6. Sedimentary Micro Structure

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    Rock Physics Properties and

    Sedimentary Microstructure-2Hilfan Khairy

    UTP

    Texture, and lithology: Rock physics basis

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    Rock physics and AVO-Universiti Teknologi PETRONAS

    Dr. Hilfan Khairy

    Theory and Model

    `

    The information of rock microstructure can be extracted from the relation ofvelocity-porosity.

    Avseth, 2003

    Rock physics properties change with the depositional environmentand burial depth

    Adjusting an effective-medium theoretical model

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    A. Clean sandstones

    1. Unconsolidated sand (friable model)

    Model developed for this following contacttheory model of Hertz-Mindlin. The criticalporosity is relatively high about 0.4 and

    very well sorted packing. The poorly sortedsand is accomplished by adding smallergrain deposited in the pore space. Thisadditional grain induced deterioratesorting thus decrease the porosity andslightly increase the velocity.

    Avseth, 2007

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    1/322 2

    22

    1

    18 1

    c

    HM

    nK P

    1/322 2

    22

    3 15 4

    5 2 2 1

    c

    HM

    nP

    3 2

    2 3K

    K

    0

    z

    b flP g dz

    220 34 14n

    Bulk modulus at critical porosity (c)

    Shear modulus at critical porosity (c)

    Poissons ratio

    Pressure at certain depth

    Coordination number

    Kand are solid bulk and shear modulus respectively

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    1

    / 1 / 4

    4 / 3 4 / 3 3

    c cdry HM

    HM HM HM

    K

    K K

    1

    / 1 /c cdry

    HM

    zz z

    9 8

    6 2

    HM HM HM

    HM HM

    Kz

    K

    Bulk and Shear modulusof friable sand

    How to establish thesaturation model??

    FLUID SUBSTITUTION BY USING GASSMANNS EQUATIONS

    min1b fl

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    2. Contact cement model

    During burial, the sand becomecemented sandstone. The effect of cement provides the rock become stifferand rigid, due to the grains are mergedtogether.

    1 / 6dry c c nK n M S

    3 3 1

    5 20

    dry c c

    dry

    K n S

    (Dvorkin and Nur., 1996)

    Saturation model? Gassmanns equations

    Morecement

    Avseth, 2007

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    3. Constant cement model

    Constant cement model assumes that theporosity reduction come from noncontactpore-filling material, such asdeteriorating sorting. This model is a

    combination of contact-cement andfriable sand model. At the beginning theporosity of sand-pack reduce to contact-cement porosity (b), and its continuesgoing down following the friable sandmodel. The friable sand model associates

    with the sorting trend while the contactcement due toburial.

    b

    c

    Avseth, 2007

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    1

    / 1 / 4

    4 / 3 4 / 3 3

    b b

    dry b

    b b b bK K K

    / 1 /b bdry

    b bz z

    9 8

    6 2

    b b b

    b b

    KzK

    1 / 6b c c nK n M S

    3 135 20

    c cbb

    n SK

    Kb and b following thecontact cement :

    The effect of fluid ?? Gassmanns equations

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    Avseth and Jrstad (2008)

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    B. Shales

    B1. Constant-clay model for sandy shales

    Silts are commonly suspended in the clay matrix and not cemented. Thus, it isfeasible to use Friable-sand model to calculate bulk modulus of constant clay.

    The critical porosity for model should be very high for shales about 60%-70%.

    Calculate Kmixed and mixed (quartz-clay)

    Input into Friable sand model to get Kdryand dry

    Performing Gassmanns fluid substitution for saturationmodeling scenario

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    1 1

    mixed qz clay

    C C

    K K K

    1 1

    mixed qz clay

    C C

    Elastic moduli of clay minerals

    1/322 2

    22

    1

    18 1

    c

    HMclay

    nK P

    1/322 2

    22

    3 15 4

    5 2 2 1

    c

    HMclay

    n

    P

    3 2

    2 3

    mixed mixed

    mixed mixed

    K

    K

    0

    z

    b flP g dz

    220 34 14n

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    1

    _

    / 1 / 4

    4 / 3 4 / 3 3

    c cdry ssh HM

    HM HM HM

    K

    K K

    1

    _

    / 1 /c cdry ssh

    HM

    zz z

    9 8

    6 2

    HM HM HM

    HM HM

    Kz

    K

    Bulk and Shear modulusSandy Shale

    How to establish thesaturation model??

    FLUID SUBSTITUTION BY USING GASSMANNS EQUATIONS

    min1b fl

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    B2. Dvorkin-Gutierrez silty shale model

    shC

    1

    1 4

    4 / 3 4 / 3 3

    sat sh

    sh sh q sh

    C CK

    K K

    1

    1sat sh

    sh sh sh sh

    C Cz

    z z

    9 8

    6 2

    sh sh shsh

    sh sh

    Kz

    K

    Porosity of shale as a function of clay content

    Ksh and sh are saturatedelastic moduli of shale andthey are derived from well-log measurement of Vp, Vsand density in a pure shalezone.

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    C. Shaly sandstones

    C1. Constant-clay model for shaly sand

    Since this model has the assumption of clay mineral dispersed in the grainand fill the pores between grains, thus it can be modeled the prediction ofelastic modulus by using Friable-sand model. The process has a similartechnique with the constant-clay model for sandy shale. However, the critical

    porosity should be adjusted in between 10% to 40%, depending on the claycontent. Mineral modulus of mixed between quartz grain and shale can beestimated by applying lower bound ofHashin-Shtrikman or average of

    Voigt-Reuss model. Special note should be addressed if the claycomposition is very soft such as smectite and illite (please refer to the elasticmoduli of clay minerals) and mixed with relatively stiff quartz.

    Because the quartz grain are cemented and stiffer than the shale (smectiteand illite), the mixed of those two mineral should be stiffest possiblealternative. Thus, it is recommended to useVoigt bounds.

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    Calculate Kmixed and mixed (quartz-clay)

    Input into Friable sand model to get Kdryand dry

    Performing Gassmanns fluid substitution for saturationmodeling scenario

    1

    mixed q clayK C K CK

    1

    mixed q clayC C

    1/322 2

    22

    1

    18 1

    c

    HMclay

    nK P

    1/322 2

    22

    3 15 4

    5 2 2 1

    c

    HMclay

    nP

    3 2

    2 3

    mixed mixed

    mixed mixed

    K

    K

    0

    z

    b flP g dz

    220 34 14n

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    1

    _

    / 1 / 4

    4 / 3 4 / 3 3

    c cdry ss HM

    HM HM HM

    K

    K K

    1

    _

    / 1 /c cdry ss

    HM

    zz z

    9 8

    6 2

    HM HM HM

    HM HM

    Kz

    K

    Bulk and Shear modulusSandy Shale

    How to establish thesaturation model??

    FLUID SUBSTITUTION BY USING GASSMANNS EQUATIONS

    min1b fl

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    C2. Yin-Marion shaly sand model

    The model is dedicated to predict the elastic modulus with the increasing ofclay content. By assuming the total porosity will decrease with the increasingof clay content (C) , and again it increases after threshold point, the totalporosity can be formulated as follows:

    1 for C

    s sh s

    s sh s

    sh s

    C

    Shaly sand

    Sandy shale

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    Marion et.al., 1992

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    dry pf sat

    q sat q dry s q pf

    K KK

    K K K K K K

    1 1

    pf clay fluidK K K

    sat dry

    1 1 1s q sh clay s sh flC C

    Kdry= dry sand frame bulk modulus

    dry= dry sand frame shear modulusKq = quartz bulk modulusKpf= bulk modulus pore filling material (fluid and clay)

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    Marion et.al., 1992

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    Avseth, 2007

    Clean sand line

    Shale line

    Unconsolidated sand

    Shaly sand

    Silty sand

    Clean sand line:constant-cement model

    Shale line:constant clay model

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    Chi and Han., 2009

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    Chi and Han., 2009

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    Avseth and Jrstad (2008)

    Quantifying cement from Vs-porosity graph

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    Avseth and Jrstad (2008)

    Quantifying sorting from Vs-porosity graph