Technical Papers
Jul 6, 2022

Three-Dimensional Seismic Bearing Capacity Assessment of Heterogeneous and Anisotropic Slopes

Publication: International Journal of Geomechanics
Volume 22, Issue 9

Abstract

This study proposed an effective approach to accurately evaluate the three-dimensional (3D) seismic bearing capacity of heterogeneous and anisotropic slopes in the framework of the upper-bound limit analysis theorem. An improved discretized horn mechanism was first developed so that the properties of heterogeneous and anisotropic soils could be involved in the slope stability analysis. To incorporate the impact of seismic forces, the modified pseudo dynamic approach was adopted, which ensured that the complete time-history of the seismic-induced ground movement, the soil-damping properties, and the amplification effect could be considered in this study. The seismic bearing capacity of slopes was then calculated by using a method that integrated the upper-bound limit analysis theorem and the modified pseudo dynamic approach. The proposed method was validated by comparisons with previous analytical solutions for some available cases, showing that the proposed method is an effective approach to determine the 3D seismic bearing capacity of heterogeneous and anisotropic slopes. The effects of model parameters on the ultimate bearing capacity and the critical failure surface are then presented. Finally, the influence of pore–water pressure on the seismic slope stability is discussed.

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Acknowledgments

The first author thanks the financial support from the China Scholarship Council project (CSC No. 202006370322). This study is also financially supported by the National Key R&D Program of China (2017YFB1201204).

Notation

The following symbols are used in this paper:
Aj
element area of the surface Pmax,jPmax,j+1Pmax,j+1Pmax,j;
ah0 and av0
horizontal and vertical seismic accelerations at the slope toe;
B
width of the slope failure mechanism;
b
width of plane insert;
CF and CF
boundaries of failure mechanism;
Cs, Csz, Ss, Ssz, ys1, ys2, Cp, Sp, Cpz, Spz, yp1 and yp2
dimensionless functions;
c
soil cohesion;
ch0 and cht
horizontal principal cohesions at the slope crest and the slope toe;
cj
horizontal cohesion at the depth zj;
cv
vertical principal cohesion;
cɛi,j and cεi,j
soil cohesions at the points Pi,j and Pi,j;
g
gravity acceleration;
H
slope height;
hi,j and hi,j
vertical distances from points Pi,j and Pi,j to the slope surface;
Kc
anisotropic cohesion coefficient;
kh and kv
horizontal and vertical seismic acceleration coefficients at the slope toe;
nj and nj
unit normal vectors of the vectors PjPj+1 and PjPj+1;
Pi,j, Pi+1,j, Pi,j+1, Pi+1,j+1, Qi,j, Qi+1,j, Qi,j+1 and Qi+1,j+1
points at the failure surface;
Ri,j and Ri,j
distances between the centers of the elements Pi,jPi+1,jPi+1,j+1 and Pi,jPi,j+1Pi+1,j+1Pi+1,j to the rotation axis;
Pj and Pj
points at the discretized boundaries of the failure surface;
Pmax,j and Pmax,j
last points of the failure surface at the radial plane ψj and the radial plane ψj;
qcr
ultimate bearing capacity;
qj
surcharge acting on the surface Aj;
Rj
radius of the radial plane ψj;
rF
rotation radius of point F;
rh and rh
rotation radius of points C and C′;
rj, rj, rj+1 and rj+1
rotation radius of points Pj, Pj, Pj+1, and Pj+1;
ru
pore–water pressure coefficient;
r0 and r0
rotation radius of points A and A′;
Sh and Sp
areas of surfaces for the horn failure part and plane-strain insert part;
Si,j and Si,j
areas of the surfaces Pi,jPi+1,jPi+1,j+1 and Pi,jPi,j+1Pi+1,j+1Pi+1,j;
Sm
area of the failure surface at the slope crest;
Sr
area of surface at the slope crest and the slope surface;
St
area of the velocity discontinuity surface bounding the failure mechanism;
T
period of the harmonic seismic acceleration;
t
time;
u
pore–water pressure;
uhb and uvb
horizontal and vertical seismic accelerations at the slope base;
uhs(zi, t) and uvs(zi, t)
horizontal and vertical displacement at depth zi and time t;
uh0 and uv0
horizontal and vertical seismic accelerations at the slope toe;
Vi,j
volume of the element Pi,jPi+1,jPi+1,j+1Qi,jQi+1,jQi+1,j+1 (or Pi,jPi,j+1Pi+1,j+1Qi,jQi,j+1Qi+1,j+1) (Fig. 4);
Vs and Vp
velocity of shear and primary wave propagating;
vj and vj
unit normal vectors of vectors OPj and OPj;
WD
internal energy dissipation rate;
Wq
work rate of the static surcharge at the slope crest;
Wqs
work rate of the earthquake-induced inertia forces from the surcharge on the slope crest;
Wu
work rate of pore–water pressure;
Wγ
work rate of the soil weight;
Wγs
work rate of seismic forces;
zi and zj
depth from points Pi and Pj to the slope crest;
αi
angle between line CjPi,j with the negative y axis at the local coordinate axis;
β
slope angle;
δθ
angle between lines OPj and OPj+1 or lines OPj and OPj+1;
δj+1
unit vector of the vector OPj+1;
ɛi,j
angle between the major principal stress σ1 with the vertical direction;
γ
soil unit weight;
η
ratio between the vertical seismic acceleration coefficient kv and the horizontal seismic acceleration coefficient kh (kv = ηkh);
φ
internal friction angle;
φi,j and φi,j
friction angles at points Pi,j and Pi,j;
φj
friction angle at the depth zj;
φ0 and φt
friction angles at the slope crest and the slope toe;
λ
angle between the plane perpendicular to major principal stress σ1 and failure surface;
θGi,j and RGi,j
polar coordinates of the barycenter corresponding to the volume Vi,j;
θi,j
angle between the point Pi,j and rotation axis;
θ0, θh, θj and θF
angles between lines OA, OC, OPj and OF with the horizontal direction;
σ1
major principal stress;
ω
angular velocity of the failure mechanism;
ϖ
angle velocity of the shear/primary wave;
ξ
soil damping ratio; and
ψj
radial plane at the failure surface.

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International Journal of Geomechanics
Volume 22Issue 9September 2022

History

Received: Oct 30, 2021
Accepted: Mar 29, 2022
Published online: Jul 6, 2022
Published in print: Sep 1, 2022
Discussion open until: Dec 6, 2022

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Ph.D. Student, School of Civil Engineering, Central South Univ., Changsha, Hunan 410075, PR China. ORCID: https://orcid.org/0000-0002-7051-4424. Email: [email protected]
Jin-Feng Zou [email protected]
Professor, School of Civil Engineering, Central South Univ., Changsha, Hunan 410075, PR China. Email: [email protected]
Yu-Ming Sheng [email protected]
Ph.D. Student, School of Civil Engineering, Central South Univ., Changsha, Hunan 410075, PR China (corresponding author). Email: [email protected]
Jing-Yu Chen [email protected]
Ph.D. Student, School of Civil Engineering, Central South Univ., Changsha, Hunan 410075, PR China. Email: [email protected]
Ph.D. Student, School of Civil Engineering, Central South Univ., Changsha, Hunan 410075, PR China. Email: [email protected]

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Cited by

  • Stability Analyses of Shallow Rectangular Tunnels in Anisotropic and Nonhomogeneous Soils Using a Kinematic Approach, International Journal of Geomechanics, 10.1061/IJGNAI.GMENG-8959, 24, 7, (2024).
  • Three-dimensional blow-out stability analysis of shield tunnel face in anisotropic and heterogeneous soils, Tunnelling and Underground Space Technology, 10.1016/j.tust.2022.104851, 131, (104851), (2023).
  • Three-dimensional modified pseudo-dynamic analysis of reinforced slopes with inclined soil nails, Bulletin of Engineering Geology and the Environment, 10.1007/s10064-022-02886-7, 81, 9, (2022).

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