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Modeling and Detection of Limit-Cycle Oscillations Using Adaptable Linear Models

机译:使用自适应线性模型对极限环振荡进行建模和检测

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摘要

A method for modeling the flutter response of a thin winged aircraft is presented. A hybrid physical-adaptive modeling framework is proposed to separate the autoregressive and moving average flutter components. Adaptive oscillators set at the structural free-vibration modal frequencies of the wing represent the structure (the autoregressive component). The moving average filters represent signal changes caused by aerodynamic forces encountered during flight. Connected in series, these modules form a hybrid model for wing flutter under changing flight conditions. The moving average component is trained to predict the signal produced by an accelerometer at the wing tip. The residual is segmented using an analysis of variance. The resulting family of linear moving average models provides a synthesis of the wing's response over time. Our analysis shows that this modeling paradigm performs well with data taken at increasing Mach numbers in level flight. Network parameters are shown to correlate linearly with Mach. Network components can themselves be predicted as functions of Mach number, allowing the accelerometer signals to be predicted with a high degree of accuracy. The paradigm is further validated by using an adapted model with a separate set of data from a different but similar flight condition.
机译:提出了一种对薄机翼飞机的颤振响应进行建模的方法。提出了一种混合的物理自适应建模框架来分离自回归和移动平均颤振分量。设置在机翼的结构自由振动模态频率处的自适应振荡器代表结构(自回归分量)。移动平均滤波器表示由飞行过程中遇到的空气动力引起的信号变化。这些模块串联连接,形成了在变化的飞行条件下机翼颤振的混合模型。训练移动平均分量以预测由机翼尖端的加速度计产生的信号。使用方差分析对残差进行细分。所得的线性移动平均值模型系列提供了机翼随时间变化的响应的综合信息。我们的分析表明,这种建模范例在水平飞行中以增加的马赫数获取的数据表现良好。网络参数显示与马赫线性相关。网络成分本身可以作为马赫数的函数进行预测,从而可以高精度地预测加速度计信号。通过使用具有来自不同但相似的飞行条件的单独数据集的适应模型进一步验证了范例。

著录项

  • 来源
    《Journal of Aircraft》 |2005年第6期|p.1576-1588|共13页
  • 作者单位

    U.S. Air Force SEEK EAGLE Office, Eglin Air Force Base, Florida;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 航空;
  • 关键词

  • 入库时间 2022-08-18 02:34:08

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