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Inverse Identification of Asymmetric Creep Parameters Using the I-DIC Technique

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HAL Id: hal-02611997

https://hal.archives-ouvertes.fr/hal-02611997

Submitted on 18 May 2020

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Inverse Identification of Asymmetric Creep Parameters Using the I-DIC Technique

Lucas Breder Teixeira, Jean Gillibert, Eric Blond, Thomas Sayet

To cite this version:

Lucas Breder Teixeira, Jean Gillibert, Eric Blond, Thomas Sayet. Inverse Identification of Asymmetric

Creep Parameters Using the I-DIC Technique. XVI European Ceramic Society Conference, Jun 2019,

Torino, Italy. �hal-02611997�

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ESR Position 09

Inverse Identification of Asymmetric Creep Parameters Using the I-DIC Technique

Lucas BREDER TEIXEIRA Early Stage Researcher

mail: lucas.breder-teixeira@univ-orleans.fr

Advanced THermomechanical multiscale mOdelling of Refractory Linings

Supervisors & University

Consortium of 15 European Partners

Eric BLOND, Thomas SAYET, Jean GILLIBERT

Lucas BREDER TEIXEIRA, Jean GILLIBERT, Eric BLOND, Thomas SAYET Univ Orléans, Univ Tours, INSA CVL, LaMé EA 7494, 45000 Orléans, France

Acknowledgments

This project has received funding from the European Union's Horizon 2020 research and innovation program under grant agreement no.764987

1 – Introduction:

• The creep characterization of refractory materials at high temperatures requires complex tests

• This work intends to apply the Integrated Digital Image Correlation technique to the determination of the secondary creep properties of refractories at high temperatures

• It’s expected to fully characterize the materials (tension, compression and shear) using a reduced number of tests, making use of the Brazilian test

• Images taken at 1200°C were virtually deformed using an asymmetric creep law (different behavior under tension and compression) with known materials’ parameters. Later, starting from an initial guess for the parameters, an inverse identification was run to check the I-DIC software robustness

7 – Conclusions:

• The I-DIC technique is a convenient option to perform inverse identification of mechanical parameters at high temperatures

• For future works, the creep parameters of refractory materials will be identified using experimental images

3 – I-DIC algorithm:

5 – Experimental setup:

Ventilators Furnace

Window

Blue light sources

200mm lens CCD camera Blue

filters (c) (d) (e)

(f)

Ideal image Room temperature

1200°C - Without blue light

1200°C - With blue light

(b)

(a)

(a) High temperature test setup and Brazilian test samples used with I-DIC. (b) Virtual image. (c) Room temperature. (d) 1200°C without using the blue lights. (e) 1200°C using the blue lights. (f) Images’ histograms.

4 – Mathematical model:

𝜺̇ = 3 2 𝒔 𝜎

𝜎 − 𝜎

𝐾 − 3

2 𝒔 𝜎

𝜎 − 𝜎 𝐾 Asymmetric viscoplastic strain rate 1

where 𝜎 is the yield stress, 𝒔 is the deviatoric stress and 𝜎 is the von Mises stress.

1E. Blond, N. Schmitt, F. Hild, P. Blumenfeld, J. Poirier, Journal

of the European Ceramic Society, 25[11] 1819-1827 (2005).

6 – Results:

Solution 1 Solution 2 Solution 3 Value Error Value Error Value Error 𝐾 5127.6 -11.19% 5543.3 -3.99% 5264.70 -8.81%

𝑛 2.01 0.27% 1.99 -0.46% 1.99 -0.58%

𝐾 9.71E+05 -2.91% 1.25E+06 24.97% 1.08E+06 8.14%

𝑛 1.51 0.71% 1.48 -1.10% 1.51 0.35%

Table 2 – Three best solutions given by the Genetic Algorithm Table 1 – Reference values for the creep properties

Reference values Range of variation Tension

𝐾 = 5773.5 𝐾 = 5000

𝐾 = 6000

𝑛 = 2 𝑛 = 2.2

𝑛 = 1.8

Compression

𝐾 = 1.0 × 10 𝐾 = 5.0 × 10 𝐾 = 5.0 × 10

𝑛 = 1.5 𝑛 = 1.8

𝑛 = 1.2

A Genetic Algorithm was used to perform the inverse identification of the parameters. Tables 1 and 2 show the reference values used to create the deformed images, the range of variation used in the optimization and the identification results.

2 – Brazilian test:

F

Shear Tension Compression

The Brazilian test presents a complex stress distribution, with tension, compression and shear observed in the sample at the same time. This allows the identification of the asymmetric behavior using a reduce number of tests

Initial guess for the material’s properties (𝐾 , 𝐾 , 𝑛 , 𝑛 )

Finite Element Model - Displacements

Reference Image

Theoretical Image Interpolation

F

Experimental Images (1200°C)

-

Minimization of the difference?

NO

Parameters update – Optimization algorithm

Yes

Material’s properties

(𝐾 , 𝐾 , 𝑛 , 𝑛 )

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