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a rapidly advancing liquid wedge breaks up, propagating a stationary vortical stripe on the liquid surface. the critical angular velocity for the transition of a wedge into a stripe is different in dilute and dense liquid. this is due to the different streaming conditions for the different fluids: in dilute solution, the vorticity is an additive property, and surface waves can still be excited. in dense solution, on the other hand, the vorticity is not additive, and due to the presence of density-dependent coupling to the basic flow, the film of the vorticity appears stationary. in a fluid of varying density, we see a dynamically-controlled transition of the vorticity stripe instability. we compare the fluid properties to the measured dynamics, and show that the film vorticity could indeed be used to predict the transition frequency in concentrated fluids.


we consider the interplay of two phenomena in liquids: long-range, 'c-structures', and confinement effects, which we attempt to link via the laplace surface tension. by means of molecular dynamics (md) simulations, we show that the two effects combine in a way which is reminiscent of the well-known third-body phenomenon. we perform md simulations of a mixture of hard-spheres and hard disks and observe the depletion of the number of c-structures and their relaxation into the liquid, as well as the increase of the film area. averaged over the simulations, the area of the film is indeed correlated with the number of c-structures. by combining md simulations with a continuum model, which treats the arrangement of the structures as a function of the reduced area, we show that this correlation can be described by an effective surface tension. 84d34552a1