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竹巴龙金沙江大桥水毁破坏机理

杨万理 秦军武 侯海林 吴文博 周凌远

杨万理, 秦军武, 侯海林, 吴文博, 周凌远. 竹巴龙金沙江大桥水毁破坏机理[J]. 西南交通大学学报, 2022, 57(1): 120-128. doi: 10.3969/j.issn.0258-2724.20200732
引用本文: 杨万理, 秦军武, 侯海林, 吴文博, 周凌远. 竹巴龙金沙江大桥水毁破坏机理[J]. 西南交通大学学报, 2022, 57(1): 120-128. doi: 10.3969/j.issn.0258-2724.20200732
YANG Wanli, QIN Junwu, HOU Hailin, WU Wenbo, ZHOU Lingyuan. Failure Mechanism of Flood Damage to Jinsha River Bridge at Zhubalong[J]. Journal of Southwest Jiaotong University, 2022, 57(1): 120-128. doi: 10.3969/j.issn.0258-2724.20200732
Citation: YANG Wanli, QIN Junwu, HOU Hailin, WU Wenbo, ZHOU Lingyuan. Failure Mechanism of Flood Damage to Jinsha River Bridge at Zhubalong[J]. Journal of Southwest Jiaotong University, 2022, 57(1): 120-128. doi: 10.3969/j.issn.0258-2724.20200732

竹巴龙金沙江大桥水毁破坏机理

doi: 10.3969/j.issn.0258-2724.20200732
基金项目: 国家自然科学基金 (51678491);四川省科技厅重点研发计划 (2019YFG0001, 2019YFG0460);四川省科技计划(2021JDTD0012)
详细信息
    作者简介:

    杨万理(1979—),男,教授,博士,研究方向为滨海结构波流力,E-mail:68360903@qq.com

    通讯作者:

    周凌远(1969—),男,教授,博士,研究方向为桥梁结构,E-mail:1090511907@qq.com

  • 中图分类号: U447

Failure Mechanism of Flood Damage to Jinsha River Bridge at Zhubalong

  • 摘要:

    为了研究竹巴龙金沙江大桥的破坏机理,基于泄洪实测数据,并考虑T梁底部横隔板腔室中裹挟空气的影响,建立了该桥1∶20缩尺数值仿真模型,对洪水作用下简支T梁桥上部结构洪水作用力特征、流场特征和破坏机理开展了深入研究. 研究结果表明:当淹没率不超过1.342时,水平力系数随淹没率的增大而增大,当淹没率大于1.342时,水平力系数随淹没率的增大逐渐减小;在壅水翻越护栏前,竖向力和倾覆弯矩系数随着淹没率的增大而逐渐增大;当壅水翻越护栏后,竖向力和倾覆弯矩系数将急剧减小;在淹没率接近1.000时,上部结构发生破坏的风险最大;该桥破坏过程中首先发生了水平运动,随后大概率发生上浮和翻转,梁体运动导致挡块破坏,部分梁体在跌落中发生翻转;实心栏杆贡献了多达31%的水平力,裹挟空气对竖向力的贡献最高达到18%,实心栏杆和裹挟空气是引起该桥水毁破坏或加速该桥破坏的重要原因.

     

  • 图 1  白格堰塞湖泄洪冲毁竹巴龙金沙江大桥

    Figure 1.  Jinsha River Bridge at Zhubalong destroyed by discharge from Baige landslide dam

    图 2  梁体淹没深度与断面平均流速

    Figure 2.  Submergence depth of beam body and average velocity at cross section

    图 3  实桥T梁跨中断面(单位:cm)

    Figure 3.  Cross section at middle span of actual T-girder bridge (unit: cm)

    图 4  数值模拟简化模型示意

    Figure 4.  Simplified model for numerical simulation

    图 5  $ {h}^{\mathrm{*}}= $ 0.805,1.000,1.678时水流力时程曲线

    Figure 5.  Time histories of flow force for cases with $ {\mathit{h}}^{\mathit{*}}= $ 0.805, 1.000 and 1.678

    图 6  工况h* = 1.678中t = 1413.894 s时刻云图

    Figure 6.  Contour of case with h* = 1.678 at t = 1413.894 s

    图 7  水流力系数随着淹没率 $ {h}^{\mathrm{*}} $的变化趋势(不考虑壅水漫顶)

    Figure 7.  Variation trend of flow force coefficient with submergence ratio $ {\mathit{h}}^{\mathit{*}} $ (backwater overtopping is not considered)

    图 8  节段梁体洪水作用力和相应的抗力随 $ {h}^{\mathrm{*}} $变化趋势(不考虑壅水漫顶)

    Figure 8.  Variation trend of flood force and resistance of segmental beam with submergence ratio $ {\mathit{h}}^{\mathit{*}} $ (backwater overtopping is not considered)

    图 9  上部结构破坏形态

    Figure 9.  Failure modes of superstructure

    图 10  竹巴龙金沙江大桥破坏情况

    Figure 10.  Damage of Jinsha River Bridge at Zhubalong

    图 11  水流力系数随着淹没率 $ {h}^{\mathrm{*}} $变化趋势(壅水漫顶)

    Figure 11.  Variation of flow force coefficient with submergence ratio $ {\mathit{h}}^{\mathit{*}} $ (backwater overtopping)

    图 12  节段梁体作用力和相应的抗力随淹没率 $ {h}^{\mathrm{*}} $变化趋势(壅水漫顶)

    Figure 12.  Variation of flood force and resistance of segmental beam with submergence ratio $ {\mathit{h}}^{\mathit{*}} $ (backwater overtopping)

    表  1  CFD数值模拟计算工况

    Table  1.   Cases of CFD numerical simulation

    工况$ {h}^{*} $流速/(m•s−1)工况$ {h}^{*} $流速/(m•s−1)
    C1 0.336 0.136 C10 1.342 0.235
    C2 0.671 0.190 C11 1.678 0.250
    C3 0.805 0.212 C12 2.013 0.275
    C4 0.872 0.223 C13 2.349 0.295
    C5 0.889 0.226 C14 2.685 0.316
    C6 0.906 0.229 C15 3.02 0.335
    C7 0.940 0.235 C16 3.691 0.380
    C8 0.973 0.242 C17 4.362 0.438
    C9 1.007 0.248 C18 5.369 0.532
    下载: 导出CSV

    表  2  网格划分精细程度对数值模拟计算精度和计算效率的影响

    Table  2.   Influence of grids generation accuracy on calculation precision and efficiency of numerical simulation

    工况y+dcb/mmN/个T/hCDCL
    模型试验         1.250 −1.240
    粗糙 60 3 413086 11 1.176 −1.259
    中等 45 2 507650 23 1.224 −1.124
    精细 30 1 701862 36 1.238 −1.157
    下载: 导出CSV
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出版历程
  • 收稿日期:  2020-10-29
  • 修回日期:  2021-04-19
  • 网络出版日期:  2021-11-22
  • 刊出日期:  2021-04-22

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