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    Master of Petroleum Well EngineeringMaster of Petroleum Well Engineering dvanced Drilling Practices

    dvanced Drilling Practices

    AprilApril20052005

    Assoc. Prof. SampaioAssoc. Prof. [email protected]@peteng.curtin.edu.au

    FORMATION FRACTURE GRADIENT

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    Formation Fracture GradientFormation Fracture Gradient

    May be predicted from:May be predicted from:

    Pore pressure (vs. depth)Pore pressure (vs. depth)

    Effective stressEffective stress

    Overburden stressOverburden stress

    Formation strengthFormation strength

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    Rock MechanicsRock Mechanics

    HowHow a rock reacts to an imposeda rock reacts to an imposedstress, is important in determiningstress, is important in determining

    FormationFormation drillabilitydrillability

    Perforating gun performancePerforating gun performance

    Control of sand productionControl of sand production

    Effect of compaction on reservoir performanceEffect of compaction on reservoir performance

    Creating a fracture by applying a pressure to aCreating a fracture by applying a pressure to a

    wellborewellbore

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    Elastic Properties of RockElastic Properties of Rock

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    Elastic Properties of RockElastic Properties of Rockcontcontdd

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    Elastic Properties of RockElastic Properties of Rockcontcontdd

    The vertical stressThe vertical stressat any point can beat any point can be

    calculated by:calculated by:

    a

    F

    A

    =

    The axial and transverse strains are:The axial and transverse strains are:

    2 1 2 1

    1 1a tr

    L L d d

    L d

    = =

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    A

    B C

    D

    StressStressStrain DiagramStrain Diagram

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    HookeHookess andand PiossonPiossonss

    E =

    HookeHookess Law forLaw for UniaxialUniaxial Loading:Loading:

    PoissonPoissons Ratios Ratio

    a

    tr

    =

    EEis called Modulus of Elasticityis called Modulus of Elasticity

    or Youngor Youngs Moduluss Modulus

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    Typical Elastic Properties of RockTypical Elastic Properties of Rock

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    GeneralizedGeneralized HookeHookess LawLaw

    ( )

    ( )

    ( )

    1

    1

    1

    xyx x y z xy

    yz

    y x y z yz

    zx

    z x y z zx

    E G

    E G

    E G

    = =

    = + =

    = + =

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    Modulus 0f RigidityModulus 0f Rigidity

    G is called Modulus or Rigidity or Shear ModulusG is called Modulus or Rigidity or Shear ModulusIt can be shown thatIt can be shown that

    12E

    G = +

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    Volumetric StrainVolumetric Strain

    f i

    V

    i

    V V

    V =

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    Bulk ModulusBulk Modulus

    For small StrainsFor small Strains

    ForFor xx== yy== zz== (hydrostatic stress state)(hydrostatic stress state)

    V x y z = + +

    ( )

    ( )

    3 1 2

    3 1 2

    V

    V

    V

    E

    E

    k

    =

    =

    =

    kkis calledis called

    Bulk ModulusBulk Modulus

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    Bulk ModulusBulk Moduluscontcontdd

    CompressibilityCompressibility

    Incompressible material:Incompressible material: c = 0c = 0

    1c k=

    ( )3 1 21 0 0.5ck E

    = = = =

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    General Elastic Relations:General Elastic Relations:

    ( )

    ( )

    ( )

    12

    3 1 2

    3 1 2

    2 1

    EG

    Ek

    G

    k

    = +

    =

    =

    +

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    InIn--situ stressessitu stresses

    Vertical Equilibrium in a rock element:Vertical Equilibrium in a rock element:

    ob p zp = +

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    InIn--situ stressessitu stressescontcontdd

    With increasing depthWith increasing depth pore pressure increases approximately 0.445pore pressure increases approximately 0.445

    psipsi/ft/ft

    overburden stress increases betweenoverburden stress increases between0.850.85 psipsi/ft to 1.1/ft to 1.1 psipsi/ft/ft

    ThenThen

    matrix stress increases betweenmatrix stress increases between0.4050.405 psipsi/ft to 0.665/ft to 0.665 psipsi/ft/ft

    ob p zp = +

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    InIn--situ stressessitu stressescontcontdd

    Te increase in matrix stress is theTe increase in matrix stress is theprimary responsible for the decreaseprimary responsible for the decrease

    in the porosity with depth.in the porosity with depth.

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    InIn--situ stressessitu stressescontcontdd

    Sedimentary rockSedimentary rock is the result ofis the result ofmillions of years of continuingmillions of years of continuing

    deposition of sediments that deepensdeposition of sediments that deepens

    and compact.and compact.

    As depth increases, grain to grainAs depth increases, grain to grain

    stresses increase.stresses increase.

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    InIn--situ stressessitu stressescontcontdd

    Due to theDue to the zz, a tendency exists to the, a tendency exists to theformation to expand laterallyformation to expand laterally(Poisson(Poissons ratio).s ratio).

    Lateral expansion is prevented fromLateral expansion is prevented from

    occurring by the surrounding rock,occurring by the surrounding rock,

    This generates horizontal matrixThis generates horizontal matrixstresses (stresses (xx andand yy).).

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    InIn--situ stressessitu stressescontcontdd

    Simplifying Assumptions:Simplifying Assumptions:1. The rock behaves as an elastic material,

    2. The horizontal stresses are equal

    (x = y = H),

    3. No horizontal strain (x = y = 0), and

    4. Rock properties are constant withdepth.

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    InIn--situ stressessitu stressescontcontdd

    Using GeneralizedUsing Generalized HookeHookess LawLaw

    ( ) ( )

    ( ) ( )

    1 10

    1 10

    x x y z H H z

    y x y z H H z

    E E

    E E

    = =

    = + = +

    1H z

    =

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    Pressure Required to

    Fracture a Formation

    To hydraulically fracture a formation,To hydraulically fracture a formation,the pressure of fluid in a cavity of thethe pressure of fluid in a cavity of the

    formationformation

    Must overcome the cohesive strength ofMust overcome the cohesive strength of

    the grains PLUSthe grains PLUS

    The matrix stress (and any stressThe matrix stress (and any stressconcentration) at the cavity wall PLUSconcentration) at the cavity wall PLUS

    The fluid pressure in the pores of theThe fluid pressure in the pores of the

    rock.rock.

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    Pressure Required to Fracture

    a Formation contd

    For formation deep enough, theFor formation deep enough, thecohesive stresses are much less thancohesive stresses are much less than

    the matrix stresses and are, thereforethe matrix stresses and are, therefore

    neglected.neglected.

    The same is not true for shallowThe same is not true for shallow

    formations.formations.Too shallow (or young) formations areToo shallow (or young) formations are

    normally unconsolidated.normally unconsolidated.

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    Pressure Required to Fracture

    a Formation contd

    A typical circularA typical circular

    hole in an infinitehole in an infiniteplate subjectedplate subjectedto anto an uniaxialuniaxialstress causes astress causes astressstress

    concentration ofconcentration ofmagnitudemagnitude 33 ononthe wall of thethe wall of the

    hole.hole.

    3

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    Pressure Required to Fracture

    a Formation contd

    This means thatThis means that

    to initiate ato initiate afracture, thefracture, thematrix stressmatrix stressthat must bethat must beovercame is 3overcame is 3

    times larger thantimes larger thanthe originalthe originalundisturbedundisturbed

    matrix stress.matrix stress.

    3

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    Pressure Required to Fracture

    a Formation contd

    However at aHowever at a

    short distanceshort distance

    from the wall offrom the wall of

    the hole, thethe hole, thematrix stressmatrix stress

    reduces rapidlyreduces rapidly

    to theto the

    undisturbedundisturbed

    matrix stressmatrix stress

    3

    Pl f F tPl f F t

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    Plane of FracturePlane of Fracture

    The plane of fracture is perpendicularThe plane of fracture is perpendicularto the direction of the least principalto the direction of the least principal

    matrix stress.matrix stress.

    In a geologically relaxed regionIn a geologically relaxed region

    fractures tend to be horizontal.fractures tend to be horizontal.

    In regions subjected to tectonicIn regions subjected to tectonicforces, things may be much moreforces, things may be much more

    complicated.complicated.

    Pl f F tPl f F t ttdd

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    Plane of FracturePlane of Fracturecontcontdd

    Rock propertiesRock properties

    assumedassumed

    constant withconstant withdepthdepth

    Pl f F tPl f F t ttdd

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    Plane of FracturePlane of Fracturecontcontdd

    obob

    is the max.is the max.

    principalprincipal

    stressstress

    Failure occursFailure occursperpendicular toperpendicular to

    the leastthe least

    principal stressprincipal stress

    Pl f F tPlane of Fracture tcontdd

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    Plane of FracturePlane of Fracturecontcontdd

    HH >>

    obob can becan be

    created bycreated byTectonic forcesTectonic forces

    PostPost--depositionaldepositionalerosionerosion

    Glacial action orGlacial action or

    melting of glaciermelting of glacier

    Plane of FracturePlane of Fracture contcontdd

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    Plane of FracturePlane of Fracturecontcontdd

    Effect ofEffect of

    tectonictectonic

    stresses onstresses onfracture planefracture plane

    directiondirection

    Plane of FracturePlane of Fracture contcontdd

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    Plane of FracturePlane of Fracturecontcontdd

    Effect ofEffect of

    topographtopography ony on obob

    Formation Fracture PressureFormation Fracture Pressure

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    Formation Fracture PressureFormation Fracture Pressure

    Fracture Pressure:Fracture Pressure:

    Least Matrix Stress:Least Matrix Stress:

    Horizontal MatrixHorizontal Matrix

    StrtessStrtess::

    minff pp p = +

    1H z

    =

    min H =

    Formation Fracture PressureFormation Fracture Pressure

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    CombiningCombining

    Matrix Stress:Matrix Stress:

    contcontdd

    1ff p zp p

    = +

    z ob pp =

    Formation Fracture PressureFormation Fracture Pressure

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    contcontdd

    Combining againCombining again

    oror

    1 2

    1 1ff ob pp p

    = +

    1 21

    ff ob zp

    = +

    FromationFromation Fracture GradientFracture Gradient

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    FromationFromation Fracture GradientFracture Gradient

    Gradient at a given depthGradient at a given depth DD

    (psi/ft)

    19.25 (lb/gal)

    ff

    ff

    ffff

    p

    p D

    pp

    D

    =

    =

    Rock PoissonRock Poissons Ratios Ratio

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    Rock PoissonRock Poisson s Ratios Ratio

    This is a key parameter.This is a key parameter.PoissonPoissons Ratio is depth dependents Ratio is depth dependent

    A great deal of data from hydraulicA great deal of data from hydraulicfracturing treatments and leakfracturing treatments and leak--of testof test

    in nearby areas are needed to obtainin nearby areas are needed to obtain

    accurate values ofaccurate values of

    Rock PoissonRock Poissonss

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    RatioRatio

    contcont

    dd

    ExampleExample

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    ExampleExample

    Calculate the formation fracturegradient at 10,000 ft depth for the datain Example 7 in Pore Pressure.

    Use pore pressure calculated usingboth (a) Equivalent Matrix Stressmodel and (b) Empirical Correlationmodel

    Assume Poissons ratio for

    overburden gradient equal to 1.0 psi/ftin shales.

    SolutionSolution

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    SolutionSolution

    a) Equivalent Matrix StressFrom Example 6 results

    (pp)10,000 = 7,669 psi

    (ob)10,000 = 10,378 psi

    From graph: = 0.423

    SolutionSolution contcontdd

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    SolutionSolution contcontdd

    1 2

    1 1

    ff ob pp p

    = +

    0.423 1 2 0.423

    10,378 7,669 9,655 psi1 0.423 1 0.423

    9,655 psi

    10,000 ft

    ff

    ff

    ff

    p

    pp

    D

    = + =

    = =

    0.966 psi/ft 18.6 lb/galffp = =

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    b) Equivalent Matrix StressFrom Example 6 results

    (pp)10,000 = 8,100 psi

    (ob

    )10,000

    = 10,378 psi

    = 0.423

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    LeakLeak--Off TestOff Test

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    LeakLeak Off TestOff Test

    PurposePurpose1. Test the casing couplings sealing,

    2. Test the sealing of the annular between

    the casing and the cement, and betweencement and cased formations,

    3. Test the resistance of the formations

    below the last casing shoe (normally theformation right below the casing shoeand also the first sand below the casing

    shoe).

    LeakLeak--Off TestOff Test contcontdd

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    LeakLeak Off TestOff Test contcontdd

    Remarks:Remarks:

    a) casing tests are performed before the cement isdrilled from the bottom joint.

    b) the annular sealing and leak-off test areperformed simultaneously, after the formation is

    drilled about 10 ft below casing shoe. A largedeparture from the expected pressure increaseline indicates a fail in the cement bonding.Cement must be squeezed in order to promote

    sealing.c) fracturing the formation will not decrease the

    resistance of the formation, since the stress dueto the surrounding rocks and pore pressure are

    the responsible for the formation fractureresistance.

    Calculation of the Leak off Pressure

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    pf=frictional pressure loss (small)Gel strength may be large. track pressures in both annular and

    drillstring gages noting the maximum

    difference as the gel strength

    LO ff fp p g D p= +

    Calculation of the Leak off Pressure contd

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    Circulate the fluid before the test to Homogenize the fluid,

    Break the gel, and

    Remove solids in suspension and

    contaminants.

    Pump Rates for shales in the range of0.25bbl/min to 0.5 bbl/min. For Porous

    sandstones, 1.5 bbl/min.

    Calculation of the

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    Leak off Pressure

    contd

    Graph the surface

    pressure vs.

    injected volume.

    Include theanticipated leak-off

    pressure and

    anticipated slope ofthe pressure line.

    Slope of Pressure LineSlope of Pressure Line

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    pp

    Equivalent compressibility of the fluid ce

    ce= cwfw+ cofo+ csfs

    0.2x10-6Solids

    5.0x10-6Oil

    3.0x10-6Water

    Compressibility

    (psi-1)

    Component

    Slope of Pressure LineSlope of Pressure Linecontcontdd

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    pp

    By definitionBy definition

    1e

    dVc V dp=

    Slope of Pressure LineSlope of Pressure Linecontcontdd

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    pp

    The injection if a volumeThe injection if a volume VVii into ainto a

    constant well volumeconstant well volume VV00 correspondscorrespondstoto reduvereduve the volume fromthe volume from VV00+V+Vii toto VV00,,

    that is a change of volume equal tothat is a change of volume equal toVVii

    Therefore the anticipated slope isTherefore the anticipated slope is

    0

    1

    i e

    dp

    dV c V

    =

    LeakLeak--Off TestOff Testcontcontdd

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    After the end of the test, measure thevolume of mud that is bled from the

    well. The volume should be very close

    to the injected volume (the differenceis the amount of filtrate lost in the test).

    If fracture occurred, or leak due to badcementing job, this difference will be

    larger.

    LeakLeak--Off TestOff Testcontcontdd

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    Poor cementbonding in theannular betweencasing and borehole

    This behavior is anindication that fluid isseeping between the

    casing and cementlayer of between thecement layer and the

    formation, or both.