2013
DOI: 10.1016/j.ijsolstr.2012.10.001
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A geometrically nonlinear analysis of coplanar crack propagation in some heterogeneous medium

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Cited by 22 publications
(20 citation statements)
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“…More precisely, modeling the simplified 3D problem [64][65][66][67][68][69] may be combined with the out-of-theplane fluctuations (namely the current work) to yield a full 3D theory. Various elements needed in that direction can be found in the literature [50,[70][71][72][73] but such a theory is still far from being formulated.…”
Section: Discussionmentioning
confidence: 99%
“…More precisely, modeling the simplified 3D problem [64][65][66][67][68][69] may be combined with the out-of-theplane fluctuations (namely the current work) to yield a full 3D theory. Various elements needed in that direction can be found in the literature [50,[70][71][72][73] but such a theory is still far from being formulated.…”
Section: Discussionmentioning
confidence: 99%
“…where G eff C is the average adhesion energy of the interface (see Vasoya et al, 2013 for the analogous result in fracture). We observe good agreement between the experiments and the theoretical model.…”
Section: Stripesmentioning
confidence: 99%
“…To explore the non-linear response of cracks pinned by defects of larger contrasts, Leblond et al (2012) extended Rice (1985)'s first-order formula for a semi-infinite crack in an infinite body to second order, under the assumption of independence of the unperturbed stress intensity factor imposed by the loading with respect to the average crack front location. Then, Vasoya et al (2013) released this hypothesis, thus extending the range of application of Leblond et al (2012)'s formula to general loading conditions. Recently, Willis (2013) and Willis and Movchan (2014) investigated the dynamic perturbation of a crack up to second order.…”
Section: Introductionmentioning
confidence: 99%
“…Still, since both Leblond et al (2012)'s and Vasoya et al (2013)'s works considered only infinite bodies, the combined effect of the finite size of the specimens and the geometrical nonlinearities induced by strong defects remains unexplored, and it is the aim of this work to address this question. The results of our calculations apply to several experimental situations involving strong heterogeneities, and for which the crack front perturbation wavelength compares with the thickness of the specimen (Santucci et al, 2010;Chopin et al, 2011).…”
Section: Introductionmentioning
confidence: 99%