Adhesion dynamics of confined membranes
Autor: | Olivier Pierre-Louis, Thomas Le Goff, Tung B.T. To |
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Přispěvatelé: | Institut de Biologie du Développement de Marseille (IBDM), Aix Marseille Université (AMU)-Collège de France (CdF (institution))-Centre National de la Recherche Scientifique (CNRS), Institut Lumière Matière [Villeurbanne] (ILM), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS) |
Jazyk: | angličtina |
Rok vydání: | 2018 |
Předmět: |
0301 basic medicine
Materials science Tension (physics) [SDV]Life Sciences [q-bio] FOS: Physical sciences Flexural rigidity General Chemistry Adhesion Mechanics Condensed Matter - Soft Condensed Matter Condensed Matter Physics 01 natural sciences Quantitative Biology::Subcellular Processes 03 medical and health sciences 030104 developmental biology Domain wall (magnetism) Membrane Phase (matter) 0103 physical sciences Lubrication Soft Condensed Matter (cond-mat.soft) 010306 general physics Nonlinear Sciences::Pattern Formation and Solitons ComputingMilieux_MISCELLANEOUS Linear stability |
Zdroj: | Soft Matter Soft Matter, 2018, 14 (42), pp.8552-8569. ⟨10.1039/c8sm01567h⟩ Soft Matter, Royal Society of Chemistry, 2018, 14 (42), pp.8552-8569. ⟨10.1039/c8sm01567h⟩ |
ISSN: | 1744-683X 1744-6848 |
DOI: | 10.1039/c8sm01567h⟩ |
Popis: | We report on the modeling of the dynamics of confined lipid membranes. We derive a thin film model in the lubrication limit which describes an inextensible liquid membrane with bending rigidity confined between two adhesive walls. The resulting equations share similarities with the Swift–Hohenberg model. However, inextensibility is enforced by a time-dependent nonlocal tension. Depending on the excess membrane area available in the system, three different dynamical regimes, denoted as A, B and C, are found from the numerical solution of the model. In regime A, membranes with small excess area form flat adhesion domains and freeze. Such freezing is interpreted by means of an effective model for curvature-driven domain wall motion. The nonlocal membrane tension tends to a negative value corresponding to the linear stability threshold of flat domain walls in the Swift–Hohenberg equation. In regime B, membranes with intermediate excess areas exhibit endless coarsening with coexistence of flat adhesion domains and wrinkle domains. The tension tends to the nonlinear stability threshold of flat domain walls in the Swift–Hohenberg equation. The fraction of the system covered by the wrinkle phase increases linearly with the excess area in regime B. In regime C, membranes with large excess area are completely covered by a frozen labyrinthine pattern of wrinkles. As the excess area is increased, the tension increases and the wavelength of the wrinkles decreases. For large membrane area, there is a crossover to a regime where the extrema of the wrinkles are in contact with the walls. In all regimes after an initial transient, robust localised structures form, leading to an exact conservation of the number of adhesion domains. |
Databáze: | OpenAIRE |
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