Abstract
Considering a one-dimensional problem of debonding in the context of Griffith theory, we show that the dynamical solution converges, when the speed of loading goes to 0, to a quasi-static solution including an unstable phase of propagation. In particular, the jump of the debonding induced by this instability is governed by a principle of balance of the total quasi-static energy, the kinetic energy being negligible. To cite this article: P.-E. Dumouchel et al., C. R. Mecanique 335 (2007).
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