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Sepaage and flownets Lecture 4

Flownet Seepage

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Soil Mechanics, Civil

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  • Sepaage and flownets

    Lecture 4

  • References

    Braja M Das, Principal of Geotechnical Engineering, fourth edition, PWS Publishing Company, 1998, BostonMuni Budu, Soil Mechanics and Foundations, 2ndedition, John Wiley & Sons, 2007, USAR.F. Craig, Soil Mechanics, (English & terjemahan Prof.Dr.Ir Budi S Supandji)Cernica, J.N., Soil Mechanics, John Wiley & Sons,1995Holtz, R.D., Kovacs, W.D., An introduction to Geotechnical Engineering, Prentice Hall, N.J., 1981

  • Laplace equations

    The assumptions :Darcys law is validThe soil is homogeneous and saturatedThe soil and water are imcompressibleNo volume change occurs

  • Laplace equations of continuity A B

    Impermeable soil layerWater incompressible and no vol. change :Flow x direction

    Flow z direction

  • Laplace equations of continuity A B

    Impermeable soil layer

    Darcys law : Isotrpic soil kx=kz

  • Simple flow S F Flow in Z direction

    A1 dan A2 are constant;

    For flow through layer 1 :

  • Simple flow S F Flow in Z direction

    A1 dan A2 are constant;

    For flow through layer 2 :

    From condtion 2:

  • Simple flow S F from and

    Flow of layer 1 = flow of layer2

  • Simple flow S F Example

    H1 = 300mm, H2 = 500mm, h1=600mm at z=200mm and h=500mm

    Determine h at z=600 mm

    Solution Z=200mm hence

    Because z=600mm is located in soil layer 2 hence,

    h = 179.9 mm

  • Water In

    )h =hA - hB

    Head Loss orHead Difference or Energy Loss

    hA

    hB

    i = Hydraulic Gradient

    (q)Water

    out

    Datum

    hA

    W.T.

    hB

    )h = hA - hB

    W.T.

    Impervious Soil

    Impervious Soil

    ZA

    Datum

    ZB

    q = v . A = k i A = k AhL

  • Three different scenarios (a) Static (b) Flow-up (c) Flow-down

    Stresses due to Flow

  • 12

    Stresses due to Flow

    X

    soil

    hw

    L

    Static Situation (No flow)

    z

    v = whw + satz

    u = w (hw + z)

    v ' = ' z

    At X,

  • 14 ft

    3 ft

    12 ft

    In Flow

    Out Flow 2 ft

    4 ft

    Datum

    3 ft

    3 ft

    8 ft

    Piezometer

    A

    B

    C

    D

    u =

    6 x

    62.4

    u =

    14 x

    62.

    4

    No Seepage

    Buoyancy

    Ws

    Ws

    Ws

    Ws

    Ws

  • Stresses due to FlowDownward Flow

    hw

    L

    flow

    X

    soil

    z

    v = whw + satz

    w hw + w(L-hL)(z/L)

    v ' = ' z + wiz

    At X,

    hLu = w hw

    u = w (hw+L-hL)

    as for static case

    = w hw + w(z-iz)

    = w (hw+z) - wiz

    Reduction due to flow

    Increase due to flow

    u =

  • 10 ft

    3 ft

    12 ft

    In Flow

    Out Flow

    2 ft

    4 ft

    Datum

    3 ft

    3 ft

    8 ft

    Piezometer

    A

    B

    C

    D

    u =

    6 x

    62.4

    -

    u

    u =

    17 x

    62.

    4

    Downward Seepage

    Buoyancy - Seepage Force

    Ws

    Ws

    Ws

    Ws

    Ws

    Seepage Force

  • 16

    Stresses due to Flow

    flow

    Upward Flow

    hw

    LX

    soil

    z

    v = whw + satz

    w hw + w(L+hL)(z/L)

    v ' = ' z - wiz

    At X,

    hL

    u = w hw

    u = w (hw+L+hL)

    as for static case

    = w hw + w(z+iz)

    = w (hw+z) + wiz

    Increase due to flow

    Reduction due to flow

    u =

  • 17 ft

    3 ft

    12 ft

    In Flow

    Out Flow 2 ft

    4 ft

    Datum

    3 ft

    3 ft

    8 ft

    Piezometer

    A

    B

    C

    D

    u =

    6 x

    62.4

    +

    u

    u

    u =

    17 x

    62.

    4

    Upward Seepage

    Buoyancy + Seepage Force

    Ws

    Ws

    Ws

    Ws

    Ws

  • 18

    Quick Condition in Granular SoilsDuring upward flow, at X:

    v ' = ' z - wizflow

    hw

    LX

    soil

    z

    hL

    = izw

    w '

    Critical hydraulic gradient (ic)

    If i > ic, the effective stresses is negative.

    i.e., no inter-granular contact & thus failure.

    - Quick condition

  • Flow nets

    To construct a flownet The Equipotensial lines intersect the flow line at right angle The flow elemens formed aproximate squares

    Flownet is a combination of flow lines and equipotensial lineA flow line is a line along which water particle will travel from upstream to downstream.An equipotensial line is line along which the potensial head at all points is equal

  • Seepage Terminology

    concrete dam

    impervious strata

    soil

    Stream/flow line is simply the path of a water molecule.

    datum

    hL

    TH = 0TH = hL

    From upstream to downstream, total head steadily decreases along the stream line.

  • Seepage TerminologyEquipotential line is simply a contour of constant total head.

    concrete dam

    impervious strata

    soil

    datum

    hL

    TH = 0TH = hL

    TH=0.8 hL

  • FlownetA network of selected stream lines and equipotentiallines.

    concrete dam

    impervious strata

    soil

    curvilinear square

    90

  • Equipotential Lines

    Flow Element

    Principles of the Flow Net

  • Piezometer

    )h = head loss = one drop

    Datum

    1

    2

    3

    4

    5

    Principles of the Flow Net

    Equipotential LinesTotal heads along this line are the same

    Flow Element

  • Seepage calculation from flow net 1 Square

    From Darcys law v=k i A

    and

    where H= head difference between upstream and down streamNd = number of potential drops

  • Seepage calculation from flow net cont

    2 Rectangular

    or

  • Seepage calculation from flow net cont

    Flow channels 1&2 have square elements

    Flow channel 3 has elemenrectangular b/l=0.38

  • Flow nets in anisotropic soil

    4.

    For anisotropic soil kx kz

    To construct the flow net use the following procedures:1. Adopt vertical scale (z axis) fro drawing the cross section2. Adopt horisontal scale (x axis) such that horisontal scale =

    kz/kx3. Plot the vertical section through the permeable layer

    parallel to the direction of flow 4. Draw the flow net for the permeable layer on the section

    obtained from step 3; with flow line intersecting equipotential line at right angles and the elements as approximate squares

    The rate of seepage can be calculated :

    where H =total head loss,Nf dan Nd = number of flow channels and potensial

    drops

  • Quantity of Seepage (Q)

    d

    fL N

    NkhQ = .per unit length normal to the plane

    # of flow channels

    # of equipotential drops

    impervious strata

    concrete dam

    hL

    head loss from upstream to downstream

  • Heads at a Point X

    impervious strata

    concrete dam

    datum

    X

    z

    hL

    TH = hL TH = 0

    Total head = hL - # of drops from upstream x h

    h

    Elevation head = -z

    Pressure head = Total head Elevation head d

    L

    Nh

    =

  • Uplift pressure under hydraulic structures

    Assuming kx = kz = k Nd =7 H=21ft Head loss for each potensial

    drop = H/Nd=3 Uplift pressure at a =

    (Pressure head at a) x w[(21+6)-3]x w =24 w

    Uplift pressure at b =[27-(2)(3)] w= 21 w

    Uplift pressure at f =[27-(6)(3)] w = 9 w

    Weir

    Uplift force under hydraulic structures

  • Seepage through an earth dam on impervious base

    Flow through a homogeniuos earth dam constructed over impervious baseConsidering cde

    Rate of seepage at the section bf

  • 33

    FiltersUsed for: facilitating drainage preventing fines from being washed away

    Used in:

    earth dams

    retaining walls

    Filter Materials:

    granular soils

    geotextiles

  • 34

    Granular Filter DesignTwo major criteria:

    (a) Retention Criteria

    (b) Permeability Criteria

    - to prevent washing out of fines

    - to facilitate drainage and thus avoid build-up of pore pressures

    Filter grains must not be too coarse

    Filter grains must not be too fine

    granular filter

  • 35

    Granular Filter DesignRetention criteria:D15, filter < 5 D85,soil

    - after Terzaghi & Peck (1967)

    Permeability criteria:D15, filter > 4 D15,soil

    average filter pore size

    D15, filter < 20 D15, soil

    D50, filter < 25 D50, soil- after US Navy (1971)

    GSD Curves for the soil and filter must be parallel

  • Example

    From the left figure Nf =3 Nd = 6

    Head loss for each drop = h/Nd = 10/6 = 1.667

    Potensial drop at a = 1x 1.667 ftWater in the piezometerAt a = 15-1.667=13.333 ft above ground surface

    (ags)At b = 15-2x1.667= 11.67 ft agsAt c = 15-5x1.667= 8.67 ft agsAt d = 15-5x1.667= 8.67 ft ags

    kx= kz =k = 5x 10-3 cm/sec= 1.64 x 10-4 ft/sec

    q = (1.64 x 10-4) x 1.667= 2.73x10-4

    ft3/sec/ft

    Impermeable layer

    Lecture 4Slide Number 2Laplace equationsLaplace equations of continuityLaplace equations of continuitySimple flow Simple flow Simple flow Simple flow Slide Number 10Slide Number 11Slide Number 12Slide Number 13Slide Number 14Slide Number 15Slide Number 16Slide Number 17Slide Number 18Flow netsSeepage TerminologySeepage TerminologyFlownetSlide Number 23Slide Number 24Seepage calculation from flow netSeepage calculation from flow net contSeepage calculation from flow net cont Flow nets in anisotropic soilQuantity of Seepage (Q)Heads at a Point XUplift pressure under hydraulic structuresSeepage through an earth dam on impervious baseSlide Number 33Granular Filter DesignSlide Number 35Example