Lowengrub John, Allard Jun, Aland Sebastian
Department of Mathematics, UC Irvine, Irvine, CA 92697, USA; Department of Biomedical Engineering, UC Irvine, Irvine, CA 92697, USA; Center for Complex Biological Systems, UC Irvine, CA 92697, USA.
Department of Mathematics, UC Irvine, Irvine, CA 92697, USA; Department of Physics and Astronomy, UC Irvine, Irvine, CA 92697, USA; Center for Complex Biological Systems, UC Irvine, CA 92697, USA.
J Comput Phys. 2016 Mar 15;309:112-128. doi: 10.1016/j.jcp.2015.12.055.
The formation of membrane vesicles from a larger membrane that occurs during endocytosis and other cell processes are typically orchestrated by curvature-inducing molecules attached to the membrane. Recent reports demonstrate that vesicles can form de novo in a few milliseconds. Membrane dynamics at these scales are strongly influenced by hydrodynamic interactions. To study this problem, we develop new diffuse interface models for the dynamics of inextensible vesicles in a viscous fluid with stiff, curvature-inducing molecules. The model couples the Navier-Stokes equations with membrane-induced bending forces that incorporate concentration-dependent bending stiffness coefficients and spontaneous curvatures, with equations for molecule transport and for a Lagrange multiplier to enforce local inextensibility. Two forms of surface transport equations are considered: Fickian surface diffusion and Cahn-Hilliard surface dynamics, with the former being more appropriate for small molecules and the latter being better for large molecules. The system is solved using adaptive finite element methods in 3D axisymmetric geometries. The results demonstrate that hydrodynamics can indeed enable the rapid formation of a small vesicle attached to the membrane by a narrow neck. When the Fickian model is used, this is a transient state with the steady state being a flat membrane with a uniformly distributed molecule concentration due to diffusion. When the Cahn-Hilliard model is used, molecule concentration gradients are sustained, the neck stabilizes and the system evolves to a steady-state with a small, compact vesicle attached to the membrane. By varying the membrane coverage of molecules in the Cahn-Hilliard model, we find that there is a critical (smallest) neck radius and a critical (fastest) budding time. These critical points are associated with changes in the vesicle morphology from spherical to mushroom-like as the molecule coverage on the membrane is increased.
在胞吞作用和其他细胞过程中,由较大膜形成膜泡通常是由附着在膜上的曲率诱导分子精心安排的。最近的报道表明,囊泡可以在几毫秒内从头形成。这些尺度下的膜动力学受到流体动力学相互作用的强烈影响。为了研究这个问题,我们针对粘性流体中具有刚性、曲率诱导分子的不可伸展囊泡的动力学,开发了新的扩散界面模型。该模型将纳维 - 斯托克斯方程与包含浓度依赖性弯曲刚度系数和自发曲率的膜诱导弯曲力耦合,同时还有分子传输方程和用于强制局部不可伸展性的拉格朗日乘子方程。考虑了两种形式的表面传输方程:菲克表面扩散和相场表面动力学,前者更适用于小分子,后者更适用于大分子。该系统在三维轴对称几何结构中使用自适应有限元方法求解。结果表明,流体动力学确实能够使通过狭窄颈部附着在膜上的小囊泡快速形成。当使用菲克模型时,这是一种瞬态,稳态是由于扩散而分子浓度均匀分布的平膜。当使用相场模型时,分子浓度梯度得以维持,颈部稳定,系统演化为附着在膜上的小而紧密的囊泡的稳态。通过改变相场模型中分子的膜覆盖率,我们发现存在一个临界(最小)颈部半径和一个临界(最快)出芽时间。随着膜上分子覆盖率的增加,这些临界点与囊泡形态从球形到蘑菇状的变化相关。