SLIDE 1 Mathematical models for biofilms on the surface of monuments
Magali Ribot
Laboratoire J.-A. Dieudonn´ e Universit´ e de Nice, UMR 6621 CNRS in collaboration with
- F. Clarelli (Univ. dell’Aquila & I.A.C. – C.N.R. Roma),
- C. Di Russo (Univ. Roma 3 & I.A.C. – C.N.R. Roma),
- R. Natalini (I.A.C. – C.N.R. Roma)
Thursday, September 4 th, 2008
SLIDE 2 Outline
- 1. What is a biofilm ?
- 2. Previous mathematical models for biofilms
- 3. A new multidimensional model for biofilms
- 4. Numerical scheme
- 5. Numerical results
- 6. Perspectives
SLIDE 3 Definition of biofilm
◮ A biofilm is a complex mix of microorganisms (bacteria,
cyanobacteria, algae, protozoa and fungi) that are associated
- r embedded within a polymer matrix and which are
colonizing a certain surface.
◮ At one time, this term was confined to surfaces in constant
contact with water (solid/liquid interface), but now has been extended to any interface (air/solid, liquid/liquid or air/liquid), where growth of microorganisms occurs.
SLIDE 4
Staph Infection (Staphylococcus aureus biofilm) of the surface of a catheter.
SLIDE 5 Biofilm formation
- 1. Attachment : Bacteria approach the surface and get attached.
- 2. Colonization : Bacteria lose flagella and produce EPS.
- 3. Growth : Bacteria build the 3D biofilms and then specialize
(fixed cells, motile cells, monolayer cells).
SLIDE 6
Biofilm properties
◮ Combination of moisture, nutrients and surface. ◮ Surface attachment.
SLIDE 7
Biofilm properties
◮ Combination of moisture, nutrients and surface. ◮ Surface attachment.
⊲ Complex community interactions (cooperation between many species of bacteria) and mechanism. ⊲ Formation of an Extracellular matrix of Polymeric Substances (EPS).
SLIDE 8
Biofilm properties
◮ Combination of moisture, nutrients and surface. ◮ Surface attachment.
⊲ Complex community interactions (cooperation between many species of bacteria) and mechanism. ⊲ Formation of an Extracellular matrix of Polymeric Substances (EPS). ◮ EPS : Resistance to antibiotics and immune system, disinfectants and cleaning fluids. ◮ Possible bioremediation of waste sites, water-cleaning systems, formation of biobarriers to protect soil from contamination.
SLIDE 9
Multispecies biofilm growing on a biofilm carrier
◮ Finger type structures.
SLIDE 10
Stone degradation
Two types of degradation :
◮ Epilithic zones : De-cohesion and loss of substrate material
from the surface of the monuments (granular disaggregation, flaking and pitting).
◮ Endolithic zones : Degradation of internal structure
(penetration, geomechanical effects).
SLIDE 11
SLIDE 12
Cyanobacteria [Tiano]
◮ Develop on a water film on the stone’s surface. ◮ Die during cold and dry seasons & deposit of dead cells, which
lead to rapid new growth at warm time.
◮ Need warmth and light to develop. ◮ Nutrients : CO2, N2 and salt minerals traces. ◮ Anaesthetic coloured patinas.
SLIDE 13 Outline
- 1. What is a biofilm ?
- 2. Previous mathematical models for biofilms
- 3. A new multidimensional model for biofilms
- 4. Numerical scheme
- 5. Numerical results
- 6. Perspectives
SLIDE 14 Delft team’s models [Picioreanu, Noguera et al.]
Characteristics :
◮ Multi-dimensional, multispecies and multi-substrates ODEs
model.
◮ Discrete models : Individual-based approach (hard spheres) or
Cellular Automata.
◮ Simulation of detachment.
Problems :
- Large system of equations .
- Very sensitive to initial conditions.
- Difficult to take into account spatial behaviour of particles.
SLIDE 15
Delft team’s models(2)
SLIDE 16 A multiD & multispecies model [Alpkvist & Klapper, 2007]
◮ Extension of the one-dimensional model of Wanner & Gujer
[Wanner & Gujer, 1986].
◮ Multi-dimensional, multispecies and multi-substrates PDEs
model.
◮ Biofilms are divided into two phases : biomass and liquid. ◮ Equations :
- Elliptic equations for substrates and transport equations for
biomass.
- Transport of all biomass species with the same velocity u that
follows Darcy’s law.
◮ Numerical simulations : front tracking and level set
methods.
SLIDE 17
Alpkvist & Klapper’s model (2)
Problems :
◮ Difficult to obtain sharp interfaces and finger like structures.
⇒ Implementation of level set methods.
SLIDE 18 A 1D model with quorum sensing [Anguige, King & Ward, 2006]
◮ Medical setting (Pseidomonas aeruginosa biofilm). ◮ One-dimensional, multispecies PDEs model. ◮ 4 phases : live cells(C), dead cells(D) , EPS(E) and liquid(W). ◮ Influence of nutrients (oxygen) and of Quorum Sensing (QS). ◮ Tests of different treatments (antibiotic and antiQS drugs). ◮ Equations :
- Hyperbolic equations for B, D, E and W .
- 1 common velocity for B, D and E and 1 velocity for W .
- Advection-diffusion equations for nutrients, antibiotics,
antiQS...
- BUT closure of system by condition : W = W0 + αE.
◮ Travelling waves analysis.
SLIDE 19 A 2D fluid multicomponents model[Zhang, Cogan, Wang, 2008]
◮ 2 phases : polymer network and solvent(=substrate with
nutrients ?).
◮ Nutrients are coming from the substrate. ◮ Equations :
- Momentum equation for the average velocity v.
- Transport equation for nutrient concentration
- Transport equation for polymer networks with a modified
velocity (modified Cahn-Hilliard equation).
◮ Numerical simulations of pitching-off (or detachment) and
shedding.
SLIDE 20
Zhang, Cogan & Wang’s model (2)
SLIDE 21 Outline
- 1. What is a biofilm ?
- 2. Previous mathematical models for biofilms
- 3. A new multidimensional model for biofilms
- 4. Numerical scheme
- 5. Numerical results
- 6. Perspectives
SLIDE 22 Mass balance equations
Unknowns :
- B,D,E, L = volume ratios of cyanoBacteria, Dead
cyanobacteria, EPS and Liquid.
- vS=velocity of cells and EPS ; vL =velocity of liquid.
- ΓB, ΓD, ΓE, ΓL= mass exchange rates of B, D, E, L.
◮ Equations of mass balance are :
∂tY + ∇ · (Y vS) = ΓY , (Y = B, D, E), (1) ∂tL + ∇ · (LvL) = ΓL. (2)
◮ Volume constraint :
B + D + E + L = 1. (3)
SLIDE 23 Mass exchange rates
- I=lux intensity ; θ=temperature ; N=nutrients.
◮ Conservation of mass :
ΓB + ΓD + ΓE + ΓL = 0. (4)
◮ Mass exchange rate for B (cyanobacteria) :
ΓB = kB(I, θ, N) BL
− kD(I, θ, N) B
.
◮ Mass exchange rate for D (dead bacteria) :
ΓD = αkD(I, θ, N) B
− kN(θ) D
natural decay
.
◮ Mass exchange rate for E (EPS) :
ΓE = kE(θ) BL
− εE
.
SLIDE 24 Force balance conservation [Preziosi et al, ...]
- P=hydrostatic pressure.
- Σ=stress function (Σ = γ(1 − L)).
- Assumption : interaction forces for the liquid as Darcy’s
law : −M(vL − vS).
◮ Force balance for B, D and E :
∂t((1 − L)vS) + ∇ · ((1 − L)vS ⊗ vS) = −(1 − L)∇P + ∇Σ + M(vL − vS) − ΓLvL, (5)
◮ Force balance for L :
∂t(LvL) + ∇ · (LvL ⊗ vL) = −L∇P − M(vL − vS) + ΓLvL. (6)
SLIDE 25 Closure of the system & Boundary conditions
Closure of the system :
◮ Sum of the 4 mass balance equations (1), (2) & Volume
constraint (3) & Conservation of mass (4) give : ∇ · ((1 − L)vS + LvL) = 0. (7)
◮ Divergence of the sum of the 2 force balance equations (5),
(6) & Equation (7) give : −∆P = ∇ · (∇ · ((1 − L)vS ⊗ vS + LvL ⊗ vL)) − ∆Σ. Boundary conditions :
- No-flux BC for the velocities : vS · n|∂Ω = vL · n|∂Ω = 0.
- Neumann BC for the volume ratios :
∇B · n|∂Ω = ∇E · n|∂Ω = ∇D · n|∂Ω = 0.
SLIDE 26
Final system
◮ Equations for the volume ratios :
∂tB + ∇ · (BvS) = B (LkB(I, θ, N) − kD(I, θ, N)) , (S1) ∂tD + ∇ · (DvS) = αBkD(I, θ, N) − DkN(θ), (S2) ∂tE + ∇ · (EvS) = BLkE(θ) − εE, (S3) L = 1 − (B + D + E) (S4)
◮ Equations for the velocities :
∂t((1 − L)vS) + ∇ · ((1 − L)vS ⊗ vS) + (1 − L)∇P = ∇Σ + (M − ΓL)vL − MvS, (S5) ∂t(LvL) + ∇ · (LvL ⊗ vL) + L∇P = −(M − ΓL)vL + MvS, (S6)
◮ Equation for the pressure :
−∆P = ∇ · (∇ · ((1 − L)vS ⊗ vS + LvL ⊗ vL)) − ∆Σ. (S7)
SLIDE 27 Remarks about the model
◮ Simplifications in the 1D case :
- Expression of ∂xP on behalf of vS and vL :
−∂xP = ∂x((1 − L)vS
2 + LvL 2) − ∂xΣ.
- Relation between vL and vS :
(1 − L)vS + LvL = 0.
◮ {(B, D, E) ∈ [0, 1]3; 0 ≤ B + D + E ≤ 1} is an invariant
domain under the following conditions : kD, kE ≥ 0, [(1 − α)B + D]kD0 + εE + (vS − vL)∇L ≥ 0, if L = 0.
SLIDE 28 Extension of the model with the influence of light, temperature and nutrients
kB(I, θ, N) = kB0 ∗ p(I) ∗ N ∗ e− (θ−θc )2
d2
, kD(I, θ, N) = kD0
- 1 − 0.4 ∗ p(I) ∗ N ∗ e− (θ−θc )2
d2
kE(θ) = kE0 ∗ e− (θ−θc )2
d2
, kN(θ) = kN0 ∗ e− (θ−θc )2
d2
. where
◮ p(I) = (b + 2√ac) ×
I aI 2 + bI + c ,
◮ I(x, z, t) = I0(t) exp
Lz
z
g(1 − L(x, s, t))ds
◮ N satisfies a reaction-diffusion equation.
SLIDE 29 Outline
- 1. What is a biofilm ?
- 2. Previous mathematical models for biofilms
- 3. A new multidimensional model for biofilms
- 4. Numerical scheme
- 5. Numerical results
- 6. Perspectives
SLIDE 30 Numerical scheme
Notations : δt= time step ; tn = nδt= iteration time ; Y n=approximation of function Y at time tn.
- 1. Resolution of equations (S1), (S2), (S3) as (Y = B, D, E) :
Y n+1 = Y n − δt (∇ · (Y vS))n + δt Γn
Y .
- 2. Computation of Ln+1 = 1 − (Bn+1 + Dn+1 + E n+1).
- 3. Resolution of equations (S5), (S6) (Φ = (M − ΓL)vL − MvS) :
(1 − Ln+1)vSn+1 = (1 − Ln)vSn − δt (∇ · ((1 − L)vS ⊗ vS))n − δt ((1 − L)∇P)n + δt (∇Σ)n+1 + δtΦn. Ln+1vLn+1 = LnvLn − δt (∇ · (LvL ⊗ vL) + L∇P)n − δtΦn.
- 4. Resolution of equation (S7) :
−∆Pn+1 = ∇·(∇ · ((1 − L)vS ⊗ vS + LvL ⊗ vL))n+1−∆Σn+1.
SLIDE 31 An implicit scheme
Problem :
- Computed : (1 − Ln+1)vSn+1 and Ln+1vLn+1.
- Needed : vSn+1 and vLn+1.
How we compute vSn+1 if Ln+1 = 1 (resp. vLn+1 if Ln+1 = 0) ? Trick : use an implicit scheme, i. e. :
- 1. System of equations for B,D and E :
Y n+1 = Y n − δt (∇ · (Y vS))n + δt Γn+1
Y
.
- 3. System of equations for vS and vL (Φ = (M − ΓL)vL − MvS) :
(1 − Ln+1)vSn+1 = (1 − Ln)vSn − δt (∇ · ((1 − L)vS ⊗ vS))n − δt ((1 − L)∇P)n + δt (∇Σ)n+1 + δtΦn+1. Ln+1vLn+1 = LnvLn − δt (∇ · (LvL ⊗ vL) + L∇P)n − δtΦn+1.
SLIDE 32 Outline
- 1. What is a biofilm ?
- 2. Previous mathematical models for biofilms
- 3. A new multidimensional model for biofilms
- 4. Numerical scheme
- 5. Numerical results
- 6. Perspectives
SLIDE 33
One-dimensional case
SLIDE 34
One-dimensional case (2)
SLIDE 35
Two-dimensional case
Long-time behaviour. Evolution of B, E, L.
SLIDE 36
Two-dimensional case (2)
Short-time behaviour. Evolution of B.
SLIDE 37
Two-dimensional case (3)
Short-time behaviour. Evolution of B.
SLIDE 38
Two-dimensional case (4)
Short-time behaviour. Evolution of E.
SLIDE 39
Two-dimensional case (5)
Short-time behaviour. Evolution of B.
SLIDE 40 Outline
- 1. What is a biofilm ?
- 2. Previous mathematical models for biofilms
- 3. A new multidimensional model for biofilms
- 4. Numerical scheme
- 5. Numerical results
- 6. Perspectives
SLIDE 41
Perspectives
◮ Mathematical analysis of the model and of the numerical
scheme.
◮ Different conditions of temperature, humidity, light, nutrients
(CO2 and O2) etc...
◮ Confrontation with experiments of ICVBC (Istituto per la
Conservazione e la Valorizzazione dei Beni Culturali) of Firenze.
◮ Study of the influence of signalization. ◮ Coupling with chemical deterioration of monuments.
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