HAL Id: hal-01511167
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Submitted on 20 Apr 2017
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Public Domain
Chemical degradation of a numerical material - Application to a Fontainbleau sandstone
Kajetan Wojtacki, Loïc Daridon, Yann Monerie
To cite this version:
Kajetan Wojtacki, Loïc Daridon, Yann Monerie. Chemical degradation of a numerical material - Application to a Fontainbleau sandstone. InterPore - 8th International Conference on Porous Media
& Annual Meeting, May 2016, Cincinnati, United States. �hal-01511167�
Elasticity - Periodic Homogenization Highlights
1. Simple and efficient method that allows to obtain morphologically equivalent realisations of Fontainebleau sandstone
2. New method allowing to impose periodic B.C. on non-periodic geometries
3. Two simple models of chemical degradation
4. Heuristic relation coupling elastic moduli and permeability
Context
Carbon Capture and Storage (CCS) consists of injecting large quantities of CO
2in supercritical form directly into deeply located geological formations e.g. saline aquifers. During geological storage, chemical dissolution induces important and irreversible changes of the rock properties.
Objective is to propose a methodology which allows us to predict the evolution of effective mechanical behaviour of saline aquifers caused by microstructural changes due to CCS.
Numerical Samples - Generation
The method is inspired by natural formation process of sandstones [Bakke and Øren, 1997] and adjusted in order to
respect aforementioned morphological properties:
1. grain deposit - monodisperse grains assembly of initial radius 14 px, deposed into 3D box,
2. triaxial compaction - bulk volume reduction, 3. diagenesis - mixed uniform and random radii increment to obtain desired value of porosity.
Generated samples (red box) are validated a posteriori.
Method of numerical, periodic homogenisation:
problem: non-periodic geometry.
solution: additional layer of homogeneous material associated with
CT scan is naturally discretised (regular cubic mesh).
The influence of such discretization on the estimation of elastic moduli is given by [Garboczi and Day, 1995]:
M resolution
P0 searched value [Reconstruction method]
[Comparison of covariance functions] [Generated microstructure]
P(·) elastic moduli P(·) computed
Advanced Morphological Analysis of Sandstone
The starting point is CT scan of microstructure of Fontainebleau sandstone of size 256x256x 256 px, where 1 px = 5.01 microns.
Numerous types of morphological descriptors:
porosity, sizing (granulometry), covariance function, connectivity (tortuosity).
⌅(·) operator extracting percolated network morphological dilation
Xi binary image of i-th dissolution step
B cubic SE (3x3)
X0 binary image representing initial porous phase [Tomography - pores]
X porous phase x arbitrary point
~h translation vector
Covariance Function
P{·} probability Br structuring element of size r
/ erosion / dilation X Br = (X Br) Br X solid phase
Granulometry Function
|·| measure
' = 0.046 Summary:
'ef f = 0.029 percolated in all directions rmean 2 (17, 23) isotropy
Isotropic Percolated Network
[Evolution of covariance functions of generated samples (red) and real microstructure (blue)]
Numerical Dissolution by Morphological Dilation
Chemical dissolution of porous matrix is homogeneous at sample scale
[Egermann et al, 2006]. We investigate two different scenarii of dissolution:
[External layer]
[Roberts and Garboczi, 2002]
Increasing characteristic size Constant characteristic size
Darcy’s law:
Coupling:
K permeability µ dyn. viscosity Q flux
A surface area
p grad. of pressure L sample length
Percolated network dissolution Isotropic dissolution
Permeability - Elasticity Coupling
Percolated network dissolution Isotropic dissolution
fixed point method:
X
i= X
i 1B
P (K ) = 1 K
↵ K = µQL
pA P (M ) = P
0+ a
M
X
i= [⌅(X
i 1) B ] + X
0C (X, ~ h) = P n
x 2 X, x + ~ h 2 X o
c
layerklmn[i] = c
homklmn[i 1]
G
r(X ) = 1 | X B
r|
| X |
0 0.2 0.4 0.6 0.8 1
0 10 20 30 40 50 60
Volume fraction of the solid matrix
size of opening r [pixels]
spherical SE diamond SE
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45
0 10 20 30 40 50 60 70 80 90 100 110 120 130
C(X,h)
h [pixels]
Generated Samples - direction x Fontainebleau Sandstone - direction x φ2 dissolution step 0 φ2 dissolution step 1 φ2 dissolution step 2 φ2 dissolution step 3 φ2 dissolution step 4
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45
0 10 20 30 40 50 60 70 80 90 100 110 120 130
C(X,h)
h [pixels]
Generated Samples - direction x Fontainebleau Sandstone - direction x φ2 dissolution step 0 φ2 dissolution step 2 φ2 dissolution step 4 φ2 dissolution step 6
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
Normalized elastic moduli
Dissolution - induced porosity GS - k
- µ FS - k - µ Arns* - k - µ
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
Normalized elastic moduli
Dissolution - induced porosity GS - k
- µ FS - k - µ Arns* - k - µ
* Arns et al. 2002
0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0 2000 4000 6000 8000 10000 12000 14000 16000 18000
Normalized elastic moduli
Permeability K [mD]
GS - k (α = 12.13; β = 0.22) - µ (α = 9.23; β = 0.20) FS - k (α = 12.27; β = 0.22) - µ (α = 9.32; β = 0.21)
0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
0 5000 10000 15000 20000 25000 30000 35000 40000
Normalized elastic moduli
Permeability K [mD]
GS - k (α = 15.12; β = 0.22) - µ (α = 10.87; β = 0.20) FS - k (α = 16.57; β = 0.23) - µ (α = 11.85; β = 0.21) 0
0.01 0.02 0.03 0.04 0.05
0 10 20 30 40 50 60 70 80 90 100 110 120 130
Cov(X,h)
h [pixels]
GS - x FS - x φ2
0 0.002 0.004 0.006 0.008 0.01
0 10 20 30 40
0 0.005 0.01 0.015 0.02 0.025 0.03 0.035 0.04 0.045 0.05
0 15 30 45 60 75 90 105 120
Cov(X,h)
h [pixels]
X - direction Y - direction Z - direction φ2
0 0.002 0.004 0.006 0.008 0.01
0 15 30
K. Wojtacki
1,*, L. Daridon
1,2, Y. Monerie
1,21
Laboratoire de Mécanique et Génie Civil (LMGC), CNRS UMR 5508, Montpellier, France
2
Laboratoire de Micromécanique et Intégrité des Structures (MIST), UM, CNRS, IRSN, France
CHEMICAL DEGRADATION OF A NUMERICALLY GENERATED MATERIAL - APPLICATION FOR FONTAINEBLEAU SANDSTONE
* kajetan.wojtacki@umontpellier.fr