Module hyperelastic

Module hyperelastic 

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Hyperelastic solid constitutive models.


Hyperelastic solid constitutive models are defined by a Helmholtz free energy density function of the deformation gradient.

\mathbf{P}:\dot{\mathbf{F}} - \dot{a}(\mathbf{F}) \geq 0

Satisfying the second law of thermodynamics (here, equivalent to extremized or zero dissipation) yields a relation for the stress.

\mathbf{P} = \frac{\partial a}{\partial\mathbf{F}}

Consequently, the tangent stiffness associated with the first Piola-Kirchhoff stress is symmetric for these constitutive models.

\mathcal{C}_{iJkL} = \mathcal{C}_{kLiJ}

Structs§

ArrudaBoyce
The Arruda-Boyce hyperelastic solid constitutive model.
Fung
The Fung hyperelastic solid constitutive model.
Gent
The Gent hyperelastic solid constitutive model.
Hencky
The Hencky hyperelastic solid constitutive model.
MooneyRivlin
The Mooney-Rivlin hyperelastic solid constitutive model.,
NeoHookean
The Neo-Hookean hyperelastic solid constitutive model.
SaintVenantKirchhoff
The Saint Venant-Kirchhoff hyperelastic solid constitutive model.
Yeoh
The Yeoh hyperelastic solid constitutive model.

Traits§

FirstOrderMinimize
First-order minimization methods for elastic solid constitutive models.
Hyperelastic
Required methods for hyperelastic solid constitutive models.
SecondOrderMinimize
Second-order minimization methods for elastic solid constitutive models.