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In this paper we consider the additive logarithmic finite strain plasticityformulation from the view point of loss of ellipticity in elastic unloading. Weprove that even if an elastic energy $F\mapsto W(F)=\hat{W}(\log U)$ defined interms of logarithmic strain $\log U$, where $U=\sqrt{F^T\, F}$, is everywhererank-one convex as a function of $F$, the new function $F\mapsto\widetilde{W}(F)=\hat{W}(\log U-\log U_p)$ need not remain rank-one convex atsome given plastic stretch $U_p$ (viz. $E_p^{\log}:=\log U_p$). This is incomplete contrast to multiplicative plasticity in which $F\mapsto W(F\,F_p^{-1})$ remains rank-one convex at every plastic distortion $F_p$ if$F\mapsto W(F)$ is rank-one convex. We show this disturbing feature with thehelp of a recently considered family of exponentiated Hencky energies.

Loss of ellipticity for non-coaxial plastic deformations in additive logarithmic finite strain plasticity