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| author | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 19:04:04 +0100 |
|---|---|---|
| committer | Claudius "keldu" Holeksa <mail@keldu.de> | 2025-11-11 19:04:04 +0100 |
| commit | 07ef13c9335e26e4bf0f27139923b319fd3cb126 (patch) | |
| tree | 0de5e53e5e1e2ead559ad86a1275acb2b81cae0b | |
| parent | 15ab84f083234ea6eddac6e1481991bbfd86e44d (diff) | |
| download | phd-fluid_mechanics_report-07ef13c9335e26e4bf0f27139923b319fd3cb126.tar.gz | |
progress
| -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 8ff3227..410a685 100644 --- a/typst/main.typ +++ b/typst/main.typ @@ -50,7 +50,7 @@ $ ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f,\ While we are often interested in Navier-Stokes flows, a generalized analytical solution does not exist, most analytical approaches rely on a set of restrictions or assumptions. -Luckily we decided to work on a fluid which tends $"Re" arrow 0$ where due to the viscous forces +Luckily we decided to work on a fluid which tends $"Re" arrow 0$ or at least $"Re" << 1$ where due to the viscous forces the inertial term is negligable and is assumed to be zero. Which is why we arrive at this term |