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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 19:27:18 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 19:27:18 +0100 |
| commit | 53e391f99ee69ff9036c85f2e754f99fe54b4921 (patch) | |
| tree | 59bbc2b74111e24a4eef1c8f21c292b49f8075b0 | |
| parent | 07ef13c9335e26e4bf0f27139923b319fd3cb126 (diff) | |
| download | phd-fluid_mechanics_report-53e391f99ee69ff9036c85f2e754f99fe54b4921.tar.gz | |
progress
| -rw-r--r-- | typst/main.typ | 15 |
1 files changed, 7 insertions, 8 deletions
diff --git a/typst/main.typ b/typst/main.typ index 410a685..f1f6d43 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -63,17 +63,16 @@ $ μ∇²u + f = ∇p,\ == Solid-Fluid interaction with Stokes flow -For a solid sphere of radius a moving with velocity $U$ in an unbounded creeping flow, -we define the - -// Insert analytical solution - +With the previous assumptions a solid sphere of radius $r$ moving with velocity $u$ in an unbounded creeping flow, +we receive the drag force provided by Stokes +#math.equation( +block: true, +$ F = 6 pi mu r u $ +) -Since -// Boundary -// +// Insert analytical solution // Different boundary examples ? |