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

TL;DR

This paper investigates the time continuous limits of phase-field evolutions in fracture mechanics, establishing conditions under which Griffith's criterion is satisfied in steady states and analyzing the effects of different numerical schemes.

Contribution

It provides a general theoretical framework for the limits of phase-field evolutions, proving Griffith's criterion in steady states and examining scheme dependence in unsteady regimes.

Findings

Steady state evolutions satisfy Griffith's criterion in terms of toughness.

Limit evolutions depend on the numerical scheme in unsteady regimes.

Thermodynamical consistency of the irreversibility constraint is established.

Abstract

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 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.