thermo.cc

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//LIC// ====================================================================
//LIC// This file forms part of oomph-lib, the object-oriented, 
//LIC// multi-physics finite-element library, available 
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//LIC// 
//LIC//    Version 1.0; svn revision $LastChangedRevision$
//LIC//
//LIC// $LastChangedDate$
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//LIC// Copyright (C) 2006-2016 Matthias Heil and Andrew Hazel
//LIC// 
//LIC// This library is free software; you can redistribute it and/or
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//LIC// version 2.1 of the License, or (at your option) any later version.
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//LIC// Lesser General Public License for more details.
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//LIC// The authors may be contacted at oomph-lib@maths.man.ac.uk.
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//LIC//====================================================================
//Driver for a multi-physics problem that couples the 
//unsteady heat equation to the equations of large-displacement solid
//mechanics

//Oomph-lib headers, we require the generic, unsteady heat
//and and elements.
#include "generic.h"
#include "solid.h"
#include "unsteady_heat.h"

// The mesh is our standard rectangular quadmesh
#include "meshes/rectangular_quadmesh.h"

// Use the oomph and std namespaces 
using namespace oomph;
using namespace std;



//=====================================================================
/// A class that solves the equations of steady thermoelasticity by 
/// combining the UnsteadyHeat and PVD equations into a single element.
/// A temperature-dependent growth term is added to the PVD equations by
/// overloading the member function get_istotropic_growth()
//======================class definition==============================
template<unsigned DIM>
class QThermalPVDElement : public virtual QPVDElement<DIM,3>,
                           public virtual QUnsteadyHeatElement<DIM,3>
{
private:

 /// Pointer to a private data member, the thermal expansion coefficient
 double* Alpha_pt;
 
 /// The static default value of Alpha
 static double Default_Physical_Constant_Value;

public:
 /// \short Constructor: call the underlying constructors and 
 /// initialise the pointer to Alpha to point
 /// to the default value of 1.0.
 QThermalPVDElement() : QPVDElement<DIM,3>(),
                        QUnsteadyHeatElement<DIM,3>() 
  {
   Alpha_pt = &Default_Physical_Constant_Value;
  }

 ///\short The required number of values stored at the nodes is the sum of the
 ///required values of the two single-physics elements. Note that this step is
 ///generic for any multi-physics element of this type.
 unsigned required_nvalue(const unsigned &n) const
  {return (QUnsteadyHeatElement<DIM,3>::required_nvalue(n) +
           QPVDElement<DIM,3>::required_nvalue(n));}

 ///Access function for the thermal expansion coefficient (const version)
 const double &alpha() const {return *Alpha_pt;}

 ///Access function for the pointer to the thermal expansion coefficientr
 double* &alpha_pt() {return Alpha_pt;}
  
 ///  Overload the standard output function with the broken default
 void output(ostream &outfile) {FiniteElement::output(outfile);}

 /// \short Output function:  
 ///  Output x, y, u, v, p, theta at Nplot^DIM plot points
 // Start of output function
 void output(ostream &outfile, const unsigned &nplot)
  {
   //vector of local coordinates
   Vector<double> s(DIM);
   Vector<double> xi(DIM);
   
   // Tecplot header info
   outfile << this->tecplot_zone_string(nplot);
   
   // Loop over plot points
   unsigned num_plot_points=this->nplot_points(nplot);
   for (unsigned iplot=0;iplot<num_plot_points;iplot++)
    {
     // Get local coordinates of plot point
     this->get_s_plot(iplot,nplot,s);
     
     // Get the Lagrangian coordinate
     this->interpolated_xi(s,xi);

     // Output the position of the plot point
     for(unsigned i=0;i<DIM;i++) 
      {outfile << this->interpolated_x(s,i) << " ";}

     // Output the temperature (the advected variable) at the plot point
     outfile << this->interpolated_u_ust_heat(s) << std::endl;   
    }
   outfile << std::endl;
   
   // Write tecplot footer (e.g. FE connectivity lists)
   this->write_tecplot_zone_footer(outfile,nplot);
  } //End of output function

 /// \short C-style output function: Broken default
 void output(FILE* file_pt)
  {FiniteElement::output(file_pt);}

 ///  \short C-style output function: Broken default
 void output(FILE* file_pt, const unsigned &n_plot)
  {FiniteElement::output(file_pt,n_plot);}

 /// \short Output function for an exact solution: Broken default
 void output_fct(ostream &outfile, const unsigned &Nplot,
                 FiniteElement::SteadyExactSolutionFctPt 
                 exact_soln_pt)
  {FiniteElement::output_fct(outfile,Nplot,exact_soln_pt);}


 /// \short Output function for a time-dependent exact solution:
 /// Broken default.
 void output_fct(ostream &outfile, const unsigned &Nplot,
                 const double& time,
                 FiniteElement::UnsteadyExactSolutionFctPt 
                 exact_soln_pt)
  {
   FiniteElement::
    output_fct(outfile,Nplot,time,exact_soln_pt);
  }
  
 /// \short Compute norm of solution: use the version in the unsteady heat
 /// class 
 void compute_norm(double& el_norm)
 {
  QUnsteadyHeatElement<DIM,3>::compute_norm(el_norm);
 }

 /// \short Validate against exact solution at given time
 /// Solution is provided via function pointer.
 /// Plot at a given number of plot points and compute L2 error
 /// and L2 norm of velocity solution over element
 /// Call the broken default
 void compute_error(ostream &outfile,
                    FiniteElement::UnsteadyExactSolutionFctPt exact_soln_pt,
                    const double& time,
                    double& error, double& norm)
  {FiniteElement::compute_error(outfile,exact_soln_pt,
                                time,error,norm);}
 
 /// \short Validate against exact solution.
 /// Solution is provided via function pointer.
 /// Plot at a given number of plot points and compute L2 error
 /// and L2 norm of velocity solution over element
 /// Call the broken default
 void compute_error(ostream &outfile,
                    FiniteElement::SteadyExactSolutionFctPt exact_soln_pt,
                    double& error, double& norm)
  {FiniteElement::compute_error(outfile,exact_soln_pt,error,norm);}

 /// \short Overload the growth function in the advection-diffusion equations.
 /// to be temperature-dependent.
 void get_isotropic_growth(const unsigned& ipt, const Vector<double> &s, 
                           const Vector<double>& xi, double &gamma) const
 {
  //The growth is the undeformed coefficient plus linear thermal
  //expansion
  gamma = 1.0 + (*Alpha_pt)*this->interpolated_u_ust_heat(s);
 }
 
 /// \short Calculate the contribution to the residual vector.
 /// We assume that the vector has been initialised to zero
 /// before this function is called.
 void fill_in_contribution_to_residuals(Vector<double> &residuals)
  {
   //Call the residuals of the advection-diffusion eqautions
   UnsteadyHeatEquations<DIM>::
    fill_in_contribution_to_residuals(residuals);
   //Call the residuals of the Navier-Stokes equations
   PVDEquations<DIM>::
    fill_in_contribution_to_residuals(residuals);
  }

 ///\short Compute the element's residual Vector and the jacobian matrix
 /// We assume that the residuals vector and jacobian matrix have been
 /// initialised to zero before calling this function
 void fill_in_contribution_to_jacobian(Vector<double> &residuals,
                                       DenseMatrix<double> &jacobian)
  {
   //Just call standard finite difference for a SolidFiniteElement so 
   //that variations in the nodal positions are taken into account
   SolidFiniteElement::fill_in_contribution_to_jacobian(residuals,jacobian);
  }

};

//=========================================================================
/// Set the default physical value to be one
//=========================================================================
template<>
double QThermalPVDElement<2>::Default_Physical_Constant_Value=1.0;

//======start_of_namespace============================================
/// Namespace for the physical parameters in the problem
//====================================================================
namespace Global_Physical_Variables
{
 /// Thermal expansion coefficient 
 double Alpha=0.0;
 
 /// Young's modulus for solid mechanics
 double E = 1.0; // ADJUST 

 /// Poisson ratio for solid mechanics
 double Nu = 0.3; // ADJUST

 /// We need a constitutive law for the solid mechanics
 ConstitutiveLaw* Constitutive_law_pt;

} // end_of_namespace

//////////////////////////////////////////////////////////////////////
//////////////////////////////////////////////////////////////////////
//////////////////////////////////////////////////////////////////////

//====== start_of_problem_class=======================================
/// 2D Thermoelasticity problem on rectangular domain, discretised 
/// with refineable elements. The specific type
/// of element is specified via the template parameter.
//====================================================================
template<class ELEMENT> 
class ThermalProblem : public Problem
{

public:

 ///Constructor
 ThermalProblem();

 /// Destructor. Empty
 ~ThermalProblem() {}

 /// \short Update the problem specs before solve (empty)
 void actions_before_newton_solve() {}

 /// Update the problem after solve (empty)
 void actions_after_newton_solve(){}

 /// Actions before adapt:(empty)
 void actions_before_adapt(){}
 
 /// \short Doc the solution.
 void doc_solution();

 /// \short Overloaded version of the problem's access function to 
 /// the mesh. Recasts the pointer to the base Mesh object to 
 /// the actual mesh type.
 ElasticRectangularQuadMesh<ELEMENT>* mesh_pt() 
  {
   return dynamic_cast<ElasticRectangularQuadMesh<ELEMENT>*>(
    Problem::mesh_pt());
  }
 
private:
 
 /// DocInfo object
 DocInfo Doc_info;

}; // end of problem class

//========================================================================
/// \short Constructor for Convection problem
//========================================================================
template<class ELEMENT>
ThermalProblem<ELEMENT>::ThermalProblem()
{
 // Set output directory
 Doc_info.set_directory("RESLT");
 
 // # of elements in x-direction
 unsigned n_x=8;

 // # of elements in y-direction
 unsigned n_y=8;
 
 // Domain length in x-direction
 double l_x=3.0;

 // Domain length in y-direction
 double l_y=1.0;

 // Build a standard rectangular quadmesh
 Problem::mesh_pt() = 
  new ElasticRectangularQuadMesh<ELEMENT>(n_x,n_y,l_x,l_y);

 // Set the boundary conditions for this problem: All nodes are
 // free by default -- only need to pin the ones that have Dirichlet 
 // conditions here
 {
  //The temperature is prescribed on the lower boundary
  unsigned n_boundary_node = mesh_pt()->nboundary_node(0);
  for(unsigned n=0;n<n_boundary_node;n++)
   {
    //Get the pointer to the node
    Node* nod_pt = mesh_pt()->boundary_node_pt(0,n);
    //Pin the temperature at the node 
    nod_pt->pin(0);
    //Set the temperature to 0.0 (cooled)
    nod_pt->set_value(0,0.0);
   }
  
  //The temperature is prescribed on the upper boundary
  n_boundary_node = mesh_pt()->nboundary_node(2);
  for(unsigned n=0;n<n_boundary_node;n++)
   {
    Node* nod_pt = mesh_pt()->boundary_node_pt(2,n);
    //Pin the temperature at the node
    nod_pt->pin(0);
    //Set the temperature to 1.0 (heated)
    nod_pt->set_value(0,1.0);
   }
  
  //The horizontal-position is fixed on the vertical boundary (symmetry)
  n_boundary_node = mesh_pt()->nboundary_node(1);
  for(unsigned n=0;n<n_boundary_node;n++)
   {
    static_cast<SolidNode*>(mesh_pt()->boundary_node_pt(1,n))->pin_position(0);
   }
  
  //We need to completely fix the lower-right corner of the block to 
  //prevent vertical rigid-body motions
  static_cast<SolidNode*>(mesh_pt()->boundary_node_pt(1,0))->pin_position(1);
 }

 // Complete the build of all elements so they are fully functional 

 // Loop over the elements to set up element-specific 
 // things that cannot be handled by the (argument-free!) ELEMENT 
 // constructor.
 unsigned n_element = mesh_pt()->nelement();
 for(unsigned int i=0;i<n_element;i++)
  {
   // Upcast from GeneralsedElement to the present element
   ELEMENT *el_pt = dynamic_cast<ELEMENT*>(mesh_pt()->element_pt(i));

   // Set the coefficient of thermal expansion
   el_pt->alpha_pt() = &Global_Physical_Variables::Alpha;

   // Set a constitutive law
   el_pt->constitutive_law_pt() = 
    Global_Physical_Variables::Constitutive_law_pt;
  }

 // Setup equation numbering scheme
 cout <<"Number of equations: " << assign_eqn_numbers() << endl; 

} // end of constructor


//========================================================================
/// Doc the solution
//========================================================================
template<class ELEMENT>
void ThermalProblem<ELEMENT>::doc_solution()
{ 
 //Declare an output stream and filename
 ofstream some_file;
 char filename[100];

 // Number of plot points: npts x npts
 unsigned npts=5;

 // Output solution 
 //-----------------
 sprintf(filename,"%s/soln%i.dat",Doc_info.directory().c_str(),
         Doc_info.number());
 some_file.open(filename);
 mesh_pt()->output(some_file,npts);
 some_file.close();

 Doc_info.number()++;
} // end of doc


//=====================================================================
/// Driver code for 2D Thermoelasticity problem
//====================================================================
int main(int argc, char **argv)
{

 // "Big G" Linear constitutive equations:
 Global_Physical_Variables::Constitutive_law_pt = 
  new GeneralisedHookean(&Global_Physical_Variables::Nu,
                         &Global_Physical_Variables::E);

 //Construct our problem
 ThermalProblem<QThermalPVDElement<2> > problem;

 //Number of quasi-steady steps
 unsigned n_steps = 11;
 //If we have additional command line arguemnts, take fewer steps
 if(argc > 1) {n_steps = 2;}
 for(unsigned i=0;i<n_steps;i++)
  {
   //Increase the thermal expansion coefficient
   Global_Physical_Variables::Alpha = 0.1*i;
   
   //Perform a single steady newton solve
   problem.newton_solve();
   //Document the solution
   problem.doc_solution();
  }
} // end of main