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Research Article

Analytical solution for laterally loaded non-uniform circular piles in multi-layered inhomogeneous soil

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Pages 408-422 | Received 17 Mar 2023, Accepted 13 Aug 2023, Published online: 18 Sep 2023
 

ABSTRACT

Non-prismatic piles are typically used in cases where large lateral loads must be resisted. In many applications, piles are partially or fully embedded in multi-layered non-homogeneous soil, with each layer having its own set of properties. Analytical, simple solutions to study this problem are more limited and complex than that of prismatic ones. The analysis becomes even more complicated when both the variation of the cross-sectional area of the element and the soil inhomogeneity are included in the formulation. This work presents the derivation of the stiffness matrix and load vector of a non-uniform section of pile partially or fully embedded in non-homogeneous soil. The analysis of non-uniform piles in multi-layered soil is carried out by dividing the pile into multiple sub-elements and then assembling them using conventional matrix methods. Four examples, encompassing partially and fully embedded piles, are presented to validate the simplicity and accuracy of the proposed solution.

Disclosure statement

No potential conflict of interest was reported by the author(s).

List of Symbols

A(x)=

Area of the element at a depth x

B(x)=

Diameter of the element at a depth x

E=

Young’s modulus of the element

Gp=

Shear modulus of the pile

I(x)=

Second moment of inertia of the element at a depth x

KL=

First-parameter of the Pasternak foundation

Ko=

Modulus of subgrade reaction

Le=

Embedded length of the pile

Lp=

Total length of the pile

Lu=

Unembedded length of the pile

M=

Bending moment

m=

Taper ratio

mh=

Variation of the modulus of subgrade reaction with depth

Po=

Axial load

q(x)=

Applied transverse load

rb=

Radius at the bottom of the element

req=

Equivalent radius at half of the length of the element

rt=

Radius at the top of the element

Sa, Sb=

Shear stiffness of the linear transverse springs at ends A and B, respectively.

V=

Shear force

x=

Coordinate along the longitudinal axis

y=

Transverse deflection

Y=

Non-dimensional term for the transverse deflection

kg=

Second-parameter of elastic foundation

κa, κb=

Flexural stiffness of the flexural springs at ends A and B, respectively.

ξ=

Non-dimensional term for the length

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