Size dependence, stability, and a transition to buckling in model reverse bilayers

dc.creatorStecki, J.
dc.date2004-12-10
dc.date2006-07-03
dc.date.accessioned2026-07-07T06:37:24Z
dc.date.available2026-07-07T06:37:24Z
dc.descriptionMolecular Dynamics simulations of a model bilayer made of surfactant dimers in a Lennard-Jones solvent are reported for three sizes of the systems up to an area of $100σ\times 100σ$ and for a large interval of specific areas:from hole formation under tension to the floppy state of a compressed bilayer. The transition to the floppy state appears quite abrupt and discontinuous; in the floppy state the lateral tension is negative. Lateral tension and the structure factor were determined for all 3 sizes and all areas; the apparent rigidity constant and apparent surface tension are determined and correlated with the specific area and the finite size. The replacement of the $1/q^2$ capillary-wave divergence by a pole is accounted for and explained. The derivative of the lateral tension jumps from a high value in a flat bilayer to a low value in the floppy, rough, and buckling state, where the tension itself is negative.
dc.descriptionno18new.tex +no18new.ps + 11 figures *.ps; v2: improvements in the references
dc.identifierhttps://arxiv.org/abs/cond-mat/0412268
dc.identifierhttp://arxiv.org/abs/cond-mat/0412268
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/100380
dc.subjectSoft Condensed Matter
dc.titleSize dependence, stability, and a transition to buckling in model reverse bilayers
dc.typetext

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