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The investigation of common structural motifs provides additional information on why proteins conserve similar topologies yet may have non-conserved amino acid sequences. Proteins containing the ubiquitin superfold have similar topologies, although the sequence conservation is rather poor. Here, we present novel similarities and differences between the proteins ubiquitin and NEDD8. They have 57% identical sequence, almost identical backbone topology and similar functional strategy, although their physiological functions are mutually different. Using variable pressure NMR spectroscopy, we found that the two proteins have similar conformational fluctuation in the evolutionary conserved enzyme-binding region and contain a structurally similar locally disordered conformer (I) in equilibrium with the basic folded conformer (N). A notable difference between the two proteins is that the equilibrium population of I is far greater for NEDD8 (DeltaG(0)(NI)5 kJ/mol) than for ubiquitin (DeltaG(0)(NI)=15.2(+/-1.0) kJ/mol), and that the tendency for overall unfolding (U) is also far higher for NEDD8 (DeltaG(0)(NU)=11.0(+/-1.5) kJ/mol) than for ubiquitin (DeltaG(0)(NU)=31.3(+/-4.7) kJ/mol). These results suggest that the marked differences in thermodynamic stabilities of the locally disordered conformer (I) and the overall unfolding species (U) are a key to determine the functional differences of the two structurally similar proteins in physiology.

A single mutation in the wild-type transthyretin (WT TTR) such as V30M causes a familial amyloidotic polyneuropathy disease. Comparison of the three-dimensional crystal structures of WT and V30M does not tell much about the reason. High-pressure NMR revealed that at neutral pH both WT and V30M exist as equilibrium between the native tetramer and the dissociated/unfolded monomer. The native tetramer is highly stable in WT (deltaG(0)=104 kJ/mol at 37 degrees C, pH 7.1), but the stability is significantly reduced in V30M (deltadeltaG(0)=-18 kJ/mol), increasing the fraction of the unfolded monomer by a 1000-fold. Significant reduction of thermodynamic stability of WT TTR by mutation could be a crucial factor for familial amyloidotic polyneuropathy.

Structure formation in two species of the two-disulfide variant of hen lysozyme was investigated by means of CD spectroscopy, disulfide exchange measurement, and 1H-NMR spectroscopy. One species, 2SS [6-127, 30-115], which contained the two disulfide bonds found in the alpha-domain of authentic lysozyme, had amounts of secondary and tertiary structures, and bacteriolytic activity comparable to those of authentic lysozyme, and showed a cooperative thermal unfolding. By contrast, the other species, 2SS [64-80, 76-94], which contained the beta-domain disulfide bond as well as the inter-domain one, had a limited amount of secondary structure and little tertiary structure. Disulfide-exchange did not occur for 2SS [6-127, 30-115], whereas it occurred for 2SS [64-80, 76-94], indicating that the protein main-chain fold coupled with the formation of two disulfide bonds is relatively stable for the former variant, while unstable for the latter. 1H-NMR spectra of 2SS [6-127, 30-115] showed that native-like local environment is present within the region that corresponds to the alpha-domain, while it is absent within the region that corresponds to the beta or inter-domain. These results indicate that the alpha-domain of hen lysozyme can be an independent folding domain at equilibrium. Although the bipartite nature in the structure formation of hen lysozyme is similar to that reported for alpha-lactalbumin, differences exist between the disulfide-intermediates of the two proteins in terms of the structural domain that accomplishes tertiary structure.

High pressure 1 H/ 15 N two-dimensional NMR spectroscopy has been used to study conformational fluctuation in bovine β-lactoglobulin at pH 2.0 and 36 °C. Pressure dependencies of 1 H and 15 N chemical shifts and cross-peak intensities were analyzed at more than 80 independent atom sites between 30 and 2000 bar. Unusually large and non-linear chemical shift pressure dependencies are found for residues centering in the hydrophobic core region, suggesting the existence of low-lying excited native states (N′) of the protein. Measurement of 1 H/ 15 N cross-peak intensities at individual amide sites as a function of pressure suggests that unfolding events occur independently in two sides of the β-barrel, i.e. the hydrophobic core side (βF-H) (producing I 2 ) and the non-core side (βB-E) (producing I 1 ). At 1 bar the stability is higher for the core region (Δ G 0 =6.5(±2.0) kcal/mol) than for the non-core region (4.6(±1.3) kcal/mol), but at high pressure the stability is reversed due to a larger Δ V value of unfolding for the core region (90.0(±35.2) ml/mol) than that for the non-core region (57.4(±14.4) ml/mol), possibly due to an uneven distribution of cavities. The Δ G 0 profile along the amino acid sequence obtained from the pressure experiment is found to coincide well with that estimated from hydrogen exchange experiments. Altogether, the high pressure NMR experiment has revealed a variety of fluctuating conformers of β-lactoglobulin, notably N, N′, I 1 , I 2 and the totally unfolded conformer U. Fluctuation of N to I 1 and I 2 conformers with open barrel structures could be a common design of lipocalin family proteins which bind various hydrophobic compounds in its barrel structure.

Methanol-induced conformational transitions of cytochrome c(cyt c) at acidic pH values were investigated with a combined use of far and near-UV CD, fluorescence, NMR spectroscopy and small-angle X-ray scattering. At pH 3.0 and 25 degrees C, two methanol-induced non-native states were characterized. First, addition of methanol up to 25% (v/v) induced a compact denatured conformer (I(M)). Further addition of methanol transformed this I(M) state into the expanded and highly helical denatured state (H). The existence of the I(M) state was shown by the discrepancy in transition curves obtained from the ellipticity at 222 nm, the ellipticity at 282 nm, the tryptophan fluorescence monitored at 350 nm and the native peak intensity of the (1)H NMR spectrum. These CD, fluorescence and NMR results showed that the I(M) state has no specific tertiary structure but has a secondary structural content and tryptophan environment similar to those in the native state. The radius of gyration of the I(M) state, 17.7 angstroms, obtained from the Guinier plot of the small-angle X-ray scattering data was significantly smaller than that of the acid-denatured state (30.1 angstroms) and was closer to that of the native state (14.6 angstroms), showing that the I(M) state is compact. The Kratky plot for the I(M) state exhibited a bell-shaped profile, indicating a globular conformation. These structural features indicate that the structure of the I(M) state is quite similar to that of the anion-induced molten globule state of this protein. Furthermore the alcohol-denatured state (H) of cyt C in 60% (v/v) methanol was structurally characterized. Though the H state had a helical content much higher than the native state monitored by far-UV CD spectroscopy, the radius of gyration, 31.7 angstroms, was similar to that of the acid-denatured state, showing that this H state is an expanded denatured state. The Kratky plot for the H state did not show a clear peak, indicating a chain-like conformation. Thus we conclude that the H state has an expanded and chain-like conformation with a high helical content. Finally, we constructed a phase diagram of cyt c involving the native, I(M), acid-denatured and H states against pH and the methanol concentration. The result indicates that the I(M) state is found in the pH range from 2.5 to at least 4.5 with a pH-dependent optimum methanol concentration of 10 to 40%.

We report, based on proteolytic experiments and high resolution 1H nuclear magnetic resonance studies that the terminal regions of the monomeric hook protein are highly mobile and exposed to the solvent. The disordered parts of the hook protein span approximately the first 70 and the last 30 amino acid residues. Although the amino acid sequences of flagellin and hook protein do not resemble each other at all, both proteins have now been shown to contain large disordered terminal regions. Sequential similarities of flagellin and hook protein, especially near the NH2 and COOH termini, to other axial components of bacterial flagellum suggest that terminal disorder may be a common structural feature of the axial proteins of the bacterial flagellum.

The dissociation and reassociation processes of amyloid protofibrils initiated by pressure-jump have been monitored with real-time (1)H NMR spectroscopy using an intrinsically denatured disulfide-deficient variant of hen lysozyme. Upon pressure-jump up to 2 kbar, the matured protofibrils grown over several months become fully dissociated into monomers within a few days. Upon pressure-jump down to 30 bar, the dissociated monomers immediately start reassociating. The association and dissociation cycle can be repeated reproducibly by alternating pressure, establishing a notion that the protofibril formation is simply a slow kinetic process toward thermodynamic equilibrium. The outstanding simplicity and effectiveness of pressure in controlling the protofibril formation opens a new route for investigating mechanisms of amyloid fibril-forming reactions. The noted variation in the pressure-induced dissociation rate with the progress of the association reaction suggests multiple mechanisms for the elongation of the protofibril. The disulfide-deficient hen lysozyme offers a particularly simple model system for thermodynamic and kinetic studies of protofibril formation as well as for screening drugs for amyloidosis.

Conformational fluctuation plays a key role in protein function, but we know little about the associated structural changes. Here we present a general method for elucidating, at the atomic level, a large-scale shape change of a protein molecule in solution undergoing conformational fluctuation. The method utilizes the intimate relationship between conformation and partial molar volume and determines three-dimensional structures of a protein at different pressures using variable pressure NMR technique, whereby NOE distance and torsion angle constraints are used to create average coordinates. Ubiquitin (pH 4.6 at 20 degrees C) was chosen as the first target, for which structures were determined at 30 bar and at 3 kbar, giving "NMR snapshots" of a fluctuating protein structure at atomic resolution. The result reveals that the helix swings in and out by >3 angstroms with a simultaneous reorientation of the C-terminal segment, providing an "open" conformer suitable for enzyme recognition. Spin relaxation analysis indicates that this fluctuation occurs in the ten microsecond time range with activation volumes -4.2(+/-3.2) and 18.5(+/-3.0) ml/mol for the "closed-to-open" and the "open-to-closed" transitions, respectively.

The “rules” governing protein structure and stability are still poorly understood. Important clues have come from proteins that operate under extreme conditions, because these clarify the physical constraints on proteins. One obvious extreme is pressure, but so far little is known of the behavior of proteins under pressure, largely for technical reasons. We have therefore developed new methodology for calculating structure change in solution with pressure, using NMR chemical shift changes, and we report the change in structure of lysozyme on going from 30 bar to 2000 bar, this being the first solution structure of a globular protein under pressure. The α-helical domain is compressed by approximately 1%, due to tighter packing between helices. The interdomain region is also compressed. By contrast, the β-sheet domain displays very little overall compression, but undergoes more structural distortion than the α-domain. The largest volume changes tend to occur close to hydrated cavities. Because isothermal compressibility is related to volume fluctuation, this suggests that buried water molecules play an important role in conformational fluctuation at normal pressures, and are implicated as the nucleation sites for structural changes leading to pressure denaturation or channel opening.

The conformational transitions of a small oncogene product, p13(MTCP1), have been studied by high-pressure fluorescence of the intrinsic tryptophan emission and high-pressure 1D and 2D 1H-15N NMR. While the unfolding transition monitored by fluorescence is cooperative, two kinds of NMR spectral changes were observed, depending on the pressure range. Below approximately 200 MPa, pressure caused continuous, non-linear shifts of many of the 15N and 1H signals, suggesting the presence of an alternate folded conformer(s) in rapid equilibrium (taums) with the basic native structure. Above approximately 200 MPa, pressure caused a sharp decrease in the intensity of the folded proteins signals, while the peaks corresponding to disordered structures increased, yielding a free energy of unfolding change of 6.0 kcal/mol and associated volume change of -100 ml/mol, in agreement with the fluorescence result. Differential scanning calorimetry also reveals two transitions between 21 and 65 degrees C, confirming the existence of an additional species under mildly denaturing conditions. We report here a real-time observation of pressure-jump unfolding kinetics by 2D NMR spectroscopy on P13MTCP1 made possible due to its very long relaxation times at high pressure revealed by fluorescence studies. Within the dead-time after the pressure-jump, the NMR spectra of the native conformer changed to those of the transient conformational species, identified in the equilibrium studies, demonstrating the equivalence between a transient species and an equilibrium excited state. After these rapid spectral changes, the intensities of all of the individual 15N-1H cross-peaks decreased gradually, and those of the disordered structure increased, consistent with the slow relaxation to the unfolded form at this pressure. Rate constants of unfolding monitored at individual amide sites within the beta-barrel were similar to those obtained from fluorescence and from side-chain protons in the hydrophobic core region, consistent with nearly cooperative unfolding. However, some heterogeneity in the apparent unfolding rate constants is apparent across the sequence and can be understood as non-uniform effects of pressure on the unfolding rate constant due to non-uniform hydration.

Pressure-induced reversible conformational changes of sperm whale apomyoglobin have been studied between 30 bar and 3000 bar on individual residue basis by utilizing 1H/15N hetero nuclear single-quantum coherence two-dimensional NMR spectroscopy at pH 6.0 and 35 °C. Apomyoglobin showed a series of pressure-dependent NMR spectra as a function of pressure, assignable to the native (N), intermediates (I), molten globule (MG) and unfolded (U) conformers. At 30 bar, the native fold (N) shows disorder only in the F helix. Between 500 bar and 1200 bar, a series of locally disordered conformers I are produced, in which local disorder occurs in the C helix, the CD loop, the G helix and part of the H helix. At 2000 bar, most cross-peaks exhibit severe line-broadening, suggesting the formation of a molten globule, but at 3000 bar all the cross-peaks reappear, showing that the molten globule turns into a well-hydrated, mobile unfolded conformation U. Since all the spectral changes were reversible with pressure, apomyoglobin is considered to exist as an equilibrium mixture of the N, I, MG and U conformers at all pressures. MG is situated at 2.4±(0.1) kcal/mol above N at 1 bar and the unfolding transition from the combined N–I state to MG is accompanied by a loss of partial molar volume by 75±(3) ml/mol. On the basis of these observations, we postulate a theorem that the partial molar volume of a protein decreases in parallel with the loss of its conformational order.

The thermodynamic stability of staphylococcal nuclease was studied against the variation of both temperature and pressure by utilizing (1)H NMR spectroscopy at 750 MHz in 20 mM Mes buffer containing 99.9 % (2)H(2)O, pH 5.3. Equilibrium fractions of folded and unfolded protein species were evaluated with the proton signals of two histidine residues as monitor in the pressure range of 30-3300 bar and in the temperature range of 1.5 degrees C-35 degrees C. From the multi-parameter fit of the experimental data to the Gibbs energy equation expressed as a simultaneous function of pressure and temperature, we determined the compressibility change (Deltabeta), the volume change at 1 bar (DeltaV degrees ) and the expansivity change (Deltaalpha) upon unfolding among other thermodynamic parameters: Deltabeta=0.02(+/-0.003) ml mol(-1) bar(-1); Deltaalpha=1.33(+/-0.2) ml mol(-1) K(-1); DeltaV degrees =-41.9(+/-6. 3) ml mol(-1) (at 24 degrees C); DeltaG degrees =13.18(+/-2) kJ mol(-1) (at 24 degrees C); DeltaC(p)=13.12(+/-2) kJ mol(-1) K(-1); DeltaS degrees =0.32(+/-0.05) kJ mol(-1) K(-1 )(at 24 degrees C). The result yields a three-dimensional free energy surface, i.e. the free energy-landscape of staphylococcal nuclease on the P-T plane. The significantly positive Deltabeta and Deltaalpha values suggest that, in the pressure-denatured state, staphylococcal nuclease forms a loosely packed and fluctuating structure. The slight but statistically significant difference between the unfolding transitions of the His8 and His124 environments is considered to reflect local fluctuations in the native state, leading to pre-melting of the His124 environment prior to the cooperative unfolding of the major part of the protein.

We demonstrate, for the first time in solution, that pressure induces changes in the overall folded structure of a protein (lysozyme). This was made possible by using a home-developed, on-line continuously variable pressure cell on a high resolution NMR spectrometer operating at 750 MHz. We could follow pressure-induced diamagnetic chemical shifts of more than 26 protons of lysozyme at variable pressure in the range of 1 to 2000 bar. The results indicate that the main effect of the pressure is a compaction of the hydrophobic core part of the protein consisting of bulky side-chains. The technique introduced here provides a general method with which one can probe microscopic internal flexibility of a protein in solution.

Streptomyces subtilisin inhibitor (SSI), a homo-dimeric protein with a subunit of 113 residues with two disulfide bonds, is known to exist at low pH in at least three distinct thermodynamic states namely, the native (N), cold-denatured (D′) and heat-denatured (D). Small-angle X-ray scattering was used to analyze and to compare overall chain conformations of SSI in typical, N, D′, D, and urea-denatured states (D urea ). Molecular masses were determined from scattering intensities extrapolated to a scattering angle of zero, which showed that SSI exists as a homo-dimer in the N state, but as dissociated monomers in the D′, D and D urea states. From Guinier plots of the scattering intensities, radii of gyration (R g ) were determined to be 20.1(±1.8) A for N, and 20.7(±1.3), 25.8(±1.5) and 32 to 35 A for D′, D and D urea , respectively. Kratky plots for both N and D′ exhibited a bell-shape indicating that the polypeptide chain has a globular part not only in N but also in D′, while Kratky plots for D and D urea showed that the polypeptide chain has no globular part either in D urea or D. Combined with the results from circular dichroism and 1 H NMR spectra, a picture emerges for the polypeptide chain conformation of SSI such that in N it is a globular dimer close to that in the crystal, in D urea it is totally disordered and expanded nearly to a fully random chain with restrictions only from the disulfide bridges, in D the entire chain is disordered and expanded but with considerable local intra-chain interactions, and in D′ the chain consists of part with a unique tertiary structure and a part disordered and expanded to a degree comparable to D. f2

Thermodynamic stability of ribonuclease A (6.2 mM pH 1.0, 0.15 M KCl, in 2H2O) has been studied in the pressure range of 1 to 2000 atm and in the temperature range of 7.5 to 40 degrees C with a high pressure 1H NMR technique at 400 MHz. His epsilon proton resonances were used as reporter groups to measure fractions of folded and unfolded species. Gibbs energy differences between folded and unfolded species were obtained as functions of pressure for different temperatures and as functions of temperature for different pressures. The volume increase upon unfolding, delta V, was negative and temperature-dependent, decreasing from -10 ml/mol at 7.5 degrees C to -30 ml/mol at 37 degrees C. From the least squares-fitting of experimental Gibbs energy differences to a theoretical expression holding pressure and delta Cp constant, we determined best-fit values of delta G, delta H, delta S and delta Cp for different values of pressure in the temperature range 7.5 to 40 degrees C. We found that delta Cp is dependent on pressure, decreasing from 1.79 kcal/mol K at 1 atm to 1.08 kcal/mol K at 2000 atm. These findings appear to be consistent with a notion that the state of hydration of non-polar side-chains upon unfolding of the protein is a major factor that determines the pressure dependence of the conformational stability of ribonuclease A under the chosen experimental condition.

The terminal regions of Salmonella flagellin are essential for polymerization to form the flagellar filament. It has recently been suggested, on the basis of results from circular dichroism spectroscopy and scanning calorimetry, that these regions are disordered in solution. We report here direct evidence for disorder and mobility in the terminal regions of flagellin using 400 MHz proton nuclear magnetic resonance (n.m.r.) spectroscopy. Comparison of the n.m.r. spectra of monomeric and polymeric flagellin shows that the terminal regions become organized when polymerized to form the filament.