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TRANSCRIPT
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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
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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