1 One Dimensional Seepage

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    Priyantha Jayawickrama, Ph.D.

    Associate Professor

    One-Dimensional SeepagePermeability and Darcys Law

    Texas Tech UniversityDepartment of Civil and Environmental Engineering

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    CE 5321-001: Advanced Soil Engineering 2

    References

    Chapters 17, 18 and 19,

    Lambe and Whitman, John Wiley

    Chapter 17: One-dimensional flowChapter 18: Two-dimensional flow

    Chapter 19: Soil Permeability and Filter

    Requirements

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    CE 5321-001: Advanced Soil Engineering 3

    Permeability and Seepage

    Why would geotechnical engineers be

    concerned with this topic?

    What applications come to mind?

    What are the principles governing this

    process?

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    CE 5321-001: Advanced Soil Engineering 4

    Subsurface Water

    Vadose Zone

    (zone of aeration)

    Ground Surface

    capill ary fr inge Water Table

    (Phreatic Surface)

    Zone of Phreatic Water

    (zone of saturation)

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    CE 5321-001: Advanced Soil Engineering 5

    Artesian Conditions

    Confined

    sandstone

    aquifer

    Impermeable

    shale

    Non-flowing

    well

    Artesian pressure

    surface

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    CE 5321-001: Advanced Soil Engineering 6

    Seepage Illustration:Loop 287, Lufkin, TX

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    CE 5321-001: Advanced Soil Engineering 7

    Roadbed Excavation in Sandy Soilk 1 x 10 -4cm/sec

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    CE 5321-001: Advanced Soil Engineering 8

    High Head: Dewatering Required(grid of French drains)

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    Antilley Road Bridge, Abilene

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    CE 5321-001: Advanced Soil Engineering 10

    Antilley Road Bridge,Abilene

    30-ft

    100.1-ft92.3-ft

    79.9-ft

    61.6-ft

    67.3-ft

    61.4-ft

    70.0-ft

    Seepage location

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    To Estimate Seepage Loss

    Seepage through the body of the dam

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    To Estimate Seepage LossSeepage through the body of the dam and the foundation soil

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    To Estimate Seepage LossSeepage through the body of the dam and the foundation soil

    Anisotropic Soil

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    To Estimate Pore WaterPressures

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    15

    To Estimate Pore Water Pressures

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    16

    To Evaluate Quicksand Conditions

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    CE 5321-001: Advanced Soil Engineering

    17Dewatering Excavations

    Other ApplicationsDewatering System Design

    http://images.google.com/imgres?imgurl=http://www.godwinpumps.com/images/Wellpointphoto.jpg&imgrefurl=http://www.godwinpumps.com/wellpoint.html&h=253&w=400&sz=33&tbnid=LbTzrFXsfrcJ:&tbnh=75&tbnw=120&hl=en&start=10&prev=/images%3Fq%3Ddewatering%26svnum%3D10%26hl%3Den%26lr%3D%26sa%3DN
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    Other ApplicationsDrainage System Design

    Pavement Drainage

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    Drainage behind Retaining Walls

    Other ApplicationsDrainage System Design

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    Other ApplicationsDrainage System Design

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    Other ApplicationsDrainage System Design

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    H

    b

    d

    w

    1

    2 3

    4

    P

    Other ApplicationsDrainage System Design

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    Other ApplicationsDrainage System Design

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    Flow through soil and rockmaterial Soil and rock are porous

    materials

    Fluid flow takes place through

    interconnected void spacesbetween particles and notthrough the particlesthemselves

    No soil or rock material isstrictly impermeable

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    Question

    What causes flow of waterthrough soil?

    Answer:

    A difference in TOTAL HEAD

    We will focus on Water Movement withinSaturated Soils!

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    Total Head = pressure head +elevation head

    soil

    No Flow!

    5ft 5ft

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    soil

    Flow from left to right!

    5ft

    9ft

    Total Head = pressure head +elevation head

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    soil

    Flow from left to right!

    Total Head = pressure head +elevation head

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    5ft

    5ft7ft

    Total Head = pressure head +elevation head

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    Comments re: Total Head

    A differencein to tal headis required to cause

    movement of water through soil.

    Total head is measured in units of length;e.g., feet or meters; not psf, kPa, etc.

    Darcys Law, governing fluid flow through a

    porous medium, takes this one step further:

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    Pressure Head, hp= pressure/w

    Elevation Head, he= distance from

    datum

    Total head = hp+ he

    Velocity head is negligibly small, e.g.at flux = 2ft/min, velocityhead=0.00002 ft.

    Total Head

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    How do you estimate flow rate ?

    Flow rate will be controlled by Difference in total head between Point A & Point B

    Distance between Point A & Point B

    Type of Soil

    5ft

    5ft7ft

    A

    B

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    Some Definitions

    Quantity of Flow, Q Cu.ft

    Flow Rate, q = Q/t Cu.ft/min

    Flux, v = q/A Cu.ft/min/sq.ft = ft/min

    5ft

    5ft7ft

    A

    B

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    Some Definitions

    Hydraulic Gradient, i (no units)

    L

    h

    L

    HHi

    AB

    BA

    5ft

    5ft7ft

    A

    B

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    Darcys Law

    k= coefficient of permeability

    i = hydraulic gradient (i < 5, laminar flow)

    L

    hi

    A

    tQ

    A

    qv

    )/(

    ikv

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    Darcys Law; Applications

    Elev. 0 ft

    Elev. 30 ft

    12ft

    57ft

    Confined Aquifer

    Very low

    permeable

    soil

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    Coefficient of Permeability

    k= coefficient ofpermeability, or

    hydraulic conductivity

    k depends on the poresize in the soil

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    Some typical k - values

    uniform coarse sand .. k = 4 x 10 -1cm/sec

    clean sand & gravel.. k = 1 x 10 -2cm/sec

    silty sand . k = 1 x 10 -4cm/sec

    sandy clay .. k = 5 x 10 -6cm/sec

    Compacted clay .. k = 1 x 10 -7cm/sec

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    Order of Magnitude ofk - values

    Uniform coarse sand is1000 times more

    permeable thansilty sand

    Silty sand is 1000 times more permeable thanCompacted clay

    Coarse Sand . Drainage Layers

    Compacted Clay . Liner Material for Ponds

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    Empirical relationships toestimate permeability, k

    21010Dk

    2155.3 Dk

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    Grain Size Distribution Curves

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    Head DistributionBelow Ground Water Table

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    Head DistributionAbove Ground Water Table

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    Calculation of Pressure Head inSeepage Conditions

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    Calculation of Pressure Head inSeepage Conditions

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    Calculation of Pressure Head inSeepage Conditions

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    Calculation of Pressure Head inSeepage Conditions

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    Oil Refinery Site, Kawasaki, Japan

    Previously, for static ground water conditions

    (Chapter 16, Lambe and Whitman)

    Now modified for steady seepage conditions

    See Handout

    Calculation of Effective Stress underSeepage Conditions

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    +4

    -11

    -21

    -36

    -51

    C l l i f Eff i S d

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    Calculation of Effective Stress underSeepage Conditions

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    Calculating Seepage Force

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    Calculating Seepage Force

    This is what you havewhen upward seepage

    is occurring

    This is what you wouldhave had under staticwater conditions

    The differencerepresents the energylost due to seepage

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    Calculating Seepage Force, iw

    L

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    Consider:

    Boundary water forces + Total weights

    OR seepage forces + submergedweights

    Seepage force/volume = iw

    Force Equilibrium

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    Evaluating Quick Conditions

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    Evaluating Quick Sand Conditions

    wstwv hqba

    :00 sqandaWhen

    wtv hbb )(

    wwtv hb )(

    0: vc andiiconditionsquickFor

    w

    sub

    w

    wt

    c

    cwwtb

    hihb

    )(,thereforeand)(0

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    FOS against Quick SandConditions

    w

    sub

    w

    wt

    c

    cb

    hi

    )(

    Factor of Safety against quicksand conditions, F

    actual

    c

    i

    iF