permeabilityscalingandflowstructuresin …massonr/momasmultiphasique2015/... · 2015. 10. 14. ·...
TRANSCRIPT
Jean-Raynald de Dreuzy1, Olivier Bour1, Caroline Darcel2, PhilippeDavy1, Jocelyne Erhel3, Romain Le Goc2, Julien Maillot1,2, Yves Méheust1,
Géraldine Pichot2
1 Géosciences Rennes, UMR CNRS 6118, University of Rennes 1, France2 Itasca Consultants S. A., Group HCItasca, Ecully, France
3 IRISA/INRIA, University of Rennes 1, France
PERMEABILITY SCALING AND FLOW STRUCTURES INFRACTURE NETWORKS
What is a fracture?Why fractures matter?
2
What is a fracture? Geology Ubiquitous: Fault, Fracture, Joint, Diaclase Plate tectonics, sismology
3
San Francisco (1906)Magnitude 8,2San Andreas
(Californie, USA)
Simpevarp (Suède)100 m
Simpevarp (Suède)1 m
Energy Minerals Division; Gas shale tricky to understandBrian Cardott (EMD Gas Shale Committee member).http://www.aapg.org/explorer/divisions/2006emd.cfm/
Ivory Coast
core Lineament mapsoutcrop
10-3 10-2 10-1 100 101 102 103 104 105
scale (m)
What is a fracture? Geology Ubiquitous: Fault, Fracture, Joint, Diaclase Plate tectonics, sismology
Mathematical modeling 2D features in 3D space (lower dimensionality)
Hydraulics Flow barriers, flow highways High permeablity, low storativity Low surface/volume features
Long, J. C. S., et al. (1985), A Model for Steady Fluid Flow inRandom Three-Dimensional Networks of Disc-Shaped
Fractures, Water Resources Research, 21(8), 1105-1115.
Maryka, J., et al. (2004), Numerical simulation of fracture flowwith a mixed-hybrid FEM stochastic discrete fracture network
model, Computational Geosciences, 8(3).
Martin, V., et al. (2005), Modeling fractures and barriers asinterfaces for flow in porous media, SIAM Journal in
Scientific Computing, 26, 1667-1691.
Tsang, C. F., et al. (2008),Simple model representations oftransport in a complex fractureand their effects on long-termpredictions, Water Resources
Research, 44(8), 13.
Geology Ubiquitous: Fault, Fracture, Joint, Diaclase Plate tectonics, sismology
Mathematical modeling 2D features in 3D space (lower dimensionality)
Hydraulics Flow barriers, flow highways High permeablity, low storativity Low surface/volume features
Mechanics Dynamic, Chaotic Energy dissipation
Physics Statistics, emergence
What is a fracture?
Stauffer, D., and A. Aharony (1992),Introduction to percolation theory, second
edition, Taylor and Francis, Bristol.
Why fractures matter? Negative fracture perception Waste storage, connectivity issues Interacting energetic and environmental applications
Positive impact of fractures on resources oil and gas recovery 3D volume (geothermal energy STES) Groundwater (India, Africa) , Aquifer (connectivity)
Fractures (more generally geological complexity) Source of uncertainty Coexistence of services (storage, resources, environment)
Requires CONTROL Observations, Monitoring Modeling Data processing, calibration, assimilation
6
7
Fracture versus rock permeability
10-5 10-4 10-3
10-11
10-10
10-9
10-8
10-7
10-6
10-5
Equivalent fr
acture perm
eability
n=0.01m-1
n=0.1m-1
Keq
(m/s
)
a (m)
mm100 m Matrix permeability
n=0.001m-1
L/n
L
Km
W
a: hydraulic aperture
High Fracture DensitiesExtreme flow channeling
Small Permeability
8
Flow structures in natural fractured mediaMultiple-scale Channeling and limited permeability
9
Fracture scale
Network scaleStripa
http://www.imstunnel.com/page_03.htmBolmen channels 2
Quality of Water from CrystallineRock Aquifers in New England, NewJersey, and New York, 1995–2007http://pubs.usgs.gov/sir/2011/5220/
80 % of flow100 % of flow
Stripa, Olsson [1992]
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical-issued correlation patterns (fracture
organization)10
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical-issued correlation patterns (fracture
organization)11
=1arithmetic meanparallel model
KN=K(d,L) exp[w(d,a).s2(log K1)/2]
=-1harmonic meanin series model
=0geometric mean
2D Poissonian fracture networksa: length distribution parameterd: density parameters2(log K1): fracture log-permeability variance
de Dreuzy, J. R., et al. (2001a), Hydraulic properties of two-dimensional random fracture networks following a power law length distribution: 2-Permeability of networks based on log-normal distribution of apertures, Water Resources Research, 37(8), 2079-2095.de Dreuzy, J. R., et al. (2001b), Hydraulic properties of two-dimensional random fracture networks following a power law length distribution: 1-Effective connectivity, Water Resources Research, 37(8).de Dreuzy, J. R., et al. (2002), Permeability of 2D fracture networks with power-law distributions of length and aperture, Water Resources Research, 38(12).
K(d=dc)~L-1
K(d>dc)~d
MODELS ARE MUCH TOO PERVIOUSReduction for sparse networks by
tortuosity and BOTTLE NECKSBUT
Large fractures prevent sparsityand enhance permeability
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE: bottle necks versus large fractures Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical-issued correlation patterns (fracture
organization)13
Permeability of rough fractures
Méheust, Y., and J. Schmittbuhl (2000), Flow enhancement of a rough fracture, Geophysical Research Letters, 27(18).Méheust, Y., and J. Schmittbuhl (2001), Geometrical heterogeneities and permeability anisotropy of rough fractures, Journal of Geophysical Research-Solid Earth, 106(B2),2089-2102.14
http://www.comsol.com/products/4.2/
15
Local aperture distributionTruncated Gaussian with abounded self-affine correlation pattern http://www.comsol.com/products/4.2/
00
02
1/
2
2
2
1/
ifa
ifaec=aap
frac
m
c
aa
fracm
a/am
16
Frac
ture
aper
ture
and t
rans
missi
vity d
istrib
ution
show
nby
dash
ed an
d soli
d lin
es re
spec
tively
.
10-2 10-1 100 101 102
10-4
10-3
10-2
10-1
100
101 Aperturec=1.5
Transmissivityc=1.5
p(T l/T
lm)
Tl/Tlm
10-2 10-1 100 101 102
10-4
10-3
10-2
10-1
100
101Aperture
c=1.5p(
a /a
m)
a/am
00
02
1/
2
2
2
1/
ifa
ifaec=aap
frac
m
c
aa
fracm
2
23/1
3/23/12 2
/exp
3β1
2π1 cβT
T=TpT
From local apertureto local transmissivity
http://www.comsol.com/products/4.2/
T~a3
Effective permeability KAnormalized by the equivalent parallel platepermeability K1
17
http://www.comsol.com/products/4.2/
0 1 20,0
0,5
1,0
Reduction by a factor of 4
cfrac
Single Fracture
Reduction by a factor of 2
1K
K A
Roughness:Reduction factor of K :2 to 4 at most
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE: reduction factor of 2 to 4 at most Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE: bottle necks versus large fractures Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical-issued correlation patterns (fracture organization)COMBINATION FRACTURE/NETWORK
18
10-1 100 101 10210-710-610-510-410-310-210-1100101102
n(l)~ LD2d=1.75 l-a2d=2.75
n(l)/
LD
fracture length, l
Multi-Scale Discrete Fracture Network models (DFNs)
19
Field-based DFNs Power-law length distribution Orientation distribution Correlation patterns (mechanics) Fracture density Fracture roughness Fracture aperture Intersection structure Matrix permeability
Simplifications Keep connected clusters Keep large fractures
Hydraulic simulations Large scale, highly resolved 3D
Odling, N. E. (1997), Scaling and connectivity of joint systems insandstones from western Norway, Journal of Structural Geology,
19(10), 1257-1271.Bour, O., et al. (2002), A statistical scaling model for fracture
network geometry, with validation on a multiscale mapping of ajoint network (Hornelen Basin, Norway), Journal of Geophysical
Research, 107(B6).
Hornelen, Norway
Broad power-law length distribution n(l)~l-a withlmin<l<L
Large number of fractures: ~15 103
L=50
l min
MP_FRAC
Multi-scale DFN hydraulic simulations
20
Field-based DFNs Power-law length distribution Orientation distribution Correlation patterns (mechanics) Fracture density Fracture roughness Fracture aperture Intersection structure Matrix permeability
Simplifications Keep connected clusters Keep large fractures
Hydraulic simulations Large scale, highly resolved 3D
MP_FRAC
Network Fracture
Network+
Fracture
.a3h=0
Log a3
Flow equation PermeameterBoundary conditions
KN KF
KN+F
K=QL/(DhS)
Combined fracture- andnetwork-scale effects
21
Fracture Network Flows withuniform apertures
KN
Flows withdistributed apertures
KN+Fde Dreuzy, J.-R., Y. Méheust, and G. Pichot (2012), Influence of fracture scale heterogeneity onthe flow properties of three-dimensional Discrete Fracture Networks (DFN), J. Geophys. Res.-Earth Surf., 117(B11207), 21 PP.
Effective permeability KN+ADense Networks
22
0 1 20,0
0,5
1,0
Reduction by a factor of 4
cfrac
Single Fracture
Reduction by a factor of 2
1K
K FN
Hihgly limited effects
Effective permeability KN+ASparse Networks
23
0 1 20,0
0,5
1,0
Reduction by a factor of 4
cfrac
Single Fracture
Reduction by a factor of 2
1K
K FN
Additional reduction by a factor of 2 to 3
Effective permeability KN+FPercolation Networks
24
0 1 20,0
0,5
1,0
Reduction by a factor of 4
cfrac
Single Fracture
Reduction by a factor of 2
1K
K FN
Additional reduction by a factor of 5 to 10
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE: reduction factor of 2 to 4 at most Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE: bottle necks versus large fractures Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical-issued correlation patterns (fracture organization)COMBINATION FRACTURE/NETWORK: reduction factor of 2 to 10
25
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE: reduction factor of 2 to 4 at most Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE: bottle necks versus large fractures Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical-issued correlation patterns (fracture organization)COMBINATION FRACTURE/NETWORK: reduction factor of 2 to 10
26
Mechanical induced organization of thefracture network (preliminary results)
27
High connectivity
Low connectivityTypical trace
map view1.0 1.5 2.0
0.01
0.1
1 BCBSAC
K
P32
AS
UFM
Poisson
Reduction factor of K :3 to 10
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE: reduction factor of 2 to 4 at most Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE: bottle necks versus large fractures Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections) Mechanical correlation patterns: reduction factor of 3 to 10COMBINATION FRACTURE/NETWORK: reduction factor of 2 to 10
28
Impact of Intersection length (l2)
29 With an analytical image method adapted from Long [1985]
10-6 10-4 10-2 1000,00
0,25
0,50
0,75
1,00
l1
Teq
(l2)/
T1
l2
IntersectionLimiting
l 2
0
l 1
1
2ln
1~
l
l
Reduction factor of K :2 to 4
Why are flows so channelled andpermeability so limited?
FRACTURE SCALE: reduction factor of 2 to 4 at most Fracture roughness Fracture sealing/dissolution (chemistry) Fracture closing/opening (mechanical)NETWORK SCALE: bottle necks versus large fractures Fracture length distribution Global connectivity (network effects) Effective transmissivity variability (orientations, depth) Local connectivity (intersections): reduction factor of 2 to 3 Mechanical correlation patterns: reduction factor of 3 to 10COMBINATION FRACTURE/NETWORK: reduction factor of 2 to 10
30
Modeling frameworksRelevant-RealisticSimple-Tractable
31
« Historical » modelling frameworks
32
Warren and Root (1963), The Behavior ofNaturally Fractured Reservoirs, Society ofPetroleum Engineers Journal, September,
245-255.
Double Porosity
Neretnieks, I. (1980), Diffusion in the RockMatrix: An Important Factor in
Radionucleside Retardation?, Journal ofGeophysical Research, 85(B8), 4379-4397.
Neuman SP (1987) Stochastic continuumrepresentation of fractured rock permeability as
an alternative to the REV andfracture network concepts. Proceedings of the
28th US Symposium, Tucson, Arizona
Stochastic Continuum
Snow, D. T. (1969), Anisotropic permeabilityof fractured media, Water Resources
Research(5), 1273-1289.
Discrete FractureNetwork
Long, J. C. S., et al. (1982), Porous MediaEquivalents for Networks of Discontinuous
Fractures, Water Resources Research, 18(3), 645-658.
Simpevarp (Sweden) 1 m
Stripa, 1980s
L
LO
G10
()
K
-9
-12
-15
-18
-21
-24 cm m km 100 km
Clauser, C. (1992), Permeability of crystalline rock, EosTrans. AGU, 73(21), 237-238.
10-1 100 101 10210-710-610-510-410-310-210-1100101102
n(l)~ LD2d=1.75 l-a2d=2.75
n(l)/
LD
fracture length, l
Multi-Scale DFN models: building simplifications
33
Field-based DFNs Power-law length distribution Orientation distribution Correlation patterns (mechanics) Fracture density Fracture roughness Fracture aperture Intersection structure Matrix permeability
Simplifications Keep connected clusters Keep large fractures
Hydraulic simulations Large scale, highly resolved 3D
Hornelen, Norway
Broad power-law length distribution n(l)~l-a withlmin<l<L
Large number of fractures: ~15 103
L=50
l min
MP_FRAC
Equivalent Permeability,controls on the flow structure
34 de Dreuzy, J. R., Y. Méheust, G. Pichot (2012), Influence of fracture scale heterogeneity on the flow properties of three-dimensional discrete fracturenetworks (DFN), Journal of Geophysical Research-Solid Earth, 117.
< 1 > 1= 1
Bottlenecks Parallel paths
KN
KN+F K0
KF KN
KN+F K0
KF KN
KN+F K0
KF
Reference Multi-Scale DFN modelsAlternative modeling concepts
35
Field-based DFNs Power-law length distribution Orientation distribution Correlation patterns (mechanics) Fracture density Fracture roughness Fracture aperture Intersection structure Matrix permeability
Simplifications Keep connected clusters Keep large fractures
Hydraulic simulations Large scale, highly resolved 3D
Elementary cellStructured Interacting Continua
Multiple-scaleRenormalizationGroup Method
Gavrilenko, P., and Y. Guéguen (1998), Flow in fractured media: A modifiedrenormalization method, Water Resources Research, 34(2), 177-191.
Discrete Double-PorosityD. Roubinet
Elementary cellSingle Rate Mass Transfer
Comparisonto double porosityComparison
to Multiple Interacting Continua
Pruess, K., and T. N. Narasimhan (1985), A practical method for modeling fluid and heat-flowin fractured porous-media, Society of Petroleum Engineers Journal, 25(1), 14-26.
Discrete multiple-porosity media
36
Multi-scale Fractured Media Fracture structures Network complexity Fracture/Matrix interactions
Hydraulic DFN MP_FRAC High-resolution 3D flow simulations Training basic
Alternative modeling concepts Structured Interacting Continua Multiple-scale permeability Discrete Double porosity
Calibration and Testing Synthetic training Field testing
Elementary cellStructured Interacting Continua
Multiple-scaleRenormalizationGroup Method
Discrete Double-PorosityD. Roubinet
Conclusions
Hydraulics in fractured media Large structures are essential Details matter!
Permeability Scaling and sampling Variable, High channeling
Modeling Main discrete structrues Multi-porosity
37
Elementary cellStructured Interacting Continua
Multiple-scaleRenormalizationGroup Method
Discrete Double-PorosityD. Roubinet