黄 坤, 温建明, 冯 奇. 悬索承重梁索耦合结构的垂向运动动力学模型及主共振分析[J]. 工程力学, 2013, 30(2): 182-189. DOI: 10.6052/j.issn.1000-4750.2011.07.0478
引用本文: 黄 坤, 温建明, 冯 奇. 悬索承重梁索耦合结构的垂向运动动力学模型及主共振分析[J]. 工程力学, 2013, 30(2): 182-189. DOI: 10.6052/j.issn.1000-4750.2011.07.0478
HUANG Kun, WEN Jian-ming, FENG Qi. DYNAMIC MODEL AND PRINCIPAL RESONANCE OF A COUPLED STRUCTURE BY SUSPENDED CABLE AND STAYED BEAM[J]. Engineering Mechanics, 2013, 30(2): 182-189. DOI: 10.6052/j.issn.1000-4750.2011.07.0478
Citation: HUANG Kun, WEN Jian-ming, FENG Qi. DYNAMIC MODEL AND PRINCIPAL RESONANCE OF A COUPLED STRUCTURE BY SUSPENDED CABLE AND STAYED BEAM[J]. Engineering Mechanics, 2013, 30(2): 182-189. DOI: 10.6052/j.issn.1000-4750.2011.07.0478

悬索承重梁索耦合结构的垂向运动动力学模型及主共振分析

DYNAMIC MODEL AND PRINCIPAL RESONANCE OF A COUPLED STRUCTURE BY SUSPENDED CABLE AND STAYED BEAM

  • 摘要: 该文建立了描述结构大变形和主缆初始曲率产生的几何非线性对系统动力学影响的悬索承重梁索耦合结构垂向运动动力学偏微分方程组。通过Galerkin方法一次截断把偏微分方程组化为时域上的两自由度常微分方程组。使用多尺度法得到简谐激励下常微分方程组主共振时的一次近似解。结果显示,当外激励仅激发低频或高频主共振时,系统的振幅随激励的幅值或激励频率的变化出现突然的跳跃。当激励同时激发低频和高频主共振时则有两种情况:1) 若固定高频激励幅值和频率,则系统的低频和高频振动成分的振幅随低频激励参数变化同时增加或减小;2) 若固定低频激励的幅值和频率,则系统的低频和高频振动成分的振幅随高频激励参数变化以相反的趋势变化。即高频振动幅值增大时,低频振幅减小,反之亦然。

     

    Abstract: The mathematical model for the vertical vibration of the coupled structure of a suspended-cable and stayed beam is established. The model of partial differential equations (PDEs) describes the effects of geometric nonlinearity that are induced by the large deformation and initial curvature of the mail cable. The ordinary differential equations (ODEs) are obtained from the PDEs by Galerkin method. In the principal resonance case, the first approximate analytical solutions of the ODEs are attained by the multiscale method under harmonic excitations. The results show that when the excitation frequency is close to the structure low or high natural frequency, the amplitudes of vibration appear jump phenomenon. When both low and high frequency principal resonances occur there are two cases: 1) if the amplitude and frequency of high frequency excitation are fixed, the amplitudes of the low and high frequency vibration will increase or decrease synchronously when the parameters of a low frequency excitation change; 2) if the amplitude and frequency of the low frequency excitation are fixed, the amplitudes of the low and high frequency vibration will vary in an opposite trend when the parameters of a high frequency excitation change.

     

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