Technical Papers
Jul 1, 2021

Euler–Bernoulli Pile Element for Nonlinear Buckling Analysis of Single Piles in Slope

Publication: International Journal of Geomechanics
Volume 21, Issue 9

Abstract

Piles are sometimes unavoidably embedded in slopes for supporting buildings on hills. In contrast to a pile on a horizontal ground, a pile in slope is acted on by additional sliding force from the slope, impairing its load-bearing capacity and buckling resistance. Nevertheless, proper assessment for the buckling of piles in slopes is difficult because of the simulation of distributed sliding forces and nonlinear pile–soil interactions. This paper refines the newly developed Euler–Bernoulli pile element formulation for the nonlinear buckling analysis of single piles in slopes by including the sliding force in element formulation, enabling a rigorous consideration of soil–pile interactions. Detailed mathematical derivations are provided. The numerical implementation is illustrated with a flowchart. Four examples for verification are demonstrated to reveal the robustness of the proposed method and the importance of considering the sliding force.

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Acknowledgments

The work described in this paper was partially supported by a grant from the Research Grants Council of the Hong Kong Special Administrative Regain, China (Project No. UGC/FDS13/E06/18) and a grant from the National Natural Science Foundation of China (No. 52008410).

Notation

The following symbols are used in this paper:
A
cross-sectional area;
Aji
coefficients in the secant relations;
Bji
coefficients in the secant relations;
Cji
coefficients in the secant relations;
E
Young's modulus;
FE
element resisting force vector from the element strains;
FS
element resisting force vector from the soil resistance and sliding force;
FT
total resisting force vector;
Fx1
force on the x-axis at the upper side;
Fx2
force on the x-axis at the lower side;
Fy1
force on the y-axis at the upper side;
Fy2
force on the y-axis at the lower side;
Hi
weight of the ith Gauss point;
I
moment of inertia;
[k]
global stiffness matrix;
[k]E
tangent stiffness matrix of the whole element;
[k]G
geometric stiffness matrix;
[k]L
linear stiffness matrix;
[k]LS
impaired stiffness matrix cause by the sliding force;
[k]S
soil stiffness matrix;
k(v)
tangential value of the py curve at a specified lateral deflection;
L
element length;
M1
bending moment at the upper side;
M2
bending moment at the lower side;
P
axial load;
p
lateral soil resistance per unit length;
q(x)
value of the sliding force at a specified location of the element;
R
global resisting force vector;
TOL
value for the acceptable accuracy in the Newton–Raphson numerical procedure;
U
global nodal displacement vector;
UE
potential energy accumulating in the pile;
US
potential energy accumulating in the surrounding soil;
USP
energy consumed by lateral soil resistance;
U
energy consumed by shaft resistance;
u
axial deflection along the element;
u1
axial deflection at the upper side;
u2
axial deflection at the lower side;
ui
axial defection at the ith Gauss point;
V1
shear force at the upper side;
V2
shear force at the lower side;
v
lateral deflection along the element;
v1
lateral deflection at the upper side;
v2
lateral deflection at the lower side;
vi
lateral defection at the ith Gauss point;
W
work done by total external forces;
WL
work done by the sliding force;
WP
work done by external point load;
xi
axial defection at the ith Gauss point;
[γ]i
initial transformation matrix for describing the initial position of the element at during the ith step;
ΔF
incremental force or the unbalanced force vector;
Δr
element resisting force vector;
ΔU
incremental nodal displacement vector;
ɛx
element normal strain;
ɛxy
element shear strain;
θ1
rotation at the upper side;
θ2
rotation at the lower side;
κij
coefficients in the stiffness matrix;
λ(u)
tangential value of the τz curve at a specified axial deflection;
μij
coefficients in the stiffness matrix;
Π
total potential energy;
σx
element normal stress;
τ
shaft friction per unit length;
τxy
element shear stress; and
ωji
coefficients in the stiffness matrix.

References

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Go to International Journal of Geomechanics
International Journal of Geomechanics
Volume 21Issue 9September 2021

History

Received: Dec 30, 2020
Accepted: May 13, 2021
Published online: Jul 1, 2021
Published in print: Sep 1, 2021
Discussion open until: Dec 1, 2021

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Authors

Affiliations

Weihang Ouyang
School of Civil Engineering, Sun Yat-Sen Univ., Zhuhai 519060, Guangdong, P.R. China.
Si-Wei Liu
Dept. of Civil and Environmental Engineering, The Hong Kong Polytechnic Univ., Hung Hom, Kowloon, Hong Kong 999077, China.
Jianhong Wan
School of Civil Engineering, Sun Yat-Sen Univ., Zhuhai 519060, Guangdong, P.R. China.
Dept. of Civil Engineering, Chu Hai College of Higher Education, Tuen Mun, N.T. Hong Kong 999077, China (corresponding author). Email: [email protected]

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