Fractional hereditariness of lipid membranes: Instabilities and linearized evolution

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• 作者：L. Deseri^a ; ^b ; ^c ; ^d ; ^e ; ^{deseri@andrew.cmu.edu" class="auth_mail" title="E-mail the corresponding author} ; P. Pollaci^b ; ^{pietro.pollaci@unitn.it" class="auth_mail" title="E-mail the corresponding author} ; M. Zingales^f ; ^g ; ^{massimiliano.zingales@unipa.it" class="auth_mail" title="E-mail the corresponding author} ; K. Dayal^d ; ^{kaushik@cmu.edu" class="auth_mail" title="E-mail the corresponding author}
• 关键词：Fractional hereditary lipid membranes ; Viscoelastic lipid membranes ; Phase transitions ; Material instabilities
• 刊名：Journal of the Mechanical Behavior of Biomedical Materials
• 出版年：2016
• 出版时间：May 2016
• 年：2016
• 卷：58
• 期：Complete
• 页码：11-27
• 全文大小：1479 K

文摘

In this work lipid ordering phase changes arising in planar membrane bilayers is investigated both accounting for elasticity alone and for effective viscoelastic response of such assemblies. The mechanical response of such membranes is studied by minimizing the Gibbs free energy which penalizes perturbations of the changes of areal stretch and their gradients only (Deseri and Zurlo, 2013). As material instabilities arise whenever areal stretches characterizing homogeneous configurations lie inside the spinoidal zone of the free energy density, bifurcations from such configurations are shown to occur as oscillatory perturbations of the in-plane displacement. Experimental observations (Espinosa et al., 2011) show a power-law in-plane viscous behavior of lipid structures allowing for an effective viscoelastic behavior of lipid membranes, which falls in the framework of Fractional Hereditariness. A suitable generalization of the variational principle invoked for the elasticity is applied in this case, and the corresponding Euler–Lagrange equation is found together with a set of boundary and initial conditions. Separation of variables allows for showing how Fractional Hereditariness owes bifurcated modes with a larger number of spatial oscillations than the corresponding elastic analog. Indeed, the available range of areal stresses for material instabilities is found to increase with respect to the purely elastic case. Nevertheless, the time evolution of the perturbations solving the Euler–Lagrange equation above exhibits time-decay and the large number of spatial oscillation slowly relaxes, thereby keeping the features of a long-tail type time-response.