#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, 2, 2, 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 |
W = a[exp(Q)-1]/2 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.
Note, by default, the fibre direction is assumed to be THE X-DIRECTION, and the sheet direction the Y-DIRECTION (ie sheets in the XY plane). Call SetChangeOfBasisMatrix() before ComputeStressAndStressDerivative(), with the matrix P = [fibre_vec, sheet_vec, normal_vec] if this is not the case.
Definition at line 51 of file SchmidCostaExponentialLaw2d.hpp.
SchmidCostaExponentialLaw2d::SchmidCostaExponentialLaw2d | ( | ) |
Constructor.
Definition at line 31 of file SchmidCostaExponentialLaw2d.cpp.
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, 2, 2, 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}
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 59 of file SchmidCostaExponentialLaw2d.cpp.
References AbstractMaterialLaw< DIM >::ComputeTransformedDeformationTensor(), mA, mB, mIdentity, AbstractMaterialLaw< DIM >::TransformStressAndStressDerivative(), and FourthOrderTensor< DIM1, DIM2, DIM3, DIM4 >::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 129 of file SchmidCostaExponentialLaw2d.cpp.
double SchmidCostaExponentialLaw2d::mA [private] |
Parameter a. (kPa)
Definition at line 56 of file SchmidCostaExponentialLaw2d.hpp.
Referenced by ComputeStressAndStressDerivative(), GetA(), and SchmidCostaExponentialLaw2d().
std::vector<std::vector<double> > SchmidCostaExponentialLaw2d::mB [private] |
Matrix of parameters b (dimensionless).
Definition at line 59 of file SchmidCostaExponentialLaw2d.hpp.
Referenced by ComputeStressAndStressDerivative(), GetB(), and SchmidCostaExponentialLaw2d().
c_matrix<double,2,2> SchmidCostaExponentialLaw2d::mIdentity [private] |
2D identity matrix.
Definition at line 62 of file SchmidCostaExponentialLaw2d.hpp.
Referenced by ComputeStressAndStressDerivative(), and SchmidCostaExponentialLaw2d().