Homogenization and Geometric Linearization for Multi-Well Energies

The concept of linear elasticity is to assume that the stored energy has one‐well structure and to consider small displacements. The energy function is then expanded around the equilibrium state and higher‐order terms are neglected. It was proved in [3] that this concept really gives results that pr...

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Bibliographic Details
Published inProceedings in applied mathematics and mechanics Vol. 13; no. 1; pp. 355 - 356
Main Authors Jesenko, Martin, Schmidt, Bernd
Format Journal Article
LanguageEnglish
Published Berlin WILEY-VCH Verlag 01.12.2013
WILEY‐VCH Verlag
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Summary:The concept of linear elasticity is to assume that the stored energy has one‐well structure and to consider small displacements. The energy function is then expanded around the equilibrium state and higher‐order terms are neglected. It was proved in [3] that this concept really gives results that provide a good approximation for the actual problem. On the other hand, for materials with fine periodic structure we accomplish a simplification of the problem in an analogous manner by homogenizing the energy. It was recently shown by Müller and Neukamm in [8] that both processes, homogenization and linearization, are interchangeable for such elastic energies. If we consider an energy with multiple wells then, under some reasonable conditions, it is also possible to (geometrically) linearize the problem. The second author proved that quasiconvexification of the limit function yields the desired result. We present that in this case both processes still commute. This is not a priori clear since the proof by Müller and Neukamm significantly rests upon the one‐well structure and properties of quadratic forms. They also provide an example when the statement does not hold. (© 2013 Wiley‐VCH Verlag GmbH & Co. KGaA, Weinheim)
Bibliography:istex:C470395BCBBBCFFDF75BEFA4032610F63E6B1A67
ArticleID:PAMM201310173
ark:/67375/WNG-Z9S4JJ0M-5
ISSN:1617-7061
1617-7061
DOI:10.1002/pamm.201310173