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高内压力下引水隧洞透水衬砌限裂理论分析研究

陈洁 王艳强 乐萍 董启暖 曹亚军 王伟

陈洁, 王艳强, 乐萍, 董启暖, 曹亚军, 王伟. 高内压力下引水隧洞透水衬砌限裂理论分析研究[J]. 岩土工程技术, 2025, 39(4): 567-575. doi: 10.20265/j.cnki.issn.1007-2993.2024-0317
引用本文: 陈洁, 王艳强, 乐萍, 董启暖, 曹亚军, 王伟. 高内压力下引水隧洞透水衬砌限裂理论分析研究[J]. 岩土工程技术, 2025, 39(4): 567-575. doi: 10.20265/j.cnki.issn.1007-2993.2024-0317
Chen Jie, Wang Yanqiang, Le Ping, Dong Qinuan, Cao Yajun, Wang Wei. Analytical study on the crack limitation theory of permeable lining of diversion tunnels under high internal pressure[J]. GEOTECHNICAL ENGINEERING TECHNIQUE, 2025, 39(4): 567-575. doi: 10.20265/j.cnki.issn.1007-2993.2024-0317
Citation: Chen Jie, Wang Yanqiang, Le Ping, Dong Qinuan, Cao Yajun, Wang Wei. Analytical study on the crack limitation theory of permeable lining of diversion tunnels under high internal pressure[J]. GEOTECHNICAL ENGINEERING TECHNIQUE, 2025, 39(4): 567-575. doi: 10.20265/j.cnki.issn.1007-2993.2024-0317

高内压力下引水隧洞透水衬砌限裂理论分析研究

doi: 10.20265/j.cnki.issn.1007-2993.2024-0317
基金项目: 中国博士后基金面上项目(2021M690047)
详细信息
    作者简介:

    陈 洁,男,1995年生,硕士,主要从事地下隧道工程研究。E-mail:chenjie@ssdepci.com

    通讯作者:

    乐 萍,女,2001年生,在读硕士研究生,主要从事水工隧洞衬砌设计工程研究。E-mail:1173958714@qq.com

  • 中图分类号: TV31

Analytical study on the crack limitation theory of permeable lining of diversion tunnels under high internal pressure

  • 摘要: 为了研究高内水压力下引水隧洞衬砌开裂的影响因素,进而对衬砌限裂进行优化设计,基于透水衬砌理论确定了透水衬砌的设计步骤,并给出了钢筋混凝土衬砌不同裂缝宽度的计算公式,结合实际工程,分别采用中国规范和美国规范的裂缝宽度计算公式计算得到混凝土衬砌配筋方案,并对混凝土衬砌裂缝宽度的影响因素进行了分析。结果表明:(1)中国规范计算得到的配筋面积比美国规范要更大,钢筋的应力更小;(2)影响混凝土裂缝宽度的影响因素主要有内水压力、配筋面积、渗透系数和衬砌的厚度,可以通过调整这几种影响因素来限制混凝土开裂。

     

  • 图  1  厚壁圆筒计算模型

    图  2  配筋面积对裂缝宽度的影响

    图  3  衬砌厚度对裂缝宽度的影响

    图  4  保护层厚对裂缝宽度的影响

    图  5  隧洞半径对裂缝宽度的影响

    图  6  渗透系数对裂缝宽度的影响

    图  7  内水压力对裂缝宽度的影响

    表  1  厚壁圆筒模型解析计算公式

    计算工况 衬砌混凝土未开裂 衬砌混凝土已开裂
    径向应力 $ \sigma\mathrm{_r}=\dfrac{(p_1-p_2)}{2(1-\mu)}\left(\dfrac{\mathrm{ln}\;\left(r_2/r\right)}{\mathrm{ln}\;t}+\dfrac{1-r_2^2/r^2}{t^2-1}\right) $ $ {\sigma }_{\rm{r}}=\dfrac{{(2-\mu )(p}_{1}-{p}_{2})}{3(1-\mu )}\left(\dfrac{1-{r}_{2}^{2}/{r}^{2}}{{t}^{2}-1}+\dfrac{{r}_{2}-r}{{r}_{2}-{r}_{1}}\right) $
    环向应力 $ \sigma{_{{\text{θ}}}}=\dfrac{(p_1-p_2)}{2(1-\mu)}\left(\dfrac{\mathrm{ln}\;\left(r_2/r\right)+1-2\mu}{\mathrm{ln}\;t}+\dfrac{1+r_2^2/r^2}{t^2-1}\right) $ $ \sigma_{{{\text{θ}}}}=\dfrac{(2-\mu)(p_1-p_2)}{3(1-\mu)}\left(\dfrac{1+r_2^2/r^2}{t^2-1}+\dfrac{r_2}{r_2-r_1}-\dfrac{(1+\mu)r}{(r_2-r_1)(2-\mu)}\right) $
    位移 $ {u}_{\rm{r}}=\dfrac{r{(p}_{1}-{p}_{2}\left)\right(1+\mu )}{2E(1-\mu )}\left(\dfrac{(1-2\mathrm{\mu })(\mathrm{l}\mathrm{n}\;\left({r}_{2}/r\right)+1-\mathrm{\mu })}{\mathrm{l}\mathrm{n}\; t}+\dfrac{1-2\mu +{r}_{2}^{2}/{r}^{2}}{{t}^{2}-1}\right) $ $ {u}_{\rm{r}}=\dfrac{r{(p}_{1}-{p}_{2}\left)\right(1+\mu \left)\right(2-\mu )}{3E(1-\mu )}\left(\dfrac{(1-2\mathrm{\mu })\left[\right(2-\mathrm{\mu }){r}_{2}-\mathrm{r}]}{({r}_{2}-{r}_{1})(2-\mu )}+\dfrac{1-2\mu +{r}_{2}^{2}/{r}^{2}}{{t}^{2}-1}\right) $
    下载: 导出CSV

    表  2  中、美规范中混凝土最大裂缝计算公式

    规范或方法 计算公式
    《水工混凝土结构设计规范》
    (SL 191—2008)[14]
    $ w\mathrm{_{\rm{max}}}=\alpha\dfrac{\sigma_{\mathrm{sk}}}{E_{\mathrm{s}}}\left(0.03+c+0.07\dfrac{d}{\rho_{\mathrm{te}}}\right) $
    《水工隧洞设计规范》
    (SL 279—016)[15]
    $ w_{\mathrm{max}}=2\left(\dfrac{\sigma_{\mathrm{s}}}{E_{\mathrm{s}}}\phi-0.7\times10^{-4}\right)l_{\mathrm{f}} $
    Z系数法[17] $ w_{\mathrm{max}}=1.1\beta f_{\mathrm{s}}\sqrt[3]{d\mathrm{_c}A}\times10^{-5} $
    Frosch法[19] $ w\mathrm{_{\rm{max}}}=2\dfrac{f\mathrm{_s}}{E_{\mathrm{s}}}\beta\sqrt[]{d_{\mathrm{c}}^2+\left(\dfrac{s}{2}\right)^2} $
    Broms-Lutz法[20] $ w\mathrm{_{\rm{max}}}=1.45\sigma_{\mathrm{s}}\sqrt[3]{d\mathrm{_c}A}\times10^{-5} $
    注:《水工混凝土结构设计规范》(SL 191—2008)中,$ \alpha $为考虑构件受力特征和荷载长期作用的综合影响系数,本文按轴心受拉计算,取$ \alpha $=2.4;$ \sigma\mathrm{_{sk}} $为纵向受拉钢筋的应力,MPa;$ E_{\mathrm{s}} $为钢筋的杨氏模量,$ \mathrm{M}\mathrm{P}\mathrm{a} $;$ c $为保护层厚度,mm;$ d $为钢筋的直径,mm;$ \rho\mathrm{_{te}} $为钢筋的配筋率。《水工隧洞设计规范》(SL279—2016)中,$ \sigma\mathrm{_s} $为纵向受拉钢筋的应力,MPa;$ E\mathrm{_s} $为钢筋的杨氏模量,MPa;$ \phi $为裂缝间纵向受拉钢筋应变不均匀系数,当$ \phi $<0.3时,取0.3;$ l\mathrm{_f} $为平均裂缝间距,m;Z系数法中,$ \beta $为钢筋到界面受拉边缘的应变梯度的影响,在本文中,近似取1.2;$ f\mathrm{_s} $为受拉钢筋应力,MPa;$ d\mathrm{_c} $从受拉区底面至最靠近该面的受拉钢筋界面形心的距离,mm;$ A $为包围一根钢筋的混凝土截面面积。Frosch法中,$ f\mathrm{_s},\beta,d_{\mathrm{c}},E\mathrm{_s} $均与上述相同,$ s $为钢筋的间距,mm;Broms-Lutz法中,参数含义均与上述相同。
    下载: 导出CSV

    表  3  计算参数

    计算参数取值
    内水压力/MPa1.3
    衬砌外径/m11.8
    衬砌内径/m11
    保护层厚度/mm25
    围岩弹性模量/GPa4
    围岩泊松比0.35
    围岩渗透系数/(m·s–15×10−6
    单位弹抗系数/(MPa·cm–112.5
    衬砌混凝土弹性模量/GPa28
    衬砌混凝土泊松比0.167
    衬砌混凝土渗透系数/(m·s–11×10−9
    钢筋弹性模量/GPa200
    围岩渗透半径/m118
    下载: 导出CSV

    表  4  采用 《水工隧洞设计规范》(SL 279—2016)限裂宽度计算公式透水衬砌配筋计算结果

    钢筋的直径/m钢筋的间距/m钢筋的面积/mm2脱开水头/MPa衬砌与围岩接触面之间的水压力$ {p}_{2} $/MPa钢筋应力/MPa裂缝宽度/mm
    0.0200.2001570.7960.2631.138608.0981.992
    0.0220.2001900.6640.2671.134516.3251.520
    0.0250.2002454.3690.2751.126418.4221.065
    0.0280.2003078.7610.2841.117350.8580.782
    0.0300.2003534.2920.2911.110316.8740.651
    0.0320.2004021.2390.2991.103289.2060.549
    0.0360.2005089.3800.3161.087247.3400.442
    0.0400.2006283.1850.3371.068217.6030.414
    0.0200.1003141.5930.2911.109358.9680.574
    0.0220.1003801.3270.3031.097314.4520.450
    0.0250.1004908.7390.3241.078266.9760.393
    0.0280.1003141.5930.3501.056234.0940.366
    0.0300.1003801.3270.3691.039217.4400.349
    0.0320.1004908.7380.3901.022203.7710.333
    0.0360.1006157.5240.4380.985182.7460.304
    0.0400.1007068.5830.4950.944167.3500.279
    下载: 导出CSV

    表  5  工程案例1最终配筋方案对比

    规范 配筋方案 钢筋应力
    /MPa
    裂缝宽度
    /mm
    《水工混凝土结构设计规范》
    (SL 191—2008)
    ϕ36@100 155.197 0.291
    《水工隧洞设计规范》
    (SL 279—2016)
    ϕ40@100 167.350 0.279
    Z系数法 ϕ30@100 262.525 0.173
    Frosch法 ϕ25@100 214.545 0.265
    Broms-Lutz法 ϕ25@200 274.932 0.251
    下载: 导出CSV

    表  6  工程案例2最终配筋方案对比

    规范 配筋方案 钢筋应力
    /MPa
    裂缝宽度
    /mm
    《水工混凝土结构设计规范》
    (SL 191—2008)
    ϕ40@100 142.002 0.284
    《水工隧洞设计规范》
    (SL 279—2016)
    ϕ40@100 181.325 0.298
    Z系数法 ϕ36@200 287.680 0.239
    Frosch法 ϕ28@100 237.806 0.294
    Broms-Lutz法 ϕ30@100 282.616 0.205
    下载: 导出CSV
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  • 收稿日期:  2024-07-11
  • 修回日期:  2024-10-23
  • 录用日期:  2024-10-29
  • 刊出日期:  2025-08-08

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