Improved calculation method for settlement of rectangular pipe jacking based on random medium theory and Peck formula
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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。Abstract: The calculation of the settlement caused by pipe jacking has always been a critical aspect in the design of pipe jacking engineering. The commonly used Peck formula was summarized on the basis of a large number of circular pipe jacking, and there are some errors in the application of rectangular pipe jacking. The random medium theory, which is suitable for both circular and rectangular pipe jacked, only gives the integral formula without the final integral calculation result, which leads to the complex calculation process and is difficult to be applied in engineering design. This study improves the integrand function in the random medium theory, proposes a simpler approximation function, and derives the final integration result, which greatly simplifies the calculation process. The relative error between the calculated result of the improved method and the measured settlement value (except for some measuring points) is approximately 5%, which indicates that the improved method demonstrates reasonable accuracy. The improved method was used to analyze the influence of various factors on the surface settlement, which provides a reference for future engineering design.
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Key words:
- rectangular pipe jacking /
- settlement /
- random medium theory /
- Peck formula
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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 (ξ′1,η′1) $ \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 (ξ′2,η′1) 左下 (ξ1,η2) 左下 (ξ′1,η′2) 右下 (ξ2,η2) 右下 (ξ′2,η′2) 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 -
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