AbstractIsotropicIncompressibleMaterialLaw.cpp

00001 /*
00002 
00003 Copyright (C) University of Oxford, 2005-2009
00004 
00005 University of Oxford means the Chancellor, Masters and Scholars of the
00006 University of Oxford, having an administrative office at Wellington
00007 Square, Oxford OX1 2JD, UK.
00008 
00009 This file is part of Chaste.
00010 
00011 Chaste is free software: you can redistribute it and/or modify it
00012 under the terms of the GNU Lesser General Public License as published
00013 by the Free Software Foundation, either version 2.1 of the License, or
00014 (at your option) any later version.
00015 
00016 Chaste is distributed in the hope that it will be useful, but WITHOUT
00017 ANY WARRANTY; without even the implied warranty of MERCHANTABILITY or
00018 FITNESS FOR A PARTICULAR PURPOSE.  See the GNU Lesser General Public
00019 License for more details. The offer of Chaste under the terms of the
00020 License is subject to the License being interpreted in accordance with
00021 English Law and subject to any action against the University of Oxford
00022 being under the jurisdiction of the English Courts.
00023 
00024 You should have received a copy of the GNU Lesser General Public License
00025 along with Chaste. If not, see <http://www.gnu.org/licenses/>.
00026 
00027 */
00028 
00029 #include "AbstractIsotropicIncompressibleMaterialLaw.hpp"
00030 
00031 template<unsigned DIM>
00032 AbstractIsotropicIncompressibleMaterialLaw<DIM>::~AbstractIsotropicIncompressibleMaterialLaw()
00033 {
00034 }
00035 
00036 template<unsigned DIM>
00037 void AbstractIsotropicIncompressibleMaterialLaw<DIM>::ComputeStressAndStressDerivative(
00038         c_matrix<double,DIM,DIM>& C,
00039         c_matrix<double,DIM,DIM>& invC,
00040         double                    pressure,
00041         c_matrix<double,DIM,DIM>& T,
00042         FourthOrderTensor2<DIM>&  dTdE,
00043         bool                      computeDTdE)
00044 {
00045     // this is covered, but gcov doesn't see this as being covered
00046     // for some reason, maybe because of optimisations
00047     #define COVERAGE_IGNORE
00048     assert((DIM==2) || (DIM==3));
00049     #undef COVERAGE_IGNORE
00050 
00051     static c_matrix<double,DIM,DIM> identity = identity_matrix<double>(DIM);
00052 
00053     double I1 = Trace(C);
00054     double I2 = SecondInvariant(C);
00055 
00056     double  dW_dI1 = Get_dW_dI1(I1,I2);
00057     double  dW_dI2; // only computed if DIM==3
00058 
00059     double  d2W_dI1;
00060     double  d2W_dI2;
00061     double  d2W_dI1I2;
00062 
00063     // Compute stress:
00064     //
00065     //  T = dW_dE
00066     //    = 2 * dI1_dC_MN * dI1_dC_MN   +   2 * dI1_dC_MN * dI1_dC_MN  -  p * invC
00067     //    = 2 * dI1_dC_MN * delta_MN    +   2 * dI1_dC_MN * (I1 delta_MN - C_MN)  -  p * invC
00068 
00069     T = 2*dW_dI1*identity - pressure*invC;
00070     if (DIM==3)
00071     {
00072         dW_dI2 = Get_dW_dI2(I1,I2);
00073         T += 2*dW_dI2*(I1*identity - C);
00074     }
00075 
00076 
00077     // Compute stress derivative if required:
00078     //
00079     // The stress derivative dT_{MN}/dE_{PQ} can be expanded to be seen to be
00080     //
00081     //  dT_dE =    4 * true_d2WdI1 * dI1_dC_MN * dI1_dC_PQ
00082     //           + 4 * true_dWdI1  * d2I1_dC2
00083     //           + 4 * true_d2WdI2 * dI2_dC_MN * dI2_dC_PQ
00084     //           + 4 * true_dWdI2  * d2I2_dC2
00085     //           + 4 * true_d2WdI1I2 * (dI1_dC_MN*dI2_dC_PQ + dI1_dC_PQ*dI2_dC_MN)
00086     //          - 2 * pressure * d_invC_dC;
00087     //
00088     // where
00089     //   dI1_dC_MN = (M==N); // ie delta_{MN}
00090     //   dI1_dC_PQ = (P==Q);
00091     //   d2I1_dC2  = 0;
00092     //
00093     //   dI2_dC_MN = I1*(M==N)-C[M][N];
00094     //   dI2_dC_PQ = I1*(P==Q)-C[P][Q];
00095     //   d2I2_dC2  = (M==N)*(P==Q)-(M==P)*(N==Q);
00096     //
00097     //   d_invC_dC = -invC[M][P]*invC[Q][N];
00098     if (computeDTdE)
00099     {
00100         d2W_dI1 = Get_d2W_dI1(I1,I2);
00101 
00102         if (DIM==3)
00103         {
00104             d2W_dI2   = Get_d2W_dI2(I1,I2);
00105             d2W_dI1I2 = Get_d2W_dI1I2(I1,I2);
00106         }
00107 
00108         for (unsigned M=0;M<DIM;M++)
00109         {
00110             for (unsigned N=0;N<DIM;N++)
00111             {
00112                 for (unsigned P=0;P<DIM;P++)
00113                 {
00114                     for (unsigned Q=0;Q<DIM;Q++)
00115                     {
00116                         dTdE(M,N,P,Q)  =    4 * d2W_dI1  * (M==N) * (P==Q)
00117                                           + 2 * pressure * invC(M,P) * invC(Q,N);
00118 
00119                         if (DIM==3)
00120                         {
00121                             dTdE(M,N,P,Q) +=    4 * d2W_dI2   * (I1*(M==N)-C(M,N)) * (I1*(P==Q)-C(P,Q))
00122                                               + 4 * dW_dI2    * ((M==N)*(P==Q)-(M==P)*(N==Q))
00123                                               + 4 * d2W_dI1I2 * ((M==N)*(I1*(P==Q)-C(P,Q)) + (P==Q)*(I1*(M==N)-C(M,N)));
00124                         }
00125                     }
00126                 }
00127             }
00128         }
00129     }
00130 }
00131 
00132 template<>
00133 double AbstractIsotropicIncompressibleMaterialLaw<2>::GetZeroStrainPressure()
00134 {
00135     return 2*Get_dW_dI1(2,0);
00136 }
00137 
00138 template<>
00139 double AbstractIsotropicIncompressibleMaterialLaw<3>::GetZeroStrainPressure()
00140 {
00141     return 2*Get_dW_dI1(3,3) + 4*Get_dW_dI2(3,3);
00142 }
00143 
00145 // Explicit instantiation
00147 
00148 template class AbstractIsotropicIncompressibleMaterialLaw<2>;
00149 template class AbstractIsotropicIncompressibleMaterialLaw<3>;

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