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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 10:34:05 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 10:34:05 +0100 |
| commit | dbf44aa8131acabf9c7d1cbcea474d34791c9096 (patch) | |
| tree | d0772a17acc9d1ab495e05e0cca687f603519c1f /typst | |
| parent | 96af1217da5d3851faf5fad2eb2b8365b29a4bf0 (diff) | |
| download | phd-fluid_mechanics_report-dbf44aa8131acabf9c7d1cbcea474d34791c9096.tar.gz | |
progress
Diffstat (limited to 'typst')
| -rw-r--r-- | typst/main.typ | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/typst/main.typ b/typst/main.typ index 136dc6c..6076b9f 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -58,7 +58,7 @@ velocity field $u(x,t)$ the Navier-Stokes formulation is primarly defined by the #math.equation( block: true, -$ rho D/(Dt)u = ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f,\ +$ rho D/(D t)u = ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f,\ ∇ · u = 0 $ ) |