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On the power of virtual
experimentation in MT2.0:
a VFORM-xSteels outlook
Sam Coppieters, A. Gil Andrade-Campos et al.
MatchID Global User Meeting
On the power of virtual experimentation in MT2.0 : a
VFORM outlook
22 February2023 | Southampton, UK
Outline
• The vForm-xSteels project;
• The power of virtual experimentation in MT2.0
 Virtual experimentation (DVT)
 DVT vs. Actual Experiment
 CMAT: stress integration algorithms
• The power of virtual experimentation in ML approaches
 The methodology
 The case study of the Biaxial cruciform test
 The virtual experiments data-base
 Robustness analysis
Team Work: vForm-xSteels
Just some faces
but many more
are contributing!
VFORM-xSteels
Toward virtual forming and design:
Thermomechanical characterization of advanced
high strength steels through full-field
measurements and a single designed test
Call: RFCS-2019
Instrument: (RP / PDP / AM)
Start date: 01/06/2020
End date: 31/05/2024
Budget: €1,496,357.52
Type of Action: RFCS-RPJ
Number: 888153
Duration: 48 months
GA based on the: RFCS MGA — Multi - 2.null
Estimated Project Cost: €2,521,389.20
Requested EU Contribution: €1,496,357.52
This project has received funding from the Research Fund for Coal and Steel under grant agreement No 888153
Problem
Decades ago…
Problem
Today…
Problem and need
Increase information &
reduce time in material testing
Realistic simulations and material
behavior reproduction
Faster and accurate
development & production
Problem
Limited quality and amount of data
"The data we have is provided by suppliers. In some
cases it is limited."
André Ferreira
Designer Projectist @ OLI Oliveira e Irmãos
The new paradigm of
Material Testing 2.0
(previous seminar from F.
Pierron)
Problem
Error in material behavior virtual
predictions
"It would be important to have a service that could identify and
provide these data to companies in due time."
Mário Marques
Country Manager Iberia @ Autoform
Project goal
Nowadays, the use of numerical simulation in general and particularly finite element analysis (FEA) has
become a mandatory step (…) However, todays methods to characterize the materials through constitutive
models, including damage, and their parameters are expensive and not robust.
The main goal of the project VForm-XSteels is to develop an
efficient and accurate methodology for material characterization
and determining the material parameters of thermomechanical
models, from a dedicated single test that involve non-homogeneous
temperature and strain fields. Indeed, (…) A database and online library with calibrated
material constitutive models, particularly for AHSS, is also developed.
The benefits of the proposed methodology and consequent implemented numerical tool developed within
this project are (…) cost and time reduction in the overall development process are also benefits of this
proposal.
Project goal
Project goal and technology
IP test Optical
technology
Optimization
algorithms
Flexible
Accurate
Robust
Fast
Innovative ​experimental
test​ (1 000+ points)
Advanced Data analytics
to calibrate the material
models
WP3 - Design of a novel test using an integrated topology-shape
optimisation methodology and a thermo-mechanical indicator
• Mafalda Gonçalves, Thibault Barret, Antonio Andrade-Campos, Sandrine Thuillier
• Design by topology optimisation of a heterogeneous test to calibrate a viscoplastic model
• First from homogeneous tests (reference), then heterogenous tests Future work: thermal dependence to enhance the strain rate sensitivity
• KPI to quantify the
heterogeneity level: stress and
strain fields, stress triaxiality
and Lode parameter, rotation
angle, identifiability metrics,
DIC errors
• A heterogeneous test to
calibrate a viscoplastic model
• Synthetic images generated
with MatchID
• Investigation of the viscoplastic contribution
from hydraulic bulge test, DP600, thickness
0.8 mm
• Strain rate ranging from 10-3 up to 80 s-1
• Hydraulic bulge test, in quasi-static and
dynamic conditions (Hopkinson bars), strain
field measure using MatchID software
VISCOPLASTICITY HETEROGENEITY
Design of new heterogeneous specimens
Linear analysis; id = 0.0359 Nonlinear geometric
analysis; id = 0.0190
Nonlinear material and
geometric analysis; id = 0.0215
[6]
[7]
Thermomechanical heterogeneous test
Objective: developing a test with a combined
heterogenous temperature and strain field using a
Gleeble system
Multiphysics – coupled thermal-electrical-structural analysis
Select the best specimen and set-up
Thermomechanical heterogeneous test
Example of numerical results for one configuration
Temperature distribution
Plastic strain distribution
Testing zone
Status of UMAT structure in the VFM module and
integration with UMMDP/Fortran communication
D4.1 A large set of material user routines validated for commercial FEA software:
UMMDP has Fortran legacy (old Fortran)
Intermediate HUB
Status of Implementation of constitutive models in
UMAT routines
D4.1 A large set of material user routines validated for commercial FEA software
• Fully implemented for stress reconstruction
• Integrated within the Virtual Fields Module
• Youtube Tutorial XXXVII
• Stresses returned in global and material frame
• Fully parallelized
• Available in MatchID 2022.2
• Demo
Constitutive model: both plasticity and damage
behaviour depend on stress triaxiality and Lode angle!
Plasticity and damage behaviour
The power of virtual
experimentation (DVT) in MT2.0
FEDEF
Digital Virtual Twin (DVT)
Lava, P., Cooreman, S., Coppieters, S., De Strycker, M., Debruyne, D. (2009).
Assessment of measuring errors in DIC using deformation fields generated by plastic FEA.
Optics and lasers in engineering, 47 (7), 747-753.
Digital Virtual Twin (DVT)
FEMU platform
Calibrated material model
3D plastic anisotropy though FEMU and DIC
Denys, K., Coppieters, S., Seefeldt, M., Debruyne, D. (2016). Multi-DIC setup for the identification of a 3D
anisotropic yield surface of thick high strength steel using a double perforated specimen. Mechanics of Materials,
100, 96-108.
DVT without FEDEF
1.1
1.2
1.3
1.4
1.5
1.6
1.7
1.8
1.9
2
0 2 4 6
Anisotropic
parameter
Iteration
N
M
L
ref
0.47
0.48
0.49
0.5
0.51
0.52
0.53
0.54
0 1 2 3 4 5 6
Anisotropic
parameter
Iteration
F
H
ref
DVT with FEDEF: two stereo DIC setups
Front data Side data
DVT with FEDEF: two stereo DIC setups
1.1
1.2
1.3
1.4
1.5
1.6
1.7
1.8
1.9
2
0 2 4 6
Anisotropic
parameter
Iteration
N
M
L
ref
0.47
0.48
0.49
0.5
0.51
0.52
0.53
0.54
0 1 2 3 4 5 6
Anisotropic
parameter
Iteration
F
H
ref
Actual experiments
Stereo 1: through-
thickness surface
Stereo 2: front
surface
Actual experiments: multi cam module
DVT vs. Actual Experiments
Virtual DIC data
2
C(θ)=
FEMU
Digital virtual
Twins
Initial Mesh
Load-
displacement
Numerical
simulations
Yld2000-2d (DH)
Real speckle pattern
Yld2000-2d
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
1.15
1.2
1.25
0 0.05 0.1 0.15 0.2 0.25 0.3
a1
a2
a3
a4
a5
a6
a7
a8
Prediction of what we will measure experimentally
DVT vs. Actual Experiments
Stress reconstruction (CMAT/AppStore)
IMPLICIT (SAMSTRESS)
Stress reconstruction (CMAT/AppStore)
EXPLICIT (MIRKOSTRESS)
Prof. M. Halilovič
The power of experimentation
in data-driven approaches
Numerical data meets real data through virtual experimentation
What’s the fuss about AI & data-driven approaches?
• Inverse methodologies for full-field measurements
Data-driven and Machine Learning methods
characterization by Dall-E
What’s the fuss about AI & data-driven approaches?
• Inverse methodologies for full-field measurements
Dall-E:
Full-field deformation measurement tools
designed for a complete engineering
analysis
MatchID global
user meeting
pencil drawing of
a finite element
analysis
• Builds the inverse problem model as non-linear
regressor (using data)
• Build the inverse model LLM and finds directly the
parameters solving A = LLM(εexp,Fexp).
• The inverse model LLM is boundary conditions’
dependent
• High computational cost for the creation of a suitable
samples’ database (direct problem database)
• A simulation software is required
Inverse methodologies for full-field measurements
General goal
for parameter identification
Data-driven and Machine Learning (ML) methods
The objective function can be written as
where
The objective function can be written as
Procedure for material parameter identification
Constitutive parameters Input Space
σ0 [MPa] 120-300
n 0.1-0.3
K [MPa] 280-700
R0 0.6-2.5
R45 0.6-2.5
R90 0.6-2.5
The case of the biaxial cruciform test
ML approach for the Cruciform test with swift’s hardening and Hill’s anisotropy
Cruciform tensile test
Total displacement ux=uy = 2 mm
405 CPS4R elements (reduced integration)
Anisotropic plastic behaviour (Hill 1948)
Latin Hypercube Sampling – 2000 simul.
R = 7 mm
30
mm
0x RD
0y TD
R = 2.5 mm
15 mm
ux = 2 mm
Symmetry boundary conditons
(uy = 0 mm)
Symmetry
boundary
conditons
(u
x
=
0
mm)
uy = 2 mm
Biaxial Cruciform test
XGBoost
Model
σ0
n
K
Strain xy
(20 time steps *
405 features per time step)
Strain yy
(20 time steps *
405 features per time step)
Strain xx
(20 time steps *
405 features per time step)
Total force 0x
(20 time steps *
1 feature per time step)
Total force 0y
(20 time steps *
1 feature per time step)
R0
R45
R90
24340 features 6 Outputs
In/out features definition for the ML inverse model
However…
Features importance analysis: SHAP
• Results
• ML approach - Cruciform test
σ0
n K
Features importance analysis: SHAP
46
R0 R45 R90
XGBoost
Model
σ0
n
K
Strain xy
(20 time steps *
114 features per time step)
Strain yy
(20 time steps *
114 features per time step)
Strain xx
(20 time steps *
114 features per time step)
Total force 0x
(20 time steps *
1 feature per time step)
Total force 0y
(20 time steps *
1 feature per time step)
R0
R45
R90
6280 features 6 Outputs
In/out features definition for the ML inverse model
Becoming …
Testing result
50
σ0 n K
R0 R45 R90
Test – 200 samples
2000 samples were generated, 1800 for training and 200 for testing
DIC levelling: the power of digital virtual testing (DVT)
DIC levelling: the power of DVT
Comparison of the displacement
magnitude in the cruciform test,
between FEA (left) and virtual
experiments (right).
Digital virtual tests (DVT) database
ML database for training
ML architecture
Synthetic
image
generator
FEA program
(e.g. Abaqus)
?
?
?
?
?
Each sample was divided into 6455 subsets. In each subset, the location in
pixels and the strains εxx, εyy, and εxy were recorded.
2000 samples were generated, 1800 for training and 200 for testing.
Synthetic
image
generator
FEA program
(e.g. Abaqus)
?
?
?
?
?
Digital virtual tests (DVT) database
… resulting in more than
400k features for each
sample.
To validate the models,
2000 images were
generated (1800 for training
and 200 for test).
only the regions of interest found with the SHAP values
were used to train the models (just 10% of the data)
number of
features was too
large
impossible to train
the model with
every feature
Digital virtual tests (DVT) database
Performance evaluation
σ0 n K
R0 R45 R90
Predictive
Simulated
R2=0.9980 R2=0.9610
R2=0.9779
R2=0.9779
R2=0.9923 R2=0.9925
Predicted (vertical axis) vs. real (horizontal axis) values of the constitutive
parameters
2000 samples were generated, 1800 for training and 200 for testing
DVT database results
• Results: virtual experiments database
• ML approach - Cruciform test
R2 and MAE for Abaqus vs MatchID database
The results are
still robust
even with DIC
noise/errors!
Robustness Analysis: material rotation
0
2
4
6
8
10
12
14
16
18
0 5 10 15 20 25 30 35 40 45
Relative
error
(%)
Rotation ( )
Y0
K
n
r0
r45
r90
Relative error in the
prediction of the
material parameters as
a function of the
rotation of the material
axes w.r.t. the global
axes system.
In this context, one of the samples
from the testing set was chosen
(Y0=172 MPa, n=0.16; K=486 MPa;
r0=2.38; r45=1.8; r90=1.06) and the
orientation of the material axes was
varied w.r.t. the global axes system
0xy
P.A. Prates, J. Henriques, J. Pinto, N. Bastos and A. Andrade-Campos, Coupling machine learning
and synthetic image DIC-based techniques for the calibration of elastoplastic constitutive
models, Esaform conference 2023
On the power of virtual
experimentation in MT2.0:
a VFORM-xSteels outlook
Sam Coppieters, A. Gil Andrade-Campos et al.
MatchID Global User Meeting
On the power of virtual experimentation in MT2.0 : a
VFORM outlook
22 February2023 | Southampton, UK

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On the power of virtual experimentation in MT2.0: a VFORM-xSteels outlook

  • 1. On the power of virtual experimentation in MT2.0: a VFORM-xSteels outlook Sam Coppieters, A. Gil Andrade-Campos et al. MatchID Global User Meeting On the power of virtual experimentation in MT2.0 : a VFORM outlook 22 February2023 | Southampton, UK
  • 2. Outline • The vForm-xSteels project; • The power of virtual experimentation in MT2.0  Virtual experimentation (DVT)  DVT vs. Actual Experiment  CMAT: stress integration algorithms • The power of virtual experimentation in ML approaches  The methodology  The case study of the Biaxial cruciform test  The virtual experiments data-base  Robustness analysis
  • 3. Team Work: vForm-xSteels Just some faces but many more are contributing!
  • 5. Toward virtual forming and design: Thermomechanical characterization of advanced high strength steels through full-field measurements and a single designed test Call: RFCS-2019 Instrument: (RP / PDP / AM) Start date: 01/06/2020 End date: 31/05/2024 Budget: €1,496,357.52 Type of Action: RFCS-RPJ Number: 888153 Duration: 48 months GA based on the: RFCS MGA — Multi - 2.null Estimated Project Cost: €2,521,389.20 Requested EU Contribution: €1,496,357.52 This project has received funding from the Research Fund for Coal and Steel under grant agreement No 888153
  • 8. Problem and need Increase information & reduce time in material testing Realistic simulations and material behavior reproduction Faster and accurate development & production
  • 9. Problem Limited quality and amount of data "The data we have is provided by suppliers. In some cases it is limited." André Ferreira Designer Projectist @ OLI Oliveira e Irmãos The new paradigm of Material Testing 2.0 (previous seminar from F. Pierron)
  • 10. Problem Error in material behavior virtual predictions "It would be important to have a service that could identify and provide these data to companies in due time." Mário Marques Country Manager Iberia @ Autoform
  • 11. Project goal Nowadays, the use of numerical simulation in general and particularly finite element analysis (FEA) has become a mandatory step (…) However, todays methods to characterize the materials through constitutive models, including damage, and their parameters are expensive and not robust. The main goal of the project VForm-XSteels is to develop an efficient and accurate methodology for material characterization and determining the material parameters of thermomechanical models, from a dedicated single test that involve non-homogeneous temperature and strain fields. Indeed, (…) A database and online library with calibrated material constitutive models, particularly for AHSS, is also developed. The benefits of the proposed methodology and consequent implemented numerical tool developed within this project are (…) cost and time reduction in the overall development process are also benefits of this proposal.
  • 13. Project goal and technology IP test Optical technology Optimization algorithms Flexible Accurate Robust Fast Innovative ​experimental test​ (1 000+ points) Advanced Data analytics to calibrate the material models
  • 14. WP3 - Design of a novel test using an integrated topology-shape optimisation methodology and a thermo-mechanical indicator • Mafalda Gonçalves, Thibault Barret, Antonio Andrade-Campos, Sandrine Thuillier • Design by topology optimisation of a heterogeneous test to calibrate a viscoplastic model • First from homogeneous tests (reference), then heterogenous tests Future work: thermal dependence to enhance the strain rate sensitivity • KPI to quantify the heterogeneity level: stress and strain fields, stress triaxiality and Lode parameter, rotation angle, identifiability metrics, DIC errors • A heterogeneous test to calibrate a viscoplastic model • Synthetic images generated with MatchID • Investigation of the viscoplastic contribution from hydraulic bulge test, DP600, thickness 0.8 mm • Strain rate ranging from 10-3 up to 80 s-1 • Hydraulic bulge test, in quasi-static and dynamic conditions (Hopkinson bars), strain field measure using MatchID software VISCOPLASTICITY HETEROGENEITY
  • 15. Design of new heterogeneous specimens Linear analysis; id = 0.0359 Nonlinear geometric analysis; id = 0.0190 Nonlinear material and geometric analysis; id = 0.0215 [6] [7]
  • 16. Thermomechanical heterogeneous test Objective: developing a test with a combined heterogenous temperature and strain field using a Gleeble system Multiphysics – coupled thermal-electrical-structural analysis Select the best specimen and set-up
  • 17. Thermomechanical heterogeneous test Example of numerical results for one configuration Temperature distribution Plastic strain distribution Testing zone
  • 18. Status of UMAT structure in the VFM module and integration with UMMDP/Fortran communication D4.1 A large set of material user routines validated for commercial FEA software: UMMDP has Fortran legacy (old Fortran) Intermediate HUB
  • 19. Status of Implementation of constitutive models in UMAT routines D4.1 A large set of material user routines validated for commercial FEA software • Fully implemented for stress reconstruction • Integrated within the Virtual Fields Module • Youtube Tutorial XXXVII • Stresses returned in global and material frame • Fully parallelized • Available in MatchID 2022.2 • Demo
  • 20. Constitutive model: both plasticity and damage behaviour depend on stress triaxiality and Lode angle! Plasticity and damage behaviour
  • 21. The power of virtual experimentation (DVT) in MT2.0
  • 22. FEDEF
  • 23. Digital Virtual Twin (DVT) Lava, P., Cooreman, S., Coppieters, S., De Strycker, M., Debruyne, D. (2009). Assessment of measuring errors in DIC using deformation fields generated by plastic FEA. Optics and lasers in engineering, 47 (7), 747-753.
  • 24. Digital Virtual Twin (DVT) FEMU platform Calibrated material model
  • 25. 3D plastic anisotropy though FEMU and DIC Denys, K., Coppieters, S., Seefeldt, M., Debruyne, D. (2016). Multi-DIC setup for the identification of a 3D anisotropic yield surface of thick high strength steel using a double perforated specimen. Mechanics of Materials, 100, 96-108.
  • 26. DVT without FEDEF 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2 0 2 4 6 Anisotropic parameter Iteration N M L ref 0.47 0.48 0.49 0.5 0.51 0.52 0.53 0.54 0 1 2 3 4 5 6 Anisotropic parameter Iteration F H ref
  • 27. DVT with FEDEF: two stereo DIC setups Front data Side data
  • 28. DVT with FEDEF: two stereo DIC setups 1.1 1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2 0 2 4 6 Anisotropic parameter Iteration N M L ref 0.47 0.48 0.49 0.5 0.51 0.52 0.53 0.54 0 1 2 3 4 5 6 Anisotropic parameter Iteration F H ref
  • 29. Actual experiments Stereo 1: through- thickness surface Stereo 2: front surface
  • 31. DVT vs. Actual Experiments Virtual DIC data 2 C(θ)= FEMU Digital virtual Twins Initial Mesh Load- displacement Numerical simulations Yld2000-2d (DH) Real speckle pattern Yld2000-2d 0.75 0.8 0.85 0.9 0.95 1 1.05 1.1 1.15 1.2 1.25 0 0.05 0.1 0.15 0.2 0.25 0.3 a1 a2 a3 a4 a5 a6 a7 a8 Prediction of what we will measure experimentally
  • 32. DVT vs. Actual Experiments
  • 34. Stress reconstruction (CMAT/AppStore) EXPLICIT (MIRKOSTRESS) Prof. M. Halilovič
  • 35. The power of experimentation in data-driven approaches Numerical data meets real data through virtual experimentation
  • 36. What’s the fuss about AI & data-driven approaches? • Inverse methodologies for full-field measurements Data-driven and Machine Learning methods characterization by Dall-E
  • 37. What’s the fuss about AI & data-driven approaches? • Inverse methodologies for full-field measurements Dall-E: Full-field deformation measurement tools designed for a complete engineering analysis MatchID global user meeting pencil drawing of a finite element analysis
  • 38. • Builds the inverse problem model as non-linear regressor (using data) • Build the inverse model LLM and finds directly the parameters solving A = LLM(εexp,Fexp). • The inverse model LLM is boundary conditions’ dependent • High computational cost for the creation of a suitable samples’ database (direct problem database) • A simulation software is required Inverse methodologies for full-field measurements General goal for parameter identification Data-driven and Machine Learning (ML) methods The objective function can be written as where
  • 39. The objective function can be written as Procedure for material parameter identification
  • 40. Constitutive parameters Input Space σ0 [MPa] 120-300 n 0.1-0.3 K [MPa] 280-700 R0 0.6-2.5 R45 0.6-2.5 R90 0.6-2.5 The case of the biaxial cruciform test ML approach for the Cruciform test with swift’s hardening and Hill’s anisotropy Cruciform tensile test Total displacement ux=uy = 2 mm 405 CPS4R elements (reduced integration) Anisotropic plastic behaviour (Hill 1948) Latin Hypercube Sampling – 2000 simul. R = 7 mm 30 mm 0x RD 0y TD R = 2.5 mm 15 mm ux = 2 mm Symmetry boundary conditons (uy = 0 mm) Symmetry boundary conditons (u x = 0 mm) uy = 2 mm
  • 42. XGBoost Model σ0 n K Strain xy (20 time steps * 405 features per time step) Strain yy (20 time steps * 405 features per time step) Strain xx (20 time steps * 405 features per time step) Total force 0x (20 time steps * 1 feature per time step) Total force 0y (20 time steps * 1 feature per time step) R0 R45 R90 24340 features 6 Outputs In/out features definition for the ML inverse model However…
  • 43. Features importance analysis: SHAP • Results • ML approach - Cruciform test σ0 n K
  • 44. Features importance analysis: SHAP 46 R0 R45 R90
  • 45. XGBoost Model σ0 n K Strain xy (20 time steps * 114 features per time step) Strain yy (20 time steps * 114 features per time step) Strain xx (20 time steps * 114 features per time step) Total force 0x (20 time steps * 1 feature per time step) Total force 0y (20 time steps * 1 feature per time step) R0 R45 R90 6280 features 6 Outputs In/out features definition for the ML inverse model Becoming …
  • 46. Testing result 50 σ0 n K R0 R45 R90 Test – 200 samples 2000 samples were generated, 1800 for training and 200 for testing
  • 47. DIC levelling: the power of digital virtual testing (DVT)
  • 48. DIC levelling: the power of DVT Comparison of the displacement magnitude in the cruciform test, between FEA (left) and virtual experiments (right).
  • 49. Digital virtual tests (DVT) database ML database for training ML architecture Synthetic image generator FEA program (e.g. Abaqus) ? ? ? ? ? Each sample was divided into 6455 subsets. In each subset, the location in pixels and the strains εxx, εyy, and εxy were recorded. 2000 samples were generated, 1800 for training and 200 for testing.
  • 51. … resulting in more than 400k features for each sample. To validate the models, 2000 images were generated (1800 for training and 200 for test). only the regions of interest found with the SHAP values were used to train the models (just 10% of the data) number of features was too large impossible to train the model with every feature Digital virtual tests (DVT) database
  • 52. Performance evaluation σ0 n K R0 R45 R90 Predictive Simulated R2=0.9980 R2=0.9610 R2=0.9779 R2=0.9779 R2=0.9923 R2=0.9925 Predicted (vertical axis) vs. real (horizontal axis) values of the constitutive parameters 2000 samples were generated, 1800 for training and 200 for testing
  • 53. DVT database results • Results: virtual experiments database • ML approach - Cruciform test R2 and MAE for Abaqus vs MatchID database The results are still robust even with DIC noise/errors!
  • 54. Robustness Analysis: material rotation 0 2 4 6 8 10 12 14 16 18 0 5 10 15 20 25 30 35 40 45 Relative error (%) Rotation ( ) Y0 K n r0 r45 r90 Relative error in the prediction of the material parameters as a function of the rotation of the material axes w.r.t. the global axes system. In this context, one of the samples from the testing set was chosen (Y0=172 MPa, n=0.16; K=486 MPa; r0=2.38; r45=1.8; r90=1.06) and the orientation of the material axes was varied w.r.t. the global axes system 0xy P.A. Prates, J. Henriques, J. Pinto, N. Bastos and A. Andrade-Campos, Coupling machine learning and synthetic image DIC-based techniques for the calibration of elastoplastic constitutive models, Esaform conference 2023
  • 55. On the power of virtual experimentation in MT2.0: a VFORM-xSteels outlook Sam Coppieters, A. Gil Andrade-Campos et al. MatchID Global User Meeting On the power of virtual experimentation in MT2.0 : a VFORM outlook 22 February2023 | Southampton, UK

Editor's Notes

  1. Decades ago, when designing engineering structures, such as bridges, planes and automobiles, the development required many engineers and time.
  2. Today, everything is done on the computer, using simulation tools, reducing delivering time and resources.  However, these simulations are only as good as the data & modelling they use.
  3. We need to increase the speed and accuracy of development and production. However, we need realistic engineering simulations, which needs accurate material behaviour reproduction that is only obtained with sophisticated and complex models! However, these models required full material knowledge, that is cost and time consuming.
  4. You know how these classical tests work, today. There are many ways of testing the materials. As an example, the material is stretched until it breaks providing a single or few data points in time. Here, the dots represent the data points. Several different tests are required to fairly characterize the material behaviour. It is not only a matter of quantity but also quality. This confirmed limited data (obtained from such procedures) is not enough to make the sophisticated models work… Resulting….
  5. Resulting… in errors in material behaviour predictions. Therefore, the need for a solution was easily confirmed by software users in the field.
  6. This vForm-xSteels project brings a solution… The main goal of the project VForm-XSteels is to develop an accurate methodology for material characterization and determining the material parameters of thermomechanical models, from a dedicated single test that involve non-homogeneous temperature and strain fields. A database and online library with calibrated material constitutive models, particularly for AHSS, is also developed.
  7. we are designing a new test with a unique shape that, when stretched and using optical technology, generates more than 1 000 data points from a single test. This data is processed using optimization algorithms and data analytics, providing a fast solution, accurate and robust technology, flexible for a wide range of steels. This is something that no others have yet provided.
  8. Cruciform test Swift Law + Hill’48
  9. Cruciform test Swift Law + Hill’48
  10. As observed in the previous case study, σ 0 and K depend almost exclusively on the initial and last force, respectively.
  11. Only a few elements located at specific regions of the cruciform sample are important to predict R0, R45 and R90. R0, R45 and R90 also use only a tiny region of the cruciform to obtain excellent results. Each parameter needs just up to 50 features to obtain a model with almost the same precision as the one with every parameter (6020).
  12. Results with 100 best features As good as obtained with every feature
  13. Results keep getting better with more training samples
  14. Simulated vs Predicted Good results!
  15. Since the number of features was too large, it was impossible to train the model with every feature. To solve this problem, only the regions of interest found with the SHAP values were used to train the models (just 10% of the information is used to train each parameter). Better results can be expected using more information, but …
  16. Since the number of features was too large, it was impossible to train the model with every feature. To solve this problem, only the regions of interest found with the SHAP values were used to train the models (just 10% of the information is used to train each parameter). Better results can be expected using more information, but they are still great and can be compared with the Abaqus database using the same number of samples. Another way to improve the results would be to use the same number of samples used before to train the models presented above.
  17. Since the number of features was too large, it was impossible to train the model with every feature. To solve this problem, only the regions of interest found with the SHAP values were used to train the models (just 10% of the information is used to train each parameter). Better results can be expected using more information, but they are still great and can be compared with the Abaqus database using the same number of samples. Another way to improve the results would be to use the same number of samples used before to train the models presented above.
  18. shows the relative error in the prediction of each material parameter, for rotations of the material axes ranging between 0º and 10º w.r.t. the global axes system (the 0º case is taken as reference for calculating the relative error in predictions); this figure also includes an extreme case of 45º. In general, the parameter predictions remain robust regarding possible sample misalignments in-between 0º and 10º; in this interval, the maximum variation of the relative error occurs for parameter r0 (about 2.65%). This preliminary robustness analysis suggests that sample misalignments do not significantly influence the predictive performance of the ML model, regardless of the overall quality of predictions obtained for each parameter (poor quality for parameters n, r45 and Y0, which requires careful analysis to assess the cause).