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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 18:46:32 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 18:46:32 +0100 |
| commit | 08e74a4d2fefaae372fc3af3388acf977cfc7039 (patch) | |
| tree | 3a644bd8fff1d35d1136cdf4d50beb006d62bfd5 /typst | |
| parent | 3faab036a18c882f99a0eb6d1b2068d8fe4cac66 (diff) | |
| download | phd-fluid_mechanics_report-08e74a4d2fefaae372fc3af3388acf977cfc7039.tar.gz | |
progress
Diffstat (limited to 'typst')
| -rw-r--r-- | typst/main.typ | 4 |
1 files changed, 2 insertions, 2 deletions
diff --git a/typst/main.typ b/typst/main.typ index 08ce3a9..2676c32 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -44,7 +44,7 @@ The incompressible Navier Stokes equations are derived from Newton are a set of #math.equation( block: true, -$ ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f\ +$ ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f,\ ∇ · u = 0 $ ) @@ -55,7 +55,7 @@ and is assumed to be zero. // Stokes #math.equation( block: true, -$ μ∇²u − ∇p +f \ +$ μ∇²u − ∇p +f = 0,\ ∇ · u = 0 $ ) |
