Wittmer Corinne R, Van Tassel Paul R
Department of Chemical Engineering, Yale University, P.O. Box 208286, New Haven, CT 06520-8286, USA.
Colloids Surf B Biointerfaces. 2005 Mar 25;41(2-3):103-9. doi: 10.1016/j.colsurfb.2004.10.030. Epub 2004 Dec 21.
Adsorbed protein layers are often away from equilibrium and thus exhibit history dependent structures. We use the kinetics of monoclonal antibody binding, as measured using optical waveguide lightmode spectroscopy (OWLS), to investigate the structure of adsorbed fibronectin (Fn) layers formed under different kinetic paths. For all of the layers investigated, we find no difference between the apparent adsorption rate constants of (i) monoclonal antibodies specific to Fn's cell binding site (alpha-Fn) and (ii) monoclonal antibodies specific to cytochrome c (alpha-CC, as a control), indicating initial adsorption of antibodies to be non-specific. For certain layers, the saturation density and the initial projected area per antibody differ significantly between alpha-Fn and alpha-CC, suggesting specific binding to follow the initial non-specific attachment. The fraction of antibodies binding specifically to the Fn layer, and the number of Fn binding sites per specific binding event, are estimated in terms of the difference in initial projected areas between alpha-Fn and alpha-CC. For a Fn layer formed at a bulk concentration of 2 microg/mL, we find a decrease in specific binding with an increase in Fn layer formation time, suggesting post-adsorption structural changes of a lower density adsorbed layer diminish binding site availability. Conversely, for a Fn layer formed at a bulk concentration of 40 microg/mL, we find an increase in specific binding with an increase in the aging time of the Fn layer, implying post-adsorption structural changes reveal binding sites for a higher density adsorbed layer.
吸附的蛋白质层通常处于非平衡状态,因此呈现出依赖于历史的结构。我们利用单克隆抗体结合动力学,通过光波导光模式光谱法(OWLS)进行测量,来研究在不同动力学路径下形成的吸附纤连蛋白(Fn)层的结构。对于所有研究的层,我们发现(i)针对Fn细胞结合位点的单克隆抗体(α-Fn)和(ii)针对细胞色素c的单克隆抗体(α-CC,作为对照)的表观吸附速率常数之间没有差异,这表明抗体的初始吸附是非特异性的。对于某些层,α-Fn和α-CC之间的饱和密度和每个抗体的初始投影面积存在显著差异,这表明特异性结合是在初始非特异性附着之后发生的。根据α-Fn和α-CC之间初始投影面积的差异,估计了特异性结合到Fn层的抗体比例以及每个特异性结合事件中Fn结合位点的数量。对于在本体浓度为2μg/mL下形成的Fn层,我们发现随着Fn层形成时间的增加,特异性结合减少,这表明较低密度吸附层的吸附后结构变化降低了结合位点的可用性。相反,对于在本体浓度为40μg/mL下形成的Fn层,我们发现随着Fn层老化时间的增加,特异性结合增加,这意味着吸附后结构变化揭示了较高密度吸附层的结合位点。