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  • 8/14/2019 Latsis - Rainfall Induced Landslides - Why They Occur and Some Mitigating Measures [Compatibility Mode]

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    Rainfall Induce Landslides Why they occur and some

    mitigating measures

    Tan S.A1, David Toll2, and K.K.Phoon11The National University of Singapore

    2University of Durham, UK

    Latsis Symposium by CCES at ETH-Z,Zurich, Switzerland, 17-19 Sep 2007

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    2

    Outline

    Introduction Climate and slope stability

    Soil Strength as function of Infiltration Cases: Kranji Racecourse and NUS

    Biz School

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    3

    Introduction

    Climate in the tropics

    Singapore landslides and rainfall events empirical observations

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    Inference from Measured Pore-Water Pressures

    (pwp) at NTU-CSE

    Wet period rainfall=86mm in Dec 1999; dry period rainfall = 1mm inMar 2000

    Small rainfall in Mar 2000 produce large change pwp near surface at1-1.5m depth

    After 24 hr equalization; pwp near surface drop back and pwp at 1-1.5m depth increased slightly, due to water infiltration

    But at deeper depth of 2.5-3m no significant pwp change For large rainfall in Dec 1999; observe only small cahnges in pwp

    near surface, with pwp approaching hydrostatic condition

    Data suggests that there is still suction in slope even wettest time of

    the year

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    Unsaturated soil strength

    State Variables defined as:

    =

    =

    )(

    )(

    wa

    an

    uu

    u Net normal stress

    Matric suction

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    Unsaturated soil strength

    Shear Strength is the Extended Mohr-Coulomb failure criteria:

    =

    =

    =

    =

    =

    =

    ++=

    )(

    )(

    '

    '

    :

    tan)('tan)('

    wa

    an

    b

    bwaan

    uu

    u

    c

    where

    uuuc

    Shear strength

    Effective cohesion for saturated soils

    Effective friction angle for saturated soils

    Friction angle with respect to matric suction in unsaturated soils

    Net normal stress

    Matric suction

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    Saturated soil strength

    Shear Strength is Mohr-Coulomb:

    ==

    =

    =

    +=

    =

    )('

    '

    :

    'tan)('

    ,'

    wn

    wn

    b

    u

    c

    where

    uc

    and

    Shear strength

    Effective cohesion for saturated soils

    Effective friction angle for saturated soils

    Normal effective stress

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    Infiltration Seepage Analysis

    Transient Seepage FEM Analysis

    Soil Water Characteristic Function

    Soil Permeability Function

    Infiltration Input Results of Analysis

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    Equation of Continuity

    Constitutive Equation: Darcys Law

    yx qq h

    Q c

    x y t

    + + =

    Groundwater Flow Theory

    x x hq kx

    =

    y y hq ky

    =

    q : the specific discharge (m/s)c : the storage coefficient (m-1)h: total head (m)Q: a source (m3/s) per unit vol.

    k : the coefficient of permeability (m/s)

    Flow in Flow out

    Flow out

    Flow in

    Stored in

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    Water flow in unsaturated soilWater content and permeability in unsaturated zone is a

    function of suction pressure

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    Water flow in unsaturated soil

    () Soil water characteristic curve

    K () permeability curve

    ( )s

    CStorage Coefficient

    =

    ( )k kSoil Permeability =

    These curves are from experiments

    Unsaturated soil has k severalorders less than saturated soils

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    Precipitation:

    max

    rain max min

    min

    if Ponding

    if and

    if No infiltrationx x y y

    h y h

    q n q n q h y h h y h

    h y h

    = +

    + = < + > +

    = +

    Boundary Conditions for Rainfall

    Flux boundary condition

    ClosedClosed

    Closed

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    Result of 1-D Infiltration Analysis1D Infiltration

    -0.5

    0

    0.5

    1

    1.5

    2

    2.5

    3

    3.5

    -5 0 5 10 15 20 25 30 35

    Suction Pressure [kN/m2]

    El

    evation[m]

    Initial SST=0.1 day

    T=0.25day

    T=0.5day

    T=1.0day

    T=5.0day

    Gardner's Theory

    Gardner's 1D Infiltration Problem

    alpha 2

    Sres= 0.23 ksat= 1 m/day

    Ssat= 1

    p S(p) K(p)

    0 1.00 1.00

    0.5 0.51 0.37

    1 0.33 0.14

    1.5 0.27 0.05

    2 0.24 0.02

    2.5 0.24 0.01

    3 0.23 0.00

    Gardner's Theory

    q ksat y p [m] P[kN/m2]

    2 0.1 1 0.00 0.00 0

    2 0.1 1 0.50 0.42 4

    2 0.1 1 1.00 0.75 8

    2 0.1 1 1.50 0.97 10

    2 0.1 1 2.00 1.08 11

    2 0.1 1 2.50 1.12 11

    2 0.1 1 3.00 1.14 11

    +

    =

    sat

    y

    sat

    pk

    qe

    k

    q

    .1ln

    1

    peSSSS ressatres

    += )(

    pekksat

    = .

    Input rainfall = 0.1 m/day

    SS solution

    after 5 days

    Infiltration caused significant loss of suction

    Loss of suction result in reduction of shear strength, which may trigger slope failure

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    1D Infiltration Video

    Click for Video

    Input flux= 0.1mm/day

    ClosedClosed

    Closed

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    Case 1: Kranji Racecourse About Dec 1998, a 70m long slope with

    gradient of 1(V):2(H) was cut in medium stiff

    residual clayey soil

    After period of intense rainfall, slip failure

    landslip about 1 to 1.5m deep over slopeof 30m length

    Slope repaired using dry cut fill soil obtainedfrom same site failed repeatedly without useof subsurface drains

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    Develop tension crack below crest of slope, why?

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    Infiltration Analysis Rain 20 mm/dayEvolution of Saturation Zone

    ConstantH2

    Click for Video

    ConstantH1

    Closed No Flow

    Input flux = 20mm/day

    Input flux = 20mm/day

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    Shallow Slip of Saturated Zone (Head)

    Click for Video

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    Shallow Slip of Saturated Zone (Flow)

    Click for Video

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    Site investigation

    Distance (m)

    0 2 4 6 8 10 12Distance (m)

    98

    100

    102

    104

    106

    108

    110

    Eleva

    tion(mRL)

    Observed Slip Plane

    Probable GroundWater TableP1

    P2

    P3

    104.5

    103.8

    1V:2H

    104.6

    106.3

    Waterstandpipes

    After a few days

    without rain, measured

    GWT appears to

    coincide with level ofobserved slip surface

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    Influence of Infiltration on Suctions and Soil Strengths

    Kranji Pore Pressure Distribution at Mid-Slope (3m up)

    100

    101

    102

    103

    104

    105

    106

    107

    -70 -60 -50 -40 -30 -20 -10 0 10 20

    Total Pore Pressures [kPa]

    Elevation[m]

    1-day

    2-day

    3-day

    4-day

    5-day

    Kranji Pore Pressure Distribution at 4.5 m Up-Slope

    102

    103

    104

    105

    106

    107

    108

    -30 -20 -10 0 10 20 30 40

    Total Pore Pressures [kPa]

    Elevation[m]

    1-day

    2-day

    3-day

    4-day

    5-day

    After 5 days of rain, nearly all suction is removed up to mid-slope height

    Suction of < 15 kPa remains at 4.5m height above toe of slope; c < 3 kPa

    Table 1. Variation of Cohesion with Matric Suction

    Matric suction [kPa] 5 10 15 20 25 30

    b[deg] kPa

    10 0.88 1.76 2.64 3.53 4.41 5.29

    15 1.34 2.68 4.02 5.36 6.70 8.0420 1.82 3.64 5.46 7.28 9.10 10.92

    bwa uuc tan)(' =

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    GWT

    Parallel Seepage

    Hh

    slip plane

    Failure analysis of Shallow Slip = slope angle (degrees)H = depth to slip surface (m)

    h = height of GWT from slip surface (m)

    tan

    'tan))/()(1(

    cossin

    ' Hh

    H

    cFS w

    +=

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    Design for permanent stable slope

    Internal drainage design to maintain

    significant unsaturated soil zone inshallow soils along slope

    Transient seepage analysis to validate

    design

    Stability analysis to show that design

    has adequate long-term FOS

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    Transient Seepage with 8m deep drains

    at toe of slope and 20 mm/day rain-15.000 -10 .000 -5 .000 0 .000 5 .000 10 .000 15.000 20.000 25 .000

    85.000

    90.000

    95.000

    100.000

    105.000

    110.000

    115.000

    Active groundwater hea d

    Phase number: 1 Phase time: 5 day, Extreme groundwater head 109.10 m

    m

    99.600

    100.000

    100.400

    100.800

    101.200

    101.600

    102.000

    102.400

    102.800

    103.200

    103.600

    104.000

    104.400

    104.800

    105.200

    105.600

    106.000

    106.400

    106.800

    107.200

    107.600

    108.000

    108.400

    108.800

    109.200

    Near Steady-State condition after 5 dayof rain at 20 mm/day

    Unsaturated Zone

    8m-deep drains

    ConstantH2

    ConstantH1

    Closed No Flow

    Input flux = 20mm/day

    Input flux = 20mm/day

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    Infiltration Analysis Rain 20 mm/daySaturation Zone for Slope with 8m Deep Internal Drains

    8m-deep pipe drains

    Click for Video

    I fil i A l i R i /d

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    Infiltration Analysis Rain 20 mm/dayGW Head for Slope with 8m Deep Internal Drains

    8m-deep pipe drains

    Click for Video

    I filt ti A l i R i 20 /d

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    Infiltration Analysis Rain 20 mm/dayTransient Flow for Slope with 8m Deep Internal Drains

    8m-deep pipe drains

    Click for Video

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    Influence of Infiltration on Suction Pressures in

    Shallow Soils with 8m Deep drainsKranji Pore Pressure Distribution at Mid-Slope (3m up)

    100

    101

    102

    103

    104

    105

    106

    107

    -30 -20 -10 0 10 20 30Total Pore Pressures [kPa]

    Elevation[m]

    1-day

    2-day

    3-day

    4-day

    5-day

    Kranji Pore Pressure Distribution at 4.5 m Up-Slope

    102

    103

    104

    105

    106

    107

    108

    -20 -10 0 10 20 30 40

    Total Pore Pressures [kPa]

    Elevation

    [m]

    1-day

    2-day

    3-day

    4-day

    5-day

    +ve suction

    -ve pressure

    Small changes of soil suction up to 1m depth at mid-slope (3m up slope)

    No changes to soil suction at 4.5m up slope

    Soil strength is little affected by Infiltration for rain at 20mm/day over 5 days

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    Seepage with 4m deep drains

    GEONET 4m Depth

    Pond le vel a t 104 .6 m R L

    GEONET

    Co ncrete Liner

    Recom pacted Res idual Soi l 0 .5 m Sand Track

    15 0 mm /h Rainfa l l

    GWT

    2.1829e-012

    5.2122e-008

    5.2122e-008

    1.4009e-011

    3.0994e-004

    Distance (m)

    0 5 10 15 20 25 30 35 4090

    92

    94

    96

    98100

    102

    104

    106

    108

    110

    112

    114

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    FOS with 4m Deep Drains

    1.8

    1.8 2

    2.2

    2.4

    1.269

    D e s c r i p t io n : P o n d W a t e r

    U n i t W e igh t : 9 . 8 0 7

    D e s c r ip t io n : R e c o m p a c te d R e s id u a l S o il

    U n it W e ig h t : 1 8C o he s io n : 3

    P h i: 2 0

    D e s c r ip t io n : In s it u R e s id u a l S o il

    U n i t W e i g h t : 1 8

    C o h e s io n : 1 0

    Ph i : 2 7

    G W T

    E O N ET 4 m D e p th

    G E O N E T

    0 .5 m S a nd Tr ac k

    1 5 0 m m /h R ain fa l l

    Dis tance (m )

    0 5 10 15 20 25 30 35 4090

    92

    94

    96

    98

    100

    102

    104

    106

    108

    110

    112

    114

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    Seepage with 8m Deep Drains

    GEON ET 8m Depth

    Pon d le vel a t 104.6 m RL

    GEONET

    Concrete L iner

    Recom pacted Res idua l So ilGW T

    0.5m Sand track

    150 m m /h R ain fa ll

    7.0160e-008

    7.0158e-008

    7.6699e-012

    3.1082e-004

    Distance (m)

    0 5 10 15 20 25 30 35 4090

    92

    94

    96

    98100

    102

    104

    106

    108

    110

    112

    114

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    FOS with 8m Deep Drains

    1.7

    1.8

    1.9

    2

    2.2

    2.2

    1.617

    D e s c r i p t io n : P o n d W a t e rU n it W e ig h t : 9 .8 07

    D e s c r ip t io n : R ec o m p a c t e d R e s id u a l S o ilU n i t W eig h t: 1 8

    C o h e s io n : 5

    P h i : 2 1De s c ri p t io n : In s it u R e s id u a l S o il

    U n i t W e ig h t : 1 8

    C o h e s io n : 1 0

    P h i : 2 7

    G W T

    0 .5 m S a n d T r a c k

    G E O N E T 8 m D e p th

    1 5 0 m m / h R a in f a ll

    G E O N E T

    D is tanc e (m)

    0 5 10 15 20 25 30 35 4090

    92

    94

    96

    98

    100

    102104

    106

    108

    110

    112

    114

    Parametric Study of influence of Depth of Internal

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    Parametric Study of influence of Depth of InternalDrains

    Table 2: Influence of GEONET depth on GWT and FOS of repaired slope

    GEONET Depth

    (m)

    0 1 2 4 8 12 15

    GWT at Slope

    Crest (m RL)

    108.1 108.0 107.9 107.6 106.8 104.7 104.7

    GWT at Mid-

    Slope (m RL)

    107.1 106.9 106.4 105.7 104.7 104.7 104.7

    Seepage intoSlope (m

    3/s /m)

    1.89x 10

    -8 1.72x 10

    -9 9.80x 10

    -12 2.18x 10

    -12 < 1.0x 10

    -12 < 1.0x 10

    -12 < 1.0x 10

    -12

    Soil State in Slope Fully

    Soak

    Fully

    Soak

    Fully

    Soak

    Fully

    Soak

    Soften Comp-

    acted

    Comp-

    acted

    Drained cohesion

    c (kPa)

    3 3 3 3 5 10 10

    Drained friction

    angle, deg

    20 20 20 20 21 22 22

    Drained FS 0.923 0.968 1.137 1.269 1.617 1.780 1.808

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    Installation of 8m Deep DrainsModified Mannings Eqn. for discharge of equivalent pipedrain in-place of GEONET drain

    Q = 1.137A RH0.66 S0.5 (m3/s)A=flow cross-section area (sq-m)

    RH=hydraulic radius (m)

    =R/2 for full flowS=slope (m/m)

    Actual Repair used 75mm diameter perforated drainswrapped with geotextile filters at 1.5m centers to achievesame discharge capacity as Geonet Sheet Drain

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    Install geotextile-wrapped 15m long, 75-mm

    diameter pipe drains at 1.5 m intervals

    GW di h f i l i d i h

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    GW discharge from internal geo-pipe drains has

    performed well over last 10 years

    C S S

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    Case 2 Failure at NUS Biz School

    I filt ti A l i

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    Infiltration Analysis0.000 20.000 40.000 60.000 80.000

    80.000

    100.000

    120.000

    140.000

    Active groundwater head

    Phase number: 6 Phase time: 5 day, Extreme groundwater head 126.01 m

    m

    108.000

    109.000

    110.000

    111.000

    112.000

    113.000

    114.000

    115.000

    116.000

    117.000

    118.000

    119.000

    120.000

    121.000

    122.000

    123.000

    124.000

    125.000

    126.000

    127.000

    Building No influx

    Unsaturated Zone

    Near Steady-State condition after 30days of rain at 0.02 mm/day

    Nature of Slip is fairly deep seated

    Likely cause is combination of rain induced saturation leading to loss ofsuction and rising GWT

    Raised GWT

    Estimated Slip SurfaceConstantH2

    Constant

    H1

    Closed No Flow

    Input flux = 20mm/day

    S i f Sl b I fil i

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    Saturation of Slope by Infiltration

    Takes more than 20 days of rain at 20 mm/day to raisedGWT sufficiently to cause deep seated failure

    Initial GWT

    Click for Video

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    Transient Flow in Slope by Infiltration

    Takes more than 20 days of rain at 20 mm/day to raisedGWT sufficiently to cause deep seated failure

    Initial GWT

    Click for Video

    Long term Repair Strategy

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    Re-gradeslope

    Soil Nails

    Better drainsto minimize

    infiltration

    Long-term Repair Strategy

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    Conclusions Why shallow slip occurs is the result of unsaturated soilcreating a buffer with very low permeability thatprevents the saturation front from penetrating into

    deeper soils; where GWT are greater than 10m deep Infiltration analysis of the Kranji slope failure illustrates

    the saturation of a shallow slip mass for a small slope

    With the inclusion of a horizontal deep drains at the toe

    of the slope; a large unsaturated soil zone can bemaintained despite sustained heavy rainfall, providing apermanent safe slope over the last 10 years

    For the case of NUS large slope failure; it is more likelythat sustained heavy rain during the period of Dec 05 toJan 06 caused the rise of GWT to saturate the slopemass and trigger the deeper seated failure