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不同攻角下扁平箱梁颤振机理

李志国 王骑 伍波 廖海黎

李志国, 王骑, 伍波, 廖海黎. 不同攻角下扁平箱梁颤振机理[J]. 西南交通大学学报, 2018, 53(4): 687-695, 755. doi: 10.3969/j.issn.0258-2724.2018.04.004
引用本文: 李志国, 王骑, 伍波, 廖海黎. 不同攻角下扁平箱梁颤振机理[J]. 西南交通大学学报, 2018, 53(4): 687-695, 755. doi: 10.3969/j.issn.0258-2724.2018.04.004
LI Zhiguo, WANG Qi, WU Bo, LIAO Haili. Flutter Mechanism of Flat Box Girder under Different Attack Angles[J]. Journal of Southwest Jiaotong University, 2018, 53(4): 687-695, 755. doi: 10.3969/j.issn.0258-2724.2018.04.004
Citation: LI Zhiguo, WANG Qi, WU Bo, LIAO Haili. Flutter Mechanism of Flat Box Girder under Different Attack Angles[J]. Journal of Southwest Jiaotong University, 2018, 53(4): 687-695, 755. doi: 10.3969/j.issn.0258-2724.2018.04.004

不同攻角下扁平箱梁颤振机理

doi: 10.3969/j.issn.0258-2724.2018.04.004
基金项目: 

国家自然科学基金资助项目 51678508

国家973计划资助项目 2013CB036301

国家自然科学基金高铁联合基金资助项目 U1434205

国家自然科学基金资助项目 51778547

详细信息
    作者简介:

    李志国(1977-), 男, 讲师, 博士研究生, 研究方向为桥梁与结构风工程, 电话:13699098648, E-mail:lizhiguo@swjtu.edu.cn

    通讯作者:

    王骑(1980-), 男, 副教授, 博士, 研究方向为桥梁与结构风工程, 电话:13688348778, E-mail:wangchee_wind@swjtu.edu.cn

  • 中图分类号: U448.43

Flutter Mechanism of Flat Box Girder under Different Attack Angles

  • 摘要: 静风效应产生的附加风攻角对大跨度桥梁的颤振性能有着重要的影响,因此研究不同风攻角下主梁的颤振机理有重要意义.以扁平箱梁为研究对象,基于不同攻角下的颤振导数,采用双模态耦合解法掌握了颤振性能,继而通过分析气动阻尼、相位差和气动力幅值的变化研究了颤振机理.研究结果表明:在0°和3°攻角下,非耦合气动力为扁平箱梁断面提供了较大的正阻尼,颤振临界风速较高;在5°攻角下,非耦合气动力产生的正阻尼显著减小,使得耦合气动力产生的负阻尼迅速增加,导致颤振临界风速显著降低;耦合运动相位角增大是大攻角下气动负阻尼增加的主要原因,耦合气动力振幅则对颤振风速没有影响;此颤振机理表明大攻角下扁平箱梁颤振性能的弱化是由耦合效应增大引起,而非扭转运动产生的气动负阻尼引起.

     

  • 图 1  扁平箱梁模型断面

    Figure 1.  Cross-section of model

    图 2  不同攻角下颤振导数

    Figure 2.  Flutter derivatives under different attack angles

    图 3  气动阻尼及模态频率随折算风速的变化

    Figure 3.  Flutter analysis of aerodynamic damping ratio and modal frequency

    图 4  耦合气动力项及非耦合气动力项对气动阻尼的影响

    Figure 4.  Contributions of coupled and uncoupled terms to damping ratios

    图 5  总阻尼及其子项随折算风速的变化规律

    Figure 5.  Total damping and sub-items varying with reduced velocity

    图 6  case 1~3中相位差随折算风速的变化曲线

    Figure 6.  Phase lag varying with reduced velocity in case 1-3

    图 7  sin ψ1随折算风速的变化

    Figure 7.  sin ψ1 varying with reduced velocity

    图 8  气动阻尼幅值因子Ψ1相关的各参数变化规律

    Figure 8.  Regularity of sub items of amplitude factor Ψ1

    图 9  不同攻角下的气动阻尼幅值因子

    Figure 9.  Amplitude factor under different attack angles

    表  1  计算参数和试验参数

    Table  1.   Parameters for calculation and tests

    α1 case m/kg I/(kg·m2) ωα0/(rad·s-1) ωh0/(rad·s-1) ωα0/ωh0
    1 10.56 0.327 18.85 10.21 1.85
    2 9.61 0.325 19.44 11.00 1.77
    3 10.56 0.372 17.67 10.21 1.73
    1 10.56 0.327 18.85 10.21 1.85
    2 9.61 0.325 19.44 11.00 1.77
    3 10.56 0.372 17.67 10.21 1.73
    1 10.56 0.327 18.85 10.21 1.85
    2 9.61 0.325 19.44 11.00 1.77
    3 10.56 0.372 17.67 10.21 1.73
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  • 收稿日期:  2017-06-21
  • 刊出日期:  2018-08-01

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