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On Seismic Earth Pressures with some observations on
Seismic Performance of Dams
Nicholas Sitar Professor
Dept. of Civil and Environmental Engineering UC Berkeley
Presented at
Hydroelectric Generation DepartmentPublic Power Corporation
Athens, GreeceJanuary 26, 2010
N. Sitar, PPC, January 26, 20092
“Mononobe-Okabe solution”–
Assume a fully developed Coulomb wedge-
Force applied at 1/3H
N. Sitar, PPC, January 26, 20093
What is the basis for “M-O Method”
?
Mononobe
and Matsuo, 1929
N. Sitar, PPC, January 26, 20094
•
Two categories of walls:–
“yielding”
walls –
walls
that can move
sufficiently to develop minimum active earth pressures
–
“nonyielding”
walls –
walls
that do not satisfy the movement condition
FEMA 369
Source: Marshall Lew & SEAOSC
N. Sitar, PPC, January 26, 20095
•
For yielding walls, the FEMA 369 commentary states that there is consensus in the geotechnical engineering practice that a simplified Mononobe-
Okabe seismic coefficient analysis reasonably represents the dynamic (seismic) lateral earth pressure increment for yielding retaining walls. The the
dynamic increment of earth pressure is based
on Seed and Whitman (1970):
ΔPAE
~ (1/2)(3/4)kh γΗ 2
•
where kh
is the “horizontal ground acceleration divided by gravitational acceleration.”
FEMA 369 cont.
N. Sitar, PPC, January 26, 20096
•
For nonyielding
walls, the FEMA 369 commentary presents an equation developed by Wood (1973) for a rigid nonyielding
wall retaining a homogeneous
linear elastic soil and connected to a rigid base. The dynamic thrust, ∆PE
, is approximately:
ΔPE
= kh
γΗ 2
•
As for yielding walls, the point of application of the dynamic thrust is typically taken at a height of 0.6H above the base of the wall.
FEMA 369 cont.
N. Sitar, PPC, January 26, 20097
Mononobe and Matsuo, 1929 Seed and Whitman, 1970
N. Sitar, PPC, January 26, 20098
N. Sitar, PPC, January 26, 20099
Delphi: polygonal wall and temple of Apollo 548 B.C., temple destroyed by quake 373 B.C., other major quakes 551, and 1870 A.D.
N. Sitar, PPC, January 26, 200910
Kobe, 1995
N. Sitar, PPC, January 26, 200911
Taiwan, 1999
A lot of problems with old walls onsloping ground and with sloping backfill. No problems with base-ments
and flat ground ….
N. Sitar, PPC, January 26, 200912
Wenchuan
–
2008 –
Traditional retaining structures
N. Sitar, PPC, January 26, 200913
U-Wall Damage During 1971 San Fernando Earthquake, Clough & Fragaszy
(1977)
N. Sitar, PPC, January 26, 200914
Comparison of Total Horizontal Earth Pressures (T. Boardman, 2006)
0
5
10
15
20
0 500 1000 1500 2000 2500
Total Horizontal Earth Pressure (psf)
Dep
th (f
eet)
Flexible Wall Design Values
Rigid Wall Design Values
Ostadan&White (1998) ElCentro Motion
Davis (2003) G = f(z)
N. Sitar, PPC, January 26, 200915
•
What is the magnitude of seismic earth pressures on retaining structures in native ground?
•
Do seismic earth pressures need to be applied on subterranean building walls?
•
How do we reconcile designing walls for seismic earth pressures that are stronger and larger when walls designed without consideration of seismic earth pressures have not shown any evidence of distress in recent earthquakes?
Source: WHITE PAPER ON SEISMIC INCREMENT OF ACTIVE EARTH PRESSURE Marshall Lew, Ph.D., Martin B. Hudson, Ph.D., and J. Adolfo Acosta, Ph.D.,MACTEC Engineering and Consulting, Inc., Rami Elhassan, Ph.D., S.E., Integrated Design Services, Inc., Structural Engineers
Where does all this leave us?
N. Sitar, PPC, January 26, 200916
Example: Proposed BART Prototype
N. Sitar, PPC, January 26, 200917
Our Approach: Use Physical Modeling to Verify Failure Mechanisms
•
Why centrifuge? –
Good scaling relationships–
Repeatability–
Reproducibility–
Cost effectiveness
•
UC Davis centrifuge: –
9.1m radius, 4,500Kg maximum payload, area of bucket 4m2
N. Sitar, PPC, January 26, 200918
Scaling Relationships
N. Sitar, PPC, January 26, 200919
Centrifuge Model Design
•
Assume “typical”
BART stiff and flexible concrete retaining wall structures
•
Match the stiffness of aluminum model and concrete prototype
•
Match the mass of the aluminum model and concrete prototype
N. Sitar, PPC, January 26, 200920
Wall Instrumentation –
3 separate measurement systems
•
Array of 10 FlexiForce
pressure sensors on each wall
•
Array of 6 strain gauges on one rigid and one flexible
•
10 Instrumented “load”
bolts for direct force measurement at the wall base junction –
5 on one rigid and 5 on one flexible wall
N. Sitar, PPC, January 26, 200921
Model Construction
N. Sitar, PPC, January 26, 200922
Physical Model Layout
N. Sitar, PPC, January 26, 200923
Peak Accelerations for LAA02
N. Sitar, PPC, January 26, 200924
Ground Motion Amplification
N. Sitar, PPC, January 26, 200925
Moments and Lateral Earth Pressures
•
Observed response:–
Moments directly measured by instrumented load bolts and strain gauges
–
Lateral earth pressures directly measured by Flexiforce
sensors and interpreted from strain
gauges responses assuming a cubic fit for moment distributions on the walls
N. Sitar, PPC, January 26, 200926
Static Moments –
After Initial Gravity Applied
Initial - Before Shaking, LAA01
0
50
100
150
200
0 20 40 60x106Static Moment (lb-in)
Z (in
)
Meas. SG-StiffMeas. SG-FlexibleMeas. LB-StiffMeas. LB-FlexibleStatic At RestStatic Active
Initial - Before Shaking, LAA02
0
50
100
150
200
0 20 40 60x106
Static Moment (lb-in)
Z (in
)
Meas. SG-Stiff
Meas. SG-Flexible
Meas. LB-StiffMeas. LB-Flexible
Static At Rest
Static Active
φ
= 32° φ
= 35°
N. Sitar, PPC, January 26, 200927
Static Moments –
After First Shake
φ
= 32° φ
= 35°
After Loma Prieta-2, LAA01
0
50
100
150
200
0 20 40 60x106
Static Moment (lb-in)
Z (in
)
Meas. SG-Stiff
Meas. SG-Flexible
Meas. LB-Stiff
Meas. LB-Flexible
Static At Rest
Static Active
After Loma Prieta-SC-1LAA02
0
50
100
150
200
0 20 40 60x106Static Moment (lb-in)
Z (in
)
Meas. SG-Stiff
Meas. SG-Flexible
Meas. LB-Stiff
Meas. LB-Flexible
Static At Rest
Static Active
N. Sitar, PPC, January 26, 200928
Dynamic Moment and Earth Pressure Time History
N. Sitar, PPC, January 26, 200929
Maximum Dynamic Earth Pressure –
without
wall inertia
N. Sitar, PPC, January 26, 200930
0
1
2
3
4
5
6
0 20 40 60 80
Z (m
)
Pressure (KPa)
Loma Prieta-SC-2
Flexiforce-StiffFlexiforce-FlexibleSG-StiffSG-FlexibleM-O with PGAM-O with 65% PGA
0
1
2
3
4
5
6
0 10 20 30 40
Z (m
)
Pressure (KPa)
Kocaeli-YPT060-2
Maximum Dynamic Earth Pressure –
without
wall inertia
N. Sitar, PPC, January 26, 200931
Supporting Data?
Nakamura, S. 2006. Reexamination of Mononobe-Okabe Theory of Gravity Retaining Walls Using Centrifuge Model Tests, Soils and Foundations, Vol. 46, No.2, 135-146.
N. Sitar, PPC, January 26, 200932
Ortiz, L.A, R.F. Scott, and J. Lee (1983). Dynamic Centrifuge Testing of Cantilever Retaining Wall.Earthquake Engineering and Structural Dynamics, Vol. 11, 251-268.
N. Sitar, PPC, January 26, 200933
-0.2
0
0.2
0.4
0.6
0.8
0.2 0.4 0.6 0.8 1
ΔK
ae
PGA
Seismic Coefficient versus PGAFlexible Wall
SG-Flexible
LB-Flexible
ΔKae at Max. Dynamic Wall Moment
y = 1.0221x - 0.4548R2 = 0.85
y = 1.0822x - 0.3853R² = 0.85
-0.2
0
0.2
0.4
0.6
0.8
0.2 0.4 0.6 0.8 1Δ
Kae
PGA
Seismic Coefficient versus PGAStiff Wall
SG-StiffLB-StiffΔKae at Max. Dynamic Wall Moment
Seismic Earth Pressure Coefficient IncrementCentrifuge Data
N. Sitar, PPC, January 26, 200934
KitayamaKitayama
Dam, KobeDam, Kobe
N. Sitar, PPC, January 26, 200935
Zipingpu
Dam
Photo by J. Sun
N. Sitar, PPC, January 26, 20093636
Favorable performance under seismic loadCrest Acceleration at Zipingpu Dam during Wenchuan Earthquake
N. Sitar, PPC, January 26, 200937
Crest Settlement ~ 73 cm at center
N. Sitar, PPC, January 26, 200938
~13 cm settlement, right abutment
N. Sitar, PPC, January 26, 200939
Photo by K. Mosalam
Crack repair in progress, expansion seals in process of being replaced
N. Sitar, PPC, January 26, 200940
Photo by K. Mosalam
4 unit, 760 MW powerhouse with minor damage
Wall shear cracks
Photo by K. Mosalam Photo by K. Mosalam
N. Sitar, PPC, January 26, 200941
N. Sitar, PPC, January 26, 200942
N. Sitar, PPC, January 26, 200943
Spillway
N. Sitar, PPC, January 26, 200944
Conclusions•
Earth pressure during seismic loading increases with depth similar to static and the “inverse triangle”
does not represent this condition
•
Mononobe
–
Okabe solution is strictly applicable only within the range of original model tests and cannot be simply extrapolated as has been done in the past
•
Seed & Whitman (1970) solution is similarly flawed since it relies on Mononobe-Okabe’s original work. However, their recommendation that no special provisions are needed for well designed retaining structures subject to ground motions <0.3 g are well supported by data and most recent experimental results
•
Nakamura’s (2006) experiments on gravity walls suggest no increment in lateral earth pressure in cohesionless
soil under seismic loading
•
Our results similarly suggest that lateral earth pressure increment is insignificant for a large range of ground motions. However, inertial forces on the walls have to be properly accounted for. Same conclusions
were reached by Clough and Fragaszy
(1977) who suggested that cantilever structures properly designed for inertial loading could handle seismic loads up to 0.5-0.6 g in granular backfill
N. Sitar, PPC, January 26, 200945
What does it mean for dam design/performance?
•
The data show that maximum earth pressure and maximum moment do not occur at the same instant of time. Consequently, the actual
loads will be less than conventional computations suggest
•
Current test results are valid for medium dense dry sand –
preliminary recommendation
∆KAE
= PGAff
– 0.4
•
Dam embankments are 3-D structures and the spillway structures need be designed for kinematic response of the whole embankment
•
In absence of other data, design for full passive force may be most appropriate for structures crossing dam embankments
•
Given the dimensions of the actual structures the structural design must consider the inertial loads due to the structure response itself
N. Sitar, PPC, January 26, 200946
Thank You!