// element for the correct transformation.
switch (fe[fe_index].conforming_space)
{
- case FiniteElementData<dim>::H1:
- DEAL_II_FALLTHROUGH;
- case FiniteElementData<dim>::L2:
- // See Monk, Finite Element Methods for Maxwell's Equations,
- // p. 77ff, formula (3.74).
- // For given mapping F_K: \hat K \to K, we have to transform
- // \hat p = p\circ F_K
- // i.e., do nothing.
- break;
-
case FiniteElementData<dim>::Hcurl:
// See Monk, Finite Element Methods for Maxwell's Equations,
// p. 77ff, formula (3.76) and Corollary 3.58.
}
break;
+ case FiniteElementData<dim>::H1:
+ DEAL_II_FALLTHROUGH;
+ case FiniteElementData<dim>::L2:
+ // See Monk, Finite Element Methods for Maxwell's Equations,
+ // p. 77ff, formula (3.74).
+ // For given mapping F_K: \hat K \to K, we have to transform
+ // \hat p = p\circ F_K
+ // i.e., do nothing.
+ //
+ break;
+
default:
- Assert(false,
- ExcMessage(
- "The supplied finite element has an unknown conformity."));
+ // In case we deal with an unknown conformity, just assume we
+ // deal with a Lagrange element and do nothing.
+ break;
+
} /*switch*/
FETools::convert_generalized_support_point_values_to_dof_values(