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Fluid-fluid pinch-off in presence of polymeric surface agents. Matthieu ROCHÉ (1), Hamid KELLAY CPMOH, Universite Bordeaux 1, France (1) Now at Complex fluids group MAE – Princeton University APS DFD Meeting November, 22 2009 Minneapolis. Motivation. Polymers inside. [1,2]. [3]. - PowerPoint PPT Presentation
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Fluid-fluid pinch-off in presence of polymeric surface agents
Matthieu ROCHÉ (1), Hamid KELLAYCPMOH, Universite Bordeaux 1, France
(1) Now at Complex fluids groupMAE – Princeton University
APS DFD Meeting November, 22 2009
Minneapolis
Motivation
What happens if polymers are added to the outer fluid?
Polymeric fluids in airA viscous fluid in another
viscous fluid
)()(min ttth c )(min )( ttceth
[1] J. R. Lister and H. A. Stone, Phys. Fluids 10, 2758-2764 (1998).[2] I. Cohen, M. P. Brenner, J. Eggers, and S. R. Nagel, Phys. Rev. Lett. 83, 1147 (1999).[3] Y. Amarouchene, D. Bonn, J. Meunier, and H. Kellay, Phys. Rev. Lett. 86, 3558-3561 (2001).
[1,2] [3]
Polymers inside
Main observationsWith polymers lying at the interface between the
fluids, we observe that:Polymers in the outer phase modify the shape of
the neckPolymers in the outer phase modify the thinning
dynamicsStructures analogous to those observed with bulk
polymeric fluids (polymers inside the fluid led to break-up) arise during the thinning
We can obtain a good measurement of the surface viscosity induced by the presence of polymers
Set-up
Black: continuous outer phase (aqueous solutions of surface agents)White: to-be-dispersed inner phase (5CB liquid crystal)
Polymers in the outer phase only
Polymers in the outer phase modify the shape of the neck
= tc-t, time away from singularitytc: pinch-off time
[SDS] = 0.1 CMCNo PVA
[SDS] = 0.1 CMC[PVA] = 1 wt%Average Mw = 105 Da
Similarities between our experiments and the pinch-off of bulk polymeric fluids
a: M. S. N. Oliveira and G. H. McKinley, Phys. Fluids 17, 71704 (2005). Polymers inside the neck
b: R. Sattler, C. Wagner, and J. Eggers, Phys. Rev. Lett. 100, 3-6 (2008). Polymers inside the neck
c: our experiment. Polymers outside the neck
= tc-t, time away from singularitytc: pinch-off time
Qout=2 mL/h
sd = 3.89 ms
Polymers in the outer phase modify the thinning dynamics
hmin
Comparison between the thinning slowdown for bulk polymeric fluids and the slow-down we
observed
Y. Amarouchene, D. Bonn, J. Meunier, and H. Kellay, Phys. Rev. Lett. 86, 3558-3561 (2001).
Exponential tendency
The slow down is well fitted by an exponential function
= tc-t, time away from singularitytc: pinch-off time
[SDS] = 0.1 CMC[PVA] = 1 wt%
Qout=2 mL/h
sd = 3.89 ms
Observations for a silicone oil in a PVA outer solution : purely viscous effect
~1140 s-1
Effect not related to the properties of the liquid crystal
Surface viscosity induced by polymers lying on the interface
s
s on the order of a few 10-6 to a few 10-5 kg/s
Good order of magnitude compared to values
reported in the literature
Deflate Inflate
5CB in a 1 wt% PVA solution
Conclusion
Surface effects induced by polymers in the outer phase of a liquid-liquid system led to break-up
Growing structures analogous to those observed with bulk polymeric fluids, where polymers are inside the liquid led to break-up
Thinning dynamics for the neck similar to those observed with bulk polymeric fluids
Good agreement with reported values for surface viscosity of polymers