2014
DOI: 10.1016/j.mspro.2014.06.192
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Thermodynamic Formulation of a Material Model for Microcracking Applied to Creep Damage

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Cited by 3 publications
(4 citation statements)
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“…A similar partition is obtained for rectilinear microcracks in a two-dimensional body [12] and for penny-shaped microcracks in a three-dimensional body [30]. Based on Equations (11) and (14) where is the elastic strain tensor, is the damage strain tensor, is the ε e ε d ε sw porosity swelling strain tensor and is the inelastic strain tensor. Equations (17) ε i and (18) 1 give It is worth noting that Expression (18) does not include models for all potential deformation mechanisms.…”
Section: Spherical Microvoids With the Hookean Matrix Responsementioning
confidence: 86%
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“…A similar partition is obtained for rectilinear microcracks in a two-dimensional body [12] and for penny-shaped microcracks in a three-dimensional body [30]. Based on Equations (11) and (14) where is the elastic strain tensor, is the damage strain tensor, is the ε e ε d ε sw porosity swelling strain tensor and is the inelastic strain tensor. Equations (17) ε i and (18) 1 give It is worth noting that Expression (18) does not include models for all potential deformation mechanisms.…”
Section: Spherical Microvoids With the Hookean Matrix Responsementioning
confidence: 86%
“…Model (37) 2 is valid for a Hookean matrix deformation with spherical microvoids [see Equation (20)]. According to Santaoja [11,30,36], it is valid for a Hookean matrix deformation with penny-shaped microcracks and for rectilinear microcracks in a 2D solid [12], although for these latter two cases the damage strain tensor has to be made symmetric. Therefore, Equations (38) are valid for g d these three types of material behaviours.…”
Section: Analytical Relation Between the Stress Tensors σ And σ For Tmentioning
confidence: 99%
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