gen_axisym_advection_diffusion_elements.h

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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// 
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//LIC//
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//LIC// Copyright (C) 2006-2016 Matthias Heil and Andrew Hazel
//LIC// 
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//Header file for Advection Diffusion elements
#ifndef OOMPH_GEN_AXISYM_ADV_DIFF_ELEMENTS_HEADER
#define OOMPH_GEN_AXISYM_ADV_DIFF_ELEMENTS_HEADER


// Config header generated by autoconfig
#ifdef HAVE_CONFIG_H
  #include <oomph-lib-config.h>
#endif

//OOMPH-LIB headers
#include "../generic/nodes.h"
#include "../generic/Qelements.h"
#include "../generic/oomph_utilities.h"

namespace oomph
{

//=============================================================
// DOXYERROR: the maths below is wrong somehow but I have no idea what it's supposed to be doing!
/// \short A class for all elements that solve the Advection 
/// Diffusion equations in conservative form using isoparametric elements
/// in a cylindrical polar coordinate system.
/// \mbox{\boldmath$\nabla\cdot$} \left(
/// Pe \mbox{\boldmath$w$}(\mbox{\boldmath$x$}) u
///  - D(\mbox{\boldmath$x$)\mbox{\boldmath$\nabla$} u\right)
/// = f(\mbox{\boldmath$x$})
/// This contains the generic maths. Shape functions, geometric
/// mapping etc. must get implemented in derived class.
//=============================================================
class GeneralisedAxisymAdvectionDiffusionEquations : 
 public virtual FiniteElement
{

public:

 /// \short Function pointer to source function fct(x,f(x)) -- 
 /// x is a Vector! 
 typedef void (*GeneralisedAxisymAdvectionDiffusionSourceFctPt)
  (const Vector<double>& x, double& f);

 /// \short Function pointer to wind function fct(x,w(x)) -- 
 /// x is a Vector! 
 typedef void (*GeneralisedAxisymAdvectionDiffusionWindFctPt)
  (const Vector<double>& x, Vector<double>& wind);


 /// \short Function pointer to a diffusivity function
 typedef void (*GeneralisedAxisymAdvectionDiffusionDiffFctPt)
  (const Vector<double> &x, DenseMatrix<double> &D);

 /// \short Constructor: Initialise the Source_fct_pt and Wind_fct_pt 
 /// to null and set (pointer to) Peclet number to default
 GeneralisedAxisymAdvectionDiffusionEquations() : 
 Source_fct_pt(0), Wind_fct_pt(0),
  Conserved_wind_fct_pt(0), Diff_fct_pt(0), ALE_is_disabled(false)
  {
   //Set Peclet number to default
   Pe_pt = &Default_peclet_number;
   //Set Peclet Strouhal number to default
   PeSt_pt = &Default_peclet_number;
  }
 
 /// Broken copy constructor
 GeneralisedAxisymAdvectionDiffusionEquations(
  const GeneralisedAxisymAdvectionDiffusionEquations& dummy) 
  { 
   BrokenCopy::broken_copy("GeneralisedAxisymAdvectionDiffusionEquations");
  } 
 
 /// Broken assignment operator
//Commented out broken assignment operator because this can lead to a conflict warning
//when used in the virtual inheritence hierarchy. Essentially the compiler doesn't
//realise that two separate implementations of the broken function are the same and so,
//quite rightly, it shouts.
 /*void operator=(const GeneralisedAxisymAdvectionDiffusionEquations&) 
  {
   BrokenCopy::broken_assign("GeneralisedAxisymAdvectionDiffusionEquations");
   }*/

 /// \short Return the index at which the unknown value
 /// is stored. The default value, 0, is appropriate for single-physics
 /// problems, when there is only one variable, the value that satisfies
 /// the advection-diffusion equation. 
 /// In derived multi-physics elements, this function should be overloaded
 /// to reflect the chosen storage scheme. Note that these equations require
 /// that the unknown is always stored at the same index at each node.
 virtual inline unsigned u_index_cons_axisym_adv_diff() const {return 0;}

/// \short du/dt at local node n. 
 /// Uses suitably interpolated value for hanging nodes.
 double du_dt_cons_axisym_adv_diff(const unsigned &n) const
 {
  // Get the data's timestepper
  TimeStepper* time_stepper_pt= this->node_pt(n)->time_stepper_pt();
  
  //Initialise dudt
  double dudt=0.0;
  //Loop over the timesteps, if there is a non Steady timestepper
  if (!time_stepper_pt->is_steady())
   {
    //Find the index at which the variable is stored
    const unsigned u_nodal_index = u_index_cons_axisym_adv_diff();
    
     // Number of timsteps (past & present)
     const unsigned n_time = time_stepper_pt->ntstorage();
     
     for(unsigned t=0;t<n_time;t++)
      {
       dudt += time_stepper_pt->weight(1,t)*nodal_value(t,n,u_nodal_index);
      }
    }
   return dudt;
  }

 /// \short Disable ALE, i.e. assert the mesh is not moving -- you do this
 /// at your own risk!
 void disable_ALE()
  {
   ALE_is_disabled=true;
  }


 /// \short (Re-)enable ALE, i.e. take possible mesh motion into account
 /// when evaluating the time-derivative. Note: By default, ALE is 
 /// enabled, at the expense of possibly creating unnecessary work 
 /// in problems where the mesh is, in fact, stationary. 
 void enable_ALE()
  {
   ALE_is_disabled=false;
  }


 /// Output with default number of plot points
 void output(std::ostream &outfile) 
  {
   unsigned nplot=5;
   output(outfile,nplot);
  }

 /// \short Output FE representation of soln: r,z,u at 
 /// nplot^2 plot points
 void output(std::ostream &outfile, const unsigned &nplot);

 /// C_style output with default number of plot points
 void output(FILE* file_pt)
  {
   unsigned n_plot=5;
   output(file_pt,n_plot);
  }

 /// \short C-style output FE representation of soln: r,z,u at 
 /// n_plot^2 plot points
 void output(FILE* file_pt, const unsigned &n_plot);


 /// Output exact soln: r,z,u_exact at nplot^2 plot points
 void output_fct(std::ostream &outfile, const unsigned &nplot, 
                 FiniteElement::SteadyExactSolutionFctPt 
                 exact_soln_pt);

 /// \short Output exact soln: r,z,,u_exact at 
 /// nplot^2 plot points (dummy time-dependent version to 
 /// keep intel compiler happy)
 virtual void output_fct(std::ostream &outfile, const unsigned &nplot,
                         const double& time, 
  FiniteElement::UnsteadyExactSolutionFctPt exact_soln_pt)
  {
   throw OomphLibError(
    "There is no time-dependent output_fct() for Advection Diffusion elements",
    OOMPH_CURRENT_FUNCTION,
    OOMPH_EXCEPTION_LOCATION);
  }


 /// Get error against and norm of exact solution
 void compute_error(std::ostream &outfile, 
                    FiniteElement::SteadyExactSolutionFctPt 
                    exact_soln_pt, double& error, double& norm);


 /// Dummy, time dependent error checker
 void compute_error(std::ostream &outfile, 
                    FiniteElement::UnsteadyExactSolutionFctPt 
                    exact_soln_pt,
                    const double& time, double& error, double& norm)
  {
   throw OomphLibError(
    "No time-dependent compute_error() for Advection Diffusion elements",
    OOMPH_CURRENT_FUNCTION,
    OOMPH_EXCEPTION_LOCATION);
  }

 /// \short Integrate the concentration over the element
 double integrate_u();


 /// Access function: Pointer to source function
 GeneralisedAxisymAdvectionDiffusionSourceFctPt& source_fct_pt() 
  {return Source_fct_pt;}
 

 /// Access function: Pointer to source function. Const version
 GeneralisedAxisymAdvectionDiffusionSourceFctPt source_fct_pt() const 
  {return Source_fct_pt;}
 
 
 /// Access function: Pointer to wind function
 GeneralisedAxisymAdvectionDiffusionWindFctPt& wind_fct_pt() 
  {return Wind_fct_pt;}

 
 /// Access function: Pointer to wind function. Const version
 GeneralisedAxisymAdvectionDiffusionWindFctPt wind_fct_pt() const 
 {return Wind_fct_pt;}
 
 
 /// Access function: Pointer to additional (conservative) wind function
 GeneralisedAxisymAdvectionDiffusionWindFctPt& conserved_wind_fct_pt() 
  {return Conserved_wind_fct_pt;}
 
 
 /// \short Access function: Pointer to additional (conservative) 
 /// wind function. 
 /// Const version
 GeneralisedAxisymAdvectionDiffusionWindFctPt conserved_wind_fct_pt() const 
  {return Conserved_wind_fct_pt;}
 
 /// Access function: Pointer to diffusion  function
 GeneralisedAxisymAdvectionDiffusionDiffFctPt& diff_fct_pt() 
  {return Diff_fct_pt;}
 
 /// Access function: Pointer to diffusion function. Const version
 GeneralisedAxisymAdvectionDiffusionDiffFctPt diff_fct_pt() const 
  {return Diff_fct_pt;}

 /// Peclet number
 const double &pe() const {return *Pe_pt;}

 /// Pointer to Peclet number
 double* &pe_pt() {return Pe_pt;}

 /// Peclet number multiplied by Strouhal number
 const double &pe_st() const {return *PeSt_pt;}

 /// Pointer to Peclet number multipled by Strouha number
 double* &pe_st_pt() {return PeSt_pt;}

 /// \short Get source term at (Eulerian) position x. This function is
 /// virtual to allow overloading in multi-physics problems where
 /// the strength of the source function might be determined by
 /// another system of equations 
 inline virtual void get_source_cons_axisym_adv_diff(const unsigned& ipt,
                                                     const Vector<double>& x,
                                                     double& source) const
 {
  //If no source function has been set, return zero
   if(Source_fct_pt==0) {source = 0.0;}
   else
    {
     // Get source strength
     (*Source_fct_pt)(x,source);
    }
 }
 
 /// \short Get wind at (Eulerian) position x and/or local coordinate s. 
 /// This function is
 /// virtual to allow overloading in multi-physics problems where
 /// the wind function might be determined by
 /// another system of equations 
 inline virtual void get_wind_cons_axisym_adv_diff(const unsigned& ipt,
                                                   const Vector<double> &s,
                                                   const Vector<double>& x,
                                                   Vector<double>& wind) const
 {
  //If no wind function has been set, return zero
  //There are three components of the wind, but only two matter
  if(Wind_fct_pt==0)
   {
    for(unsigned i=0;i<3;i++) {wind[i]= 0.0;}
   }
  else
   {
    // Get wind
    (*Wind_fct_pt)(x,wind);
   }
 }


 /// \short Get additional (conservative) 
 /// wind at (Eulerian) position x and/or local coordinate s. 
 /// This function is
 /// virtual to allow overloading in multi-physics problems where
 /// the wind function might be determined by
 /// another system of equations 
 inline virtual void get_conserved_wind_cons_axisym_adv_diff(
  const unsigned& ipt,
  const Vector<double> &s, 
  const Vector<double>& x,
  Vector<double>& wind) const
 {
   //If no wind function has been set, return zero
   if(Conserved_wind_fct_pt==0)
    {
     for(unsigned i=0;i<3;i++) {wind[i]= 0.0;}
    }
   else
    {
     // Get wind
     (*Conserved_wind_fct_pt)(x,wind);
    }
  }


 /// \short Get diffusivity tensor at (Eulerian) position 
 /// x and/or local coordinate s. 
 /// This function is
 /// virtual to allow overloading in multi-physics problems where
 /// the wind function might be determined by
 /// another system of equations 
 inline virtual void get_diff_cons_axisym_adv_diff(const unsigned& ipt,
                                                   const Vector<double> &s,
                                                   const Vector<double>& x,
                                                   DenseMatrix<double>& D) const
 {
   //If no wind function has been set, return identity
   //Again three components, but not all of them matter
   //Those in the theta direction are ignored
   if(Diff_fct_pt==0)
    {
     for(unsigned i=0;i<3;i++) 
      {
       for(unsigned j=0;j<3;j++)
        {
         if(i==j) {D(i,j) = 1.0;} else {D(i,j) = 0.0;}
        }
      }
    }
   else
    {
     // Get diffusivity tensor
     (*Diff_fct_pt)(x,D);
    }
  }


 /// Get flux: \f$\mbox{flux}[i] = \mbox{d}u / \mbox{d}x_i \f$
 void get_flux(const Vector<double>& s, Vector<double>& flux) const
  {
   //Find out how many nodes there are in the element
   const unsigned n_node = this->nnode();
   
   //Get the nodal index at which the unknown is stored
   const unsigned u_nodal_index = this->u_index_cons_axisym_adv_diff();

   //Set up memory for the shape and test functions
   Shape psi(n_node);
   DShape dpsidx(n_node,2);
 
   //Call the derivatives of the shape and test functions
   dshape_eulerian(s,psi,dpsidx);
     
   //Initialise to zero
   for(unsigned j=0;j<2;j++) {flux[j] = 0.0;}
   
   // Loop over nodes
   for(unsigned l=0;l<n_node;l++) 
    {
     const double u_value = this->nodal_value(l,u_nodal_index);
     //Add in the derivative directions
     flux[0] += u_value*dpsidx(l,0);
     flux[1] += u_value*dpsidx(l,1);
    }
  }

 /// Get flux: \f$\mbox{flux}[i] = \mbox{d}u / \mbox{d}x_i \f$
 void get_total_flux(const Vector<double>& s, 
                     Vector<double>& total_flux) const
  {
   //Find out how many nodes there are in the element
   const unsigned n_node = nnode();
   
   //Get the nodal index at which the unknown is stored
   const unsigned u_nodal_index = u_index_cons_axisym_adv_diff();
   
   //Set up memory for the shape and test functions
   Shape psi(n_node);
   DShape dpsidx(n_node,2);
 
   //Call the derivatives of the shape and test functions
   dshape_eulerian(s,psi,dpsidx);
   
   //Storage for the Eulerian position
   Vector<double> interpolated_x(2,0.0);
   //Storage for the concentration
   double interpolated_u = 0.0;
   //Storage for the derivatives of the concentration
   Vector<double> interpolated_dudx(2,0.0);

    // Loop over nodes
   for(unsigned l=0;l<n_node;l++) 
    {
     //Get the value at the node
     const double u_value = this->nodal_value(l,u_nodal_index);
     interpolated_u += u_value*psi(l);
     // Loop over directions
     for(unsigned j=0;j<2;j++)
      {
       interpolated_x[j] += this->nodal_position(l,j)*psi(l);
       interpolated_dudx[j] += u_value*dpsidx(l,j);
      }
    }

   //Dummy integration point 
   unsigned ipt=0;

   //Get the conserved wind (non-divergence free)
   Vector<double> conserved_wind(3);
   get_conserved_wind_cons_axisym_adv_diff(ipt,s,interpolated_x,conserved_wind);

   //Get diffusivity tensor
   DenseMatrix<double> D(3,3);
   get_diff_cons_axisym_adv_diff(ipt,s,interpolated_x,D);

   //Calculate the total flux made up of the diffusive flux
   //and the conserved wind only bother with the
   //first two components in each case becuase there can be no
   //variation in the azimuthal direction
   for(unsigned i=0;i<2;i++)
    {                               
     total_flux[i] = 0.0;
     for(unsigned j=0;j<2;j++)
      {
       total_flux[i] +=  D(i,j)*interpolated_dudx[j];
      }
     total_flux[i] -= conserved_wind[i]*interpolated_u;
    }
  }

 
 /// Add the element's contribution to its residual vector (wrapper)
 void fill_in_contribution_to_residuals(Vector<double> &residuals)
  {
   //Call the generic residuals function with flag set to 0 and using
   //a dummy matrix
   fill_in_generic_residual_contribution_cons_axisym_adv_diff(
    residuals,GeneralisedElement::Dummy_matrix,
    GeneralisedElement::Dummy_matrix,0);
  }

 
 /// \short Add the element's contribution to its residual vector and 
 /// the element Jacobian matrix (wrapper)
 void fill_in_contribution_to_jacobian(Vector<double> &residuals,
                                   DenseMatrix<double> &jacobian)
  {
   //Call the generic routine with the flag set to 1
   fill_in_generic_residual_contribution_cons_axisym_adv_diff(
    residuals,jacobian,GeneralisedElement::Dummy_matrix,1);
  }
 

 /// Add the element's contribution to its residuals vector,
 /// jacobian matrix and mass matrix
 void fill_in_contribution_to_jacobian_and_mass_matrix(
  Vector<double> &residuals, DenseMatrix<double> &jacobian, 
  DenseMatrix<double> &mass_matrix)
  {
   //Call the generic routine with the flag set to 2
   fill_in_generic_residual_contribution_cons_axisym_adv_diff(residuals,
                                                  jacobian,mass_matrix,2);
  }


 /// Return FE representation of function value u(s) at local coordinate s
 inline double interpolated_u_cons_axisym_adv_diff(const Vector<double> &s) 
  const
  {
   //Find number of nodes
   unsigned n_node = nnode();

   //Get the nodal index at which the unknown is stored
   unsigned u_nodal_index = u_index_cons_axisym_adv_diff();

   //Local shape function
   Shape psi(n_node);

   //Find values of shape function
   shape(s,psi);

   //Initialise value of u
   double interpolated_u = 0.0;

   //Loop over the local nodes and sum
   for(unsigned l=0;l<n_node;l++) 
    {
     interpolated_u += nodal_value(l,u_nodal_index)*psi[l];
    }

   return(interpolated_u);
  }


 /// \short Self-test: Return 0 for OK
 unsigned self_test();

protected:


 /// \short Shape/test functions and derivs w.r.t. to global coords at 
 /// local coord. s; return  Jacobian of mapping
 virtual double dshape_and_dtest_eulerian_cons_axisym_adv_diff(
  const Vector<double> &s, 
  Shape &psi, 
  DShape &dpsidx, 
  Shape &test, 
  DShape &dtestdx) const=0;
 
 /// \short Shape/test functions and derivs w.r.t. to global coords at 
 /// integration point ipt; return  Jacobian of mapping
 virtual double dshape_and_dtest_eulerian_at_knot_cons_axisym_adv_diff(
  const unsigned &ipt, 
  Shape &psi, 
  DShape &dpsidx,
  Shape &test, 
  DShape &dtestdx) 
  const=0;

 /// \short Add the element's contribution to its residual vector only 
 /// (if flag=and/or element  Jacobian matrix 
 virtual void fill_in_generic_residual_contribution_cons_axisym_adv_diff(
  Vector<double> &residuals, DenseMatrix<double> &jacobian, 
  DenseMatrix<double> &mass_matrix, unsigned flag); 
  
 /// Pointer to global Peclet number
 double *Pe_pt;

 /// Pointer to global Peclet number multiplied by Strouhal number
 double *PeSt_pt;

 /// Pointer to source function:
 GeneralisedAxisymAdvectionDiffusionSourceFctPt Source_fct_pt;
 
 /// Pointer to wind function:
 GeneralisedAxisymAdvectionDiffusionWindFctPt Wind_fct_pt;

  /// Pointer to additional (conservative) wind function:
 GeneralisedAxisymAdvectionDiffusionWindFctPt Conserved_wind_fct_pt;
 
 /// Pointer to diffusivity funciton
 GeneralisedAxisymAdvectionDiffusionDiffFctPt Diff_fct_pt;

 /// \short Boolean flag to indicate if ALE formulation is disabled when 
 /// time-derivatives are computed. Only set to false if you're sure
 /// that the mesh is stationary.
 bool ALE_is_disabled;

  private:

 /// Static default value for the Peclet number
 static double Default_peclet_number;
  
};


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



//======================================================================
/// \short QGeneralisedAxisymAdvectionDiffusionElement elements are 
/// linear/quadrilateral/brick-shaped Advection Diffusion elements with 
/// isoparametric interpolation for the function.
//======================================================================
template <unsigned NNODE_1D>
 class QGeneralisedAxisymAdvectionDiffusionElement : 
 public virtual QElement<2,NNODE_1D>,
 public virtual GeneralisedAxisymAdvectionDiffusionEquations
{

private:

 /// \short Static array of ints to hold number of variables at 
 /// nodes: Initial_Nvalue[n]
 static const unsigned Initial_Nvalue;
 
  public:


 ///\short  Constructor: Call constructors for QElement and 
 /// Advection Diffusion equations
 QGeneralisedAxisymAdvectionDiffusionElement() : QElement<2,NNODE_1D>(), 
  GeneralisedAxisymAdvectionDiffusionEquations()
  { }

 /// Broken copy constructor
 QGeneralisedAxisymAdvectionDiffusionElement(
  const QGeneralisedAxisymAdvectionDiffusionElement<NNODE_1D>&  dummy) 
  { 
   BrokenCopy::broken_copy("QGeneralisedAxisymAdvectionDiffusionElement");
  } 
 
 /// Broken assignment operator
 /*void operator=(const QGeneralisedAxisymAdvectionDiffusionElement<NNODE_1D>&) 
  {
   BrokenCopy::broken_assign("QGeneralisedAxisymAdvectionDiffusionElement");
   }*/

 /// \short  Required  # of `values' (pinned or dofs) 
 /// at node n
 inline unsigned required_nvalue(const unsigned &n) const 
  {return Initial_Nvalue;}

 /// \short Output function:  
 ///  r,z,u
 void output(std::ostream &outfile)
  {GeneralisedAxisymAdvectionDiffusionEquations::output(outfile);}

 /// \short Output function:  
 /// r,z,u  at n_plot^2 plot points
 void output(std::ostream &outfile, const unsigned &n_plot)
  {GeneralisedAxisymAdvectionDiffusionEquations::output(outfile,n_plot);}


 /// \short C-style output function:  
 ///  r,z,u
 void output(FILE* file_pt)
  {
   GeneralisedAxisymAdvectionDiffusionEquations::output(file_pt);
  }

 ///  \short C-style output function:  
 ///   r,z,u at n_plot^2 plot points
 void output(FILE* file_pt, const unsigned &n_plot)
  {
   GeneralisedAxisymAdvectionDiffusionEquations::output(file_pt,n_plot);
  }

 /// \short Output function for an exact solution:
 ///  r,z,u_exact at n_plot^2 plot points
 void output_fct(std::ostream &outfile, const unsigned &n_plot,
                 FiniteElement::SteadyExactSolutionFctPt 
                 exact_soln_pt)
  {GeneralisedAxisymAdvectionDiffusionEquations
    ::output_fct(outfile,n_plot,exact_soln_pt);}


 /// \short Output function for a time-dependent exact solution.
 ///  r,z,u_exact  at n_plot^2 plot points
 /// (Calls the steady version)
 void output_fct(std::ostream &outfile, const unsigned &n_plot,
                 const double& time,
                 FiniteElement::UnsteadyExactSolutionFctPt 
                 exact_soln_pt)
  {
   GeneralisedAxisymAdvectionDiffusionEquations::
    output_fct(outfile,n_plot,time,exact_soln_pt);
  }


protected:

 /// Shape, test functions & derivs. w.r.t. to global coords. Return Jacobian.
 inline double dshape_and_dtest_eulerian_cons_axisym_adv_diff(
  const Vector<double> &s, 
  Shape &psi, 
  DShape &dpsidx, 
  Shape &test, 
  DShape &dtestdx) const;
 
 /// \short Shape, test functions & derivs. w.r.t. to global coords. at
 /// integration point ipt. Return Jacobian.
 inline double dshape_and_dtest_eulerian_at_knot_cons_axisym_adv_diff(
  const unsigned& ipt,
  Shape &psi, 
  DShape &dpsidx, 
  Shape &test,
  DShape &dtestdx) 
  const;

};

//Inline functions:


//======================================================================
/// \short Define the shape functions and test functions and derivatives
/// w.r.t. global coordinates and return Jacobian of mapping.
///
/// Galerkin: Test functions = shape functions
//======================================================================
template<unsigned NNODE_1D>
double QGeneralisedAxisymAdvectionDiffusionElement<NNODE_1D>::
 dshape_and_dtest_eulerian_cons_axisym_adv_diff(const Vector<double> &s,
                                         Shape &psi, 
                                         DShape &dpsidx,
                                         Shape &test, 
                                         DShape &dtestdx) const
{
 //Call the geometrical shape functions and derivatives  
 double J = this->dshape_eulerian(s,psi,dpsidx);

 //Loop over the test functions and derivatives and set them equal to the
 //shape functions
 for(unsigned i=0;i<NNODE_1D;i++)
  {
   test[i] = psi[i]; 
   for(unsigned j=0;j<2;j++)
    {
     dtestdx(i,j) = dpsidx(i,j);
    }
  }
 
 //Return the jacobian
 return J;
}



//======================================================================
/// Define the shape functions and test functions and derivatives
/// w.r.t. global coordinates and return Jacobian of mapping.
///
/// Galerkin: Test functions = shape functions
//======================================================================
template<unsigned NNODE_1D>
double QGeneralisedAxisymAdvectionDiffusionElement<NNODE_1D>::
 dshape_and_dtest_eulerian_at_knot_cons_axisym_adv_diff(
 const unsigned &ipt,
 Shape &psi, 
 DShape &dpsidx,
 Shape &test, 
 DShape &dtestdx) const
{
 //Call the geometrical shape functions and derivatives  
 double J = this->dshape_eulerian_at_knot(ipt,psi,dpsidx);

 //Set the test functions equal to the shape functions (pointer copy)
 test = psi;
 dtestdx = dpsidx;

 //Return the jacobian
 return J;
}


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



//=======================================================================
/// \short Face geometry for the QGeneralisedAxisymAdvectionDiffusionElement elements: 
/// The spatial dimension of the face elements is one lower than that 
/// of the bulk element but they have the same number of points along 
/// their 1D edges.
//=======================================================================
template<unsigned NNODE_1D>
class FaceGeometry<QGeneralisedAxisymAdvectionDiffusionElement<NNODE_1D> >: 
 public virtual QElement<1,NNODE_1D>
{

  public:
 
 /// \short Constructor: Call the constructor for the
 /// appropriate lower-dimensional QElement
 FaceGeometry() : QElement<1,NNODE_1D>() {}

};

}

#endif