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| -rw-r--r-- | typst/main.typ | 12 |
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. |