吉林大学学报(工学版) ›› 2025, Vol. 55 ›› Issue (7): 2354-2364.doi: 10.13229/j.cnki.jdxbgxb.20230871

• 交通运输工程·土木工程 • 上一篇    

集束群钉装配式钢-混组合梁桥自振特性与车桥耦合分析

范亮1,2(),曾文1,文强1,赵富裕3,徐英铭4   

  1. 1.重庆交通大学 土木工程学院,重庆 400074
    2.重庆交通大学 山区桥梁及隧道工程国家重点实验室,重庆 400074
    3.中国建筑第八工程局有限公司西南分公司,成都 610041
    4.重庆市开州区交通局,重庆 405400
  • 收稿日期:2023-08-16 出版日期:2025-07-01 发布日期:2025-09-12
  • 作者简介:范亮(1979-),女,教授,博士.研究方向:桥梁工程.E-mail: fanliang@cqjtu.edu.cn
  • 基金资助:
    国家自然科学基金项目(U20A20312);重庆市技术创新与应用发展专项重点项目(CSTB2022TIAD - KPX0103)

Vibration characteristics of prefabricated steel-concrete composite beam bridges with clustered grouping bolt connection and analysis of vehicle-bridge coupling

Liang FAN1,2(),Wen ZENG1,Qiang WEN1,Fu-yu ZHAO3,Ying-ming XU4   

  1. 1.School of Civil Engineering,Chongqing Jiaotong University,Chongqing 400074,China
    2.State Key Laboratory of Mountain Bridge and Tunnel Engineering,Chongqing Jiaotong University,Chongqing 400074,China
    3.Southwest Branch,China Construction Eighth Engineering Bureau Co. ,Ltd. ,Chengdu 610041,China
    4.Chongqing Kaizhou District Transportation Bureau,Chongqing 405400,China
  • Received:2023-08-16 Online:2025-07-01 Published:2025-09-12

摘要:

为研究考虑集束群钉非连续剪力连接影响的装配式钢-混组合梁桥动力特性,基于欧拉梁理论和Rayleigh-Ritz法,推导了该类组合梁桥自振特性理论公式,构建了多点不连续剪力约束的装配式组合梁桥车桥耦合模型,分析了路面不平整度、车速、车体质量和集束度对组合梁桥车载动力响应及冲击效应影响特征。结果表明:集束度越大,无剪力连接区越长,桥梁刚度和固有频率越低;路面不平整度提高,冲击系数增大;车速对动力响应影响呈非线性,当车速由100 km/h提高至120 km/h时,冲击系数突增68.10%,车速对动力性能影响显著;车辆质量越大,冲击系数越大,动力响应越强;集束度由0增至0.31时,最大动位移增长较静位移增长略高,冲击系数降低5.25%,集束度对冲击系数影响不显著。

关键词: 桥梁工程, 车桥耦合, 自振特性, 有限元, 不平整度, 冲击系数

Abstract:

In order to study the dynamic characteristics of assembled steel-concrete composite beam bridges considering the influence of discontinuous shear connection caused by cluster-group bolts, a theoretical formula for the self-vibration characteristics of this type of composite girder bridges based on the Euler beam theory and Rayleigh-Ritz method was proposed. A coupled model of the assembled composite beam bridge with multi-point discontinuous shear constraints was established to analyze the effects of road roughness, vehicle speed, vehicle mass, and clustering degree on the dynamic response of the composite beam bridge under vehicle loading and the impact characteristics. The results indicate that as the clustering degree increases and the length of the shear-free connection zone becomes longer, the bridge stiffness and natural frequency decrease. An increase in road roughness leads to a higher impact coefficient. The influence of vehicle speed on dynamic response shows nonlinearity, and when the vehicle speed increases from 100 km/h to 120 km/h, the impact coefficient suddenly increases by 68.10%, significantly affecting the dynamic performance. A greater vehicle mass results in a larger impact coefficient and stronger dynamic response. For clustering degrees ranging from 0 to 0.31, the increase in maximum dynamic displacement is slightly higher than the increase in static displacement, leading to a decrease of 5.25% in the impact coefficient. The effect of clustering degree on the impact coefficient is not significant.

Key words: bridge engineering, vehicle-bridge coupling, natural vibration characteristics, finite element, road roughness, impact coefficient

中图分类号: 

  • TU318.1

图1

集束栓钉连接的钢-混组合梁桥结构"

图2

组合梁的剪力连接区布置"

图3

截面上某点的位移图"

图4

简化车辆模型图"

图5

梁桥模型"

图6

跨中挠度曲线验证"

图7

箱梁桥横断面图"

表1

集束栓钉连接的钢-混双箱梁桥自振频率"

阶数振型图

ωs

/Hz

ωc

/Hz

ωs-ωcωs/%
12.2192.0238.83
25.1404.9922.88
37.3387.1163.03
47.8027.2347.28

图8

路面不平整度的动力响应"

图9

冲击系数随路面等级变化趋势"

表2

施加在光滑路面上的最大动、静位移与冲击系数"

位移与冲击系数光滑B级C级D级
?max/mm10.06710.36911.04013.358
?'max/mm6.3296.3296.3296.329
μ0.5900.6380.7441.111

图10

不同车辆速度动力响应"

图11

冲击系数随车辆速度变化趋势"

表3

仿真得到的最大动、静位移与冲击系数"

位移与冲击系数车速/(km·h-1
406080100120
?max/mm9.82210.63610.3698.98910.800
?'max/mm6.3296.3296.3296.3296.329
μ0.5520.6810.6380.4200.706

图12

不同车体质量动力响应"

图13

冲击系数变化趋势"

表4

车体质量模拟得到的最大动、静位移与冲击系数"

位移与

冲击系数

车体质量/t
1520253035
?max/mm4.5606.0918.12210.15012.110
?'max/mm3.3544.3115.2686.2257.183
μ0.3600.4130.5420.6300.687

图14

不同集束度动力响应"

图15

冲击系数随集束度变化趋势"

表5

集束度模拟得到的最大动、静位移与冲击系数"

位移与

冲击系数

集束度
0(均布)0.040.060.080.120.31
?max/mm9.9679.9869.99410.01610.05110.356
?'max/mm6.2636.3006.3156.3476.4006.722
μ0.5920.5850.5830.5780.5710.541
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