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authorClaudius "keldu" Holeksa <mail@keldu.de>2025-11-11 17:23:21 +0100
committerClaudius "keldu" Holeksa <mail@keldu.de>2025-11-11 17:23:21 +0100
commitd54fdc99d978f93d164b51609f02d52601793893 (patch)
tree8c9b8c14149ee92a08ec402446ccc0c1ed91f1ec /typst
parent5defae18eaa7e7baf47efdf26c537d45691b7fe9 (diff)
downloadphd-fluid_mechanics_report-d54fdc99d978f93d164b51609f02d52601793893.tar.gz
progress
Diffstat (limited to 'typst')
-rw-r--r--typst/main.typ12
1 files changed, 5 insertions, 7 deletions
diff --git a/typst/main.typ b/typst/main.typ
index 81dd6ae..10c7663 100644
--- a/typst/main.typ
+++ b/typst/main.typ
@@ -13,7 +13,7 @@
email: "clho@norceresearch.no"
),
),
- index-terms: ("Scientific writing", "Typesetting", "Document creation", "Syntax"),
+ index-terms: ("Fluid Mechanics", "Review"),
bibliography: bibliography("refs.bib"),
figure-supplement: [Fig.],
)
@@ -36,7 +36,8 @@ This report delves into the central aspects governing the known behaviour past s
Explores the effect of it in porous media and examines the more recent particle bridging behaviour found in porous structures.
-== Navier
+
+== Stokes Flow
// Write about Navier
The incompressible Navier Stokes equations are a set of equations
@@ -47,16 +48,13 @@ $ ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f\
∇ · u = 0 $
)
-// Introduction
-== Stokes flow
-
While we are often interested in Navier-Stokes flows, on higher viscous fluid such as in the earth's mantle the inertial term is negligable.
-Since we
+Since we can assume the inertial term
// Stokes
#math.equation(
block: true,
-$ ρ((∂)/(∂t)u + (u · ∇)u) = −∇p + μ∇²u + f\
+$ 0 = −∇p + μ∇²u + f\
∇ · u = 0 $
)