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Building a
    Pore Network Model from a
     Pore Space 3D Image to
         Precisely Predict
           Permeability


D. BERNARD, N. COMBARET, E. PLOUGONVEN,
J. LESSEUR
Institut de Chimie de la Matière Condensée de Bordeaux,
ICMCB-CNRS, Univ. Bordeaux, PESSAC
Availability of large high-resolution 3D images
Direct computation of the permeability
                          At the local scale


                                    
                               

                              Ae
From STOKES to DARCY        Closure problem
Direct computation of the permeability



     Numerical code




Pressure          Vx      Vy         Vz
Pores network model
Pores network model
Pores network model

Represent


   TOPOLOGY          Skeleton      Noise effects




   GEOMETRY             Local resistance
Skeletonisation
Pore space partitioning
PNM construction
Example
Local resistances computation
Example
Conclusions
Skeletonisation
Binary image

Homotopic thining
Skeletonisation
Skeletonization
Skeletonisation
Skeletonization
Skeletonisation
Filtering : morphological closing, majority filter, median filter, …
Problems:
              Modifies too many irrelevant pixels
              Does not remove all artefacts

 New solution: directly identify
 pixels causing artefacts in the
 skeleton

          0D, 1D, 2D




                          EP & DB, AWR, 34 (2011) 731–736
Skeletonisation
Pore space partitioning
Pore space partitioning
Pores identification
Pore space partitioning
Pores construction
Skeletonisation
Pore space partitioning
PNM construction
PNM construction
PNM construction
PNM construction
Skeletonisation
Pore space partitioning
PNM construction
Example
Example
Example
Example
Example
Example
Example
Skeletonisation
Pore space partitioning
PNM construction
Example
Local resistances computation
Local resistances computation
                                                                  j

    .v  0
   
   
    p   2 v  0
   
B.C. : v  0 on A fs

       M

      Q
       j 1
              ij   0



Cij 

     p.c dC    2 v.c dC  0
                Cij
                                   p H j   pH i   ij .Qij  0
     1                2 
Local resistances computation
Local resistances computation




                                0,636
                                0,722
Skeletonisation
Pore space partitioning
PNM construction
Example
Local resistances computation
Example
Example




500 x 500 x 500
 voxels of 5m
Example
PNM construction
Example
PNM construction
Example
PNM construction
Example
Local resistances computation
Example




DNM: 92.62 m2

PNM: 88.26 m2




  500 x 500 x 500
   voxels of 5m
Skeletonisation
Pore space partitioning
PNM construction
Example
Local resistances computation
Example
Conclusions
Conclusions

PNM based only on 3D geometry
Good comparison with DNM
Different examples are presently treated
Comparison with experimental data


Local resistances computation to be simplified
Full permeability tensor is considered

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Building a pore network model from a pore space 3D image to precisely predict permeability tensor