Department of Physics and Astronomy, University of North Carolina, Chapel Hill, North Carolina, USA.
Biophys J. 2009 Nov 18;97(10):2820-8. doi: 10.1016/j.bpj.2009.08.042.
Fibrin, the structural scaffold of blood clots, spontaneously polymerizes through the formation of 'A-a' knob-hole bonds. When subjected to external force, the dissociation of this bond is accompanied by two to four abrupt changes in molecular dimension observable as rupture events in a force curve. Herein, the configuration, molecular extension, and kinetic parameters of each rupture event are examined. The increases in contour length indicate that the D region of fibrinogen can lengthen by approximately 50% of the length of a fibrin monomer before rupture of the 'A-a' interaction. The dependence of the dissociation rate on applied force was obtained using probability distributions of rupture forces collected at different pull-off velocities. These distributions were fit using a model in which the effects of the shape of the binding potential are used to quantify the kinetic parameters of forced dissociation. We found that the weak initial rupture (i.e., event 1) was not well approximated by these models. The ruptured bonds comprising the strongest ruptures, events 2 and 3, had kinetic parameters similar to those commonly found for the mechanical unfolding of globular proteins. The bonds ruptured in event 4 were well described by these analyses, but were more loosely bound than the bonds in events 2 and 3. We propose that the first event represents the rupture of an unknown interaction parallel to the 'A-a' bond, events 2 and 3 represent unfolding of structures in the D region of fibrinogen, and event 4 is the rupture of the 'A-a' knob-hole bond weakened by prior structural unfolding. Comparison of the activation energy obtained via force spectroscopy measurements with the thermodynamic free energy of 'A-a' bond dissociation indicates that the 'A-a' bond may be more resistant to rupture by applied force than to rupture by thermal dissociation.
纤维蛋白是血栓的结构支架,可通过“A-a”扣环键的形成自发聚合。当受到外力时,这种键的解离伴随着分子尺寸的两到四个突然变化,可在力曲线中观察到作为断裂事件。在此,检查了每个断裂事件的构型、分子延伸和动力学参数。轮廓长度的增加表明,纤维蛋白原的 D 区在“A-a”相互作用断裂之前可以延长大约纤维蛋白单体长度的 50%。通过在不同的拉开速度下收集断裂力的概率分布,获得了解离速率对施加力的依赖性。使用这些分布拟合模型,该模型利用结合势的形状来量化强制解离的动力学参数。我们发现,这些模型不能很好地近似初始弱断裂(即事件 1)。由最强断裂(即事件 2 和 3)组成的断裂键具有与通常在球形蛋白的机械展开中发现的相似的动力学参数。这些分析很好地描述了事件 4 中发生的断裂键,但比事件 2 和 3 中的断裂键结合得更松。我们提出,第一个事件代表与“A-a”键平行的未知相互作用的断裂,事件 2 和 3 代表纤维蛋白原的 D 区结构的展开,事件 4 是“A-a”扣环键的断裂,该键的断裂是由先前的结构展开而减弱的。通过力谱测量获得的活化能与“A-a”键解离的热力学自由能进行比较表明,与热解离相比,“A-a”键可能更能抵抗施加力的断裂。