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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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  • 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

  • IIT Bombay, DC 2

    Module – 9

    Seismic Analysis and

    Design of Various

    Geotechnical Structures

  • IIT Bombay, DC 3

    Seismic Design of Pile

    Foundation

  • 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

  • 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]

  • Case-Specific Design of Pile

    Foundations under

    Earthquake Conditions

  • 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

    -

    EQUIVALENT GROUND

    RESPONSE ANALYSIS

    See Phanikanth (2011), PhD Thesis, IIT Bombay, Mumbai, India.

  • 8

    Amplification of acceleration vs. depth (m)

    Typical Results

    EQUIVALENT GROUND

    RESPONSE ANALYSIS

  • 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]

  • 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]

  • 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]

  • 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]

  • Combined Pile – Raft

    Foundation (CPRF)

    Under Earthquake Conditions

  • 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)

  • 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)

  • 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

  • → 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

  • 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)

  • 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:

  • 20

    Three dimensional view of pile group and pile-raft model in ABAQUS

    (Eslami et al. 2011)

  • 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

  • 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

  • 9%

    reduction

    Horizontal displacement response under El- centro seismic

    loading

    Piled raft pile group

    (Eslami et al. 2011) 23

  • Case Study

    Combined Pile – Raft

    Foundation (CPRF)

    under Earthquake

    Conditions

  • Case study of pile-raft foundation during 2011 Tohoku earthquake

    Yamashita et al. (2011):

    Building located at JAPAN PROTON ACCELERATOR RESEARCH COMPLEX (JPARC).

    25

    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)

  • 26

    Plan of foundation profile with monitoring

    devices Profiles of vertical ground displacements

    Yamashita et al. (2011) (Yamashita et al. (2012)

  • 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

  • International Guideline on CPRF – 2012

    by

    ISSMGE Technical Committee

    TC 212 – Deep Foundations

    (www.issmge.org)

    D. Choudhury, IIT Bombay, India

  • IIT Bombay, DC 32

    Seismic Design of

    Ground Anchors

    See, Rangari, S. M. (2013), PhD Thesis, IIT Bombay, Mumbai, India.

  • 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

  • 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

  • 35

    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)

  • 36

    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.

  • 37

    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.

  • 38

    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

  • 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

  • • 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,

    40

    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.

  • 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

  • 42

    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.

  • 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.

  • 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.

  • 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.

  • 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.

  • 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.

  • 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.