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Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
CONTROLLING FOLDS WITH AN
IMPLICIT MODELLING APPROACH
AND
RIGID ELEMENT METHOD FOR GEOLOGICAL
STRUCTURAL MODELLING
Gautier Laurent
Laurent Aillères
Lachlan Grose
Guillaume Caumon
Monash
GeoRessources
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
 Expert-driven approach
 Sparse Data
 Qualitative Models
Modelling Geological Structures
 The modeller’s approach:
• Honour data
• One state = current state
 The geologist’s approach:
• Geological scenario
• Multiple phases
Approaches to GeomodellingIntroduction
1/31
Data
(current state)
time
Geological structures
(current state) Geological scenario
 Tectonics / kinematics concepts
Need to reconcile these
two approaches
 Data-driven approach
 Lots of Data
 Quantitative Models
 Part I: Provide tools to implement interactive Deformation Events
 Part II: Better integrate Structural Data for Folding
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Interactive deformation tool
ReedPart I
2/31
Part I
-
Rigid Element Embedding Deformation
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Deformation algorithm for Geomodelling
ReedPart I
3/31
Our specifications:Usage:
 Physical Consistency: looks like natural
deformations
 Interactive: fast and handy
 Robustness: don’t break during computation
 Adapted Scale: don’t loose details but don’t
compute too finely
 Parsimony: limited number of parameters
Why?
1. Rely more on geologist interpretation
2. Allow easier automation
3. Ease meshing problems
4. And we don’t have enough information
anyway…
Editing
Forward modelling
Restoration
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Another world of deformation tools
 Computer Graphics:
• Physically-based deformable models
• Extensive literature with active research
• Eg. Adaptive space deformations based on rigid cells [Botsch et al, 2007]
 Transfer to Geosciences [Laurent, 2013]
ReedPart I
4/31
Eg. [Nealen et al., 2006]
Rigid
Element
Embedding
Deformation
eed
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Reed in Geosciences [Laurent, 2013]
 Using this interactive tool in Geoscience:
• Dynamic editing of Folding structures
ReedPart I
5/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
How does Reed work?
 Four main steps:
ReedPart I
6/31
Object to be deformed
Deformation tool
Reed
1: Encapsulation in
Rigid Elements
Cost
Function0 1
3: Deformation computation
= Optimisation of a cost function
4: Displacement
Interpolation
Deformed object
2: Define Boundary Conditions
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Cost function
 Neighbourhood constraint:
• Minimise difference of displacement
• Integrated over element’s volume
ReedPart I
7/31
Ri
Ti
Rj
Tj
x
Dij
ci cj
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Displacement interpolation
 The displacement of the rigid elements is
• Interpolated on the embedded objects
• Only once at the end (performance)
• Locate each point to deform
• Compute displacement for each element
• Combine linearly
ReedPart I
8/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
A more complete example [Laurent, 2013]
 Deformation history modelling (as in Noddy [Jessell and Valenta, 1996])
ReedPart I
9/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
A more complete example [Laurent, 2013]
ReedPart I
10/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
A more complete example [Laurent, 2013]
 Parameters:
• Shortening
• Axial surfaces
• Amplitude
ReedPart I
11/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
A more complete example [Laurent, 2013]
ReedPart I
12/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Reed Pros and Cons
ReedPart I
13/31
Cons:
• Some missing behaviours
(eg. No Poisson effect)
• No Faults…
Pros:
• Interative
• Space Deformation
• Robust to extreme deformation
• Good approximation of flexural
behaviour
until now!
[Molino et al., 2004]
Question: How to introduce faults in Reed?
 Any lead in Computer Graphics?
[O’Brien and Hodgins, 1999]
Not really
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
 Requirements:
• Being able to evaluate anywhere in 3D
 The “distance” to the fault
 The direction towards the fault
 Result:
Defining a cost function for faults
ReedPart I
14/31
f = 0
f = 1
f = -1 f = -2
f = 2
f
Init
i
i+1
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Implicit Folding
Implicit modelling
Part II
-
Modifying Implicit Methods
To Actually Model Folds
Part II
15/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Defining the problems
 Time:
• 1st event: S0 (stratigraphy)
• 2nd event: F1 (folding)
• … may have more  fold interference
 Current geometry =
result of complex (multi event) history
 Data/ Measurements:
• Bedding observation:
• Stratigraphy
• Position of a contact
• Orientation of a contact
• Other structural observations:
• Hinges and Limbs
• Axial surfaces (+Fold axis)
• Vergence
• Fold type (Similar/parallel)
• Opening, Cylindricity…
ProblemsPart II
16/31
[Hudleston and Treagus, 2010]
Where
Geomodelling
packages
stops.
What we are adding.
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Implicit Modelling overview
Stratigraphy  Data Control Points + Regularisation term
BasicsPart II
17/31
 Stratigraphic value
 Orientation
 Continuous values
 Gradient vary progressively
Stratigraphy
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Discrete Implicit Modelling overview
 Discretised Region of Interest  Mesh
 Stratigraphy = piecewise-linear scalar field
 How to take fold measurements into account?
 How to overcome “constant gradient” limitations?
 limits folding and promotes parallel fold style
BasicsPart II
18/31
Stratigraphy
x
x0
v0 x1
v1
x2
v2
f(x) = λi vi
f = T . v
Build a global
system of linear
equations
Solve to build the
scalar field
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Geological structures parameterisation
 How are geological structures taken into account?
• Faults:
• Described by structural parameters
• Centre, Azimuth, Dip, Slip…
• Locality alter the mesh  interpolation
• Fold:
• Result of the smoothing of data
 Not really controlled
 Proposal:
• Fold structure  additional fields:
• Axial surface field F1:
• Related (parallel) to foliation field S1
• Easier to measure (visible in the limbs)
• Relatively consistent over the whole area
• Fold Intensity field:
• Derived from vergence and S0 observation
• Quantitative version of the vergence
• Fold axis field P1:
• Vectorial field to impose non cylindricity
MethodPart II
19/31
Vergence: Hey,
Next antiform is this
way!
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Fold Interpolation Process
 Interpolate S1
 Analyse the vergence to infer the Fold Intensity field
 Infer gradient direction:
• Rotation around fold axis direction P1
 Interpolate S0
MethodPart II
20/31
S1
Fold intensity
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Fold parameter control
 Fold centre position
MethodPart II
With classic constraints
21/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Fold parameter control
 Fold centre position
 Inter-limb angle
MethodPart II
With classic constraints
22/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Fold parameter control
 Fold centre position
 Inter-limb angle
 Axial surface orientation
MethodPart II
With classic constraints
23/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Fold parameter control
 Fold centre position
 Inter-limb angle
 Axial surface orientation
 Wavelength
MethodPart II
With classic constraints
24/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Fold parameter control
 Fold centre position
 Inter-limb angle
 Axial surface orientation
 Wavelength
 Tightness
MethodPart II
With classic constraints
25/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Regularisation term
 Constant gradient (classic) Parallel Fold
 Similar Fold:
• Conservation:
• Normalisation:
MethodPart II
26/31
Z
X
X0
X1
f0
f1
f0X0 . f1 = 0- X1 .
fi = LXi .
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
What can we do with that?
 Actually simulate folds instead of smoothing stratigraphy.
 Eg. Somebody said this is not possible (yet):
• ie. Interpolator smooth the folds.
 But with our constraints:
 Need to infer fold parameter.
 Optimisation/simulation process instead of simple interpolation.
ResultPart II
27/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
What else can we do?
 Fold parameters simulation:
 To infer uncertainty related to structural parameters
ResultsPart II
28/31
Measurement-related uncertainty Structural uncertainty
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
What else can we do?
 Interference patterns:
• Fold is defined by scalar field
 Use deformed geometries as S1
 Produce a deformed fold
 Strategy:
 Model latest folds first
 Constrain the geometry Fn-1 based on Fn observations
ResultsPart II
29/31
S1 (deformed by F2) S0 (deformed by F1 and F2)
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Some 3D…
 The formulation is fully 3D so no problem to go in 3D
 Implementation in 3D packages to come soon (StructuralLab/Gocad)
ResultsPart II
30/31
Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014
Contributions:
 Tools to model 3D folded geometries:
• Take advantage of complete structural observations
• Time-aware approaches:
• Reed: simulate deformation sequence
• Implicit Folding: use latest events to constrain previous ones
• Take fully advantage of implicit approaches… and extend them.
Thank you for your attention.
 Any questions?
conclusionsConclusion
31/31

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Gautier Laurent - Implicit Modelling and volume deformation

  • 1. 0/31 Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 CONTROLLING FOLDS WITH AN IMPLICIT MODELLING APPROACH AND RIGID ELEMENT METHOD FOR GEOLOGICAL STRUCTURAL MODELLING Gautier Laurent Laurent Aillères Lachlan Grose Guillaume Caumon Monash GeoRessources
  • 2. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014  Expert-driven approach  Sparse Data  Qualitative Models Modelling Geological Structures  The modeller’s approach: • Honour data • One state = current state  The geologist’s approach: • Geological scenario • Multiple phases Approaches to GeomodellingIntroduction 1/31 Data (current state) time Geological structures (current state) Geological scenario  Tectonics / kinematics concepts Need to reconcile these two approaches  Data-driven approach  Lots of Data  Quantitative Models  Part I: Provide tools to implement interactive Deformation Events  Part II: Better integrate Structural Data for Folding
  • 3. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Interactive deformation tool ReedPart I 2/31 Part I - Rigid Element Embedding Deformation
  • 4. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Deformation algorithm for Geomodelling ReedPart I 3/31 Our specifications:Usage:  Physical Consistency: looks like natural deformations  Interactive: fast and handy  Robustness: don’t break during computation  Adapted Scale: don’t loose details but don’t compute too finely  Parsimony: limited number of parameters Why? 1. Rely more on geologist interpretation 2. Allow easier automation 3. Ease meshing problems 4. And we don’t have enough information anyway… Editing Forward modelling Restoration
  • 5. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Another world of deformation tools  Computer Graphics: • Physically-based deformable models • Extensive literature with active research • Eg. Adaptive space deformations based on rigid cells [Botsch et al, 2007]  Transfer to Geosciences [Laurent, 2013] ReedPart I 4/31 Eg. [Nealen et al., 2006] Rigid Element Embedding Deformation eed
  • 6. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Reed in Geosciences [Laurent, 2013]  Using this interactive tool in Geoscience: • Dynamic editing of Folding structures ReedPart I 5/31
  • 7. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 How does Reed work?  Four main steps: ReedPart I 6/31 Object to be deformed Deformation tool Reed 1: Encapsulation in Rigid Elements Cost Function0 1 3: Deformation computation = Optimisation of a cost function 4: Displacement Interpolation Deformed object 2: Define Boundary Conditions
  • 8. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Cost function  Neighbourhood constraint: • Minimise difference of displacement • Integrated over element’s volume ReedPart I 7/31 Ri Ti Rj Tj x Dij ci cj
  • 9. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Displacement interpolation  The displacement of the rigid elements is • Interpolated on the embedded objects • Only once at the end (performance) • Locate each point to deform • Compute displacement for each element • Combine linearly ReedPart I 8/31
  • 10. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 A more complete example [Laurent, 2013]  Deformation history modelling (as in Noddy [Jessell and Valenta, 1996]) ReedPart I 9/31
  • 11. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 A more complete example [Laurent, 2013] ReedPart I 10/31
  • 12. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 A more complete example [Laurent, 2013]  Parameters: • Shortening • Axial surfaces • Amplitude ReedPart I 11/31
  • 13. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 A more complete example [Laurent, 2013] ReedPart I 12/31
  • 14. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Reed Pros and Cons ReedPart I 13/31 Cons: • Some missing behaviours (eg. No Poisson effect) • No Faults… Pros: • Interative • Space Deformation • Robust to extreme deformation • Good approximation of flexural behaviour until now! [Molino et al., 2004] Question: How to introduce faults in Reed?  Any lead in Computer Graphics? [O’Brien and Hodgins, 1999] Not really
  • 15. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014  Requirements: • Being able to evaluate anywhere in 3D  The “distance” to the fault  The direction towards the fault  Result: Defining a cost function for faults ReedPart I 14/31 f = 0 f = 1 f = -1 f = -2 f = 2 f Init i i+1
  • 16. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Implicit Folding Implicit modelling Part II - Modifying Implicit Methods To Actually Model Folds Part II 15/31
  • 17. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Defining the problems  Time: • 1st event: S0 (stratigraphy) • 2nd event: F1 (folding) • … may have more  fold interference  Current geometry = result of complex (multi event) history  Data/ Measurements: • Bedding observation: • Stratigraphy • Position of a contact • Orientation of a contact • Other structural observations: • Hinges and Limbs • Axial surfaces (+Fold axis) • Vergence • Fold type (Similar/parallel) • Opening, Cylindricity… ProblemsPart II 16/31 [Hudleston and Treagus, 2010] Where Geomodelling packages stops. What we are adding.
  • 18. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Implicit Modelling overview Stratigraphy  Data Control Points + Regularisation term BasicsPart II 17/31  Stratigraphic value  Orientation  Continuous values  Gradient vary progressively Stratigraphy
  • 19. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Discrete Implicit Modelling overview  Discretised Region of Interest  Mesh  Stratigraphy = piecewise-linear scalar field  How to take fold measurements into account?  How to overcome “constant gradient” limitations?  limits folding and promotes parallel fold style BasicsPart II 18/31 Stratigraphy x x0 v0 x1 v1 x2 v2 f(x) = λi vi f = T . v Build a global system of linear equations Solve to build the scalar field
  • 20. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Geological structures parameterisation  How are geological structures taken into account? • Faults: • Described by structural parameters • Centre, Azimuth, Dip, Slip… • Locality alter the mesh  interpolation • Fold: • Result of the smoothing of data  Not really controlled  Proposal: • Fold structure  additional fields: • Axial surface field F1: • Related (parallel) to foliation field S1 • Easier to measure (visible in the limbs) • Relatively consistent over the whole area • Fold Intensity field: • Derived from vergence and S0 observation • Quantitative version of the vergence • Fold axis field P1: • Vectorial field to impose non cylindricity MethodPart II 19/31 Vergence: Hey, Next antiform is this way!
  • 21. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Fold Interpolation Process  Interpolate S1  Analyse the vergence to infer the Fold Intensity field  Infer gradient direction: • Rotation around fold axis direction P1  Interpolate S0 MethodPart II 20/31 S1 Fold intensity
  • 22. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Fold parameter control  Fold centre position MethodPart II With classic constraints 21/31
  • 23. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Fold parameter control  Fold centre position  Inter-limb angle MethodPart II With classic constraints 22/31
  • 24. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Fold parameter control  Fold centre position  Inter-limb angle  Axial surface orientation MethodPart II With classic constraints 23/31
  • 25. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Fold parameter control  Fold centre position  Inter-limb angle  Axial surface orientation  Wavelength MethodPart II With classic constraints 24/31
  • 26. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Fold parameter control  Fold centre position  Inter-limb angle  Axial surface orientation  Wavelength  Tightness MethodPart II With classic constraints 25/31
  • 27. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Regularisation term  Constant gradient (classic) Parallel Fold  Similar Fold: • Conservation: • Normalisation: MethodPart II 26/31 Z X X0 X1 f0 f1 f0X0 . f1 = 0- X1 . fi = LXi .
  • 28. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 What can we do with that?  Actually simulate folds instead of smoothing stratigraphy.  Eg. Somebody said this is not possible (yet): • ie. Interpolator smooth the folds.  But with our constraints:  Need to infer fold parameter.  Optimisation/simulation process instead of simple interpolation. ResultPart II 27/31
  • 29. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 What else can we do?  Fold parameters simulation:  To infer uncertainty related to structural parameters ResultsPart II 28/31 Measurement-related uncertainty Structural uncertainty
  • 30. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 What else can we do?  Interference patterns: • Fold is defined by scalar field  Use deformed geometries as S1  Produce a deformed fold  Strategy:  Model latest folds first  Constrain the geometry Fn-1 based on Fn observations ResultsPart II 29/31 S1 (deformed by F2) S0 (deformed by F1 and F2)
  • 31. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Some 3D…  The formulation is fully 3D so no problem to go in 3D  Implementation in 3D packages to come soon (StructuralLab/Gocad) ResultsPart II 30/31
  • 32. Dr Gautier Laurent 3D Interest Group Meeting 10th June 2014 Contributions:  Tools to model 3D folded geometries: • Take advantage of complete structural observations • Time-aware approaches: • Reed: simulate deformation sequence • Implicit Folding: use latest events to constrain previous ones • Take fully advantage of implicit approaches… and extend them. Thank you for your attention.  Any questions? conclusionsConclusion 31/31

Editor's Notes

  • #2: - merci au jury -> évaluer mes travaux de thèse - portent sur : (voir titre)