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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 10:01:38 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-12 10:01:38 +0100 |
| commit | 575b5b337e35c337caca39810974f51780fc6522 (patch) | |
| tree | 5506c220cd8f53d1d528ac83e5475428eba6c85c | |
| parent | d6a75f8c33488a2b50f89266a0394a5862c891d5 (diff) | |
| download | phd-fluid_mechanics_report-575b5b337e35c337caca39810974f51780fc6522.tar.gz | |
progress
| -rw-r--r-- | typst/main.typ | 6 |
1 files changed, 4 insertions, 2 deletions
diff --git a/typst/main.typ b/typst/main.typ index 31fc934..9ca5a8c 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -51,8 +51,10 @@ Explores the effect of it in porous media and examines the more recent particle == Stokes Flow // Write about Navier -The incompressible Navier Stokes equations are a set of equations defined with the density $rho$, the dynamic viscosity $mu$ and the -velocity field $u(x,t)$ +The governing equations for incompressible flow arise from the Navier-Stokes formulation, which describes the conservation of momentum +and mass in a viscous fluid. +For a fluid with density $rho$, the dynamic viscosity $mu$ and the +velocity field $u(x,t)$ the Navier-Stokes formulation is primarly defined by the equations #math.equation( block: true, |