Please wait a minute...
J4  2011, Vol. 45 Issue (9): 1657-1663    DOI: 10.3785/j.issn.1008-973X.2011.09.024
    
Dynamic response of tunnel in viscoelastic saturated
soil subjected to blast loads
CAI Yuan-qiang1, CHEN Cheng-zhen2, SUN Hong-lei1
1.MOE Key Laboratory of Soft Soils and Geoenvironmental Engineering, Zhejiang University,
Hangzhou 310058,China;2.China Resources Land(Suzhou)Limited, Suzhou 215000, China
Download:   PDF(0KB) HTML
Export: BibTeX | EndNote (RIS)      

Abstract  

The dynamic response of a circular tunnel in the viscoelastic poroelastic soil was investigated using an analytical method to provide theoretical basis for antiblast protection design of tunnel. Assuming that the blast occured in the center of the circular tunnel, a model was established using decrease three-stage triangle loads. Biots theory was used to describe saturated soil and Kelvin-Voigt model was used for soil skeleton. The motions of the liner were considered specially based on Flügge theory. By introducing potential functions, numerical results were obtained in time-domain by using the Laplace transforms and inversion of Laplace transforms. The curves of displacement and hoop stress with time for different b*, which denotes the permeability of the soil, on the interface between the liner and soil were presented, and compared with those of the single-phase medium. The influences of viscous damping coefficient η on the displacement and stress response were emphatically analyzed in the viscoelastic saturated soil. The results show that the amplituds of displacement and hoop stress increase with the increasing parameter b*. The amplitudes of displacement and stress in the viscoelastic saturated soil are smaller than that in the viscoelastic medium. With the increasing of η, the amplitude of the wave attenuates fast, whereas the maximum the displacement and stress response get smaller.



Published: 01 September 2011
CLC:  TU 435  
Cite this article:

CAI Yuan-qiang, CHEN Cheng-zhen, SUN Hong-lei. Dynamic response of tunnel in viscoelastic saturated
soil subjected to blast loads. J4, 2011, 45(9): 1657-1663.

URL:

https://www.zjujournals.com/eng/10.3785/j.issn.1008-973X.2011.09.024     OR     https://www.zjujournals.com/eng/Y2011/V45/I9/1657


黏弹性饱和土中隧道在爆炸荷载作用下的动力响应

为了给隧道的抗爆防护设计提供理论依据,采用解析法研究了爆炸荷载作用下黏弹性饱和土体中圆形隧道的动力响应问题.假定爆炸发生在圆形隧道中心处,爆炸荷载采用峰值递减的三段突加三角形荷载,应用Biot波动方程模拟饱和土体,将土骨架视为KelvinVoigt饱和土体,衬砌运动方程基于Flügge壳体理论,通过引入势函数,利用Laplace变换及数值逆变换,得到爆炸荷载作用下土体响应的时域计算结果,给出了在不同土体渗透性参数b*时的黏弹性饱和土中位移、应力的时程曲线,并与单相介质进行了对比;讨论了黏滞阻尼系数η对黏弹性饱和土中位移和应力响应的影响.数值分析结果表明:在爆炸荷载作用下,b*越大,位移和应力幅值振荡越显著,黏弹性饱和土中应力和位移响应幅值小于单相介质;在黏弹性饱和土中,η值越大,波衰减越快,位移和应力响应峰值越小.

[1] CHEUNG Y K,ZHU J X. Dynamic interaction analysis of a circular cylindrical shell of finite length in a halfspace[J]. Earthquake Engineering & Structural Dynamics,1992,21(9): 799-809.
[2] 曹志远,曾三平.爆炸波作用下地下防护结构与围岩的非线性动力相互作用分析[J].爆炸与冲击,2003,23(5):385-390.
CAO Zhiyuan, ZENG Sanping. Nonlinear dynamic interaction between under ground structure and surrounding medium under blast loading[J]. Explosion and Shock Waves,2003,23(5): 385-390.
[3] ABOZENA A M. Radiation form a finite cylindrical explosive source[J].Geophysics,1977,42(7): 1384-1393.
[4] ZAKOUT U, AKKAS N. Transient response of a cylindrical cavity with and without a bonded shell in an infinite elastic medium[J]. International Journal of Engineering Science, 1981,19(5):1341-1352.
[5] SENJUNTICHAI T, RAJAPAKSE R K N D. Transient response of a circular cavity in a poroelastic medium[J]. International Journal for Numerical and Analytical Method in Geomechanics, 1993, 17(5): 357-383.
[6] 杨俊,宫全美,吴世明,等.饱和土体中圆柱形孔洞的动力分析[J].上海力学,1996,17(1):37-44.
YANG Jun,GONG Quanmei,WU Shiming. Transient response of a cylindrical cavity in a saturated soil body[J]. Shanghai Journal of Mechanics,1996, 17(1):37-44.
[7] XIE Kanghe, LIU Ganbin, SHI Zuyuan. Dynamic response of partially sealed circular tunnel in viscoelastic saturated soil[J]. Soil Dynamic and Earthquake Engineering, 2004, 24(3): 1003-1011.
[8] BIOT M A.Mechanics of deformation and acoustic propagation in porous medium[J].Journal of Applied Physics,1962,33(4):1482-1498.
[9] 楼梦麟, 林皋.黏弹性地基中人工边界的波动反射效应[J].水利学报,1986,22(6):20-30.
LOU Mengling, LIN Gao. Reflection effects of fluctuations of artificial boundary in Viscoelastic foundation[J]. Journal of Hydraulic Engineering,1986, 22(6):20-30.
[10] 曹玉忠,卢泽生. 抗爆容器内爆炸流场数值模拟[J]. 高压物理学报, 2001, 15(2): 127-132.
CAO Yuzhong, LU Zesheng. Numerical simulations of blast flowfields in closed blastresistant containers[J]. Chinese Journal of High Pressure Physics, 2001, 15(2): 127-132.
[11] DURBIN F. Numerical inversion of Laplace transformation : An efficient improvement to Durbin and Abateps method[J]. The Computer Journal , 1974 ,17 (4) : 371-376.
[12] HONIG G, HIRDES U. A method for the numerical inversion of Laplace transforms[J]. Journal of Computational and Applied Mathematics, 1984, 10(1): 113-132.

[1] WEN Min-jie, XU Jin-ming, LI Qiang. Comparative analysis for torsional vibration of an end-bearing pile in saturated viscoelastic soil[J]. J4, 2013, 47(12): 2146-2152.
[2] GAO Hua-xi, WEN Min-jie, ZHANG Bin. Dynamic response of nearly saturated viscoelastic soil with circular tunnel[J]. J4, 2013, 47(4): 615-621.
[3] WANG Peng, DING Guang-ya, CAI Yuan-qiang, WANG Jun. Analysis model for dynamic vibration of
embedded foundation excited by plane waves
[J]. J4, 2012, 46(12): 2224-2230.
[4] HOU Jian, XIA Tang-dai, SUN Miao-miao, KONG Xiang-bing. Multiple scattering of plane SH wave by arbitrary configuration of
rigid pile as barrier for vibration isolation
[J]. J4, 2012, 46(7): 1269-1274.
[5] HU Xiu-Jing, CA Yuan-Jiang, XU Chang-Jie. Dynamic response factor for rocking vibration of embedded
foundation in saturated soil
[J]. J4, 2010, 44(5): 935-941.