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Porescale modelling of WAG: impact of wettability

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Title: Porescale modelling of WAG: impact of wettability


1
Pore-scale modelling of WAGimpact of wettability
  • Rink van Dijke and Ken Sorbie
  • Institute of Petroleum Engineering
  • Heriot-Watt University
  • WAG Workshop FORCE, Stavanger, 18 March 2009

1
2
Introduction
  • 3-phase (immiscible) flow processes, e.g.
  • water-alternating-gas injection (WAG) improved
    oil recovery
  • NAPL in unsaturated zone ground water
    remediation
  • modelled with Darcys law
  • capillary pressure and relative permeability
    functions
  • difficult to measure
  • pore-scale modelling

3
Introduction
  • Pore-scale modelling
  • pore space structure
  • connectivity (topology)
  • geometry (pore sizes and shapes)
  • flow mechanisms
  • capillary forces
  • conductance (viscous forces)
  • wettability (contact angles)
  • incorporated in
  • idealized network models (quasi-static invasion
    percolation or dynamic)
  • capillary bundle models

3
4
Introduction
  • Capillary forces
  • invasion of a single tube (cylinder)
  • rule for displacement of water by oilwith
    capillary entry pressure according to
    Young-Laplace

4
5
Introduction
  • Wettability
  • wettability of pore surface defined in terms of
    oil-water contact angle (measured through water)
  • water-wet if
  • oil-wet if

water
oil
SOLID SURFACE
5
6
Introduction
  • Wettability
  • in 3-phase flow contact angles
  • related by Bartell-Osterhof equation
  • constitute capillary entry pressures for
    gas-water and gas-oil displacements, e.g.
  • determine presence of wetting films and spreading
    layers

6
7
Introduction
  • Micromodel experiments
  • understand flow mechanisms
  • validate pore-scale network models
  • Sohrabi et al. (HWU)

7
8
Outline effects of wettability
  • Saturation-dependencies of three-phase capillary
    pressures and relative permeabilities
  • Intra-pore physics
  • fluid configurations
  • capillary entry pressures and layer criteria
  • non-uniform wettability
  • Network displacement mechanisms
  • phase continuity and displacement chains
  • WAG simulations
  • comparison simulations and WAG micromodel
    experiments
  • Concluding remarks

8
9
Saturation-dependencies
  • Traditional example (Corey et al., 1956)
  • Curved oil isoperms
  • Straight water and gas isoperms

10
Saturation-dependencies
  • Traditional assumptions for saturation-dependencie
    s
  • Water-wet system water wetting to oil wetting to
    gas ? water in small pores, gas in big pores

pore occupancy (number fraction)
water
oil
gas
pore size r
11
Saturation-dependencies
  • Wettability distributions in porous medium often
    correlated to pore size
  • mixed-wet with larger pores oil-wet (MWL) may
    occur after primary drainage and aging (similarly
    MWS)

11
12
Saturation-dependencies
  • Paths in saturation space gas flood into oil,
    followed by water flood into gas and oil
  • capillary bundle model

water-wet
oil-wet
I
II
III
13
Saturation-dependencies
  • Regions in saturation space iso-capillary
    pressure curves

II
II
II
gas is intermediate-wetting
14
Saturation-dependencies
  • Regions in saturation space iso-relative
    permeability curves

II
II
II
gas is intermediate-wetting
15
Saturation-dependencies
  • numerical example FW capillary bundle

16
Intra-pore physics
  • Films and layers
  • water-wet micromodel WAG flood
  • water wetting films around both oil and gas
  • possible oil layers separating water and gas

16
17
Intra-pore physics
  • Fluid configurations in angular pores
  • water-wet pores, e.g. strongly water-wet
    all close to 0
  • water wetting films around both oil and gas
  • possible oil layers separating water and gas
    affected by oil spreading coefficient
  • oil-wet pores, e.g. weakly oil-wet close to
    90 degrees, close to 0
  • no oil wetting films around water
  • only oil wetting films around gas
  • ensures phase continuity along pores

17
18
Intra-pore physics
  • true 3-phase capillary entry pressures (improved
    Y-L)
  • gas-oil entry pressure depends on water wetting
    film pressure
  • determined by free energy calculation (MS-P)
  • also criterion for (oil) layers

bulk displacement
layer displacement
18
19
Intra-pore physics
  • consistent relation 3-phase pressure differences
    and occupancies

oil-water bulk displacement
gas-oil bulk displacement (true varying)
gas-oil bulk displacement, with layer (constant)
layer displacement
20
Intra-pore physics
  • mixed-wet bundle of triangular pores
  • small pores strongly water-wet
  • large pores weakly oil-wet

20
21
Intra-pore physics
  • water injection
  • no difference true (3-phase) and constant
    (2-phase) during invasion of water-wet pores
  • huge differences during invasion of oil-wet
    pores
  • true simultaneous w-gto and w-gtg
  • volume effectoil films

21
22
Intra-pore physics
  • nonuniform wettability
  • after primary - after imbibition drainage
  • strongly affects water flood Sor (Ryazanov et
    al., 2009)

surface rendered oil-wet aging(Kovscek)
oil layers (2-phase)
oil
water
22
23
Intra-pore physics
  • non-uniform wettability
  • layers in 3-phase configuration
  • consistent entry pressures and layer criteria

23
24
Intra-pore physics
high Pow drainage
24
25
Network displacement mechanisms
  • phase continuity
  • connectivity
  • films and layers (wettability)
  • water-wet micromodel WAG flood

25
26
Network displacement mechanisms
  • connected, trapped and disconnected phases
  • phase cluster map

disconnected oil cluster
water cluster connected to outlet
invading gas cluster
outlet
inlet
trapped oil cluster
oil cluster connected to outlet
disconnected water cluster
disconnected gas cluster
26
27
Network displacement mechanisms
  • multiple displacement chains displace
    disconnected clusters
  • based on target pressure difference
  • determining lowest target requires shortest path
    algorithm

e.g. gas-gtoil-gtgas-gtwater
28
Network simulations
  • 3-phase flow simulator 3PhWetNet regular
    lattice, arbitrary wettability,
    capillary-dominated flow
  • few free parameters describing essence of
    pore-scale displacements (needs anchoring)
  • coordination number z
  • pore size distribution
  • volume and conductanceexponents
  • wettability (contact angledistribution)
  • film and layers (notional)

29
Network simulations
  • Network model
  • parameters anchored to easy-to-obtain data
    network structure and wettability
  • example mixed-wet North Sea reservoir data

water flood
gas flood
29
30
Network simulations
  • Network model
  • predict difficult-to-obtain data, e.g. 3-phase kr
    and Pc

three-phase gas relperms
three-phase gas injection displacement paths
30
31
WAG network simulations
  • mixed-wet
  • no films or layers
  • varying coordinationnumber z
  • high residual, but additional recovery during WAG
    for z3

32
WAG network simulations
  • displacement statistics (chain lengths), z5
  • few multiple, many double displacements
  • continuing phase movement but no additional
    recovery

33
WAG network simulations
  • displacement statistics (types), z5
  • mainly 3 displacement types, corresponding to
    doubles, e.g. g-gto and o-gtw during gas flood

34
WAG occupancy statistics (z5)
after water flood 1
35
WAG occupancy statistics (z5)
during gas flood 1
gas intermediate-wetting
36
WAG occupancy statistics (z5)
end of gas flood 1
oil moved into water-wet pores
37
WAG occupancy statistics (z5)
end of water flood 2
oil moved back into oil-wet pores
38
WAG network simulations
  • WAG occupancy statistics (z5) end gas flood 2
  • oil and gas in both water-wet and oil-wet pores

39
WAG network simulations
  • Chain lengths (z3)
  • significant
    number of multiple chains

z5
40
WAG network simulations
  • Displacementtypes (z3)

z5
additional types of displacements g-gto for water
and o-gtg for gas floods
41
WAG simulation micromodel experiment
water-wet
oil-wet
  • weakly wetted little evidence of (continuous)
    water and oil wetting films (around water)
  • spreading oil assume oil layers and oil wetting
    films around gas

mN/m
41
42
WAG simulation micromodel experiment
  • Fractionally-wet
  • 50 water-wet oil-wet pores
  • angles distributed between 60-120 degrees
  • oil layers and oil wetting films around gas
  • Comparison simulated and experimental
    recoveries
  • recoveryceases afterWAG 2

42
43
WAG simulation micromodel experiment
  • Displacement chain lengths
  • many multiples (few films low phase continuity)
  • multiples dying out after WAG 3

43
44
WAG simulation micromodel experiment
  • Type of displacements
  • all types of displacements occur
  • many displacements involving oil movement
  • after WAG 3 mainly w-gtg, g-gtw

44
45
WAG simulation micromodel experiment
  • fluid distributions aftergas flood 1
  • narrow gas finger in both simulation and
    experiment
  • significant amount of oil displaced
  • multiple displacements e.g. gas-gtoil-gtgas-gtwater

45
46
WAG simulation micromodel experiment
  • fluid distributions after water flood 1
  • water disperses gas
  • slightly more extensive in experiment

46
47
WAG simulation micromodel experiment
  • fluid distributions after gas flood 2
  • different gas finger appears
  • additional oil production

47
48
WAG simulation micromodel experiment
  • fluid distributions after gas flood 3
  • new gas finger in simulation
  • some additional oil displaced (jump in
    recovery)
  • after this flood mainly water displacing gas and
    vice versa

48
49
Conclusions
  • Mixed wettability leads to three types of pore
    occupancy and corresponding saturation-dependenci
    es of three-phase capillary pressures and
    relative permeabilities
  • difficult to capture in empirical model
  • True three-phase capillary entry pressures and
    layer criteria essential for consistent and
    accurate modelling
  • Phase continuity driver for WAG at pore-scale
  • strongly affected by network connectivity and
    presence films and layers precise wettability
  • multiple displacement chains
  • new fluid patterns during each cycle
    (micromodels)
  • recovery ceases after few WAG floods, oil
    movement may continue

49
50
Near-miscible WAG micromodel
After 2 hours
After 1 hour
  • Continued gas injection in strongly water-wet
    experiment
  • Much oil displaced through film flow mass
    transfer (?)

50
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