blob: 112ed12a215746ab2537165ae765a4c9587bb5ca (
plain)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
|
// Title Page
= Solid particle interaction in Stokes flow
Author: "Claudius Holeksa"
Date: 2025-11-09
// Abstract
// == Abstract
// This is a brief summary of the report. It gives an overview of the objectives, methods, and conclusions.
// Table of Contents
[toc]
== 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
|