The NTA-His6 bond is strong enough for AFM single-molecular recognition studies

There is a need in current atomic force microscopy (AFM) molecular recognition studies for generic methods for the stable, functional attachment of proteins on tips and solid supports. In the last few years, the site-directed nitrilotriacetic acid (NTA)-polyhistidine (Hisn) system has been increasingly used towards this goal. Yet, a crucial question in this context is whether the NTA-Hisn bond is sufficiently strong for ensuring stable protein immobilization during force spectroscopy measurements. Here, we measured the forces between AFM tips modified with NTA-terminated alkanethiols and solid supports functionalized with His6-Gly-Cys peptides in the presence of Ni2+. The force histogram obtained at a loading rate of 6600 pN s(-1) showed three maxima at rupture forces of 153 +/- 57 pN, 316 +/- 50 pN and 468 +/- 44 pN, that we attribute primarily to monovalent and multivalent interactions between a single His6 moiety and one, two and three NTA groups, respectively. The measured forces are well above the 50-100 pN unbinding forces typically observed by AFM for receptor-ligand pairs. The plot of adhesion force versus log (loading rate) revealed a linear regime, from which we deduced a kinetic off-rate constant of dissociation, k(off) approximately 0.07 s(-1). This value is in the range of that estimated for the multivalent interaction involving two NTA, using fluorescence measurements, and may account for an increased binding stability of the NTA-His6 bond. We conclude that the NTA-His6 system is a powerful, well-suited platform for the stable, oriented immobilization of proteins in AFM single-molecule studies.     

Specific molecular interactions by force spectroscopy: from single bonds to collective properties

Interactions involving multiple bonds occur throughout biology, and have distinct properties that are fundamentally different from those present in single bond systems. We have developed a new method to analyse the AFM force measurements in order to extract relevant information and to characterise the interactions involving from single to multiple bonds. Our study reveals a surprising behaviour in the presence of multiple bonds with a high rebinding probability: the mean binding forces increase with decreasing pulling velocity. Such behaviour is different from the force dependence on the loading rate for single bond rupture or existing models for multiple bonds rupture.     

Multi-step fibrinogen binding to the integrin (alpha)IIb(beta)3 detected using force spectroscopy

The regulated ability of integrin alphaIIbbeta3 to bind fibrinogen plays a crucial role in platelet aggregation and hemostasis. We have developed a model system based on laser tweezers, enabling us to measure specific rupture forces needed to separate single receptor-ligand complexes. First of all, we performed a thorough and statistically representative analysis of nonspecific protein-protein binding versus specific alphaIIbbeta3-fibrinogen interactions in combination with experimental evidence for single-molecule measurements. The rupture force distribution of purified alphaIIbbeta3 and fibrinogen, covalently attached to underlying surfaces, ranged from approximately 20 to 150 pN. This distribution could be fit with a sum of an exponential curve for weak to moderate (20-60 pN) forces, and a Gaussian curve for strong (>60 pN) rupture forces that peaked at 80-90 pN. The interactions corresponding to these rupture force regimes differed in their susceptibility to alphaIIbbeta3 antagonists or Mn2+, an alphaIIbbeta3 activator. Varying the surface density of fibrinogen changed the total binding probability linearly >3.5-fold but did not affect the shape of the rupture force distribution, indicating that the measurements represent single-molecule binding. The yield strength of alphaIIbbeta3-fibrinogen interactions was independent of the loading rate (160-16,000 pN/s), whereas their binding probability markedly correlated with the duration of contact. The aggregate of data provides evidence for complex multi-step binding/unbinding pathways of alphaIIbbeta3 and fibrinogen revealed at the single-molecule level.     

Single molecule characterization of P-selectin/ligand binding

P-selectin expressed on activated platelets and vascular endothelium mediates adhesive interactions to polymorphonuclear leukocytes (PMNs) and colon carcinomas critical to the processes of inflammation and blood-borne metastasis, respectively. How the overall adhesiveness (i.e. the avidity) of receptor/ligand interactions is controlled by the affinity of the individual receptors to single ligands is not well understood. Using single molecule force spectroscopy, we probed in situ both the tensile strength and off-rate of single P-selectin molecules binding to single ligands on intact human PMNs and metastatic colon carcinomas and compared them to the overall avidity of these cells for P-selectin substrates. The use of intact cells rather than purified proteins ensures the proper orientation and preserves post-translational modifications of the P-selectin ligands. The P-selectin/PSGL-1 interaction on PMNs was able to withstand forces up to 175 pN and had an unstressed off-rate of 0.20 s(-1). The tensile strength of P-selectin binding to a novel O-linked, sialylated protease-sensitive ligand on LS174T colon carcinomas approached 125 pN, whereas the unstressed off-rate was 2.78 s(-1). Monte Carlo simulations of receptor/ligand bond rupture under constant loading rate for both P-selectin/PSGL-1 and P-selectin/LS174T ligand binding give distributions and mean rupture forces that are in accord with experimental data. The pronounced differences in the affinity for P-selectin/ligand binding provide a mechanistic basis for the differential abilities of PMNs and carcinomas to roll on P-selectin substrates under blood flow conditions and underline the requirement for single molecule affinity measurements.     

Direct force measurement of single DNA–peptide interactions using atomic force microscopy

The selective interactions between DNA and miniature (39 residues) engineered peptide were directly measured at the single‐molecule level by using atomic force microscopy. This peptide (p007) contains an α‐helical recognition site similar to leucine zipper GCN4 and specifically recognizes the ATGAC sequence in the DNA with nanomolar affinity. The average rupture force was 42.1 pN, which is similar to the unbinding forces of the digoxigenin–antidigoxigenin complex, one of the strongest interactions in biological systems. The single linear fit of the rupture forces versus the logarithm of pulling rates showed a single energy barrier with a transition state located at 0.74 nm from the bound state. The smaller k_off compared with that of other similar systems was presumably due to the increased stability of the helical structure by putative folding residues in p007. This strong sequence‐specific DNA–peptide interaction has a potential to be utilized to prepare well‐defined mechanically stable DNA–protein hybrid nanostructures. Copyright © 2013 John Wiley & Sons, Ltd.     

Application of atomic force microscopy for characteristics of single intermolecular interactions

Atomic force microscopy (AFM) can be used to make measurements in vacuum, air, and water. The method is able to gather information about intermolecular interaction forces at the level of single molecules. This review encompasses experimental and theoretical data on the characterization of ligand-receptor interactions by AFM. The advantage of AFM in comparison with other methods developed for the characterization of single molecular interactions is its ability to estimate not only rupture forces, but also thermodynamic and kinetic parameters of the rupture of a complex. The specific features of force spectroscopy applied to ligand-receptor interactions are examined in this review from the stage of the modification of the substrate and the cantilever up to the processing and interpretation of the data. We show the specificities of the statistical analysis of the array of data based on the results of AFM measurements, and we discuss transformation of data into thermodynamic and kinetic parameters (kinetic dissociation constant, Gibbs free energy, enthalpy, and entropy). Particular attention is paid to the study of polyvalent interactions, where the definition of the constants is hampered due to the complex stoichiometry of the reactions.     

Mechanics of cellular adhesion to artificial artery templates

We are using polymer templates to grow artificial artery grafts in vivo for the replacement of diseased blood vessels. We have previously shown that adhesion of macrophages to the template starts the graft formation. We present a study of the mechanics of macrophage adhesion to these templates on a single cell and single bond level with optical tweezers. For whole cells, in vitro cell adhesion densities decreased significantly from polymer templates polyethylene to silicone to Tygon (167, 135, and 65 cells/mm(2)). These cell densities were correlated with the graft formation success rate (50%, 25%, and 0%). Single-bond rupture forces at a loading rate of 450 pN/s were quantified by adhesion of trapped 2-microm spheres to macrophages. Rupture force distributions were dominated by nonspecific adhesion (forces <40 pN). On polystyrene, preadsorption of fibronectin or presence of serum proteins in the cell medium significantly enhanced adhesion strength from a mean rupture force of 20 pN to 28 pN or 33 pN, respectively. The enhancement of adhesion by fibronectin and serum is additive (mean rupture force of 43 pN). The fraction of specific binding forces in the presence of serum was similar for polystyrene and polymethyl-methacrylate, but specific binding forces were not observed for silica. Again, we found correlation to in vivo experiments, where the density of adherent cells is higher on polystyrene than on silica templates, and can be further enhanced by fibronectin adsorption. These findings show that in vitro adhesion testing can be used for template optimization and to substitute for in-vivo experiments.     

Force spectroscopy of barnase-barstar single molecule interaction

Results of the single molecule force spectroscopy study of specific interactions between ribonuclease barnase and its inhibitor barstar are presented. Experimental data obtained for the force loading rate ranging 2-70 nN/s are well approximated by a single straight line, from which the dissociation barrier of the width of 0.12 nm and height of 0.75-0.85 × 10(-19)J can be inferred. The measured value of specific interaction does not depend on the NaCl concentration. This apparently contradicts the well-known dependence of the binding energy of this pair on the salt concentration, but such a "contradiction" is explained by the insensitivity of the force spectroscopy data to the relatively long-range electrostatic interaction. The latter essentially contributes to the value of barnase-barstar binding energy revealed by biochemical measurements, and it is exactly this electrostatic interaction which is influenced by the salt concentration.     

Dynamic strength of molecular adhesion bonds.

In biology, molecular linkages at, within, and beneath cell interfaces arise mainly from weak noncovalent interactions. These bonds will fail under any level of pulling force if held for sufficient time. Thus, when tested with ultrasensitive force probes, we expect cohesive material strength and strength of adhesion at interfaces to be time- and loading rate-dependent properties. To examine what can be learned from measurements of bond strength, we have extended Kramers' theory for reaction kinetics in liquids to bond dissociation under force and tested the predictions by smart Monte Carlo (Brownian dynamics) simulations of bond rupture. By definition, bond strength is the force that produces the most frequent failure in repeated tests of breakage, i.e., the peak in the distribution of rupture forces. As verified by the simulations, theory shows that bond strength progresses through three dynamic regimes of loading rate. First, bond strength emerges at a critical rate of loading (> or = 0) at which spontaneous dissociation is just frequent enough to keep the distribution peak at zero force. In the slow-loading regime immediately above the critical rate, strength grows as a weak power of loading rate and reflects initial coupling of force to the bonding potential. At higher rates, there is crossover to a fast regime in which strength continues to increase as the logarithm of the loading rate over many decades independent of the type of attraction. Finally, at ultrafast loading rates approaching the domain of molecular dynamics simulations, the bonding potential is quickly overwhelmed by the rapidly increasing force, so that only naked frictional drag on the structure remains to retard separation. Hence, to expose the energy landscape that governs bond strength, molecular adhesion forces must be examined over an enormous span of time scales. However, a significant gap exists between the time domain of force measurements in the laboratory and the extremely fast scale of molecular motions. Using results from a simulation of biotin-avidin bonds (Izrailev, S., S. Stepaniants, M. Balsera, Y. Oono, and K. Schulten. 1997. Molecular dynamics study of unbinding of the avidin-biotin complex. Biophys. J., this issue), we describe how Brownian dynamics can help bridge the gap between molecular dynamics and probe tests.     

Atomic force microscopy-based molecular studies on the recognition of immunogenic chlorinated ovalbumin by macrophage receptors

This report presents simple and reliable approach developed to study the specific recognition events between chlorinated ovalbumin (OVA) and macrophages using atomic force microscopy (AFM). Thanks to the elimination of nonspecific adhesion, the interactions of the native and chlorinated OVA with a membrane of macrophages could be quantified using exclusively the so-called adhesion frequency (AF). The proposed system not only enabled the application of AFM-based force measurements for such poorly defined ligand-receptor pairs but also significantly improved both the acquisition and the processing of the data. The proteins were immobilized on the gold-coated AFM tips from the aqueous solutions containing charged thiol adsorbates. Such surface dilution of the proteins ensured the presence of single or just a few macromolecules at the tip-surface contact. The formation of negatively charged monolayer on the tip dramatically limited its nonspecific interactions with the macrophage surface. In such systems, AF was used as a measure of the recognition events even if the interaction forces varied significantly for sets of measurements. The system with the native OVA, a weak immunogen, showed only negligible AF compared with 85% measured for the immunogenic chlorinated OVA. The AF values varied with the tip-macrophage contact time and loading velocity. Blocking of the receptors by the chlorinated OVA was also confirmed. The developed approach can be also used to study other ligand-receptor interactions in poorly defined biological systems with intrinsically broad distribution of the rupture forces, thus opening new fields for AFM-based recognition on molecular level.     

Discrete interactions in cell adhesion measured by single-molecule force spectroscopy

Cell-cell adhesion mediated by specific cell-surface molecules is essential for multicellular development. Here we quantify de-adhesion forces at the resolution of individual cell-adhesion molecules, by controlling the interactions between single cells and combining single-molecule force spectroscopy with genetic manipulation. Our measurements are focused on a glycoprotein, contact site A (csA), as a prototype of cell-adhesion proteins. csA is expressed in aggregating cells of Dictyostelium discoideum, which are engaged in development of a multicellular organism. Adhesion between two adjacent cell surfaces involves discrete interactions characterized by an unbinding force of 23 +/- 8 pN, measured at a rupture rate of 2.5 +/- 0.5 microm s-1.     

Successive detection of insulin‐like growth factor‐II bound to receptors on a living cell surface using an AFM

In this study, we have developed a method of mechanical force detection for ligands bound to receptors on a cell surface, both of which are involved in a signal transduction pathway. This pathway is an autocrine pathway, involving the production of insulin‐like growth factor‐II (IGF‐II) and activation of the IGF‐I receptor, involved in myoblast differentiation induced by MyoD in C3H10T1/2 mouse mesenchymal stem cells. Differentiation of C3H10T1/2 was induced with the DNA demethylation agent 5‐azacytidine (5‐aza). The etched AFM tip used in the force detection had a flat surface of which about 10 µm² was in contact with a cell surface. The forces required to rupture the interactions of IGF‐IIs on a cell and anti mouse IGF‐II polyclonal antibody immobilized on an etched AFM tip were measured within 5 days of induction of differentiation. The mean unbinding force for a single paired antibody–ligand on a cell was about 81 pN, which was measured at a force loading rate of about 440 nN/s. The percentage of unbinding forces over 100 pN increased to 32% after 2 days from the addition of 5‐aza to the medium. This method could be used in non‐invasive and successive evaluation of a living cell's behavior. Copyright © 2009 John Wiley & Sons, Ltd.     

Mg2+ modulates integrin–extracellular matrix interaction in vascular smooth muscle cells studied by atomic force microscopy

Atomic force microscopy (AFM) was used to investigate the interaction between α5β1 integrin and fibronectin (FN) in the presence of divalent cations. AFM probes were labeled with FN and used to measure binding strength between α5β1 integrin and FN by quantifying the force required to break single FN–integrin bonds on a physiological range of loading rates (100–10 000 pN/s). The force necessary to rupture single α5β1–FN bond increased twofold over the regime of loading rates investigated. Changes in Mg²⁺ and Ca²⁺ concentration affected the thermodynamical parameters of the interaction and modulated the binding energy. These data indicate that the external ionic environment in which vascular smooth muscle cells reside, influences the mechanical parameters that define the interaction between the extracellular matrix and integrins. Thus, in a dynamic mechanical environment such as the vascular wall, thermodynamic binding properties between FN and α5β1 integrin vary in relation to locally applied loads and divalent cations concentrations. These changes can be recorded as direct measurements on live smooth muscle cells by using AFM. Copyright © 2009 John Wiley & Sons, Ltd.     

Methods for reducing nonspecific interaction in antibody-antigen assay via atomic force microscopy

We developed a method to measure the rupture forces between antibody and antigen by atomic force microscopy (AFM). Previous studies have reported that in the measurement of antibody–antigen interaction using AFM, the specific intermolecular forces are often obscured by nonspecific adhesive binding forces between antibody immobilized cantilever and substrate surfaces on which antigen or nonantigen are fixed. Here, we examined whether detergent and nonreactive protein, which have been widely used to reduce nonspecific background signals in ordinary immunoassay and immunoblotting, could reduce the nonspecific forces in the AFM measurement. The results showed that, in the presence of both nonreactive protein and detergent, the rupture forces between anti-ferritin antibodies immobilized on a tip of cantilever and ferritin (antigen) on the substrate could be successfully measured, distinguishing from nonspecific adhesive forces. In addition, we found that approach/retraction velocity of the AFM cantilever was also important in the reduction of nonspecific adhesion. These insights will contribute to the detection of specific molecules at nanometer scale region and the investigation of intermolecular interaction by the use of AFM.     

Probing the interaction between p53 and the bacterial protein azurin by single molecule force spectroscopy

p53 is a human tumour suppressor which regulates multiple cellular processes, including cell growth, genomic stability and cell death. Recent works have demonstrated the bacterial redox protein azurin to enter cancer cells and induce apoptosis through p53 stabilization, resulting in a tumour growth regression. Azurin has been shown to bind p53 although many details of the complex formed by these two proteins are still poorly characterized. Here, we get insight into the kinetics of this complex formation, by exploring the interaction between p53 and azurin in their environment by single molecule force spectroscopy. To this aim, azurin has been linked to the atomic force microscope tip, whereas p53 has been immobilized onto a gold substrate. Therefore, by performing force-distance cycles we have detected specific recognition events between p53 and azurin, displaying unbinding forces of around 70 pN for an applied loading rate of 3 nN s(-1). The specificity of these events has been assessed by the significant reduction of their frequency observed after blocking the p53 sample by an azurin solution. Moreover, by measuring the rupture force as a function of the loading rate we have determined the dissociation rate constant of this complex to be approximately 0.1 s(-1). Our findings are here discussed in connection with results obtained in bulk experiments, with the aim of clarifying some molecular details of the p53-azurin complex that may help designing new anticancer strategy.     

Dynamic force spectroscopy of the digoxigenin-antibody complex

Small ligands and their receptors are widely used non-covalent couplers in various biotech applications. One prominent example, the digoxigenin-antibody complex, was often used to immobilize samples for single molecule force measurements by optical trap or AFM. Here, we employed dynamic AFM spectroscopy to demonstrate that a single digoxigenin-antibody bond is likely to fail even under moderate loading rates. This effect potentially could lower the yield of measurements or even obscure the unbinding data of the sample by the rupture events of the coupler. Immobilization by multiple antibody-antigen bonds, therefore, is highly recommended. The analysis of our data revealed a pronounced loading rate dependence of the rupture force, which we analyzed based on the well-established Bell-Evans-model with two subsequent unbinding barriers. We could show that the first barrier has a width of Deltax(1)=1.15 nm and a spontaneous rate of k(off1)=0.015 s(-1) and the second has a width of Deltax(2)=0.35 nm and a spontaneous rate of k(off2)=4.56 s(-1). In the crossover region between the two regimes, we found a marked discrepancy between the predicted bond rupture probability density and the measured rupture force histograms, which we discuss as non-Markovian contribution to the unbinding process.     

Force spectroscopy of the double-tethered concanavalin-A mannose bond

We present the measurement of the force required to rupture a single protein-sugar bond using a methodology that provides selective discrimination between specific and nonspecific binding events and helps verify the presence of a single functional molecule on the atomic force microscopy tip. In particular, the interaction force between a polymer-tethered concanavalin-A protein (ConA) and a similarly tethered mannose carbohydrate was measured as 47 +/- 9 pN at a bond loading rate of approximately 10 nN/s. Computer simulations of the polymer molecular configurations were used to determine the angles that the polymers could sweep out during binding and, in conjunction with mass spectrometry, used to separate the angular effects from the effects due to a distribution of tether lengths. We find that when using commercially available polymer tethers that vary in length from 19 to 29 nm, the angular effects are relatively small and the rupture distributions are dominated by the 10-nm width of the tether length distribution. In all, we show that tethering both a protein and its ligand allows for the determination of the single-molecule bond rupture force with high sensitivity and includes some validation for the presence of a single-tethered functional molecule on the atomic force microscopy tip.     

Differences in zero-force and force-driven kinetics of ligand dissociation from beta-galactoside-specific proteins (plant and animal lectins, immunoglobulin G) monitored by plasmon resonance and dynamic single molecule force microscopy

Protein-carbohydrate interactions are involved in diverse regulatory processes. To help understand the mechanics and kinetics of dissociation of receptor-ligand complexes, we have analyzed the separation of lactose and the N-glycan chains of asialofetuin (ASF) from three lectins and an immunoglobulin G fraction by surface plasmon resonance at zero force and by atomic force microscopy with variations of the external force. While the (AB)2 agglutinins from Ricinus communis (RCA) and Viscum album (VAA) show structural homology, the homodimeric galectin-1 from bovine heart (BHL) has no similarity to the two plant lectins except for sharing this monosaccharide specificity. The beta-galactoside-binding immunoglobulin G (IgG) fraction from human serum provides a further model system with distinct binding-site architecture. The k(off) constants for the two plant agglutinins were independent of the nature of the ligand at 1.1-1.3 x 10(-3) s(-1), whereas the geometry of ligand and binding site presentation affected this parameter for BHL (0.5 x 10(-3) s(-1) for lactose and 1 x 10(-3) s(-1) for ASF) and IgG (1.3 x 10(-3) s(-1) for lactose and 0.55 x 10(-3) s(-1) for ASF). When assessing comparatively the rupture forces at a loading rate of 3 nN/s with lactose as ligand, 34 +/- 6 pN (BHL), 36 +/- 4 pN (IgG), 47 +/- 7 pN (VAA), and 58 +/- 9 pN (RCA) were measured. For the same loading rate the rupture forces for the receptor-ASF interactions were found to be 37 +/- 3 pN (BHL), 43 +/- 5 pN (VAA), 45 +/- 6 pN (IgG), and 65 +/- 9 pN (RCA). The variation of the pulling velocity revealed in all cases a linear dependence between the rupture force and the natural logarithm of the loading rate. Performing probability density and Monte Carlo calculations, the potential barrier widths, which determine the inverse dynamic dependence with the rate of force elevation, increased from 4 A (RCA) and 7 A (VAA and IgG) to 10 A (BHL) for the receptor-lactose interactions. Presenting ASF as ligand potential widths of 4 A for RCA and IgG and 6 A for VAA and BHL were obtained. Since the dissociation kinetics at zero force apparently cannot predict the behavior in force-driven experiments, these results reveal new insights into biological functions. The dissociation kinetics under force helps to explain the difference in the toxic potency of VAA and RCA and points to a function of the galectin in cis-crosslinking and in transient trans-bridging.     

OXTR methylation modulates exogenous oxytocin effects on human brain activity during social interaction

Oxytocin (OT) effects on brain function and behavior are mediated by the oxytocin receptor (OXTR). The distribution of OXTR in the brain can profoundly influence social behavior. Emerging evidence suggests that DNA methylation of OXTR influences OXTR expression. Previously, we conducted a pharmaco‐functional Magnetic Resonance Imaging (fMRI) study in which healthy subjects were randomized to 24 IU intranasal OT or placebo and imaged with fMRI while playing a dyadic social interaction task known as the iterated Prisoner's Dilemma (PD) game with same‐sex partners. Here, we investigate whether DNA methylation of OXTR modulates the effect of intranasal OT on the neural response to positive and negative social interactions in the PD game. OXTR methylation did not modulate OT effects within brain regions where we previously reported OT effects in response to reciprocated (caudate nucleus) and unreciprocated cooperation (amygdala and anterior insula). However, OXTR methylation did modulate OT effects on the response to both reciprocated and unreciprocated cooperation in other brain regions such as the precuneus and visual cortex. Further restricting the analysis to OXTR rs53576 GG individuals revealed that OXTR methylation modulated OT effects on the precuneus response to reciprocated cooperation in men, the lateral septum response to reciprocated cooperation in women, and the visual cortex response to unreciprocated cooperation in men. These results suggest that OXTR methylation status may influence OT effects on mentalizing, attention and reward processing during social interactions. OXTR methylation may be important to consider if exogenous OT is used to treat social behavioral disorders in the future.     

Force spectroscopy of the fibrin(ogen)-fibrinogen interaction

Fibrin aggregation is of vital importance in many physiological and pathological processes, such as blood coagulation, wound healing, and thrombosis. In the present study, we investigated the forces involved in the initial steps of the fibrinogen fibrin aggregation by force spectroscopy using the atomic force microscope. Our data confirm the existence of strong specific interactions between fibrin and fibrin(ogen), with unbinding forces ranging from 290 to 375 pN and a logarithmic dependence on the loading rate between 0.8 and 23 nN/s.