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gassmoeller committed Nov 19, 2024
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104 changes: 52 additions & 52 deletions doc/modules/to-3.0.0.h
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* (Rene Gassmoeller, Menno Fraters, 2024/11/08)
*
* <li> 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.
* <br>
* (Daniel Douglas, 2024/11/06)
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*
* <li> 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.
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* (Rene Gassmoeller, 2024/10/08)
*
* <li> 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
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* (Timo Heister, 2024/06/18)
*
* <li> 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.
* <br>
* (Menno Fraters, 2024/06/15)
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* (Juliane Dannberg, 2024/06/14)
*
* <li> 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.
* <br>
* (Daniel Douglas, 2024/06/13)
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* <br>
* (Juliane Dannberg, 2024/06/10)
*
* <li> New: The CPO particle property plugin can now use the Geodynamic
* <li> New: The CPO particle property plugin can now use the Geodynamic
* World Builder to set initial grain-sizes and grain orientations
* <br>
* (Menno Fraters, 2024/06/09)
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*
* <li> 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.
* <br>
* (Menno Fraters, 2024/06/06)
*
* <li> 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.
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* <br>
* (Juliane Dannberg, 2024/06/06)
*
* <li> New: Added fluid reaction and properties calculations to the
* <li> 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.
* <br>
* (Grant Block, 2024/06/06)
*
* <li> 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.
* <br>
* (Arushi Saxena, 2024/06/06)
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* <br>
* (Timo Heister, 2024/06/05)
*
* <li> New: There is now a new cookbook based on the
* setup of Allken et al, G3, 2012 which models
* <li> 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.
* <br>
* (Cedric Thieulot, 2024/06/05)
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* <br>
* (Daniel Douglas, 2024/06/05)
*
* <li> 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
* <li> 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.
* <br>
* (Shangxin Liu, 2024/06/04)
*
* <li> 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.
* <br>
* (Shangxin Liu, 2024/06/04)
*
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* (Rene Gassmoeller, 2024/06/01)
*
* <li> 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
* <br>
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* (Bob Myhill, 2024/05/29)
*
* <li> 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.
* <br>
* (Grant Block, 2024/05/29)
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* <br>
* (Juliane Dannberg, 2023/10/01)
*
* <li> Added: There is now a prescribed viscosity material model plugin, which can
* <li> 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.
* <br>
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* <br>
* (Maaike Weerdesteijn, 2023/07/14)
*
* <li> 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
* <li> 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.
* <br>
* (John Naliboff, 2023/07/14)
*
* <li> Fixed: The strain rheology now uses the correct 'old strain'
* when computing the reaction term updates.
* when computing the reaction term updates.
* <br>
* (John Naliboff 2023/07/14)
*
* <li> New: There is now a new cookbook which models
* <li> New: There is now a new cookbook which models
* the (Poiseuille) flow of the lower crust around a rigid obstacle.
* <br>
* (Cedric Thieulot, 2023/07/13)
*
* <li> 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.
* <br>
* (Anne Glerum, 2023/07/13)
Expand All @@ -712,13 +712,13 @@
* <li> 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.
* <br>
* (Arushi Saxena, Juliane Dannberg, and Rene Gassmoeller 2023/07/13)
*
* <li> New: There is now a new cookbook which is a very
* simple subduction initiation model as published
* by Matsumoto and Tomoda (1983).
* <li> New: There is now a new cookbook which is a very
* simple subduction initiation model as published
* by Matsumoto and Tomoda (1983).
* <br>
* (Cedric Thieulot, 2023/07/12)
*
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* <br>
* (Rene Gassmoeller, 2023/07/12)
*
* <li> New: A cookbook which replicates the model setup of the
* <li> New: A cookbook which replicates the model setup of the
* van Keken et al., 2008 2D corner flow subduction benchmark.
* <br>
* (Daniel Douglas, Cedric Thieulot, Wolfgang Bangerth, Max Rudolph, 2023/07/12)
*
* <li> New: There is now a new cookbook which models
* <li> New: There is now a new cookbook which models
* the deformation of elliptical and rectangular inclusions
* in simple shear and pure shear.
* <br>
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* <br>
* (Wolfgang Bangerth, 2023/07/10)
*
* <li> New: The base code for the computation and output of
* Crystal Preferred Orientation (CPO) has been added to
* ASPECT.
* <li> New: The base code for the computation and output of
* Crystal Preferred Orientation (CPO) has been added to
* ASPECT.
* <br>
* (Menno Fraters, 2023/07/09)
*
* <li> Changed: The input parameter 'Include viscoelasticity' has been
* <li> 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.
* <br>
* (Anne Glerum, 2023/07/09)
*
Expand All @@ -785,17 +785,17 @@
* (Haoyuan Li, Bob Myhill, 2023/07/08)
*
* <li> 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.
* <br>
* (Juliane Dannberg, 2023/07/08)
*
* <li> 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.
* <br>
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* <li> 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.
*
*
* <br>
* (Derek Neuharth, Anne Glerum, Sascha Brune, Esther Heckenbach 2023/03/01)
*
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