Integrability conditions between the first and second Cosserat deformation tensor in geometrically nonlinear micropolar models and existence of minimizers

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Authors

  • J. Lankeit
  • P. Neff
  • F. Osterbrink

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Original languageEnglish
Article number11
JournalZeitschrift fur Angewandte Mathematik und Physik
Volume68
Issue number1
Publication statusPublished - 2017

Abstract

In this note, we extend integrability conditions for the symmetric stretch tensor U in the polar decomposition of the deformation gradient ∇φ=F=RU to the nonsymmetric case. In doing so, we recover integrability conditions for the first Cosserat deformation tensor. Let (Formula presented.). Then, (Formula presented.), giving a connection between the first Cosserat deformation tensor U¯ and the second Cosserat tensor K. (Here, Anti denotes an isomorphism between R 3 × 3 and So(3):={A∈R 3×3×3|A.u∈so(3)∀u∈R 3}). The formula shows that it is not possible to prescribe U¯ and K independent from each other. We also propose a new energy formulation of geometrically nonlinear Cosserat models which completely separate the effects of nonsymmetric straining and curvature. For very weak constitutive assumptions (no direct boundary condition on rotations, zero Cosserat couple modulus, quadratic curvature energy), we show existence of minimizers in Sobolev spaces.

Keywords

    Compatibility conditions, Cosserat continuum, Extended continuum mechanics, Geometrically nonlinear micropolar elasticity, Integrability conditions, Strain and curvature measures

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Integrability conditions between the first and second Cosserat deformation tensor in geometrically nonlinear micropolar models and existence of minimizers. / Lankeit, J.; Neff, P.; Osterbrink, F.
In: Zeitschrift fur Angewandte Mathematik und Physik, Vol. 68, No. 1, 11, 2017.

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abstract = "In this note, we extend integrability conditions for the symmetric stretch tensor U in the polar decomposition of the deformation gradient ∇φ=F=RU to the nonsymmetric case. In doing so, we recover integrability conditions for the first Cosserat deformation tensor. Let (Formula presented.). Then, (Formula presented.), giving a connection between the first Cosserat deformation tensor U¯ and the second Cosserat tensor K. (Here, Anti denotes an isomorphism between R 3 × 3 and So(3):={A∈R 3×3×3|A.u∈so(3)∀u∈R 3}). The formula shows that it is not possible to prescribe U¯ and K independent from each other. We also propose a new energy formulation of geometrically nonlinear Cosserat models which completely separate the effects of nonsymmetric straining and curvature. For very weak constitutive assumptions (no direct boundary condition on rotations, zero Cosserat couple modulus, quadratic curvature energy), we show existence of minimizers in Sobolev spaces.",
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AU - Lankeit, J.

AU - Neff, P.

AU - Osterbrink, F.

N1 - Publisher Copyright: © 2016, Springer International Publishing.

PY - 2017

Y1 - 2017

N2 - In this note, we extend integrability conditions for the symmetric stretch tensor U in the polar decomposition of the deformation gradient ∇φ=F=RU to the nonsymmetric case. In doing so, we recover integrability conditions for the first Cosserat deformation tensor. Let (Formula presented.). Then, (Formula presented.), giving a connection between the first Cosserat deformation tensor U¯ and the second Cosserat tensor K. (Here, Anti denotes an isomorphism between R 3 × 3 and So(3):={A∈R 3×3×3|A.u∈so(3)∀u∈R 3}). The formula shows that it is not possible to prescribe U¯ and K independent from each other. We also propose a new energy formulation of geometrically nonlinear Cosserat models which completely separate the effects of nonsymmetric straining and curvature. For very weak constitutive assumptions (no direct boundary condition on rotations, zero Cosserat couple modulus, quadratic curvature energy), we show existence of minimizers in Sobolev spaces.

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