Xu Hai, Zhao Xiubo, Grant Colin, Lu Jian R, Williams David E, Penfold Jeff
Biological Physics Group, School of Physics and Astronomy, University of Manchester, Manchester M60 1QD, UK.
Langmuir. 2006 Jul 4;22(14):6313-20. doi: 10.1021/la0532454.
Conformational orientations of a mouse monoclonal antibody to the beta unit of human chorionic gonadotrophin (anti-beta-hCG) at the hydrophilic silicon oxide/water interface were investigated using atomic force microscopy (AFM) and neutron reflectivity (NR). The surface structural characterization was conducted with the antibody concentration in solution ranging from 2 to 50 mg.L(-1) with the ionic strength kept at 20 mM and pH = 7.0. It was found that the antibody adopted a predominantly "flat-on" orientation, with the Fc and two Fab fragments lying flat on the surface. The AFM measurement revealed a thickness of 30-33 A of the layer formed in contact with 2 mg.L(-1) antibody in water, but, interestingly, the flat-on antibody molecules formed small nonuniform clusters equivalent to 2-15 antibody molecules. Parallel AFM scanning in air revealed even larger surface clusters, suggesting that surface drying induced further aggregation. The AFM study thus demonstrated that the interaction between protein and the hydrophilic surface is weak and indicated that surface aggregation can be driven by the attraction between neighboring protein molecules. NR measurements at the solid/water interface confirmed the flat-on layer orientation of adsorbed molecules over the entire concentration range studied. Thus, at 2 mg.L(-1), the adsorbed antibody layer was well represented by a uniform layer with a thickness of 40 A. This value is thicker than the 30-33 A observed from AFM, suggesting possible layer compression caused by the tip tapping. An increase in the antibody concentration to 10 mg.L(-1) led to increasing surface adsorption. The corresponding layer structure was well represented by a three-layer model consisting of an inner sublayer of 10 A, a middle sublayer of 30 A, and an outer sublayer of 25 A, with the protein volume fractions in each sublayer being 0.22, 0.42, and 0.10, respectively. The structural transition can be interpreted as a twisting and tilting of segments of the adsorbed molecules, driven by an electrostatic repulsion between them that increases with the surface packing density. Hindrance of antigen access to antibody binding sites, resulting from the change in surface packing, can account for the decrease in antigen binding capacity (AgBC) with increasing surface density of the antibody that is observed.
利用原子力显微镜(AFM)和中子反射率(NR)研究了小鼠单克隆抗体与人绒毛膜促性腺激素β亚基(抗β-hCG)在亲水性氧化硅/水界面的构象取向。在溶液中抗体浓度为2至50 mg·L⁻¹、离子强度保持在20 mM且pH = 7.0的条件下进行了表面结构表征。发现抗体主要采取“平躺”取向,Fc和两个Fab片段平躺在表面。AFM测量显示,在水中与2 mg·L⁻¹抗体接触形成的层厚度为30 - 33 Å,但有趣的是,平躺的抗体分子形成了相当于2 - 15个抗体分子的小的不均匀聚集体。在空气中进行的平行AFM扫描显示出更大的表面聚集体,表明表面干燥诱导了进一步聚集增加。因此,AFM研究表明蛋白质与亲水性表面之间的相互作用较弱,并表明表面聚集可由相邻蛋白质分子之间的吸引力驱动。在固体/水界面进行的NR测量证实了在所研究的整个浓度范围内吸附分子的平躺层取向。因此,在2 mg·L⁻¹时,吸附的抗体层可用厚度为40 Å的均匀层很好地表示。该值比从AFM观察到的30 - 33 Å厚,表明可能是由针尖轻敲引起的层压缩。抗体浓度增加到10 mg·L⁻¹导致表面吸附增加。相应的层结构可用三层模型很好地表示,该模型由一个10 Å的内子层、一个30 Å的中子层和一个25 Å的外子层组成,每个子层中的蛋白质体积分数分别为0.22、0.42和0.10。这种结构转变可以解释为吸附分子片段的扭曲和倾斜,这是由它们之间的静电排斥驱动的,这种排斥随着表面堆积密度的增加而增加。表面堆积的变化导致抗原进入抗体结合位点受阻,可以解释所观察到的随着抗体表面密度增加抗原结合能力(AgBC)的下降。