In the name of God Three-Phase Flow in Mixed-Wet Porous Media Mohammad Piri Prof. Martin Blunt...
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Transcript of In the name of God Three-Phase Flow in Mixed-Wet Porous Media Mohammad Piri Prof. Martin Blunt...
In the name of God
Three-Phase Flow in Mixed-Wet Porous Media
Mohammad PiriMohammad Piri
Prof. Martin BluntProf. Martin Blunt
Petroleum Eng. and Rock Mechanics (PERM) Research Group Department of Earth Science and Engineering
Imperial College
Acknowledgments
Enterprise OilEnterprise Oil StatoilStatoil ShellShell BHPBHP Gas de FranceGas de France PDVSA – Intevep PDVSA – Intevep SchlumbergerSchlumberger Japan National Oil Corporation (JNOC)Japan National Oil Corporation (JNOC) Department of Trade and Industry Department of Trade and Industry
(DTI)(DTI)
We Thank the Members of the Imperial College Consortium on Pore-Scale Modelling for Their Generous and Continued Support of our Research:
Outline Why Three-Phase Flow and Physically-Based Network
Modelling ?
Model We Use
Three-Phase Physics • Layer Formation • Wettability and Contact Angles
• Three-Phase Generic Configurations
• Network of Displacements for Every Type of Possible Two and Three
Phase Processes – Example, Water-Wet System
Network Modelling and Some of Its Complications• How to Choose the Right Displacement at Each Time?
• Single, Double and Multiple Displacements and Their Volume Errors• Relative Permeability Computation• Connectivity and Clustering and How Important They Are !
Three-Phase Results
Applications, Future Works and Conclusions
Why Three_Phase Flow ?
Gas Injection in Oil ReservoirsGas Injection in Oil Reservoirs
DepressurisationDepressurisation
Solution Gas DriveSolution Gas Drive
Gravity DrainageGravity Drainage
Thermal FloodingThermal Flooding
Steam InjectionSteam Injection
NAPL Migration in the Unsaturated ZoneNAPL Migration in the Unsaturated Zone
NAPL Flow in the Saturated Zone in the Presence of NAPL Flow in the Saturated Zone in the Presence of Gas Gas
We Face with Three Phase Systems at Following Processes:
Very Difficult to to Measure 3-Phase Relative Very Difficult to to Measure 3-Phase Relative
Permeabilities Particularly for Whole Range of O/W, Permeabilities Particularly for Whole Range of O/W, G/WG/W
and G/O Contact Anglesand G/O Contact Angles
Empirical Correlations have Little or No Physical BasisEmpirical Correlations have Little or No Physical Basis
Enormously Reduces the Uncertainty Associated with Enormously Reduces the Uncertainty Associated with the the
Assessment of Gas Injection ProjectsAssessment of Gas Injection Projects
Significantly Improves our Understanding of Three-Significantly Improves our Understanding of Three-Phase Phase
Physics for the Design of Recovery Processes Physics for the Design of Recovery Processes
Guide to Construct New Empirical ModelsGuide to Construct New Empirical Models
Directly in a Dynamic Up-scaling ApproachDirectly in a Dynamic Up-scaling Approach
Why Physically-Based Three-Phase Network Models ?
A Realization of Berea Sandstone (A Realization of Berea Sandstone (Statoil’s Statoil’s Network)Network)
Porosity = 24.02 %Porosity = 24.02 %
Cube Size = 3 mm*3mm*3mmCube Size = 3 mm*3mm*3mm
No. of Pores=12349No. of Pores=12349
No. of Throats=26146No. of Throats=26146
Coordination Number=1 to 19Coordination Number=1 to 19
Pores Inscribed Radius= 3.62 to 73.54 (um)Pores Inscribed Radius= 3.62 to 73.54 (um)
Throats Inscribed Radius= 0.90 to 56.85 (um)Throats Inscribed Radius= 0.90 to 56.85 (um)
Clay Volume=5.7%Clay Volume=5.7%
Triangular Shape (Irregular & Equilateral)=92.27 %Triangular Shape (Irregular & Equilateral)=92.27 %
Rectangular Shape=6.51 %Rectangular Shape=6.51 %
Circular Shape=1.22 %Circular Shape=1.22 %
Model We Use
Configuration E Configuration F Configuration G Configuration H
Configuration C Configuration DConfiguration A Configuration B
Two and Three-Phase Generic Configurations
GasWaterOil
Configuration J Configuration KConfiguration I Configuration L
Configuration NConfiguration M Configuration oConfiguration P
Two and Three-Phase Generic Configurations(Cont.)
GasWaterOil
WF= Water Flooding
GI = Gas Injection
PD = Primary Drainage
OI = Oil Injection
/ = OR
C
D
E
A B
F
G
H
K
J
I
L MN
F
E
O
P
C
D
WF
PD
WF
WF
WF
WF
GI
GI
GI
WF
GI
GI/OI
GI
GI/WF
GI/WF
GI OI
WF/O
I
WF/O
I
OI
WF/OI
WF/O
I
WF
WF/O
I
GI/WF
WF/OI
WF
GI/WF
WF WF
GI/WF
WF
GI GI
A B
C E
G
I
Displacements Network
PD,WF and GI in Strongly Water-Wet Systems
Configuration CConfiguration A Configuration B
Configuration EConfiguration G
Primary Drainage
Water Flooding
Gas Injection
Configuration I
Layer Collapsing
gw
go Gas Injection
GasWaterOil
How to Choose Right Disp. Each Time?1. A capillary pressure between any two phases is defined as:
jiCij PPP
2. The capillary pressure required to do Piston-Like, Snap-off or Layer Collapsing events that leads to configuration change is calculated using pore inscribed radius, right contact angle, corner angle(s) and interfacial tension.
3. Calculated capillary pressures are placed in one of six following sorted lists corresponding to what phase displaces what phase : Water to Gas, Water to Oil, Gas to Oil, Gas to Water, Oil to Water, Oil to Gas4. In every list we favour the event that needs lower pressure of displacing phase. This corresponds to the event with the lowest capillary pressure in Drainage processes and the highest capillary pressure in Imbibition processes.
5. During injection of phase I, it displaces either phase J or K at each time (i.e. event). To find which of these should be done at every time:
5-A) Find the most favourable event in I to J and I to K lists
5-B) Between the two most favourable events the one that needs lower
I pressure is favoured
How to Choose Right Disp. Each Time?
Example:
Gas injection after water flooding in a strongly oil-wet system:
Pcgw1
Pcgw2
Pcgw3
.
.
.
Pcgwn
Pcgo1
Pcgo2
Pcgo3
.
.
.
Pcgon
Pg1=Pw+Pcgw1
Pcgw = Pg - Pw
Pgn=Po+Pcgon
Pcgo = Pg - Po
Gas Invasion into Oil Imbibition
Process
Gas Invasion into water Drainage
Process
If Pg1<Pgn do G/W
Else do G/OAscending
Ascending
Single Displacements
1. Both Displacing and Displaced Phases Need to be Connected to Either Inlet or Outlet
2. There is no Volume Error
Gas Injection into Oil in a Strongly Water-wet System (Drainage Process)
Gas
Oil
Double Displacements and Volume Error
1. Only the First and the Third Phases are Connected to Either Inlet or Outlet in the case of Double Displacements
2. There is Volume Error that Needs to be Dealt With
3. Multiple Displacements Involving More Than One Intermediate Stage are Also Possible if Two Phases are Trapped.
Gas Injection into Oil in a Strongly Oil-wet System
Gas into Water is an Imbibition Process
Water into Oil is a Drainage Process
GasOil
Water
= Circular Cross Section
Test for Trapping of all Three PhasesTest for Trapping of all Three Phases
Use Theoretical and Empirical Use Theoretical and Empirical Expressions to Calculate Layer, Corner Expressions to Calculate Layer, Corner and Centre Conductance and Centre Conductance
Relative Permeability
Pore I
Pore J
IJL
)( ,,,
, JiIiIJ
IJiIJi PP
L
gq (I)
Ji
J
Ii
I
ti
t
IJi
IJ
g
L
g
L
g
L
g
L
,,,, 2
1(II)
Connectivity and Clustering(Cont.)
Inlet
Outlet
Cluster is Connected
*
Dead End
Periodic Boundary Condition
Cluster Connectivity(Cont.)
The pore that displacement is happening in it
Clusters with different phases surrounding the pore
Using phase connectivity could be very time consuming because:
1. For every single displacement connectivity of both displacing and displaced phases need to be checked
2. For double and multiple displacements we need to define the trapped and connected clusters
3. It is necessary to know the connectivity of all the site-phases in the network in order to calculate the relative permeabilities
How can we deal with this?
Before displacement
1 Check whether the pore allows clusters with the same fluids to be connected to each other through its sites
2 If yes store “ Connected “ else “ Not-Connected “
After displacement
4 Check whether the pore allows clusters with the same fluids to get connected to each other through its sites
5 If yes store “ Connected “ else “ Not-Connected “
6 Compare the connection of clusters with same fluids before and after the displacement and decide whether to check the continuity of clusters to inlet or outlet, based on the type of displacement and their flags before the displacements.
Cluster Connectivity(Cont.)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Sw (frac.)
Kro
Krw
Dr. Paal-Eric OerenMohammad Piri
Per Valvatne
Two-Phase Results
Reassuring that Three Independent Codes
Give the Same Results.
0
10000
20000
30000
40000
50000
60000
70000
0 0.2 0.4 0.6 0.8 1
Pcow
Sw (frac.)
Tertiary Gas Injection, Strongly Water-wet System
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1Oil Saturation (frac.)
Oil
Re
lati
ve
Pe
rme
ab
ility
TGI, Soi = 0.60
TGI, Soi = 0.665
TGI, Soi = 0.53
SGI, Soi=0.745
Tertiary Gas Injection, Strongly Water-wet System(Cont.)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Gas Saturation (frac.)
Ga
s R
ela
tiv
e P
erm
ea
bil
ity
TGI, Soi = 0.53TGI, Soi = 0.60
TGI, Soi = 0.665SGI, Soi=0.745
0
0.002
0.004
0.006
0.008
0.01
0.012
0.014
0.016
0.018
0.02
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Water Saturation (frac.)
Wa
ter
Re
lati
ve
Pe
rme
ab
ilit
y
TGI, Soi = 0.53
TGI, Soi = 0.60
TGI, Soi = 0.665
Tertiary Gas Injection, Strongly Water-wet System(Cont.)
Tertiary Gas Injection, Strongly Oil-wet System
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Oil Saturation (frac.)
Oil
Re
taiv
e P
erm
ea
bil
ity
Soi=0.665, Teta_ow=180.0 deg.
Soi = 0.665, Teta_ow=60.0 deg.
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Gas Sauration (frac.)
Ga
s R
ela
tiv
e P
erm
ea
bil
ity
Soi=0.665, Teta_ow=180.0 deg.
Soi = 0.665, Teta_ow=60.0 deg.
Tertiary Gas Injection, Strongly Oil-wet System
WAG Flooding, Water-wet System
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Oil Saturation (frac.)
Oil
Re
lati
ve
Pe
rme
ab
ilit
y
First WF Soi=0.745 to So=0.264TGI from Soi=0.662 to So=0.543Second WF from Soi=0.543 to So=0.185TGI from Soi=0.662 to So=0.514Second WF from Soi=0.514 to So=0.157 TGI from Soi=0.662 to So=0.056TGI from Soi=0.662 to So=0.597Second WF from Soi=0.597 to So=0.219TGI from Soi=0.662 to So=0.636Second WF from Soi=0.636 to So=0.238
Effects of Initial Oil Saturation on Second Water Flooding
WAG Flooding, Water-wet System
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
Oil Saturation (frac.)
Oil
Rel
ativ
e P
erm
eabi
lity
First WF Soi=0.745 to So=0.264TGI from Soi=0.64 to So=0.52Second WF from Soi=0.52 to So=0.185TGI from Soi=0.616 to So=0.526Second WF from Soi=0.526 to So=0.2 TGI from Soi=0.662 to So=0.528Second WF from Soi=0.528 to So=0.179TGI from Soi=0.687 to So=0.504Second WF from Soi=0.504 to So=0.157Secondary Gas InjectionTGI from Soi=0.590 to So=0.523Second WF from Soi=0.522 to So=0.222
WAG FloodingWAG Flooding
Gas Injection into Different SoiGas Injection into Different Soi
Secondary vs. Tertiary Gas Secondary vs. Tertiary Gas InjectionInjection
Applications
Couple Pore Scale Network Couple Pore Scale Network Model to 3D Simulator to Model to 3D Simulator to Capture a Physically Based Kr Capture a Physically Based Kr for the Correct Displacement for the Correct Displacement PathPath
Solution Gas Drive Solution Gas Drive
Future Work
Conclusions
Three-Phase ModelThree-Phase Model
Relative Permeability and Capillary Relative Permeability and Capillary Pressure ResultsPressure Results
Working on Coupling a Pore-Scale Working on Coupling a Pore-Scale Network Model with Larger-Scale Network Model with Larger-Scale Simulation and Including More PhysicsSimulation and Including More Physics