J. Haber Institute of Catalysis and Surface Chemistry, Polish Academy of Sciences, 30-239 Kraków, Niezapominajek 8, Poland.
Langmuir. 2011 Jun 7;27(11):6868-78. doi: 10.1021/la200798d. Epub 2011 May 5.
Adsorption of fibrinogen, modeled as a linear chain of touching beads of various sizes, was theoretically studied using the random sequential adsorption (RSA) model. The adsorption process was assumed to consist of two steps: (i) formation of an irreversibly bound fibrinogen monolayer under the side-on orientation, which is independent of the bulk protein concentration and (ii) formation of the reversibly bound, end-on monolayer, whose coverage was dependent on the bulk concentration. Calculation based on the RSA model showed that the maximum surface concentration of the end-on (reversible) monolayer equals N(⊥∞) = 6.13 × 10(3) μm(-2) which is much larger than the previously found value for the side-on (irreversible) monolayer, equal to N(∞) = 2.27 × 10(3) μm(-2). Hence, the maximum surface concentration of fibrinogen in both orientations is determined to be 8.40 × 10(3) μm(-2) corresponding to the protein coverage of 5.70 mg m(-2) assuming 20% hydration. Additionally, the surface blocking function (ASF) was determined for the end-on fibrinogen adsorption, approximated for the entire range of coverage by the interpolating polynomial. For the coverage approaching the jamming limit, the surface blocking function (ASF) was shown to vanish proportionally to (θ(⊥∞) - θ(⊥))(2). These calculation allowed one to theoretically predict adsorption isotherms for the end-on regime of fibrinogen and adsorption kinetics under various transport conditions (diffusion and convection). Using these theoretical results, a quantitative interpretation of experimental data obtained by TIRF and ellipsometry was successfully performed. The equilibrium adsorption constant for the end-on adsorption regime was found to be 8.04 × 10(-3) m. On the basis of this value, the depth of the adsorption energy minimum, equal to -17.4 kT, was predicted, which corresponds to ΔG = -41.8 kJ mol(-1). This is in accordance with adsorption energy derived as the sum of the van der Waals and electrostatic interactions. Besides having significance for predicting fibrinogen adsorption, theoretical results derived in this work also have implications for basic science providing information on mechanisms of anisotropic protein molecule adsorption on heterogeneous surfaces.
纤维蛋白原被模拟为一系列不同大小的点状链,采用随机顺序吸附(RSA)模型对其吸附过程进行了理论研究。该吸附过程被假设由两个步骤组成:(i)在侧向上形成不可逆结合的纤维蛋白原单层,其与本体蛋白浓度无关;(ii)形成可还原结合的、端到端的单层,其覆盖率取决于本体浓度。基于 RSA 模型的计算表明,端到端(可还原)单层的最大表面浓度等于 N(⊥∞) = 6.13 × 10(3) μm(-2),这远大于之前在侧向上(不可逆)单层中发现的 N(∞) = 2.27 × 10(3) μm(-2)的值。因此,在两种取向中,纤维蛋白原的最大表面浓度被确定为 8.40 × 10(3) μm(-2),对应于蛋白质覆盖率为 5.70 mg m(-2),假设 20%水合。此外,还确定了端到端纤维蛋白原吸附的表面阻塞函数(ASF),该函数在整个覆盖率范围内由插值多项式近似。对于接近阻塞极限的覆盖率,ASF 被证明与(θ(⊥∞) - θ(⊥))(2)成比例消失。这些计算允许从理论上预测端到端纤维蛋白原的吸附等温线和各种传输条件(扩散和对流)下的吸附动力学。使用这些理论结果,成功地对通过 TIRF 和椭偏仪获得的实验数据进行了定量解释。发现端到端吸附态的平衡吸附常数为 8.04 × 10(-3) m。基于该值,预测了吸附能最小值的深度,等于-17.4 kT,这对应于 ΔG = -41.8 kJ mol(-1)。这与从范德华和静电相互作用之和得出的吸附能一致。除了对预测纤维蛋白原吸附具有重要意义外,本文的理论结果还为基础科学提供了有关各向异性蛋白质分子在异质表面上吸附机制的信息。