We study three “incompressibility flavors” of linearly-elastic anisotropic solids that exhibit volumetric constraints: isochoric, hydroisochoric and rigidtropic. An isochoric material deforms without volume change under any stress system. An hydroisochoric material does so under hydrostatic stress. A rigidtropic material undergoes zero deformations under a certain stress pattern. Whereas the three models coalesce for isotropic materials, important differences appear for anisotropic behavior. We find that isochoric and hydroisochoric models under certain conditions may be hampered by unstable physical behavior. Rigidtropic models can represent semistable physical materials of arbitrary anisotropy while including isochoric and hyd...
For a given class of materials, universal deformations are those that can be maintained in the absen...
Incompressible nonlinearly hyperelastic materials are rarely simulated in finite element numerical e...
We present a set of explicit conditions, involving the components of the elastic stiffness tensor, w...
We study three “incompressibility flavors” of linearly-elastic anisotropic solids that e...
We define stress and strain splittings appropriate to linearly elastic anisotropic materia...
In order to avoid the numerical difficulties in locally enforcing the incompressibility constraint u...
An investigation for directions of extreme - maximum or minimum - values of the longitudinal and tra...
We give conditions on the strain–energy function of nonlinear anisotropic hyperelastic materials tha...
The Holzapfel–Gasser–Ogden (HGO) model for anisotropic hyperelas-tic behaviour of collagen fibre rei...
Abstract We give conditions on the strain–energy function of nonlinear anisotropic hyperelastic mate...
AbstractA new notion of stability for compressible, transversely isotropic hyperelastic, nonlinear m...
We give conditions on the strain-energy function of nonlinear anisotropic hyperelastic materials tha...
AbstractA material is of coaxial type if the Cauchy stress tensor T and the strain tensor B are coax...
Anisotropic elastic materials, such as homogenized model of fiber-reinforced matrix, can display nea...
Universal deformations of an elastic solid are deformations that can be achieved for all possible st...
For a given class of materials, universal deformations are those that can be maintained in the absen...
Incompressible nonlinearly hyperelastic materials are rarely simulated in finite element numerical e...
We present a set of explicit conditions, involving the components of the elastic stiffness tensor, w...
We study three “incompressibility flavors” of linearly-elastic anisotropic solids that e...
We define stress and strain splittings appropriate to linearly elastic anisotropic materia...
In order to avoid the numerical difficulties in locally enforcing the incompressibility constraint u...
An investigation for directions of extreme - maximum or minimum - values of the longitudinal and tra...
We give conditions on the strain–energy function of nonlinear anisotropic hyperelastic materials tha...
The Holzapfel–Gasser–Ogden (HGO) model for anisotropic hyperelas-tic behaviour of collagen fibre rei...
Abstract We give conditions on the strain–energy function of nonlinear anisotropic hyperelastic mate...
AbstractA new notion of stability for compressible, transversely isotropic hyperelastic, nonlinear m...
We give conditions on the strain-energy function of nonlinear anisotropic hyperelastic materials tha...
AbstractA material is of coaxial type if the Cauchy stress tensor T and the strain tensor B are coax...
Anisotropic elastic materials, such as homogenized model of fiber-reinforced matrix, can display nea...
Universal deformations of an elastic solid are deformations that can be achieved for all possible st...
For a given class of materials, universal deformations are those that can be maintained in the absen...
Incompressible nonlinearly hyperelastic materials are rarely simulated in finite element numerical e...
We present a set of explicit conditions, involving the components of the elastic stiffness tensor, w...