2.4 Rock Permeability

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    2.4 Permeabili t y of reservoir rock

    2 The unit of permeability

    3 The conditions of measuring absolutepermeability

    4 Applicable condition of Darcy's law

    as ermea y an ec o as ppage

    on Permeabilityra ua on o orma on n permea y

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    2.4 Permeability of reservoir rock

    7 Factors af fect in the ma nitude of

    permeabil ity

    9 Flow Syst ems of Sim ple Geomet ry

    10 Average perm eabilit y of combinat ion

    layers11 The relat ionship of permeabilit y and

    ot her ro ert of rock

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    rock

    In 1856, Darcy investigated the flow ofwa er roug san ers .

    s exper men a appara us s s ownin Fig

    Darcy interpreted his observations soas to y e resu ts essent a y as g ven n

    equation.

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    hhK

    upstream pressure

    21

    L

    of rockexperimental apparatus

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    Definition of ermeabilit

    Permeability is the ability of fluids to

    pass roug a porous ma er a .

    3

    1 Darcy =

    ( ) ( )cmatmcm 112

    1 Darcy = 0.987 x 10-8 cm2

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    ere,

    cylindrical sand pack of cross-sectional area A

    P is pressures drop across the cylindrical

    sand pack .

    s v scos y o e u

    , ,

    characteristic of the sand pack.

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    2 The unit of permeability

    Darc CGS PERM SI

    L cm cm ft cm

    A cm2 cm2 ft2 cm2

    P atm dyn/cm2 psia MPa cp p cp mpa.s

    Q cm3/s cm3/s bbl/day cm3/s

    Kdarcy cm

    2

    perm m

    2

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    Physical significance of one Darcy

    One Darcy is defined as the permeability that

    to flowat a rate of 1 cm3/s through a cross

    sectional area of 1 cm2 when the pressure

    gradient is 1 atm/cm.

    1 Darcy (d)=1000 millidarcy (md)

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    permeability

    The orous medium must be 100 er centsaturated with the flowing fluid.

    No interaction between the fluid and theporous media

    Laminar flow .

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    EXAMPLE 4

    If the length of a core sample is 3cm ,and the

    cross-sec on area s cm . n er a pressure

    difference of 2atm, the core sample will bepermit a fluid of 1 cp (centipoise ) viscosity to

    flow at a rate of 0.5cm3/s throu h.

    Calculate permeability of core sample .

    :

    .0.375K D= = = ( )

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    ,be permit a fluid of 3 cp (centipoise ) viscosity

    to flow at a rate of 0.167cm3/s through,

    n er t e same pressure erence.

    0.167 3 3L

    .

    2 2

    K D

    A P

    = = =

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    Characteristic of absolute permeability:

    The permeability is a property of rockalone,dependent on the porous media size and

    s r u on o roa on y, no on e uused.

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    '

    1) Mid-high permeability

    3 23.5u=

    c

    K

    2) Low permeabilityFig.1 relations between velocity and

    pressure gradient

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    2). Klinkenberg Effect

    Klinkenberg Effect Effect of Gas Slippage

    expressed that the flow rate of gas at solid

    surface of pore is not zero.

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    is greater than liquid Permeability

    It has been found that gas permeabilitiessometimes vary with the pressure of gas,

    and that gas permeability is greater than

    .

    ca illar tubes.

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    3). Effect of gas slippage on Permeability

    Measurements

    800

    001um2

    1

    200

    400

    0.

    2

    3

    0

    0 2 4 6 8 10 co2

    p,

    the reciprocal of the mean pressure

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    or eac gas a s ra g ne s o a ne or eobserved permeability as a function of the reciprocal

    o e mean pressure o e es .

    - -gas yield the straight line with the greatest slope

    , .

    All the lines when extra olated to infinite meanpressure ( ) intercept the permeability axis

    at a common oint.

    1 0p

    =

    This point is designated kL or the equivalent liquidpermea ty.

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    The linear relationship between the observed

    permea y an e rec proca o mean pressuremay be expressed as follows:

    K = K 1+ b /

    =

    permeability,

    b=constant for a given gas in a given medium

    g=measure permea y us ng e arcy equa on

    for gas flow.

    = mean flowing pressure of the gasp

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    )b

    1(K KgKp

    K

    P

    1r

    b 22 d n=

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    permeability

    grade permeability evaluation

    2u m

    3 210 um

    > 1 >1000 Very good

    10.1 1000100 good

    . .

    0.010.001 101 fair

    - .

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    ac ors a ec ng e magn u e opermeability

    (a) Shape and size of sand grains(b) Grain packing and Cementation

    (c) Fracturing and solution

    ore ze an onnec v y

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    1) The experimental laboratory determinations

    A . determinations on small samples of

    Apparatus for measuring of permeability with liquid

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    0 02Q P u L2 2

    1 2

    ( )P P

    Apparatus for measuring of permeability with gas

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    310K =

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    a

    C b

    w iS

    =

    . . ,

    of the fluid and the porous medium

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    9 Flow S stems of Sim le Geometr

    Horizontal Flow.

    Horizontal rectilinear( steady-state flow is

    .

    1 2( )kA P P

    L

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    .

    A radial-flow system, analogous

    , .

    e wQ

    =

    e w

    e eis measured

    rw the radius at which Pwis measured.

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    10 Average permeability of combination

    1 . Consider the case where the flow s stem islayers

    comprised of layers of porous rock separated

    from each other b infinitel thin im ermeablebarriers as shown in Fig. Parallel combination

    n

    k h

    1j

    nk

    =

    =jh

    =

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    Radial flow

    Qt = Q1+ Q2 + Q3

    t = 1 2 3

    j jk hn

    k=

    =

    1

    j

    j =

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    2 Another ossible combination for flow

    systems is to have the beds of different

    shown in Fig. series combination

    Linear flowP1- P2 = P1+P2+P3

    Qt = Q1= Q2 = Q3

    n

    k =

    /j j

    L k

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    Radial flow

    - = + +Qt = Q1= Q2 = Q3

    ln

    e wQu R R

    =e w

    ln e

    wRRadial flow- series combination

    1ln i

    R

    1i i

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    11 The relationship of permeability and

    other property of rock

    Fig. parallel bundle of capillary tubes pack

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    Consider a system comprised of a bundle of

    cap ary u es o e same ra us an eng ;The e uation for flow of fluids in circular conduits:

    4

    0 1 2( )r P P

    8uLq e vo ume ra e o ow, cm s

    fluid viscosit mPa.s(P1-P2)pressure loss over length L,

    ro ra us o cap ary u e , cm,

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    2)The relationship of permeability and pore radius

    If the fluid-conducting channels in a porous medium

    tubes of same diameters, then the flow rate through

    4

    nA r P

    8uL=nnumber of capillary tubes per unit cross-

    rradius of capillary tube

    A total cross-sectional area

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    From Darcys law it is also known that :

    ' K A P

    u L

    =

    Equating Darcys and Poiseuilles equation:

    'Q Q=4 4

    KA P nA r P n r = = (1)8 8uL uL

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    ,

    2PV n A r L

    n r

    = = =(2)

    b

    r

    K r= =(3)

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    3)The relationship of permeability and specific

    sur acesurface area S is the total area exposed within

    the pore space per unit of bulk volume .

    22a n r

    S n r n r

    = = = = =

    b

    2 322 4

    S S

    = = = 28 KK

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    Let Sp be the internal surface area per unit of pore

    volume ,Ss be the total area exposed within thepore space per unit of grain volume

    a=

    PV

    (1 )P SS S S = =

    1 1S

    S = =

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    Gaocaini-Equation

    3 3

    3 2 2 22 2 2 (1 )P SK

    S S S = = =

    LLL

    2 2 2 2K = = =

    S P

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    EXAMPLE 1

    A core sample from a uniform sandstone formation-3 2

    of 0.17

    (b) Specific surface areas Sp and Ss.

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    .conditions that should be met when measuring

    .

    to measure permeability of reservoir rock? How

    .