During blood vessel injury, fibrinogen is converted to fibrin, a polymer that serves as the structural scaffold of a blood clot. The primary function of fibrin is to withstand the large shear forces in blood and provide mechanical stability to the clot, protecting the wound. Understanding the biophysical forces involved in maintaining fibrin structure is of great interest to the biomedical community. Previous reports have identified the "A-a" knob-hole interaction as the dominant force responsible for fibrin's structural integrity. Herein, biochemical force spectroscopy is used to study knob-hole interactions between fibrin fragments and variant fibrinogen molecules to identify the forces occurring between individual fibrin molecules. The rupture of the "A-a" knob-hole interaction results in a characteristic profile previously unreported in fibrin force spectroscopy with two distinct populations of specific forces: 110 +/- 34 and 224 +/- 31 pN. In the absence of a functional "A" knob or hole "a", these forces cease to exist. We propose that the characteristic pattern represents the deformation of the D region of fibrinogen prior to the rupture of the "A-a" knob-hole bond.
A method is described that takes advantage of the intermittency ("blinking") in the fluorescence of quantum dots (QDs) to measure absolute positions of closely spaced QDs. The concept is that even if two QDs are separated by only tens of nanometers, the position of each QD is resolvable if the point spread function of each can be imaged independently of the other. In the case of QDs, this is possible if each QD separately blinks completely on and off during a time-lapse sequence. To demonstrate the principle of this method, time-lapse sequences of single blinking QDs were acquired and the centroids of the point spread functions determined. Images of the blinking QDs were then overlapped in software, pixel by pixel, generating a range of submicroscopic distances between QD pairs. Methods were developed for analyzing the overlapped time sequences of the QD pairs so that the positions of the QDs and the distances between them could be determined without prior knowledge of the single QD positions. We subsequently used this method to measure the end-to-end length of a 122-basepair double-stranded DNA fragment.
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.
Since its invention in 1986 by Binnig, Quate, and Gerber, the atomic force microscope (AFM) has proven to be an extremely useful tool for examining the interactions of proteins with surfaces. Fibrinogen in particular has been used as a model protein to demonstrate new methodologies for studying protein behavior with AFM due to its unique size, shape, and function. Indeed, fibrinogen's central role in both blood coagulation and blood-based infections has made it the primary protein used to interrogate the biocompatibility of surfaces. The goal of this review is to provide an analytical perspective on the utility of AFM for investigating the interaction of fibrinogen with surfaces.
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