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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.