From 9fbcb390463bf0af4d37b3795e54bfc7219c875b Mon Sep 17 00:00:00 2001 From: Lars Bilke <lars.bilke@ufz.de> Date: Fri, 29 May 2020 10:51:53 +0200 Subject: [PATCH] [web] Migrated GitLab links in benchmarks. --- .../elliptic-dirichlet-volumetric-source-term.pandoc | 2 +- .../docs/benchmarks/elliptic/elliptic-neumann.pandoc | 4 ++-- web/content/docs/benchmarks/elliptic/elliptic-robin.pandoc | 4 ++-- .../docs/benchmarks/elliptic/poisson_equation.pandoc | 4 ++-- .../heatconduction/heatconduction-dirichlet.pandoc | 2 +- .../heatconduction/heatconduction-line_source_term.pandoc | 6 +++--- .../mechanics-linear-element_deactivation.pandoc | 4 ++-- web/layouts/shortcodes/data-url.html | 2 +- 8 files changed, 14 insertions(+), 14 deletions(-) diff --git a/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc b/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc index fff0386e117..90a50f487f7 100644 --- a/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc +++ b/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc @@ -48,7 +48,7 @@ $$ ## Input files The main project file is -[`square_1e2_volumetricsourceterm.prj`](https://github.com/ufz/ogs/blob/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion/square_1e2_volumetricsourceterm.prj). It describes the +[`square_1e2_volumetricsourceterm.prj`](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion/square_1e2_volumetricsourceterm.prj). It describes the processes to be solved and the related process variables together with their initial and boundary conditions. It also references the bulk mesh and the boundary meshes associated with the bulk mesh. diff --git a/web/content/docs/benchmarks/elliptic/elliptic-neumann.pandoc b/web/content/docs/benchmarks/elliptic/elliptic-neumann.pandoc index 722b93b67a1..bc12faf7fcf 100644 --- a/web/content/docs/benchmarks/elliptic/elliptic-neumann.pandoc +++ b/web/content/docs/benchmarks/elliptic/elliptic-neumann.pandoc @@ -47,7 +47,7 @@ where $C_k = \frac{2k-1}{2} \pi$ and $A_k = 2 \Big/ \Big(C_k^2 \cosh\big(C_k\big ## Input files -The main project file is [square_1e2_neumann.prj](https://github.com/ufz/ogs-data/blob/master/Elliptic/square_1x1_SteadyStateDiffusion/square_1e2.prj). It describes the processes to be solved and the related process variables together with their initial and boundary conditions. It also references the mesh and geometrical objects defined on the mesh. +The main project file is [square_1e2_neumann.prj](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion/square_1e2.prj). It describes the processes to be solved and the related process variables together with their initial and boundary conditions. It also references the mesh and geometrical objects defined on the mesh. As of now a small portion of possible inputs is implemented; one can change: - the mesh file @@ -55,7 +55,7 @@ As of now a small portion of possible inputs is implemented; one can change: - introduce more/different Dirichlet boundary conditions (different geometry or other constant values) - introduce more/different Neumann boundary conditions (different geometry or other constant values) -The geometries used to specify the boundary conditions are given in the [square_1x1.gml](https://github.com/ufz/ogs-data/blob/master/Elliptic/square_1x1_SteadyStateDiffusion/square_1x1.gml) file. +The geometries used to specify the boundary conditions are given in the [square_1x1.gml](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion/square_1x1.gml) file. The input mesh `square_1x1_quad_1e2.vtu` is stored in the VTK file format and can be directly visualized in Paraview for example. diff --git a/web/content/docs/benchmarks/elliptic/elliptic-robin.pandoc b/web/content/docs/benchmarks/elliptic/elliptic-robin.pandoc index bf0b709d02f..85de8341698 100644 --- a/web/content/docs/benchmarks/elliptic/elliptic-robin.pandoc +++ b/web/content/docs/benchmarks/elliptic/elliptic-robin.pandoc @@ -44,7 +44,7 @@ $$ h(x) = g_D &\quad \text{for } x=1, }$$ see -[`line_1e1_robin_left_picard.prj`](https://github.com/ufz/ogs/tree/master/Tests/Data/Elliptic/line_1_SteadyStateDiffusion/line_1e1_robin_left_picard.prj). +[`line_1e1_robin_left_picard.prj`](https://gitlab.opengeosys.org/ogs/ogs/-/tree/master/Tests/Data/Elliptic/line_1_SteadyStateDiffusion/line_1e1_robin_left_picard.prj). ### Analytical solution @@ -117,7 +117,7 @@ h(x) = g_D &\quad \text{for } x=0,\cr {\partial h \over \partial n} = \alpha (h_0 - h(x)) &\quad \text{for } x=1, }$$ see -[`line_1e1_robin_right_picard.prj`](https://github.com/ufz/ogs/tree/master/Tests/Data/Elliptic/line_1_SteadyStateDiffusion/line_1e1_robin_right_picard.prj). +[`line_1e1_robin_right_picard.prj`](https://gitlab.opengeosys.org/ogs/ogs/-/tree/master/Tests/Data/Elliptic/line_1_SteadyStateDiffusion/line_1e1_robin_right_picard.prj). One particular solution is $$ diff --git a/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc b/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc index 4806a714781..cfe1d1f83f4 100644 --- a/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc +++ b/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc @@ -82,11 +82,11 @@ $$ ## Input files The project file is -[`square_1e3_poisson_sin_x_sin_y.prj`](https://github.com/ufz/ogs/tree/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion_Python/square_1e3_poisson_sin_x_sin_y.prj). It describes the +[`square_1e3_poisson_sin_x_sin_y.prj`](https://gitlab.opengeosys.org/ogs/ogs/-/tree/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion_Python/square_1e3_poisson_sin_x_sin_y.prj). It describes the process to be solved and the related process variable together with their initial, boundary conditions and source terms. The definition of the source term $Q$ is in a [Python -script](https://github.com/ufz/ogs/tree/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion_Python/sin_x_sin_y_source_term.py). +script](https://gitlab.opengeosys.org/ogs/ogs/-/tree/master/Tests/Data/Elliptic/square_1x1_SteadyStateDiffusion_Python/sin_x_sin_y_source_term.py). The script for setting the source terms is referenced in the project file as follows: ``` diff --git a/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc b/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc index 8617c578fb3..a785c6355f9 100644 --- a/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc +++ b/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc @@ -51,7 +51,7 @@ where $T_\textrm{b}$ is the boundary temperature, $\textrm{erfc}$ is the complem ## Input files -The main project file is [line_60_heat.prj](https://github.com/ufz/ogs-data/blob/master/Parabolic/T/1D_dirichlet/line_60_heat.prj). It describes the processes to be solved and the related process variables together with their initial and boundary conditions. It also references the mesh and geometrical objects defined on the mesh. +The main project file is [line_60_heat.prj](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Parabolic/T/1D_dirichlet/line_60_heat.prj). It describes the processes to be solved and the related process variables together with their initial and boundary conditions. It also references the mesh and geometrical objects defined on the mesh. As of now a small portion of possible inputs is implemented; one can change: - the mesh file diff --git a/web/content/docs/benchmarks/heatconduction/heatconduction-line_source_term.pandoc b/web/content/docs/benchmarks/heatconduction/heatconduction-line_source_term.pandoc index 28432bb766b..3095cc5caae 100644 --- a/web/content/docs/benchmarks/heatconduction/heatconduction-line_source_term.pandoc +++ b/web/content/docs/benchmarks/heatconduction/heatconduction-line_source_term.pandoc @@ -92,9 +92,9 @@ src="../LineSourceTermFigures/comparison_plot_over_line_rel_diff_analytical_solu #### Input files The project files for the described models are -[49k.prj](https://github.com/ufz/ogs-data/blob/master/Parabolic/T/3D_line_source_term_tests/3D_line_source_term_in_cylinder/49k_prisms/line_source_term_in_cylinder.prj) +[49k.prj](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Parabolic/T/3D_line_source_term_tests/3D_line_source_term_in_cylinder/49k_prisms/line_source_term_in_cylinder.prj) and -[286k.prj](https://github.com/ufz/ogs-data/blob/master/Parabolic/T/3D_line_source_term_tests/3D_line_source_term_in_cylinder/286k_prisms/line_source_term_in_cylinder.prj). +[286k.prj](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Parabolic/T/3D_line_source_term_tests/3D_line_source_term_in_cylinder/286k_prisms/line_source_term_in_cylinder.prj). The project files describe the processes to be solved and the related process variables together with their initial and boundary conditions as well as the source terms. @@ -123,4 +123,4 @@ src="../LineSourceTermFigures/plot_over_line_diff_and_rel_diff_analytical_soluti #### Input files The project file for the described model is -[line_source_term_in_cylinder.prj](https://github.com/ufz/ogs-data/blob/master/Parabolic/T/3D_line_source_term_tests/3D_line_source_term_in_cylinder_axisymmetric/line_source_term_in_cylinder.prj). +[line_source_term_in_cylinder.prj](https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/Parabolic/T/3D_line_source_term_tests/3D_line_source_term_in_cylinder_axisymmetric/line_source_term_in_cylinder.prj). diff --git a/web/content/docs/benchmarks/small-deformations/mechanics-linear-element_deactivation.pandoc b/web/content/docs/benchmarks/small-deformations/mechanics-linear-element_deactivation.pandoc index c622db3e9d6..ba444788724 100644 --- a/web/content/docs/benchmarks/small-deformations/mechanics-linear-element_deactivation.pandoc +++ b/web/content/docs/benchmarks/small-deformations/mechanics-linear-element_deactivation.pandoc @@ -37,8 +37,8 @@ The input data set of the element deactivation approach is specified inside the The input syntax can be also found in the project files of the two benchmarks: -* [2D](https://github.com/ufz/ogs/tree/master/Tests/Data/Mechanics/Linear/square_with_deactivated_hole.prj) -* [3D](https://github.com/ufz/ogs/tree/master/Tests/Data/Mechanics/Linear/ElementDeactivation3D/element_deactivation_M_3D.prj) +* [2D](https://gitlab.opengeosys.org/ogs/ogs/-/tree/master/Tests/Data/Mechanics/Linear/square_with_deactivated_hole.prj) +* [3D](https://gitlab.opengeosys.org/ogs/ogs/-/tree/master/Tests/Data/Mechanics/Linear/ElementDeactivation3D/element_deactivation_M_3D.prj) ## Mesh 2D and 3D meshes: diff --git a/web/layouts/shortcodes/data-url.html b/web/layouts/shortcodes/data-url.html index e5a30429979..9214fde932f 100644 --- a/web/layouts/shortcodes/data-url.html +++ b/web/layouts/shortcodes/data-url.html @@ -1 +1 @@ -https://github.com/ufz/ogs-data/blob/master/{{ .Get 0 }} +https://gitlab.opengeosys.org/ogs/ogs/-/blob/master/Tests/Data/{{ .Get 0 }} -- GitLab