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//! Hyperviscoelastic solid constitutive models.
//!
//! ---
//!
//! Hyperviscoelastic solid constitutive models are defined by a Helmholtz free energy density and a viscous dissipation function.
//!
//! ```math
//! \mathbf{P}:\dot{\mathbf{F}} - \dot{a}(\mathbf{F}) - \phi(\mathbf{F},\dot{\mathbf{F}}) \geq 0
//! ```
//! Satisfying the second law of thermodynamics though a minimum viscous dissipation principal yields a relation for the stress.
//!
//! ```math
//! \mathbf{P} = \frac{\partial a}{\partial\mathbf{F}} + \frac{\partial\phi}{\partial\dot{\mathbf{F}}}
//! ```
//! Consequently, the rate tangent stiffness associated with the first Piola-Kirchhoff stress is symmetric for these constitutive models.
//!
//! ```math
//! \mathcal{U}_{iJkL} = \mathcal{U}_{kLiJ}
//! ```
pub use SaintVenantKirchhoff;
use ;
/// Required methods for hyperviscoelastic solid constitutive models.