2020
DOI: 10.1016/j.euromechsol.2020.104070
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Comparison of the finite strain macroscopic behavior and local damage of a soft matrix highly reinforced by spherical or polyhedral particles

Abstract: Motivated by the different uniaxial responses of two actual materials filled with either sifted glass beads or sifted glass grits, the influence of the fillers shape on the finite strain behavior of highly filled composites (>50%) is examined through micromechanical finite element simulations accounting for matrix/filler debonding with a cohesive-zone model. Three-dimensional matrix cells filled with 64 monosized spherical particles are compared to cells filled with the same number of monosized polyhedra. For … Show more

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Cited by 12 publications
(8 citation statements)
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“…In order to describe the mechanical properties of interfaces, the bilinear cohesive zone model (BCZM) was introduced in this work due to its highly efficient and simple formula. 18,35,[37][38][39] The BCZM theory assumes that interface mainly goes through three stages: (1) elastic stage: interface stress has a linear increasing relation with opening displacement; (2) Damage softening stage: when interface stress reaches maximum strength, interface damage would germinate and evolve. At this stage, interface stress decreases linearly with the increase of opening displacement; (3) Failure stage: when opening displacement reaches critical failure value, interface stress drops to zero and interface completely fails.…”
Section: Computational Modelmentioning
confidence: 99%
“…In order to describe the mechanical properties of interfaces, the bilinear cohesive zone model (BCZM) was introduced in this work due to its highly efficient and simple formula. 18,35,[37][38][39] The BCZM theory assumes that interface mainly goes through three stages: (1) elastic stage: interface stress has a linear increasing relation with opening displacement; (2) Damage softening stage: when interface stress reaches maximum strength, interface damage would germinate and evolve. At this stage, interface stress decreases linearly with the increase of opening displacement; (3) Failure stage: when opening displacement reaches critical failure value, interface stress drops to zero and interface completely fails.…”
Section: Computational Modelmentioning
confidence: 99%
“…To provide a rationale on these experimental results, finite element simulations have been run on representative volume elements made of polyhedral particles randomly dispersed in a soft hyperelastic matrix with an account of possible matrix/filler interfacial damage thanks to CZM elements. A specific effort has been carried on the generation of representative microstructures with a relatively high volume fraction of fillers (up to 55%), randomly dispersed to avoid undesired anisotropy (de Francqueville et al, 2020b). Fillers are non regular polyhedra randomly translated and rotated to avoid possible numerical bias in damage appearance due to similar parallel edges facing each others.…”
Section: Micro-scale Observations Of the Matrix/filler Debondingmentioning
confidence: 99%
“…This provides with spherical displacement. The model equations are detailed in de Francqueville et al (2020b). For simplicity reasons and in order to reduce the number of adjustable parameters, the normal and tangent behaviors have been assumed similar.…”
Section: Computational Frameworkmentioning
confidence: 99%
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