Volume 22, Issue 1 e202200185
Section 14
Open Access

Remarks on rank-one convexity and quasiconvexity for planar functions with an additive volumetric–isochoric split

Robert J. Martin

Robert J. Martin

Chair for Nonlinear Analysis and Modeling, University of Duisburg-Essen, Thea-Leymann-Str. 9, 45127 Essen, Germany

Institute for Technologies of Metals, University of Duisburg-Essen, Friedrich-Ebert-Str. 12,47119 Duisburg, Germany

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Jendrik Voss

Corresponding Author

Jendrik Voss

Chair for Nonlinear Analysis and Modeling, University of Duisburg-Essen, Thea-Leymann-Str. 9, 45127 Essen, Germany

Institute for Structural Mechanics and Dynamics, Technical University Dortmund, August-Schmidt-Str. 8, 44227 Dortmund, Germany

Jendrik Voss

Chair for Nonlinear Analysis and Modeling, University of Duisburg-Essen, Thea-Leymann-Str. 9, 45127 Essen, Germany

Institute for Structural Mechanics and Dynamics, Technical University Dortmund, August-Schmidt-Str. 8, 44227 Dortmund, Germany

Email: [email protected]

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Oliver Sander

Oliver Sander

Institute of Numerical Mathematics, Technische Universität Dresden, Zellescher Weg 12–14, 01069 Dresden, Germany

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Patrizio Neff

Patrizio Neff

Chair for Nonlinear Analysis and Modeling, University of Duisburg-Essen, Thea-Leymann-Str. 9, 45127 Essen, Germany

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First published: 24 March 2023

Abstract

We study convexity properties of isotropic energy functions in planar nonlinear elasticity in the context of Morrey's conjecture, which states that rank-one convexity does not imply quasiconvexity in the two-dimensional case. Recently, it has been shown that for the special case of isochoric energy functions on GL+(2) = {F ∈ ℝ2×2 | det F > 0}, i.e. for any isotropic function W : GL+(2) → ℝ with W(aF) = W(F) for all a > 0, these two notions of generalized convexity are, in fact, equivalent. Here, we consider the more general case of functions on GL+(2) with an additive volumetric–isochoric split of the form

urn:x-wiley:16177061:media:PAMM202200185:pamm202200185-math-0001
with an isochoric function Wiso on GL+(2) and a function Wvol on (0, ∞). In particular, we investigate the importance of the function
urn:x-wiley:16177061:media:PAMM202200185:pamm202200185-math-0002
and its convexity properties; here, λmax ≥ λmin > 0 are the ordered singular values of the deformation gradient F ∈ GL+(2). This function arises naturally as an “extremal” case in the class of volumetric–isochorically split energies with respect to rank-one convexity.

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