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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 20:04:00 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 20:04:00 +0100 |
| commit | ad20dc17e7639f83a8cb3d6c1c84e7d3c75945e3 (patch) | |
| tree | 065fa8f41d1dba6ffedb186cc5e4219884177c89 /typst | |
| parent | a49f595c42d6c26e8b130dc6487caeceb80d8775 (diff) | |
| download | phd-fluid_mechanics_report-ad20dc17e7639f83a8cb3d6c1c84e7d3c75945e3.tar.gz | |
progress
Diffstat (limited to 'typst')
| -rw-r--r-- | typst/main.typ | 9 |
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 ? |
