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    The description of reservoir and its contained is theMost important phase of Reservoir Engineering job .

    More precisely reservoir description , known asformation evaluation involves:

    Gathering of appropriate and accurate data on thephysical characteristics of the Formation rocks and onthe characteristics of fluid within these rocks.

    Interpretation of these data for accuracy and reliability

    Evaluation of potential sources of reservoir producingenergy such as an Aquifer or Gas cap.

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    A Data gathering program for a newlydiscovered field should be designed to

    answer two fundamental questions :

    Oil or Gas present in the Formation is in economicquantities or not .

    How can the reservoir be developed and producedfor maximum economic return?

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    Kinds of data :

    Original reservoir pressure and temperature

    Gross reservoir thickness at the well and the thickness of other

    productive zones penetrated

    The lithology of the reservoir rock

    The stratigraphic sequence of the rock encountered in the well

    Reservoir porosity and initial fluid saturations

    The natural productivity index of the well

    Characteristic of the reservoir fluid

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    sources of data :

    Cores

    Logs including Fullset logs and MDT,XPT,PLT &FMI

    Fluid samples

    DST & Production tests

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    Other data that should be obtained from wells drilled afterdiscovery:

    Areal variation in reservoir permeability , porosity and water saturation

    Continuity of reservoir zones between wells

    Vertical permeability variations within the reservoir

    The subsea depth of the top and base of the reservoir for structure maps

    Structural position of the reservoir Gas-Oil and Water-Oil contacts

    Variation in reservoir fluid composition within the reservoir

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    CLASIFICATION OF RESERVOIR ANDRESERVOIR FLUID

    Petroleum reservoirs are classified as oiland gas reservoirs.

    This clasification is subdivided dependingon :

    The composition of the reservoir Hydrocarbon mixture

    Initial reservoir pressure and temperature

    Pressure and temperature of the surface production

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    PRESSURE TEMPERATURE DIAGRAM

    Although differentHydrocarbon systemwould have a different

    phase diagram ,thegeneral configurationis similar.

    These diagrams areessentially used to:1. Classify the reservoir

    2. Describe the phase behaviorof reservoir fluid

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    OIL RESERVOIR

    Depending upon initial

    reservoir pressure oilreservoirs can besubclassified into thefollowing categories :

    Undersaturated oil reservoir

    Saturated oil reservoir

    Gas cap reservoir

    1

    2

    3

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    OIL RESERVOIR

    Crude oils arecommonly classified

    into the followingtypes:

    Ordinary black oil

    Volatile oil

    Near critical crude oil

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    GAS RESERVOIR

    On the basis of phase diagram andreservoir condition Natural gases are

    classified into four categories:

    Retrograde gas condensate

    Near critical gas condensate Wet gas

    Dry gas

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    GAS RESERVOIR

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    COMPOSITION OF VARIOUS RESERVOIR FLUIDTYPE

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    RESERVOIR FLUID PROPERTIES

    To understand and predict of volumetric behavior of oil and gasreservoirs as a function of pressure, knowledge of physicalproperties of reservoir fluid must be gained.

    These fluid properties are usually determined by laboratoryexperiments on reservoir fluid.

    In the absence of experimentally measured properties , it isnecessary for the petroleum engineers to determine properties

    from empirically correlations.

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    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    SAMPLING :

    Samples of reservoir fluid arecollected and dispatch to a

    laboratory for the full PVTanalysis.

    There are basically two wayof collecting PVT samples.

    1. Direct subsurface sampling

    2. Recombination of surfacesamples

    quality of the samplesshould be checked

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    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    Accurate laboratorystudies of PVTexperiments are

    necessary forcharacterizing thereservoir fluids andevaluating their

    volumetric performanceat various pressurelevels.

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    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    PVT sampling

    Three main type oflaboratoryexperiments are asfollows:

    Primary tests

    Routin laboratory tests

    Special laboratoryPVT tests

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    Primary tests

    including routin onsite field

    tests involving themeasurement of specific gravity& GOR of the producedhydrocarbon fluids.

    LABORATORY ANALYSIS FOR RESERVOIR FLUID

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    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    Routin laboratory testsAfter checking the samples There are several laboratory tests that

    are routinely conducted to characterize the reservoirhydrocarbon fluid which is included:

    Compositional analysis of the system

    Constant composition expansion

    Differential liberation

    Separator tests

    Constant volume depletion

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    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    Compositionalanalysis of thesystem

    Most of the parametersmeasured in a reservoirfluid study can becalculated with somedegree of accuracyfrom the composition.

    It is the most completedescription of thereservoir fluid that can bemade

    Stock Tank Oil Solution Gas Reservoir Oil

    (mol%) (mol%) (mol%)

    H2S 0.00 9.69 5.78

    N2 0.00 0.02 0.01

    CO2 0.00 4.07 2.43

    C1 0.00 59.21 35.35

    C2 0.16 10.74 6.48

    C3 0.99 6.98 4.56

    iC4 0.58 1.67 1.23

    nC4 1.87 3.51 2.85

    iC5 1.31 1.25 1.27

    nC5 1.37 1.27 1.31

    C6 9.84 1.17 4.66

    C7 8.82 0.35 3.76

    C8 8.35 0.08 3.41

    C9 8.69 0.01 3.51

    C10 8.01 0.00 3.23

    C11 6.05 0.00 2.44C12+ 43.96 0.00 17.71

    241

    414

    89

    0.8962Sp.Gr. of C12+ Fraction @ 60/60 oF

    * Recombined oil separated at atmospheric condition( 0 psig and T=70OF)

    Reservoir F lu id Compositi on

    Components

    100.00GOR* : 669.33 SCF/STB

    Molecular weight of residual oil

    Molecular weight of C12+ fraction

    Molecular weight of Reservoir oil

    -Relative Density - 0.6865

    FLUID - - -

    Reservoir Flu id(g/cm

    3)

    3-DensitySep a ra t or L iq u i d Sep a ra t or Ga s

    FLUID 82.94 19.90 25.33

    C12+ - - -

    C7+ - - -

    0.55

    Total 100.00 100.00 100.00

    C12+ 6.43 0.00

    Pseudo C11 2.73 0.00 0.23

    Pseudo C10 4.41 0.00 0.38

    Pseudo C9 7.12 0.02 0.63

    Pseudo C8 9.84 0.06 0.90

    Pseudo C7 9.77 0.09 0.92

    10.82 83.68 77.38

    C2H6 4.62 4.19 4.23

    CH4

    4.87

    H2S 8.49 4.24 4.61

    2.18CO2 5.12

    RESERVOIR FLUID ANALYSIS

    1-COMPOSITION (mol % )

    C om p on en t S ep ar at or L iq ui d S ep ar at or G as R es er vo ir f lu id

    N2 0.11 0.10 0.10

    C3H8 6.24 1.49 1.91

    iC4H10 2.68 0.25 0.46

    nC4H10 7.03 0.42 1.00

    iC5H12 5.10 0.11 0.54

    Pseudo C6 8.43 0.13 0.84

    nC5H12 4.00 0.11 0.45

    2-Molar Mass S ep ar at o r L i qu id S ep ar at o r G as R es er v oi r F lu i d g /mo l

    C12+ - - -

    C7+ - - -

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    Constant compositionexpansion

    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    Press. Total F.V.F Compressibility

    psia Bt E-6

    8535 0.8625 2.0857 29.34

    8036 0.8752 2.1163 29.63

    7537 0.8881 2.1476 29.95

    7038 0.9014 2.1797 30.29

    6543 0.9149 2.2123 30.66

    6046 0.9288 2.2460 31.06

    5548 0.9432 2.2808 31.50

    5049 0.9580 2.3166 32.00

    4550 0.9733 2.3536 32.55

    4150 0.9860 2.3843 33.05

    4050 0.9893 2.3921 33.18

    3950 0.9925 2.4001 33.32

    3849 0.9959 2.4082 33.46

    3749 0.9992 2.4162

    3724 1 .000 0 2.4181

    3608 1.0156 2.4558

    3592 1.0178 2.4611

    3576 1.0200 2.4664

    3561 1.0219 2.4712

    3547 1.0238 2.4756

    3532 1.0258 2.4806

    3508 1.0291 2.4885

    3472 1.0338 2.4998

    3424 1.0404 2.5158

    3353 1.0509 2.5412

    3254 1.0668 2.5795

    3120 1.0905 2.6369

    2940 1.1262 2.7233 2.1134 2.1148 1.1261

    2719 1.1798 2.8528 2.0567 2.0546 1.1591

    2454 1.2609 3.0490 1.9841 1.9824 1.2339

    2155 1.3836 3.3456 1.8985 1.9009 1.3469

    1835 1.5680 3.7915 1.8127 1.8138 1.5186

    1515 1.8453 4.4621 1.7252 1.7266 1.7768

    1212 2.2594 5.4634 1.6459 1.6440 2.1643

    1142 2.3915 5.7828 1.6251 1.6250 2.2750

    Constant M ass Expansion @ 287 F

    ** Y = 2.7240E-04 P + 1.3139

    Smoothed VtSmoothed Y**Vt Y Function

    *

    2.0000

    2.0500

    2.1000

    2.1500

    2.2000

    2.2500

    2.3000

    0 1 0 00 2 0 0 0 3 0 0 0 4 0 0 0

    ii

    tt

    t

    iO

    PP

    VV

    VC

    ii

    i1

    11

    STOCK

    TPt V

    VB &

    1*

    t

    b

    VP

    PPY

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    Constant volumedepletion

    Press. Total F.V.F Compressibility

    psia Bt E-6

    8535 0.8625 2.0857 29.34

    8036 0.8752 2.1163 29.63

    7537 0.8881 2.1476 29.95

    7038 0.9014 2.1797 30.29

    6543 0.9149 2.2123 30.66

    6046 0.9288 2.2460 31.06

    5548 0.9432 2.2808 31.50

    5049 0.9580 2.3166 32.00

    4550 0.9733 2.3536 32.55

    4150 0.9860 2.3843 33.05

    4050 0.9893 2.3921 33.18

    3950 0.9925 2.4001 33.32

    3849 0.9959 2.4082 33.46

    3749 0. 9992 2. 4162

    37 24 1.00 00 2.41 81

    3608 1. 0156 2. 4558

    3592 1. 0178 2. 4611

    3576 1. 0200 2. 4664

    3561 1. 0219 2. 4712

    3547 1. 0238 2. 4756

    3532 1. 0258 2. 4806

    3508 1. 0291 2. 4885

    3472 1. 0338 2. 4998

    3424 1. 0404 2. 5158

    3353 1. 0509 2. 5412

    3254 1. 0668 2. 5795

    3120 1. 0905 2. 6369

    2940 1.1262 2.7233 2.1134 2.1148 1.1261

    2719 1.1798 2.8528 2.0567 2.0546 1.1591

    2454 1.2609 3.0490 1.9841 1.9824 1.2339

    2155 1.3836 3.3456 1.8985 1.9009 1.3469

    1835 1.5680 3.7915 1.8127 1.8138 1.5186

    1515 1.8453 4.4621 1.7252 1.7266 1.7768

    1212 2.2594 5.4634 1.6459 1.6440 2.1643

    1142 2.3915 5.7828 1.6251 1.6250 2.2750

    Constant M ass Expansion @ 287 F

    ** Y = 2.7240E-04P + 1.3139

    Smoothed VtSmoothed Y**Vt Y Function

    *

    2.0000

    2.0500

    2.1000

    2.1500

    2.2000

    2.2500

    2.3000

    0 1 0 00 2 0 0 0 3 0 0 0 4 0 0 0

    ii

    tt

    t

    iO

    PP

    VV

    VC

    ii

    i 1

    11

    STOCK

    TPt V

    VB &

    1*

    t

    b

    VP

    PPY

    LABORATORY ANALYSIS FOR RESERVOIR FLUID

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    Differential liberationOil

    Density

    g/cc

    8535 2.0857 0.6194

    8036 2.1163 0.6105

    7537 2.1476 0.6016

    7038 2.1797 0.5927

    6543 2.2123 0.5840

    6046 2.2460 0.5752

    5548 2.2808 0.5665

    5049 2.3166 0.5577

    4550 2.3536 0.5489

    4150 2.3843 0.5419

    4050 2.3921 0.5401

    3950 2.4001 0.5383

    3849 2.4082 0.5365

    3749 2.4162 0.5347

    3724 0.00 1953.10 2.4181 0.5343

    3047 501.68 1451.42 2.0603 0.5821

    2543 768.44 1184.67 1.8669 0.6162

    2039 992.88 960.23 1.7187 0.6453

    1534 1182.42 770.68 1.5947 0.6733

    1028 1370.90 582.21 1.4852 0.6985

    520 1601.63 351.47 1.3700 0.7208

    14.7 1953.10 0.00 1.1118 0.7456

    Bo@ 60oF = 1.0

    Pressure psia

    Cumulative

    Lib.GOR(2)

    SCF/STB

    Bo(3)

    Bbl/STB

    Solution GOR(1)

    SCF/STB

    3-Barrel of oil @ indicated pressure & temperature per barrel of residual oil @60oF Ii

    2-Cubic feet of liberated gas @ 14.696 psia & 60

    o

    F per barrel of residual oil @60

    o

    F

    1-Cubic feet of solution gas @ 14.696 psia & 60oF per barrel of residual oil @60

    oF

    Di ff erential Vapor ization @ 287 F

    LABORATORY ANALYSIS FOR RESERVOIR FLUID

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    LABORATORY ANALYSIS FOR RESERVOIR FLUID

    Special laboratoryPVT testsSlim tube test

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    Coring and core analysis

    Coring is the most basic formation evaluation

    tools. Core analysis provide the only initial means of

    determining the wettability ,capillary andrelative permeability characteristics of a

    reservoir. The successful use of quantitative logs

    requires core analysis data for log calibration.

    RESERVOIR ROCK PROPERTIES

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    There are basically two main categories of coreanalysis tests that are performed on coresamples:

    Routin core analysis tests Porosity Permeability SaturationSpecial core analysis

    Capillary pressure Relative permeability Wettability Surface and interfacial tension

    RESERVOIR ROCK PROPERTIES

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    RESERVOIR ROCK PROPERTIES

    1- POROSITY =Vp/Vb

    Is a measure of the spaceavailable for fluid storage

    ABSOLUTE POROSITY EFFECTIVE POROSITY

    - The percentage of isolated poresis usually rather unimportant for

    good reservoir rocks

    - Effective porosity shows a bettercorrelation with permeabilitythan the absolute porosity

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    RESERVOIR ROCK PROPERTIES

    Absolute porosity:

    a =total pore volume/bulk volume

    Effective porosity:

    e =interconnected pore volume/bulk volume

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    PERMEABILITY

    -The fluid conductancecapacity in the porousmedium.

    -Permeability is the propertyof a porous material thatcharacterized the ease withwhich fluids can go throughthe material by a givenpressure gradient.

    -For horizontal linear flow ofan incompressible fluidDarcys law is used :

    Q=KAdP/ dL

    RESERVOIR ROCK PROPERTIES

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    Saturationis defined as that fraction or percent of porevolume occupied by a particular fluid.

    fluid saturation= total volume of thefluid/pore volume

    So=volume of oil/pore volume

    Sg=volume of gas/pore volumeSw=volume of water/pore volume

    RESERVOIR ROCK PROPERTIES

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    RESERVOIR ROCK PROPERTIES

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    Wettabilitywettability is defined as the tendency

    of one fluid to spread on a solidsurface in the presence of otherimmiscible fluid.

    As the contact angle decrease thewetting characteristic of the fluidincrease.

    Complete wettability is at zero contactangle and a complete non wetting is

    by 180contact angle The wettability of reservoir rock to

    the fluids in the porous media is afunction of wettability

    RESERVOIR ROCK PROPERTIES

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    RESERVOIR ROCK PROPERTIES

    Surface and interfacial tensionIn multiphase system it is

    necessary to consider theeffect of the forces at the

    interface where twoimmiscible fluid are in contact.When the interface is between a

    liquid and a gas it is namedsurface tension and if it isbetween two liquid is namedinterfacial tension.

    Tensiometer and Pendent Drop istwo tools for measuringsurface and interfacialtension.

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    Capillary pressureThe capillary forces in a petroleum reservoir are the results of the

    combined effect of the surface and interfacial tension of therock and fluids.

    The pore size and geometry and the wetting characteristics of thesystem.

    The displacement of one fluid by another in the pores of a porousmedium is either aided or opposed by the surface forces ofcapillary pressure.

    Capillary pressure can be expressed as:

    Pc=Pnw-Pw

    RESERVOIR ROCK PROPERTIES

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    The capillary pressure that exist within aporous medium between two immiscible

    phases is a function of the interfacial tensionsand the average size of the capillaries whichcontrol the curvature of the interface.

    The curvature is also a function of the

    saturation distribution of the fluid involved.

    RESERVOIR ROCK PROPERTIES

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    The capillary pressure saturation data can beconverted into height-

    saturation data byarranging an equationand solving for a heighth above the free-water

    levelh=144*Pc/

    RESERVOIR ROCK PROPERTIES

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    RESERVOIR ROCK PROPERTIES

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    Calculating reservoir capillary pressure datafrom laboratory data:

    Laboratory Pc should be corrected before usingfor reservoir condition :

    Pcl= 2(COS)L/r

    PcR= 2(COS)R/r

    PcR= Pcl * (COS)R/(COS)LThe contact angles are usually unknown so

    PcR= Pcl * ()R/()L

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    Variation of transition zone withfluid gravity:

    The height above FWL increases withdecreasing the density difference

    From a practical standpoint , this meansthat in a gas reservoir having aGWC , the thickness of thetransition zone will be a minimumsince will be large.

    If all other factors remain unchanged ,

    a low API gravity oil reservoir withan OWC will have a longer transitionzone than a high API gravity oilreservoir.

    RESERVOIR ROCK PROPERTIES

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    Variation of transition zone withpermeability:

    The reservoir pore size can oftenbe related approximately topermeability, and where thisapplies, it can be stated that highpermeability reservoirs will haveshorter transition zones than low

    permeability reservoirs .So a tiltedOWC could be caused by a changein permeability across a reservoir

    RESERVOIR ROCK PROPERTIES

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    RESERVOIR ROCK PROPERTIES

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    RESERVOIR ROCK PROPERTIES

    Relative permeabilityeffective permeability of any reservoir fluid is a function of

    the reservoir fluid saturation and the wettingcharacteristic of the formation . Ko,Kg and Kw are theaccepted symbols for the effective permeability tooil,gas and water.

    The absolute permeability is a property of porous mediumand is a measure of the capacity of the medium totransmit fluids.

    When two or more fluids flow at the same time, therelative permeability of each phase at a specificsaturation is the ratio of the effective permeability ofthe phase to the absolute permeability

    Kro=Ko/KKrg=Kg/KKrw=Kw/Ksince the effective permeabilities may range from zero to K then:0Kro, Krg, Krw 1

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    RESERVOIR ROCK PROPERTIES

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    Normalization and averaging relativepermeability data

    Results of relative permeability testsperformed on several core samplesof a reservoir rock often vary.

    It is necessary to average the relativepermeability data obtained onindividual rock samples.

    For usage this data for oil recoveryprediction , the relative permeabilitycurves should first be normalized toremove the effect of different initialwater and critical oil saturations.

    The relative permeability can then bede-normalized and assigned todifferent regions of the reservoirbased on the existing critical fluidsaturation for each reservoir region.

    RESERVOIR ROCK PROPERTIES

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    LOGS

    Logging tools provide dataon the lithology of formationpenetrated by the well andon the porosity and water

    saturation of reservoir rocks. Logs provide the primary

    basis for determining bothGross and Net formationthicknesses.

    Correlation of the logs showthe degree of continuity ofthe reservoir.

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    Other logs

    1. Production log tools

    2. Image loges

    3. MDT/XPT

    LOGS

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    PLT TOOLS

    Through measuring pressure, densityand temperature will show the

    productive zone.

    LOGS

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    FMI

    This tool can give an image ofthe wellbore and some

    information about deep ofthe formation and presenceof vugs and fractures and avalue for porosity of thefracture.

    LOGS

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    LOGS

    MDT/XPT

    Best method of taking reservoirpressure, fluid gradient and

    type of layering of thereservoir is using MDT/XPTtools.

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    DST AND PRODUCTION TESTS

    A formation test of a well is a production testdesigned to determine the fluid content andthe productivity of the reservoir.

    Drill stem testing can establish theproductivity index , determine the truereservoir pressure and locate gas oil & wateroil contacts.

    Formation permeability and limitation of thereservoir can be detected by a reasonableproduction test.

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    DST AND PRODUCTION TESTS

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    DST AND PRODUCTION TESTS

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    RESERVOIR VOLUMETRICS

    Material balance methodThe data gathering program for any reservoir should

    include the collection of pressure, production andfluid sample data which is needed for materialbalance calculations.

    It is routin to accurately measure and record oilproduction,water and gas produced in associationwith the oil.

    For material balance calculations,water and gasvolumes are as important as oil volume.

    OOIP can be calculated through material balanceequation.

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    Volumetric methodThe volume of stock-tank oil originally inplace in a

    reservoir can be calculated from the net reservoir

    rock volume , porosity , connate water and oilformation volume factor by the following equation :OIP= V(N/G)(1-Swc)/ Bo

    V(N/G) is called the pore volume and is the total volume in the reservoirwhich can be occupied by fluids.

    V(N/G)(1-Swc) is called the hydrocarbon pore volume at reservoircondition

    OIP= V(N/G)(1-Swc)/ Bo is called the hydrocarbon pore volume atstandard condition

    RESERVOIR VOLUMETRICS

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    OIP calculation could be carried outthrough two software:

    1. Petrel for reservoir rock volumecalculation

    2. Mont carlo(REP) software through

    using probablistic analysis.

    RESERVOIR VOLUMETRICS

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    RESERVOIR VOLUMETRICS

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    RESERVOIR VOLUMETRICS

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    RESERVOIR VOLUMETRICS

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    RESERVOIR VOLUMETRICS

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    robabilistic GIIP Calculations:Key Results Golshan Gas: P

    G11, Kangan& U Dalan -

    Top Kanganspillpoint (-3500m)

    G14, L Dalan - Zakeen - inferred FWL (-3755m)

    (Petrel display artefact)

    G11, Kangan& U Dalan -

    Top Kanganspillpoint (-3500m)

    G14, L Dalan - Zakeen - inferred FWL (-3755m)

    (Petrel display artefact)

    Golshan all Dehram reservoirs

    0%

    10%

    20%

    30%

    40%

    50%

    60%

    70%

    80%

    90%

    100%

    0 7'20014'40021'60028'80036'00043'20050'40057'60064'80072'000

    GIIP/AGIIP in Bscf

    Cummulativeprobability

    0

    50

    100

    150

    200

    250

    300

    350

    400

    450

    Nr.ofoutcomes

    Dependent Cumulative P robability

    Independent Cumulative ProbabilityBscf

    p10 All Volumes 57882.5

    p50 All Volumes 44245.2

    p90 All Volumes 34186.8

    EXP = Mean All Volumes 45310.3

    P50: 44.2 TCF

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    FLUID PRESSURE REGIMES

    The total pressure at any depth, resultingfrom the combined weight of the formationrock and fluids , whether water,oil or gas isknown as the overburden pressure.in thesedimentary basins the overburden pressureincreases linearly in depth and typically hasa pressure gradient of 1 psi/ft .

    At a given depth , the overburden pressurecan be equated to the sum of the fluidpressure(FP) and the grain or matrixpressure(GP)

    OP=FP+GP Since the overburden pressure remains

    constant at any particular depthd(FP)=-d(GP)

    Then a reduction in fluid pressure will lead to acorresponding increase in the grainpressure.

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    Fluid pressure regimes in hydrocarbon columns aredictated by formation water of the reservoir.

    In a perfectly normal case the water pressure at any

    depth can be calculated as :Pw = (dP/dD)water *D +14.7 (psi)

    In which dP/dD , the water pressure gradient , isdependent on the chemical composition (salinity) ,and for pure water has the value of 0.4335 psi/ft

    The above equation assumes that there is bothcontinuity of water pressure to the surface and thatthe salinity does not vary with depth.

    FLUID PRESSURE REGIMES

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    In contrast to normal hydrostaticpressure , abnormal hydrostatic

    pressure are encountered and definedby:

    Pw = (dP/dD)water *D +14.7 +C

    Where C is a constant and could bepositive if the water is overpressuredand negative if underpressured.

    FLUID PRESSURE REGIMES

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    Range of pressure gradient

    (dP/dD)w=0.45-0.52 psi/ft

    (dP/dD)0=0.21-0.41 psi/ft

    (dP/dD)g=0.08-0.12 psi/ft

    At the oil-water contact , thepressure in the oil and watermust be equal otherwise astatic interface would notexist .

    FLUID PRESSURE REGIMES