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接触网风致振动频率特性的有限元数值模拟及试验验证

闵永智 张智慧 胡延文 王果 张廷荣 赵珊鹏

闵永智, 张智慧, 胡延文, 王果, 张廷荣, 赵珊鹏. 接触网风致振动频率特性的有限元数值模拟及试验验证[J]. 西南交通大学学报. doi: 10.3969/j.issn.0258-2724.20250497
引用本文: 闵永智, 张智慧, 胡延文, 王果, 张廷荣, 赵珊鹏. 接触网风致振动频率特性的有限元数值模拟及试验验证[J]. 西南交通大学学报. doi: 10.3969/j.issn.0258-2724.20250497
MIN Yongzhi, ZHANG Zhihui, HU Yanwen, WANG Guo, ZHANG Tingrong, ZHAO Shanpeng. Finite Element Numerical Simulation and Experimental Verification of Frequency Characteristics of Wind-Induced Vibration of Catenary[J]. Journal of Southwest Jiaotong University. doi: 10.3969/j.issn.0258-2724.20250497
Citation: MIN Yongzhi, ZHANG Zhihui, HU Yanwen, WANG Guo, ZHANG Tingrong, ZHAO Shanpeng. Finite Element Numerical Simulation and Experimental Verification of Frequency Characteristics of Wind-Induced Vibration of Catenary[J]. Journal of Southwest Jiaotong University. doi: 10.3969/j.issn.0258-2724.20250497

接触网风致振动频率特性的有限元数值模拟及试验验证

doi: 10.3969/j.issn.0258-2724.20250497
基金项目: 声光电信息融合的铁路牵引供电系统关键设备服役状态检测技术(24JRRA852);国铁集团系统性重大科技项目(P2024G001);国家自然科学基金项目(52467017);甘肃省科技厅联合科研基金项目(24JRRA852)
详细信息
    作者简介:

    闵永智(1975—),男,教授,博士,研究方向为人工智能测试、图像识别和电气化铁路多源接入,E-mail:minyongzhi@mail.lzjtu.cn

    通讯作者:

    胡延文(1990—),男,副教授,博士,研究方向为无线传能,E-mail:2622898791@qq.com

  • 中图分类号: U225.1

Finite Element Numerical Simulation and Experimental Verification of Frequency Characteristics of Wind-Induced Vibration of Catenary

  • 摘要:

    接触网风致振动是多风地区铁路供电系统的典型灾害,现有振动特性理论分析与有限元软件难以准确模拟现场条件,导致其计算结果难以使用现场测量数据进行验证,不利于后续非线性模型计算精度提高,为此搭建了小比例接触网模型. 首先在MATLAB中编写集成了接触网大变形几何非线性与吊弦伸缩刚度非线性的有限元数值计算程序,求解小比例接触网模型在不同频率横向激励作用下的振型,其次搭建横向激励频率可调的试验平台,采用激光位移传感器测量各个频率水平气流作用下的振型,最后对比研究两种方法所得振动波形. 计算结果表明,在一定频率范围内,模型振动频率与横向激励频率相同,且横向激励频率等于模型基频时,其水平最大位移距离达到最大;不同频率横向激励作用下测量点运动轨迹不同,频率小于基频时运动轨迹多为“8”字形,大于基频时主要为扁椭圆形,等于基频时则几乎为水平直线. 对比试验结果可知:有限元数值计算方法可准确计算模型的基频和激励下的响应频率、振型以及振幅随频率的变化趋势,但其振幅计算值与试验结果存在显著偏差. 因此,对关键振幅值的计算与预测还需结合试验修正.

     

  • 图 1  负弛度法计算过程

    Figure 1.  Calculation process of negative sag method

    图 2  平衡状态接触网形状

    Figure 2.  Shape of catenary in equilibrium state

    图 3  吊弦长度计算误差

    Figure 3.  Calculation error of suspension string length

    图 4  不同张力下测量点水平位移

    Figure 4.  Horizontal displacement of measuring point under different tensions

    图 5  模型振动特性(6.0 Hz)

    Figure 5.  Vibration characteristics of model (6.0 Hz)

    图 6  模型振动特性(9.5 Hz)

    Figure 6.  Vibration characteristics of model (9.5 Hz)

    图 7  模型振动特性(13.0 Hz)

    Figure 7.  Vibration characteristics of model (13.0 Hz)

    图 8  试验结构图

    Figure 8.  Diagram of experimental structure

    图 9  不同张力下试验测量点水平位移图

    Figure 9.  Diagram of horizontal displacement of experimental measurement points under different tensions

    图 10  试验模型测量点水平位移时程曲线(6.0 Hz)

    Figure 10.  Time-history curve of horizontal displacement of measuring point in experimental model (6.0 Hz)

    图 11  试验模型测量点水平位移时程曲线(9.5 Hz)

    Figure 11.  Time-history curve of horizontal displacement of measuring point in experimental model (9.5 Hz)

    图 12  试验模型测量点水平位移时程曲线(13.0 Hz)

    Figure 12.  Time-history curve of horizontal displacement of measuring point in experimental model (13.0 Hz)

    图 13  不同频率激励对应的最大振幅

    Figure 13.  Maximum amplitude corresponding to excitations of different frequencies

    表  1  接触网主要参数

    Table  1.   Main parameters of catenary

    结构 材质 杨氏模量/
    Gpa
    质量密度/
    kg•m−3
    张力/
    kN
    接触线 CuMg 0.5 AC120 120 8900 27
    承力索 BzII 120 120 8900 21
    吊弦 Bz 10 120 8900
    下载: 导出CSV

    表  2  试验模型主要参数

    Table  2.   Main parameters of experimental model

    结构 材料 杨氏模量/Gpa 质量密度/(kg•m−3) 张力/N
    接触线 铜线 103 8516 8.3
    承力索 铜线 103 8516 5.4
    吊弦 铜线 103 8516
    下载: 导出CSV

    表  3  模型承力索与接触线对应张力

    Table  3.   Corresponding tensions of carrier cable and contact line in model

    参数模型1模型2模型3
    承力索张力/N5.46.48.3
    接触线张力/N8.38.310.3
    下载: 导出CSV
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  • 收稿日期:  2025-09-26
  • 修回日期:  2026-01-06
  • 网络出版日期:  2026-07-03

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