Skip to content
DraconiticResearch
Search Sources API
203,203 studies31 sourcesUpdated 9 min ago
PreprintCC BY 4.0arXiv

Polyconvexity for incompressible inversion-symmetric energies of Valanis-Landel type

Abstract

{Let λi = νi(F) denote the three singular values of the deformation gradient F ∈ GL+(3).} We consider the family of incompressible isotropic energies $ W_ψ(F)=\sum_i ψ\left(|\!\logλ_i|\right)$ with ψ:[0,∞)↦ℝ. Set g(s)=ψ(arcoshs/2) for all s≥2. If g has a convex and non-decreasing extension g̅ to [0,∞), then Wψ is the restriction to SL(3) of the explicit polyconvex function \ {$ F\mapsto\sum_i \bar g\left(ν_i(F+{\rm Cof} F)\right). $} The proof uses the identity νi(F+Cof F)=λi+λi−1, up to permutation, on SL(3) and Ball's convexity theorem for functions of the singular values. We also give a direct proof along rank-one lines contained in SL(3) and derive a convenient one-dimensional differential sufficient condition. In particular, $ F\mapsto\sum_i e^{\log^2\!λ_i} $ is rank-one convex on SL(3) and possesses the stated polyconvex extension. A simple-shear computation shows that scalar convexity in log λi alone is insufficient; the quadratic Hencky energy ∑i log2λi is not rank-one convex on SL(3).

Related

  1. Concurrent enforcement of polyconvexity and true-stress-true-strain monotonicity in incompressible isotropic hyperelasticity: application to neural network constitutive models
    Maximilian P. Wollner, Dominik K. Klein, Herbert Baaser +2
    arXivPreprintCC BY 4.0Full textMathematical physicsCondensed matterarXiv
  2. Universal neural network approximation of symmetric polyconvex energies and envelopes
    Florian Gammer
    arXivPreprintarXiv licenceFull textNumerical analysis & scientific computingarXiv
  3. Illposedness of incompressible fluids in supercritical Sobolev spaces
    Xiaoyutao Luo
    Duke Mathematical JournalPeer-reviewedLicence not statedFull text12 citedGeneral mathematicsOpenAlex
  4. On putative self-similarity for incompressible 3D Euler
    Peter Constantin, Mihaela Ignatova, Vlad Vicol
    Courant Journal of Pure and Applied MathematicsPeer-reviewedLicence not statedFull text12 citedGeometry & topologyOpenAlex
  5. Dynamics of helical vortex filaments in nonviscous incompressible flows
    Martin Donati, Christophe Lacave, Évelyne Miot
    Bulletin de la Société mathématique de FrancePeer-reviewedLicence not statedFull text12 citedGeneral mathematicsOpenAlex
BibTeX
@misc{ghiba2026polyconvexity,
  title = {{Polyconvexity for incompressible inversion-symmetric energies of Valanis-Landel type}},
  author = {Ionel-Dumitrel Ghiba and Maximilian P. Wollner and Patrizio Neff},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.18660},
  eprint = {2609.18660},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.18660},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Polyconvexity for incompressible inversion-symmetric energies of Valanis-Landel type
AU  - Ionel-Dumitrel Ghiba
AU  - Maximilian P. Wollner
AU  - Patrizio Neff
PY  - 2026
DA  - 2026/09/16
PB  - arXiv
DO  - 10.48550/arxiv.2609.18660
UR  - https://arxiv.org/abs/2609.18660
AB  - {Let λ_i = ν_i(F) denote the three singular values of the deformation gradient F ∈ GL^+(3).} We consider the family of incompressible isotropic energies $ W_ψ(F)=\sum_i ψ\left(|\!\logλ_i|\right)$ with ψ:[0,∞)↦ℝ. Set g(s)=ψ(arcoshs/2) for all s≥2. If g has a convex and non-decreasing extension g̅ to [0,∞), then W_ψ is the restriction to SL(3) of the explicit polyconvex function \ {$ F\mapsto\sum_i \bar g\left(ν_i(F+{\rm Cof} F)\right). $} The proof uses the identity ν_i(F+Cof F)=λ_i+λ_i^−1, up to permutation, on SL(3) and Ball's convexity theorem for functions of the singular values. We also give a direct proof along rank-one lines contained in SL(3) and derive a convenient one-dimensional differential sufficient condition. In particular, $ F\mapsto\sum_i e^{\log^2\!λ_i} $ is rank-one convex on SL(3) and possesses the stated polyconvex extension. A simple-shear computation shows that scalar convexity in log λ_i alone is insufficient; the quadratic Hencky energy ∑_i log^2λ_i is not rank-one convex on SL(3).
ER  -