Download - Bakterienwachstum: Hydrodynamische Modelle
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IntroductionDerivation of a hydrodynamic model
Results
Bakterienwachstum: Hydrodynamische Modelle
Johannes Greber
WWU Münster
November 14, 2008
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IntroductionDerivation of a hydrodynamic model
Results
Outline
1 Introduction
2 Derivation of a hydrodynamic model
3 Results
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IntroductionDerivation of a hydrodynamic model
Results
Introduction
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IntroductionDerivation of a hydrodynamic model
Results
Experimental background
Experiments on the growth of bacterial colonies are very easyIn a petri dish with a thin layer of agar bacteria are injected ina small inoculum.Closer look to the colony via light microscopic methods.
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IntroductionDerivation of a hydrodynamic model
Results
Experimental results
The concentrations of nutrients are 0.1, 0.5, 1.0, 2.0 and3.0gl−1 from left to rightStructures become denser for higher concentration ofnutrients. For low concentration, dense patterns are onserved.
0Y. Kozlovsky et al (1999)
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IntroductionDerivation of a hydrodynamic model
Results
Envelopes
Sharp envelopes down to microscopic scales are observed.In "dry" regions bacteria produce extracellular liquid for beingabel to swim.
0Y. Kozlovsky et al (1999)0E. Ben-Jacob et al. (1994)
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IntroductionDerivation of a hydrodynamic model
Results
Dynamics and Vortices
Vortices in motion of the bacteria in water.
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IntroductionDerivation of a hydrodynamic model
Results
Derivation of a hydrodynamic model
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IntroductionDerivation of a hydrodynamic model
Results
Basics
The hydrodynamics of bacterial colonies can be discribed by fourcoupled partial differential equations for the densities of:
nutrients (S)water (W )bacteria(N)
and the dynamics of the velocity field (v)
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IntroductionDerivation of a hydrodynamic model
Results
Dynamics of nutrients
Dynamics of nutrients can be discribed by a reaction-diffusionequation:
∂S∂t
= RS(S ,N,W ) + DS∇2S
RS(S ,N,W ): consumption of nutrients by the bacteria.
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IntroductionDerivation of a hydrodynamic model
Results
Dynamics of the bacteria
Continuity equation for dynamics of bacteria:
∂N∂t
+∇ · (Nv) = RN −∇jN
With jN = −DN∇N one obtains
∂N∂t
+∇ · (Nv) = RN +∇(DN(S ,N,W )∇N).
RN represents growth of the bacterial colonie.
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IntroductionDerivation of a hydrodynamic model
Results
The bacterial liquid
The behavior of the bacterial liquid and the interaction betweenbacteria is still relativly unknown. Assumptions are:
The bacteria constitute a compressible Newtonian liquid.Bacteria are living species. They show an individuell activityrepresented by noise.
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IntroductionDerivation of a hydrodynamic model
Results
Dynamics of water
Continuity equation for density of water:
∂W∂t
+∇ · (Wv) = RW +∇(DW (S ,N,W )∇N)−∇jW
jN = −jW can be assumed.
∂W∂t
+∇·(Wv) = RW +∇(DW (S ,N,W )∇N)−∇(DN(S ,N,W )∇N)
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IntroductionDerivation of a hydrodynamic model
Results
Conservation of momentum
The conservation equation of linear momentum of the mixture isthe Navier-Stokes equation:
ρ∂v∂t
+ ρ(v · ∇v) = ∇T + F
ρ = N + W
T : stress tensorF : external forces
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IntroductionDerivation of a hydrodynamic model
Results
The stress tensor
T can be written as:
∇T = −∇p + µ∇2v + λ∇(∇v)
p = pW + pN : pressure of the complex fluidµ : dynamic viscosityλ : second viscosity takes into acount that the bacterial fluid iscompressible.
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IntroductionDerivation of a hydrodynamic model
Results
Pressure terms
Water is assumed to be incompressible, so that pW is a function ofthe velocity field vW of water so that
∇vW = 0
The pressure of the bacterial phase can be separated in aincompressible and a compressible part proportional to N2
pN = pN0 + pN
c = pN0 + γ(S ,W )N2
γ > 0 rises a force which drives bacteria away from overcrowdedareas.
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IntroductionDerivation of a hydrodynamic model
Results
External forces
The external forces can be written as:
F = Fs + Fg + Fe
Fs : interaction between the fluid and the agar (Fs = −αv)Fg : describes changes due to bacterial activity.Fe : external forces on the whole system, such as gravity.
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IntroductionDerivation of a hydrodynamic model
Results
The four differential equations
The four basic equations can be written as:
∂S∂t
= RS(S ,N,W ) + DS∇2S (1)
∂N∂t
+∇ · (Nv) = RN +∇(DN(S ,N,W )∇N) (2)
∂W∂t
+∇ · (Wv) = RW +∇(DW (S ,N,W )∇N)
−∇(DN(S ,N,W )∇N) (3)
∂v∂t
+ (v · ∇v) =1
N + W(∇T + Fs + Fg ) (4)
0J. Lega, T. Passot (2006)
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IntroductionDerivation of a hydrodynamic model
Results
Reduction on two dimensions
The fluid motion takes place in a layer of thickness smallthickness h.The problem can be reduced to a two dimensional one withv(x,y,z) = f(z)u(x,y) and integrating over h
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IntroductionDerivation of a hydrodynamic model
Results
The two dimensional problem
The four equations from above transform to:
∂S∂t
= RS(S ,N,W ) + DS∇2hS (5)
∂N∂t
+∇h · (Nv) = RN +∇h(DN(S ,N,W )∇hN) (6)
∂W∂t
+∇h · (Wv) = RW +∇h(DW (S ,N,W )∇hN)
−∇h(DN(S ,N,W )∇hN) (7)
∂v∂t
+ ζ(v · ∇hv) =1
N + W{−∇hp + µ∇2
hv + λ∇h(∇h · v)
−ηv + F s + F g )} (8)
0J. Lega, T. Passot (2006)
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IntroductionDerivation of a hydrodynamic model
Results
Last unknown quanties
In these equations the following quantities mean:
v(x ,y) = 〈f 〉u(x ,y)
ζ =〈f 2〉〈f 〉2
,
F = 〈F 〉 means:
〈F 〉 =1h
∫ 0
−hF (z)dz
For an arbitrary function F(z)The two dimensional approximation is accurate if ζ ' 1.
0J. Lega, T. Passot (2006)
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IntroductionDerivation of a hydrodynamic model
Results
Reaction terms
Taking into acount nutrient consumption by and growth of bacteriathe first reaction terms become:
RS(S ,N,W ) = −RN(S ,N,W ) = NS
In this model loss of water, e. g. by evaporation at the surface, isneglected:
RW (S ,N,W ) = 0
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IntroductionDerivation of a hydrodynamic model
Results
Results
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IntroductionDerivation of a hydrodynamic model
Results
Simulations
0J. Lega, T. Passot (2006)
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IntroductionDerivation of a hydrodynamic model
Results
A closer look at the envelope
0J. Lega, T. Passot (2006)
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IntroductionDerivation of a hydrodynamic model
Results
Abilities and Linitations of the model
AbilitiesNumerical simulations of the model show the branching ingrowth of the colony.Vortices as seen in the experiment shown above are obtained.
LimitationsThe interaction between bacteria is still almost unknownPerhaps the ansatz of a Newtonian fluid for the bacterial phaseis not the best.Quantitative description of the branching process is still anopen question.
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IntroductionDerivation of a hydrodynamic model
Results
Thank you for your attention!
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IntroductionDerivation of a hydrodynamic model
Results
Lyrics
E. Ben-Jacob et al. : Letters to Nature (1994)Genericmodeling of cooperative growth patterns in bacterial colonies.J. Lega, T. Passot : Journal of Nonlinearity (2006)Hydrodynamics of bacterial colonies.J. Lega, T. Passot : Physical Review Letters (2003)Hydrodynamics of bacterial colonies: A model.Y. Kozlovsky et al. : Physical Review Letters (1999)Lubricating bacteria model for branching growth of bacterialcolonies