From 4419c1153d7d50a51d77d4c46bd40a80ac16140a Mon Sep 17 00:00:00 2001 From: Rene Gassmoeller Date: Thu, 20 Feb 2025 17:28:21 +0100 Subject: [PATCH] Fix Sphinx warnings --- benchmarks/advection/README.md | 2 +- benchmarks/advection/doc/advection.md | 2 +- benchmarks/rayleigh_taylor_instability/README.md | 2 +- .../doc/rayleigh_taylor_instability.md | 2 +- benchmarks/sinking_block/README.md | 2 +- benchmarks/sinking_block/doc/sinking_block.md | 2 +- 6 files changed, 6 insertions(+), 6 deletions(-) diff --git a/benchmarks/advection/README.md b/benchmarks/advection/README.md index 3d2233891d7..37aee45dded 100644 --- a/benchmarks/advection/README.md +++ b/benchmarks/advection/README.md @@ -13,4 +13,4 @@ Benchmarks: 2. Rotate Shape (rotate_shape_supg.prm, rotate_shape_ev.prm) Various shapes being rotated by 360 degrees by a fixed velocity -See [doc/advection.md](doc/advection.md) for details. +See [](doc/advection) for details. diff --git a/benchmarks/advection/doc/advection.md b/benchmarks/advection/doc/advection.md index 457796a9064..fff404b9705 100644 --- a/benchmarks/advection/doc/advection.md +++ b/benchmarks/advection/doc/advection.md @@ -23,7 +23,7 @@ Both benchmarks have the identical setup in the temperature and a compositional field. The only difference is that the temperature equation contains a (small) physical diffusion term. -**[Description of benchmark files](../README.md)** +**[Description of benchmark files](../README)** ```{figure-md} fig:benchmark-drop diff --git a/benchmarks/rayleigh_taylor_instability/README.md b/benchmarks/rayleigh_taylor_instability/README.md index 72b2d434f5a..f2802511331 100644 --- a/benchmarks/rayleigh_taylor_instability/README.md +++ b/benchmarks/rayleigh_taylor_instability/README.md @@ -11,4 +11,4 @@ This file can later be processed with the 'gnuplot_script'. There is also the standalone input file `rayleigh_taylor_instability.prm` which runs only one of the cases (isoviscous and lambda=256km). -See [doc/rayleigh_taylor_instability.md](doc/rayleigh_taylor_instability.md) for more information. +See [](doc/rayleigh_taylor_instability) for more information. diff --git a/benchmarks/rayleigh_taylor_instability/doc/rayleigh_taylor_instability.md b/benchmarks/rayleigh_taylor_instability/doc/rayleigh_taylor_instability.md index 8afd0970dc1..a7a8c6a51f6 100644 --- a/benchmarks/rayleigh_taylor_instability/doc/rayleigh_taylor_instability.md +++ b/benchmarks/rayleigh_taylor_instability/doc/rayleigh_taylor_instability.md @@ -57,7 +57,7 @@ file: end -**[Description of benchmark files](../README.md)** +**[Description of benchmark files](../README)** ```{figure-md} fig:RTi_grids_a diff --git a/benchmarks/sinking_block/README.md b/benchmarks/sinking_block/README.md index e21d5ca4082..c76a8733794 100644 --- a/benchmarks/sinking_block/README.md +++ b/benchmarks/sinking_block/README.md @@ -8,4 +8,4 @@ In order to run the benchmark for many resolution, density and viscosity combina all the input files generated inside the triple loop. The `sinking_block.prm` input file is the standalone prm file for the sinking block benchmark. -For more information see [doc/sinking_block.md](doc/sinking_block.md). +For more information see [](doc/sinking_block). diff --git a/benchmarks/sinking_block/doc/sinking_block.md b/benchmarks/sinking_block/doc/sinking_block.md index ed7b247a911..ae5f76153e6 100644 --- a/benchmarks/sinking_block/doc/sinking_block.md +++ b/benchmarks/sinking_block/doc/sinking_block.md @@ -34,7 +34,7 @@ $\delta\rho=8,32,128~\text{ kg m}^{-3}$. Results are shown in {numref}`fig:sinking_block2` and we indeed recover the expected trend with all data points forming a single smooth line. -**[Description of benchmark files](../README.md)** +**[Description of benchmark files](../README)** ```{figure-md} fig:sinking_block1