Technical Papers
Nov 3, 2022

Undrained Solution for Cylindrical Cavity Expansion in Structured Clays Using a Hypoplastic Model

Publication: International Journal of Geomechanics
Volume 23, Issue 1

Abstract

This paper develops an innovative undrained solution for cylindrical cavity expansion using a hypoplastic model that could well reflect the mechanical properties of clay, especially the structural degradation of unstable clay. Then, the constitutive relationship of the hypoplastic clay model for cavity expansion problems is established by adding the strain rate–displacement relationship in cylindrical coordinates. Therefore, simple first-order ordinary differential equations are obtained to solve the problem of cavity expansion for structured clay. This paper compares the proposed solution with the Abaqus finite-element solution and conducts an extensive analysis of the model parameters. The results prove that the solution can accurately capture the expansion responses under undrained conditions. The variations and distributions of the internal cavity pressure, excess pore pressure, and sensitivity in unstable structural clay are obtained, which show obvious trends of structural degradation. The normalized expansion pressure and excess pore pressure decrease as the value of OCR increases. The normalized cavity pressure and structural degradation radius decrease as the structural parameters increase, while the opposite change is observed in the excess pore water pressure. The results of the application analysis can be used as a reference for clarifying the variation in the bearing capacities of piles and the disturbance of surrounding soil in practical engineering.

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Data Availability Statement

All data, models, or codes that support the findings of this study are available from the corresponding author upon reasonable request.

Acknowledgments

The work was supported by the National Natural Science Foundation of China, Grant/Award Number 51978105 and 52027812; the Chongqing Science Foundation for Distinguished Young Scholars, Grant/Award Number: cstc2021jcyj-jqX0017, and the Chongqing Youth Top Talent Plan, Grant/Award Number: cstc2021ycjh-bgzxm0132.

Notation

The following symbols are used in this paper:
A
fourth-order tensor in hypoplastic model formulation;
a
cavity radius after expansion;
A0
initial cavity radius;
Am
variable in hypoplastic model formulation;
af
variable in hypoplastic model formulation;
ay
hypoplastic variable equal to 0.3; the parameter controls the shape of the asymptotic state boundary surface;
a1, a2, a3, a4, a5
parameters of transversely isotropic elasticity model;
cos 3θ
lode angle function;
D
Euler stretching tensor;
D
cone diameter;
d
normalized second-order tensor specifying asymptotic strain rate direction;
dA
second-order tensor specifying asymptotic strain rate direction;
e
porosity;
Fm
factor of Matsuoka–Nakai yield condition;
fd
pyknotropy factor of hypoplastic equation;
fdA
pyknotropy factor of hypoplastic equation, asymptotic state value;
fs
barotropy factor of hypoplastic equation;
I1, I2, I3
stress invariants;
k, A, sf
structural parameters;
L
hypoplasticity fourth-order tensor;
N
hypoplasticity second-order tensor;
N
hypoplastic model parameter (position of normal compression line);
n
unit vector normal to the plane of symmetry;
OCR
overconsolidation ratio;
Oc
hypoplastic variable is equal to 2; wet of critical;
p
mean effective stress;
pe
value satisfies the relationship: 0 = q2 + M2p2M2ppe;
pe*
Hvorslev equivalent pressure;
pij
second-order tensor, pij = ninj;
pr
reference stress equal to 1 kPa;
q
deviatoric stress;
r
radial distance from the cavity position;
rc
cone radius;
subscript “0”
initial state;
subscript “a
at cavity wall;
subscript “l
limit value;
subscript “s”
at the structure degradation boundary;
subscript “sd”
structural degradation;
subscript “su”
structural undegradation;
s
sensitivity;
To
stress rate tensor;
u
pore pressure;
αE
anisotropy ratio of Young’s moduli;
αf
hypoplastic variable controlling rate of stiffness decrease; may be considered as a model parameter;
αG
anisotropy ratio of shear moduli;
αν
anisotropy ratio of Poisson’s ratios;
Δu
excess pore pressure;
Δua
excess pore pressure at cavity wall;
ɛr, ɛθ
radial strain and circumferential strain;
ɛv, ɛs
volumetric strain and deviatoric strain;
κ*
hypoplastic model parameter controlling volumetric unloading response;
λ*
hypoplastic model parameter (slope of normal compression line);
νpp
Poisson’s ratio;
ω
variable controlling asymptotic state boundary surface shape;
σa
internal cavity pressure;
σr,σθ,σz
effective radial, circumferential, and vertical stress components;
σra
radial effective stress at cavity wall;
φc
critical state friction angle;
ξ
variable controlling asymptotic strain rate direction; and
1
second-order identity tensor.

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International Journal of Geomechanics
Volume 23Issue 1January 2023

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Received: Nov 17, 2021
Accepted: Aug 8, 2022
Published online: Nov 3, 2022
Published in print: Jan 1, 2023
Discussion open until: Apr 3, 2023

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Shaohua Zeng [email protected]
Master’s Candidate, Key Laboratory of New Technology for the Construction of Cities in Mountain Areas, College of Civil Engineering, Chongqing Univ., Chongqing 400045, China. Email: [email protected]
Professor, Key Laboratory of New Technology for the Construction of Cities in Mountain Areas, College of Civil Engineering, Chongqing Univ., Chongqing 400045, China (corresponding author). Email: [email protected]
Zengliang Wang [email protected]
Ph.D. Candidate, Key Laboratory of New Technology for the Construction of Cities in Mountain Areas, College of Civil Engineering, Chongqing Univ., Chongqing 400045, China. Email: [email protected]

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