Energy release and Griffith’s criterion for phase-field fracture

Phase-field evolutions are obtained by means of time discrete schemes, providing (or selecting) at each time step an equilibrium configuration of the system, which is usually computed by descent methods for the free energy ( e.g. staggered and monolithic schemes) under a suitable irreversibility constraint on the phase-field parameter. We consider a class of phase-field energies including both volumetric-deviatoric and spectral decomposition; we study in detail the time continuous limits of these evolutions considering monotonicity as irreversibility constraint and providing a general result, which holds independently of the scheme employed in the incremental problem. In particular, we show that in the steady state regime the limit evolution is simultaneous (in displacement and phase field parameter) and satisfies Griffith’s criterion in terms of toughness and phase field energy release rate. In the unsteady regime the limit evolution may instead depend on the adopted scheme and Griffith’s criterion may not hold. We prove also the thermodynamical consistency of the monotonicity constraint over the whole evolution, and we study the system of PDEs (actually, a weak variational inequality) in the steady state regime. Technically, the proof employs a suitable reparametrization of the time discrete points, whose Kuratowski limit characterizes the set of steady state propagation. The study of the quasi-static time continuous limit relies on the strong convergence of the phase-field function together with the convergence of the power identity.