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−12Lvbe⋅be−1=V−1:τNEQ \begin{aligned} \boxed{-\frac{1}{2}\mathscr L_vb_e\cdot b_e^{-1}=\mathscr V^{-1}:\tau_{NEQ}} \end{aligned} −21​Lv​be​⋅be−1​=V−1:τNEQ​​​−12Lvbe⋅be−1=1τ∂∂τNEQ(τ2τNEQ:V−1:τNEQ)=1τ∂Φvis∂τNEQ \begin{equation} \begin{aligned} -\frac{1}{2}\m

Abstract most viscoelasticity models are restricted to linear evolution laws presents a model for finite deformation viscoelasticity that utilizes a nonlinear evolution law Thus it is not restricted to states close to the thermodynamic equilibrium Upon ap

Abstract fully 3D finite strain viscoelastic model general anisotropic response uncoupled bulk and deviator response over any range of deformation general relaxation function recovery of finite elasticity for very fast or very slow processes classical mo