Implementation of the Saint Venant-Kirchhoff material model.The energy is computed as. More...
#include <ikarus/finiteelements/mechanics/materials/svk.hh>
Public Types | |
using | ScalarType = ST |
using | StrainMatrix = Eigen::Matrix< ScalarType, worldDimension, worldDimension > |
using | StressMatrix = StrainMatrix |
using | MaterialParameters = LamesFirstParameterAndShearModulus |
using | MaterialImpl = StVenantKirchhoffT< ST > |
Type of material implementation. More... | |
Public Member Functions | |
StVenantKirchhoffT (const MaterialParameters &mpt) | |
Constructor for StVenantKirchhoffT. More... | |
MaterialParameters | materialParametersImpl () const |
Returns the material parameters stored in the material. More... | |
template<typename Derived > | |
ScalarType | storedEnergyImpl (const Eigen::MatrixBase< Derived > &E) const |
Computes the stored energy in the Saint Venant-Kirchhoff material model. More... | |
template<bool voigt, typename Derived > | |
auto | stressesImpl (const Eigen::MatrixBase< Derived > &E) const |
Computes the stresses in the Saint Venant-Kirchhoff material model. More... | |
template<bool voigt, typename Derived > | |
auto | tangentModuliImpl (const Eigen::MatrixBase< Derived > &E) const |
Computes the tangent moduli in the Saint Venant-Kirchhoff material model. More... | |
template<typename ScalarTypeOther > | |
auto | rebind () const |
Rebinds the material to a different scalar type. More... | |
constexpr const MaterialImpl & | impl () const |
Const accessor to the underlying material (CRTP). More... | |
constexpr MaterialImpl & | impl () |
Accessor to the underlying material (CRTP). More... | |
auto | materialParameters () const |
Returns the material parameters stored in the implemented material. More... | |
auto | storedEnergy (const Eigen::MatrixBase< Derived > &Eraw) const |
Return the stored potential energy of the material. More... | |
auto | stresses (const Eigen::MatrixBase< Derived > &Eraw) const |
Get the stresses of the material. More... | |
auto | tangentModuli (const Eigen::MatrixBase< Derived > &Eraw) const |
Get the tangentModuli of the material. More... | |
Static Public Member Functions | |
static constexpr std::string | nameImpl () |
static constexpr std::string | name () |
Get the name of the implemented material. More... | |
Static Public Attributes | |
static constexpr int | worldDimension = 3 |
static constexpr auto | strainTag = StrainTags::greenLagrangian |
static constexpr auto | stressTag = StressTags::PK2 |
static constexpr auto | tangentModuliTag = TangentModuliTags::Material |
static constexpr bool | energyAcceptsVoigt = true |
static constexpr bool | stressToVoigt = true |
static constexpr bool | stressAcceptsVoigt = true |
static constexpr bool | moduliToVoigt = true |
static constexpr bool | moduliAcceptsVoigt = true |
static constexpr double | derivativeFactorImpl = 1 |
static constexpr bool | isReduced |
Static constant for determining if the material has vanishing stress or strain components (is reduced). More... | |
static constexpr double | derivativeFactor |
This factor denotes the differences between the returned stresses and moduli and the passed strain. More... | |
\[ \psi(\BE) = \frac{\lambda}{2} (\tr \BE)^2 +\mu \tr (\BE^2) ,\]
where \( \BE \) denotes the Green-Lagrangian strain.
The second Piola-Kirchhoff stresses are computed as
\[ \BS(\BE) =\fracpt{\psi(\BE)}{\BE} = \lambda \tr \BE \BI +2 \mu \BE,\]
and the material tangent moduli are computed as
\[ \BBC(\BE) =\fracpt{^2\psi(\BE)}{\BE^2} = \lambda \tr \BE \CI +2 \mu \CI^{\mathrm{sym}},\]
where \( \CI_{IJKL} = \de_{IJ}\de_{KL}\) and \( \CI_{IJKL}^\mathrm{sym} = \frac{1}{2}(\de_{IK}\de_{JL}+ \de_{IL}\de_{JK})\).
ST | The scalar type used in the material. |
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inherited |
using Ikarus::StVenantKirchhoffT< ST >::MaterialParameters = LamesFirstParameterAndShearModulus |
using Ikarus::StVenantKirchhoffT< ST >::ScalarType = ST |
using Ikarus::StVenantKirchhoffT< ST >::StrainMatrix = Eigen::Matrix<ScalarType, worldDimension, worldDimension> |
using Ikarus::StVenantKirchhoffT< ST >::StressMatrix = StrainMatrix |
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mpt | The material parameters (Lamé's first parameter and shear modulus). |
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ScalarTypeOther | The target scalar type. |
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This function return the free Helmholtz energy of the material
tag | Strain tag indicating which strain tensor components are passed. |
Derived | The underlying Eigen type. |
Eraw | The strain tensor components passed in Voigt notation or matrix notation. |
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Derived | The derived type of the input matrix. |
E | The Green-Lagrangian strain. |
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tag | Strain tag indicating which strain tensor components are passed. |
voigt | Boolean indicating whether to return Voigt-shaped result. |
Derived | The underlying Eigen type. |
Eraw | The strain tensor components passed in Voigt notation or matrix notation. |
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voigt | A boolean indicating whether to return stresses in Voigt notation. |
Derived | The derived type of the input matrix. |
E | The Green-Lagrangian strain. |
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tag | Strain tag indicating which strain tensor components are passed. |
voigt | Boolean indicating whether to return Voigt-shaped result. |
Derived | The underlying Eigen type. |
Eraw | The strain tensor components passed in Voigt notation or matrix notation. |
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voigt | A boolean indicating whether to return tangent moduli in Voigt notation. |
Derived | The derived type of the input matrix. |
E | The Green-Lagrangian strain. |
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For neoHooke the inserted quantity is $C$ the Green-Lagrangian strain tensor, the function relation between the energy and the stresses is $S = 1 \dfrac{\partial\psi(E)}{\partial E}$. This factor is the pre factor, which is the difference to the actual derivative, which is written here
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