Department of Biomedical Engineering, University of California, Davis, One Shields Avenue, Davis, CA 95616, USA.
Ann Biomed Eng. 2011 Jan;39(1):427-42. doi: 10.1007/s10439-010-0143-y. Epub 2010 Sep 2.
Studies of receptor diffusion on a cell surface show a variety of behaviors, such as diffusive, sub-diffusive, or super-diffusive motion. However, most studies to date focus on receptor molecules diffusing on a single cell surface. We have previously studied receptor diffusion to probe the molecular mechanism of receptor clustering at the cell-cell junction between two opposing cell surfaces. Here, we characterize the diffusion of receptors and ligands that bind to each other across two opposing cell surfaces, as in cell-cell and cell-bilayer interactions. We use a Monte Carlo method, where receptors and ligands are simulated as independent agents that bind and diffuse probabilistically. We vary receptor-ligand binding affinity and plot the molecule-averaged mean square displacement (MSD) of ligand molecules as a function of time. Our results show that MSD plots are qualitatively different for flat and curved interfaces, as well as between the cases of presence and absence of directed transport of receptor-ligand complexes toward a specific location on the interface. Receptor-ligand binding across two opposing surfaces leads to transient sub-diffusive motion at early times provided the interface is flat. This effect is entirely absent if the interface is curved, however, in this instance we observe sub-diffusive motion. In addition, a decrease in the equilibrium value of the MSD occurs as affinity increases, something which is absent for a flat interface. In the presence of directed transport of receptor-ligand complexes, we observe super-diffusive motion at early times for a flat interface. Super-diffusive motion is absent for a curved interface, however, in this case we observe a transient decrease in MSD with time prior to equilibration for high-affinity values.
研究表明,细胞表面上的受体扩散表现出多种行为,如扩散、亚扩散或超扩散运动。然而,迄今为止的大多数研究都集中在单个细胞表面上扩散的受体分子上。我们之前研究了受体扩散,以探究细胞-细胞连接两个相对细胞表面上受体聚类的分子机制。在这里,我们描述了跨两个相对细胞表面结合并扩散的受体和配体的扩散,如细胞-细胞和细胞双层相互作用。我们使用蒙特卡罗方法,其中将受体和配体模拟为独立的、概率结合和扩散的代理。我们改变了受体-配体结合亲和力,并绘制了配体分子的平均均方位移(MSD)随时间的函数图。我们的结果表明,对于平面和曲面界面以及存在和不存在受体-配体复合物向界面上特定位置的定向运输的情况,MSD 图的定性不同。跨两个相对表面的受体-配体结合在早期导致瞬态亚扩散运动,前提是界面是平的。然而,如果界面是弯曲的,这种效果完全不存在,但是在这种情况下,我们观察到亚扩散运动。此外,随着亲和力的增加,平衡时 MSD 值会降低,而在平面界面上则不存在这种情况。在受体-配体复合物的定向运输存在的情况下,我们观察到平面界面上的早期超扩散运动。然而,对于弯曲的界面,超扩散运动不存在,但是在这种情况下,我们观察到高亲和力值时,MSD 随时间的瞬态降低,然后达到平衡。