1) The document describes research to independently validate a method for designing generic specimen geometries that optimize identification of plastic anisotropy parameters through inverse modeling.
2) Specimen designs were optimized using an Indicator-IT criteria and shape optimization algorithm. The resulting designs were then validated via identifiability analysis and finite element model updating.
3) Preliminary results found that the optimized specimens had higher Indicator-IT values, better identifiability indices, and allowed for more accurate identification of anisotropic plasticity parameters compared to initial specimen designs.
Identification of anisotropic yield functions using an information-rich tensi...vformxsteels
Yi Zhang1, António Andrade-Campos2, Sam Coppieters1
1 Department of Materials Engineering, KU Leuven
2 Department of Mechanical Engineering, University of Aveiro, 3810-193
Aveiro, Portugal
Molecular dynamics (MD) simulations were carried out with a three-body Tersoff potential force field to predict the transversely isotropic elastic properties of pristine and defected BNNTs. This is accomplished by imposing uniaxial tension, twisting moment, in-aplane shear and in-plane biaxial tension to the BNNTs. Effects of various factors such as chirality and diameter of BNNTs, vacancy concentration, and distribution of vacancy pores along the length and circumference of BNNTs were critically examined. Our study reveals that the elastic coefficients of BNNTs decrease as their diameter increase, except axial Young’s modulus. Young’s modulus of BNNT increases with the diameter and reaches its maximum value when the tube diameter is ∼14 Å and then it starts decreasing. We also found that the axial Young’s modulus of a BNNT increases as its aspect ratio increases and stabilizes at a particular value of aspect ratio (L/D ∼ 15). The vacancies greatly affect the elastic properties of BNNTs; for instance, the vacancy concentration of 2% in (10, 10) BNNT reduce its axial Young’s, shear, plane strain bulk and in-plane shear moduli by 14%, 25%, 14% and 18%, respectively. Furthermore, we studied the electronic properties of pristine and defective BNNTs under four transversely isotropic loading conditions using the strain effective method. The results reveal that the electronic properties of BNNTs can be altered via different routes: loadings conditions, diameter and vacancy concentration. Our fundamental study highlights the critical role played by vacancy defected BNNTs in determining their elastic and electronic properties as they are vastly being used in multifarious applications such as nano-electronic devices and reinforcements in multifunctional nanocomposites
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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
Identification of anisotropic yield functions using an information-rich tensi...vformxsteels
Yi Zhang1, António Andrade-Campos2, Sam Coppieters1
1 Department of Materials Engineering, KU Leuven
2 Department of Mechanical Engineering, University of Aveiro, 3810-193
Aveiro, Portugal
Molecular dynamics (MD) simulations were carried out with a three-body Tersoff potential force field to predict the transversely isotropic elastic properties of pristine and defected BNNTs. This is accomplished by imposing uniaxial tension, twisting moment, in-aplane shear and in-plane biaxial tension to the BNNTs. Effects of various factors such as chirality and diameter of BNNTs, vacancy concentration, and distribution of vacancy pores along the length and circumference of BNNTs were critically examined. Our study reveals that the elastic coefficients of BNNTs decrease as their diameter increase, except axial Young’s modulus. Young’s modulus of BNNT increases with the diameter and reaches its maximum value when the tube diameter is ∼14 Å and then it starts decreasing. We also found that the axial Young’s modulus of a BNNT increases as its aspect ratio increases and stabilizes at a particular value of aspect ratio (L/D ∼ 15). The vacancies greatly affect the elastic properties of BNNTs; for instance, the vacancy concentration of 2% in (10, 10) BNNT reduce its axial Young’s, shear, plane strain bulk and in-plane shear moduli by 14%, 25%, 14% and 18%, respectively. Furthermore, we studied the electronic properties of pristine and defective BNNTs under four transversely isotropic loading conditions using the strain effective method. The results reveal that the electronic properties of BNNTs can be altered via different routes: loadings conditions, diameter and vacancy concentration. Our fundamental study highlights the critical role played by vacancy defected BNNTs in determining their elastic and electronic properties as they are vastly being used in multifarious applications such as nano-electronic devices and reinforcements in multifunctional nanocomposites
On the power of virtual experimentation in MT2.0:a VFORM-xSteels outlookvformxsteels
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
On the inverse identification of sheet metal mechanical behaviour using a het...vformxsteels
ESAFORM 2023
João Henriquesa,*, A. Andrade-Camposa
, J. Xavierb
aTEMA, Department of Mechanical Engineering, University of Aveiro, Campus
Universitário de Santiago, 3810-193 Aveiro, Portugal
bUNIDEMI, Department of Mechanical and Industrial Engineering, NOVA School of
Science and Technology, NOVA University Lisbon, 2825-149 Lisbon, Portugal
On the inverse identification of sheet metal mechanical behaviour using a het...vformxsteels
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João Henriquesa,*, A. Andrade-Camposa
, J. Xavierb
aTEMA, Department of Mechanical Engineering, University of Aveiro, Campus
Universitário de Santiago, 3810-193 Aveiro, Portugal
bUNIDEMI, Department of Mechanical and Industrial Engineering, NOVA School of
Science and Technology, NOVA University Lisbon, 2825-149 Lisbon, Portugal
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Available at:
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Independent Validation of Generic Specimen Design for Inverse Identification of Plastic Anisotropy
1. Department of Materials Engineering
1
Independent Validation of Generic Specimen Design for Inverse Identification
of Plastic Anisotropy
Yi Zhanga , S. Coppietersa,*, S. Gothivarekara, A. Van de Veldea , D. Debruynea
a Department of Materials Engineering, KU Leuven, Technology Campus Ghent, 9000 Gent, Belgium
Belgium,19 March 2021
Presented by Yi Zhang
https://www.kuleuven.be/wieiswie/en/person/00127451
2. Department of Materials Engineering
2
I. Design optimal heterogeneous mechanical test based on Indicator- IT and shape optimization
algorithm.
II. Validate the optimization scheme via identifiability analysis and FEMU(Finite Element Model
Updating ).
III. Preliminary exploration of the identification quality assessed via identifiability analysis method.
Objectives of this Research Work
3. Department of Materials Engineering
3
• Sheet metal forming
• Modeling and simulation
Intro Problem Statement “Independent Validation of Generic Specimen
Design for Inverse Identification of Plastic Anisotropy”
High cost due to
try-and-error
manufacturing
Try-less manufacturing
Computer simulation
Die design
Accurate numerical
simulation
Material modelling
s Heterogeneous test
specimens
?
Complex
Model
Anisotropic
Behavior
Multiple
parameters
Reduce mechanical tests
Assessment of identifiability for specimen
Accuracy parameters identification
4. Department of Materials Engineering
4
2 1
2 1 Max
1 2 3 4 5
1 2 3 4 5
Mean Std
Mean Std /
/
p p
R
r r r r r
a a a a a
Av p
w w w w w
w w w w w
T
I
Strain state Strain level
Rank/Rate/Guide
Specimen
design[1]
Higher Indicator
Better specimen
Richer Strain
state
Richer Strain
Level
Wr Relative weighting factors Wa Absolute weighting factors
Formability Resistance to deformation
𝜺𝟐 𝜺𝟏 𝑹
Scatter
Standard deviation
(a)
(b)
(1)
Intro - Definition of an Indicator-IT
[1] N. Souto, Thuillier S, Andrade-Campos A. Design of an indicator to characterize and classify mechanical tests for sheet metals.
International Journal of Mechanical Sciences, 2015, 101-102, pp.252-271.
5. 5
Identifiability
Purpose:
• Identify unique parameters or improve identification accuracy.
Structural & Practical
• Equations vs Data
Non-identified and identified parameters subset:
• Model structure, parameters sensitivity(Geometry, material orientation, loading… )
Evaluate the identification quality potential before the FEMU.
Intro -Identifiability
comic by Olivia walch!(UM)
http://mogenquest.net
Example: Y=(m1+m2)X+b
6. TD
(b)
(a)
(c)
AOI
R4
30
L
ΔL
L=[0-9]
69
30
30
Fixed
t = 1.2
RD
Fixed edge
(U1,2,3=UR1,2,3=0)
Set:‘AOI’
3D-Shell (S4R)
Global seed: 2
Local seed: 0.3
Displacement, U2=δ
(U1,3=UR1,2,3=0)
𝛿
RD
TD
Symmetry
LA
LC
LD
LB
30o
.
.
. .
C
D
A
B
30o
30o
Spline
Fig. 1 FE model information with (a) specimen gemotry, (b) material orientations (c) mesh information and boundary conditions.
The research object
Model
7. Department of Materials Engineering
7
Table 1. Swift’s hardening law fitted in a strain range from εeq
pl = 0.002 up to the maximum uniform strain 𝜀𝑚𝑎𝑥. The reported R-values are measured at an engineering strain 𝜀𝑒𝑛𝑔 = 0.10[1]
The research object
Material properties
[1] Coppieters, S., Hakoyama, T., Eyckens, P. et al. On the synergy between physical and virtual sheet metal testing: calibration
of anisotropic yield functions using a microstructure-based plasticity model
0
50
100
150
200
250
300
350
400
0 0.05 0.1 0.15 0.2 0.25
True
stress
σ
(Mpa)
Logarithmic plastic strain εp
Swift's hardening law
𝝈 =K(εo+εp)𝒏
RD
45D
90D
Tensile direction σ0.2(MPa) K(MPa) ε0 n r εmax
RD 153 564 0.0059 0.275 1.85 0.248
45D 161 558 0.0072 0.272 1.93 0.254
TD 162 549 0.0080 0.272 2.82 0.259
Fig. 2 Uniaxial stress-strain curves at 0o, 45o and 90o with respect to rolling direction(RD).
Fig. 1(a) Orthotropic axes of the rolled sheet metals, (b) specimen orientation.
8. Optimization procedures
Fig. 1 Python Script structure for automatic numerical model, data post-processing and optimization
9. Table 1. IT value for different initial geometry parameters set and optimal geometry parameters.
Fig. 1 Geometry of mechanical tests (a) Test A, (b) Test B (c) Test C.
Optimization Results
* IT value at maximum uniform strain. Note: Anisotropic parameters change as a function of the plastic deformation[3]
[3] Coppieters S, Hakoyama T, Eyckens P, et al. On the synergy between physical and virtual sheet metal testing: calibration of anisotropic yield functions using a microstructure-based
plasticity model. International Journal of Material Forming, 2018, pp.741-759.
Test
Length vector L - [LA, LB, LC, LD] Post-Necking Equal Max 𝜀𝑒𝑞
𝑝𝑙
LA/mm LB/mm LC/mm LD/mm IT IT
Test A Initial 0.00 0.00 0.00 0.00 0.25 0.01*
Test B
Initial 2.80 2.80 2.80 2.80 0.23
Optimal 2.12 3.54 3.49 2.10 0.26 0.14
Test C
Initial 3.00 3.00 6.00 6.00 0.26
Optimal 2.87 4.81 7.23 7.23 0.34 0.15
IT –Necking criterion/strain level
IT value: Test A close to zero
IT Rank: Test C>Test B>Test A
10. Department of Materials Engineering
10
Optimization Results- Stress states
(a) Test B (b)Test C
Similar distribution shape
Test C covers bigger area
Fig. 1 Stress states for Test B and Test C at TD material orientation using Hill1948 criterion
11. Fig. 1 Strain states for Test B and Test C.
(a) Test B and Test C
(b) Test B (c) Test C
1.14
1.43
0
0.4
0.8
1.2
1.6
Test B Test C
Strain state range
(1)
0.12
0.13
0.1
0.11
0.12
0.13
0.14
Test B Test C
Standard deviation of strain state
(2)
Optimization Results- Strain states
Fig.2 (1)-strain state range ((ε2/ε1)max-(ε2/ε1)min) , (2)-std(ε2/ε1) for Test B and Test C
12. 12
Fig. 1 IT value at certain load step of last increment of numerical simulation (a) and corresponding identifiability index using IK criterion (b) and 𝛾𝑘 criterion(c) for
three mechanical tests.
4.28
4.63
4.96
0 5 10 15 20 25
Test C
Test B
Test A
Collinearity index 𝛾K for three mechanical tests
1.48
1.60
1.68
0 1 2 3 4
Test C
Test B
Test A
Identifiability index IK for three mechanical tests
(b) (c)
Poor identifiability
(IK>3)
Moderate
(2<IK >3)
Good
(IK <2)
Poor identifiability
(𝛾𝐾 >20)
0.15
0.14
0.01
0 0.05 0.1 0.15 0.2
Test C
Test B
Test A
IT value at certain load step for three mechanical tests
(a)
Validation- Identifiability
Lower Indentifiability Index
Better Indentifiability
IT value:
Test C>Test B>Test A
validation
IK, 𝛾𝐾
value :
Test A>Test B>Test C
• Both of the specimens could be well identified.
• Identifiability exhibits good correlation with IT
13. Fig. 1 The detailed flowchart of FEMU procedure.
FEMU process
14. 14
F G H N
R.E.
Reference values 0.2302 0.3509 0.6492 1.4120
Identified
values
Test A 0.2274 0.3824 0.6176 1.3419 3.68%
Test B 0.2210 0.3658 0.6342 1.3679 3.13%
Test C 0.2192 0.3824 0.6340 1.3936 2.49%
Table 1. Comparison of correct parameters values and identified parameters values for Test A, Test B and Test C, respectively.
Fig. 1. Normalized identified yield loci compared with the reference yield locus. Test A (a), Test B (b) and Test C (c).
Validation- FEMU
Identified Accuracy:
Test C>Test B>Test A
IT value:
Test C>Test B>Test A
IK value 𝜸𝑲
:
Test A>Test B>Test C
IT , IK and 𝜸𝑲
show good
correlation with
Identified accuracy
15. Department of Materials Engineering
15
Limitations:
IT -based design probably be enhanced by adjusting the weight factors and didn’t consider
material orientation.
Identifiability analysis is only the numerical simulation, the high quality identification need sufficient
and accuracy experiment data.
Conclusions:
Optimal mechanical test was obtained via IT and shape optimization method .
IT value, identifiability index and identification accuracy show good correlation.
Identifiability analysis could quantitatively predict the identification potential/quality
for anisotropic plastic constitutive parameters.
Limitations &Conclusions
Hello everyone, my presentation topic is Independent Validation of Generic Specimen Design for Inverse Identification
of Plastic Anisotropy
This sides shows the objectives for the research work. It include for sections: Firstly
In the past, trial and error method was used to design components, such as automotive, aircraft. Owing to the development of finite element method analysis , the numerical simulation has been widely used in industry. For sheet forming process, owing to cold rolling, it will induces anisotropy /,ænaɪ'sɒtrəpɪ/ and affects the material behavior during the following the forming process. In order to predict the accuracy behavior of the model, it required well defined Constitutive equations and parameters value to characterize the complex model parameters value. Accuracy parameters required many classic tests, while it was time and cost –consuming. Many researcher proposed to design heterogeneous specimen to reduce mechanical tests and identify parameters accurately. While most of the specimen based on engineering judgement and experience, the current research is to design heterogeneous specimen by quantitatively to maximize the identifiability of parameters. The final purpose is to reduce the mechanical tests and accuracy parameters identification.
This is the equation of indicator, which include two parts. The first term is range of strain state, which means the scope of strain state, and the second term means the standard deviation of strain state, which means the scatter degree or diversity of strain state, the first and second terms means the formability of the specimen and second part represent the strain level, which means equivalent plastic strain and average strain deformation , which represent the resistance ability to deformation. The higher indicator value means richness of strain information, indicating better specimen.
The purpose is to identified unique or close to unique parameters and improve identification accuracy. The identifiability include two parts, one is the structural identifiability, which mainly related to equation of the model, such as right graph, X, and Y represent input and output respectively. The m1 and m2, have 100 percent correlation, so this equation have structural problem. The practical identifiability was focused on sensitivity about cost function to maximize the parameters identifiability.
Identifiability analysis , it will help to partition the parameters into unidentifiable or identified parameters, and final purpose to identified reliable parameters. In current work, the identifiability analysis was used to the validate optimal specimen shape for maximizing the parameters. Moreover, the identification quality pre-assessment before FEMU.
A simple notch tensile specimen as research object. Figure a is the geometry, the AOI are is indicated by red rectangle, only the AOI shape was optimized, four control point was used and connected by cubic spline, the length change from 0 to 9mm during the optimization. The Figure C is mesh, material orientation, boundary conditions, and the specimen pulling direction is along with TD direction.
This slide is material properties. And swift hardening law is used to describe the behavior of hardening process.
The Swift hardening law parameters and Lankford ratio of the specimen measured along with rolling , transverse, 45 directions could be seen in table 1, the detailed date is available in reference.
This slide show the optimization procedures. Python script was created for automatic numerical model and data post-processing communicating with Abaqus. Each simulation include two model, mode l-0 and model -1, unless the load step is different , the geometry, material properties, mesh are the same. The model-0 is find the critical load which make specimen onset necking. So model-0 will apply excessive load to make model-0 necking, and the each frame will compute which frame begin to necking based on stopping criterion. Then the corresponding displacement which be used in model-1. After model completed, the It calculation and optimization process will begin. The GN and LM was used to in the optimization process.
Two heterogeneous specimens are obtained during the optimization process. Fig.1 show the detailed geometry for test A, test B and test C. Test A was a standard test, which was used to compared to test B and test C. As showed in AOI area, The The Table1 is the initial, optimal length vector, and corresponding It value. According to the necking criterion, both of them It value is higher for at post necking state. When keep maximum uniform deformation for test A the corresponding it value is 0.01 close to zero. Some research indicated that the PEEQ will have influence the identified parameters, so in this cases the lever and equal PEEP strain around 0.5 for test B and test C, the It value is 0.14, and 0.15 respectively.
In order to better understanding the heterogeneity of the Test B and Test C.
For test A as a standard test, the stress distribution is almost uniform and cluster around the uniaxial tension axis (TD), as showed in Fig.1(a). Concerning the Test B and Test C, the stress states exhibit similar distribution of shape and appear to cluster between two stress states between equibiaxial tension and simple shear, while most of points cluster around uniaxial. Compared to stress space of Test B, Test C stress states cover a large area and higher diversity stress, indicated a good candidate for inverse identification through FEMU
Fig.1 displays the strain states of the two tests in the AOI area. The strain state (ε2/ε1) is defined as the ratio between of the minor ε 2 and the major ε 1 principal strains. The range of these scatter points indicates the different strain states. The graphs in Fig.9 is characterized by straight lines, each one with a different angle because it is related to a certain strain state. For test B and test C, the graphs suggest that most of the material strain state are above pure shear and under uniaxial tension, while scatter points of Test B are closer to uniaxial tension as shown in Fig.9 (b). In addition, test C presents higher dispersion points in Fig.9 (c), suggesting higher heterogeneity. However, the above result is based on qualitatively analysis. For better explaining the strain state information, the quantitative calculation about strain state was conducted as shown in Fig.10. The stain sate standard deviation and stain sate range and was calculated based on equation (a) and equation (b) in Table 3. Compared to Test B, it illustrates that not only strain state range and its standard deviation both are higher for Test C, which further validate that Test C have bigger strain state cover and larger diversification of mechanical test.
In the previous section, two heterogeneous specimens (Test B and Test C) were found via an IT-based design. The basic research question addressed in this section is whether heterogeneity correlates with the collinearity index and/or the identifiability index of the sought anisotropic parameters. To this end, the identifiability methodology (section 3) is used to evaluate the strain fields generated by the mechanical tests A, B and C. The results are shown in Fig. 4. Fig.4 (a) shows that the IT value of Test A (IT = 0.01) is smallest, while Test C is largest (IT = 0.15) yet very close to Test B (IT = 0.14). Fig.4 (b) and (c) illustrate the corresponding identifiability and collinearity index of the full parameters set (F, H, N), indicating that both of them are good for Test A, test B and test C. However, both IK and 𝛾 𝑘 indexes suggest that Test C is best choice. This basically shows that – for the identification problem (i.e. plasticity model and notched specimen) studied here – there is correlation between heterogeneity (measured by IT) and identifiability (defined as IK and 𝛾 𝑘 ). Based on this correlation, it can be stated from a theoretical point of view that Test C will yield the best identification quality when applying FEMU. The latter is scrutinized in the next section.
This slide show the result parameters identification, The table is the comparison of the identified parameters and identified value, the lower R.E value the higher identified accuracy. we could know that both of the three specimens exhibit good identification compared to reference, this result have good correlation with previous identifiability index. In addition, as for identified accuracy is that , test C is the best, and test B greater than test A. The yield locus was showed in the Fig1, we could know that both of the three specimens exhibit good identification compared to reference, but test B and test C is indeed better that Test A, form the graph, the locus almost completely overlap with reference, which is difficult to distinguish which one is better. The average relative error is completely opposite with order of It value for the three specimen. Which could proof that the indicator is validate.