Mechanical Stress Decreases the Amplitude of Twisting and Bending Fluctuations of Actin Filaments.

A variety of biological roles of mechanical forces have been proposed in cell biology, such as cell signaling pathways for survival, development, growth, and differentiation. Mechanical forces alter the mechanical conditions within cells and their environment, which strongly influences the reorganization of the actin cytoskeleton. Single-molecule imaging studies of actin filaments have led to the hypothesis that the actin filament acts as a mechanosensor; e.g., increases in actin filament tension alter their conformation and affinity for regulatory proteins. However, our understanding of the molecular mechanisms underlying how tension modulates the mechanical behavior of a single actin filament is still incomplete. In this study, a direct measurement of the twisting and bending of a fluorescently labeled single actin filament under different tension levels by force application (0.8-3.4 pN) was performed using single-molecule fluorescence polarization (SMFP) microscopy. The results showed that the amplitude of twisting and bending fluctuations of a single actin filament decreased with increasing tension. Electron micrograph analysis of tensed filaments also revealed that the fluctuations in the crossover length of actin filaments decreased with increasing filament tension. Possible molecular mechanisms underlying these results involving the binding of actin-binding proteins, such as cofilin, to the filament are discussed.

A cryo-TSEM with temperature cycling capability allows deep sublimation of ice to uncover fine structures in thick cells.

The scanning electron microscope (SEM) has been reassembled into a new type of cryo-electron microscope (cryo-TSEM) by installing a new cryo-transfer holder and anti-contamination trap, which allowed simultaneous acquisition of both transmission images (STEM images) and surface images (SEM images) in the frozen state. The ultimate temperatures of the holder and the trap reached - 190 °C and - 210 °C, respectively, by applying a liquid nitrogen slush. The STEM images at 30 kV were comparable to, or superior to, the images acquired with conventional transmission electron microscope (100 kV TEM) in contrast and sharpness. The unroofing method was used to observe membrane cytoskeletons instead of the frozen section and the FIB methods. Deep sublimation of ice surrounding unroofed cells by regulating temperature enabled to emerge intracellular fine structures in thick frozen cells. Hence, fine structures in the vicinity of the cell membrane such as the cytoskeleton, polyribosome chains and endoplasmic reticulum (ER) became visible. The ER was distributed as a wide, flat structure beneath the cell membrane, forming a large spatial network with tubular ER.

D-Loop Mutation G42A/G46A Decreases Actin Dynamics.

Depolymerization and polymerization of the actin filament are indispensable in eukaryotes. The DNase I binding loop (D-loop), which forms part of the interface between the subunits in the actin filament, is an intrinsically disordered loop with a large degree of conformational freedom. Introduction of the double mutation G42A/G46A to the D-loop of the beta cytoskeletal mammalian actin restricted D-loop conformational freedom, whereas changes to the critical concentration were not large, and no major structural changes were observed. Polymerization and depolymerization rates at both ends of the filament were reduced, and cofilin binding was inhibited by the double mutation. These results indicate that the two glycines at the tip of the D-loop are important for actin dynamics, most likely by contributing to the large degree of conformational freedom.

Dynamic Properties of Human α-Synuclein Related to Propensity to Amyloid Fibril Formation.

α-Synuclein (αSyn) is an intrinsically disordered protein that can form amyloid fibrils. Fibrils of αSyn are implicated with the pathogenesis of Parkinson's disease and other synucleinopathies. Elucidating the mechanism of fibril formation of αSyn is therefore important for understanding the mechanism of the pathogenesis of these diseases. Fibril formation of αSyn is sensitive to solution conditions, suggesting that fibril formation of αSyn arises from the changes in its inherent physico-chemical properties, particularly its dynamic properties because intrinsically disordered proteins such as αSyn utilize their inherent flexibility to function. Characterizing these properties under various conditions should provide insights into the mechanism of fibril formation. Here, using the quasielastic neutron scattering and small-angle x-ray scattering techniques, we investigated the dynamic and structural properties of αSyn under the conditions, where mature fibrils are formed (pH 7.4 with a high salt concentration), where clumping of short fibrils occurs (pH 4.0), and where fibril formation is not completed (pH 7.4). The small-angle x-ray scattering measurements showed that the extended structures at pH 7.4 with a high salt concentration become compact at pH 4.0 and 7.4. The quasielastic neutron scattering measurements showed that both intra-molecular segmental motions and local motions such as side-chain motions are enhanced at pH 7.4 with a high salt concentration, compared to those at pH 7.4 without salt, whereas only the local motions are enhanced at pH 4.0. These results imply that fibril formation of αSyn requires not only the enhanced local motions but also the segmental motions such that proper inter-molecular interactions are possible.

Facile preparation of optically active jasmonates and their biological activities in rice.

A facile and efficient method has been developed for the optical resolution of racemic jasmonic acid (JA) on a relatively large scale and was successfully utilized for the preparation of optically pure (+)-JA and (-)-JA. We indicated that (+)-JA has lower growth inhibitory activity than (-)-JA in the rice seedling growth test and confirmed in line with an earlier observation that their respective biologically-active forms, (+)-JA-Ile and (-)-JA-Ile, show comparable inhibitory activities. We compared the metabolism of (+)-JA and (-)-JA into (+)-JA-Ile and (-)-JA-Ile, respectively, in the JA-deficient rice cpm2, and found that the exogenously applied (+)-JA was metabolized to the corresponding Ile conjugate less efficiently as compared with (-)-JA. Such metabolic rate difference may cause a discrepancy between biological potencies of (+)-JA and (-)-JA in rice. Abbreviations: FW: fresh weight; Ile: isoleucine; JA: jasmonic acid; JA-Ile: jasmonoyl-l-isoleucine; LC-ESI-MS/MS: liquid chromatography and electrospray ionization tandem mass spectrometry; MeJA: methyl jasmonate; OPDA: 12-oxophytodienoic acid.

Direct observation of the actin filament by tip-scan atomic force microscopy.

Actin filaments, the actin-myosin complex and the actin-tropomyosin complex were observed by a tip-scan atomic force microscope (AFM), which was recently developed by Olympus as the AFM part of a correlative microscope. This newly developed AFM uses cantilevers of similar size as stage-scan AFMs to improve substantially the spatial and temporal resolution. Such an approach has previously never been possible by a tip-scan system, in which a cantilever moves in the x, y and z directions. We evaluated the performance of this developed tip-scan AFM by observing the molecular structure of actin filaments and the actin-tropomyosin complex. In the image of the actin filament, the molecular interval of the actin subunits (∼5.5 nm) was clearly observed as stripes. From the shape of the stripes, the polarity of the actin filament was directly determined and the results were consistent with the polarity determined by myosin binding. In the image of the actin-tropomyosin complex, each tropomyosin molecule (∼2 nm in diameter) on the actin filament was directly observed without averaging images of different molecules. Each tropomyosin molecule on the actin filament has never been directly observed by AFM or electron microscopy. Thus, our developed tip-scan AFM offers significant potential in observing purified proteins and cellular structures at nanometer resolution. Current results represent an important step in the development of a new correlative microscope to observe nm-order structures at an acceptable frame rate (∼10 s/frame) by AFM at the position indicated by the fluorescent dye observed under a light microscope.

Proper calibration of ultrasonic power enabled the quantitative analysis of the ultrasonication-induced amyloid formation process.

To elucidate the mechanisms of ultrasonication on the amyloid fibril formation, we quantitatively determined the ultrasonic power using both calorimetry and potassium iodide (KI) oxidation, and under the properly calibrated ultrasonic power, we investigated the ultasonication-induced amyloid formation process of the mouse prion protein (mPrP(23-231)). These methods revealed that the ultrasonic power in our system ranged from 0.3 to 2.7 W but entirely dependent on the positions of the ultrasonic stage. Intriguingly, the nucleation time of the amyloid fibrils was found to be shortened almost proportionally to the ultrasonic power, indicating that the probability of the occurrence of nucleus formation increases proportionally to the ultrasonic power. Moreover, mPrP(23-231) formed two types of aggregates: rigid fibrils and short fibrils with disordered aggregates, depending on the ultrasonic power. The nucleation of rigid fibrils required an ultrasonic power larger than 1.5 W. While at the strong ultrasonic power larger than 2.6 W, amyloid fibrils were formed early, but simultaneously fine fragmentation of fibrils occurred. Thus, an ultrasonic power of approximately 2.0 W would be suitable for the formation of rigid mPrP(23-231) fibrils under the conditions utilized (ultrasonication applied for 30 s every 9 min). As ultrasonication has been widely used to amplify the scrapie form of the prion protein, or other amyloids in vitro, the calorimetry and KI oxidation methods proposed here might help determining the adequate ultrasonic powers necessary to amplify them efficiently.

Cold destabilization and temperature jump of the murine prion protein mPrP(23-231).

We analyzed the thermal stability of the recombinant murine prion protein mPrP(23-231) with a single tryptophan mutation (F174W) and its perturbation by cold temperature. Compared to the N-terminally truncated ones, full-length construct is significantly unstable and forms intermediate state of urea denaturation, and also undergoes the cold destabilization under the ambient pressure. In order to detect the very early phase of the folding, we also applied a laser-induced temperature jump kinetic measurement and observed a kinetic phase of several microseconds, suggesting the barrierless folding process. The conformational instability and low barriers between different conformers may explain the unusual flexibility leading to the pathogenic conversion and the strain diversity.

Critical region for amyloid fibril formation of mouse prion protein: unusual amyloidogenic properties of the helix 2 peptide.

To gain insight into the structural mechanism of the conformational conversion process of prion, we examined the potential amyloidogenic property of each secondary structural element in a mouse prion protein (mPrP) and discriminated their relative significance for the formation of amyloid fibrils. Although peptides corresponding to alpha-helix 2 and alpha-helix 3 (named H2 peptide and H3 peptide, respectively) formed the amyloid-like fibrils, their structures were quite different. H2 fibrils formed the ordered beta-sheet with the beta-turn conformation, and the resultant fibrils were long and straight. In contrast, H3 fibrils consisted of the beta-sheet with the random conformation, and the resultant fibrils were short and flexible. These properties are basically consistent with their hydrophobicity and beta-strand propensity profiles. To examine the cross reactivity between peptide fragments and full-length mPrP, we then carried out seeding experiments. While H2 seeds induced the formation of fibrils of full-length mPrP as quickly as full-length mPrP seeds, H3 seeds exhibited a long lag time. This implies that the region of alpha-helix 2 rather than alpha-helix 3 in mPrP has great potential for initiating fibril formation. As a whole, the alpha-helix 2 region would be crucial for the nucleation-dependent replication process of the prion protein.

Hot spots in prion protein for pathogenic conversion.

Prion proteins are key molecules in transmissible spongiform encephalopathies (TSEs), but the precise mechanism of the conversion from the cellular form (PrP(C)) to the scrapie form (PrP(Sc)) is still unknown. Here we discovered a chemical chaperone to stabilize the PrP(C) conformation and identified the hot spots to stop the pathogenic conversion. We conducted in silico screening to find compounds that fitted into a "pocket" created by residues undergoing the conformational rearrangements between the native and the sparsely populated high-energy states (PrP*) and that directly bind to those residues. Forty-four selected compounds were tested in a TSE-infected cell culture model, among which one, 2-pyrrolidin-1-yl-N-[4-[4-(2-pyrrolidin-1-yl-acetylamino)-benzyl]-phenyl]-acetamide, termed GN8, efficiently reduced PrP(Sc). Subsequently, administration of GN8 was found to prolong the survival of TSE-infected mice. Heteronuclear NMR and computer simulation showed that the specific binding sites are the A-S2 loop (N159) and the region from helix B (V189, T192, and K194) to B-C loop (E196), indicating that the intercalation of these distant regions (hot spots) hampers the pathogenic conversion process. Dynamics-based drug discovery strategy, demonstrated here focusing on the hot spots of PrP(C), will open the way to the development of novel anti-prion drugs.

SAXSANA: an interactive program for the analysis and monitoring of static and time-resolved small-angle X-ray solution scattering measurements.

An interactive analytical program, SAXSANA, for small-angle X-ray scattering measurements of solutions is described. The program processes scattered data without disciplined knowledge of small-angle scattering. SAXSANA also assists in finding the best experimental conditions, thus avoiding blind runs of experiments. SAXSANA consists of the following procedures: (i) determination of the centre of scattered X-rays and moment transfer Q (Q = 4pisintheta/lambda, where 2theta is the scattering angle and lambda is the wavelength) for each measured channel; (ii) conversion of the data format to the format of Q versus scattered intensities J(Q); (iii) truncation of unnecessary data and smoothing of scattering curves by cubic-spline function; (iv) correction of the absorption effect and subtraction of the scattered intensity of the buffer (solvent) solution from that of the sample solution; (v) creation of a data file for a three-dimensional representation of time-resolved scattering curves; (vi) determination of radii of gyration by Guinier plots; (vii) determination of persistent lengths by Kratky plots; (viii) extrapolation of the small-angle part by Guinier plots; (ix) extrapolation of the wide-angle part by Porod's & Luzzati's laws for the Hankel transformation in order to obtain the distance distribution function p(r); (x) calculation of p(r) and computation of the invariant, the chord length, the Volume, the spherical radius, the maximum dimension D(max) and the radius of gyration (Rg). SAXSANA also serves as an on-site monitor for the validity of an experimental result during the measurements.