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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 0Satisfying 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§
- Arruda
Boyce - 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.
- Mooney
Rivlin - The Mooney-Rivlin hyperelastic solid constitutive model.,
- NeoHookean
- The Neo-Hookean hyperelastic solid constitutive model.
- Saint
Venant Kirchhoff - The Saint Venant-Kirchhoff hyperelastic solid constitutive model.
- Yeoh
- The Yeoh hyperelastic solid constitutive model.
Traits§
- First
Order Minimize - First-order minimization methods for elastic solid constitutive models.
- Hyperelastic
- Required methods for hyperelastic solid constitutive models.
- Second
Order Minimize - Second-order minimization methods for elastic solid constitutive models.