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2nd International FLAC/DEM Symposium
Lateral Earth Pressures with
Layered Backfill
Jim S. Shiau, PhD (Newcastle)
Senior Lecturer in Geotechnical Engineering
Faculty of Engineering and SurveyingUniversity of Southern Queensland
Toowoomba, QLD, Australia
7/13/2011 Dr. Jim Shiau 2
USQ, Toowoomba, Queensland, Australia
1.5 hr drive to Brisbane
2.0 hrs drive to Gold Coast
13 July 2011 Dr. Jim Shiau 3
Background to research
To make use of the existing resources at USQ ( both 2D and 3D
FLAC licences), we aim to develop numerical models for various
geotechnical applications.
Research at USQ also involves developing various physical models
for teaching purposes, so as to complement the numerical
approach using computer modeling.
Dr. Jim Shiau 4
Background to research
USQ Geotechnical Stability Testing Rigs
P
Δ
Pu
13 July 2011
13 July 2011 Dr. Jim Shiau 5
7/13/2011 Dr. Jim Shiau 6
What is physical model?
A landslide model to
simulate the failure pattern
of a slope.
13 July 2011 Dr. Jim Shiau 7
Bonsai vs. Physical Model
The knowledge gained in the
process of Bonsai making would
help to understand the behaviour
of a real tree.
Bonsai
7/13/2011 Dr. Jim Shiau 8
USQ Geotechnical Stability Testing
Rigs
13 July 2011 Dr. Jim Shiau 9
Various Stability Models using FLAC
Classical earth pressure problems
Slotted wall
Trapdoor
Tunnel heading
Uplift of buried pipe
Uplift of ground anchor
FLAC (Version 4.00)
LEGEND
8-Jun-06 20:23
step 72142
-1.111E+00 <x< 2.111E+01
-7.111E+00 <y< 1.511E+01
Max. shear strain-rate
0.00E+00
2.80E-08
5.60E-08
8.40E-08
1.12E-07
1.40E-07
1.68E-07
1.96E-07
2.24E-07
Contour interval= 7.00E-09
-0.400
0.000
0.400
0.800
1.200
(*10^1)
0.200 0.600 1.000 1.400 1.800
(*10^1)
JOB TITLE :
USQ
USQ
FLAC (Version 4.00)
LEGEND
8-Jun-06 14:22
step 75374
-4.444E-01 <x< 8.444E+00
-1.444E+00 <y< 7.444E+00
Max. shear strain-rate
0.00E+00
6.00E-08
1.20E-07
1.80E-07
2.40E-07
3.00E-07
3.60E-07
4.20E-07
4.80E-07
5.40E-07
Contour interval= 6.00E-09
-0.500
0.500
1.500
2.500
3.500
4.500
5.500
6.500
0.500 1.500 2.500 3.500 4.500 5.500 6.500 7.500
JOB TITLE :
USQ
FLAC (Version 4.00)
LEGEND
6-Jul-06 20:30
step 100000
-3.900E-01 <x< 7.410E+00
-2.400E+00 <y< 5.400E+00
Max. shear strain-rate
0.00E+00
3.70E-07
7.40E-07
1.11E-06
1.48E-06
1.85E-06
2.22E-06
2.59E-06
2.96E-06
3.33E-06
Contour interval= 1.00E-08
-1.500
-0.500
0.500
1.500
2.500
3.500
4.500
0.500 1.500 2.500 3.500 4.500 5.500 6.500
JOB TITLE :
USQ
USQ
FLAC (Version 4.00)
LEGEND
8-Dec-04 16:35
step 5500
-3.333E+00 <x< 3.333E+00
-2.833E+00 <y< 3.833E+00
Material model
mohr-coulomb
Velocity vectors
Max Vector = 1.005E-04
0 2E -4
Boundary plot
0 2E 0
-2.000
-1.000
0.000
1.000
2.000
3.000
-2.500 -1.500 -0.500 0.500 1.500 2.500
JOB TITLE :
Computational Engineering Researc
13 July 2011 Dr. Jim Shiau 10
Background to research
Had some experience in Upper and Lower Bound Limit Analyses
during my stay in Newcastle Geotechnical Group during 1998-
2003.
Overall, my research interests at USQ
• To develop stability models using FLAC.
• To develop stability models using Upper and Lower limit analyses.
• Physical modeling using simple stability testing rigs at USQ.
Two papers in this symposium:• Modeling Uplift of Plate Anchor
• Earth Pressures with Layered Backfill
7/13/2011 Dr. Jim Shiau 11
Goal and Objective
Lateral Earth Pressures with Layered Backfill
To investigate the situation of active and passive earth
pressures on the back of a retaining wall with layered backfill.
To compare FLAC results with those using classical earth
pressure theory and FE Limit Analyses - Upper and Lower Limt
Analyses.
• FLAC
• Rankine/Coulomb/Log Spiral
• Upper and Lower bounds
For smooth and rough wall cases!
7/13/2011 Dr. Jim Shiau 12
The problem definition
7/13/2011 Dr. Jim Shiau 13
The problem definition
7/13/2011 Dr. Jim Shiau 14
To solve a static system using the dynamic equation of motion, an
artificial nodal damping is needed so that kinetic energy can be
gradually removed.
Smooth case - Active wall
FLAC solution
Textbook solution – Rankine
Upper and Lower bound solutions
7/13/2011 Dr. Jim Shiau 15
Textbook solution of the problem
7/13/2011 Dr. Jim Shiau 16
Active wall – smooth wall case – Rankine’s solution
2.71 kPa
25.46 kPa
16.12 kPa
73.16 kPa
Active Pressure Diagram
Rankine: Total horizontal active thrust = 176.18 kN/m
FLAC solution = 167.20 kN/m
Upper and lower bound solutions of
the problem
7/13/2011 Dr. Jim Shiau 17
Active wall – smooth wall case
FLAC solution
= 167.20 kN/m
Smooth case - Passive wall
FLAC solution
Textbook solution – Rankine
Upper and Lower bound solutions
7/13/2011 Dr. Jim Shiau 18
Textbook solution of the problem
7/13/2011 Dr. Jim Shiau 19
Passive wall – Smooth wall case – Rankine’s solution
36.9 kPa
219.6 kPa
93.0 kPa
140.2 kPa
Active Pressure Diagram
Rankine: Total horizontal passive thrust = 734.55 kN/m
FLAC solution = 744.50 kN/m
Upper and lower bound solutions of
the problem
7/13/2011 Dr. Jim Shiau 20
Passive wall – smooth wall case
FLAC solution
= 744.50 kN/m
7/13/2011 Dr. Jim Shiau 21
Rough case - Active wall
FLAC solution
Textbook solution – Coulomb
Upper and Lower bound solutions
7/13/2011 Dr. Jim Shiau 22
Upper and lower bound solutions of
the problem
7/13/2011 Dr. Jim Shiau 23
Active wall – rough wall case
FLAC solution
= 127.60 kN/m
Rough case - Passive wall
FLAC solution
Textbook solution – Coulomb
Upper and Lower bound solutions
7/13/2011 Dr. Jim Shiau 24
Upper and lower bound solutions of
the problem
7/13/2011 Dr. Jim Shiau 25
Passive wall – rough wall case
FLAC solution
= 837.20 kN/m
7/13/2011 Dr. Jim Shiau 26
Results Summary
7/13/2011 Dr. Jim Shiau 27
7/13/2011 Dr. Jim Shiau 28
Summary
FLAC results favorably compared with upper and lower bound
solutions in all cases.
Classical earth pressure theories favorably compared with FLAC
and upper and lower bound solutions only in smooth wall cases
(active and passive) and rough active wall case.
For the rough passive wall case, the log-spiral failure surface
Shields & Tolunay’s (1973) theory is not particularly accurate for
the layered problem. It’s on the unsafe side with some 20%
overestimation ~ needless to mention Coulomb’s solution with
linear slip assumtion.
7/13/2011 Dr. Jim Shiau 29
Future Work
• Pressure distribution behind the wall.
• Velocity jump and change of velocity direction across layered
media.
• Shear stresses across the layered media for the passive + rough
wall case