A polyconvex extension of the logarithmic Hencky strain energy

Abstract

Adapting a method introduced by Ball, Muite, Schryvers and Tirry, we construct a polyconvex isotropic energy function $W:\mathrm{G}{\mathrm{L}}^{+}(n)\to \mathbb{R}$ which is equal to the classical Hencky strain energy \[ W_{\mathrm{H}}(F) = μ\,\lVert\operatorname{dev}_n\log U\rVert^2+\fracκ{2}\,[\operatorname{tr}(\log U)]^2 = μ\,\lVert\log U\rVert^2+\fracΛ{2}\,[\operatorname{tr}(\log U)]^2 \] in a neighborhood of the identity matrix; here, $\mathrm{G}{\mathrm{L}}^{+}(n)$ denotes the set of $n\times n$-matrices with positive determinant, $F\in \mathrm{G}{\mathrm{L}}^{+}(n)$ denotes the deformation gradient, $U=\sqrt{F^{T}F}$ is the corresponding stretch tensor, $\log U$ is the principal matrix logarithm of $U$, $\mathrm{tr}$ is the trace operator, $\Vert X\Vert$ is the Frobenius matrix norm and ${\mathrm{dev}}_{n}X$ is the deviatoric part of $X\in {\mathbb{R}}^{n\times n}$. The extension can also be chosen to be coercive, in which case Ball's classical theorems for the existence of energy minimizers under appropriate boundary conditions are immediately applicable. We also generalize the approach to energy functions $W_{\mathrm{VL}}$ in the so-called Valanis-Landel form \[ W_{\mathrm{VL}}(F) = \sum_{i=1}^n w(λ_i) \] with $w:(0,\infty )\to \mathbb{R}$, where $\hat{I}{»}_1,\dots ,\hat{I}{»}_n$ denote the singular values of $F$.