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Convective Instability in quasi 2D foams Eric Janiaud, Stefan Hutzler, Denis Weaire. Trinity College, Dublin

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Presentation on theme: "Convective Instability in quasi 2D foams Eric Janiaud, Stefan Hutzler, Denis Weaire. Trinity College, Dublin"— Presentation transcript:

1 Convective Instability in quasi 2D foams Eric Janiaud, Stefan Hutzler, Denis Weaire. Trinity College, Dublin janiaude@tcd.ie

2 Convection in (3d) foams  Add liquid on top of a foam :  if Q> Threshold: plastic flow of bubbles.  Add liquid on top of a foam :  if Q> Threshold: plastic flow of bubbles. L. Alonso

3 Analogy with Thermal convection Driving force: Damping:     + d  Gravity thought density variation Viscosity: energy dissipated in T1 Capillary diffusion: reduces density variation Plastic yield stress: capillary stress balances non uniform hydrostatic pressure    + d  Gravity thought density variation

4 Difference with Thermal convection Heat diffusion Gaussian continuous media Newtonian liquid Heat diffusion Gaussian continuous media Newtonian liquid Liquid diffusion non linear (chemistry) Discrete network Yield stress+dilatency Liquid diffusion non linear (chemistry) Discrete network Yield stress+dilatency Ra = F Archimede / F viscosity Nu = Q convection /Q no convection Pr = D mvt / D heat Pe = T diffusion / T convection ?

5 Issues Mix Rheology and drainage Onset: dilatency, surfactants, bubble size,  gradient... After the onset : Shear bands, efficiency on liquid transport, size sorting... Mix Rheology and drainage Onset: dilatency, surfactants, bubble size,  gradient... After the onset : Shear bands, efficiency on liquid transport, size sorting...

6 From 3D to 2D...  Decoration theorem:  Quasi 2D in a Hele-Shaw : Film Vertex “decorated” Pseudo Plateau Border No liquid flow between vertex Drainage is possible !

7 Quasi 2D foams in Hele-Shaw cell

8 What is the Volume fraction?  Wetting Plateau border V~R 2 L  Film V~L 2 e  “Perpendicular” Plateau border V~R 2 d  Vertices V~R 3  Wetting Plateau border V~R 2 L  Film V~L 2 e  “Perpendicular” Plateau border V~R 2 d  Vertices V~R 3 Needs experiments and Evolver Simulations Cox

9 Hele-Shaw Cell setup  Sensitive to the wetting film  Bidisperse foam Area ~90 and 130 pixel  Sensitive to the wetting film  Bidisperse foam Area ~90 and 130 pixel Projector Q

10 Steady state Drainage  Injection point  Uniform: free convection  Local: forced convection  Injection point  Uniform: free convection  Local: forced convection Q Q What is the solution to the drainage equation? What is the caracteristic length for roll?

11 Local injection Q

12 Vertical Velocity Velocity (pi/s) Horizontal coordinate (pi) 3 pictures Smooth profile = No shear Band

13 Non uniform liquid Fraction How to measure the volume fraction?

14 Image Analysis : Vertices Velocity: tracking bubbles T1: neighbourhood relations Local Volume fraction: ration of Pixel Stress/Strain field: Vertex position Capillary pressure curvature measurement

15 Plugin for ImageJ  Public/free Java software developed by the NIH  Object oriented easy implementation  Already rich  Multiplatform  Public/free Java software developed by the NIH  Object oriented easy implementation  Already rich  Multiplatform

16 Perspectives  Forced 2D convection impose and measure  measure the velocity field  Free 2D convection homogenous liquid input !!! boundary conditions !!! destabilisation length?  Back to 3D convection  Forced 2D convection impose and measure  measure the velocity field  Free 2D convection homogenous liquid input !!! boundary conditions !!! destabilisation length?  Back to 3D convection


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