Local rigidity of a protein molecule

Distribution of soft and rigid substructures within a protein molecule has been implicated in several occasions and most recently from the imaging and indentation experiments using an atomic force microscope. In this paper, previously reported result of mechanical extension experiments on the recombinant bovine carbonic anhydrase II, Q253C, is re-analyzed to estimate the distribution of Young's modulus, Y, in this protein. The force vs. extension curve of the enzymatically active, type I conformer gave an estimate of Y increasing from 40 to 220 MPa as the polypeptide chain was extended from 10 to 75 nm indicating the presence of a rigid core structure. The enzymatically inactive type II, in contrast, gave an almost constant modulus of 55+/-15 MPa in the same extension range in agreement with the previous proposal that it lacked a core structure.     

Topography and mechanical properties of single molecules of type I collagen using atomic force microscopy

Although the mechanical behavior of tendon and bone has been studied for decades, there is still relatively little understanding of the molecular basis for their specific properties. Thus, despite consisting structurally of the same type I collagen, bones and tendons have evolved to fulfill quite different functions in living organisms. In an attempt to understand the links between the mechanical properties of these collageneous structures at the macro- and nanoscale, we studied trimeric type I tropocollagen molecules by atomic force microscopy, both topologically and by force spectroscopy. High-resolution imaging demonstrated a mean (+/- SD) contour length of (287 +/- 35) nm and height of (0.21 +/- 0.03) nm. Submolecular features, namely the coil-pitch of the molecule, were also observed, appearing as a repeat pattern along the length of the molecule, with a length of approximately 8 nm that is comparable to the theoretical value. Using force spectroscopy, we established the stretching pattern of the molecule, where both the mechanical response of the molecule and pull-off peak are convoluted in a single feature. By interpreting this response with a wormlike chain model, we extracted the value of the effective contour length of the molecule at (202 +/- 5) nm. This value was smaller than that given by direct measurement, suggesting that the entire molecule was not being stretched during the force measurements; this is likely to be related to the absence of covalent binding between probe, sample, and substrate in our experimental procedure.     

Fabrication of single carbonic anhydrase nanogel against denaturation and aggregation at high temperature

A two-step procedure to encapsulate a single bovine carbonic anhydrase (BCA) molecule into a spherical nanogel was proposed. BCA was reacted first with N-acryloxysuccinimide to introduce surface vinyl groups, followed by in-situ aqueous polymerization. Characterization of the nanogel by dynamic light scattering, transmission electron microscopy, and atomic force microscopy confirmed that each nanogel contained a single BCA molecule. The encapsulated BCA maintained 70% of the activity of its free counterpart, but exhibited an increase in the molten temperature from 64 to 81 degrees C demonstrated by differential scanning calorimetry and an extension of the half-life from less than 3 to over 90 min at 75 degrees C. Circular dichroism spectroscopy indicated that the encapsulation and the multi-point covalent linkage between BCA and the polymer shell strengthened the secondary structure and thus inhibited the aggregation at high temperature. The uniform BCA nanogel with enhanced structural stability against denaturation and aggregation expands the applications of BCA catalysis, particularly those carried out at high temperatures.     

Frequency modulation atomic force microscopy reveals individual intermediates associated with each unfolded I27 titin domain

In this study, we apply a dynamic atomic force microscopy (AFM) technique, frequency modulation (FM) detection, to the mechanical unfolding of single titin I27 domains and make comparisons with measurements made using the AFM contact or static mode method. Static mode measurements revealed the well-known force transition occurring at 100-120 pN in the first unfolding peak, which was less clear, or more often absent, in the subsequent unfolding peaks. In contrast, some FM-AFM curves clearly resolved a force transition associated with each of the unfolding peaks irrespective of the number of observed unfolded domains. As expected for FM-AFM, the frequency shift response of the main unfolding peaks and their intermediates could only be detected when the oscillation amplitudes used were smaller than the interaction lengths being measured. It was also shown that the forces measured for the dynamical interaction of the FM-AFM technique were significantly lower than those measured using the static mode. This study highlights the potential for using dynamic AFM for investigating biological interactions, including protein unfolding and the detection of novel unfolding intermediates.     

Viscoelastic study of the mechanical unfolding of a protein by AFM

We have applied a dynamic force modulation technique to the mechanical unfolding of a homopolymer of immunoglobulin (Ig) domains from titin, (C47S C63S I27)5, [(I27)5] to determine the viscoelastic response of single protein molecules as a function of extension. Both the stiffness and the friction of the homopolymer system show a sudden decrease when a protein domain unfolds. The decrease in measured friction suggests that the system is dominated by the internal friction of the (I27)5 molecule and not solvent friction. In the stiffness-extension spectrum we detected an abrupt feature before each unfolding event, the amplitude of which decreased with each consecutive unfolding event. We propose that these features are a clear indication of the formation of the known unfolding intermediate of I27, which has been observed previously in constant velocity unfolding experiments. This simple force modulation AFM technique promises to be a very useful addition to constant velocity experiments providing detailed viscoelastic characterization of single molecules under extension.     

Mechanical unfolding of TNfn3: the unfolding pathway of a fnIII domain probed by protein engineering, AFM and MD simulation

Protein engineering Phi-value analysis combined with single molecule atomic force microscopy (AFM) was used to probe the molecular basis for the mechanical stability of TNfn3, the third fibronectin type III domain from human tenascin. This approach has been adopted previously to solve the forced unfolding pathway of a titin immunoglobulin domain, TI I27. TNfn3 and TI I27 are members of different protein superfamilies and have no sequence identity but they have the same beta-sandwich structure consisting of two antiparallel beta-sheets. TNfn3, however, unfolds at significantly lower forces than TI I27. We compare the response of these proteins to mechanical force. Mutational analysis shows that, as is the case with TI I27, TNfn3 unfolds via a force-stabilised intermediate. The key event in forced unfolding in TI I27 is largely the breaking of hydrogen bonds and hydrophobic interactions between the A' and G-strands. The mechanical Phi-value analysis and molecular dynamics simulations reported here reveal that significantly more of the TNfn3 molecule contributes to its resistance to force. Both AFM experimental data and molecular dynamics simulations suggest that the rate-limiting step of TNfn3 forced unfolding reflects a transition from the extended early intermediate to an aligned intermediate state. As well as losses of interactions of the A and G-strands and associated loops there are rearrangements throughout the core. As was the case for TI I27, the forced unfolding pathway of TNfn3 is different from that observed in denaturant studies in the absence of force.     

Origin of mechanical strength of bovine carbonic anhydrase studied by molecular dynamics simulation

The forced unfolding process of bovine carbonic anhydrase II (BCA II) was examined at the atomic level by the molecular dynamics (MD) simulation. By force spectroscopy, experimentally obtained force-extension curves (F-E curves) showed a prominent force peak after 50 nm extension. F-E curves obtained from our simulation had three force peaks appearing after extensions of 10-17 nm, 40 nm, and 53 nm, each signifying a brittle fracture of a specific local structure. Upon undergoing the final fracture at 53 nm of extension, the entire molecule became a single flexible chain and was further extended to its full theoretical length, almost as a random coil. This feature of the 53-nm peak strongly suggested its close correspondence to the experimentally observed force peak at approximately 60-nm extension. The 53-nm peak in the molecular dynamics simulation corresponded to the unfolding process of the beta-sheeted core that includes zinc-coordinating histidine residues. These results suggest that the structural change occurring at 50-60 nm in atomic force microscopy experiments corresponded to the destruction of the zinc coordination site.     

Single molecule mechanical properties of type II collagen and hyaluronan measured by optical tweezers

Type II collagen and hyaluronan are the two major components of extracellular molecules in cartilage and play an important role in mechanical functions of extracellular matrix. Currently, their mechanical properties have been investigated only at the gross-level. In this study, the mechanical properties of single type II collagen and hyaluronan molecules were directly measured using optical tweezers technique. The persistence length was found to be 11.2+/-8.4 nm in type II collagen and 4.5+/-1.2 nm in hyaluronan. This result suggested that type II collagen is stiffer than hyaluronan at the individual molecule level, which supports the general concept that collagen is responsible for resisting tensile force. The experimental system developed here also provides a powerful tool for quantifying mechanical properties of extracellular matrix at the single molecule level.     

Nanobiomechanics of proteins and biomembrane

A review of the work done in the Laboratory of Biodynamics of Tokyo Institute of Technology in the last decade has been summarized in this article in relation to the results reported from other laboratories. The emphasis here is the application of nanomechanics based on the force mode of atomic force microscopy (AFM) to proteins and protein-based biological structures. Globular proteins were stretched in various ways to detect the localized rigidity inside of the molecule. When studied by this method, bovine carbonic anhydrase II (BCA II), calmodulin and OspA protein all showed the presence of localized rigid structures inside the molecules. Protein compression experiments were done on BCA II to obtain an estimate of the Young modulus and its change in the process of denaturation. Then, the AFM probe method was turned on to cell membranes and cytoplasmic components. Force curves accompanying the extraction process of membrane proteins from intact cells were analysed in relation to their interaction with the cytoskeletal components. By pushing the AFM probe further into the cytoplasm, mRNAs were recovered from a live cell with minimal damage, and multiplied using PCR technology for their identification. Altogether, the work introduced here forms the basis of nanomechanics of protein and protein-based biostructures and application of the nanomechanical technology to cell biology.     

Passive properties of the diaphragm in COPD.

Structural adaptations that occur in the diaphragm muscle of patients with chronic obstructive pulmonary disease (COPD), namely an increase in type I fibers and a decrease in type II fibers, have been explored in terms of the active contractile properties of the diaphragm. The aim of this study was to test the passive properties of the diaphragm by measuring the force response of relaxed diaphragm muscle fibers to stretching to determine the effect of COPD on these properties. Costal diaphragm biopsies were taken from patients with COPD and from controls with normal pulmonary function. From these biopsies, titin expression was assessed in diaphragm homogenates by gel electrophoresis, and the restoring force was measured by incremental stretching of single fibers in the relaxed state and measuring the force response to stretching. A quadratic model was used to illustrate the relationship between restoring force and muscle fiber length, and it revealed that COPD fibers generate significantly lower restoring forces than control fibers as judged by the area under the force-length curve. Furthermore, this finding applies to both type I and type II fibers. Gel electrophoresis revealed different titin isoforms in COPD and controls, consistent with the conclusion that COPD results not only in a change in muscle fiber-type distribution but in a structural change in the titin molecule in all muscle fiber types within the diaphragm. This may assist the muscle with the energetic changes in the length of the diaphragm required during breathing in COPD.     

Conformational changes and inactivation of bovine carbonic anhydrase II in 2,2,2-trifluoroethanol solutions

Changes in unfolding and enzymatic activity of bovine carbonic anhydrase II (BCA II) in different concentrations of 2,2,2-trifluoroethanol (TFE) were investigated by 1-anilino-8-naphthalenesulfonate (ANS) fluorescence emission spectra, far-UV CD spectra, and enzyme activity. The results showed that the activity and conformation of BCA II changed according to the concentration of TFE. Significant aggregation was observed when BCA II was denatured at TFE concentrations between 10 and 35% (v/v). When the concentration of TFE exceeded 40%, the aggregation of BCA II was not very obvious. The activity of BCA II decreased almost to zero as the TFE concentration reached 26%. The ANS fluorescence spectra indicated the tertiary conformations of BCA II were more stable in solutions with TFE concentrations lower than 15% (v/v) and higher than 40% (v/v). Far-UV CD spectra showed that high concentrations (higher than 25%) of TFE could induce BCA II to form more alpha-helix structures and caused these structures to be in relatively stable states. The native conformation of BCA II being destroyed after its inactivity indicated that the active sites of BCA II is situated in a limited region and has more flexibility than the whole enzyme molecule.     

Dynamic measurement of single protein's mechanical properties

Dimerized (tandemly repeated) protein was constructed, and the stretching force during the unfolding of the single protein molecule was measured using an atomic force microscope. In quasistatic measurements using normal force-distance curve measurements, each monomer unit was unfolded step by step. To elucidate the conformational state at each extension length, we measured the relax-stress response of the protein using short stroke sinusoidal movements of the sample stage. This allowed us to investigate the dynamic response of the protein repeatedly without full stretching or rupturing. Although the protein molecule responded in-phase to the applied movement in most cases, we found a novel out-of-phase response around the stretching length where the second monomer unit unfolded. Applying the spring constant measured in the quasistatic experiment, the out-of-phase response was reproduced in the simple calculation, which suggested the folding and the unfolding at the second monomer unit were taking place repeatedly during the relax-stress response measurement.     

Metal thiolate coordination in the E7 proteins of human papilloma virus 16 and cottontail rabbit papilloma virus as expressed in Escherichia coli.

The oncogenic E7 proteins of human papilloma virus (HPV 16) and of cottontail rabbit papilloma virus (CRPV) have been purified from an expression system in Escherichia coli. The proteins as purified from E. coli contain one tightly bound Zn(II) ion per molecule. The metal site shows facile exchange with either Cd(II) or Cu(I). The HPV 16 E7 maximally bound one Cd(II) or two Cu(I) ions, while the CRPV E7 bound two Cd(II) or three Cu(I) ions. The Cd(II) and Cu(I) E7 molecules exhibited optical transitions in the ultraviolet suggestive of metal:thiolate coordination. E7 proteins from HPV 16 and CRPV contain 7 and 8 cysteines/molecule, respectively. Reaction of the E7 proteins with the sulfhydryl reagent, dithiodipyridine, revealed that all the cysteinyl sulfurs are present in the reduced thiol state. Cu(I)-E7 molecules are luminescent with maximal emission at 570 nm. The observed emission at room temperature is indicative of metal coordination within a compact protein environment shielded from solvent interactions. The emission maxima occurs at the same wavelength (570 nm) as Cu(I)-cysteinyl sulfur clusters in Cu(I)-metallothioneins. The single Zn(II) atom in each protein can be removed from E7 in the presence of EDTA. The resulting apoE7 molecules remain soluble and can be partially reconstituted with Cd(II) to regain the ultraviolet charge transfer transitions.     

Mechanical restitution at different temperatures in papillary muscles from rabbit, rat, and hedgehog

Mechanical restitution curves, i.e., peak isometric force as a function of the duration of the preceding test interval, were investigated in papillary muscles from rabbit, rat, and hedgehog. Peak force of rabbit papillary muscle increased with prolongation of the test interval from about 0.3 s to about 1.0 s and for longer intervals peak force declined (called type I mechanical restitution). On the other hand, in rat and hedgehog, papillary muscles' force reached a maximum value at intervals of 30-120 s (called type II mechanical restitution). When temperature was decreased from 35 to 15 degrees C, maximum force of type I mechanical restitution shifted from 1.0 to 10 s, whereas maximum force of type II restitution did not change significantly. Type II mechanical restitution consisted of two different phases, designated phase A and phase B, respectively. As temperature was decreased from 35 to 0 degree C in the hedgehog preparation, the two phases became even more separated. At 35 degrees C, the rising part of mechanical restitution in the rabbit muscle could not be distinguished from phase A of the hedgehog preparation and was also very similar to phase A of the rat muscle. Phase A is thus present in both type I and type II mechanical restitution, but phase B is a special feature of type II mechanical restitution. Phase A and phase B might be a manifestation of activator calcium originating from two different sources, e.g., the sarcoplasmic reticulum and the sarcolemma.     

Conformational changes and inactivation of bovine carbonic anhydrase II in 2,2,2-Trifluoroethanol solutions

Changes in unfolding and enzymatic activity of bovine carbonic anhydrase II (BCA II) in different concentrations of 2,2,2-trifluoroethanol (TFE) were investigated by 1-anilino-8-naphthalenesulfonate (ANS) fluorescence emission spectra, far-UV CD spectra, and enzyme activity. The results showed that the activity and conformation of BCA II changed according to the concentration of TFE. Significant aggregation was observed when BCA II was denatured at TFE concentrations between 10 and 35% (v/v). When the concentration of TFE exceeded 40%, the aggregation of BCA II was not very obvious. The activity of BCA II decreased almost to zero as the TFE concentration reached 26%. The ANS fluorescence spectra indicated the tertiary conformations of BCA II were more stable in solutions with TFE concentrations lower than 15% (v/v) and higher than 40% (v/v). Far-UV CD spectra showed that high concentrations (higher than 25%) of TFE could induce BCA II to form more α-helix structures and caused these structures to be in relatively stable states. The native conformation of BCA II being destroyed after its inactivation indicated that the active site of BCA II is situated in a limited region and has more flexibility than the whole enzyme molecule.     

Conformations of cyclo(L-orD-Phe-L-Pro-Aca) and cyclo(L-Pro-L- or D-Phe-Aca). Cyclized dipeptide models for specific types of beta-bends

Conformational analyses on four cyclic model peptides of the beta-bend, cyclo(L- or D-Phe-L-Pro-epsilon-aminocaproyl(Aca] and cyclo(L-Pro-L- or D-Phe-Aca), were carried out both experimentally and theoretically. Cyclo(D-Phe-L-Pro-Aca) was shown to exist as a single conformer taking the type II' beta-bend. The comparison of its CD spectra with those of cyclo(L-Ala-L-Ala-Aca) revealed that type I and II' beta-bends, both with alpha-helix-like CD spectra, can be distinguished. Cyclo(L-Phe-L-Pro-Aca) was shown to exist as a single conformer with a cis L-Phe-L-Pro peptide bond, taking the type VI beta-bend. Its CD spectrum has thus been observed for the first time for the bend containing a cis peptide bond. Cyclo(L-Pro-L-Phe-Aca) was shown to exist as a mixture of two conformers, the major one taking the type I beta-bend with a trans Aca-L-Pro peptide bond and the minor one with a cis Aca-L-Pro peptide bond. Cyclo(L-Pro-D-Phe-Aca) was suggested to exist as a mixture of two conformers, the major one taking the type II beta-bend with a trans Aca-L-Pro peptide bond and the minor one with a cis Aca-L-Pro peptide bond.     

Locally disordered conformer of the hamster prion protein: a crucial intermediate to PrPSc?

A crucial step for transformation of the normal cellular isoform of the prion protein (PrP(C)) to the infectious prion protein (PrP(Sc)) is thought to entail a previously uncharacterized intermediate conformer, PrP*, which interacts with a template PrP(Sc) molecule in the conversion process. By carrying out (15)N-(1)H two-dimensional NMR measurements under variable pressure on Syrian hamster prion protein rPrP(90-231), we found a metastable conformer of PrP(C) coexisting at a population of approximately 1% at pH 5.2 and 30 degrees C, in which helices B and C are preferentially disordered. While the identity is still unproven, this observed metastable conformer is most logically PrP* or a closely related precursor. The structural characteristics of this metastable conformer are consistent with available immunological and pathological information about the prion protein.     

Chronotropic and inotropic dependence of the myocardium in patients with rheumatic heart disease before and after amiodarone treatment

Characteristic features of the electromechanical coupling of the myocardium were studied in patients with heart failure caused by rheumatic heart disease. Experiments were performed on muscle trabeculae isolated from the right atrial auricle in the course of surgical correction of a valve defect. The trabeculae displayed two types of mechanical responses, recorded in the isometric mode, to the postrest test. In the type I response, the mechanical restitution had an ascending pattern, the interval between electrical stimuli increasing. In type II, the mechanical restitution pattern was descending. Amiodarone (1 μM) treatment of the myocardium with the type I response enhanced the postrest potentiation of the mechanical response of trabeculae by more than 30%, but it had no effect on the muscles with the type II response. All patients whose biopsy material displayed the type II response had long episodes of atrial fibrillation. It is conceivable that the observed differences in the rhythm inotropic dependence of the human myocardium in rheumatic heart disease reflect different degrees of cardiomyocyte remodeling. The direction of this process is determined by the range of adaptive changes in intracellular structures, primarily, the sarcoplasmic reticulum.     

Mechanical Network in Titin Immunoglobulin from Force Distribution Analysis

The role of mechanical force in cellular processes is increasingly revealed by single molecule experiments and simulations of force-induced transitions in proteins. How the applied force propagates within proteins determines their mechanical behavior yet remains largely unknown. We present a new method based on molecular dynamics simulations to disclose the distribution of strain in protein structures, here for the newly determined high-resolution crystal structure of I27, a titin immunoglobulin (IG) domain. We obtain a sparse, spatially connected, and highly anisotropic mechanical network. This allows us to detect load-bearing motifs composed of interstrand hydrogen bonds and hydrophobic core interactions, including parts distal to the site to which force was applied. The role of the force distribution pattern for mechanical stability is tested by in silico unfolding of I27 mutants. We then compare the observed force pattern to the sparse network of coevolved residues found in this family. We find a remarkable overlap, suggesting the force distribution to reflect constraints for the evolutionary design of mechanical resistance in the IG family. The force distribution analysis provides a molecular interpretation of coevolution and opens the road to the study of the mechanism of signal propagation in proteins in general.     

Mechanical recruitment of N- and C-crosslinks in collagen type I

Collagen type I is an extracellular matrix protein found in connective tissues such as tendon, ligament, bone, skin, and the cornea of the eyes, where it functions to provide tensile strength; it also serves as a scaffold for cells and other extracellular matrix components. A single collagen type I molecule is composed of three amino acid chains that form a triple helix for most of the molecule's length; non-triple-helical extensions called N- and C-telopeptides are located at the amino/N-terminal and carboxy/C-terminal ends of the molecule, respectively. In two of the three chains, the C-telopeptide has been reported to possess a hair-pin/hook conformation, while the three N-telopeptides display a more extended structure. These telopeptides are crucial for the formation of enzymatic covalent crosslinks that form in collagens near their N- and C-ends. Such crosslinks provide structural integrity, strength, and stiffness to collagenous tissues. However, deformation mechanisms of N- and C-crosslinks and functional roles for the N- and C-telopeptide conformations are not yet well known. By performing molecular dynamics simulations, we demonstrated that two dehydro-hydroxylysino-norleucine crosslinks, positioned at the N- and C-crosslinking sites, exhibited a two-stage response to the mechanical deformation of their parent molecules. We observed that the N-crosslink served as the first responder to mechanical deformation, followed by the C-crosslink. The results of our simulations suggest a mechanical recruitment mechanism for N- and C-crosslinks. Understanding this mechanism will be crucial for the development of larger-scale predictive models of the mechanical behavior of native collagenous tissues, engineered tissues, and collagen-based materials.