diff --git a/doc/modules/to-3.0.0.h b/doc/modules/to-3.0.0.h
index 54ec0943a89..eb76178f7ee 100644
--- a/doc/modules/to-3.0.0.h
+++ b/doc/modules/to-3.0.0.h
@@ -31,7 +31,7 @@
* (Rene Gassmoeller, Menno Fraters, 2024/11/08)
*
*
Added: When using the Geodynamic World Builder, ASPECT will create a file
- * called 'original.wb' in the output directory which contains the exact
+ * called 'original.wb' in the output directory which contains the exact
* worldbuilder file used to run the ASPECT model.
*
* (Daniel Douglas, 2024/11/06)
@@ -58,7 +58,7 @@
*
* Removed: A number of deprecated source code functions and input parameters
* have been removed. In particular the deprecated option to specify
- * individual material properties in the parameter
+ * individual material properties in the parameter
* 'Postprocess/Visualization/List of output variables' has been removed.
* Input files will be automatically fixed and updated
* by the update scripts in the directory contrib/utilities.
@@ -84,7 +84,7 @@
* (Rene Gassmoeller, 2024/10/08)
*
* New: The interface for particle property plugins has been updated.
- * The new interface can update particles cell-wise and is more efficient.
+ * The new interface can update particles cell-wise and is more efficient.
* In addition, the interface is more extensible for future improvements.
* All particle property plugins in ASPECT have been updated, user plugins
* will have to be updated accordingly before the support for the now deprecated
@@ -176,7 +176,7 @@
* (Timo Heister, 2024/06/18)
*
* Changed: The particle plugin functions declare_parameters and parse_parameters
- * now assume that they are already in the particles subsection. User plugins will
+ * now assume that they are already in the particles subsection. User plugins will
* have to change accordingly.
*
* (Menno Fraters, 2024/06/15)
@@ -190,9 +190,9 @@
* (Juliane Dannberg, 2024/06/14)
*
* Added: A postprocessor 'darcy velocity' that visualizes the fluid
- * velocity in models with a compositional field named 'porosity'.
- * This postprocessor is independent of the method the porosity is actually
- * advected with, i.e. it could be static, advected with the Darcy velocity,
+ * velocity in models with a compositional field named 'porosity'.
+ * This postprocessor is independent of the method the porosity is actually
+ * advected with, i.e. it could be static, advected with the Darcy velocity,
* or advected according to the two-phase flow equations.
*
* (Daniel Douglas, 2024/06/13)
@@ -214,7 +214,7 @@
*
* (Juliane Dannberg, 2024/06/10)
*
- * New: The CPO particle property plugin can now use the Geodynamic
+ * New: The CPO particle property plugin can now use the Geodynamic
* World Builder to set initial grain-sizes and grain orientations
*
* (Menno Fraters, 2024/06/09)
@@ -258,7 +258,7 @@
*
* New: The CPO particle property plugin set now contains a plugin
* which can compute the symmetry decompositions of the elastic
- * tensor. There are now also tests which test the whole CPO
+ * tensor. There are now also tests which test the whole CPO
* particle property plugin set.
*
* (Menno Fraters, 2024/06/06)
@@ -266,7 +266,7 @@
* New: Added a Rayleigh Taylor instability benchmark with a free surface.
* The benchmark was described by Kaus et al. (2010) and reproduced with
* ASPECT with different stabilization schemes for the free surface by
- * Rose et al. (2017). It can be used to show that the stabilization
+ * Rose et al. (2017). It can be used to show that the stabilization
* scheme implemented by I. Rose allows for larger timesteps, and that
* the projection of velocities onto the surface leads to significantly
* different topography.
@@ -279,16 +279,16 @@
*
* (Juliane Dannberg, 2024/06/06)
*
- * New: Added fluid reaction and properties calculations to the
+ * New: Added fluid reaction and properties calculations to the
* Katz2003MantleMelting model in the ReactionModels module. These calculations
* were taken from MeltSimple and the model now calls Katz2003MantleMelting. Additionally,
- * the katz 2003 option in ReactiveFluidTransport calls these calculations, allowing for
- * melting and melt transport to be composited with any material model via ReactiveFluidTransport.
+ * the katz 2003 option in ReactiveFluidTransport calls these calculations, allowing for
+ * melting and melt transport to be composited with any material model via ReactiveFluidTransport.
*
* (Grant Block, 2024/06/06)
*
* New: There is now a python script in the contrib folder that
- * creates netcdf files from an input ascii file
+ * creates netcdf files from an input ascii file
* formatted following structured ascii data file convention.
*
* (Arushi Saxena, 2024/06/06)
@@ -298,8 +298,8 @@
*
* (Timo Heister, 2024/06/05)
*
- * New: There is now a new cookbook based on the
- * setup of Allken et al, G3, 2012 which models
+ * New: There is now a new cookbook based on the
+ * setup of Allken et al, G3, 2012 which models
* rift interaction in 3D brittle-ductile coupled systems.
*
* (Cedric Thieulot, 2024/06/05)
@@ -320,20 +320,20 @@
*
* (Daniel Douglas, 2024/06/05)
*
- * Fixed: There was a bug in spherical harmonic data reading of S40RTS
- * and SAVANI initial temperature models when a maximum degree lower
- * than the maximum degree of the spherical harmonic coefficients of
- * the data file is specified by users to set up temperature field
+ * Fixed: There was a bug in spherical harmonic data reading of S40RTS
+ * and SAVANI initial temperature models when a maximum degree lower
+ * than the maximum degree of the spherical harmonic coefficients of
+ * the data file is specified by users to set up temperature field
* from spherical harmonic summation. This bug is now fixed.
*
* (Shangxin Liu, 2024/06/04)
*
* Changed: In S40RTS and SAVANI initial temperature models, the input parameter,
* 'Specify a lower maximum order' is changed to 'Specify a lower maximum degree',
- * and the input parameter, 'Maximum order' is changed to 'Maximum degree'.
+ * and the input parameter, 'Maximum order' is changed to 'Maximum degree'.
* This avoids confusion because the function of these two parameters is to
* allow users to specify a maximum degree lower than the maximum degree
- * of the spherical harmonic data file to calculate the temperature field.
+ * of the spherical harmonic data file to calculate the temperature field.
*
* (Shangxin Liu, 2024/06/04)
*
@@ -370,7 +370,7 @@
* (Rene Gassmoeller, 2024/06/01)
*
* Added: Functionality for multiplying the dislocation and/or diffusion creep
- * viscosities by prefactors which depend on the model composition. Created a
+ * viscosities by prefactors which depend on the model composition. Created a
* specific use-case for multiplying the viscosity by a factor that accounts for
* bound H2O from Hirth & Kohlstaedt 2004 10.1029/138GM06
*
@@ -432,8 +432,8 @@
* (Bob Myhill, 2024/05/29)
*
* Changed: A pressure term was added to the Frank Kamenetskii viscous flow law
- * in the Visco Plastic material model. The new FK function is given by
- * viscosity = A * exp(E * 0.5 * (1.0-(T/ref_T)) + F * (P-ref_P)/(ref_rho*g*h)),
+ * in the Visco Plastic material model. The new FK function is given by
+ * viscosity = A * exp(E * 0.5 * (1.0-(T/ref_T)) + F * (P-ref_P)/(ref_rho*g*h)),
* where F * (P-ref_P)/(ref_rho*g*h) are the new terms added here.
*
* (Grant Block, 2024/05/29)
@@ -585,7 +585,7 @@
*
* (Juliane Dannberg, 2023/10/01)
*
- * Added: There is now a prescribed viscosity material model plugin, which can
+ * Added: There is now a prescribed viscosity material model plugin, which can
* overwrite the viscosity of a specified location with a viscosity prescribed
* by a function.
*
@@ -674,28 +674,28 @@
*
* (Maaike Weerdesteijn, 2023/07/14)
*
- * New: There is now a new material model ('reactive fluid
- * transport') that is designed to advect fluids and
- * compute fluid release and absorption based on
+ * New: There is now a new material model ('reactive fluid
+ * transport') that is designed to advect fluids and
+ * compute fluid release and absorption based on
* different models for fluid-rock interaction. The
- * properties of the solid are taken from a
- * base material model.
+ * properties of the solid are taken from a
+ * base material model.
*
* (John Naliboff, 2023/07/14)
*
* Fixed: The strain rheology now uses the correct 'old strain'
- * when computing the reaction term updates.
+ * when computing the reaction term updates.
*
* (John Naliboff 2023/07/14)
*
- * New: There is now a new cookbook which models
+ * New: There is now a new cookbook which models
* the (Poiseuille) flow of the lower crust around a rigid obstacle.
*
* (Cedric Thieulot, 2023/07/13)
*
* Improved: The initial lithostatic pressure plugin for
* boundary tractions now includes the initial topography
- * of the reference point into its pressure profile
+ * of the reference point into its pressure profile
* instead of the maximum topography within the domain.
*
* (Anne Glerum, 2023/07/13)
@@ -712,13 +712,13 @@
* New: Added a cookbook on how to set up global instantaneous models
* based on recent geophysical constraints with a heterogeneous density and
* viscosity distribution and weak plate boundaries prescribed using
- * different plate boundary configurations.
+ * different plate boundary configurations.
*
* (Arushi Saxena, Juliane Dannberg, and Rene Gassmoeller 2023/07/13)
*
- * New: There is now a new cookbook which is a very
- * simple subduction initiation model as published
- * by Matsumoto and Tomoda (1983).
+ * New: There is now a new cookbook which is a very
+ * simple subduction initiation model as published
+ * by Matsumoto and Tomoda (1983).
*
* (Cedric Thieulot, 2023/07/12)
*
@@ -735,12 +735,12 @@
*
* (Rene Gassmoeller, 2023/07/12)
*
- * New: A cookbook which replicates the model setup of the
+ * New: A cookbook which replicates the model setup of the
* van Keken et al., 2008 2D corner flow subduction benchmark.
*
* (Daniel Douglas, Cedric Thieulot, Wolfgang Bangerth, Max Rudolph, 2023/07/12)
*
- * New: There is now a new cookbook which models
+ * New: There is now a new cookbook which models
* the deformation of elliptical and rectangular inclusions
* in simple shear and pure shear.
*
@@ -753,17 +753,17 @@
*
* (Wolfgang Bangerth, 2023/07/10)
*
- * New: The base code for the computation and output of
- * Crystal Preferred Orientation (CPO) has been added to
- * ASPECT.
+ * New: The base code for the computation and output of
+ * Crystal Preferred Orientation (CPO) has been added to
+ * ASPECT.
*
* (Menno Fraters, 2023/07/09)
*
- * Changed: The input parameter 'Include viscoelasticity' has been
+ * Changed: The input parameter 'Include viscoelasticity' has been
* removed from the visco_plastic material model. When
* 'Enable elasticity' in the Formulation subsection is
* switched on, elasticity will automatically be included
- * in the visco_plastic material model.
+ * in the visco_plastic material model.
*
* (Anne Glerum, 2023/07/09)
*
@@ -785,17 +785,17 @@
* (Haoyuan Li, Bob Myhill, 2023/07/08)
*
* Fixed: The computation of the upper box origin in the 'box
- * with lithosphere boundary indicators' geometry model did not
+ * with lithosphere boundary indicators' geometry model did not
* take into account a nonzero origin. This is fixed now.
*
* (Juliane Dannberg, 2023/07/08)
*
* Changed: Default field types are now defined by ASPECT
* based on Field Names if the types are not defined by the user.
- * The logic is as follows: if the name contains the substring stress,
- * it has type stress. If the name is equal to
+ * The logic is as follows: if the name contains the substring stress,
+ * it has type stress. If the name is equal to
* s11, s12, s22, s13, s23, s33, it has type strain.
- * If the name is equal to grain_size, porosity, density_field,
+ * If the name is equal to grain_size, porosity, density_field,
* or entropy it has the types grain size, porosity, density or entropy
* respectively. Otherwise it has the type chemical composition.
*
@@ -825,12 +825,12 @@
* New: Mesh deformation plugin that uses the landscape
* evolution code FastScape to deform the surface through
* erosion and sediment deposition.
- *
+ *
* Citations:
* Neuharth, D., Brune, S., Wrona, T., Glerum, A., Braun, J., & Yuan, X. (2022). Evolution of rift systems and their fault networks in response to surface processes. Tectonics, 41(3), e2021TC007166.
- *
+ *
* Neuharth, D., Brune, S., Glerum, A., Morley, C. K., Yuan, X., & Braun, J. (2022). Flexural strike-slip basins. Geology, 50(3), 361-365.
- *
+ *
*
* (Derek Neuharth, Anne Glerum, Sascha Brune, Esther Heckenbach 2023/03/01)
*