From: Jean-Paul Pelteret Date: Mon, 5 Dec 2016 09:26:31 +0000 (+0100) Subject: Step-44 now uses the newly implemented physics classes and functions. X-Git-Tag: v8.5.0-rc1~337^2 X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=refs%2Fpull%2F3034%2Fhead;p=dealii.git Step-44 now uses the newly implemented physics classes and functions. --- diff --git a/examples/step-44/step-44.cc b/examples/step-44/step-44.cc index 57a807e254..13f1616a36 100644 --- a/examples/step-44/step-44.cc +++ b/examples/step-44/step-44.cc @@ -72,6 +72,12 @@ #include #include +// Defined in these two headers are some operations that are pertinent to +// finite strain elasticity. The first will help us compute some kinematic +// quantities, and the second provides some stanard tensor definitions. +#include +#include + #include #include @@ -431,44 +437,6 @@ namespace Step44 } } -// @sect3{Some standard tensors} - -// Now we define some frequently used second and fourth-order tensors: - template - class StandardTensors - { - public: - - // $\mathbf{I}$ - static const SymmetricTensor<2, dim> I; - // $\mathbf{I} \otimes \mathbf{I}$ - static const SymmetricTensor<4, dim> IxI; - // $\mathcal{S}$, note that as we only use this fourth-order unit tensor - // to operate on symmetric second-order tensors. To maintain notation - // consistent with Holzapfel (2001) we name the tensor $\mathcal{I}$ - static const SymmetricTensor<4, dim> II; - // Fourth-order deviatoric tensor such that - // $\textrm{dev} \{ \bullet \} = \{ \bullet \} - - // [1/\textrm{dim}][ \{ \bullet\} :\mathbf{I}]\mathbf{I}$ - static const SymmetricTensor<4, dim> dev_P; - }; - - template - const SymmetricTensor<2, dim> - StandardTensors::I = unit_symmetric_tensor(); - - template - const SymmetricTensor<4, dim> - StandardTensors::IxI = outer_product(I, I); - - template - const SymmetricTensor<4, dim> - StandardTensors::II = identity_tensor(); - - template - const SymmetricTensor<4, dim> - StandardTensors::dev_P = deviator_tensor(); - // @sect3{Time class} // A simple class to store time data. Its functioning is transparent so no @@ -560,7 +528,7 @@ namespace Step44 det_F(1.0), p_tilde(0.0), J_tilde(1.0), - b_bar(StandardTensors::I) + b_bar(Physics::Elasticity::StandardTensors::I) { Assert(kappa > 0, ExcInternalError()); } @@ -577,7 +545,8 @@ namespace Step44 const double J_tilde_in) { det_F = determinant(F); - b_bar = std::pow(det_F, -2.0 / dim) * symmetrize(F * transpose(F)); + const Tensor<2, dim> F_bar = Physics::Elasticity::Kinematics::F_iso(F); + b_bar = Physics::Elasticity::Kinematics::b(F_bar); p_tilde = p_tilde_in; J_tilde = J_tilde_in; @@ -653,7 +622,7 @@ namespace Step44 // volumetric Kirchhoff stress $\boldsymbol{\tau}_{\textrm{vol}}$: SymmetricTensor<2, dim> get_tau_vol() const { - return p_tilde * det_F * StandardTensors::I; + return p_tilde * det_F * Physics::Elasticity::StandardTensors::I; } // Next, determine the isochoric Kirchhoff stress @@ -661,7 +630,7 @@ namespace Step44 // \mathcal{P}:\overline{\boldsymbol{\tau}}$: SymmetricTensor<2, dim> get_tau_iso() const { - return StandardTensors::dev_P * get_tau_bar(); + return Physics::Elasticity::StandardTensors::dev_P * get_tau_bar(); } // Then, determine the fictitious Kirchhoff stress @@ -677,8 +646,8 @@ namespace Step44 { return p_tilde * det_F - * ( StandardTensors::IxI - - (2.0 * StandardTensors::II) ); + * ( Physics::Elasticity::StandardTensors::IxI + - (2.0 * Physics::Elasticity::StandardTensors::S) ); } // Calculate the isochoric part of the tangent $J @@ -689,17 +658,17 @@ namespace Step44 const SymmetricTensor<2, dim> tau_iso = get_tau_iso(); const SymmetricTensor<4, dim> tau_iso_x_I = outer_product(tau_iso, - StandardTensors::I); + Physics::Elasticity::StandardTensors::I); const SymmetricTensor<4, dim> I_x_tau_iso - = outer_product(StandardTensors::I, + = outer_product(Physics::Elasticity::StandardTensors::I, tau_iso); const SymmetricTensor<4, dim> c_bar = get_c_bar(); return (2.0 / dim) * trace(tau_bar) - * StandardTensors::dev_P + * Physics::Elasticity::StandardTensors::dev_P - (2.0 / dim) * (tau_iso_x_I + I_x_tau_iso) - + StandardTensors::dev_P * c_bar - * StandardTensors::dev_P; + + Physics::Elasticity::StandardTensors::dev_P * c_bar + * Physics::Elasticity::StandardTensors::dev_P; } // Calculate the fictitious elasticity tensor $\overline{\mathfrak{c}}$. @@ -724,7 +693,7 @@ namespace Step44 public: PointHistory() : - F_inv(StandardTensors::I), + F_inv(Physics::Elasticity::StandardTensors::I), tau(SymmetricTensor<2, dim>()), d2Psi_vol_dJ2(0.0), dPsi_vol_dJ(0.0), @@ -764,9 +733,7 @@ namespace Step44 const double p_tilde, const double J_tilde) { - const Tensor<2, dim> F - = (Tensor<2, dim>(StandardTensors::I) + - Grad_u_n); + const Tensor<2, dim> F = Physics::Elasticity::Kinematics::F(Grad_u_n); material->update_material_data(F, p_tilde, J_tilde); // The material has been updated so we now calculate the Kirchhoff @@ -2275,7 +2242,7 @@ namespace Step44 { data.cell_matrix(i, j) += N[i] * det_F * (symm_grad_Nx[j] - * StandardTensors::I) + * Physics::Elasticity::StandardTensors::I) * JxW; } // and lastly the $\mathsf{\mathbf{k}}_{ \widetilde{J} \widetilde{p}}$