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基于叠加流场面元法的民用飞机跨声速气动伺服弹性分析

吴善强 陈琦 孙亚军 尼早 陈文

吴善强,陈琦,孙亚军,等. 基于叠加流场面元法的民用飞机跨声速气动伺服弹性分析[J]. 北京航空航天大学学报,2026,52(1):167-179
引用本文: 吴善强,陈琦,孙亚军,等. 基于叠加流场面元法的民用飞机跨声速气动伺服弹性分析[J]. 北京航空航天大学学报,2026,52(1):167-179
WU S Q,CHEN Q,SUN Y J,et al. Transonic aeroservoelastic analysis of civil aircraft based on overset field-panel method[J]. Journal of Beijing University of Aeronautics and Astronautics,2026,52(1):167-179 (in Chinese)
Citation: WU S Q,CHEN Q,SUN Y J,et al. Transonic aeroservoelastic analysis of civil aircraft based on overset field-panel method[J]. Journal of Beijing University of Aeronautics and Astronautics,2026,52(1):167-179 (in Chinese)

基于叠加流场面元法的民用飞机跨声速气动伺服弹性分析

doi: 10.13700/j.bh.1001-5965.2024.0729
基金项目: 

中国商飞公司科技创新专项(Y23GS29)

详细信息
    通讯作者:

    E-mail:chenwen1@comac.cc

  • 中图分类号: V221+.3

Transonic aeroservoelastic analysis of civil aircraft based on overset field-panel method

Funds: 

Scientific and Technological Innovation Project of COMAC (Y23GS29)

More Information
  • 摘要:

    与亚声速相比,民用飞机进入跨声速飞行时,其气动伺服弹性特性出现明显的频率偏移和稳定裕度下降等问题。对于研发阶段的飞机而言,研发成本昂贵、试飞风险高、设计更改周期长,故在初步设计阶段需充分考虑跨声速区域的气动伺服弹性设计。采用偶极子格网法计算的非定常气动力无法考虑跨声速激波和边界层的影响。针对跨声速非定常气动力计算,将非定常小扰动速度势分为定常项和非定常项,通过计算流体力学求解跨声速定常项,使用非定常流场面元法求解时间线化的跨声速小扰动速度势方程来计算非定常项。将得到的跨声速非定常气动力影响系数代入气动伺服弹性机体频响函数中,并与试飞结果、偶极子气动力模型计算结果进行对比,结果表明:基于叠加流场面元法的跨声速气动伺服弹性分析在频率和稳定裕度等方面与试飞结果更吻合。探索跨声速区域传递函数频率和稳定裕度变化规律,为民用飞机跨声速气动伺服弹性设计提供方法。

     

  • 图 1  气动力影响系数求解流程图

    Figure 1.  Flow chart for solving aerodynamic influence coefficient

    图 2  机翼平板气动力网格

    Figure 2.  Wing-shaped slab aerodynamic mesh

    图 3  飞机物面网格

    Figure 3.  Aircraft surface grid

    图 4  飞机物面和空间重叠网格模型

    Figure 4.  Aircraft surface and space overlapping grid model

    图 5  飞机CFD网格示意图

    Figure 5.  Schematic diagram of aircraft CFD grid

    图 6  跨声速风洞试验

    Figure 6.  Transonic wind tunnel test

    图 7  Ma=0.8时数值模拟和风洞试验结果对比

    Figure 7.  Comparison of numerical simulation and wind tunnel test results with Ma=0.8

    图 8  k=0.2和 k=0.6时不同模态下不同站位的非定常压力系数对比

    Figure 8.  Comparison of unsteady pressure coefficient of different Root Chord due to different mode with k=0.2 and k=0.6

    图 9  跨声速机体传递函数

    Figure 9.  Transonic aircraft transfer function

    图 10  飞机固有模态示意图

    Figure 10.  Diagram of aircraft natural modes

    图 11  气动伺服弹性试飞原理示意图

    Figure 11.  Schematic diagram of aeroservoelastic flight test principle

    图 12  扫频激励信号

    Figure 12.  Sweep frequency excitation signal

    图 13  反馈信号

    Figure 13.  Feedback signal

    图 14  叠加信号

    Figure 14.  Superposed signal

    图 15  亚声速偶极子格网法分析与试飞结果对比

    Figure 15.  Comparison of DLM analysis and flight test results of subsonic

    图 16  速度为Ma=0.75时分析与试飞结果对比

    Figure 16.  Comparison of analysis and flight test results with Ma=0.75

    图 17  速度为Ma=0.80时分析与试飞结果对比

    Figure 17.  Comparison of analysis and flight test results with Ma=0.80

    图 18  不同马赫数的机体传递函数对比

    Figure 18.  Comparison of aircraft transfer function with different Mach numbers

    表  1  飞机风洞模型参数

    Table  1.   Aircraft wind tunnel model parameters

    机翼参考面积/m2机翼展长/m展弦比平均气动弦长/m
    0.351.829.60.25
    下载: 导出CSV

    表  2  不同试验马赫数下试验雷诺数

    Table  2.   Test Reynolds number at different Mach numbers

    试验马赫数 试验雷诺数
    0.40 1.88×106
    0.50 2.23×106
    0.60 2.51×106
    0.70 2.74×106
    0.80 2.90×106
    0.82 2.93×106
    0.87 2.98×106
    0.89 3.00×106
    下载: 导出CSV

    表  3  飞机固有模态和频率

    Table  3.   Aircraft natural modes and frequencies

    模态名称频率/Hz
    机翼反对称一弯2.1
    发动机对称俯仰3.0
    机身水平一弯3.4
    机身垂直一弯3.8
    发动机反对称侧偏4.0
    下载: 导出CSV

    表  4  ASE试飞激励信号

    Table  4.   ASE flight test excitation signal

    激励方法 激励位置 激励方式 激励频带/Hz 激励幅值/(°) 激励时间/s
    扫频 升降舵 对称 0.5~40 ≤1 ≤30
    扫频 副翼 反对称 0.5~40 ≤1 ≤30
    扫频 方向舵 0.5~40 ≤1 ≤30
    下载: 导出CSV
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出版历程
  • 收稿日期:  2024-10-09
  • 录用日期:  2025-01-23
  • 网络出版日期:  2025-03-14
  • 整期出版日期:  2026-01-31

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