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迈向囊泡相场模型的热力学一致图景:曲率能。

Toward a thermodynamically consistent picture of the phase-field model of vesicles: curvature energy.

作者信息

Jamet D, Misbah C

机构信息

DEN/DER/SSTH/LMDL, CEA-Grenoble, 17 rue des Martyrs, 38054 Grenoble Cedex 9, France.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Sep;78(3 Pt 1):031902. doi: 10.1103/PhysRevE.78.031902. Epub 2008 Sep 3.

Abstract

We extend our recent work on phase-field model for vesicles [D. Jamet and C. Misbah, Phys. Rev. E 76, 051907 (2007)]-where only the membrane local incompressibility was treated-to the situation where the bending forces and spontaneous curvature are included. We show how the general phase-field equations can be derived within a thermodynamic consistent picture. We analyze a general form of the bending energy, where the Helfrich bending force is treated as a special case. The dynamical evolution equation derived here for the velocity field allows one to write down a constitutive law of the composite fluid: The ambient fluid plus the membrane. This constitutive law has a viscoelastic form, the viscous part arises from the fluid, while the elastic one represents the action of the membrane. It is shown that the elastic stress tensor is not symmetric, owing to bending torque, inherent to a diffuse membrane model.

摘要

我们将近期关于囊泡相场模型的工作[D. 雅梅特和C. 米斯巴,《物理评论E》76,051907 (2007)]——其中仅考虑了膜的局部不可压缩性——扩展到包含弯曲力和自发曲率的情形。我们展示了如何在热力学自洽的框架内推导一般的相场方程。我们分析了弯曲能的一般形式,其中赫尔弗里希弯曲力被视为一种特殊情况。这里导出的速度场动力学演化方程使我们能够写出复合流体(环境流体加膜)的本构定律。该本构定律具有粘弹性形式,粘性部分源于流体,而弹性部分代表膜的作用。结果表明,由于扩散膜模型固有的弯曲扭矩,弹性应力张量不对称。

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