寒区考虑非均质特性的隧道衬砌及围岩应力位移统一弹塑性解

IF 2.3 4区 地球科学 Q4 GEOGRAPHY, PHYSICAL
Bin Wang , ZiHao Zhang , XiuLing Liang , ChuanXin Rong , HaiBing Cai
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The displacement in the elastic zone of the frozen surrounding rock intensified with increasing relative radius, whereas the shift in the plastic zone experienced a gradual decline. The displacement of the inner wall of the lining was always greater than that of the outer wall, and this phenomenon occurred only after the frozen surrounding rock exhibited a plastic zone. The maximum displacements of the liner in its elastically limited and plastically limited states were 1.39, 1.77, 2.28, and 2.37 mm and 15.93, 25.51, 44.28, and 48.58 mm based on the Drucker–Prager (DP), Mohr–Coulomb (MC), Tresca, and double-shear strength criteria, respectively; the maximum limit displacements of the frozen surrounding rock were 12.74, 20.41, 35.43, and 38.87 mm and 85.32, 103.38, 569.23, and 680.43 mm, respectively. 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引用次数: 0

摘要

由于温度场的存在,寒冷地区隧道的衬砌和围岩表现出不均匀的材料特性。本研究考虑了这些特性对隧道结构完整性的影响。通过建立弹塑性力学模型,推导了五种不同弹塑性状态下的应力和位移解析解,并基于不同屈服准则进行了比较。结果表明:随着相对半径的增大,衬砌弹性区的位移先减小后增大,而塑性区的位移则继续增大;冻结围岩弹性区的位移随相对半径的增大而增大,塑性区的位移则逐渐减小。衬砌内墙的位移总是大于外墙的位移,这种现象只有在冻结围岩出现塑性区后才会发生。基于Drucker-Prager (DP)、Mohr-Coulomb (MC)、Tresca和双剪强度准则,衬垫在弹性和塑性极限状态下的最大位移分别为1.39、1.77、2.28和2.37 mm和15.93、25.51、44.28和48.58 mm;冻结围岩最大极限位移分别为12.74、20.41、35.43、38.87 mm和85.32、103.38、569.23、680.43 mm。随着相对半径的增大,衬砌和冻结围岩内的径向应力均增大;衬砌弹性区切向应力减小,塑性区切向应力变化规律相反。冻结围岩和衬砌的切向应力表现出相同的变化趋势。根据4种不同强度准则计算,衬砌的弹塑性极限承载力分别为1.81、2.31、2.95、3.07 MPa和3.31、4.84、7.48、8.05 MPa,冻结围岩的弹塑性极限承载力分别为8.52、13.24、22.17、24.18 MPa和16.76、32.46、74.15、85.64 MPa。此外,随着塑性区的扩大,r2位置切向应力突变的现象逐渐减弱。研究结果可为寒冷地区隧道的设计和施工提供一定的理论指导。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Unified elastoplastic solution for the stress and displacement of tunnel lining and surrounding rock in cold areas considering heterogeneous characteristics
The lining and surrounding rock around tunnels constructed in cold areas exhibit nonuniform material properties due to the existence of a temperature field. This study considered the effects of these properties on the integrity of tunnel structures. By establishing an elastoplastic mechanical model, analytical solutions to the stress and displacement under five different elastoplastic states were derived and compared based on distinct yield criteria. The findings showed that with increasing relative radius, the displacement in the lining elastic zone initially decreased before increasing, whereas the shift in the plastic zone continued to increase. The displacement in the elastic zone of the frozen surrounding rock intensified with increasing relative radius, whereas the shift in the plastic zone experienced a gradual decline. The displacement of the inner wall of the lining was always greater than that of the outer wall, and this phenomenon occurred only after the frozen surrounding rock exhibited a plastic zone. The maximum displacements of the liner in its elastically limited and plastically limited states were 1.39, 1.77, 2.28, and 2.37 mm and 15.93, 25.51, 44.28, and 48.58 mm based on the Drucker–Prager (DP), Mohr–Coulomb (MC), Tresca, and double-shear strength criteria, respectively; the maximum limit displacements of the frozen surrounding rock were 12.74, 20.41, 35.43, and 38.87 mm and 85.32, 103.38, 569.23, and 680.43 mm, respectively. With increasing relative radius, the radial stresses within both the lining and the frozen surrounding rock intensified; and the tangential stress in the elastic zone of the lining decreased whereas the opposite change rule was observed in the plastic zone. The tangential stresses in the frozen surrounding rock and lining exhibited the same variation trend. Based on calculations with four distinct strength criteria, the elastic and plastic ultimate bearing capacities of the lining were 1.81, 2.31, 2.95, and 3.07 MPa, and 3.31, 4.84, 7.48, and 8.05 MPa, while those of the frozen surrounding rock were 8.52, 13.24, 22.17, and 24.18 MPa, and 16.76, 32.46, 74.15, and 85.64 MPa. In addition, with the expansion of the plastic zone, the phenomenon of a sudden change in the tangential stress at location r2 became progressively attenuated. The study findings can provide some theoretical guidance for the design and construction of tunnels in cold areas.
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