refineable_b_convection.cc

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//LIC//====================================================================
//Driver for a multi-physics problem that couples the Navier--Stokes
//equations to the advection diffusion equations, 
//giving Boussinesq convection
 
//Oomph-lib headers, we require the generic, advection-diffusion
//and navier-stokes elements.
#include "generic.h"
#include "advection_diffusion.h"
#include "navier_stokes.h"
#include "multi_physics.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;
 
 
/// ///////////////////////////////////////////////////////////////////
/// ///////////////////////////////////////////////////////////////////
/// ///////////////////////////////////////////////////////////////////
 
 
//======start_of_namespace============================================
/// Namespace for the physical parameters in the problem
//====================================================================
namespace Global_Physical_Variables
{
 
 /// Peclet number (identically one from our non-dimensionalisation)
 double Peclet=1.0;
 
 /// 1/Prandtl number
 double Inverse_Prandtl=1.0;
 
 /// Rayleigh number, set to be greater than 
 /// the threshold for linear instability
 double Rayleigh = 1800.0;
 
 /// Gravity vector
 Vector<double> Direction_of_gravity(2);
  
} // end_of_namespace
 
 
/// ///////////////////////////////////////////////////////////////////
/// ///////////////////////////////////////////////////////////////////
/// ///////////////////////////////////////////////////////////////////
 
 
 
//=======start_of_problem_class=======================================
/// 2D Convection  problem on rectangular domain, discretised 
/// with refineable elements. The specific type
/// of element is specified via the template parameter.
//====================================================================
template<class ELEMENT> 
class RefineableConvectionProblem : public Problem
{
 
public:
 
 /// Constructor
 RefineableConvectionProblem();
 
 /// Destructor. Empty
 ~RefineableConvectionProblem() {}
 
 /// Update the problem specs before solve:
 void actions_before_newton_solve();
 
 /// Update the problem after solve (empty)
 void actions_after_newton_solve(){}
 
 /// Overloaded version of the problem's access function to 
 /// the mesh. Recasts the pointer to the base Mesh object to 
 /// the actual mesh type.
 RectangularQuadMesh<ELEMENT>* mesh_pt() 
  {
   return dynamic_cast<RectangularQuadMesh<ELEMENT>*>(
    Problem::mesh_pt());
  } //end of access function to specic mesh
 
 /// Actions before adapt:(empty)
 void actions_before_adapt() {}
 
 /// Actions after adaptation,
 /// Re-pin a single pressure degree of freedom
 void actions_after_adapt()
  {
   //Unpin all the pressures to avoid pinning two pressures
   RefineableNavierStokesEquations<2>::
    unpin_all_pressure_dofs(mesh_pt()->element_pt());
 
   //Pin the zero-th pressure dof in the zero-th element and set
   // its value to zero
   fix_pressure(0,0,0.0);
  }
 
 /// Fix pressure in element e at pressure dof pdof and set to pvalue
 void fix_pressure(const unsigned &e, const unsigned &pdof, 
                   const double &pvalue)
  {
   //Cast to specific element and fix pressure
   dynamic_cast<ELEMENT*>(mesh_pt()->element_pt(e))->
    fix_pressure(pdof,pvalue);
  } // end_of_fix_pressure
 
 /// Set the
 /// boundary condition on the upper wall to be perturbed slightly
 /// to force the solution into the symmetry broken state.
 void enable_imperfection() {Imperfect = true;}
 
 /// Set the
 /// boundary condition on the upper wall to be unperturbed.
 void disable_imperfection() {Imperfect = false;}
 
 /// Doc the solution.
 void doc_solution();
 
private:
 
 /// DocInfo object
 DocInfo Doc_info;
 
 /// Is the boundary condition imperfect or not
 bool Imperfect;
 
}; // end of problem class
 
 
//=======start_of_constructor=============================================
/// Constructor for adaptive thermal convection problem
//========================================================================
template<class ELEMENT>
RefineableConvectionProblem<ELEMENT>::
RefineableConvectionProblem() : Imperfect(false)
{ 
 // Set output directory
 Doc_info.set_directory("RESLT");
 
 // # of elements in x-direction
 unsigned n_x=9;
 
 // # 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 the mesh
 RefineableRectangularQuadMesh<ELEMENT>* cast_mesh_pt =
  new RefineableRectangularQuadMesh<ELEMENT>(n_x,n_y,l_x,l_y);
 
 //Set the problem's mesh pointer
 Problem::mesh_pt() = cast_mesh_pt;
 
 
 // Create/set error estimator
 cast_mesh_pt->spatial_error_estimator_pt()=new Z2ErrorEstimator;
 
 // Set error targets for adaptive refinement
 cast_mesh_pt->max_permitted_error()=0.5e-3; 
 cast_mesh_pt->min_permitted_error()=0.5e-4; 
 
 
 // Set the boundary conditions for this problem: All nodes are
 // free by default -- only need to pin the ones that have Dirichlet 
 // conditions here
 
 //Loop over the boundaries
 unsigned num_bound = mesh_pt()->nboundary();
 for(unsigned ibound=0;ibound<num_bound;ibound++)
  {
   //Set the maximum index to be pinned (all values by default)
   unsigned val_max=3;
   //If we are on the side-walls, the v-velocity and temperature
   //satisfy natural boundary conditions, so we only pin the
   //first value
   if((ibound==1) || (ibound==3)) {val_max=1;}
 
   //Loop over the number of nodes on the boundry
   unsigned num_nod= mesh_pt()->nboundary_node(ibound);
   for (unsigned inod=0;inod<num_nod;inod++)
    {
     //Loop over the desired values stored at the nodes and pin
     for(unsigned j=0;j<val_max;j++)
      {
       mesh_pt()->boundary_node_pt(ibound,inod)->pin(j);
      }
    }
  }
 
 // Pin the zero-th pressure value in the zero-th element and
 // set its value to zero.
 fix_pressure(0,0,0.0);
 
 // 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 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 Peclet number
   el_pt->pe_pt() = &Global_Physical_Variables::Peclet;
 
   // Set the Peclet Strouhal number
   el_pt->pe_st_pt() = &Global_Physical_Variables::Peclet;
 
   // Set the Reynolds number (1/Pr in our non-dimensionalisation)
   el_pt->re_pt() = &Global_Physical_Variables::Inverse_Prandtl;
 
   // Set ReSt (also 1/Pr in our non-dimensionalisation)
   el_pt->re_st_pt() = &Global_Physical_Variables::Inverse_Prandtl;
 
   // Set the Rayleigh number
   el_pt->ra_pt() = &Global_Physical_Variables::Rayleigh;
 
   //Set Gravity vector
   el_pt->g_pt() = &Global_Physical_Variables::Direction_of_gravity;
  }
 
 // Setup equation numbering scheme
 cout <<"Number of equations: " << assign_eqn_numbers() << endl; 
 
} // end of constructor
 
 
//===================start_actions_before_newton_solve===========================
/// Update the problem specs before solve: (Re-)set boundary conditions
/// to include an imperfection (or not) depending on the control flag.
//========================================================================
template<class ELEMENT>
void RefineableConvectionProblem<ELEMENT>::actions_before_newton_solve()
{
 // Loop over the boundaries
 unsigned num_bound = mesh_pt()->nboundary();
 for(unsigned ibound=0;ibound<num_bound;ibound++)
  {
   // Loop over the nodes on boundary 
   unsigned num_nod=mesh_pt()->nboundary_node(ibound);
   for(unsigned inod=0;inod<num_nod;inod++)
    {
     // Get pointer to node
     Node* nod_pt=mesh_pt()->boundary_node_pt(ibound,inod);
 
     //Set the number of velocity components
     unsigned vel_max=2;
     //If we are on the side walls we only pin the x-velocity.
     if((ibound==1) || (ibound==3)) {vel_max = 1;}
     //Set the pinned velocities to zero
     for(unsigned j=0;j<vel_max;j++) {nod_pt->set_value(j,0.0);}
 
     //If we are on the top boundary
     if(ibound==2) 
      {
       //Set the temperature to -0.5 (cooled)
       nod_pt->set_value(2,-0.5);
       //Add small velocity imperfection if desired
       if(Imperfect)
        {
         //Read out the x position
         double x = nod_pt->x(0);
         //Set a sinusoidal perturbation in the vertical velocity
         //This perturbation is mass conserving
         double value = sin(2.0*3.141592654*x/3.0);
         nod_pt->set_value(1,value);
        }
      }
 
     //If we are on the bottom boundary, set the temperature
     //to 0.5 (heated)
     if(ibound==0) {nod_pt->set_value(2,0.5);}
    }
  }
 
}  // end of actions before solve
 
 
 
//====================start_of_doc_solution===============================
/// Doc the solution
//========================================================================
template<class ELEMENT>
void RefineableConvectionProblem<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
 
 
//===============start_of_main========================================
/// Driver code for 2D Boussinesq convection problem with 
/// adaptivity.
//====================================================================
int main()
{
 
 // Set the direction of gravity
 Global_Physical_Variables::Direction_of_gravity[0] = 0.0;
 Global_Physical_Variables::Direction_of_gravity[1] = -1.0;
 
 // Create the problem with 2D nine-node refineable elements.
 RefineableConvectionProblem<
  RefineableBuoyantQCrouzeixRaviartElement<2> > problem;
 
 // Apply a perturbation to the upper boundary condition to
 // force the solution into the symmetry-broken state.
 problem.enable_imperfection();
 
 //Solve the problem with (up to) two levels of adaptation
 problem.newton_solve(2);
 
 //Document the solution
 problem.doc_solution();
 
 // Make the boundary conditions perfect and solve again. 
 // Now the slightly perturbed symmetry broken state computed
 // above is used as the initial condition and the Newton solver
 // converges to the symmetry broken solution, even without
 // the perturbation
 problem.disable_imperfection();
 problem.newton_solve(2);
 problem.doc_solution();
 
} // end of main