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#import "@preview/charged-ieee:0.1.3": ieee
#show: ieee.with(
title: [Stokes flow - Particle interaction in low Reynolds Number environments],
abstract: [
],
authors: (
(
name: "Claudius Holeksa",
department: [CSSR],
organization: [NORCE Research AS],
location: [Bergen, Norway],
email: "clho@norceresearch.no"
),
),
index-terms: ("Scientific writing", "Typesetting", "Document creation", "Syntax"),
bibliography: bibliography("refs.bib"),
figure-supplement: [Fig.],
)
= Introduction
For the understanding of near-well injections multiple elements such as multiphase behaviour, particle-solid interaction and
the geometry of the porous structure is required.
While at heart most numerical modelling approaches such as the Lattice-Boltzmann-Method are based on the Navier-Stokes Equations,
here we will take a glance on a more special case.
Since we are interested in very viscous cases with our Reynolds number (Re \< \< 1) our base equation reduces itself to the Stokes Equations,
which are well understand in terms of the description by Stokes [dummy, I mean the old paper from 1851].
So the Navier-Stokes equations
todo insert NS eqs here
are reduced to
todo insert S eqs here
// Rather move this to the lower chapters and use book citations I guess. Well, maybe also Stokes paper. The initial rant is quite fun
== Navier
The Navier Stokes equations are governed as follows
// we don't really need the external force here? do we?
#math.equation(
block: true,
$ 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 fluids the viscosity dominates.
== Solid-Fluid interaction with Stokes flow
So while
// References
== References
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