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    一種塊體–顆粒–桿件的耦合方法及其在隧道支護模擬中的應用

    李曉光 李長洪 馮春

    李曉光, 李長洪, 馮春. 一種塊體–顆粒–桿件的耦合方法及其在隧道支護模擬中的應用[J]. 工程科學學報, 2023, 45(6): 1023-1033. doi: 10.13374/j.issn2095-9389.2022.03.25.005
    引用本文: 李曉光, 李長洪, 馮春. 一種塊體–顆粒–桿件的耦合方法及其在隧道支護模擬中的應用[J]. 工程科學學報, 2023, 45(6): 1023-1033. doi: 10.13374/j.issn2095-9389.2022.03.25.005
    LI Xiao-guang, LI Chang-hong, FENG Chun. A block–particle–bar coupled algorithm to simulate tunnel excavation and support[J]. Chinese Journal of Engineering, 2023, 45(6): 1023-1033. doi: 10.13374/j.issn2095-9389.2022.03.25.005
    Citation: LI Xiao-guang, LI Chang-hong, FENG Chun. A block–particle–bar coupled algorithm to simulate tunnel excavation and support[J]. Chinese Journal of Engineering, 2023, 45(6): 1023-1033. doi: 10.13374/j.issn2095-9389.2022.03.25.005

    一種塊體–顆粒–桿件的耦合方法及其在隧道支護模擬中的應用

    doi: 10.13374/j.issn2095-9389.2022.03.25.005
    基金項目: 國際科技創新合作專項資助項目(2018YFE0101100);佛山市人民政府科技創新專項—產學研合作資助項目(BK20BE008)
    詳細信息
      通訊作者:

      E-mail: fengchun@imech.ac.cn

    • 中圖分類號: TG142.71

    A block–particle–bar coupled algorithm to simulate tunnel excavation and support

    More Information
    • 摘要: 為了模擬隧道開挖過程中邊幫的失穩垮塌過程以及錨桿對隧道的支護過程,提出了一種基于罰彈簧的塊體–顆粒–桿件的耦合方法。該耦合方法基于連續–非連續的數值模擬方法(CDEM),采用離散顆粒簇表征隧道周邊松動圈以內的破碎巖體,采用塊體單元表征松動圈以外的完整巖體,采用桿件單元描述錨桿及錨索等桿系類支護結構,采用插值耦合的方式實現桿件單元與離散顆粒及塊體單元間力與位移的傳遞,從而實現高應力環境下隧道開挖失穩過程的模擬及支護效果的評價。顆粒與塊體之間采用1根法向線性彈簧及2根切向線性彈簧進行耦合,法向彈簧引入拉伸斷裂本構,切向彈簧引入Mohr–Coulomb脆性斷裂本構。桿件與顆粒及桿件與塊體之間的耦合模式基本一致,包含1根沿著桿件軸向的罰彈簧Sgn及1根垂直于桿件軸向的罰彈簧SgsSgn主要用于描述桿件與圍巖之間的拉拔效應及推壓效應,Sgs則主要用于描述桿件與圍巖之間的側向擠壓效應。圓形盾構隧道彈性場分析、預應力錨桿加固矩形巷道模擬、全長連接錨桿對巖塊的錨固作用分析、以及碎裂巖體中的隧道開挖支護效果分析等案例,證明了本文所述塊體–顆粒–桿件耦合算法的準確性及合理性。

       

    • 圖  1  塊體–顆粒–桿件耦合示意圖

      Figure  1.  Block–particle–bar coupling model

      圖  2  塊體–顆粒間的接觸耦合示意

      Figure  2.  Block–particle coupling model

      圖  3  塊體–桿件間的插值耦合示意

      Figure  3.  Block–bar coupling model

      圖  4  桿件與圍巖之間的拉拔(推壓)失效示意. (a)軸向視圖;(b)側向視圖

      Figure  4.  Pull and push failure between the bar and surrounding rock: (a) axial view; (b) lateral view

      圖  5  桿件與圍巖之間的側向擠壓失效示意. (a)軸向視圖;(b)側向視圖

      Figure  5.  Lateral compression failure between the bar and surrounding rock: (a) axial view; (b) lateral view

      圖  6  顆粒–桿件間的插值耦合示意

      Figure  6.  Particle–bar coupling model

      圖  7  圓形隧道數值模型

      Figure  7.  Numerical model of a circular shield tunnel

      圖  8  數值解與理論解的對比

      Figure  8.  Comparison of numerical and analytical solutions

      圖  9  矩形巷道預應力錨桿支護數值模型

      Figure  9.  Numerical model of a rectangular tunnel reinforced by prestressed rock bolts

      圖  10  最小主應力云圖

      Figure  10.  Contour of the minimal principal stress

      圖  11  典型錨桿上的軸力分布

      Figure  11.  Axial force distribution of typical anchors

      圖  12  錨桿加固巖塊的計算模型

      Figure  12.  Numerical model of rock reinforced by full-anchored bolts

      圖  13  錨桿加固后巖塊上的豎向應力云圖

      Figure  13.  Vertical stress contour of the rock reinforced by full-anchored bolts

      圖  14  錨桿上的軸力變化規律

      Figure  14.  Distribution law of the axial force on the bolts

      圖  15  隧道開挖支護模型

      Figure  15.  Tunnel excavation support model

      圖  16  三種模擬工況下隧道的總位移云圖. (a)工況A; (b)工況B; (c)工況C

      Figure  16.  Displacement magnitude contour of the tunnel under three numerical cases: (a) case A; (b) case B; (c) case C

      圖  17  錨桿中的軸力分布

      Figure  17.  Axial force distribution in bolts

      圖  18  錨桿的破壞狀態

      Figure  18.  Failure state of bolts

      圖  19  典型錨桿軸力的變化規律

      Figure  19.  Relationship between axial force and bolt length

      圖  20  典型錨桿軸向位移的變化規律

      Figure  20.  Relationship between axial displacement and bolt length

      表  1  力學參數

      Table  1.   Mechanical parameters

      MaterialsDensity/(kg·m–3)Elasticity
      modulus/
      GPa
      Poisson’s
      ratio
      Cohesion/MPaTensile
      strength/MPa
      Internal friction
      angle/(°)
      Dilation angle/(°)
      Surrounding rock2200100.3332510
      Broken zone220050.33112010
      Lining structure2500360.25843515
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    出版歷程
    • 收稿日期:  2022-03-25
    • 網絡出版日期:  2022-05-17
    • 刊出日期:  2023-05-31

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