From: David Wells Date: Sun, 11 Dec 2016 00:53:52 +0000 (-0500) Subject: Fix some typos in the documentation headers. X-Git-Tag: v8.5.0-rc1~334^2 X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=c492d5e78c6c46e44a65f925facd828c9041668c;p=dealii.git Fix some typos in the documentation headers. --- diff --git a/doc/doxygen/headers/coding_conventions.h b/doc/doxygen/headers/coding_conventions.h index ab72494b63..ec99b9b5da 100644 --- a/doc/doxygen/headers/coding_conventions.h +++ b/doc/doxygen/headers/coding_conventions.h @@ -163,7 +163,7 @@ source files.

Instantiation of templated functions/classes

-

Majority of classes and functions in deal.II are templated. This brings a +

The majority of classes and functions in deal.II are templated. This brings a question of how and where such objects are instantiated, if at all. Throughout deal.II we adopt the following convention:

diff --git a/doc/doxygen/headers/constraints.h b/doc/doxygen/headers/constraints.h index 5e1f7943e4..24bf77be98 100644 --- a/doc/doxygen/headers/constraints.h +++ b/doc/doxygen/headers/constraints.h @@ -359,7 +359,7 @@ * until we hit a certain fraction of the norm of the initial * residual. * - In the second approach, we get the same problem if the starting vector - * in the iteration is zero, since then then the residual may be + * in the iteration is zero, since then the residual may be * dominated by constrained degrees of freedom having values that do not * match the values we want for them at the solution. We can again * circumvent this problem by setting the corresponding elements of the @@ -451,7 +451,7 @@ * International Journal for Numerical Methods in Engineering * 20(11):2107-2112, 1985). * - * Here, $A$ is a given (unconstrained) system matrix for wich we only + * Here, $A$ is a given (unconstrained) system matrix for which we only * assume that we can apply it to a vector but can not necessarily access * individual matrix entries. $b$ is the corresponding right hand side of a * system of linear equations $A\,x=b$. The matrix $C$ describes the diff --git a/doc/doxygen/headers/fe.h b/doc/doxygen/headers/fe.h index af7c19dc14..59b827e834 100644 --- a/doc/doxygen/headers/fe.h +++ b/doc/doxygen/headers/fe.h @@ -31,7 +31,7 @@ /** * @defgroup febase Base classes * - * The members of this sub-module describe the implementational mechanics of + * The members of this sub-module describe the implementation mechanics of * finite element classes, without actually implementing a concrete * element. For example, the FiniteElement base class declares the virtual * functions a derived class has to implement if it wants to describe a finite diff --git a/doc/doxygen/headers/fe_vs_mapping_vs_fevalues.h b/doc/doxygen/headers/fe_vs_mapping_vs_fevalues.h index b31f1e8c3e..ed41f71ba6 100644 --- a/doc/doxygen/headers/fe_vs_mapping_vs_fevalues.h +++ b/doc/doxygen/headers/fe_vs_mapping_vs_fevalues.h @@ -62,7 +62,7 @@ * quadrature points -- these quadrature points are then simply the vertices * of the cells (provided, for example, by QTrapez). * - * FEValues's role is to provide a user the values of shape functions, their + * FEValues' role is to provide a user the values of shape functions, their * gradients, etc, at quadrature points. The same is true with some geometric * information, e.g., the normal vectors at the quadrature points. To this end, * it provides a large number of member functions in the FEValuesBase base diff --git a/doc/doxygen/headers/multithreading.h b/doc/doxygen/headers/multithreading.h index 26805561af..bdbecda5d3 100644 --- a/doc/doxygen/headers/multithreading.h +++ b/doc/doxygen/headers/multithreading.h @@ -586,7 +586,7 @@ * then take the square root of the result. This is what the * parallel::accumulate_from_subranges function does (note that you * have to specify the result type as a template argument and that, as - * usual, the minimumum number of elements of the outer loop that can + * usual, the minimum number of elements of the outer loop that can * be scheduled on a single CPU core is given as the last argument): * @code double diff --git a/doc/doxygen/headers/update_flags.h b/doc/doxygen/headers/update_flags.h index 9f54646b91..ee9d6e111d 100644 --- a/doc/doxygen/headers/update_flags.h +++ b/doc/doxygen/headers/update_flags.h @@ -243,7 +243,7 @@ *
  • FEValues::reinit() calls Mapping::fill_fe_values(), then FiniteElement::fill_fe_values() *
  • FEFaceValues::reinit() calls Mapping::fill_fe_face_values(), then FiniteElement::fill_fe_face_values() *
  • FESubfaceValues::reinit() calls Mapping::fill_fe_subface_values(), - * thenFiniteElement::fill_fe_subface_values() + * then FiniteElement::fill_fe_subface_values() * * * This is where the actual data fields for FEValues, stored in diff --git a/doc/doxygen/headers/vector_valued.h b/doc/doxygen/headers/vector_valued.h index a14bca76fc..ac84956453 100644 --- a/doc/doxygen/headers/vector_valued.h +++ b/doc/doxygen/headers/vector_valued.h @@ -532,7 +532,7 @@ * would represent the gradient of the scalar pressure component, which * is of type Tensor@<1,dim@>, whereas the gradient of the * velocities components, fe_values[velocities].gradient(i,q) - * is a Tensor@<2,dim@>, i.e. a matrix $G_{ij}$ that consits + * is a Tensor@<2,dim@>, i.e. a matrix $G_{ij}$ that consists * of entries $G_{ij}=\frac{\partial\phi_i}{\partial x_j}$. Finally, * both scalar and vector views can be asked for the second derivatives * ("Hessians") and vector views can be asked for the symmetric gradient,