SchmidCostaExponentialLaw2d Class Reference
#include <SchmidCostaExponentialLaw2d.hpp>
Public Member Functions | |
| SchmidCostaExponentialLaw2d () | |
| void | ComputeStressAndStressDerivative (c_matrix< double, 2, 2 > &rC, c_matrix< double, 2, 2 > &rInvC, double pressure, c_matrix< double, 2, 2 > &rT, FourthOrderTensor< 2 > &rDTdE, bool computeDTdE) |
| double | GetA () |
| std::vector< std::vector < double > > | GetB () |
| double | GetZeroStrainPressure () |
Private Attributes | |
| double | mA |
| std::vector< std::vector < double > > | mB |
| c_matrix< double, 2, 2 > | mIdentity |
Detailed Description
A 2d version of the material law in Costa, Holmes, McCulloch "Modelling Cardiac Mechanical Properties in Three Dimensions" Philo. Trans. R. Soc.W = aexp(Q-1) where Q = bff*Eff^2 + bfs*Efs^2 + bsf*Esf^2 + bss*Ess^2
where the parameters are taken from the fitting in Schmid,Nash,Young,Hunter "Myocardial Material Parameter Estimation - A Comparative Study for Simple Shear" Transactions of the ASME.
Definition at line 46 of file SchmidCostaExponentialLaw2d.hpp.
Constructor & Destructor Documentation
| SchmidCostaExponentialLaw2d::SchmidCostaExponentialLaw2d | ( | ) |
Constructor.
Definition at line 31 of file SchmidCostaExponentialLaw2d.cpp.
Member Function Documentation
| void SchmidCostaExponentialLaw2d::ComputeStressAndStressDerivative | ( | c_matrix< double, 2, 2 > & | rC, | |
| c_matrix< double, 2, 2 > & | rInvC, | |||
| double | pressure, | |||
| c_matrix< double, 2, 2 > & | rT, | |||
| FourthOrderTensor< 2 > & | rDTdE, | |||
| bool | computeDTdE | |||
| ) |
Compute the (2nd Piola Kirchoff) stress T and the stress derivative dT/dE for a given strain.
NOTE: the strain E is not expected to be passed in, instead the Lagrangian deformation tensor C is required (recall, E = 0.5(C-I))
dT/dE is a fourth-order tensor, where dT/dE[M][N][P][Q] = dT^{MN}/dE_{PQ}
- Parameters:
-
rC The Lagrangian deformation tensor (F^T F) rInvC The inverse of C. Should be computed by the user. (Change this?) pressure the current pressure rT the stress will be returned in this parameter rDTdE the stress derivative will be returned in this parameter, assuming the final parameter is true computeDTdE a boolean flag saying whether the stress derivative is required or not.
Definition at line 58 of file SchmidCostaExponentialLaw2d.cpp.
References mA, mB, mIdentity, and FourthOrderTensor< DIM >::Zero().
| double SchmidCostaExponentialLaw2d::GetA | ( | ) |
| std::vector< std::vector< double > > SchmidCostaExponentialLaw2d::GetB | ( | ) |
| double SchmidCostaExponentialLaw2d::GetZeroStrainPressure | ( | ) | [virtual] |
Get the pressure corresponding to E=0, ie C=identity.
Implements AbstractIncompressibleMaterialLaw< 2 >.
Definition at line 112 of file SchmidCostaExponentialLaw2d.cpp.
Member Data Documentation
double SchmidCostaExponentialLaw2d::mA [private] |
Parameter a.
Definition at line 51 of file SchmidCostaExponentialLaw2d.hpp.
Referenced by ComputeStressAndStressDerivative(), GetA(), and SchmidCostaExponentialLaw2d().
std::vector<std::vector<double> > SchmidCostaExponentialLaw2d::mB [private] |
Matrix of parameters b.
Definition at line 54 of file SchmidCostaExponentialLaw2d.hpp.
Referenced by ComputeStressAndStressDerivative(), GetB(), and SchmidCostaExponentialLaw2d().
c_matrix<double,2,2> SchmidCostaExponentialLaw2d::mIdentity [private] |
2D identity matrix.
Definition at line 57 of file SchmidCostaExponentialLaw2d.hpp.
Referenced by ComputeStressAndStressDerivative(), and SchmidCostaExponentialLaw2d().
The documentation for this class was generated from the following files:
- /tmp/release_1.1/pde/src/problem/common/SchmidCostaExponentialLaw2d.hpp
- /tmp/release_1.1/pde/src/problem/common/SchmidCostaExponentialLaw2d.cpp
