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// $Id: fe_nedelec.h 31791 2013-11-25 10:36:38Z felix.gruber $
//
// Copyright (C) 2002 - 2013 by the deal.II authors
//
// This file is part of the deal.II library.
//
// The deal.II library is free software; you can use it, redistribute
// it, and/or modify it under the terms of the GNU Lesser General
// Public License as published by the Free Software Foundation; either
// version 2.1 of the License, or (at your option) any later version.
// The full text of the license can be found in the file LICENSE at
// the top level of the deal.II distribution.
//
// ---------------------------------------------------------------------
#ifndef __deal2__fe_nedelec_h
#define __deal2__fe_nedelec_h
#include <deal.II/base/config.h>
#include <deal.II/base/table.h>
#include <deal.II/base/tensor.h>
#include <deal.II/base/tensor_base.h>
#include <deal.II/base/polynomials_nedelec.h>
#include <deal.II/base/polynomial.h>
#include <deal.II/base/tensor_product_polynomials.h>
#include <deal.II/base/geometry_info.h>
#include <deal.II/fe/fe.h>
#include <deal.II/fe/fe_poly_tensor.h>
#include <vector>
DEAL_II_NAMESPACE_OPEN
template <int dim, int spacedim> class MappingQ;
/*!@addtogroup fe */
/*@{*/
/**
* @warning Several aspects of the implementation are
* experimental. For the moment, it is safe to use the element on
* globally refined meshes with consistent orientation of faces. See
* the todo entries below for more detailed caveats.
*
* Implementation of Nédélec elements, conforming with the
* space H<sup>curl</sup>. These elements generate vector fields with
* tangential components continuous between mesh cells.
*
* We follow the convention that the degree of Nédélec elements
* denotes the polynomial degree of the largest complete polynomial subspace
* contained in the Nédélec space. This leads to the
* consistently numbered sequence of spaces
* @f[
* Q_{k+1}
* \stackrel{\text{grad}}{\rightarrow}
* \text{Nedelec}_k
* \stackrel{\text{curl}}{\rightarrow}
* \text{RaviartThomas}_k
* \stackrel{\text{div}}{\rightarrow}
* DGQ_{k}
* @f]
* Consequently, approximation order of
* the Nédélec space equals the value <i>degree</i> given to the constructor.
* In this scheme, the lowest order element would be created by the call
* FE_Nedelec<dim>(0). Note that this follows the convention of Brezzi and
* Raviart, though not the one used in the original paper by Nédélec.
*
* This class is not implemented for the codimension one case
* (<tt>spacedim != dim</tt>).
*
* @todo Even if this element is implemented for two and three space
* dimensions, the definition of the node values relies on
* consistently oriented faces in 3D. Therefore, care should be taken
* on complicated meshes.
*
* <h3>Restriction on transformations</h3>
*
* In some sense, the implementation of this element is not complete,
* but you will rarely notice. Here is the fact: since the element is
* vector-valued already on the unit cell, the Jacobian matrix (or its
* inverse) is needed already to generate the values of the shape
* functions on the cells in real space. This is in contrast to most
* other elements, where you only need the Jacobian for the
* gradients. Thus, to generate the gradients of Nédélec shape
* functions, one would need to have the derivatives of the inverse of
* the Jacobian matrix.
*
* Basically, the Nédélec shape functions can be understood as the
* gradients of scalar shape functions on the real cell. They are thus
* the inverse Jacobian matrix times the gradients of scalar shape
* functions on the unit cell. The gradient of Nédélec shape functions
* is then, by the product rule, the sum of first the derivative (with
* respect to true coordinates) of the inverse Jacobian times the
* gradient (in unit coordinates) of the scalar shape function, plus
* second the inverse Jacobian times the derivative (in true
* coordinates) of the gradient (in unit coordinates) of the scalar
* shape functions. Note that each of the derivatives in true
* coordinates can be expressed as inverse Jacobian times gradient in
* unit coordinates.
*
* The problem is the derivative of the inverse Jacobian. This rank-3
* tensor can actually be computed (and we did so in very early
* versions of the library), but is a large task and very time
* consuming, so we dropped it. Since it is not available, we simply
* drop this first term.
*
* What this means for the present case: first the computation of
* gradients of Nédélec shape functions is wrong in general. Second,
* in the following two cases you will not notice this:
*
* - If the cell is a parallelogram, then the usual bi-/trilinear mapping
* is in fact affine. In that case, the gradient of the Jacobian vanishes
* and the gradient of the shape functions is computed exactly, since the
* first term is zero.
*
* - With the Nédélec elements, you will usually want to compute
* the curl, not the general derivative tensor. However, the curl of the
* Jacobian vanishes, so for the curl of shape functions the first term
* is irrelevant, and the curl will always be computed correctly even on
* cells that are not parallelograms.
*
*
* <h3>Interpolation</h3>
*
* The @ref GlossInterpolation "interpolation" operators associated
* with the Nédélec element are constructed such that
* interpolation and computing the curl are commuting operations on
* rectangular mesh cells. We require this from interpolating
* arbitrary functions as well as the #restriction matrices.
*
* <h4>Node values</h4>
*
* The @ref GlossNodes "node values" for an element of degree <i>k</i>
* on the reference cell are:
* <ol>
* <li> On edges: the moments of the tangential component with respect
* to polynomials of degree <i>k</i>.
* <li> On faces: the moments of the tangential components with
* respect to <tt>dim</tt>-1 dimensional FE_Nedelec
* polynomials of degree <i>k</i>-1.
* <li> In cells: the moments with respect to gradients of polynomials
* in FE_Q of degree <i>k</i>.
* </ol>
*
* <h4>Generalized support points</h4>
*
* The node values above rely on integrals, which will be computed by
* quadrature rules themselves. The generalized support points are a
* set of points such that this quadrature can be performed with
* sufficient accuracy. The points needed are those of
* QGauss<sub>k+1</sub> on each edge and QGauss<sub>k+2</sub> on each face and in
* the interior of the cell (or none for N<sub>1</sub>).
*
* @author Markus Bürg
* @date 2009, 2010, 2011
*/
template <int dim>
class FE_Nedelec : public FE_PolyTensor<PolynomialsNedelec<dim>, dim>
{
public:
/**
* Constructor for the Nédélec
* element of degree @p p.
*/
FE_Nedelec (const unsigned int p);
/**
* Return a string that uniquely
* identifies a finite
* element. This class returns
* <tt>FE_Nedelec<dim>(degree)</tt>, with
* @p dim and @p degree
* replaced by appropriate
* values.
*/
virtual std::string get_name () const;
/**
* Check whether a shape function
* may be non-zero on a face.
*/
virtual bool has_support_on_face (const unsigned int shape_index,
const unsigned int face_index) const;
/**
* Return whether this element implements its
* hanging node constraints in the new way, which
* has to be used to make elements "hp compatible".
*
* For the <tt>FE_Nedelec</tt> class the result is
* always true (independent of the degree of the
* element), as it implements the complete set of
* functions necessary for hp capability.
*/
virtual bool hp_constraints_are_implemented () const;
/**
* Return whether this element dominates the one,
* which is given as argument.
*/
virtual FiniteElementDomination::Domination
compare_for_face_domination (const FiniteElement<dim> &fe_other) const;
/**
* If, on a vertex, several finite elements are active, the hp code
* first assigns the degrees of freedom of each of these FEs
* different global indices. It then calls this function to find out
* which of them should get identical values, and consequently can
* receive the same global DoF index. This function therefore
* returns a list of identities between DoFs of the present finite
* element object with the DoFs of @p fe_other, which is a reference
* to a finite element object representing one of the other finite
* elements active on this particular vertex. The function computes
* which of the degrees of freedom of the two finite element objects
* are equivalent, both numbered between zero and the corresponding
* value of dofs_per_vertex of the two finite elements. The first
* index of each pair denotes one of the vertex dofs of the present
* element, whereas the second is the corresponding index of the
* other finite element.
*/
virtual std::vector<std::pair<unsigned int, unsigned int> >
hp_vertex_dof_identities (const FiniteElement<dim> &fe_other) const;
/**
* Same as hp_vertex_dof_indices(), except that
* the function treats degrees of freedom on lines.
*/
virtual std::vector<std::pair<unsigned int, unsigned int> >
hp_line_dof_identities (const FiniteElement<dim> &fe_other) const;
/**
* Same as hp_vertex_dof_indices(), except that
* the function treats degrees of freedom on lines.
*/
virtual std::vector<std::pair<unsigned int, unsigned int> >
hp_quad_dof_identities (const FiniteElement<dim> &fe_other) const;
/**
* Return the matrix interpolating from a face of one
* element to the face of the neighboring element. The
* size of the matrix is then <tt>source.dofs_per_face</tt>
* times <tt>this->dofs_per_face</tt>.
*
* Derived elements will have to implement this function.
* They may only provide interpolation matrices for certain
* source finite elements, for example those from the same
* family. If they don't implement interpolation from a given
* element, then they must throw an exception of type
* <tt>FiniteElement<dim>::ExcInterpolationNotImplemented</tt>.
*/
virtual void
get_face_interpolation_matrix (const FiniteElement<dim> &source,
FullMatrix<double> &matrix) const;
/**
* Return the matrix interpolating from a face of one element
* to the subface of the neighboring element. The size of
* the matrix is then <tt>source.dofs_per_face</tt> times
* <tt>this->dofs_per_face</tt>.
*
* Derived elements will have to implement this function.
* They may only provide interpolation matrices for certain
* source finite elements, for example those from the same
* family. If they don't implement interpolation from a given
* element, then they must throw an exception of type
* <tt>ExcInterpolationNotImplemented</tt>.
*/
virtual void
get_subface_interpolation_matrix (const FiniteElement<dim> &source,
const unsigned int subface,
FullMatrix<double> &matrix) const;
virtual void interpolate (std::vector<double> &local_dofs,
const std::vector<double> &values) const;
virtual void interpolate (std::vector<double> &local_dofs,
const std::vector<Vector<double> > &values,
unsigned int offset = 0) const;
virtual void interpolate (std::vector<double> &local_dofs,
const VectorSlice<const std::vector<std::vector<double> > > &values)
const;
virtual std::size_t memory_consumption () const;
virtual FiniteElement<dim> *clone() const;
private:
/**
* Only for internal use. Its
* full name is
* @p get_dofs_per_object_vector
* function and it creates the
* @p dofs_per_object vector that is
* needed within the constructor to
* be passed to the constructor of
* @p FiniteElementData.
*
* If the optional argument
* <tt>dg</tt> is true, the
* vector returned will have all
* degrees of freedom assigned to
* the cell, none on the faces
* and edges.
*/
static std::vector<unsigned int>
get_dpo_vector (const unsigned int degree, bool dg=false);
/**
* Initialize the @p
* generalized_support_points
* field of the FiniteElement
* class and fill the tables with
* interpolation weights
* (#boundary_weights and
* interior_weights). Called
* from the constructor.
*/
void initialize_support_points (const unsigned int degree);
/**
* Initialize the interpolation
* from functions on refined mesh
* cells onto the father
* cell. According to the
* philosophy of the
* Nédélec element, this
* restriction operator preserves
* the curl of a function
* weakly.
*/
void initialize_restriction ();
/**
* Fields of cell-independent data.
*
* For information about the
* general purpose of this class,
* see the documentation of the
* base class.
*/
class InternalData : public FiniteElement<dim>::InternalDataBase
{
public:
/**
* Array with shape function
* values in quadrature
* points. There is one row
* for each shape function,
* containing values for each
* quadrature point. Since
* the shape functions are
* vector-valued (with as
* many components as there
* are space dimensions), the
* value is a tensor.
*
* In this array, we store
* the values of the shape
* function in the quadrature
* points on the unit
* cell. The transformation
* to the real space cell is
* then simply done by
* multiplication with the
* Jacobian of the mapping.
*/
std::vector<std::vector<Tensor<1, dim> > > shape_values;
/**
* Array with shape function
* gradients in quadrature
* points. There is one
* row for each shape
* function, containing
* values for each quadrature
* point.
*
* We store the gradients in
* the quadrature points on
* the unit cell. We then
* only have to apply the
* transformation (which is a
* matrix-vector
* multiplication) when
* visiting an actual cell.
*/
std::vector<std::vector<Tensor<2, dim> > > shape_gradients;
};
/**
* These are the factors
* multiplied to a function in
* the
* #generalized_face_support_points
* when computing the
* integration.
*
* See the @ref GlossGeneralizedSupport "glossary entry on generalized support points"
* for more information.
*/
Table<2, double> boundary_weights;
/**
* Allow access from other
* dimensions.
*/
template <int dim1> friend class FE_Nedelec;
};
/* -------------- declaration of explicit specializations ------------- */
#ifndef DOXYGEN
template <>
void
FE_Nedelec<1>::initialize_restriction();
#endif // DOXYGEN
/*@}*/
DEAL_II_NAMESPACE_CLOSE
#endif
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