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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 Surveying University of Southern Queensland Toowoomba, QLD, Australia

2nd International FLAC/DEM Symposium

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Page 1: 2nd International FLAC/DEM Symposium

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

Page 2: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 2

USQ, Toowoomba, Queensland, Australia

1.5 hr drive to Brisbane

2.0 hrs drive to Gold Coast

Page 3: 2nd International FLAC/DEM Symposium

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.

Page 4: 2nd International FLAC/DEM Symposium

Dr. Jim Shiau 4

Background to research

USQ Geotechnical Stability Testing Rigs

P

Δ

Pu

13 July 2011

Page 5: 2nd International FLAC/DEM Symposium

13 July 2011 Dr. Jim Shiau 5

Page 6: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 6

What is physical model?

A landslide model to

simulate the failure pattern

of a slope.

Page 7: 2nd International FLAC/DEM Symposium

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

Page 8: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 8

USQ Geotechnical Stability Testing

Rigs

Page 9: 2nd International FLAC/DEM Symposium

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

Page 10: 2nd International FLAC/DEM Symposium

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

Page 11: 2nd International FLAC/DEM Symposium

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!

Page 12: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 12

The problem definition

Page 13: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 13

The problem definition

Page 14: 2nd International FLAC/DEM Symposium

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.

Page 15: 2nd International FLAC/DEM Symposium

Smooth case - Active wall

FLAC solution

Textbook solution – Rankine

Upper and Lower bound solutions

7/13/2011 Dr. Jim Shiau 15

Page 16: 2nd International FLAC/DEM Symposium

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

Page 17: 2nd International FLAC/DEM Symposium

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

Page 18: 2nd International FLAC/DEM Symposium

Smooth case - Passive wall

FLAC solution

Textbook solution – Rankine

Upper and Lower bound solutions

7/13/2011 Dr. Jim Shiau 18

Page 19: 2nd International FLAC/DEM Symposium

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

Page 20: 2nd International FLAC/DEM Symposium

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

Page 21: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 21

Page 22: 2nd International FLAC/DEM Symposium

Rough case - Active wall

FLAC solution

Textbook solution – Coulomb

Upper and Lower bound solutions

7/13/2011 Dr. Jim Shiau 22

Page 23: 2nd International FLAC/DEM Symposium

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

Page 24: 2nd International FLAC/DEM Symposium

Rough case - Passive wall

FLAC solution

Textbook solution – Coulomb

Upper and Lower bound solutions

7/13/2011 Dr. Jim Shiau 24

Page 25: 2nd International FLAC/DEM Symposium

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

Page 26: 2nd International FLAC/DEM Symposium

7/13/2011 Dr. Jim Shiau 26

Page 27: 2nd International FLAC/DEM Symposium

Results Summary

7/13/2011 Dr. Jim Shiau 27

Page 28: 2nd International FLAC/DEM Symposium

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.

Page 29: 2nd International FLAC/DEM Symposium

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