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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 19:31:17 +0100 |
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| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 19:31:17 +0100 |
| commit | 1e46dbd8fc1b76a5c53f6b414324ffe68fd6f782 (patch) | |
| tree | 2d1d6e60f1969bb1e33a4dfd58a0cbe4df225ea2 | |
| parent | 58c7224387793f9ad288ffdd4b5d5921eed23df4 (diff) | |
| download | phd-fluid_mechanics_report-1e46dbd8fc1b76a5c53f6b414324ffe68fd6f782.tar.gz | |
progress
| -rw-r--r-- | typst/main.typ | 5 |
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 |