time

    图  19  F5模型表面温度随时间变化曲线

    Figure  19.  The surface temperature of model F5 versus time

    表  1  模型模态参数

    Table  1.   Mode parameters

    Frequency/Hz Frequency ratio Damping ratio/(%)
    f1 f2 f2/f1 ξ1 ξ2
    FEM 32.3 55.8 1.73 -- --
    GVT F5 33.5 55.7 1.66 0.31 0.41
    GVT F6 32.1 54.2 1.69 0.33 0.32
    下载: 导出CSV

    表  2  模型颤振参数

    Table  2.   Flutter parameters

    Model Mach number qfm
    /(104Pa)
    ρ
    /(kg·m-3)
    ff/Hz Tt/K
    F5 4.95 4.372 0.1392 40.2 378.2
    F6 5.95 4.412 0.1059 39.1 477.3
    下载: 导出CSV

    表  3  不同方法得到的颤振动压

    Table  3.   Comparison of flutter dynamic pressures

    Model Measured Flutter marginfunction Damping ratio extrapolation
    qfm/(104Pa) qff/(104Pa) δ/% qfd/(104Pa) δ/%
    F5 4.372 4.241 -3.0 4.261 -2.5
    F6 4.412 4.305 -2.4 4.352 -1.4
    下载: 导出CSV

    表  4  颤振动压增速影响

    Table  4.   Influence of the dynamic-pressure-increasing rate

    Ma Kq
    /(Pa·s-1)
    KFM
    /(s-4·Pa-1)
    Model
    4.95 145 57617 F5-1
    4.95 767 58442 F5
    4.95 2393 55428 F5-2
    下载: 导出CSV
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出版历程
  • 收稿日期:  2017-07-03
  • 修回日期:  2017-08-31

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