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基于随机介质理论和Peck公式的矩形顶管地表沉降改进计算方法

沈青松 陈烨 叶盛华 吉乔伟 王强

沈青松, 陈烨, 叶盛华, 吉乔伟, 王强. 基于随机介质理论和Peck公式的矩形顶管地表沉降改进计算方法[J]. 岩土工程技术, 2025, 39(4): 504-510. doi: 10.20265/j.cnki.issn.1007-2993.2024-0214
引用本文: 沈青松, 陈烨, 叶盛华, 吉乔伟, 王强. 基于随机介质理论和Peck公式的矩形顶管地表沉降改进计算方法[J]. 岩土工程技术, 2025, 39(4): 504-510. doi: 10.20265/j.cnki.issn.1007-2993.2024-0214
Shen Qingsong, Chen Ye, Ye Shenghua, Ji Qiaowei, Wang Qiang. Improved calculation method for settlement of rectangular pipe jacking based on random medium theory and Peck formula[J]. GEOTECHNICAL ENGINEERING TECHNIQUE, 2025, 39(4): 504-510. doi: 10.20265/j.cnki.issn.1007-2993.2024-0214
Citation: Shen Qingsong, Chen Ye, Ye Shenghua, Ji Qiaowei, Wang Qiang. Improved calculation method for settlement of rectangular pipe jacking based on random medium theory and Peck formula[J]. GEOTECHNICAL ENGINEERING TECHNIQUE, 2025, 39(4): 504-510. doi: 10.20265/j.cnki.issn.1007-2993.2024-0214

基于随机介质理论和Peck公式的矩形顶管地表沉降改进计算方法

doi: 10.20265/j.cnki.issn.1007-2993.2024-0214
详细信息
    作者简介:

    沈青松,男,1996年生,博士,工程师,主要研究方向为市政管线及地下工程。E-mail:shen_qs1@hdec.com

  • 中图分类号: TU992

Improved calculation method for settlement of rectangular pipe jacking based on random medium theory and Peck formula

  • 摘要: 顶管施工引起的地表沉降计算是顶管工程设计中的关键环节。常用的peck公式是在总结大量圆形顶管的基础上得到的,在矩形顶管的应用中存在一定误差。圆形和矩形顶管都适用的随机介质理论只给出了积分公式,没有最终的积分计算结果,导致计算过程复杂,难以在工程设计中推广应用。本研究对随机介质理论中的被积函数进行改进处理,提出更为简单的近似函数,并推导得到最终积分结果,从而大幅简化计算过程。改进方法计算结果与工程实测沉降值(除个别测点外)的相对误差在5%左右,表明改进方法具有一定的准确度。利用该方法分析研究了各种因素对地表沉降的影响,为后续工程设计提供参考依据。

     

  • 图  1  被积原函数与改进函数

    图  2  沉降计算示意图

    图  3  工程实测沉降值与改进计算结果

    图  4  不同顶管宽度、高度对应的沉降

    图  5  不同顶管埋深和土体系数对应的沉降

    图  6  不同偏移位置和土体损失量对应的沉降

    表  1  矩形顶管开挖区域坐标计算

    区域 坐标位置 坐标 计算公式 区域 坐标位置 坐标 计算公式
    顶管区域 左上 (ξ1,η1) $ \begin{gathered} {\xi _1} = - a \\ {\xi _2} = a \\ {\eta _1} = H - b \\ {\eta _2} = H + b \\ \end{gathered} $ 超挖区域 左上 (ξ1,η1) $ \begin{gathered} \xi {'_1} = - a - \Delta {a_1} \\ \xi {'_2} = a + \Delta {a_2} \\ \eta {'_1} = H - b - \Delta {b_1} \\ \eta {'_2} = H + b + \Delta {b_2} \\ \end{gathered} $
    右上 (ξ2,η1) 右上 (ξ2,η1)
    左下 (ξ1,η2) 左下 (ξ1,η2)
    右下 (ξ2,η2) 右下 (ξ2,η2)
    下载: 导出CSV

    表  2  顶管四周超挖量

    偏移位置 四周超挖量 土体损失量 四周超挖量
    上偏 Δa1=Δa2=0.05 m; Δb1=0 m; Δb2=0.1 m 0.60 Δa1=Δa2=Δb1=Δb2=0.03 m
    下偏 Δa1=Δa2=0.05 m; Δb1=0.1 m; Δb2=0 m 0.80 Δa1=Δa2=Δb1=Δb2=0.04 m
    居中 Δa1=Δa2=Δb1=Δb2=0.05 m 1.01 Δa1=Δa2=Δb1=Δb2=0.05 m
    左偏 Δa1=0 m;Δa2=0.1 m; Δb1=Δb2=0.05 m 1.21 Δa1=Δa2=Δb1=Δb2=0.06 m
    右偏 Δa1=0.1 m;Δa2=0 m; Δb1=Δb2=0.05 m 1.42 Δa1=Δa2=Δb1=Δb2=0.07 m
    下载: 导出CSV
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出版历程
  • 收稿日期:  2024-05-17
  • 修回日期:  2024-09-26
  • 录用日期:  2025-01-02
  • 刊出日期:  2025-08-08

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