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Name: Victor Lefèvre
Type: User
Name: Victor Lefèvre
Type: User
This ABAQUS UHYPER subroutine implements the hyperelastic energy density derived in Journal of the Mechanics and Physics of Solids 99 (2017), 438-470 for the macroscopic elastic response of isotropic and incompressible filled elastomers. The results applies to general non-percolative isotropic distributions of stiff inclusions, stiff interphases, and stiff occluded rubber. This result is valid for any choice of I1-based incompressible energy density characterizing the non-Gaussian isotropic elastic response of the underlying elastomer. The present subroutine is implemented for the choice of strain energy density proposed in Comptes Rendus Mecanique 338 (2010), 3–11.
This ABAQUS UHYPER subroutine implements the hyperelastic energy density derived in Journal of the Mechanics and Physics of Solids 99 (2017), 438-470 for the macroscopic elastic response of isotropic and incompressible elastomers filled with liquid-like inclusions. The results applies to general non-percolative isotropic distributions of incompressible inclusion whith vanishing shear stiffness. This result is valid for any choice of I1-based incompressible energy density characterizing the non-Gaussian isotropic elastic response of the underlying elastomer. The present subroutine is implemented for the choice of strain energy density proposed in Comptes Rendus Mecanique 338 (2010), 3–11.
This ABAQUS UHYPER subroutine implements the hyperelastic energy density derived in Journal of the Mechanics and Physics of Solids 122 (2019), 364–380 for the macroscopic elastic response of non-Gaussian elastomers weakened by an isotropic and non-percolative distribution of equiaxed pores. This result is valid for any choice of I1-based incompressible energy density characterizing the non-Gaussian isotropic elastic response of the underlying elastomer. The present subroutine is implemented for the choice of strain energy density proposed in Comptes Rendus Mecanique 338 (2010), 3–11.
Abaqus UMAT subroutine for a large family of finite viscoelasticity models
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