Department of Biochemical Engineering, School of Chemical Engineering and Technology, Tianjin University, Tianjin 300072, China.
J Phys Chem B. 2010 Feb 18;114(6):2203-11. doi: 10.1021/jp903852c.
High ligand density is usually required in hydrophobic charge induction chromatography (HCIC) for high adsorption capacity. However, it is not clear to what extent the ligand density alters the adsorption and desorption behaviors, or if this leads to the protein conformational transition within adsorbent pores. In the present study, molecular dynamics simulation is performed to examine the effects of ligand density in HCIC using a 46-bead beta-barrel coarse-grained model protein and a coarse-grained adsorbent pore model established in our earlier work. Four ligand densities (1.474, 1.769, 2.212, and 2.949 micromol/m(2)) are simulated at 298.15 K. The simulations indicate that both the capacity and irreversibility of adsorption increase with ligand density. However, it is found that the fastest adsorption occurs at a ligand density of 2.212 micromol/m(2) rather than at the highest density studied. Analyses of adsorption trajectories, protein-ligand interaction energy, and the free energy map indicate that there is repulsion of protein when unfavorable contacts of the protein and ligands occur. There is an enhanced repulsion at 2.949 micromol/m(2), which increases the energy barrier to the transition region and reduces the opportunities to get stable adsorption, thus leading to the decreased adsorption rate. At 2.212 micromol/m(2), however, the repulsion is mild and the high ligand coverage provides abundant opportunities for the protein to get the fastest adsorption and thus causes the maximum unfolding. In the following simulations, complete and irreversible desorption is observed at all ligand densities, in agreement with the easy pH-induced elution behavior of HCIC observed experimentally. It is found that there is a suitable balance between hydrophobic attraction and electrostatic repulsion at 2.212 micromol/m(2), which leads to the slowest desorption kinetics and causes the maximum unfolding. Moreover, analysis of unfolded protein distribution indicates that unfolding occurs mainly on the ligand surface in both adsorption and desorption. The behaviors have been comprehensively elucidated by molecular and thermodynamic analyses.
高配体密度通常是疏水性电荷诱导层析(HCIC)实现高吸附容量所必需的。然而,配体密度如何改变吸附和解吸行为,或者是否导致蛋白质在吸附剂孔内构象转变,目前还不清楚。本研究采用 46 个珠β-桶粗粒化模型蛋白和我们早期工作中建立的粗粒化吸附剂孔模型,通过分子动力学模拟考察 HCIC 中配体密度的影响。在 298.15 K 下模拟了四种配体密度(1.474、1.769、2.212 和 2.949 µm ol/m²)。模拟结果表明,吸附容量和不可逆性随配体密度的增加而增加。然而,发现最快的吸附发生在配体密度为 2.212 µm ol/m²,而不是在所研究的最高密度处。吸附轨迹、蛋白-配体相互作用能和自由能图谱的分析表明,当蛋白和配体发生不利接触时,蛋白会受到排斥。在 2.949 µm ol/m²时排斥作用增强,增加了过渡区的能量势垒,减少了获得稳定吸附的机会,从而降低了吸附速率。然而,在 2.212 µm ol/m²时,排斥作用较弱,高配体覆盖率为蛋白提供了丰富的机会获得最快的吸附,从而导致最大的展开。在随后的模拟中,在所有配体密度下都观察到完全和不可逆的解吸,这与 HCIC 实验中观察到的易 pH 诱导洗脱行为一致。研究发现,在 2.212 µm ol/m²时,疏水性吸引和静电排斥之间存在适当的平衡,导致最慢的解吸动力学,并导致最大的展开。此外,展开蛋白分布的分析表明,在吸附和解吸过程中,展开主要发生在配体表面。通过分子和热力学分析对这些行为进行了全面阐述。