Numerical Analysis of Soil Nail Walls under Seismic Condition in 3D
Form Excavations
Siavash Zamiran1, a, Hadi Ghojavand 1,b, Hamidreza Saba2, c
1 Department of Civil Engineering, Science and Research Branch, Islamic Azad University, Iran
2 Assistant professor, Amirkabir University of Technology, Tehran, Iran
Keywords: Soil Nail Walls, Dynamic Analysis, Numerical Modeling
Abstract. Typically, temporary soil nailing systems are not required to provide for design level
earthquake occurrences consistent with the building or structure being constructed inside the
excavation. However, the seismic response of the permanent soil nail walls during the earthquakes
should be evaluated. On the other hand, evaluation of 3D response of soil nailing walls have some
strange manners that should be considered in the numerical analysis.
In this paper, numerical simulations of soil nail walls under vibrational input have been carried out,
and the results are compared with the function of soil nail walls under ordinary statistical loading. The
behaviour of geometry of nails are mentioned under static and seismic analysis. After that some
investigations are carried out to find respond of soil nailing walls in some 3D excavation forms. The
analysis is performed with finite difference software called FLAC3D.
The results are prepared as lateral displacement of the walls and normalized maximum tensile forces
for nails. These results can demonstrate the behavior of external and internal resistance of soil nail
walls under seismic and static analysis. The deformation of wall under the static and dynamic manner
varies in a wide range. On the other hand, tensile loads that are produced in nails under the static
manner are namely 50% less than the dynamic manner.
Introduction
In areas of high seismic activities, earthquake has a wide effect on retaining walls like soil nail walls.
A review of researchers shows the soil nail walls perform much better than classical retaining walls
like gravity walls. When cable takes effect in foundation, it retains the deformation of soil and
reinforces the foundation from failure by transferring its tensile force based on the interaction of soil
and cables. After reinforced by cables, the parameters and stress state of soil mass is improved.
In the present paper, firstly the cable elements build; then numerical models are founded by
FLAC3D. Seismic analysis is carried out to the models. And then deformation and stress responses
are obtained as well as the mechanical response of nails during calculation. Results can show the
mechanism of soil nail walls and their load transferring mode under seismic condition.
For verification of the soil nail walls in FLAC3D, a compression is carried out with Thompson and
Miller’s (1990) research. They described the design, construction and performance of Seattle’s first
nailed walls.
Verification of the finite deference model
Thompson and Miller (1990) investigated the Seattle’s first nailed walls. For this vertical soil nail
wall, nails were mostly installed at 1.8m spacing horizontally and vertically. The nail length is 10.7m,
except for the length of the top row which is 9.8m. The diameter of the drilled holes is 203mm. Nail
bars are installed at an inclination of 15 degrees, though the first row on the high wall was installed at
20 degrees to avoid utilities. A typical section of the high wall is shown in Fig. 1. In this research, the
stability of this soil nailed vertical cut is analysed by FLAC3D. [1]
Applied Mechanics and Materials Vols. 204-208 (2012) pp 2671-2676Online available since 2012/Oct/26 at www.scientific.net© (2012) Trans Tech Publications, Switzerlanddoi:10.4028/www.scientific.net/AMM.204-208.2671
All rights reserved. No part of contents of this paper may be reproduced or transmitted in any form or by any means without the written permission of TTP,www.ttp.net. (ID: 128.250.144.144, University of Melbourne, Melbourne, Australia-28/09/13,13:55:53)
Fig. 1) Typical section of Seattle’s wall
Thompson and Miller measured the highest nail forces by inclinometer and calculated the values
by the finite-element method. A comparison of maximum nail forces in measured values and
finite-element calculations in each row is shown in Figure 2 with the values that gain from finite
deference method, FLAC3D. The results show reliable convergence among calculated values, FEM
and FDM.
Fig. 2 and Fig. 3 shows the reliable convergence of the places that maximum tensile loads occur
through the nail lengths.
Fig. 2) Comparison of maximum nail forces
Fig. 3) The places that maximum tensile loads
occur through the nail lengths.
Numerical model
In this research, an excavation is carried out to the depth of 8m. Model is fixed in normal direction
for the side boundaries. Fixed in three dimensions is done for the bottom boundary. The procedure of
excavation is done by four steps to simulate the ordinary staged construction in the sites. Before
excavation, only gravity is loaded, and calculation is done to make the system become in an
equilibrium state. Then the displacement caused by gravity is eliminated. Afterwards the excavations
are done while the cable elements are placed in the model to simulate the soil nail walls.
Soil mass is modelled in the software by popular constitutive model, Mohr-Coulomb. The
calculation parameters for soil mass are shown in Table 1.
Table 1. Geomechanical parameters for soil mass
parameter value unit (SI)
Young’s modulus 70 Mpa
Poisson’s ration 0.3
Shear modulus 27 Mpa
Bulk modulus 58 Mpa
Internal friction angle 22 degree
Cohesion 25 kPa
2672 Progress in Industrial and Civil Engineering
The length of cable is 7m, with 10º inclination angle and 1m vertical and horizontal spacing. The
first layer of the cables is 1m to the top of the wall in perpendicular directions. The cable system is
considered as the elastic model.
The axial behavior of reinforcement systems may be assumed to be governed entirely by the
reinforcing element itself. Because the reinforcing element is slender, it offers little bending
resistance and is treated as a one-dimensional member with capacity to sustain uniaxial tension.
In evaluating the axial forces that develop in the reinforcement, displacements are computed at
nodal points along the axis of the reinforcement, as shown in Fig. 4. Out-of-balance forces at each
nodal point are computed from axial forces in the reinforcement as well as shear forces contributed
through shear interaction along the grout annulus. [2], [3]
According to some researchers like Wei and Cheng, a thin layer of material with a thickness of 4.0
mm surrounding the nail is used to model the shearing zone between the nail and the soil that is shown
in Fig. 5. [4]
The shear stiffness of the shear zone (grout), Kg, can be estimated in Eq. (1).
Fig. 4) Mechanical representation of fully bonded reinforcement
Which accounts for shear behaviour of the grout annulus.
2
10ln(1 2 )
GKg
tD
(1)
Where G is shear modulus of the shear zone and is identical to shear modulus of soil; can obtain
from Table 1. D is drilled hole diameter and t is annulus thickness of the shear zone and is considered
equal to 0.004 m. The shear zone cohesive strength (slider) per unit length can be estimated as Eq. (2).
(2)
Where c is cohesion of soil. Shear zone friction angle is nearly equal to friction angle of
surrounding soil. The calculation parameters for cable reinforcing are shown in Table 2. These
parameters are similar to the later study and can resist the wall against failure during the earthquake.
[5]. The shotcrete structure is simulated at the face of the wall with shell elements in FLAC3D. The
thickness of shotcrete is 20cm. The shell system is considered as the elastic model. The calculation
parameters for shotcrete are shown in Table 3.
Fig. 5) Idealization of the soil nail system.
( 2 ) cg c D t
Applied Mechanics and Materials Vols. 204-208 2673
Table 2. Cable parameters for simulation of nail
parameter value unit (SI)
Nail diameter 20 mm
Drill hole diameter 100 mm
Young’s modulus of nail 200 GPa
Young’s modulus of grout 22 GPa
Young’s modulus of grouted nail 29.12 GPa
Annulus thickness 0.004 m
shear zone cohesive strength 6.28 kPa
Shear zone friction angle 31 degree
shear stiffness of the shear zone 219.6 MPa
Compressive yield strength of the grouted nail 30 MPa
Tensile yield strength of the grouted nail 30 MPa
density of grouted nail 2200 kg/m3
Table 3. Structural parameters for shotcrete
parameter value unit (SI)
Young’s modulus 24.5 Gpa
Poisson’s ration 0.3
Density 2200 kg/m3
Comparison between static and dynamic behaviour of the wall
To demonstrate the deference between static and seismic behavior of the soil nail wall static and
dynamic analysis is carried out on a same model. The dynamic loading input is based on Kojur
earthquake accelerogram of 28 May 2004, Iran. [6]
During the earthquake, axial force in nails varies in a wide range and after the earthquake a final
value remains in the nails. Figure 6 shows the proportion of static maximum nail forces to dynamic
highest nail forces for three nail rows. The results show the nearest value of static and dynamic
maximum nail force happen in the mid nail row at the mid of the wall (53%).
Fig. 7 shows the proportion of displacements of the wall in static to dynamic analysis. The most
deformation of the wall happens at the top of the wall in the dynamic analysis. Other displacement
values are compared to displacement of the top of the wall in the dynamic analysis. The results show
that sidelong displacement of the wall in seismic condition has 60 to 95% larger than lateral
displacement of the wall in ordinary static condition.
Fig. 6) Proportion of static tensile force to
dynamic tensile force
Fig. 7) Lateral displacement of the wall to
normalized depth
2674 Progress in Industrial and Civil Engineering
Investigation of the direction of earthquake input load to 3D excavation forms
Two excavation types are considered in this study. In these two models, the excavated planes have
90 and 270 degree with each other. Figure 8 shows the 3D form of these two types of excavation.
The lateral earthquake input is impressed into one direction. Therefore, two vertical walls in each
model behave differently during the earthquake. The walls are either perpendicular to earthquake
direction or parallel to that. Figure 9 shows these two deferent manners of wall under earthquake in 90
and 270º excavation types.
Figure 10 shows sidelong wall displacement in 90 and 270º excavation types to normalize depth of
the walls. In 270º excavation, the lateral displacement of the parallel wall to earthquake direction is
20% than the perpendicular one. On the other hand, in 90º excavation type the lateral displacement of
the parallel wall to earthquake direction is 33% than the perpendicular one. The perpendicular walls in
90 and 270º excavation types can move stronger than parallel. To give a reason for this result we can
mention on more motivation of earthquakes to the perpendicular wall than parallel one. FLAC3D 3.00
Itasca Consulting Group, Inc.Minneapolis, MN USA
Step 11993 Model Perspective18:31:29 Mon Jan 23 2012
Center: X: 1.100e+001 Y: 1.200e+001 Z: 1.050e+001
Rotation: X: 40.000 Y: 0.000 Z: 310.000
Dist: 9.561e+001 Mag.: 1Ang.: 22.500
Block Groupsoil
SEL Geometry Magfac = 0.000e+000
FLAC3D 3.00
Itasca Consulting Group, Inc.Minneapolis, MN USA
Step 9693 Model Perspective18:28:53 Mon Jan 23 2012
Center: X: 1.100e+001 Y: 1.200e+001 Z: 1.050e+001
Rotation: X: 30.000 Y: 0.000 Z: 320.000
Dist: 9.561e+001 Mag.: 1Ang.: 22.500
Block Groupsoil
SEL Geometry Magfac = 0.000e+000
Fig. 8) Two types of excavated wall: 90 and 270º type
Fig. 9) The walls perpendicular and parallel to earthquake
Direction in 90 and 270º excavation types
Fig. 10) Lateral wall displacement in 90 and 270º
excavation types to normalize depth of the walls
Applied Mechanics and Materials Vols. 204-208 2675
Conclusions
A series of numerical simulations is reported using FLAC models to predict the dynamic load and
displacement response of walls. FLAC can simulate the interaction behavior of soil-grout-nail
appropriately. The Mohr-Coulomb constitutive model is used to simulate the soil behavior and nail
and shotcrete demonstrate as the elastic manner.
This paper establishes that earthquakes have great influence on the lateral displacement of the soil
nail walls. During the earthquake, bottom and top nail rows motivate more axial forces than the mid
nail rows.
In 270º excavation, the sidelong displacement of the parallel wall to earthquake direction is 20%
than the perpendicular one. On the other hand, in 90º excavation the lateral displacement of the
parallel wall to earthquake direction is 33% than the perpendicular one. Thus, the perpendicular walls
in 90 and 270º excavation types can move stronger than parallel.
References
[1] Thompson, S. R., and Miller, I. R ., (1990) “Design, Construction and Performance of a Soil
Nailed wall in Seattle, Washington”, Design and Performance of Earth Retaining Structures,
Geotechnical Special publication, No. 25, ASCE, pp. 629-643
[2] “Structural Elements”, FLAC, Fast Lagrangian Analysis of Continua, (2004) ITASCA
Consulting Eng, Minnesota, p31-32
[3] QING Du-gan et. al. (2009) “Numerical simulation for the interaction between soil and cable in
deep foundation pit”, International Conference on Computer Modeling and Simulation, IEEE
[4] W.B. Wei, Y.M. Cheng, (2010), “Soil nailed slope by strength reduction and limit equilibrium
methods”, Computers and Geotechnics journal
[5] Zamiran. Siavash, Saba. Hamidreza, Ghadimi Aroosmahalleh. Fereydoun, (2012), “Numerical
Investigation of Seismic Behavior of Soil Nail Walls”, 4th International Conference on Seismic
Retrofitting, Tabriz, Iran
[6] Building and Housing Research Center (BHRC), The ministry of housing and urban development,
Tehran, Iran, www.bhrc.ac.ir
2676 Progress in Industrial and Civil Engineering
Progress in Industrial and Civil Engineering 10.4028/www.scientific.net/AMM.204-208 Numerical Analysis of Soil Nail Walls under Seismic Condition in 3D Form Excavations 10.4028/www.scientific.net/AMM.204-208.2671