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authorClaudius "keldu" Holeksa <mail@keldu.de>2025-11-11 19:31:17 +0100
committerClaudius "keldu" Holeksa <mail@keldu.de>2025-11-11 19:31:17 +0100
commit1e46dbd8fc1b76a5c53f6b414324ffe68fd6f782 (patch)
tree2d1d6e60f1969bb1e33a4dfd58a0cbe4df225ea2 /typst
parent58c7224387793f9ad288ffdd4b5d5921eed23df4 (diff)
downloadphd-fluid_mechanics_report-1e46dbd8fc1b76a5c53f6b414324ffe68fd6f782.tar.gz
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Diffstat (limited to 'typst')
-rw-r--r--typst/main.typ5
1 files changed, 5 insertions, 0 deletions
diff --git a/typst/main.typ b/typst/main.typ
index 701d242..546dbad 100644
--- a/typst/main.typ
+++ b/typst/main.typ
@@ -61,6 +61,9 @@ $ μ∇²u + f = ∇p,\
∇ · u = 0 $
)
+An additional restriction by the creeping flow equations is the selection of boundary criteria where it depends on
+a far-field criterion
+
== Solid-Fluid interaction with Stokes flow
With the previous assumptions a solid sphere of radius $r$ moving with velocity $v$ in an unbounded creeping flow,
@@ -71,6 +74,8 @@ block: true,
$ F = 6 pi mu r v $
)
+where according to Proudman and Pearson@proudman_and_pearson the predicted drag is two percent lower than possibly more correct value
+by Proudman and Pearson@proudman_and_pearson.
// Insert analytical solution