深部隧道爆破开挖诱发围岩损伤与扰动效应数值分析

余浪浪, 王志亮, 汪书敏, 李松玉. 深部隧道爆破开挖诱发围岩损伤与扰动效应数值分析[J]. 水文地质工程地质, 2023, 50(5): 117-123. doi: 10.16030/j.cnki.issn.1000-3665.202208059
引用本文: 余浪浪, 王志亮, 汪书敏, 李松玉. 深部隧道爆破开挖诱发围岩损伤与扰动效应数值分析[J]. 水文地质工程地质, 2023, 50(5): 117-123. doi: 10.16030/j.cnki.issn.1000-3665.202208059
YU Langlang, WANG Zhiliang, WANG Shumin, LI Songyu. Numerical analysis of damage and disturbance effect of surrounding rocks induced by deep tunnel blast excavation[J]. Hydrogeology & Engineering Geology, 2023, 50(5): 117-123. doi: 10.16030/j.cnki.issn.1000-3665.202208059
Citation: YU Langlang, WANG Zhiliang, WANG Shumin, LI Songyu. Numerical analysis of damage and disturbance effect of surrounding rocks induced by deep tunnel blast excavation[J]. Hydrogeology & Engineering Geology, 2023, 50(5): 117-123. doi: 10.16030/j.cnki.issn.1000-3665.202208059

深部隧道爆破开挖诱发围岩损伤与扰动效应数值分析

  • 基金项目: 国家自然科学基金项目(12272119);国家自然科学基金雅砻江联合基金项目(U1965101)
详细信息
    作者简介: 余浪浪(1999-),男,硕士研究生,主要从事岩石动力学方面的研究。E-mail:yulanglang1999@163.com
    通讯作者: 王志亮(1969-),男,博士,教授,博士生导师,主要从事岩石力学特性与损伤破坏机理方面的研究。E-mail:cvewzL@hfut.edu.cn
  • 中图分类号: U455.6;P642.3

Numerical analysis of damage and disturbance effect of surrounding rocks induced by deep tunnel blast excavation

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  • 现阶段,不同地应力条件下深部岩体受爆破作用的损伤破坏分析尚显不足。为了研究深部隧道围岩爆破开挖损伤破坏规律,基于有限元软件ANSYS/LS-DYNA,采用Riedel-Hiermaier-Thoma本构模型,对不同地应力环境下隧道爆破效果影响因素、围岩扰动范围等问题进行数值分析。结果表明:双向等压隧道的断面损伤程度与地应力水平呈负相关;随着地应力上升,地应力对隧道底板的损伤抑制作用渐为明显;隧道腰部围岩受爆破扰动较为突出,其应力和振动速度均随侧压力系数增大而大幅升高,且振动速度增幅超过40%,明显高于顶部围岩;在垂直应力20 MPa条件下,腰部测点应力、振动速度幅值随侧压力系数增加而增大的趋势较缓;当垂直应力升高至60 MPa时,侧压力系数对围岩扰动的影响较大。相关结论对实际工程施工具有重要指导意义,同时对隧道围岩稳定性监测与支护参数优化具有一定参考价值。

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  • 图 1  1/2隧道有限元模型

    Figure 1. 

    图 2  炮孔与测点布置图(单位:cm)

    Figure 2. 

    图 3  不同应力水平下开挖损伤分布图

    Figure 3. 

    图 4  不同地应力水平下两测点的应变时程曲线

    Figure 4. 

    图 5  不同k值下开挖损伤分布图

    Figure 5. 

    图 6  不同k值下X方向应力时程图

    Figure 6. 

    图 7  不同k值影响下X方向振动速度时程图

    Figure 7. 

    图 8  垂直应力下k对应力、振动速度峰值的影响

    Figure 8. 

    表 1  堵塞材料主要参数

    Table 1.  Main parameters of the stemmed material

    参数密度
    /(kg·m−3
    剪切模量
    /GPa
    泊松比A0A1A2Pc
    取值1 8000.0640.33.4×10−137.03×10−70.3−6.9×10−8
      注:A0A1A2为屈服函数常量;Pc为拉伸压力切断值。
    下载: 导出CSV

    表 2  炸药的主要参数

    Table 2.  Main parameters of explosive

    炸药参数密度/(kg·m−3爆速/(m∙s−1A/PaR1R2E0/(J·m−3
    取值1 5007 4506.25×10115.251.60.086×1011
    下载: 导出CSV

    表 3  空气材料主要参数

    Table 3.  Main parameters of air

    空气参数ρ0/(kg·m−3C4C5E/(J∙m−3
    取值1.20.40.42.5×105
    下载: 导出CSV

    表 4  大理岩RHT主要参数

    Table 4.  Main parameters of the marble RHT model

    大理岩参数密度/(kg· m−3弹性模量/GPaB0B1T1/GPaT2/GPaANfc/MPa
    取值276312.430.90.946.7201.650.56130
    大理岩参数$f_{\rm{s}}^*$$f_{\rm{t}}^* $Q0BE0C/s−1E0T/s−1EC/s−1ET/s−1βc
    取值0.250.10.01050.73.0×10–53.0×10–63.0×10253.0×10250.009756
    大理岩参数βt$g_{\rm{c}}^* $$g_{\rm{t}}^* $ξD1D2$\varepsilon_{\rm{p}}^{\rm{m}} $AfNf
    取值0.013330.780.70.440.03710.011.590.62
    大理岩参数A1/GPaA2/GPaA3/GPaPcrush/MPaPcomp/GPaNpα0
    取值46.7242.05–4.3243.33641.078
      注:B0B1T1T2为状态方程参数;AN为失效面参数;fc为抗压强度;$f_{\rm{s}}^* $$f_{\rm{t}}^* $为相对抗压、抗拉强度;Q0B为Lode角相关系数;E0CE0T为参考压缩、拉伸应变率;ECET为压缩、拉伸应变率;βcβt为压缩、拉伸应变率指数;$ g_{\rm{c}}^*$$g_{\rm{t}}^* $为压缩、拉伸屈服面参数;ξ为剪切模量折减系数;D1D2为损伤参数;$\varepsilon_{\rm{p}}^{\rm{m}} $为最小损伤残余应变;AfNf为剩余表面参数;A1A2A3为Hugoniot系数;PcrushPcomp为挤压、压实强度;Np为孔隙指数;α0为孔隙度。
    下载: 导出CSV
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出版历程
收稿日期:  2022-08-22
修回日期:  2022-11-28
刊出日期:  2023-09-15

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