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authorClaudius "keldu" Holeksa <mail@keldu.de>2025-11-11 20:04:00 +0100
committerClaudius "keldu" Holeksa <mail@keldu.de>2025-11-11 20:04:00 +0100
commitad20dc17e7639f83a8cb3d6c1c84e7d3c75945e3 (patch)
tree065fa8f41d1dba6ffedb186cc5e4219884177c89
parenta49f595c42d6c26e8b130dc6487caeceb80d8775 (diff)
downloadphd-fluid_mechanics_report-ad20dc17e7639f83a8cb3d6c1c84e7d3c75945e3.tar.gz
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-rw-r--r--typst/main.typ9
1 files changed, 8 insertions, 1 deletions
diff --git a/typst/main.typ b/typst/main.typ
index 379a825..b2bd645 100644
--- a/typst/main.typ
+++ b/typst/main.typ
@@ -67,7 +67,7 @@ $ μ∇²u + f = ∇p,\
)
An additional restriction by the creeping flow equations is the selection of boundary criteria where it depends on
-a far-field criterion
+an infinite space with a set solid boundary interface.
== Solid-Fluid single sphere interaction with Stokes flow
@@ -82,6 +82,13 @@ $ F_S = 6 pi mu r v $
where according to Proudman and Pearson@proudman_pearson_1957 at a Reynolds number of 0.05 the predicted drag is two percent lower
than the possibly more correct value by Proudman and Pearson@proudman_pearson_1957.
+#math.equation(
+block: true,
+$ F_S = 6 pi mu r v $
+)
+
+
+
// Insert analytical solution
// Different boundary examples ?