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Applied Mathematics Colloquium


Friday, September 26, 11:30 am
Cullimore Lecture Hall II
New Jersey Institute of Technology

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Domain Evolution and Relaxation in Langmuir Films

 

Andrew Bernoff

Department of Mathematics

Harvey Mudd College

Claremont, CA

 

 

 

 

 

Abstract

 


We report on an experimental and theoretical study of Langmuir layers, defined as a molecularly thin polymer layer on the surface of a

subfluid. Langmuir layers can have multiple phases (e.g. fluid, gas, liquid crystal, isotropic or anisotropic solid); at phase

boundaries a line tension force is observed.  We first consider two co-existing fluid phases; specifically a localized phase embedded

in an infinite secondary phase. When the localized phase is stretched (by a transient stagnation flow), it takes the form of a bola

consisting of two roughly circular reservoirs connected by a thin tether. This shape then relaxes to the minimum energy configuration

of a circular domain. The tether is never observed to rupture, even when it is more than a hundred times as long as it is thin. We

model these experiments by taking previous descriptions of the full hydrodynamics (primarily those of Stone & McConnell and Lubensky &

Goldstein), identifying the dominant effects via dimensional analysis, and reducing the system to a more tractable form. The result is

a free boundary problem where motion is driven by the line tension of the domain and damped by the viscosity of the subfluid. The

problem has a boundary integral formulation which allows us to numerically simulate the tether relaxation; comparison with the

experiments allows us to estimate the line tension in the system, often to within 1%.  As time allows we will also report on some other

phenomena observed in Langmuir systems, including collapse of gas phase bubbles, creation of foams, co-existence of three or more fluid

phases, elastic buckling of surface layers, and formation of dogbone and labyrinth patterns due to dipolar repulsion in the layer.