We investigate a family of isotropic volumetric-isochoric decoupled strain
energies Fβ¦WeHββ(F):=WeHββ(U):={kΞΌβekβ₯devnβlogUβ₯2+2kΞΊβek[tr(logU)]2+ββififβdetF>0,detFβ€0,β based on the Hencky-logarithmic (true, natural)
strain tensor logU, where ΞΌ>0 is the infinitesimal shear modulus,
ΞΊ=32ΞΌ+3Ξ»β>0 is the infinitesimal bulk modulus with
Ξ» the first Lam\'{e} constant, k,k are dimensionless
parameters, F=βΟ is the gradient of deformation, U=FTFβ
is the right stretch tensor and devnβlogU=logUβn1βtr(logU)β 11 is the deviatoric part of the strain tensor logU. For small elastic strains, WeHββ approximates the classical
quadratic Hencky strain energy Fβ¦WHββ(F):=WHββ(U):=ΞΌβ₯devnβlogUβ₯2+2ΞΊβ[tr(logU)]2, which is not everywhere
rank-one convex. In plane elastostatics, i.e. n=2, we prove the everywhere
rank-one convexity of the proposed family WeHββ, for kβ₯41β and kβ₯81β. Moreover, we show that the
corresponding Cauchy (true)-stress-true-strain relation is invertible for
n=2,3 and we show the monotonicity of the Cauchy (true) stress tensor as a
function of the true strain tensor in a domain of bounded distortions. We also
prove that the rank-one convexity of the energies belonging to the family
WeHββ is not preserved in dimension n=3
In this paper we linearise the recently introduced geometrically nonlinear
constrained Cosserat-shell model. In the framework of the linear constrained
Cosserat-shell model, we provide a comparison of our linear models with the
classical linear Koiter shell model and the "best" first order shell model. For
all proposed linear models we show existence and uniqueness based on a Korn's
inequality for surfaces.Comment: arXiv admin note: text overlap with arXiv:2208.04574,
arXiv:2010.1430
We describe ellipticity domains for the isochoric elastic energy Fβ¦β₯devnβlogUβ₯2=βlog(detF)1/nFTFβββ2=41ββlog(detC)1/nCββ2 for n=2,3,
where C=FTF for FβGL+(n). Here, devnβlogU=logUβn1βtr(logU)β 11 is the deviatoric part of the
logarithmic strain tensor logU. For n=2 we identify the maximal
ellipticity domain, while for n=3 we show that the energy is
Legendre-Hadamard elliptic in the set E3β(WHβisoβ,LH,U,32β):={UβPSym(3)ββ₯dev3βlogUβ₯2β€32β}, which is similar to the
von-Mises-Huber-Hencky maximum distortion strain energy criterion.
Our results complement the characterization of ellipticity domains for the
quadratic Hencky energy WHββ(F)=ΞΌβ₯dev3βlogUβ₯2+2ΞΊβ[tr(logU)]2, U=FTFβ with ΞΌ>0 and
ΞΊ>32βΞΌ, previously obtained by Bruhns et al