Chaste Commit::ca8ccdedf819b6e02855bc0e8e6f50bdecbc5208
AbstractIsotropicCompressibleMaterialLaw.cpp
1/*
2
3Copyright (c) 2005-2024, University of Oxford.
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34*/
35
36#include "AbstractIsotropicCompressibleMaterialLaw.hpp"
37
38template<unsigned DIM>
42
43template<unsigned DIM>
45 c_matrix<double,DIM,DIM>& rInvC,
46 double pressure,
47 c_matrix<double,DIM,DIM>& rT,
49 bool computeDTdE)
50{
51 /*
52 * This is covered, but gcov doesn't see this as being covered
53 * because it runs at compile time checking templates I think.
54 */
55 assert((DIM==2) || (DIM==3)); // LCOV_EXCL_LINE
56 assert(pressure==0.0);
57
58 static c_matrix<double,DIM,DIM> identity = identity_matrix<double>(DIM);
59
60 double I1 = Trace(rC);
61 double I2 = SecondInvariant(rC);
62 double I3 = Determinant(rC);
63
64 static c_matrix<double,DIM,DIM> dI2dC;
65 dI2dC = I1*identity - rC; // MUST be on separate line to above!
66
67 double w1 = Get_dW_dI1(I1,I2,I3);
68 double w2 = Get_dW_dI2(I1,I2,I3);
69 double w3 = Get_dW_dI3(I1,I2,I3);
70
71
72 // Compute stress: **** See FiniteElementImplementations document. ****
73 //
74 // T = dW_dE
75 // = 2 dW_dC
76 // = 2 ( w1 dI1/dC + w2 dI2/dC + w3 dI3/dC )
77 // = 2 ( w1 I + w2 (I1*I - C) + w3 I3 inv(C) )
78 //
79 // where w1 = dW/dI1, etc
80 //
81 rT = 2*w1*identity + 2*w3*I3*rInvC;
82 if (DIM==3)
83 {
84 rT += 2*w2*dI2dC;
85 }
86
87 // Compute stress derivative if required: **** See FiniteElementImplementations document. ****
88 //
89 // The stress derivative dT_{MN}/dE_{PQ} is
90 //
91 //
92 // dT_dE = 2 dT_dC
93 // = 4 d/dC ( w1 I + w2 (I1*I - C) + w3 I3 inv(C) )
94 // so (in the following ** represents outer product):
95 // (1/4) dT_dE = w11 I**I + w12 I**(I1*I-C) + w13 I**inv(C)
96 // + w21 (I1*I-C)**I + w22 (I1*I-C)**(I1*I-C) + w23 (I1*I-C)**inv(C) + w2 (I**I - dC/dC)
97 // + w31 I3 inv(C)**I + w32 I3 inv(C)**(I1*I-C) + (w33 I3 + w3) inv(C)**inv(C) + w3 d(invC)/dC
98 //
99 // Here, I**I represents the tensor A[M][N][P][Q] = (M==N)*(P==Q) // ie delta(M,N)delta(P,Q), etc
100 //
101
102 if (computeDTdE)
103 {
104 double w11 = Get_d2W_dI1(I1,I2,I3);
105 double w22 = Get_d2W_dI2(I1,I2,I3);
106 double w33 = Get_d2W_dI3(I1,I2,I3);
107
108 double w23 = Get_d2W_dI2I3(I1,I2,I3);
109 double w13 = Get_d2W_dI1I3(I1,I2,I3);
110 double w12 = Get_d2W_dI1I2(I1,I2,I3);
111
112 for (unsigned M=0; M<DIM; M++)
113 {
114 for (unsigned N=0; N<DIM; N++)
115 {
116 for (unsigned P=0; P<DIM; P++)
117 {
118 for (unsigned Q=0; Q<DIM; Q++)
119 {
120 rDTdE(M,N,P,Q) = 4 * w11 * (M==N) * (P==Q)
121 + 4 * w13 * I3 * ( (M==N) * rInvC(P,Q) + rInvC(M,N)*(P==Q) ) // the w13 and w31 terms
122 + 4 * (w33*I3 + w3) * I3 * rInvC(M,N) * rInvC(P,Q)
123 - 4 * w3 * I3 * rInvC(M,P) * rInvC(Q,N);
124
125 if (DIM==3)
126 {
127 rDTdE(M,N,P,Q) += 4 * w22 * dI2dC(M,N) * dI2dC(P,Q)
128 + 4 * w12 * ((M==N)*dI2dC(P,Q) + (P==Q)*dI2dC(M,N)) // the w12 and w21 terms
129 + 4 * w23 * I3 * ( dI2dC(M,N)*rInvC(P,Q) + rInvC(M,N)*dI2dC(P,Q)) // the w23 and w32 terms
130 + 4 * w2 * ((M==N)*(P==Q) - (M==P)*(N==Q));
131 }
132 }
133 }
134 }
135 }
136 }
137}
138
139// Explicit instantiation
T Determinant(const boost::numeric::ublas::c_matrix< T, 1, 1 > &rM)
T SecondInvariant(const c_matrix< T, 3, 3 > &rM)
T Trace(const c_matrix< T, 1, 1 > &rM)
void ComputeStressAndStressDerivative(c_matrix< double, DIM, DIM > &rC, c_matrix< double, DIM, DIM > &rInvC, double pressure, c_matrix< double, DIM, DIM > &rT, FourthOrderTensor< DIM, DIM, DIM, DIM > &rDTdE, bool computeDTdE)