Weakly bound water molecules shorten single-stranded DNA

In this paper, we measure the single chain elasticity of an oligomer single-stranded DNA (ssDNA) in both aqueous and nonaqueous, apolar liquid environments by AFM-based single molecule force spectroscopy. We find a marked deviation between the force-extension relations recorded for the two conditions. This difference is attributed to the additional energy required to break the H-bond-directed water bridges around the ssDNA chain in aqueous solutions, which are nonexistent in organic solvents. The results obtained in 8 M guanidine-HCl solution provide more evidence that water bridges around ssDNA originate the observed deviation. On the basis of the results obtained by an ab initio quantum mechanics calculation, a parameter-free freely rotating chain model is proposed. We find that this model is in perfect agreement with the experimental force-extension curve obtained in organic solvents, which further corroborates our assumption. On the basis of the experimental results, it is suggested that the weak H-bonding between ssDNA and water molecules may be a precondition for stable double-stranded DNA to exist in water.     

The behavior of cellulose molecules in aqueous environments

Molecular motions of cellulose chains in aqueous environments were investigated by comparison with those in non-aqueous environments using molecular simulation techniques. The cellulose chains under non-aqueous conditions approached each other closely and then made tight aggregates that were formed by direct hydrogen bonding. Those in aqueous environments, such as in a bio-system, were separated from each other by water molecules and did not have direct hydrogen bonding between the cellulose chain molecules. Folded-chain structures were not found in either aqueous or non-aqueous environments that were somewhat crowded. In the aqueous system, the water molecules around the cellulose chains restricted their molecular motions and interrupted formation of direct, interchain hydrogen bonds. In the non-aqueous system, the cellulose chains approached each other closely and then made a tight cluster before the chain molecules could wind and bend. It was concluded that a very dilute solution of cellulose molecules in appropriate solvents is necessary to create folded-chain or random-coiled structures. We also confirmed that the driving force for making tight clusters of cellulose molecules in highly concentrated solutions is the energy of the hydrogen bonding created directly between the hydroxyl groups of the cellulose chains. These results strongly suggest that hydrogen bonding plays a very important role in the characteristics of cellulose molecules.     

The role of hydrophobic surfaces in altering water-mediated peptide-peptide interactions in an aqueous environment

Using Born-Oppenheimer molecular dynamics within the density functional framework, we calculated the effective force acting on water-mediated peptide-peptide interaction between antiparallel β-sheets in an aqueous environment and also in the vicinity of a hydrophobic surface. From the magnitude of the effective force (corresponding to the slope of the free energy as a function of the interpeptide distance) and its sign (a negative value indicates an effective attraction, whereas a positive value indicates an effective repulsion) we can elucidate the fundamental differences of the water-mediated peptide-peptide interactions in those two environments. The computed effective forces indicate that the water-mediated interaction between peptides in an aqueous environment is attractive in the range of interpeptide distance d = 7-8 ? when hydrophobic surfaces are not nearby. Due to the stabilization of the water molecules bridging between the two β-sheets, a free energy barrier exists between the direct and indirect (water-mediated) interpeptide interactions. However, when the peptides are in the proximity of hydrophobic surfaces, this free energy barrier decreases because the hydrophobic surfaces enhance the interpeptide attraction by the destabilization and ease-to-libration of the bridging water molecules between them.     

The determination of work of compression of protein monolayers at the air-water interface

Summary In the present study, monolayers of various proteins were investigated at the air-water interface. The work of compression,W _c (Helmholtz free energy) has been determined from the surface pressure-area compression isotherms. A linear relationship was found betweenW _c and the amount of protein present at the surface. Further, it is shown that this relation holds both for completely unfolded (Bovine-serum-albumin, Ovalbumin) and for incompletely unfolded (Transferrin, Myoglobin) proteins.β-Lipoprotein isotherms also gave a similar dependence. It is further shown that the amount of protein lost into the subphase can be determined from a plot ofW _c versus protein added at the interface. The results are discussed in relation to the constitution of protein molecules at the surface.     

De novo refolding and aggregation of insulin in a nonaqueous environment: an inside out protein remake

While thermodynamic penalties associated with protein-water interactions are the key driving force of folding, perturbed hydration of destabilized protein molecules may trigger aggregation, which in vivo often causes cellular and histological damage. Here we show, that the denatured state of an alpha-helical protein, insulin, converts to a non-native beta-sheet-rich structure upon de novo "refolding" in an anhydrous environment. The beta-pleated conformer precipitates from solutions of DMSO-denatured insulin upon dilution with chloroform. DMSO destroys hydrogen bond network of the native protein acting as a strong acceptor of main chain hydrogen bonds. Upon the addition of chloroform, which is a weak hydrogen bond donor per se, competitive hydrogen bonds between DMSO and chloroform are formed. This leads to the release of unfolded insulin molecules. In the absence of water, the imminent saturation of polypeptide's dandling hydrogen bonds does not produce the native and predominantly alpha-helical state but a beta-sheet-rich structure, which is morphologically and spectrally distinct from insulin amyloid fibrils. Unlike insulin fibrils, the beta-sheet conformer is metastable and refolds spontaneously to the native form in an aqueous environment. This implies that "folding" in the absence of water results in inefficient burial of hydrophobic side-chains, and thermodynamic frustration at the water-protein interface.     

Tandem repeating modular proteins avoid aggregation in single molecule force spectroscopy experiments

We have used single molecule force spectroscopy to explore the unfolding and refolding behavior of the immunoglobulin-like I27 protein in aqueous 2,2,2-trifluoroethanol (TFE). In bulk solution experiments, a 28% v/v TFE solution has previously been observed to enhance intermolecular attractions and lead to misfolding and aggregation of tandem modular proteins of high sequence identity. In our single molecule experiments, however, we measure successful refolding of the polyprotein I27(8) in all TFE solutions up to 35% v/v. Using a single molecule micromanipulation technique, we have shown that refolding of a polyprotein with identical repeats is not hindered by the presence of this cosolvent. These experimental results provide new insight into the properties of tandem repeating proteins and raise interesting questions as to the evolutionary success of such proteins in avoiding misfolding and aggregation.     

Understanding cold denaturation: the case study of Yfh1

All globular proteins undergo transitions from their native to unfolded states if exposed either to cold or to heat perturbation. While the heat-induced transition is well described for a large number of proteins, in media compatible with natural environments, the limited number of examples of cold denatured states concern proteins artificially destabilized, for instance, by the presence of denaturants, ad hoc point mutations, or both. Here, we provide a characterization of the low temperature unfolded state of Yfh1, a natural protein that undergoes cold denaturation around water freezing temperature, in the absence of any denaturant. By achieving nearly full assignment of the NMR spectrum, we show that at -1 °C, Yfh1 has all the features of an unfolded protein, although retaining some local, residual secondary structure. The effect is not uniform along the sequence and does not merely reflect the secondary structural features of the folded species. The N-terminus seems to be dynamically more flexible, although retaining some nascent helix character. Interestingly, this region is the one containing functionally important hot-spots. The β-sheet region and the C-terminal helix are completely unfolded, although experiencing some conformational exchange, partly due to the presence of several prolines. Ours is the first step toward a full characterization of the low temperature unfolded state of a natural protein, reached without the aid of any destabilizing agent. We discuss the implications of our findings for understanding cold denatured states.     

Topography of the free-energy landscape probed via mechanical unfolding of proteins

Single-molecule experiments in which proteins are unfolded by applying mechanical stretching forces generally force unfolding to proceed along a reaction coordinate that is different from that in chemical or thermal denaturation. Here we simulate the mechanical unfolding and refolding of a minimalist off-lattice model of the protein ubiquitin to explore in detail the slice of the multidimensional free-energy landscape that is accessible via mechanical pulling experiments. We find that while the free-energy profile along typical "chemical" reaction coordinates may exhibit two minima, corresponding to the native and denatured states, the free energy G(z) is typically a monotonic function of the mechanical coordinate z equal to the protein extension. Application of a stretching force along z tilts the free-energy landscape resulting in a bistable (or multistable) free energy G(z)-fz probed in mechanical unfolding experiments. We construct a two-dimensional free-energy surface as a function of both chemical and mechanical reaction coordinates and examine the coupling between the two. We further study the refolding trajectories after the protein has been prestretched by a large force, as well as the mechanical unfolding trajectories in the presence of a large stretching force. We demonstrate that the stretching forces required to destabilize the native state thermodynamically are larger than those expected on the basis of previous experimental estimates of G(z). This finding is consistent with the recent experimental studies, indicating that proteins may refold even in the presence of a substantial stretching force. Finally, we show that for certain temperatures the free energy of a polyprotein chain consisting of multiple domains is a linear function of the chain extension. We propose that the recently observed "slow phase" in the refolding of proteins under mechanical tension may be viewed as downhill diffusion in such a linear potential.     

Mechanical Deformation Accelerates Protein Ageing

A hallmark of tissue ageing is the irreversible oxidative modification of its proteins. We show that single proteins, kept unfolded and extended by a mechanical force, undergo accelerated ageing in times scales of minutes to days. A protein forced to be continuously unfolded completely loses its ability to contract by folding, becoming a labile polymer. Ageing rates vary among different proteins, but in all cases they lose their mechanical integrity. Random oxidative modification of cryptic side chains exposed by mechanical unfolding can be slowed by the addition of antioxidants such as ascorbic acid, or accelerated by oxidants. By contrast, proteins kept in the folded state and probed over week‐long experiments show greatly reduced rates of ageing. We demonstrate a novel approach whereby protein ageing can be greatly accelerated: the constant unfolding of a protein for hours to days is equivalent to decades of exposure to free radicals under physiological conditions.     

Exploring protein structure and dynamics under denaturing conditions by single-molecule FRET analysis

Proteins are highly complex biopolymers, exhibiting a substantial degree of structural variability in their properly folded, native state. In the presence of denaturants, this heterogeneity is greatly enhanced, and fluctuations take place among vast numbers of folded and unfolded conformations via many different pathways. To better understand protein folding it is necessary to explore the structural and energetic properties of the folded and unfolded polypeptide chain, as well as the trajectories along which the chain navigates through its multi-dimensional conformational energy landscape. In recent years, single-molecule fluorescence spectroscopy has been established as a powerful tool in this research area, as it allows one to monitor the structure and dynamics of individual polypeptide chains in real time with atomic scale resolution using F?rster resonance energy transfer (FRET). Consequently, time trajectories of folding transitions can be directly observed, including transient intermediates that may exist along these pathways. Here we illustrate the power of single-molecule fluorescence with our recent work on the structure and dynamics of the small enzyme RNase H in the presence of the chemical denaturant guanidinium chloride (GdmCl). For FRET analysis, a pair of fluorescent dyes was attached to the enzyme at specific locations. In order to observe conformational changes of individual protein molecules for up to several hundred seconds, the proteins were immobilized on nanostructured, polymer coated glass surfaces specially developed to have negligible interactions with folded and unfolded proteins. The single-molecule FRET analysis gave insight into structural changes of the unfolded polypeptide chain in response to varying the denaturant concentration, and the time traces revealed stepwise transitions in the FRET levels, reflecting conformational dynamics. Barriers in the free energy landscape of RNase H were estimated from the kinetics of the transitions.     

Raman spectroscopic characterization of secondary structure in natively unfolded proteins: alpha-synuclein

The application of Raman spectroscopy to characterize natively unfolded proteins has been underdeveloped, even though it has significant technical advantages. We propose that a simple three-component band fitting of the amide I region can assist in the conformational characterization of the ensemble of structures present in natively unfolded proteins. The Raman spectra of alpha-synuclein, a prototypical natively unfolded protein, were obtained in the presence and absence of methanol, sodium dodecyl sulfate (SDS), and hexafluoro-2-propanol (HFIP). Consistent with previous CD studies, the secondary structure becomes largely alpha-helical in HFIP and SDS and predominantly beta-sheet in 25% methanol in water. In SDS, an increase in alpha-helical conformation is indicated by the predominant Raman amide I marker band at 1654 cm(-1) and the typical double minimum in the CD spectrum. In 25% HFIP the amide I Raman marker band appears at 1653 cm(-1) with a peak width at half-height of approximately 33 cm(-1), and in 25% methanol the amide I Raman band shifts to 1667 cm(-1) with a peak width at half-height of approximately 26 cm(-1). These well-characterized structural states provide the unequivocal assignment of amide I marker bands in the Raman spectrum of alpha-synuclein and by extrapolation to other natively unfolded proteins. The Raman spectrum of monomeric alpha-synuclein in aqueous solution suggests that the peptide bonds are distributed in both the alpha-helical and extended beta-regions of Ramachandran space. A higher frequency feature of the alpha-synuclein Raman amide I band resembles the Raman amide I band of ionized polyglutamate and polylysine, peptides which adopt a polyproline II helical conformation. Thus, a three-component band fitting is used to characterize the Raman amide I band of alpha-synuclein, phosvitin, alpha-casein, beta-casein, and the non-A beta component (NAC) of Alzheimer's plaque. These analyses demonstrate the ability of Raman spectroscopy to characterize the ensemble of secondary structures present in natively unfolded proteins.     

Water dynamics at protein interfaces: ultrafast optical Kerr effect study

The behavior of water molecules surrounding a protein can have an important bearing on its structure and function. Consequently, a great deal of attention has been focused on changes in the relaxation dynamics of water when it is located at the protein surface. Here we use the ultrafast optical Kerr effect to study the H-bond structure and dynamics of aqueous solutions of proteins. Measurements are made for three proteins as a function of concentration. We find that the water dynamics in the first solvation layer of the proteins are slowed by up to a factor of 8 in comparison to those in bulk water. The most marked slowdown was observed for the most hydrophilic protein studied, bovine serum albumin, whereas the most hydrophobic protein, trypsin, had a slightly smaller effect. The terahertz Raman spectra of these protein solutions resemble those of pure water up to 5 wt % of protein, above which a new feature appears at ~80 cm(-1), which is assigned to a bending of the protein amide chain.     

聚N,N-二乙基丙烯酰胺低聚物水溶液的分子动力学研究

对50个单元构成的聚N,N-二乙基丙烯酰胺(PDEA)低聚物的水溶液体系进行了分子动力学的研究,分别模拟了300 K时的伸展链、310 K时的伸展链以及紧缩链与水构成的体系,对溶液中PDEA周围溶剂水分子的分布情况以及水分子形成氢键的情况进行了统计,结果表明在PDEA周围的水产生了比本体水更有序的结构,形成了更多的氢键,这种有序结构维持到第二水合层甚至更远.发生相分离后,PDEA与水分子形成的氢键大部分未被破坏,水合层中每个水分子形成的氢键数也没有明显变化,但水合层(形成有序结构的水分子)内水分子数目的减少使得总的氢键数目减少,从而造成体系能量增加及熵增加.同时还研究了聚合物及水分子的自扩散系数,表明PDEA影响周围水分子结构的同时,对水的动力学性质也产生了很大影响.     

Planar or nonplanar: what is the structure of urea in aqueous solution?

A combined quantum chemical statistical mechanical method has been used to study the solvation of urea in water, with emphasis on the structure of urea. The model system consists of three parts: a Hartree-Fock quantum chemical core, 99 water molecules described with a polarizable force-field, and a dielectric continuum. A free-energy profile along the transition of urea from planar to a nonplanar structure is calculated. This mode in aqueous solution is found to be floppy. That is, the structure of urea in water is not well-defined because the planar to nonplanar transition requires an energy of the order of the thermal energy at room temperature. We discuss the implications of this finding for simulation studies of urea in polar environments like water and proteins.     

Structure and dynamics of the solvation of bovine pancreatic trypsin inhibitor in explicit water: a comparative study of the effects of solvent and protein polarizability

To isolate the effects of the inclusion of polarizability in the force field model on the structure and dynamics of the solvating water in differing electrostatic environments of proteins, we present the results of molecular dynamics simulations of the bovine pancreatic trypsin inhibitor (BPTI) in water with force fields that explicitly include polarization for both the protein and the water. We use three model potentials for water and two model potentials for the protein. Two of the water models and one of the protein models are polarizable. A total of six systems were simulated representing all combinations of these polarizable and nonpolarizable protein and water force fields. We find that all six systems behave in a similar manner in regions of the protein that are weakly electrostatic (either hydrophobic or weakly hydrophilic). However, in the vicinity of regions of the protein with relatively strong electrostatic fields (near positively or negatively charged residues), we observe that the water structure and dynamics are dependent on both the model of the protein and the model of the water. We find that a large part of the dynamical dependence can be described by small changes in the local environments of each region that limit the local density of non-hydrogen-bonded waters, precisely the water molecules that facilitate the dynamical relaxation of the water-water hydrogen bonds. We introduce a simple method for rescaling for this effect. When this is done, we are able to effectively isolate the influence of polarizability on the dynamics. We find that the solvating water's relaxation is most affected when both the protein and the water models are polarizable. However, when only one model (or neither) is polarizable, the relaxation is similar regardless of the models used.     

Two-state folding observed in individual protein molecules

The folding dynamics of small proteins are often described in terms of a simple two-state kinetic model. Within this notion, the behavior of individual molecules is expected to be stochastic, with a protein molecule residing in either the unfolded or the folded state for extended periods of time, with intermittent rapid jumps across the free energy barrier. However, a direct observation of this bistable behavior has not been made to date. Rather, previous reports of folding trajectories of individual proteins have shown an unexpected degree of complexity. This raises the question whether the simple kinetic properties derived from classical experiments on large ensembles of molecules are reflected in the folding paths taken by individual proteins. Here we report single-molecule folding/unfolding trajectories observed by fluorescence resonance energy transfer for a protein that meets all criteria of a two state-system. The trajectories, measured on molecules immobilized in lipid vesicles, demonstrate the anticipated bistable behavior, with steplike transitions between folded and unfolded conformations. They further allow us to put an upper bound on the barrier crossing time.     

反渗透过程中双壁碳纳米管通水阻盐性能的分子动力学模拟

采用分子动力学模拟方法, 探究了非常规双壁碳纳米管(DWCNT)在反渗透过程中, 不同内外管间距对管道内水分子与盐离子运动行为的影响. 本文采用0.5 mol·L^-1氯化钠水溶液模拟海水, 内管始终采用CNT(8,8)型, 并对盐水层施加恒力模拟反渗透压. 重点考察盐离子数量分布与通水情况, 计算水分子平均力势, 并分析水分子氢键寿命与偶极矩分布. 结果表明, 管间距不仅影响上述各项性质, 还会改变盐离子与水分子在碳管中的渗透特性. 模拟结果显示, 小尺寸DWCNT可以有效实现盐水分离但水通量较小, 大尺寸DWCNT的水容量较大但阻盐效率不高, 而中尺寸DWCNT (即: 管间距为0.815 nm)则具有最佳的通水阻盐性能. 本文试图从分子层面揭示了DWCNT通水阻盐机理, 并为人们设计新型海水淡化渗透膜提供理论指导.     

Molecular dynamics simulations of end-to-end contact formation in hydrocarbon chains in water and aqueous urea solution

We probe the urea-denaturation mechanism using molecular dynamics simulations of an elementary "folding" event, namely, the formation of end-to-end contact in the linear hydrocarbon chain (HC) CH(3)(CH(2))(18)CH(3). Electrostatic effects are examined using a model HC in which one end of the chain is positively charged (+0.2e) and the other contains a negative charge (-0.2e). For these systems multiple transitions between "folded" (conformations in which the chain ends are in contact) and "unfolded" (end-to-end contact is broken) can be observed during 4 ns molecular dynamics simulations. In water and 6 M aqueous urea solution HC and the charged HC fluctuate between collapsed globular conformations and a set of expanded structures. The collapsed conformation adopted by the HC in water is slightly destablized in 6 M urea. In contrast, the end-to-end contact is disrupted in the charged HC only in aqueous urea solution. Despite the presence of a large hydrophobic patch, on length scales on the order of approximately 8-10 A "denaturation" (transition to the expanded unfolded state) occurs by a direct interaction of urea with charges on the chain ends. The contiguous patch of hydrophobic moieties leads to "mild dewetting", which becomes more pronounced in the charged HC in 6 M aqueous urea solution. Our simulations establish that the urea denaturation mechanism is most likely electrostatic in origin.     

The burial of solvent-accessible surface area is a predictor of polypeptide folding and misfolding as a function of chain elongation

The hydrophobic effect is a major driving force in all chemical and biological events involving chain collapse in aqueous solution. Here, we show that the burial of nonpolar solvent-accessible surface area (NSASA) is a powerful criterion to predict the folding and misfolding behavior of small single-domain proteins as a function of chain elongation. This bears fundamental implications for co- and post-translational protein folding in the cell and for understanding the interplay between noncovalent interactions and formation of native-like structure and topology. Comparison between the fraction of NSASA in fully unfolded and folded elongating chains shows that efficient burial of nonpolar surface area is preferentially achieved only when the polypeptide chain is almost complete. This effect has no preferential vectorial character in that it is present upon elongation from both the N and C termini. For incomplete chains that do not have the ability to fold and bury nonpolar surface intramolecularly, the overall hydrophobic nature of the polypeptide chain (expressed as FBA, i.e., fractional buried surface area per residue) dictates the tendency toward misfolding and self-association. N-terminal chains characterized by FBA exceeding 0.73 are likely to misfold and aggregate, if unable to fold intramolecularly.