groundwater hydraulics water flow in porous media...

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Groundwater hydraulics Water flow in porous media, hydraulic conductivity, Darcy’s law

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  • Groundwater hydraulics

    Water flow

    in porous media,

    hydraulic conductivity,

    Darcy’s law

  • Saturated flow

    Darcy, H., 1856. Les Fountaines de la Ville de Dijon

    Henri Darcy (1856) filtration of water for fountains in

    Dijon

    After many experiments he found that water flow

    through the soil column depends on:

    • directly proportional to pressure drop

    • inversely proportional to the length

    • directly proportional to the crossectional area

    • dependent on coefficient which is specific for

    each media

    Henry Darcy

  • Darcy’s lawHenri Darcy 1856

  • Darcy law

    Q = flow [L3.T-1]

    A = crossectional area [L2]

    Ks = saturated hydraulic conductivity [L.T-1]

    rH = H1 – H2 (hydraulic head drop) [L]

    L= sample lenght [L]

    valid in fully

    saturated porous

    media

    For example: under

    the ground water

    level

    L

    ΑΔΗΚQ S

    LH2

    H1

    datum

    z1

    z2

    h1

    h2

    Hi = hi+zi

  • Sn

    Q

    S

    Q v

    n

    p

    Darcian velocity Porous velocity

    S

    Q v

    n

    v vp Where n is porosity

  • z

    HKv

    y

    HKv

    x

    HKv

    HgradK K

    z

    y

    x

    neboJv

    for:

    Transforms to the:

    More gereneral form:

    Pro 1D vertical flow

    kde:

    q ... Volume flux [L.T-1]

    Q ... Flow rate [L3.T-1]

    A ... Crossectional area [L2]

    L

    HKq s

    A

    Qq

    dl

    dHKq s

    HKdl

    dHKq Ss

    note: negative sign

    due to the fact grad H

    aims against flow

    direction

    For 3D flow

  • Coefficient or the saturated hydraulic

    conductivity KsAlso called (sometimes) filtration coefficient, darcy’s coefficient or

    permeability (incorrect)

    commonly used units Ks (m.s-1), (cm.d-1), (cm.s-1)

    Ks is property of water-solid interaction. Parameter which is related only to

    the porous media (independently on flowing liquid)

    is:

    k = Ksn/g [ L2]

    where n kinematic viscosity when m is dynamic viscosity

    Permeability k

    m

    gk K

  • Ks for different media

    k (

    cm

    2)

    Ks

    (cm

    .s-1

    )

    Ks

    (m.s

    -1)

    source: Císlerová a Vogel, 1998

    cla

    y

    sil

    t sa

    nd

    y l

    oa

    m sa

    nd

    gra

    ve

    l

  • Permeability

    Permeability reflects porous medium only - k [m2].

    Is used for transport of solutes in porous space

    Permeability can be estimated from number of formulas by combination of porosity,

    grain distribution and shapes of particles

    2dk = cEmpirical formulas: where d is diameter of effective grain (d10),

    c=45 for clayey sand, c=140 clear sand.

    m

    m

    m d

    P

    α

    n

    ) - n(

    βk

    100

    112

    3

    21

    Where β=5, α is grain shape parameter, α=6 for spherical grains,

    α=7.7 for sharp grains, Pm is procents of grains found on the

    sieve with dm diameter

  • Physically based equation Carmana - Kozeny:

    22

    3

    S

    0 M) n- 1 (

    n Ck Where C0 is empiric constant, MS is specific surfaceof unit volume of porous space

    Formula of Carman – Kozeny for hydraulic conductivity

    72

    d e gn K e

    n

    222/3

    Where n is porosity, e is number of porosity, de is effective grain

    g is gravity acceleration, ν is kinematic viscosity of water

  • Example 1 :

    Vertical column: q=?

    b=

    10cm

    q

    const. head

    seepage face

    1) datum definition

    H = 0

    H2

    = H1 = z1

    2

    1

    2) points 1 and 2 with known hydraulic

    heads

    = z2

    +z

    3) Darcy’s law

    1

    12

    .110100

    )0110(100

    dcm

    L

    HHK

    L

    HKq ss

    WATER

    SOIL

    Ks=100cm/dL=

    100cm

  • dH=10 cm

    Water

    head inflow

    Free

    outflow

    100 cm

    Ks

    H1

    H2

    Example 2

    horizontal column: q = ?

    1) Step 1, definition of datum and coordination system

    2) Definition of points 1 and 2). Then x1 = 0 and h1 = 10 cm,

    x2=100cm, h2 = 0, z1 = z2 = 0, L = x2 - x1 = 100 cm

    3) Hydraulics heads are then H1 = h1 + z1 = 10 cm, H2 = h2 + z2 =

    0 cm

    5) Darcy’s law

    112 .10100

    )100(100

    dcm

    L

    HHK

    L

    HKq ss

  • 1) Measurements of Ks using constant head permeameter

    VODA

    PŮDA

    b

    L

    q

    Const. head

    Seepage face

    Soil column

    H1 = 0 + 0 (lower end)

    H2 = b + L (upper end)

    H = (b+L) - 0

    then:

    Ks measurements

    LbqL

    H

    qLKs

    LbAtVL

    HAt

    VLKs

    In practice we measure Q, resp. V/t, then:

    WATER

    SOIL

    Q

    A

    Ks= ?

  • sample

    po

    rou

    s d

    iscs

    Q

    measurement

    overflow

    inflowconstant head

    b

    L

    Fig. : http://www.utdallas.edu/~brikowi/Teaching/Geohydrology/LectureNotes/Darcy_Law/Permeameters.html

    Constant head permeameter

    soil sample must be carefully saturated with water to

    measure “real” Ks.

  • Constant head permeameter

  • 2) Measurement of Ks falling-head permeameter

    Ks= ?

    b(t)

    L

    q

    Falling head

    Seepage face

    Experiment is done on soil sample in the

    laboratory. Initial water level is equal to b0

    H1 = 0, H2(t) = L+b(t), H(t) = [b(t) + L] - 0

    becomes:

    b0

    L

    LbK

    dt

    dbq s

    dtL

    K

    Lb

    db s

    Lb

    LbLb

    Lb

    db bb

    b

    b

    01lnln

    1

    0

    1

    0

    Integration of the left side

    b1WATER

    SOIL

  • 11

    0

    1

    0

    t

    ss

    t

    s

    L

    tKdt

    L

    Kdt

    L

    K

    Right side integration

    dtL

    K

    Lb

    db s

    L

    tK

    Lb

    Lb s 1

    0

    1ln

    then:

    Lb

    Lb

    t

    LKs

    1

    0

    1

    ln

  • Zdroj: http://www.utdallas.edu/~brikowi/Teaching/Geohydrology/LectureNotes/Darcy_Law/Permeameters.html

    Falling-head permeameter

    sample

    Po

    rou

    s

    dis

    cs

    Q

    wa

    ter

    leve

    l d

    rop

    b0

    L

    b1

    Lb

    Lb

    t

    L

    A

    AK bs

    1

    0

    1

    ln

    Consider different

    crossectional areas of

    burette and column:

    db

    d

    where:

    t1…. time

    Ab … cross. area of burette

    A ... cross. area of the sample

  • VODA

    PŮDA

    b

    L

    h0

    h2 = b, z2=L

    h1 = 0, z1 = 0

    Ks is constant, h(z) = ?

    Darcy’s law:

    z

    zhK

    L

    LbK

    L

    HKq sss

    zh

    zL

    bz

    L

    hhh

    12

    In this case, pressure head

    profile is linear .

    Example 3 :

    Pressure head along the soil column h(z)=?

    q

    q12 q1z

    WATER

    SOIL

  • Homogeneity and inhomogeneity of the environment

    with regards to hydraulic conductivity

    The environment is homogeneous: hydraulic conductivity is same at all points

    of the environment

    The environment is inhomogeneous = heterogeneous: environment where

    hydraulic conductivity varies according to position in the area

    Heterogeneity with gradual change Heterogeneity with sudden change

    distance

  • Example of inhomogeneous environment, accepted as homogeneous

    Practical situations lead us to considerations whether accept or neglect inhomogeneity

    Calculating flow velocity

    z

    HKv

    y

    HKv

    x

    HKv

    HgradK K

    z

    y

    x

    neboJv

    Where K is the function of x,y and z.

    clay lens

    recursive pattern

    or

  • Isotropy and anisotropy of the environment

    The environment is isotropic when hydraulic conductivity is same at all directions

    The environment is anisotropic when hydraulic conductivity is direction dependent, e.g.

    Hydraulic conductivity in vertical direction is lower than in horizontal direction

    This property is due to the formation of the structure (e.g. sediments)

    Hydraulic conductivity of anisotropic environment is defined by tensor of hydraulic conductivity

    3D

    2D

    yyyx

    xyxx

    zzzyzx

    yzyyyx

    xzxyxx

    KK

    KK

    KKK

    KKK

    KKK

    KK

    Component Kxy defines part of the velocity in x direction caused

    by unit hydraulic gradient in y direction

    Vector of velocity is tilted from the direction of the hydraulic

    gradient in anisotropic environment

  • Sedimentary rock – horizontal structure

    https://commons.wikimedia.org/w/index.php?curid=8912695

    https://commons.wikimedia.org/w/index.php?curid=8912695

  • Eolic sediment – vertical structure

    https://commons.wikimedia.org/w/index.php?curid=7736690

    https://commons.wikimedia.org/w/index.php?curid=7736690

  • Main axes of anisotropy are the direction where hydraulic conductivity

    reaches maximal or minimal value

    If coordinate system x,y,z is parallel to main axes of anisotropy,

    tensor of hydraulic conductivity is

    yy

    xx

    zz

    yy

    xx

    K

    K

    K

    K

    K

    0

    0

    00

    00

    00

    KK

    3D2D

    Components of flow in anisotropic environemnt are following

    z

    H K

    y

    H K

    x

    H K v

    z

    H K

    y

    H K

    x

    H K v

    z

    H K

    y

    H K

    x

    H K v

    zzyzxzz

    yzyyyxy

    xzxyxxx

    z

    H Kv

    y

    H Kv

    x

    H Kv

    zz

    yy

    xx

    neboor

  • Combination of homogeneity (1) and isotropy (2) in the in environment

    homogeneous, isotropic homogeneous, anisotropic

    inhomogeneous, anisotropicinhomogeneous, isotropic

  • Limits of Darcy’s law validityF

    LO

    W V

    EL

    OC

    IT

    HYDRAULIC GRADIENT

    Darcy’s law is valid in certain interval of hydraulic gradient and flow velocities only

    Laminar flow

    Turbulent flow

    Prelinear zone Linear zone Postlinear zone

  • Prelinear flow

    Happens in very fine materials (clay and silt), flow velocity is

    calculated by Swartzendruber:

    . 3

    Jln

    J

    1 ,J)exp( J

    3

    4 J K v 0

    0

    0

    kde

    J0 is limit value of hydraulic gradient, where flow is actuvated.

    J0 < 0.5 for silt, J0= 0.5 - 1.0 for clay.

    Postlinear flow

    Happens in coarse materials (gravel or sandy gravel), where higher velocities occur

    Type of flow: laminar vs. turbulent is indicated by Reynolds number:

    ν

    d Re

    v

    Critical value of Re is dependent on given material. Typically 10 - 100 (1 - 10).

    D is grain size and n is kinematic viscosity

    where

  • For postlienar zone, flow can be calculated by combined method

    2 m 1.6 , B A grad B A gradm

    vvnebovv2

    A, B are constants, characterizing permeability of the environment, d or de is effective grain:

    ,11 2tKBKA

    engdedgn

    K 933.4log4Ka72

    10

    45

    t

    223

    n

    Pavlovskij equation

    ) (grad K 5.0

    v

    e

    ed

    14 d 20 n K

    In most of the cases groundwater flow meets linear zone where Darcy’s law

    is applicable. Upper limit of Darcy’s law might be overcome in carstic, dolomitic or

    volcanic areas with cavities.

    or

  • Transmissivity

    Transmissivity – is ability of aquifer to transfer water in one horizontal

    meter of aquifer of thickness B and hydraulic conductivity K

    T = KB

    Transmissivity units [m2/s]

    Transmissivity can be applied if vertical flow component is not considered

    x

    H W B K Q

    x

    y

    H W B K Q

    y