2020
DOI: 10.1016/j.mechmat.2019.103292
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Optimisation based material parameter identification using full field displacement and temperature measurements

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Cited by 23 publications
(36 citation statements)
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“…More precisely speaking, it is the intention of this work to show the impact of two different material models on the result of a parameter identification for thermo-mechanically coupled material models and, furthermore, to show what kind of experimental data is necessary to ensure a stable identification process. This work is a follow-up of a previous publication [22] and addresses further research topics such as model and experiment dependencies in the context of a parameter identification. Only brief summaries are given regarding the framework of the identification, experimental setup as well as the description of the underlying boundary value problem.…”
Section: Introductionmentioning
confidence: 94%
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“…More precisely speaking, it is the intention of this work to show the impact of two different material models on the result of a parameter identification for thermo-mechanically coupled material models and, furthermore, to show what kind of experimental data is necessary to ensure a stable identification process. This work is a follow-up of a previous publication [22] and addresses further research topics such as model and experiment dependencies in the context of a parameter identification. Only brief summaries are given regarding the framework of the identification, experimental setup as well as the description of the underlying boundary value problem.…”
Section: Introductionmentioning
confidence: 94%
“…The second approach can be found in [18] where an inverse analysis with full field displacement and temperature measurements of an inhomogeneous boundary value problem (BVP) is used to fit the mechanical parameters and the evolution of a Taylor-Quinney factor of a simple, not necessarily thermodynamically consistent model to an observed temperature field. A similar method was used in [22] to fit the mechanical as well as the thermal material parameters of a potential based material model to the experimental full field displacement and temperature data of a tensile test under monotonic loading. Apart from differences in the handling of experimental data and the employed material model, the main distinction in these two works is the set of parameters which is optimised.…”
Section: Introductionmentioning
confidence: 99%
“…The implementation of the parameter identification closely follows the work in [51]. The goal of the objective function g is to quantify the difference between the response of the simulation and the physical specimen during the experiment.…”
Section: Objective Functionmentioning
confidence: 99%
“…By dividing the difference in the displacement of two neighbouring measurement points by their distance, a simple strain-like quantity Δu is obtained, which is less sensitive to rigid body motions, cf. [51]. Since the displacement field in the experiment is evaluated at different measurement points than the finite element nodes of the simulation, it is necessary to interpolate the measured displacement field to the finite element nodes-a linear interpolation in time and space is performed.…”
Section: Objective Functionmentioning
confidence: 99%
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