From 353ef1dba4bd9d7a2a4b8b9b703ff229f3d57ae7 Mon Sep 17 00:00:00 2001 From: Daniel Arndt Date: Sun, 12 Apr 2020 19:00:29 -0400 Subject: [PATCH] Fix step-* --- .../headers/automatic_and_symbolic_differentiation.h | 2 +- doc/news/5.1.0-vs-5.2.0.h | 6 +++--- examples/step-14/doc/results.dox | 2 +- examples/step-32/step-32.cc | 4 ++-- examples/step-57/step-57.cc | 2 +- examples/step-69/step-69.cc | 2 +- examples/step-8/step-8.cc | 2 +- 7 files changed, 10 insertions(+), 10 deletions(-) diff --git a/doc/doxygen/headers/automatic_and_symbolic_differentiation.h b/doc/doxygen/headers/automatic_and_symbolic_differentiation.h index 4969c8e97a..783fd72acf 100644 --- a/doc/doxygen/headers/automatic_and_symbolic_differentiation.h +++ b/doc/doxygen/headers/automatic_and_symbolic_differentiation.h @@ -119,7 +119,7 @@ * truncation of the Taylor scheme; dual numbers do not contain any higher-order terms in their first derivative, * while for the complex-step method these existent higher-order terms are neglected. It can be shown that * both of these methods are not subject to subtractive cancellation errors and that, within their - * finite-difference scheme, they are not numerically sensitive to the internal step-size chosen for the + * finite-difference scheme, they are not numerically sensitive to the internal \step-size chosen for the * numerical perturbation. The dual number approach thus produces exact first derivatives, while the * complex-step approximation does not. The standard implementation of the dual numbers, however, cannot yield * exact values for second derivatives. Hyper-dual numbers take a different view of this idea, with numbers diff --git a/doc/news/5.1.0-vs-5.2.0.h b/doc/news/5.1.0-vs-5.2.0.h index e7d10b1c4e..9866a9c151 100644 --- a/doc/news/5.1.0-vs-5.2.0.h +++ b/doc/news/5.1.0-vs-5.2.0.h @@ -139,7 +139,7 @@ inconvenience this causes.

  1. New: - The step-19 tutorial demonstrates handling of parameters from a + The \step-19 tutorial demonstrates handling of parameters from a parameter file, as well as some simple techniques for merging output from parallel computations.
    @@ -217,7 +217,7 @@ inconvenience this causes.

  2. New: If there are references to other example programs in any of the - step-XX programs, then they will now show up as crosslinks in the HTML + \step-XX programs, then they will now show up as crosslinks in the HTML version for simpler navigation of the tutorial.
    (WB, 2005/04/04) @@ -285,7 +285,7 @@ inconvenience this causes.

  3. Extended: The ParameterHandler class now does a much better job generating output in the print_parameters() function if - parameters have documentation strings attached to them. See the step-19 + parameters have documentation strings attached to them. See the \step-19 example program output for this.
    (WB, 2005/09/12) diff --git a/examples/step-14/doc/results.dox b/examples/step-14/doc/results.dox index 8a80faf7de..38d90cdf9a 100644 --- a/examples/step-14/doc/results.dox +++ b/examples/step-14/doc/results.dox @@ -290,7 +290,7 @@ computed value of $J(u_h)$. -

    \Step-13 revisited

    +

    step-13 revisited

    If instead of the Exercise_2_3 data set, we choose diff --git a/examples/step-32/step-32.cc b/examples/step-32/step-32.cc index 9da66f2989..6877affc84 100644 --- a/examples/step-32/step-32.cc +++ b/examples/step-32/step-32.cc @@ -2371,7 +2371,7 @@ namespace Step32 // The task to be performed by the next three functions is to calculate a // mass matrix and a Laplace matrix on the temperature system. These will be // combined in order to yield the semi-implicit time stepping matrix that - // consists of the mass matrix plus a time step-dependent weight factor + // consists of the mass matrix plus a time \step-dependent weight factor // times the Laplace matrix. This function is again essentially the body of // the loop over all cells from step-31. // @@ -2649,7 +2649,7 @@ namespace Step32 // In the function that runs the WorkStream for actually calculating the // right hand side, we also generate the final matrix. As mentioned above, // it is a sum of the mass matrix and the Laplace matrix, times some time - // step-dependent weight. This weight is specified by the BDF-2 time + // \step-dependent weight. This weight is specified by the BDF-2 time // integration scheme, see the introduction in step-31. What is new in this // tutorial program (in addition to the use of MPI parallelization and the // WorkStream class), is that we now precompute the temperature diff --git a/examples/step-57/step-57.cc b/examples/step-57/step-57.cc index 31327e3295..dd475b8f50 100644 --- a/examples/step-57/step-57.cc +++ b/examples/step-57/step-57.cc @@ -708,7 +708,7 @@ namespace Step57 // // This function will provide us with an initial guess by using a // continuation method as we discussed in the introduction. The Reynolds - // number is increased step-by-step until we reach the target value. By + // number is increased \step-by-step until we reach the target value. By // experiment, the solution to Stokes is good enough to be the initial guess // of NSE with Reynolds number 1000 so we start there. To make sure the // solution from previous problem is close enough to the next one, the step diff --git a/examples/step-69/step-69.cc b/examples/step-69/step-69.cc index adbbf7d2d3..2c596e1fba 100644 --- a/examples/step-69/step-69.cc +++ b/examples/step-69/step-69.cc @@ -367,7 +367,7 @@ namespace Step69 // U and a time point t (as input arguments) // computes the updated solution, stores it in the vector // temp, swaps its contents with the vector U, - // and returns the chosen step-size $\tau$. + // and returns the chosen \step-size $\tau$. // // The other important method is prepare() which primarily // sets the proper partition and sparsity pattern for the temporary diff --git a/examples/step-8/step-8.cc b/examples/step-8/step-8.cc index cdd873336f..c85a2a0156 100644 --- a/examples/step-8/step-8.cc +++ b/examples/step-8/step-8.cc @@ -253,7 +253,7 @@ namespace Step8 // The big changes in this program are in the creation of matrix and right // hand side, since they are problem-dependent. We will go through that - // process step-by-step, since it is a bit more complicated than in previous + // process \step-by-step, since it is a bit more complicated than in previous // examples. // // The first parts of this function are the same as before, however: setting -- 2.39.5