geotechnical earthquake engineering · 2017. 8. 4. · rowe and davis (1982) finite element...
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Geotechnical Earthquake
Engineering
by
Dr. Deepankar Choudhury Humboldt Fellow, JSPS Fellow, BOYSCAST Fellow
Professor
Department of Civil Engineering
IIT Bombay, Powai, Mumbai 400 076, India.
Email: [email protected]
URL: http://www.civil.iitb.ac.in/~dc/
Lecture – 41
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IIT Bombay, DC 2
Module – 9
Seismic Analysis and
Design of Various
Geotechnical Structures
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IIT Bombay, DC 3
Seismic Design of Pile
Foundation
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4
Piles in liquefying soil under lateral loads:
Force method
Non-liquefiable layer
Non Liquefiable layer
HNL
Liquefiable layer
qL =30% of over
burden pressure Pressure
qNL = Passive earth Pressure
HL
JRA (1996): Idealisation for pile
design in liquefying soils
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5
Failure theory based on Tokimatsu et al. (1998) :
Prior to the development of pore water pressure, the inertia
force from the superstructure may dominate.
Kinematic forces from the liquefied soil start acting with
increasing pore pressure.
Towards the end of shaking, kinematic forces would dominate
and have a significant effect on pile performance particularly
when permanent displacements occur in laterally spreading soil.
III) Lateral movement
after earthquake
liquefaction
Inertia force
Ground
displacemen
t
I) During Shaking before
liquefaction
Inertia force
Bending
moment
Inertia force
I) During Shaking after
liquefaction
[see Choudhury et al., 2009, Proc. of National Academy of Sciences,
India, Springer, Sec. A]
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Case-Specific Design of Pile
Foundations under
Earthquake Conditions
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7
Typical Bore hole data for MBH# 1: Mangalwadi site, Mumbai
Layer No. Stratum Layer thickness (m) Depth
below GL
(m)
SPT ‘N’ value
1 Filled up soil 1.5 1.5 10
2 Yellowish loose sand 1.5 3.0 12
1.5 4.5 13
1.5 6.0 16
3 Black clayey soil 2.0 8.0 20
4 Yellowish clayey soil 1.8 9.8 25
5 Greyish hard rock - >9.8
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EQUIVALENT GROUND
RESPONSE ANALYSIS
See Phanikanth (2011), PhD Thesis, IIT Bombay, Mumbai, India.
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8
Amplification of acceleration vs. depth (m)
Typical Results
EQUIVALENT GROUND
RESPONSE ANALYSIS
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D. Choudhury, IIT Bombay, India
Model considered for single Pile
passing through liquefied layer
Soil-pile analysis considering
ground deformations
using finite difference technique
ANALYTICAL
MODEL
[Phanikanth et al.
(2013), Int. Jl. of
Geomech., ASCE]
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D. Choudhury, IIT Bombay, India
Governing Equations for solving the basic differential equation of
laterally loaded pile in liquefied zone is given below:
y = lateral displacement of pile; z = depth from ground; EI = flexural rigidity of pile.
Sf is scaling factor varying from 0.001 to 0.01 (Ishihara and Cubrinovski,1998)
as compared to normal soil condition where there is no liquefaction .
Tokimatsu et al. 1998
[AIJ ( 2001)]
[Phanikanth et al.
(2013), Int. Jl. of
Geomech., ASCE]
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D. Choudhury, IIT Bombay, India
Bending moment in non liquefied and liquefied soil for
free headed single pile with floating tip in Mumbai [Phanikanth, Choudhury and Reddy, 2013, Int. Jl. of Geomech., ASCE]
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D. Choudhury, IIT Bombay, India
Typical effect of thickness of liquefiable soil layer on displacement profile
of free headed single pile with floating tip subjected to 2001 Bhuj motion [Phanikanth, Choudhury and Reddy, 2013, Int. Jl. of Geomech., ASCE]
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Combined Pile – Raft
Foundation (CPRF)
Under Earthquake Conditions
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INTRODUCTION
Piled raft foundation(also called composite foundation) solve:
1. Settlement – through interaction and load sharing.
2. Differential settlement – raft provide stiffness against load.
3. Economical - reducing number of piles.
Poulos et al. (2001) has examined a number of idealized soil profiles, and found that soil profiles consisting of relatively stiff clays and relatively dense sands may be favourable for piled raft foundation.
Construction: 1988 - 1990
Foundation: CPRF
Height: 256 m Messeturm tower, Germany
(Katzenbach et al. 2005)
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Foundations of high-rise buildings in Frankfurt am
Main, Germany
The subsoil of Frankfurt am Main mainly consists of non homogeneous, stiff and
over consolidated tertiary ”Frankfurt clay” with embedded limestone bands of
varying thicknesses. 15
(Katzenbach et al. 2005)
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Tower
Lower Sections
Hydraulic Jacks
Tower 1
Tower 2
Deutsche Bank · Frankfurt am Main, Germany
Height: 162 m
Settlement: max. 22 cm / min. 10 cm
Katzenbach et al. (2009)
-12.8 m
0.0 m
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→ Combined Pile-Raft Foundation (CPRF) Katzenbach et al. (2009)
Settlements calculated for a shallow foundation:
s > 40 cm
z = 0 - 20 m → 75 - 80 %
Messeturm · Frankfurt am Main,
Germany
Settlements:
Messeturm · Frankfurt am Main, Germany
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dydxy,x,s)s(R k,raft
m
1j
k,raftj,k,pilek,tot sRsRsR
sRsRsR j,k,sj,k,bj,k,pile
Total resistance of the CPRF:
Pile resistance:
Raft resistance:
Bearing concept of a
Combined Pile-Raft Foundation (CPRF)
Katzenbach et al. (2012)
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Analytical study:
19
Katzenbach et al. (1998) had suggested that designing Combined Pile-Raft
Foundations (CPRF) requires the qualified understanding of soil-structure
interaction.
Rtotal,k = ΣRpile,k, j + RRaft, k
Total resistance of the CPRF:
Pile resistance: sRsRsR jksjkbjkpile ,,,,,,
Raft resistance:
dydxyxssR kraft ,,)(,
αCPRF is set between 0.45-0.55
s =
(Katzenbach et al. 1998).
, ,
1
,
( )
( )
m
pile k j
j
CPRF
tot k
R s
R s
CPRF coefficient:
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20
Three dimensional view of pile group and pile-raft model in ABAQUS
(Eslami et al. 2011)
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Dynamic loading response:
21
Comparison of acceleration and bending moment response of under
sinusoidal accelerations
(Eslami et al. 2011)
Input acceleration – 1 m/sec2
Input frequency – 1 Hz
36% decrease in
piled raft model
54 %
decrease in
piled raft
model
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Seismic loading response:
• El- centro acceleration time history was chosen.
• Input acceleration and displacement- 4.21m/sec2 and 37.4 cm.
22
Acceleration response
34% reduction
(Eslami et al. 2011)
piled raft pile group
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9%
reduction
Horizontal displacement response under El- centro seismic
loading
Piled raft pile group
(Eslami et al. 2011) 23
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Case Study
Combined Pile – Raft
Foundation (CPRF)
under Earthquake
Conditions
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Case study of pile-raft foundation during 2011 Tohoku earthquake
Yamashita et al. (2011):
Building located at JAPAN PROTON ACCELERATOR RESEARCH COMPLEX (JPARC).
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Pile raft foundation
371 PHC piles
Diameter – 0.6m to 0.8m
Earthquake occurred – 44
month after the end of
construction.
Epicenter -270 km from
the site
Ground acceleration –
3.24 m/s2 and 2.77 m/s2 for
the horizontal and vertical
directions .
Yamashita et al. (2011)
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Plan of foundation profile with monitoring
devices Profiles of vertical ground displacements
Yamashita et al. (2011) (Yamashita et al. (2012)
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Ratio of load carried by pile Pile P1 Pile P2
Decreased from 0.85
to 0.82 after the
earthquake
Decreased from 0.67
to 0.57 after the
earthquake
(Yamashita et al. 2012) 27
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International Guideline on CPRF – 2012
by
ISSMGE Technical Committee
TC 212 – Deep Foundations
(www.issmge.org)
D. Choudhury, IIT Bombay, India
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IIT Bombay, DC 32
Seismic Design of
Ground Anchors
See, Rangari, S. M. (2013), PhD Thesis, IIT Bombay, Mumbai, India.
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33
• To mitigate the effect of earthquake Ground Anchors can be used for structures
subjected to uplift / pullout loads.
• Estimation of Uplift Capacity of Ground Anchor is an application of passive earth
pressure theory.
• Problem is more complex under seismic conditions.
INTRODUCTION
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34
Selected Available Studies (Static Condition)
Author Method of Analysis Failure plane Seismic Analysis
Meyerhof and Adams
(1968)
Limit Equilibrium Logspiral No
Rowe and Davis (1982) Finite Element
/Experimental
-- No
Murray and Geddes (1987) Experimental/Limit
equilibrium/limit analysis
--- No
Kumar (1999) Method of slices Logspiral No
Merifield and Sloan (2006) Limit analysis (Upper and
lower bound)
Planar No
Deshmukh et al. (2011) Limit Equilibrium Planar No
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2011) in ASCE GSP 211, pp. 1821-1831
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Available Studies
• Scarcity of research and design methods for estimation of vertical uplift capacity of
horizontal and inclined strip anchors under earthquake conditions using both pseudo-
static and pseudo-dynamic approaches.
Author Method of Analysis Failure plane Seismic Analysis
Kumar (2001) Upper bound limit analysis Planar Yes
(Pseudo-static)
Choudhury and Subba
Rao (2004, 2005)
Limit Equilibrium Logspiral Yes
(Pseudo-static)
Ghosh (2009) Upper bound Limit analysis Planar Yes (Pseudo-
dynamic)
Rangari et al. (2012) Limit Equilibrium Planar Yes (Pseudo- static)
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REVIEW OF LITERATURE
Very few researchers obtained the uplift capacity of obliquely loaded horizontal
strip anchor and all under static conditions;
•
Author Analysis Method Failure plane Seismic Analysis
Meyerhof (1973) Limit equilibrium/ Model test
Logspiral No
Das and Seeley (1975)
Model Test --- No
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2012) in ASCE GSP 225, pp. 185-194.
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REVIEW OF LITERATURE
Author Analysis Method Failure plane Seismic Analysis
Meyerhof (1973) Limit Equilibrium Logspiral No
Hanna et al. (1988) Limit Equilibrium
Planar No
Maiah et.al (1986) Empirical relation --- No
Choudhury and Subba Rao (2005)
Limit equilibrium Logspiral Yes (Pseudo-static)
Choudhury and Subba Rao (2007)
Limit equilibrium Logspiral Yes (Pseudo-static)
Ghosh (2010) Upper bound limit analysis
Planar Yes (Pseudo-dynamic)
•It shows the scarcity of research for the obliquely loaded inclined strip
anchors under static condition and yet untouched under the seismic
condition.
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Kötter’s (1903) equation
Kötter’s (1903) equation gives solution for determining the distribution of soil
reaction on failure plane
Where,
dp = differential reaction pressure on the
failure Surface,
ds = differential length of failure surf ace,
p = uniform pressure on the failure surface
d = differential angle,
= angle of failure plane formed by inclination of tangent at the point of interest
with the horizontal
= unit weight of soil and
= soil friction angle
sintan2ds
dp
ds
dp
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39
The total reaction R1 and R3 on
the failure surfaces are computed
by integrating Kötter’s equation;
•W is the weight of failure
soil block,
• Pp d1 and Pp d3 are the
seismic passive
resistances,
• is soil friction angle,
• B is width and H is depth
of anchor
•Qh and Qv are total
seismic horizontal and
vertical inertial forces
respectively.
•Simple Planar failure surface. Hence the
Kötter’s (1903) equation reduces to,
sinp s
Horizontal Strip Shallow Anchor under Seismic Conditions
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• Consider failure block above the anchor.
• The mass of the elementary strip is given by;
• The horizontal and vertical acceleration at any depth z and time t below the
ground surface can be expressed as;
• Total horizontal and vertical inertial forces acting within the failure zone
(CDEF) can be expressed as,
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Proposed Method by Rangari et al. (2013)
γBdzm =
g
( , ) sin and ( , ) sinh h v vs p
H z H za z t a t a z t a t
V V
2 22 22 cos cos and 2 cos cos
4 4
h vh v
Bk BkQ t Q t
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2013) in Geotechnical and Geological
Engineering , Springer, Vol. 31(2), pp. 569-580.
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41
where, =TVs is the wavelength of the vertically propagating shear wave, = TVp
is the wave length of the vertically propagating shear wave,
and
The gross pullout capacity (Pud) is given by;
•The net seismic uplift capacity of anchor, qudnet
Proposed Method of Rangari et al. (2013) contd.
1 3 2 2sin sinud p d p d vP P P W Q
s
Ht
V p
Ht
V
2
22 tan 2 cos cos tan
2
hd p d
kF K t
B
The net seismic uplift capacity factor,
2 20.5
ud vud d
P W Qq BF
B
Where, Embedment ratio, = H/B and Kp d is a net seismic passive earth pressure
coefficient
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Typical Design Charts (Results) for Seismic Uplift Capacity
Factor of Horizontal Shallow Anchors
a. Using Pseudo-Static approach b. Using Pseudo-Dynamic approach Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2013) in Geotechnical and Geological
Engineering , Springer, Vol. 31(2), pp. 569-580.
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43
Comparison of ultimate seismic uplift capacity factor (F E = Pud/ B2) for various
values of kh and kv= 0.5 kh for = 30 , = 4 with H/ =0.3 and H/ =0.16.
kh Ghosh (2009)
Pseudo-
dynamic
Kumar
(2001)
Pseudo-
static
Choudhury and
Subba Rao
(2004)
Pseudo-static
Present study
Pseudo-
static
Pseudo-
dynamic
0.0
13.27
13.27
12.89
13.01
13.01
0.1
12.59
12.48
12.44
12.12
12.08
0.2
11.90
11.71
11.96
11.25
11.29
0.3
11.14
10.90
11.53
10.39
10.61
0.4
10.21
9.81
11.01
9.56
10.05
Comparison of Results
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2013) in Geotechnical and Geological
Engineering , Springer, Vol. 31(2), pp. 569-580.
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44
For a plane failure surface, Kötter’s equation (1903), takes the following form
where,
p = uniform pressure on failure
plane
= unit weight of soil
s = represents the distance of failure plane
as measured from ground surface
The total reaction R1 and R3 on the failure surfaces are computed by integrating
Kotter’s equation;
sinp s
Inclined Strip Shallow Anchor under Seismic Conditions
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2012) in Disaster Advances, Vol. 5(4), pp. 9-16.
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45
For Design, qudnet can is expressed as,
Net seismic uplift capacity factor ( F d) can be obtained as;
where, embedment ratio, and Kp d is net seismic passive earth pressure
coefficient.
Critical angle of failure planes:
The trial value of α1 and α3 are obtained such that the values of Ppγd1 and Ppγd3
should be same obtained from failure wedges CDF and ABE respectively.
B
H
udnet dq 0.5 BF
2 2 2
d P d
v h
F tan 0.25 tan K cos tan tan
2 1 k sin k cos
Inclined Strip Shallow Anchor under Seismic Conditions
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2012) in Disaster Advances, Vol. 5(4), pp. 9-16.
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46
Typical Design Charts (Results) for Seismic Uplift Capacity
Factor of Obliquely loaded Inclined Shallow Anchors
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2012) in Disaster Advances, Vol. 5(4), pp. 9-16.
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47
COMPARISION OF RESULTS
Comparison of net SEISMIC uplift capacity factor (F d) with results from
literature for =30 , with = 30 and ε =3.
kh Choudhury and Subba Rao
(2005)
Present study
kv=0.0kh kv=0.5kh kv=1.0kh kv=0.0kh kv=0.5kh kv=1.0kh
0.0 5.85 5.85 5.85 6.28 6.28 6.28
0.1 5.48 5.32 5.16 6.27 5.95 5.61
0.2 5.39 4.76 4.43 6.25 5.62 5.05
0.3 5.28 4.31 3.53 6.13 5.2 4.41
0.4 4.99 3.69 -- 5.94 4.73 --
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2012) in Disaster Advances, Vol. 5(4), pp. 9-16.
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48
COMPARISION OF RESULTS
Comparison for ultimate SEISMIC uplift capacity factor (F E = Pud / B2) for
=0 , ε =1 and kv = 0.0 with results from literature.
0 kh Kumar
(2001)
Ghosh
(2009)
Present
study
300
0.0 1.577 1.577 1.563
0.1 1.566 1.571 1.481
0.2 1.544 1.533 1.403
0.3 1.499 1.520 1.329
400
0.0 1.839 1.839 1.839
0.1 1.832 1.835 1.709
0.2 1.815 1.821 1.587
0.3 1.786 1.798 1.472
500
0.0 2.192 2.192 2.145
0.1 2.187 2.189 1.952
0.2 2.174 2.179 1.771
0.3 2.155 2.163 1.601
Rangari, S.M., Choudhury, D., Dewaikar, D.M. (2012) in Disaster Advances, Vol. 5(4), pp. 9-16.