爆破振动下海底隧道涌水量预测研究

李嘉诚, 王渭明, 吕显州, 王晓杰, 潘志新. 爆破振动下海底隧道涌水量预测研究[J]. 水文地质工程地质, 2023, 50(4): 127-136. doi: 10.16030/j.cnki.issn.1000-3665.202205055
引用本文: 李嘉诚, 王渭明, 吕显州, 王晓杰, 潘志新. 爆破振动下海底隧道涌水量预测研究[J]. 水文地质工程地质, 2023, 50(4): 127-136. doi: 10.16030/j.cnki.issn.1000-3665.202205055
LI Jiacheng, WANG Weiming, LYU Xianzhou, WANG Xiaojie, PAN Zhixin. Research on the prediction method of water gushing volume under the blasting vibration effect of a sub-sea tunnel[J]. Hydrogeology & Engineering Geology, 2023, 50(4): 127-136. doi: 10.16030/j.cnki.issn.1000-3665.202205055
Citation: LI Jiacheng, WANG Weiming, LYU Xianzhou, WANG Xiaojie, PAN Zhixin. Research on the prediction method of water gushing volume under the blasting vibration effect of a sub-sea tunnel[J]. Hydrogeology & Engineering Geology, 2023, 50(4): 127-136. doi: 10.16030/j.cnki.issn.1000-3665.202205055

爆破振动下海底隧道涌水量预测研究

  • 基金项目: 山东省自然科学基金(ZR2021QE187)
详细信息
    作者简介: 李嘉诚(1997-),男,硕士研究生,主要从事地下空间与隧道工程。E-mail: 985621237@qq.com
    通讯作者: 吕显州(1990-),男,博士,讲师,主要从事城市与矿山地下工程软岩变形控制与施工参数优化等方面的研究。E-mail: lyuxianzhou0608@sdust.edu.cn
  • 中图分类号: U459.5

Research on the prediction method of water gushing volume under the blasting vibration effect of a sub-sea tunnel

More Information
  • 爆破振动效应下海底隧道涌水量预测目前仍是一个难题。以青岛地铁1号线瓦屋庄站—贵州路站过海区间海底隧道为工程背景,基于等效连续介质模型,利用镜像法推导考虑损伤区因素的海底隧道涌水量计算公式,通过正演与反演的方式,结合数值模拟计算结果以及实际工程监测结果综合验证公式的正确性并分析损伤区因素对涌水量的影响机制。结果表明:爆破振动产生的挤压作用使得隧道周边围岩孔隙水压力会在短时间内急速上升,到达峰值后随着爆破振动的减弱及消失开始缓慢下降;在损伤区因素影响下,隧道涌水量随着损伤区厚度增加逐渐变大,但不会随着损伤区渗透系数的增加而不断增加;数值模拟计算考虑爆破损伤区与否的隧道涌水量比值为1.4,与文章所推公式计算结果1.342相比误差仅为4.1%,且计算结果与现场实测结果相比仅少0.53 m3/(d·m),相对于传统计算公式结果更接近实测结果,说明本文计算公式适用于考虑损伤区因素的隧道涌水量计算,具有较高的工程应用价值。

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  • 图 1  海底隧道等价圆模型

    Figure 1. 

    图 2  镜像法计算示意图

    Figure 2. 

    图 3  损伤区及外围岩水头损失示意图

    Figure 3. 

    图 4  数值模型网格图

    Figure 4. 

    图 5  自振频率计算所得位移时程曲线及爆破荷载曲线

    Figure 5. 

    图 6  施工前后水压力场对比

    Figure 6. 

    图 7  孔隙水压力场随时间步的变化

    Figure 7. 

    表 1  国内外最大涌水量(q0)传统计算公式

    Table 1.  Traditional calculation formula of the maximum water inflow at home and abroad

    名称 公式
    大岛洋志公式[10] ${ { {q} }_0} = \dfrac{ {2\text{π} { {K} }m\left( {H + {H_0} - r} \right)} }{ {\ln\left[{ {4\left( {H + {H_0} - r} \right)} }/{d} \right]} }$
    古德曼经验式[11] ${ { {q} }_0} = \dfrac{ {2\text{π}{ {K} }\left( {H + {H_0} } \right)} }{ {\ln\left[{ {4\left( {H + {H_0} } \right)} }/{d}\right] } }$
    铁路规范经验式[12] ${q_0} = \dfrac{ {2\text{π} { {K} }\left( {H + {H_0} + { {r} } } \right)} }{ {\ln({ {2H} }/{r}) } }$
      注:表中变量解释见图1
    下载: 导出CSV

    表 2  岩体物理力学计算参数

    Table 2.  Physical mechanical calculating parameters of rock mass

    地层名称 厚度/m 弹性模量/GPa 泊松比 密度/(kg·m−3 黏聚力/MPa 内摩擦角/(°) 抗拉强度/MPa
    强风化凝灰岩 1.80 0.15 0.40 2 000.00 0.01 40.00 1.00
    中风化凝灰岩 3.50 20.00 0.30 2 600.00 12.00 50.00 3.40
    微风化凝灰岩 74.70 45.00 0.28 2 700.00 25.00 70.00 5.00
    初期衬砌 0.10 30.00 0.28 1 800.00
    二次衬砌 0.45 46.00 0.20 2 500.00
      注:表中空格表示此项无数据。下同。
    下载: 导出CSV

    表 3  岩体水理参数

    Table 3.  Hydraulic parameters of rock mass

    地层名称 渗透系数
    /(m·d−1
    渗透率
    /m2
    孔隙率 体积模量
    /GPa
    切变模量
    /GPa
    强风化凝灰岩 0.0550 6.4×10−11 0.39 0.25 0.053
    中风化凝灰岩 0.0430 5×10−11 0.30 16.70 7.700
    微风化凝灰岩 0.0180 2.1×10−11 0.12 34.10 17.600
    初砌 0.0008 9.3×10−16 22.70 11.700
    二衬 0.0003 3.22×10−16 35.20 18.100
    下载: 导出CSV

    表 4  工况模拟详情

    Table 4.  Details of working condition simulation

    工况 计算条件
    1 无爆破、无渗流条件下隧道开挖施工模拟
    2 无爆破时,渗流条件下隧道开挖施工模拟
    3 流固耦合效应下隧道钻爆开挖施工模拟
    下载: 导出CSV

    表 5  海底隧道涌水量计算结果

    Table 5.  Calculating results of water inflow from submarine tunnels

    起止里程 q0/(m3·d–1·m–1
    大洋岛志公式[10] 古德曼经验式[11] 规范经验式[12] 工况2数值模拟结果 工况3数值模拟结果 现场实测结果 本文公式计算结果
    K28+410—K28+480 1.86 2.59 2.88 3.24 4.54 4.01 3.48
    下载: 导出CSV
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出版历程
收稿日期:  2022-05-18
修回日期:  2023-02-24
刊出日期:  2023-07-15

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