Surface relaxation of lyotropic lamellar phases

dc.creatorBary-Soroker, H.
dc.creatorDiamant, H.
dc.date2005-07-19
dc.date2006-03-05
dc.date.accessioned2026-07-07T06:41:23Z
dc.date.available2026-07-07T06:41:23Z
dc.descriptionWe study the relaxation modes of an interface between a lyotropic lamellar phase and a gas or a simple liquid. The response is found to be qualitatively different from those of both simple liquids and single-component smectic-A liquid crystals. At low rates it is governed by a non-inertial, diffusive mode whose decay rate increases quadratically with wavenumber, $|ω|=Aq^2$. The coefficient $A$ depends on the restoring forces of surface tension, compressibility and bending, while the dissipation is dominated by the so-called slip mechanism, i.e, relative motion of the two components of the phase parallel to the lamellae. This surface mode has a large penetration depth which, for sterically stabilised phases, is of order $(dq^2)^{-1}$, where $d$ is the microscopic lamellar spacing.
dc.description7 pages, 1 figure
dc.identifierhttps://arxiv.org/abs/cond-mat/0507447
dc.identifierhttp://arxiv.org/abs/cond-mat/0507447
dc.identifierEurophys. Lett. 73, 871 (2006)
dc.identifierdoi:10.1209/epl/i2005-10476-4
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/101649
dc.subjectSoft Condensed Matter
dc.subjectFluid Dynamics
dc.titleSurface relaxation of lyotropic lamellar phases
dc.typetext

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