Technical Papers
Nov 4, 2022

Passive Earth Pressure in Narrow Cohesive-Frictional Backfills

Publication: International Journal of Geomechanics
Volume 23, Issue 1

Abstract

A narrow backfill zone is formed when retaining walls are built near existing stabilized structures (e.g., rock faces). In such circumstances, the classical passive earth pressure coefficient is no longer applicable, and a correction factor is required for the design. This paper aims to develop analytical solutions for estimating the passive earth pressure problem of narrow cohesive-frictional backfills behind retaining walls. The novel arched differential element method considers both effects of the horizontal shear stress in backfills and the soil arching, and it is employed to estimate the passive earth pressure distribution along with wall depth. The solutions are compared against those published experimental data, analytical approaches, and finite-element limit analysis solutions. The factors influencing the distribution of passive earth pressure are also undertaken using a series of parametric studies. To implement the derived solutions into a routine design, a modified practical design equation is presented following the standard Coulomb’s solutions. This work provides a theoretical guideline for the initial design of retaining walls with narrow soils, and it should be of great interest to practitioners.

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Data Availability Statement

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

Acknowledgments

This study was supported by a CSC grant, the Postgraduate Research & Practice Innovation Program of Jiangsu Province (Grant No. KYCX20_0118), and the Scientific Research Foundation of Graduate School of Southeast University (Grant No. YBPY2041).

Notation

The following symbols are used in this paper:
B
bottom width of narrow soils behind retaining wall (m);
c
soil cohesion (kPa);
D1D22
abbreviations used in the derivation process;
D1D22
abbreviations used in the derivation process;
dz
thickness of the arched element (m);
Ep
passive earth thrust acting on rotating retaining wall (kN);
FxA1A1, FxE1E1
horizontal forces at the wall–soil interface involved in the element in the upper zone (kN);
FxA1E1, FxA1E1
horizontal forces on upper and lower boundaries of the element in the upper zone (kN);
FzA1A1, FzE1E1
vertical forces at the wall–soil interface involved in the element in the upper zone (kN);
FzA1E1, FzA1E1
vertical forces on upper and lower boundaries of the element in the upper zone (kN);
G1
gravity of arched differential element in the upper zone (kN);
H
retaining wall height (m);
H1
height of the upper zone (m);
H2
height of the lower zone (m);
Kp
passive thrust coefficient;
Kp,Coulomb
passive earth pressure coefficient calculated by Coulomb’s theory;
lA1E1
length of A1E1 (m);
lE1E1
curve length of E1E1′ (m);
N
ratio of major to minor principal stresses;
p1p7
optimal constant coefficients;
RA1E1
radius of major principal stress trajectory (m);
z
buried depth of arched element (m);
Δz
vertical distance between points A1 and i (m) ;
αf
sliding angle of the slip surface (°);
β
angle of the slope (°);
γ
unit weight (kPa);
δ1
wall–soil interface friction angle (°);
δ2
slope–soil interface friction angle (°);
η
correction factor;
θr
rotation angle of major principal stress of the rock–soil interface in Mohr’s circle (°);
θr1
rotation angle of minor principal stress on slope surface to the horizontal (°);
θs
rotation angle of minor principal stress on the slip surface to the horizontal (°) ;
θw
rotation angle of minor principal stress at the wall–soil interface to the horizontal (°);
θw
rotation angle of minor principal stress at the wall–soil interface to the vertical (°);
ϕ
soil friction angle (°);
μ1
interface roughness factor of the wall;
μ2
interface roughness factor of the slope;
σ30
minor principal stresses at the wall–soil interface (kPa);
σ3i
minor principal stress at arbitrary point i on upper boundary of the element (kPa);
σw0, σwu, σwl
lateral earth pressure exerted in upper and lower zones (kPa);
σr, τr
normal and shear stresses on the rock–soil surface (kPa); and
σs, τs
normal and shear stresses on the slip surface in backfills (kPa).

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Go to International Journal of Geomechanics
International Journal of Geomechanics
Volume 23Issue 1January 2023

History

Received: Feb 15, 2022
Accepted: Aug 14, 2022
Published online: Nov 4, 2022
Published in print: Jan 1, 2023
Discussion open until: Apr 4, 2023

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Chutian Li
Dept. of Civil and Environmental Engineering, Hong Kong Univ. of Science and Technology, Clear Water Bay, Kowloon 999077, Hong Kong; School of Civil Engineering, Chang’an Univ., Xi’an 710061, China.
Institute of Geotechnical Engineering, School of Transportation, Southeast Univ., Nanjing 211189, China; Faculty of Civil Engineering and Geosciences, Delft Univ. of Technology, Building 23, Stevinweg 1/P.O. Box 5048, 2628 CN Delft/2600 GA Delft, Netherlands (corresponding author). ORCID: https://orcid.org/0000-0002-9045-0659. Email: [email protected]; [email protected]
Jim Shiau
School of Civil Engineering and Surveying, Univ. of Southern Queensland, Toowoomba, QLD 4350, Australia.
Suraparb Keawsawasvong
Dept. of Civil Engineering, Thammasat School of Engineering, Thammasat Univ., Pathumthani 12120, Thailand.
Hanhui Huang
College of Civil Engineering, Fuzhou Univ., Fuzhou 350108, China.

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