2011
DOI: 10.1007/s00161-011-0228-3
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From the onset of damage to rupture: construction of responses with damage localization for a general class of gradient damage models

Abstract: . From the onset of damage to rupture: construction of responses with damage localization for a general class of gradient damage models. Continuum Mechanics and Thermodynamics, Springer Verlag, 2013, 25 (2-4), pp.147-171. 10.1007/s00161-011-0228-3. hal-00647860To be submitted to Continuum Mechanics and Thermodynamics Abstract We propose a construction method of non homogeneous solutions for the traction problem of an elastic damaging bar. This bar has a softening behavior which obeys a gradient damaged model. … Show more

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Cited by 103 publications
(105 citation statements)
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“…2 For a sufficient large bar, this results in the localization of damage in one single zone which corresponds to the lowest energy and is associated to a snap-back as shown by (Pham and Marigo, 2013), which the authors interpret as the nucleation of a single crack. cf.…”
Section: Irreversibilitymentioning
confidence: 99%
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“…2 For a sufficient large bar, this results in the localization of damage in one single zone which corresponds to the lowest energy and is associated to a snap-back as shown by (Pham and Marigo, 2013), which the authors interpret as the nucleation of a single crack. cf.…”
Section: Irreversibilitymentioning
confidence: 99%
“…For a discussion of the uniqueness and the stability of the homogeneous response see also (Pham et al, 2011;Pham and Marigo, 2013).…”
Section: Irreversibilitymentioning
confidence: 99%
“…A major step forward was the removal of the ill-posedness of the boundary value problem that is caused by smearing out the decohesion over a finite domain. Regularisation can be obtained by means of non-local approaches (Pijaudier-Cabot and Bažant, 1987), and more effectively in a finite element context, by gradient approaches (Peerlings et al, 1996), see also de Borst et al (2004) and Pham and Marigo (2013).…”
Section: Accepted Manuscriptmentioning
confidence: 99%
“…• g ′ (1) = 0, since the energy must converge to a finite value for the fully broken state, see Braides (1998); Pham et al (2011);Pham and Marigo (2013) for a general discussion. For the degradation function g(d) use has often been made of the quadratic function (Miehe et al, 2010b):…”
Section: A C C E P T E D Accepted Manuscriptmentioning
confidence: 99%
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