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    基于间接边界元方法的SH波倾斜入射下边坡动力响应特征

    周剑 张路青

    周剑, 张路青, 2022. 基于间接边界元方法的SH波倾斜入射下边坡动力响应特征. 地球科学, 47(12): 4350-4361. doi: 10.3799/dqkx.2022.363
    引用本文: 周剑, 张路青, 2022. 基于间接边界元方法的SH波倾斜入射下边坡动力响应特征. 地球科学, 47(12): 4350-4361. doi: 10.3799/dqkx.2022.363
    Zhou Jian, Zhang Luqing, 2022. Dynamic Response Analysis of Slope Rock Mass with Complex Shape Based on Indirect Boundary Element Method. Earth Science, 47(12): 4350-4361. doi: 10.3799/dqkx.2022.363
    Citation: Zhou Jian, Zhang Luqing, 2022. Dynamic Response Analysis of Slope Rock Mass with Complex Shape Based on Indirect Boundary Element Method. Earth Science, 47(12): 4350-4361. doi: 10.3799/dqkx.2022.363

    基于间接边界元方法的SH波倾斜入射下边坡动力响应特征

    doi: 10.3799/dqkx.2022.363
    基金项目: 

    国家重点研发计划项目 2019YFC1509703

    国家自然科学基金资助项目 41972287

    详细信息
      作者简介:

      周剑(1985-), 男, 研究员, 从事工程地质与岩体力学方面的研究工作.ORCID: 0000-0003-4093-250X.E-mail: zhoujian@bjut.edu.cn

    • 中图分类号: P64

    Dynamic Response Analysis of Slope Rock Mass with Complex Shape Based on Indirect Boundary Element Method

    • 摘要:

      地震作用下山体边坡的动力响应规律与地震波入射角度显著相关,本文基于间接边界元方法研究SH波倾斜入射下边坡的动力响应特征.基于间接边界元理论研发了用于边坡岩体动力响应分析的边界元程序,通过计算平直裂隙对弹性波的反射及散射波波场对程序进行验证,并详细探讨了不同类型的边坡在各种入射角度的应力波作用下的响应特性.SH波铅直向入射时,半圆形凹陷地形的谷肩位置地震动振幅最小,而半圆形凸起地形的最高点位置振幅最大,单面坡的坡肩位置地震动最大,楔形凸起地形的坡顶地震动最强烈;当SH波入射角增大,各类边坡的最大地震动力响应位置也有所偏移,地震放大系数亦随之变化;以樟木镇边坡为实例揭示了复杂形态边坡岩体中的局部凸起对地震动的放大作用.研究结果表明,边坡微地形特征对地震动力响应影响非常大,凸起山体坡顶的动力放大效应最为显著;同一边坡在不同入射角地震波作用下产生的动力放大系数以及发生的位置不同.本文的研究结果对评价坡体稳定性和边坡工程抗震防设等具有重要的指导意义.

       

    • 图  1  应力波以三个角度分别入射结构面的模型

      Fig.  1.  Model of the stress wave with three incident angles

      图  2  平直裂隙位移差计算结果与解析值比较图

      a.0°入射; b.30°入射; c.60°入射

      Fig.  2.  Comparison of calculation results of straight fracture displacement difference and analytic solution

      图  3  半圆形凹陷和凸起模型(单位m)

      a.凹陷地形; b.凸起地形

      Fig.  3.  Semicircular concave and convex models

      图  4  半圆形模型表面的波动曲线及相应点振幅

      a.凹陷地形; b.凸出地形

      Fig.  4.  Wave curves and amplitudes of corresponding points on the surface of the model

      图  5  不同坡角的单面坡模型

      Fig.  5.  Single slope model with different slope angles

      图  6  单面坡模型在SH波作用下地震动放大系数

      a.0°入射; b.30°入射; c.60°入射

      Fig.  6.  Ground motion amplification factor of single slope model under SH wave action

      图  7  楔形凹陷河谷模型

      Fig.  7.  Model of wedge-shaped concave valleys

      图  8  楔形凹陷河谷模型在SH波作用下地震动放大系数

      a.0°入射; b.15°入射; c.30°入射

      Fig.  8.  Ground motion amplification factor for model of wedge-shaped concave valleys under SH wave action

      图  9  楔形山脊地貌模型

      Fig.  9.  Model of wedge-shaped convex valleys

      图  10  楔形山脊地貌模型在SH波作用下地震动放大系数

      a.0°入射; b.15°入射; c.30°入射

      Fig.  10.  Ground motion amplification factor for model of wedge-shaped convex valleys under SH wave action

      图  11  樟木镇某斜坡剖面模型

      Fig.  11.  Profile model of a slope in Zhangmu Town

      图  12  樟木斜某坡体剖面地震动响应曲线及对应位置的振幅

      a.0°入射; b.30°入射; c.60°入射

      Fig.  12.  Ground motion response curves and amplitudes of the corresponding position for the profile model of a slope in Zhangmu Town

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    出版历程
    • 收稿日期:  2022-06-28
    • 网络出版日期:  2023-01-10
    • 刊出日期:  2022-12-25

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