Mechanical unfolding of cardiac myosin binding protein-C by atomic force microscopy

Cardiac myosin-binding protein-C (cMyBP-C) is a thick-filament-associated protein that performs regulatory and structural roles within cardiac sarcomeres. It is a member of the immunoglobulin (Ig) superfamily of proteins consisting of eight Ig- and three fibronectin (FNIII)-like domains, along with a unique regulatory sequence referred to as the M-domain, whose structure is unknown. Domains near the C-terminus of cMyBP-C bind tightly to myosin and mediate the association of cMyBP-C with thick (myosin-containing) filaments, whereas N-terminal domains, including the regulatory M-domain, bind reversibly to myosin S2 and/or actin. The ability of MyBP-C to bind to both myosin and actin raises the possibility that cMyBP-C cross-links myosin molecules within the thick filament and/or cross-links myosin and thin (actin-containing) filaments together. In either scenario, cMyBP-C could be under mechanical strain. However, the physical properties of cMyBP-C and its behavior under load are completely unknown. Here, we investigated the mechanical properties of recombinant baculovirus-expressed cMyBP-C using atomic force microscopy to assess the stability of individual cMyBP-C molecules in response to stretch. Force-extension curves showed the presence of long extensible segment(s) that became stretched before the unfolding of individual Ig and FNIII domains, which were evident as sawtooth peaks in force spectra. The forces required to unfold the Ig/FNIII domains at a stretch rate of 500 nm/s increased monotonically from ∼30 to ∼150 pN, suggesting a mechanical hierarchy among the different Ig/FNIII domains. Additional experiments using smaller recombinant proteins showed that the regulatory M-domain lacks significant secondary or tertiary structure and is likely an intrinsically disordered region of cMyBP-C. Together, these data indicate that cMyBP-C exhibits complex mechanical behavior under load and contains multiple domains with distinct mechanical properties.     

Mechanical design of proteins studied by single-molecule force spectroscopy and protein engineering

Mechanical unfolding and refolding may regulate the molecular elasticity of modular proteins with mechanical functions. The development of the atomic force microscopy (AFM) has recently enabled the dynamic measurement of these processes at the single-molecule level. Protein engineering techniques allow the construction of homomeric polyproteins for the precise analysis of the mechanical unfolding of single domains. alpha-Helical domains are mechanically compliant, whereas beta-sandwich domains, particularly those that resist unfolding with backbone hydrogen bonds between strands perpendicular to the applied force, are more stable and appear frequently in proteins subject to mechanical forces. The mechanical stability of a domain seems to be determined by its hydrogen bonding pattern and is correlated with its kinetic stability rather than its thermodynamic stability. Force spectroscopy using AFM promises to elucidate the dynamic mechanical properties of a wide variety of proteins at the single molecule level and provide an important complement to other structural and dynamic techniques (e.g., X-ray crystallography, NMR spectroscopy, patch-clamp).     

Cross-Species Mechanical Fingerprinting of Cardiac Myosin Binding Protein-C

Cardiac myosin binding protein-C (cMyBP-C) is a member of the immunoglobulin (Ig) superfamily of proteins and consists of 8 Ig- and 3 fibronectin III (FNIII)-like domains along with a unique regulatory sequence referred to as the MyBP-C motif or M-domain. We previously used atomic force microscopy to investigate the mechanical properties of murine cMyBP-C expressed using a baculovirus/insect cell expression system. Here, we investigate whether the mechanical properties of cMyBP-C are conserved across species by using atomic force microscopy to manipulate recombinant human cMyBP-C and native cMyBP-C purified from bovine heart. Force versus extension data obtained in velocity-clamp experiments showed that the mechanical response of the human recombinant protein was remarkably similar to that of the bovine native cMyBP-C. Ig/Fn-like domain unfolding events occurred in a hierarchical fashion across a threefold range of forces starting at relatively low forces of ∼50 pN and ending with the unfolding of the highest stability domains at ∼180 pN. Force-extension traces were also frequently marked by the appearance of anomalous force drops suggestive of additional mechanical complexity such as structural coupling among domains. Both recombinant and native cMyBP-C exhibited a prominent segment ∼100 nm-long that could be stretched by forces <50 pN before the unfolding of Ig- and FN-like domains. Combined with our previous observations of mouse cMyBP-C, these results establish that although the response of cMyBP-C to mechanical load displays a complex pattern, it is highly conserved across species.     

Mechanical Design of the Third FnIII Domain of Tenascin-C

By combining single-molecule atomic force microscopy (AFM), proline mutagenesis and steered molecular dynamics (SMD) simulations, we investigated the mechanical unfolding dynamics and mechanical design of the third fibronectin type III domain of tenascin-C (TNfn3) in detail. We found that the mechanical stability of TNfn3 is similar to that of other constituting FnIII domains of tenascin-C, and the unfolding process of TNfn3 is an apparent two-state process. By employing proline mutagenesis to block the formation of backbone hydrogen bonds and introduce structural disruption in β sheet, we revealed that in addition to the important roles played by hydrophobic core packing, backbone hydrogen bonds in β hairpins are also responsible for the overall mechanical stability of TNfn3. Furthermore, proline mutagenesis revealed that the mechanical design of TNfn3 is robust and the mechanical stability of TNfn3 is very resistant to structural disruptions caused by proline substitutions in β sheets. Proline mutant F88P is one exception, as the proline mutation at position 88 reduced the mechanical stability of TNfn3 significantly and led to unfolding forces of < 20 pN. This result suggests that Phe88 is a weak point of the mechanical resistance for TNfn3. We used SMD simulations to understand the molecular details underlying the mechanical unfolding of TNfn3. The comparison between the AFM results and SMD simulations revealed similarities and discrepancies between the two. We compared the mechanical unfolding and design of TNfn3 and its structural homologue, the tenth FnIII domain from fibronectin. These results revealed the complexity underlying the mechanical design of FnIII domains and will serve as a starting point for systematically analyzing the mechanical architecture of other FnIII domains in tenascins-C, and will help to gain a better understanding of some of the complex features observed for the stretching of native tenascin-C.     

Single-Molecule Studies on PolySUMO Proteins Reveal Their Mechanical Flexibility

Proteins with β-sandwich and β-grasp topologies are resistant to mechanical unfolding as shown by single-molecule force spectroscopy studies. Their high mechanical stability has generally been associated with the mechanical clamp geometry present at the termini. However, there is also evidence for the importance of interactions other than the mechanical clamp in providing mechanical stability, which needs to be tested thoroughly. Here, we report the mechanical unfolding properties of ubiquitin-like proteins (SUMO1 and SUMO2) and their comparison with those of ubiquitin. Although ubiquitin and SUMOs have similar size and structural topology, they differ in their sequences and structural contacts, making them ideal candidates to understand the variations in the mechanical stability of a given protein topology. We observe a two-state unfolding pathway for SUMO1 and SUMO2, similar to that of ubiquitin. Nevertheless, the unfolding forces of SUMO1 (∼130 pN) and SUMO2 (∼120 pN) are lower than that of ubiquitin (∼190 pN) at a pulling speed of 400 nm/s, indicating their lower mechanical stability. The mechanical stabilities of SUMO proteins and ubiquitin are well correlated with the number of interresidue contacts present in their structures. From pulling speed-dependent mechanical unfolding experiments and Monte Carlo simulations, we find that the unfolding potential widths of SUMO1 (∼0.51 nm) and SUMO2 (∼0.33 nm) are much larger than that of ubiquitin (∼0.19 nm), indicating that SUMO1 is six times and SUMO2 is three times mechanically more flexible than ubiquitin. These findings might also be important in understanding the functional differences between ubiquitin and SUMOs.     

Heterophilic interactions of sodium channel beta1 subunits with axonal and glial cell adhesion molecules

Voltage-gated sodium channels localize at high density in axon initial segments and nodes of Ranvier in myelinated axons. Sodium channels consist of a pore-forming alpha subunit and at least one beta subunit. beta1 is a member of the immunoglobulin superfamily of cell adhesion molecules and interacts homophilically and heterophilically with contactin and Nf186. In this study, we characterized beta1 interactions with contactin and Nf186 in greater detail and investigated interactions of beta1 with NrCAM, Nf155, and sodium channel beta2 and beta3 subunits. Using Fc fusion proteins and immunocytochemical techniques, we show that beta1 interacts with the fibronectin-like domains of contactin. beta1 also interacts with NrCAM, Nf155, sodium channel beta2, and Nf186 but not with sodium channel beta3. The interaction of the extracellular domains of beta1 and beta2 requires the region 169TEEEGKTDGEGNA181 located in the intracellular domain of beta2. Interaction of beta1 with Nf186 results in increased Nav).2 cell surface density over alpha alone, similar to that shown previously for contactin and beta2. We propose that beta1 is the critical communication link between sodium channels, nodal cell adhesion molecules, and ankyrinG.     

Single-molecule force spectroscopy reveals a stepwise unfolding of Caenorhabditis elegans giant protein kinase domains

Myofibril assembly and disassembly are complex processes that regulate overall muscle mass. Titin kinase has been implicated as an initiating catalyst in signaling pathways that ultimately result in myofibril growth. In titin, the kinase domain is in an ideal position to sense mechanical strain that occurs during muscle activity. The enzyme is negatively regulated by intramolecular interactions occurring between the kinase catalytic core and autoinhibitory/regulatory region. Molecular dynamics simulations suggest that human titin kinase acts as a force sensor. However, the precise mechanism(s) resulting in the conformational changes that relieve the kinase of this autoinhibition are unknown. Here we measured the mechanical properties of the kinase domain and flanking Ig/Fn domains of the Caenorhabditis elegans titin-like proteins twitchin and TTN-1 using single-molecule atomic force microscopy. Our results show that these kinase domains have significant mechanical resistance, unfolding at forces similar to those for Ig/Fn β-sandwich domains (30-150 pN). Further, our atomic force microscopy data is consistent with molecular dynamic simulations, which show that these kinases unfold in a stepwise fashion, first an unwinding of the autoinhibitory region, followed by a two-step unfolding of the catalytic core. These data support the hypothesis that titin kinase may function as an effective force sensor.     

Biophysical investigations of engineered polyproteins: implications for force data

Dynamic force spectroscopy is rapidly becoming a standard biophysical technique. Significant advances in the methods of analysis of force data have resulted in ever more complex systems being studied. The use of cloning systems to produce homologous tandem repeats rather than the use of endogenous multidomain proteins has facilitated these developments. What is poorly addressed are the physical properties of these constructed polyproteins. Are the properties of the individual domains in the construct independent of one another or attenuated by adjacent domains? We present data for a construct of eight fibronectin type III domains from the human form of tenascin that exhibits approximately 1 kcal mol(-1) increase in stability compared to the monomer. This effect is salt and pH dependent, suggesting that the stabilization results from electrostatic interactions, possibly involving charged residues at the interfaces of the domains. Kinetic analysis shows that this stabilization reflects a slower unfolding rate. Clearly, if domain-domain interactions affect the unfolding force, this will have implications for the comparison of absolute forces between types of domains. Mutants of the tenascin 8-mer construct exhibit the same change in stability as that observed for the corresponding mutation in the monomer. And when Phi-values are calculated for the 8-mer construct, the pattern is similar to that observed for the monomer. Therefore, mutational analyses to resolve mechanical unfolding pathways appear valid. Importantly, we show that interactions between the domains may be masked by changes in experimental conditions.     

Force-Induced Unfolding of Leucine-Rich Repeats of Glycoprotein Ibα Strengthens Ligand Interaction

Leucine-rich repeat (LRR) is a versatile motif widely present in adhesive proteins and signal-transducing receptors. The concave structure formed by a group of LRRs is thought to facilitate binding to globular protein domains with increased affinities. However, little is known about the conformational dynamics of LRRs in such a structure, e.g., whether and how force induces conformational changes in LRRs to regulate protein binding and signal transduction. Here we investigated the platelet glycoprotein Ibα (GPIbα), a demonstrated mechanoreceptor with known crystal structures for the N-terminal domain (GPIbαN), as a model for LRR-containing proteins using a combined method of steered molecular dynamics simulations and single-molecule force spectroscopy with a biomembrane force probe. We found that force-induced unfolding of GPIbαN starts with LRR2–4 and propagates to other LRRs. Importantly, force-dependent lifetimes of individual VWF-A1 bonds with GPIbα are prolonged after LRR unfolding. Enhancement of protein-protein interactions by force-induced LRR unfolding may be a phenomenon of interest in biology.     

Prying open single GroES ring complexes by force reveals cooperativity across domains

Understanding how the mechanical properties of a protein complex emerge from the interplay of intra- and interchain interactions is vital at both fundamental and applied levels. To investigate whether interdomain cooperativity affects protein mechanical strength, we employed single-molecule force spectroscopy to probe the mechanical stability of GroES, a homoheptamer with a domelike quaternary stucture stabilized by intersubunit interactions between the first and last β-strands of adjacent domains. A GroES variant was constructed in which each subunit of the GroES heptamer is covalently linked to adjacent subunits by tripeptide linkers and folded domains of protein L are introduced to the heptamer's termini as handle molecules. The force-distance profiles for GroES unfolding showed, for the first time that we know of, a mechanical phenotype whereby seven distinct force peaks, with alternating behavior of unfolding force and contour length (ΔL(c)), were observed with increasing unfolding-event number. Unfolding of (GroES)(7) is initiated by breakage of the interface between domains 1 and 7 at low force, which imparts a polarity to (GroES)(7) that results in two distinct mechanical phenotypes of these otherwise identical protein domains. Unfolding then proceeds by peeling domains off the domelike native structure by sequential repetition of the denaturation of mechanically weak (unfoldon 1) and strong (unfoldon 2) units. These results indicate that domain-domain interactions help to determine the overall mechanical strength and unfolding pathway of the oligomeric structure. These data reveal an unexpected richness in the mechanical behavior of this homopolyprotein, yielding a complex with greater mechanical strength and properties distinct from those that would be apparent for GroES domains in isolation.     

Single molecule force spectroscopy reveals that electrostatic interactions affect the mechanical stability of proteins

It is well known that electrostatic interactions play important roles in determining the thermodynamic stability of proteins. However, the investigation into the role of electrostatic interactions in mechanical unfolding of proteins has just begun. Here we used single molecule atomic force microscopy techniques to directly evaluate the effect of electrostatic interactions on the mechanical stability of a small protein GB1. We engineered a bi-histidine motif into the force-bearing region of GB1. By varying the pH, histidine residues can switch between protonated and deprotonated states, leading to the change of the electrostatic interactions between the two histidine residues. We found that the mechanical unfolding force of the engineered protein decreased by ∼34% (from 115 pN to 76 pN) on changing the pH from 8.5 to 3, due to the increased electrostatic repulsion between the two positively charged histidines at acidic pH. Our results demonstrated that electrostatic interactions can significantly affect the mechanical stability of elastomeric proteins, and modulating the electrostatic interactions of key charged residues can become a promising method for regulating the mechanical stability of elastomeric proteins.     

Differential mechanical stability of filamin A rod segments

Prompted by recent reports suggesting that interaction of filamin A (FLNa) with its binding partners is regulated by mechanical force, we examined mechanical properties of FLNa domains using magnetic tweezers. FLNa, an actin cross-linking protein, consists of two subunits that dimerize through a C-terminal self-association domain. Each subunit contains an N-terminal spectrin-related actin-binding domain followed by 24 immunoglobulinlike (Ig) repeats. The Ig repeats in the rod 1 segment (repeats 1–15) are arranged as a linear array, whereas rod 2 (repeats 16–23) is more compact due to interdomain interactions. In the rod 1 segment, repeats 9–15 augment F-actin binding to a much greater extent than do repeats 1–8. Here, we report that the three segments are unfolded at different forces under the same loading rate. Remarkably, we found that repeats 16–23 are susceptible to forces of ∼10 pN or even less, whereas the repeats in the rod 1 segment can withstand significantly higher forces. The differential force response of FLNa Ig domains has broad implications, since these domains not only support the tension of actin network but also interact with many transmembrane and signaling proteins, mostly in the rod 2 segment. In particular, our finding of unfolding of repeats 16–23 at ∼10 pN or less is consistent with the hypothesized force-sensing function of the rod 2 segment in FLNa.     

Neuronal cell adhesion molecule contactin/F11 binds to tenascin via its immunoglobulin-like domains

Adhesive interactions between neurons and extracellular matrix (ECM) play a key role in neuronal pattern formation. The prominent role played by the extracellular matrix protein tenascin/cytotactin in the development of the nervous system, tied to its abundance, led us to speculate that brain may contain yet unidentified tenascin receptors. Here we show that the neuronal cell adhesion molecule contactin/F11, a member of the immunoglobulin(Ig)-superfamily, is a cell surface ligand for tenascin in the nervous system. Through affinity chromatography of membrane glycoproteins from chick brain on tenascin-Sepharose, we isolated a major cell surface ligand of 135 kD which we identified as contactin/F11 by NH2-terminal sequencing. The binding specificity between contactin/F11 and tenascin was demonstrated in solid-phase assays. Binding of immunopurified 125I-labeled contactin/F11 to immobilized tenascin is completely inhibited by the addition of soluble tenascin or contactin/F11, but not by fibronectin. When the fractionated isoforms of tenascin were used as substrates, contactin/F11 bound preferentially to the 190-kD isoform. This isoform differs in having no alternatively spliced fibronectin type III domains. Our results imply that the introduction of these additional domains in some way disrupts the contactin/F11 binding site on tenascin. To localize the binding site on contactin/F11, proteolytic fragments were generated and characterized by NH2-terminal sequencing. The smallest contactin/F11 fragment which binds tenascin is 45 kD and also begins with the contactin/F11 NH2-terminal sequence. This implies that contactin/F11 binds to tenascin through a site within the first three Ig-domains.     

States and transitions during forced unfolding of a single spectrin repeat

Spectrin is a vital and abundant protein of the cytoskeleton. It has an elongated structure that is made by a chain of so-called spectrin repeats. Each repeat contains three antiparallel alpha-helices that form a coiled-coil structure. Spectrin forms an oligomeric structure that is able to cross-link actin filaments. In red cells, the spectrin/actin meshwork underlying cell membrane is thought to be responsible for special elastic properties of the cell. In order to determine mechanical unfolding properties of the spectrin repeat, we have used single molecule force spectroscopy to study the states of unfolding of an engineered polymeric protein consisting of identical spectrin domains. We demonstrate that the unfolding of spectrin domains can occur in a stepwise fashion during stretching. The force-extension patterns exhibit features that are compatible with the existence of at least one intermediate between the folded and the completely unfolded conformation. Only those polypeptides that still contain multiple intact repeats display intermediates, indicating a stabilisation effect. Precise force spectroscopy measurements on single molecules using engineered protein constructs reveal states and transitions during the mechanical unfolding of spectrin. Single molecule force spectroscopy appears to open a new window for the analysis of transition probabilities between different conformational states.     

Thermal effects in stretching of Go-like models of titin and secondary structures

The effect of temperature on mechanical unfolding of proteins is studied using a Go-like model with a realistic contact map and Lennard-Jones contact interactions. The behavior of the I27 domain of titin and its serial repeats is contrasted to that of simple secondary structures. In all cases, thermal fluctuations accelerate the unraveling process, decreasing the unfolding force nearly linearly at low temperatures. However, differences in bonding geometry lead to different sensitivity to temperature and different changes in the unfolding pattern. Due to its special native-state geometry, titin is much more thermally and elastically stable than the secondary structures. At low temperatures, serial repeats of titin show a parallel unfolding of all domains to an intermediate state, followed by serial unfolding of the domains. At high temperatures, all domains unfold simultaneously, and the unfolding distance decreases monotonically with the contact order, that is, the sequence distance between the amino acids that form the native contact.     

The study of protein mechanics with the atomic force microscope.

The unfolding and folding of single protein molecules can be studied with an atomic force microscope (AFM). Many proteins with mechanical functions contain multiple, individually folded domains with similar structures. Protein engineering techniques have enabled the construction and expression of recombinant proteins that contain multiple copies of identical domains. Thus, the AFM in combination with protein engineering has enabled the kinetic analysis of the force-induced unfolding and refolding of individual domains as well as the study of the determinants of mechanical stability.     

Three steps in the thermal unfolding of F-actin: an experimental evidence

The development of differential scanning calorimetry has resulted in an increased interest in studies of the unfolding process in proteins with the aim of identifying domains and interactions with ligands or other proteins. Several of these studies were done with actin and showed that the thermal unfolding of F-actin occurs in at least three steps; this was interpreted as the denaturation of independent domains. In the present work, we have followed the thermal unfolding of F-actin using differential scanning calorimetry (DSC), CD spectroscopy, and probe fluorescence. We found that the three steps revealed through DSC are not the denaturation of independent domains. These three steps are a change in the environment of cys 374 at 49.5 degrees C; a modification at the nucleotide-binding site at 55 degrees C; and the unfolding of the peptide chain at 64 degrees C. Previous interpretations of the thermograms of F-actin were thus erroneous. Since DSC is now widely used to study proteins, our experimental approach and conclusions may also be relevant in denaturation studies of proteins in general.     

Analyzing forced unfolding of protein tandems by ordered variates, 1: Independent unfolding times

Most of the mechanically active proteins are organized into tandems of identical repeats, (D)N, or heterogeneous tandems, D1-D2-...-DN. In current atomic force microscopy experiments, conformational transitions of protein tandems can be accessed by employing constant stretching force f (force-clamp) and by analyzing the recorded unfolding times of individual domains. Analysis of unfolding data for homogeneous tandems relies on the assumption that unfolding times are independent and identically distributed, and involves inference of the (parent) probability density of unfolding times from the histogram of the combined unfolding times. This procedure cannot be used to describe tandems characterized by interdomain interactions, or heteregoneous tandems. In this article, we introduce an alternative approach that is based on recognizing that the observed data are ordered, i.e., first, second, third, etc., unfolding times. The approach is exemplified through the analysis of unfolding times for a computer model of the homogeneous and heterogeneous tandems, subjected to constant force. We show that, in the experimentally accessible range of stretching forces, the independent and identically distributed assumption may not hold. Specifically, the uncorrelated unfolding transitions of individual domains at lower force may become correlated (dependent) at elevated force levels. The proposed formalism can be used in atomic force microscopy experiments to infer the unfolding time distributions of individual domains from experimental histograms of ordered unfolding times, and it can be extended to analyzing protein tandems that exhibit interdomain interactions.     

Force spectroscopy studies on protein–ligand interactions: A single protein mechanics perspective

Protein–ligand interactions are ubiquitous and play important roles in almost every biological process. The direct elucidation of the thermodynamic, structural and functional consequences of protein–ligand interactions is thus of critical importance to decipher the mechanism underlying these biological processes. A toolbox containing a variety of powerful techniques has been developed to quantitatively study protein–ligand interactions in vitro as well as in living systems. The development of atomic force microscopy-based single molecule force spectroscopy techniques has expanded this toolbox and made it possible to directly probe the mechanical consequence of ligand binding on proteins. Many recent experiments have revealed how ligand binding affects the mechanical stability and mechanical unfolding dynamics of proteins, and provided mechanistic understanding on these effects. The enhancement effect of mechanical stability by ligand binding has been used to help tune the mechanical stability of proteins in a rational manner and develop novel functional binding assays for protein–ligand interactions. Single molecule force spectroscopy studies have started to shed new lights on the structural and functional consequence of ligand binding on proteins that bear force under their biological settings.