Planar polyconvexity of exponentiated Hencky energies

For FRn×nF\in\mathbb{R}^{n\times n}, define the exponentiated Hencky energy by

WeH(F)={μkekdevnlogU2+κ2k^ek^[(logdetU)2]if detF>0,+if detF0,W_{\rm eH}(F)=\begin{cases}\displaystyle\frac{\mu}{k}e^{k\|\operatorname{dev}_n\log U\|^2}+\frac{\kappa}{2\widehat{k}}e^{\widehat{k}[(\log\det U)^2]}&\text{if }\det F>0,\\+\infty&\text{if }\det F\leq 0,\end{cases}

where UU is the right stretch tensor and μ,κ,k,k^\mu,\kappa,k,\widehat{k} are parameters. Planar polyconvexity conjecture. The functions WeHW_{\rm eH} defined above are polyconvex for n=2n=2, μ>0\mu>0, κ>0\kappa>0, k14k\geq\frac14, and k^18\widehat{k}\geq\frac18. Polyconvexity implies Legendre–Hadamard ellipticity and can support existence results when suitable growth conditions hold; the source presents this as a conjectural extension of its planar rank-one-convexity theorem.

Sources & referencesView supporting material

Primary source

Patrizio Neff, Ionel-Dumitrel Ghiba and Johannes Lankeit, “The exponentiated Hencky-logarithmic strain energy. Part I: Constitutive issues and rank-one convexity”, arXiv:1403.3843 (2014).

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