Bump crate-ci/typos from 1.14.12 to 1.15.0 (#1524)

* Bump crate-ci/typos from 1.14.12 to 1.15.0 Bumps [crate-ci/typos](https://github.com/crate-ci/typos) from 1.14.12 to 1.15.0. - [Release notes](https://github.com/crate-ci/typos/releases) - [Changelog](https://github.com/crate-ci/typos/blob/master/CHANGELOG.md) - [Commits](crate-ci/typos@v1.14.12...v1.15.0) --- updated-dependencies: - dependency-name: crate-ci/typos dependency-type: direct:production update-type: version-update:semver-minor ... Signed-off-by: dependabot[bot] <[email protected]> * Fix typos --------- Signed-off-by: dependabot[bot] <[email protected]> Co-authored-by: dependabot[bot] <49699333+dependabot[bot]@users.noreply.github.com> Co-authored-by: Michael Schlottke-Lakemper <[email protected]>
trixi-framework · Jun 16, 2023 · deb027a · deb027a
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commit deb027a
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diff --git a/.github/workflows/SpellCheck.yml b/.github/workflows/SpellCheck.yml
@@ -10,4 +10,4 @@ jobs:
       - name: Checkout Actions Repository
         uses: actions/checkout@v3
       - name: Check spelling
-        uses: crate-ci/typos@v1.14.12
+        uses: crate-ci/typos@v1.15.0
diff --git a/docs/src/visualization.md b/docs/src/visualization.md
@@ -339,7 +339,7 @@ create a [`PlotData1D`](@ref) with the keyword argument `curve` set to your list
 Let's give an example of this with the basic advection equation from above by creating
 a plot along the circle marked in green:
 
-![2d-plot-along-cirlce](https://user-images.githubusercontent.com/72009492/130951042-e1849447-8e55-4798-9361-c8badb9f3a49.png)
+![2d-plot-along-circle](https://user-images.githubusercontent.com/72009492/130951042-e1849447-8e55-4798-9361-c8badb9f3a49.png)
 
 We can write a function like this, that outputs a list of points on a circle:
 ```julia

diff --git a/examples/p4est_2d_dgsem/elixir_euler_supersonic_cylinder.jl b/examples/p4est_2d_dgsem/elixir_euler_supersonic_cylinder.jl
@@ -3,7 +3,7 @@
 # Boundary conditions are supersonic Mach 3 inflow at the left portion of the domain
 # and supersonic outflow at the right portion of the domain. The top and bottom of the
 # channel as well as the cylinder are treated as Euler slip wall boundaries.
-# This flow results in strong shock refletions / interactions as well as Kelvin-Helmholtz
+# This flow results in strong shock reflections / interactions as well as Kelvin-Helmholtz
 # instabilities at later times as two Mach stems form above and below the cylinder.
 #
 # For complete details on the problem setup see Section 5.7 of the paper: