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authorClaudius "keldu" Holeksa <mail@keldu.de>2025-11-12 13:43:37 +0100
committerClaudius "keldu" Holeksa <mail@keldu.de>2025-11-12 13:43:37 +0100
commit6b2481b8475f08deac78609aadb587a1e00b9efb (patch)
treefaf206d6b8ab625e7fa655f3299c99f41d56a1e8 /typst
parent473bd153f4b94b01cf83cde0bacaf85c69c1f6c4 (diff)
downloadphd-fluid_mechanics_report-6b2481b8475f08deac78609aadb587a1e00b9efb.tar.gz
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Diffstat (limited to 'typst')
-rw-r--r--typst/main.typ12
1 files changed, 4 insertions, 8 deletions
diff --git a/typst/main.typ b/typst/main.typ
index d53a42f..53ee1db 100644
--- a/typst/main.typ
+++ b/typst/main.typ
@@ -180,7 +180,7 @@ And while sieving and bridging results from purely mechanical forces aggregation
#figure(
image("narrow_channel.png"),
-caption: [One setup example from Laurez@laurez2025bridging]
+caption: [One example geometry from Laurez@laurez2025bridging describing]
)
@@ -193,8 +193,7 @@ Which in turn makes a stochastic analysis of particles in different conditions@l
Laurez@laurez2025bridging goes into detail based on CITE FIG how probable clogging mechanisms are, while these are quite indepth, opportunities
in relation to multiphase fluid interaction with the solid structures arise.
-Another interesting case
-
+Another interesting case is a variation in inbound pressure as usually the experimental setup
// Insert png
@@ -220,8 +219,5 @@ cell level, making it ideal for digital rock simulations and is often employed i
The equisdistant grid and the properties of a cellular automaton make it a prime target for acceleration due to the local
dependencies @krueger2017lbm.
-=== Immersed Boundary Method
-
-To couple a particle dynamics system with the LBM modell,
-
-=== Homogenized Lattice-Boltzmann
+To couple a particle dynamics system two major approaches exist within Lattice Boltzmann.
+The immersed boundary method and the homogenized Lattice-Boltzmann-Method.