Structure of variant-3 scorpion neurotoxin from Centruroides sculpturatus Ewing, refined at 1.8 A resolution

The three-dimensional structure of the variant-3 protein neurotoxin from the scorpion Centruroides sculpturatus Ewing has been determined by X-ray diffraction data. The initial model for the 65-residue protein was obtained at 3 A resolution by multiple-isomorphous-replacement methods. The structure was refined at 1.8 A resolution by restrained difference-Fourier methods, and by free-atom, block-diagonal least-squares. Considering the 4900 reflections for which d = 1.8-7 A and Fo greater than 2.5 sigma (Fo), the final R-index is 0.16 for the restrained model, and 0.14 for the free-atom model. Average estimated errors in atomic co-ordinates are about 0.1 A. The refined structure includes 492 protein atoms; one molecule of 2-methyl-2,4-pentanediol, which is tightly bound in a hydrophobic pocket on the surface of the protein; and 72 additional solvent sites. The major secondary structural features are two and a half turns of alpha-helix and a three-strand stretch of antiparallel beta-sheet. The helix is connected to the middle strand of the beta-sheet by two disulfide bridges, and a third disulfide bridge is located nearby. Several loops extend out of this dense core of secondary structure. The protein displays several reverse turns and a highly contorted proline-rich, COOH-terminal segment. One of the proline residues (Pro59) assumes a cis-conformation. The structure involves 44 intramolecular hydrogen bonds. The crystallographic results suggest two major corrections in the published primary structure; one of these has been confirmed by new chemical sequence data. The protein displays a large flattened surface that contains a high concentration of hydrophobic residues, along with most of the conserved amino acids that are found in the scorpion neurotoxins.     

Characterization of a partially denatured state of a protein by two-dimensional NMR: reduction of the hydrophobic interactions in ubiquitin

A stable, partially structured state of ubiquitin, the A-state, is formed at pH 2.0 in 60% methanol/40% water at 298 K. Detailed characterization of the structure of this state has been carried out by 2D NMR spectroscopy. Assignment of slowly exchanging amide resonances protected from the solvent in the native and A-state shows that gross structural reorganization of the protein has not occurred and that the A-state contains a subset of the interactions present in the native state (N-state). Vicinal coupling constants and NOESY data show the presence of the first two strands of the five-strand beta-sheet that is present in the native protein and part of the third beta-strand. The hydrophobic face of the beta-sheet in the A-state is covered by a partially structured alpha-helix, tentatively assigned to residues 24-34, that is considerably more flexible than the alpha-helix in the N-state. There is evidence for some fixed side-chain--side-chain interactions between these two units of structure. The turn-rich area of the protein, which contains seven reverse turns and a short piece of 3(10) helix, does not appear to be structured in the A-state and is approaching random coil.     

Preliminary crystal structure analysis of a microbial, guanine-specific ribonuclease St at 2.5 A resolution

The three-dimensional structure of Ribonuclease St (RNase St), the extracellular ribonuclease from Streptomyces erythreus, has been deduced based on a preliminary electron density map at 2.5 A resolution. RNase St has a substrate specificity similar to ribonuclease T1 which catalyzes the splitting of the phosphodiester bond of guanylic acid. Crystals grown as diamond plates have space group C2 with unit cell parameters a=88.4, b=33.0, c=69.0 A, beta = 98.4 degrees having two enzyme molecules per asymmetric unit. Phases were obtained by use of KAu(CN)4, phenylmercuric acetate and UO2 (CH3COO)2. The overall dimensions of the molecule are 40 X 30 X 25 A. The most prominent secondary structural features are two turns of alpha-helix and a three strand stretch of antiparallel beta-sheet. The alpha-carbon backbone of RNase St seems to have no apparent correlation with that of ribonuclease A.     

Protein structural perturbation and aggregation on homogeneous surfaces

We have demonstrated that globular proteins, such as hen egg lysozyme in phosphate buffered saline at room temperature, lose native structural stability and activity when adsorbed onto well-defined homogeneous solid surfaces. This structural loss is evident by alpha-helix to turns/random during the first 30 min and followed by a slow alpha-helix to beta-sheet transition. Increase in intramolecular and intermolecular beta-sheet content suggests conformational rearrangement and aggregation between different protein molecules, respectively. Amide I band attenuated total reflection/Fourier transformed infrared (ATR/FTIR) spectroscopy was used to quantify the secondary structure content of lysozyme adsorbed on six different self-assembled alkanethiol monolayer surfaces with -CH3, -OPh, -CF3, -CN, -OCH3, and -OH exposed functional end groups. Activity measurements of adsorbed lysozyme were in good agreement with the structural perturbations. Both surface chemistry (type of functional groups, wettability) and adsorbate concentration (i.e., lateral interactions) are responsible for the observed structural changes during adsorption. A kinetic model is proposed to describe secondary structural changes that occur in two dynamic phases. The results presented in this article demonstrate the utility of the ATR/FTIR spectroscopic technique for in situ characterization of protein secondary structures during adsorption on flat surfaces.     

Determination of alpha-helix and beta-sheet stability in the solid state: a solid-state NMR investigation of poly(L-alanine)

The relative stability of alpha-helix and beta-sheet secondary structure in the solid state was investigated using poly(L-alanine) (PLA) as a model system. Protein folding and stability has been well studied in solution, but little is known about solid-state environments, such as the core of a folded protein, where peptide packing interactions are the dominant factor in determining structural stability. (13)C cross-polarization with magic angle spinning (CPMAS) NMR spectroscopy was used to determine the backbone conformation of solid powder samples of 15-kDa and 21.4-kDa PLA before and after various sample treatments. Reprecipitation from helix-inducing solvents traps the alpha-helical conformation of PLA, although the method of reprecipitation also affects the conformational distribution. Grinding converts the secondary structure of PLA to a final steady-state mixture of 55% beta-sheet and 45% alpha-helix at room temperature regardless of the initial secondary structure. Grinding PLA at liquid nitrogen temperatures leads to a similar steady-state mixture with 60% beta-sheet and 40% alpha-helix, indicating that mechanical shear force is sufficient to induce secondary structure interconversion. Cooling the sample in liquid nitrogen or subjecting it to high pressure has no effect on secondary structure. Heating the sample without grinding results in equilibration of secondary structure to 50% alpha-helix/50% beta-sheet at 100 degrees C when starting from a mostly alpha-helical state. No change was observed upon heating a beta-sheet sample, perhaps due to kinetic effects and the different heating rate used in the experiments. These results are consistent with beta-sheet approximately 260 J/mol more stable than alpha-helix in solid-state PLA.     

Prediction and Fourier transform infrared spectroscopy estimation of the secondary structure of a Bacillus licheniformis endo-beta-1,3-1,4-D-glucanase.

The secondary structure of a recombinant Bacillus licheniformis endo-beta-1,3-1,4-D-glucanase (EC.3.2.1.73) has been estimated by Fourier Transform Infrared Spectroscopy and also predicted by the algorithm of Chou and Fasman. From the curve fitting of the deconvolved IR spectrum, the most probable distribution of the secondary structural classes appears to be about 40% beta-sheet, 25% reverse turn, 24% non-ordered and 11% alpha-helix. From theoretical prediction of secondary structure the protein would present 37% beta-sheet, 31% reverse turn, 22% non-ordered and 10% alpha-helix.     

Secondary structure of Escherichia coli glucosamine-6-phosphate deaminase from amino acid sequence and circular dichroism spectroscopy

The secondary structure of the purified glucosamine-6-phosphate deaminase from Escherichia coli K12 was investigated by both circular dichroism (CD) spectroscopy and empirical prediction methods. The enzyme was obtained by allosteric-site affinity chromatography from an overproducing strain bearing a pUC18 plasmid carrying the structural gene for the enzyme. From CD analysis, 34% of alpha-helix, 9% of parallel beta-sheet, 11% of antiparallel beta-sheet, 15% turns and 35% of non-repetitive structures, were estimated. A joint prediction scheme, combining six prediction methods with defined rules using several physicochemical indices, gave the following values: alpha-helix, 37%; beta-sheet, 22%; turns, 18% and coil, 23%. The structure predicted showed also a considerable degree of alternacy of alpha and beta structures; 64% of helices are amphipathic and 90% of beta-sheets are hydrophobic. Overall, the data suggest that deaminase has as dominant motif, an alpha/beta structure.     

Secondary structure of bovine beta-lactoglobulin B

Secondary-structure-prediction algorithms have been used to find the segments of beta-lactoglobulin sequence most likely to fit the circular dichroism assignment of 15% alpha-helix, 50% beta-sheet, and 15-20% reverse turn. A number of segments may have an alpha-helical conformation but the most prominent region of alpha-helix is from residue 129 to 143. A further probable alpha-helix segment is residues 65-76. The number of residues predicted to occur in segments of beta-sheet structure is less than expected. However, the most likely segments are for residues 1-6, 11-16, 39-45, 80-85, 92-96, 101-107, 117-123, and 145-151. Predicted reverse-turn tetrapeptides are residues 7-10, 49-52, 61-64, 88-91, and 112-115. These predicted secondary structures are consistent with the low-resolution structure of the molecule determined by X-ray diffraction studies.     

Minimal model for studying prion-like folding pathways

The Monte Carlo technique is used to simulate the energy landscape and the folding kinetics of a minimal prion-like protein model. We show that the competition between hydrogen-bonding and hydrophobic interactions yields two energetically favored secondary structures, an alpha-helix and a beta-hairpin. Folding simulations indicate that the probability of reaching the alpha-helix form from a denatured random conformation is much higher than the probability of reaching the beta-sheet form, even though the beta-sheet has a lower energy. The existence of a lower energy beta-sheet state gives the possibility for the normal alpha-helix structure to take a structural transformation into the beta-sheet structure under external influences.     

Crystal structure of recombinant human interleukin-4.

The crystal structure of recombinant human interleukin-4 (rhuIL-4) was initially determined at 3.5-A resolution by multiple isomorphous replacement techniques and subsequently refined to a resolution of 2.35 A by simulated annealing. The final crystallographic R-factor, based on all data in the range 6.0-2.35 A (7470 reflections), is 0.232. Bond lengths and bond angles in the molecule have root mean square deviations from ideal values of 0.016 A and 2.4 degrees, respectively. The overall structure is highly compact and globular with a predominantly hydrophobic core. The main structural feature of rhuIL-4 is a four alpha-helix bundle, which composes approximately 58% of the structure. The helices are arranged in a left-handed antiparallel bundle with two overhand connections. Within these connections is a two-stranded antiparallel beta-sheet. Both the tertiary and secondary structures of rhuIL-4 are similar to those of human granulocyte-macrophage colony-stimulating factor. Critical regions for receptor binding are proposed.     

Refined crystal structure of carboxypeptidase A at 1.54 A resolution

The crystal structure of bovine carboxypeptidase A (Cox) has been refined at 1.54 A resolution using the restrained least-squares algorithm of Hendrickson & Konnert (1981). The crystallographic R factor (formula; see text) for structure factors calculated from the final model is 0.190. Bond lengths and bond angles in the carboxypeptidase A model have root-mean-square deviations from ideal values of 0.025 A and 3.6 degrees, respectively. Four examples of a reverse turn like structure (the "Asx" turn) requiring an aspartic acid or asparagine residue are observed in this structure. The Asx turn has the same number of atoms as a reverse turn, but only one peptide bond, and the hydrogen bond that closes the turn is between the Asx side-chain CO group and a main-chain NH group. The distributions of CO-N and NH-O hydrogen bond angles in the alpha-helices and beta-sheet structures of carboxypeptidase A are centered about 156 degrees. A total of 192 water molecules per molecule of enzyme are included in the final model. Unlike the hydrogen bonding geometry observed in the secondary structure of the enzyme, the CO-O(wat) hydrogen bond angle is distributed about 131 degrees, indicating the role of the lone pair electrons of the carbonyl oxygen in the hydrogen bond interaction. Twenty four solvent molecules are observed buried within the protein. Several of these waters are organized into hydrogen-bonded chains containing up to five waters. The average temperature factor for atoms in carboxypeptidase A is 8 A2, and varies from 5 A2 in the center of the protein, to over 30 A2 at the surface.     

Peptide-chain secondary structure of bacteriorhodopsin.

Ultraviolet circular dichroism spectroscopy in the interval from 190 to 240 nm and infrared spectroscopy in the region of the amide I band (1,600 cm-1 to 1,700 cm-1) has been used to estimate the alpha-helix content and the beta-sheet content of bacteriorhodopsin. Circular dichroism spectroscopy strongly suggests that the alpha-helix content is sufficient for only five helices, if each helix is composed of 20 or more residues. It also suggests that there is substantial beta-sheet conformation in bacteriorhodopsin. The presence of beta-sheet secondary structure is further suggested by the presence of a 1,639 cm-1 shoulder on the amide I band in the infrared spectrum. Although a structural model consisting of seven alpha-helical rods has been generally accepted up to this point, the spectroscopic data are more consistent with a model consisting of five alpha-helices and four strands of beta-sheet. We note that the primary amino acid sequence can be assigned to segments of alpha-helix and beta-sheet in a way that does not require burying more than two charged groups in the hydrophobic membrane interior, contrary to the situation for any seven-helix model.     

Temperature effect on the structural stability, similarity, and reversibility of human serum albumin in different states

In order to investigate the thermal stability of human serum albumin (HAS) in three different states (aqueous solution, cast film, and solid powder), Fourier transform infrared (FTIR) spectroscopy was applied to determine the protein secondary structural changes of these HSA samples under non-isothermal or isothermal condition. The structural similarity of HSA before and after thermal treatment was also studied to estimate the thermo-reversible property of the HSA in these different states. The results indicate that with the increase of temperature, the maximum peaks at 1652 and 1547 cm(-1) (alpha-helix) shifted to 1647 and 1542 cm(-1) (random coil), respectively. An additional peak at 1620 cm(-1) assigned to intermolecular beta-sheet structure clearly appeared with temperature. The alpha-helix content was found to be reduced in favor of the formation of intermolecular hydrogen-bonded antiparallel beta-sheet structure beyond 60 degrees C in the heating process. From the data of structural similarity, HSA sample whether in solid powder or cast film form exhibited a better thermo-reversible property than HSA in aqueous solution even heating to 200 degrees C.     

Molecular dynamics simulations of the native and partially folded states of ubiquitin: influence of methanol cosolvent, pH, and temperature on the protein structure and dynamics

A series of explicit-solvent molecular dynamics simulations of the protein ubiquitin are reported, which investigate the effect of environmental factors (presence of methanol cosolvent in the aqueous solution, neutral or low pH value, room or elevated temperature) on the structure, stability, and dynamics of the protein. The simulations are initiated either from the native structure of the protein or from a model of a partially folded state (A-state) that is known to exist at low pH in methanol-water mixtures. The main results of the simulations are: (1) The ubiquitin native structure is remarkably stable at neutral pH in water; (2) the addition of the methanol cosolvent enhances the stability of the secondary structure but weakens tertiary interactions within the protein; (3) this influence of methanol on the protein structure is enhanced at low pH, while the effect of lowering the pH in pure water is limited; and (4) the A-state of ubiquitin can be described as a set of relatively rigid secondary structure elements (a native-like beta-sheet and native-like alpha-helix plus two nonnative alpha-helices) connected by flexible linkers.     

Protein unfolding at interfaces: slow dynamics of alpha-helix to beta-sheet transition

A two-phase sequential dynamic change in the secondary structure of hen egg lysozyme (Lys) adsorbed on solid substrates was observed. The first phase involved fast conversion of alpha-helix to random/turns (within the first minute or at very low coverage or high substrate wettability) with no perceptible change in beta-sheet content. The second phase (1-1200 min), however, involved a relatively slow conversion from alpha-helix to beta-sheet without a noticeable change in random/turns. An important finding of this work is that the concentration of lysozyme in the adsorbed state has a substantial effect on the fractional content of secondary structures. Attenuated total reflection Fourier transform infrared (ATR/FTIR) spectroscopy, along with a newly-developed optimization algorithm for predicting the content of secondary structure motifs, was used to correlate the secondary structure and the amount of adsorbed lysozyme with the surface wettability of six different flat nanoporous substrates. Although three independent variables, surface wettability, solution concentration and time for adsorption, were used to follow the fractional structural changes of lysozyme, the results were all normalized onto a single plot with the amount adsorbed as the universal independent variable. Consequently, lateral interactions among proteins likely drive the transition process. Direct intermolecular force adhesion measurements between lysozyme and different functionalized self-assembled alkanethiol monolayers confirm that hydrophobic surfaces interact strongly with proteins. The lysozyme-unfolding pathway during early adsorption appears to be similar to that predicted by published molecular modeling results.     

Secondary structure of the murine histocompatibility alloantigen H-2Kb: relationship between heavy chain, beta 2-microglobulin, and antigenic reactivity

The far-ultraviolet circular dichroism (CD) spectra of the extracellular portion (papain-cleaved fragment) of the histocompatibility antigen H-2Kb and its noncovalently associated components, heavy chain and beta 2-microglobulin (beta 2m), indicate that the antigen is highly structured, containing about 30% alpha-helix, 41% beta-sheet, and 29% random coil. Separation of beta 2m from the heavy chain produced a decrease in heavy chain alpha-helix and beta-sheet structure which correlated with a loss of alloantigenic reactivity. Reconstitution of the heavy chain-beta 2m complex resulted in an increase in secondary structure which was greater than the sum of the free chains and the recovery of considerable alloantigenic reactivity. This suggests that some of the secondary structure and much of the alloantigenic reactivity may depend on conformation associated with the binding of beta 2m to heavy chain. A prediction of heavy chain secondary structure based on Chou-Fasman analysis of the primary amino acid sequence agreed with results from CD measurements and suggested that the segments of alpha-helix and beta-sheet structure are distributed throughout the molecule.     

Crystal structure of thioredoxin from Escherichia coli at 1.68 A resolution

The crystal structure of thioredoxin from Escherichia coli has been refined by the stereochemically restrained least-squares procedure to a crystallographic R-factor of 0.165 at 1.68 A resolution. In the final model, the root-mean-square deviation from ideality for bond distances is 0.015 A and for angle distances 0.035 A. The structure contains 1644 protein atoms from two independent molecules, two Cu2+, 140 water molecules and seven methylpentanediol molecules. Ten residues have been modeled in two alternative conformations. E. coli thioredoxin is a compact molecule with 90% of its residues in helices, beta-strands or reverse turns. The molecule consists of two conformational domains, beta alpha beta alpha beta and beta beta alpha, connected by a single-turn alpha-helix and a 3(10) helix. The beta-sheet forms the core of the molecule packed on either side by clusters of hydrophobic residues. Helices form the external surface. The active site disulfide bridge between Cys32 and Cys35 is located at the amino terminus of the second alpha-helix. The positive electrostatic field due to the helical dipole is probably important for stabilizing the anionic intermediate during the disulfide reductase function of the protein. The more reactive cysteine, Cys32, has its sulfur atom exposed to solvent and also involved in a hydrogen bond with a backbone amide group. Residues 29 to 37, which include the active site cysteine residues, form a protrusion on the surface of the protein and make relatively fewer interactions with the rest of the structure. The disulfide bridge exhibits a right-handed conformation with a torsion angle of 81 degrees and 72 degrees about the S-S bond in the two molecules. Twenty-five pairs of water molecules obey the noncrystallographic symmetry. Most of them are involved in establishing intramolecular hydrogen-bonding interactions between protein atoms and thus serve as integral parts of the folded protein structure. Methylpentanediol molecules often pack against the loops and stabilize their structure. Cu2+ used for crystallization exhibit a distorted octahedral square bipyramid co-ordination and provide essential packing interactions in the crystal. The two independent protein molecules are very similar in conformation but distinctly different in atomic detail (root-mean-square = 0.94 A). The differences, which may be related to the crystal contacts, are localized mostly to regions far from the active site.     

Structure and properties of a dimeric N-terminal fragment of human ubiquitin.

Previous peptide dissection and kinetic experiments have indicated that in vitro folding of ubiquitin may proceed via transient species in which native-like structure has been acquired in the first 45 residues. A peptide fragment, UQ(1-51), encompassing residues 1 to 51 of ubiquitin was produced in order to test whether this portion has propensity for independent self-assembly. Surprisingly, the construct formed a folded symmetrical dimer that was stabilised by 0.8 M sodium sulphate at 298 K (the S state). The solution structure of the UQ(1-51) dimer was determined by multinuclear NMR spectroscopy. Each subunit of UQ(1-51) consists of an N-terminal beta-hairpin followed by an alpha-helix and a final beta-strand, with orientations similar to intact ubiquitin. The dimer is formed by the third beta-strand of one subunit interleaving between the hairpin and third strand of the other to give a six-stranded beta-sheet, with the two alpha-helices sitting on top. The helix-helix and strand portions of the dimer interface also mimic related features in the structure of ubiquitin. The structural specificity of the UQ(1-51) peptide is tuneable: as the concentration of sodium sulphate is decreased, near-native alternative conformations are populated in slow chemical exchange. Magnetization transfer experiments were performed to characterize the various species present in 0.35 M sodium sulphate, namely the S state and two minor forms. Chemical shift differences suggest that one minor form is very similar to the S state, while the other experiences a significant conformational change in the third strand. A segmental rearrangement of the third strand in one subunit of the S state would render the dimer asymmetric, accounting for most of our results. Similar small-scale transitions in proteins are often invoked to explain solvent exchange at backbone amide proton sites that have an intermediate level of protection.     

Is the unfolded state the Rosetta Stone of the protein folding problem?

Solving the protein folding problem is one of the most challenging tasks in the post genomic era. Identification of folding-initiation sites is very important in order to understand the protein folding mechanism. Detection of residual structure in unfolded proteins can yield important clues to the initiation sites in protein folding. A substantial number of studied proteins possess residual structure in hydrophobic regions clustered together in the protein core. These stable structures can work as seeds in the folding process. In addition, local preferences for secondary structure in the form of turns for beta-sheet initiation and helical turns for alpha-helix formation can guide the folding reaction. In this respect the unfolded states, studied at increasing structural resolution, can be the Rosetta Stone of the protein folding problem.