From: Wolfgang Bangerth Date: Thu, 26 Sep 2019 21:15:24 +0000 (-0600) Subject: Update the description of the Nedelec element. X-Git-Tag: v9.2.0-rc1~989^2~1 X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=c369367e02c69468421f9540486b53f33354f4d1;p=dealii.git Update the description of the Nedelec element. --- diff --git a/include/deal.II/fe/fe_nedelec.h b/include/deal.II/fe/fe_nedelec.h index b208cb79ba..a84c0a56eb 100644 --- a/include/deal.II/fe/fe_nedelec.h +++ b/include/deal.II/fe/fe_nedelec.h @@ -42,14 +42,52 @@ DEAL_II_NAMESPACE_OPEN * consistent orientation of faces. See the todo entries below for more * detailed caveats. * - * Implementation of Nédélec elements, conforming with the space - * Hcurl. These elements generate vector fields with tangential - * components continuous between mesh cells. + * Implementation of Nédélec elements. The Nédélec + * space is designed to solve problems in which the solution only lives in the + * space + * $H^\text{curl}=\{ {\mathbf u} \in L_2: \text{curl}\, {\mathbf u} \in L_2\}$, + * rather than in the more commonly used space + * $H^1=\{ u \in L_2: \nabla u \in L_2\}$. In other words, the solution must + * be a vector field whose curl is square integrable, but for which the + * gradient may not be square integrable. The typical application for this + * space (and these elements) is to the Maxwell equations and corresponding + * simplifications, such as the reduced version of the Maxwell equation + * that only involves the electric field $\mathbf E$ which has to satisfy + * the equation $\text{curl}\, \text{curl}\, {\mathbf E} = 0$ in the + * time independent case when no currents are present, or the equation + * $\text{curl}\,\text{curl}\,{\mathbf A} = 4\pi{\mathbf j}$ that the + * magnetic vector potential $\mathbf A$ has to satisfy in the + * time independent case. * - * 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 + * The defining + * characteristic of functions in $H^\text{curl}$ is that they are in + * general discontinuous -- but that if you draw a line in 2d (or a + * surface in 3d), then the tangential component(s) of the vector + * field must be continuous across the line (or surface) even though + * the normal component may not be. As a consequence, the + * Nédélec element is constructed in such a way that (i) it is + * @ref vector_valued "vector-valued", (ii) the shape functions are + * discontinuous, but (iii) the tangential component(s) of the vector field + * represented by each shape function are continuous across the faces + * of cells. + * + * Other properties of the Nédélec element are that (i) it is + * @ref GlossPrimitive "not a primitive element"; (ii) the shape functions + * are defined so that certain integrals over the faces are either zero + * or one, rather than the common case of certain point values being + * either zero or one. (There is, however, the FE_RaviartThomasNodal + * element that uses point values.) + * + * We follow the commonly used -- though confusing -- definition of the "degree" + * of Nédélec elements. Specifically, the "degree" of the element + * denotes the polynomial degree of the largest complete polynomial + * subspace contained in the finite element space, even if the space may + * contain shape functions of higher polynomial degree. The lowest order element + * is consequently FE_Nedelec(0), i.e., the Raviart-Thomas element "of degree + * zero", even though the functions of this space are in general polynomials of + * degree one in each variable. This choice of "degree" implies that the + * approximation order of the function itself is degree+1, as with usual + * polynomial spaces. The numbering so chosen implies the sequence * @f[ * Q_{k+1} * \stackrel{\text{grad}}{\rightarrow} @@ -59,11 +97,8 @@ DEAL_II_NAMESPACE_OPEN * \stackrel{\text{div}}{\rightarrow} * DGQ_{k} * @f] - * Consequently, approximation order of the Nédélec space equals the value - * degree given to the constructor. In this scheme, the lowest order - * element would be created by the call FE_Nedelec(0). Note that this - * follows the convention of Brezzi and Raviart, though not the one used in - * the original paper by Nédélec. + * 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 (spacedim != * dim).