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Autores principales: Indergand, Roman, Kochmann, Dennis, Rüland, Angkana, Tribuzio, Antonio, Zillinger, Christian
Formato: Preprint
Publicado: 2024
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Acceso en línea:https://arxiv.org/abs/2408.13110
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author Indergand, Roman
Kochmann, Dennis
Rüland, Angkana
Tribuzio, Antonio
Zillinger, Christian
author_facet Indergand, Roman
Kochmann, Dennis
Rüland, Angkana
Tribuzio, Antonio
Zillinger, Christian
contents We study the rigidity properties of the $T_3$-structure for the symmetrized gradient from \cite{BFJK94} qualitatively, quantitatively and numerically. More precisely, we complement the flexibility result for approximate solutions of the associated differential inclusion which was deduced in \cite{BFJK94} by a rigidity result on the level of exact solutions and by a quantitative rigidity estimate and scaling result. The $T_3$-structure for the symmetrized gradient from \cite{BFJK94} can hence be regarded as a symmetrized gradient analogue of the Tartar square for the gradient. As such a structure cannot exist in $\mathbb{R}^{2\times 2}_{sym}$ the example from \cite{BFJK94} is in this sense minimal. We complement our theoretical findings with numerical simulations of the resulting microstructure.
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spellingShingle On a $T_3$-Structure in Geometrically Linearized Elasticity: Qualitative and Quantitative Analysis and Numerical Simulations
Indergand, Roman
Kochmann, Dennis
Rüland, Angkana
Tribuzio, Antonio
Zillinger, Christian
Analysis of PDEs
We study the rigidity properties of the $T_3$-structure for the symmetrized gradient from \cite{BFJK94} qualitatively, quantitatively and numerically. More precisely, we complement the flexibility result for approximate solutions of the associated differential inclusion which was deduced in \cite{BFJK94} by a rigidity result on the level of exact solutions and by a quantitative rigidity estimate and scaling result. The $T_3$-structure for the symmetrized gradient from \cite{BFJK94} can hence be regarded as a symmetrized gradient analogue of the Tartar square for the gradient. As such a structure cannot exist in $\mathbb{R}^{2\times 2}_{sym}$ the example from \cite{BFJK94} is in this sense minimal. We complement our theoretical findings with numerical simulations of the resulting microstructure.
title On a $T_3$-Structure in Geometrically Linearized Elasticity: Qualitative and Quantitative Analysis and Numerical Simulations
topic Analysis of PDEs
url https://arxiv.org/abs/2408.13110