Systematics in the interaction of metal ions with the main-chain carbonyl group in protein structures

An analysis of the geometry of metal binding by peptide carbonyl groups in proteins is presented. Such metal ions are predominantly calcium in known protein structures. Cations tend to be located in the peptide plane, near the C = O bond direction. This distribution differs from that observed for water molecules bound to carbonyl oxygens. Most metal ions are bound to carbonyl oxygens of peptides in turns or in regions with no regular secondary structure. More infrequent binding interactions occur at the C-terminal end of alpha-helices or at the edges and sides of beta-sheets, where the geometrical preferences of the metal-carbonyl interaction may be satisfied. In many proteins carbonyl groups that are one, two, or three residues apart along the polypeptide chain bind to the same cation; these structures show a limited number of main-chain conformations around the metal center.     

An electrophile-nucleophile interaction in metalloprotein structures.

A new attractive interaction in metalloprotein structures, between the thiolate anion of a metal-bound cysteine (acting as a nucleophile) and a carbonyl carbon of a peptide group (an electrophile), has been identified. From 82 cases extracted from 23 metalloprotein structures, the interacting S and C atoms are found to be at a distance of 3.2 (+/-2) A, such that the angle S ... C-O is 109 degrees (+/-15 degrees). Usually, the interacting atoms are from the same Cys residue, and to allow the S to interact with the carbonyl group the side-chain and the main-chain torsion angles deviate from those found in cysteines not bound by metals. There is a good correlation between the S...C distance and the angular deviation of the S...C vector from the normal to the peptide plane. Various data points may be envisaged to represent "snapshots" along the reaction coordinate for the intra-residue attack of Cys S on the CO group.     

Crystal structure of an Fab fragment in complex with a meningococcal serosubtype antigen and a protein G domain.

Many pathogens present highly variable surface proteins to their host as a means of evading immune responses. The structure of a peptide antigen corresponding to the subtype P1.7 variant of the porin PorA from the human pathogen Neisseria meningitidis was determined by solution of the X-ray crystal structure of the ternary complex of the peptide (ANGGASGQVK) in complex with a Fab fragment and a domain from streptococcal protein G to 1.95 A resolution. The peptide adopted a beta-hairpin structure with a type I beta-turn between residues Gly4P and Gly7P, the conformation of the peptide being further stabilised by a pair of hydrogen bonds from the side-chain of Asn2P to main-chain atoms in Val9P. The antigen binding site within the Fab formed a distinct crevice lined by a high proportion of apolar amino acids. Recognition was supplemented by hydrogen bonds from heavy chain residues Thr50H, Asp95H, Leu97H and Tyr100H to main-chain and side-chain atoms in the peptide. Complementarity-determining region (CDR) 3 of the heavy chain was responsible for approximately 50 % of the buried surface area formed by peptide-Fab binding, with the remainder made up from CDRs 1 and 3 of the light chain and CDRs 1 and 2 of the heavy chain. Knowledge of the structures of variable surface antigens such as PorA is an essential prerequisite to a molecular understanding of antigenic variation and its implications for vaccine design.     

Analysis of the relationship between side-chain conformation and secondary structure in globular proteins

The relationship between the preferred side-chain dihedral angles and the secondary structure of a residue was examined. The structures of 61 proteins solved to a resolution of 2.0 A (1 A = 0.1 nm) or better were analysed using a relational database to store the information. The strongest feature observed was that the chi 1 distribution for most side-chains in an alpha-helix showed an absence of the g- conformation and a shift towards the t conformation when compared to the non-alpha/beta structures. The exceptions to this tendency were for short polar side-chains that form hydrogen bonds with the main-chain which prefer g+. Shifts in the chi 1 preferences for residues in the beta-sheet were observed. Other side-chain dihedral angles (chi 2, chi 3, chi 4) were found to be influenced by the main-chain. This paper presents more accurate distributions for the side-chain dihedral angles which were obtained from the increased number of proteins determined to high resolution. The means and standard deviations for chi 1 and chi 2 angles are presented for all residues according to the secondary structure of the main-chain. The means and standard deviations are given for the most popular conformations for side-chains in which chi 3 and chi 4 rotations affect the position of C atoms.     

The geometry of alpha-sheet: Implications for its possible function as amyloid precursor in proteins

alpha-sheet has been proposed as the main constituent of the prefibrillar intermediate during amyloid formation. Here the helical parameters of the alpha-sheet strand are calculated from average main-chain dihedral angles reported from molecular dynamics simulations. It is an almost linear polypeptide that forms a right-handed helix of about 100 A diameter, with 100 residues and a rise of 30 A per turn. The strands are curved but untwisted, which implies that neighboring strands need not coil to make interstrand hydrogen bonds. This suggests that compared to beta-sheets in native folded proteins, alpha-sheets can be larger and stack more easily to create extensive 3D blocks. It is shown that alpha-sheet is related to a category of structures termed "mirror" structures. Mirror structures have repetitive pairs of main-chain dihedral angles at residues i and i+1 that satisfy the condition phi(i) (+1) = -psi(i), psi(i) (+1) = -phi(i). They are uniquely identified by the two orientations of their peptide planes, specified by phi(i) and psi(i). Their side chains point alternately in opposite directions. Interestingly, their conformations are insensitive to phi(i) and psi(i) in that the pseudo dihedral angle formed by four consecutive C(alpha) atoms is always close to 180 degrees . There are two types: "beta-mirror" and "alpha-mirror" structure; beta-mirror structures relate to beta-sheet by small peptide plane rotations, of less than 90 degrees , while alpha-mirror structures are close to alpha-sheet and relate to beta-sheet by approximately 180 degrees peptide plane flips. Most mirror structures, and in particular the alpha-mirror, form wide helices with diameters 50-70 A. Their gentle curvature, and therefore that of the alpha-sheet, arises from the orientation of successive peptide units causing the difference in the bond angles at the C and N atoms of the peptide unit to gradually change the direction of the chain.     

The hydration of protein secondary structures

The hydration of the main-chain carbonyl (CO) groups in proteins have been studied using infra-red spectroscopy, and computer-graphics analysis of high resolution protein crystal structures. The IR measurements indicate that the strength of water binding to the CO groups is lower in beta-sheet proteins compared with alpha-helical ones. Analysis of the protein crystal structures shows that this is due primarily to differences in the geometry of water-CO group interactions in the two types of secondary structure.     

Importance of main-chain hydrophobic free energy to the stability of thermophilic proteins

Living organisms are found in the most unexpected places, including deep-sea vents at 100 degrees C and several hundred bars pressure, in hot springs. Needless to say, the proteins found in thermophilic species are much more stable than their mesophilic counterparts. There are no obvious reasons to say that one would be more stable than others. Even examination of the amino acids and comparison of structural features of thermophiles with mesophilies cannot bring satisfactory explanation for the thermal stability of such proteins. In order to bring out the hidden information behind the thermal stabilization of such proteins in terms of energy factors and their combinations, analysis were made on good resolution structures of thermophilic and their mesophilic homologous from 23 different families. From the structural coordinates, free energy contributions due to hydrophobic, electrostatic, hydrogen bonding, disulfide bonding and van der Waals interactions are computed. In this analysis, a vast majority of thermophilic proteins adopt slightly lower free energy contribution in each energy terms than its mesophilic counterparts. The major observation noted from this study is the lower hydrophobic free energy contribution due to carbon atoms and main-chain nitrogen atoms in all the thermophilic proteins. The possible combination of different free energy terms shows majority of the thermophilic proteins have lower free energy strategy than their mesophilic homologous. The derived results show that the hydrophobic free energy due to carbon and nitrogen atoms and such combinations of free energy components play a vital role in the thermostablisation of such proteins.     

Strategy to design peptide inhibitors: structure of a complex of proteinase K with a designed octapeptide inhibitor N-Ac-Pro-Ala-Pro-Phe-DAla-Ala-Ala-Ala-NH2 at 2.5 A resolution.

The crystal structure of a complex formed by the interaction between proteinase K and a designed octapeptide amide, N-Ac-Pro-Ala-Pro-Phe-DAla-Ala-Ala-Ala-NH2, has been determined at 2.5 A resolution and refined to an R-factor of 16.7% for 7,430 reflections in the resolution range of 8.0-2.50 A. The inhibitor forms a stable complex through a series of hydrogen bonds and hydrophobic interactions with the protein atoms and water molecules. The inhibitor is hydrolyzed between Phe4I and DAla5I (I indicates the inhibitor). The two fragments are separated by a distance of 3.2 A between the carbonyl carbon of Phe4I and the main-chain nitrogen of DAla5I. The N-terminal tetrapeptide occupies subsites S1-S5 (S5 for acetyl group), whereas the C-terminal part fits into S1'-S5' region (S5' for amide group). It is the first time that such an extended electron density for a designed synthetic peptide inhibitor has been observed in the prime region of an enzyme of the subtilisin family. In fact, the inhibitor fills the recognition site completely. There is only a slight rearrangement of the protein residues to accommodate the inhibitor. Superposition of the present octapeptide inhibitor on the hexapeptide inhibitor studied previously shows an overall homology of the two inhibitors, although the individual atoms are displaced significantly. It suggests the existence of a recognition site with flexible dimensions. Kinetic studies indicate an inhibition rate of 100% by this specifically designed peptide inhibitor.     

Signature of n→π* interactions in α-helices

The oxygen of a peptide bond has two lone pairs of electrons. One of these lone pairs is poised to interact with the electron-deficient carbon of the subsequent peptide bond in the chain. Any partial covalency that results from this n→π* interaction should induce pyramidalization of the carbon (C'(i)) toward the oxygen (O(i-1)). We searched for such pyramidalization in 14 peptides that contain both α- and β-amino acid residues and that assume a helical structure. We found that the α-amino acid residues, which adopt the main chain dihedral angles of an α-helix, display dramatic pyramidalization but the β-amino acid residues do not. Thus, we conclude that O(i-1) and C'(i) are linked by a partial covalent bond in α-helices. This finding has important ramifications for the folding and conformational stability of α-helices in isolation and in proteins.     

Analysis of protein main-chain solvation as a function of secondary structure

We have analysed the hydration of main-chain carbonyl and amide groups in 24 high-resolution well-refined protein structures as a function of the secondary structure in which these polar groups occur. We find that main-chain atoms in beta-sheets are as hydrated as those in alpha-helices, with most interactions involving "free" amide and carbonyl groups that do not participate in secondary structure hydrogen bonds. The distributions of water molecules around these non-bonded carbonyl groups reflect specific steric interactions due to the local secondary structure. Approximately 20% and 4%, respectively of bonded carbonyl and amide groups interact with solvent. These include interactions with carbonyl groups on the exposed faces of alpha-helices that have been correlated previously with bending of the helix. Water molecules interacting with alpha-helices occur mainly at the amino and carbonyl termini of the helices, in which case the solvent sites maintain the hydrogen bonding by bridging between residues i and i-3 or i-4 at the amino terminus and between i and i+3 or i+4 at the carbonyl terminus. We also see a number of solvent-mediated Ncap and Ccap interactions. The water molecules interacting with beta-sheets occur mainly at the edges, in which case they extend the sheet structure, or at the ends of strands, in which case they extend the beta-ladder. In summary, the solvent networks appear to extend the hydrogen-bonding structure of the secondary structures. In beta-turns, which usually occur at the surface of a protein, exposed amide and carbonyl groups are often hydrated, especially close to glycine residues. Occasionally water molecules form a bridge between residues i and i+3 in the turn and this may provide extra stabilization.     

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.     

Structure of the complex of Streptomyces griseus proteinase B and polypeptide chymotrypsin inhibitor-1 from Russet Burbank potato tubers at 2.1 A resolution

A low molecular weight protein inhibitor of serine proteinases from Russet Burbank potato tubers, polypeptide chymotrypsin inhibitor-1 (PCI-1), has been crystallized in complex with Streptomyces griseus proteinase B (SGPB). The three-dimensional structure of the complex has been solved at 2.1 A resolution by the molecular replacement method and has been refined to a final R-factor (= sigma[[Fo[-[Fc[[/sigma[Fo[) of 0.142 (8.0 to 2.1 A resolution data). The reactive site bond of PCI-1 (Leu38I to Asn39I) is intact in the complex, and there is no significant distortion of the peptide from planarity. The distance between the active site serine O gamma of SGPB and the carbonyl carbon of the scissile bond of PCI-1 is 2.8 A (1 A = 0.1 nm). The inhibitor has little secondary structure, having a three-stranded antiparallel beta-sheet on the side opposite the reactive site and four beta-turns. PCI-1 has four disulphide bridges; these presumably take the place of extensive secondary structure in keeping the reactive site conformationally constrained. The pairing of the cystine residues, which had not been characterized chemically, is as follows: Cys3I to Cys40I, Cys6I to Cys24I, Cys7I to Cys36I, and Cys13I to Cys49I. The molecular structure of SGPB in the PCI-1 complex agrees closely with the structure of SGPB complexed with the third domain of the turkey ovomucoid inhibitor (OMTKY3). A least-squares overlap of all atoms in SGPB gives a root-mean-square difference of 0.37 A. One of the loops of SGPB (Ser35 to Gly40) differs in conformation in the two complexes by more than 2.0 A root-mean-square for the main-chain atoms. Thr39 displays the largest differences with the carbonyl carbon atom deviating by 3.6 A. This conformational alternative is a result of the differences in the molecular structures of the P'4 residues following the reactive site bonds of the two inhibitors. This displacement avoids a close contact (1.3 A) between the carbonyl oxygen of Ser38 of SGPB and Pro42I C beta of PCI-1. The solvent structure of the PCI-1-SGPB complex includes 179 waters, two sulphate or phosphate ions, and one calcium or potassium ion, which appears to play a role in crystal formation. The molecular structure of PCI-1 determined here has allowed the proposal of a model for the structure of a two-domain inhibitor from potatoes and tomatoes, inhibitor II.(ABSTRACT TRUNCATED AT 400 WORDS)     

High resolution crystal structures of HIV-1 protease with a potent non-peptide inhibitor (UIC-94017) active against multi-drug-resistant clinical strains

The compound UIC-94017 (TMC-114) is a second-generation HIV protease inhibitor with improved pharmacokinetics that is chemically related to the clinical inhibitor amprenavir. UIC-94017 is a broad-spectrum potent inhibitor active against HIV-1 clinical isolates with minimal cytotoxicity. We have determined the high-resolution crystal structures of UIC-94017 in complexes with wild-type HIV-1 protease (PR) and mutant proteases PR(V82A) and PR(I84V) that are common in drug-resistant HIV. The structures were refined at resolutions of 1.10-1.53A. The crystal structures of PR and PR(I84V) with UIC-94017 ternary complexes show that the inhibitor binds to the protease in two overlapping positions, while the PR(V82A) complex had one ordered inhibitor. In all three structures, UIC-94017 forms hydrogen bonds with the conserved main-chain atoms of Asp29 and Asp30 of the protease. These interactions are proposed to be critical for the potency of this compound against HIV isolates that are resistant to multiple protease inhibitors. Other small differences were observed in the interactions of the mutants with UIC-94017 as compared to PR. PR(V82A) showed differences in the position of the main-chain atoms of residue 82 compared to PR structure that better accommodated the inhibitor. Finally, the 1.10A resolution structure of PR(V82A) with UIC-94017 showed an unusual distribution of electron density for the catalytic aspartate residues, which is discussed in relation to the reaction mechanism.     

Statistical and molecular dynamics studies of buried waters in globular proteins

Buried solvent molecules are common in the core of globular proteins and contribute to structural stability. Folding necessitates the burial of polar backbone atoms in the protein core, whose hydrogen-bonding capacities should be satisfied on average. Whereas the residues in alpha-helices and beta-sheets form systematic main-chain hydrogen bonds, the residues in turns, coils and loops often contain polar atoms that fail to form intramolecular hydrogen bonds. The statistical analysis of 842 high resolution protein structures shows that well-resolved, internal water molecules preferentially reside near residues without alpha-helical and beta-sheet secondary structures. These buried waters most often form primary hydrogen bonds to main-chain atoms not involved in intramolecular hydrogen bonds, providing strong evidence that hydrating main-chain atoms is a key structural role of buried water molecules. Additionally, the average B-factor of protein atoms hydrogen-bonded to waters is smaller than that of protein atoms forming intramolecular hydrogen bonds, and the average B-factor of water molecules involved in primary hydrogen bonds with main-chain atoms is smaller than the average B-factor of water molecules involved in secondary hydrogen bonds to protein atoms that form concurrent intramolecular hydrogen bonds. To study the structural coupling between internal waters and buried polar atoms in detail we simulated the dynamics of wild-type FKBP12, in which a buried water, Wat137, forms one side-chain and multiple main-chain hydrogen bonds. We mutated E60, whose side-chain hydrogen bonds with Wat137, to Q, N, S or A, to modulate the multiplicity and geometry of hydrogen bonds to the water. Mutating E60 to a residue that is unable to form a hydrogen bond with Wat137 results in reorientation of the water molecule and leads to a structural readjustment of residues that are both near and distant to the water. We predict that the E60A mutation will result in a significantly reduced affinity of FKBP12 for its ligand FK506. The propensity of internal waters to hydrogen bond to buried polar atoms suggests that ordered water molecules may constitute fundamental structural components of proteins, particularly in regions where alpha-helical or beta-sheet secondary structure is not present.     

Flexibility observed in high resolution structures of <Emphasis Type="Italic">Streptomyces aureofaciens</Emphasis> ribonucleases determined by diffraction methods

It has been widely accepted to distinguish between static structures determined by diffraction methods and dynamic structures determined by nuclear magnetic resonance (NMR). The dynamics of NMR structures is demonstrated by an ensemble of a number of overlaid structures. This cannot be seen in one structure determined by diffraction methods. However, it is possible to see the flexibility of a protein molecule in a number of structures of the same protein determined by X-ray techniques which is manifested by different conformations of main-chain. Multiple protein structure determination does not provide identical structures as a result of various factors including flexibility. Overlap of structures of a protein determined at atomic resolution with high accuracy shows that the root-mean-square deviations (rmsd) of main-chain atoms exceed several fold the accuracy of the positional parameters of each structure. Overlap of a number of structures of a protein determined by diffraction methods shows a similar distribution as that determined by NMR. These observations are demonstrated using high resolution structures of Streptomyces aureofaciens ribonucleases, their mutants and complexes with ligands.     

Crystal structures of aspartate carbamoyltransferase ligated with phosphonoacetamide, malonate, and CTP or ATP at 2.8-A resolution and neutral pH

The R-state structures of the ATP and CTP complexes of aspartate carbamoyltransferase ligated with phosphonoacetamide and malonate have been determined at 2.8-A resolution and neutral pH. These structures were solved by the method of molecular replacement and were refined to crystallographic residuals between 0.167 and 0.182. The triphosphate, the ribose, and the purine and pyrimidine moieties of ATP and CTP interact with similar regions of the allosteric domain of the regulatory dimer. ATP and CTP relatively increase and decrease the size of the allosteric site in the vicinity of the base, respectively. For both CTP and ATP at pH 7, the gamma-phosphates are bound to His20 and are also near Lys94, while the alpha-phosphates interact exclusively with Lys94. The 2'-hydroxyls of both CTP and ATP are near the amino group of Lys60. The pyrimidine ring of CTP makes specific hydrogen bonds at the allosteric site: the NH2 group donates hydrogen bonds to the main-chain carbonyls of Ile12 and Tyr89 and the pyrimidine ring carbonyl oxygen accepts a hydrogen bond from the amino group of Lys60; the nitrogen at position 3 in the pyrimidine ring is hydrogen bonded to a main-chain NH group of Ile12. The purine ring of ATP also makes numerous interactions with residues at the allosteric site: the purine NH2 (analogous to the amino group of CTP) donates a hydrogen bond to the main-chain carbonyl oxygen of Ile12, the N3 nitrogen interacts with the amino group of Lys60, and the N1 nitrogen hydrogen bonds to the NH group of Ile12. The binding of CTP and ATP to the allosteric site in the presence of phosphonoacetamide and malonate does not dramatically alter the structure of the allosteric binding site or of the allosteric domain. Nonetheless, in the CTP-ligated structure, the average separation between the catalytic trimers decreases by approximately 0.5 A, indicating a small shift of the quaternary structure toward the T state. In the CTP- and ATP-ligated R-state structures, the binding and occupancy of phosphonoacetamide and malonate are similar and the structures of the active sites are similar at the current resolution of 2.8 A.     

A conserved interaction with the chromophore of fluorescent proteins

The chromophore of fluorescent proteins, including the green fluorescent protein (GFP), contains a highly conjugated imidazolidinone ring. In many fluorescent proteins, the carbonyl group of the imidazolidinone ring engages in a hydrogen bond with the side chain of an arginine residue. Prior studies have indicated that such an electrophilic carbonyl group in a protein often accepts electron density from a main-chain oxygen. A survey of high-resolution structures of fluorescent proteins indicates that electron lone pairs of a main-chain oxygen-Thr62 in GFP-donate electron density into an antibonding orbital of the imidazolidinone carbonyl group. This n→π* electron delocalization prevents structural distortion during chromophore excitation that could otherwise lead to fluorescence quenching. In addition, this interaction is present in on-pathway intermediates leading to the chromophore, and thus could direct its biogenesis. Accordingly, this n→π* interaction merits inclusion in computational and photophysical analyses of the chromophore, and in speculations about the molecular evolution of fluorescent proteins.     

二聚体蝎钠通道毒素的1.4(A)分辨率晶体结构:反常非脯氨酸顺式肽键及其内在结构因素

报道了以二聚体存在的dimo-BmK M1的1．4A分辨率晶体结构．蛋白质中的肽键是局部双键,不可旋转,因此具有顺式（cis）和反式（trans）两种构型,它们不能通过旋转操作相互转换．非脯氨酸顺式肽键是指形成该肽键的氨基是由脯氨酸以外的氨基酸提供的（Xaa-nonPro）,这类肽键的顺式构型的自由能远比反式高,因此极少出现在天然蛋白质结构中．事实上,在长时间中,多肽链的“反式肽键连接”被视为蛋白质结构的一条基本规则,把顺式肽键视为不可能．随着高分辨率精确蛋白质结构数量的增加,近年来有详细的统计分析揭示,非脯氨酸顺式肽键（Xaa-nPro）在蛋白质结构中出现的几率为0．03％～0．05％,而且大多存在于功能敏感的结构区域,可能具有重要意义．但由于所用的基本结构数据都来自晶体结构,对这种反常肽键是否由结晶环境影响而形成,存在疑问．此前曾在以单体形式存在的蝎神经毒素mono-BmK M1的高分辨率结构中发现其中肽键Pr09-His10是非脯氨酸顺式肽键,并详细分析了其结构．功能意义．以二聚体存在的dimo-BmK M1的1．4A分辨率晶体结构表明,它与mono．BmK M1有不同的空间群、不同的分子堆积方式,不同的晶体环境．结构模型被高度精化,Rcryst达到0．109．dimo-BmK M1结构显示,在不对称单位中的两个M1分子在同一位置（残基9．10之间）都清晰地存在顺式肽键．立体化学分析显示,这一肽键的几何参数和局部结构与mono．BmK M1中的（9．10）顺式肽键基本相同．这一结果表明,非脯氨酸顺式肽键9．10的存在与结晶环境无关,是BmK M1分子的固有结构特征．在此基础上,综合分析了与顺式、反式肽键相关的结构元素,发现与残基（8．19）序列模体-KPXNC-（X为任意氨基酸）所决定的特征回折结构可能是分子内在的主要结构因素,其中第8位残基是Lys或Asp对决定肽键是顺式还是反式有关键作用．近来的突变实验及其晶体结构测定已证实,Lys8／Asp8是（9-10）肽键顺式／反式异构的结构开关,它们对该类分子与不同种属钠通道作用的专一选择性具有重要作用．通过BLAST搜索,发现在其他18个蛋白质中也存在相同的序列模体．KPXNC-,推测在这些蛋白质的相应肽键位置也可能存在反常的脯氨酸顺式肽键。     

Solution conformation of the Met 61 to His 61 mutant of Pseudomonas stutzeri ZoBell ferrocytochrome c-551

The gene encoding for bacterial cytochrome c-551 from Pseudomonas stutzeri substrain ZoBell has been mutated to convert the invariant sixth ligand methionine residue into histidine, creating the site-specific mutant M61H. Proton NMR resonance assignments were made for all main-chain and most-side chain protons in the diamagnetic, reduced form at pH 9.2 and 333 K by two-dimensional NMR techniques. Distance constraints (1074) were determined from nuclear Overhauser enhancements and main-chain torsion-angle constraints (72) from scalar coupling estimates. Solution conformations for the protein were computed by the simulated annealing approach. For 28 computed structures, the root mean squared displacement from the average structure excluding the terminal residues 1, 2, 81, and 82 was 0.52 A (sigma = 0.096) for backbone atoms and 0.90 A (sigma = 0.122) for all heavy atoms. The global folding of the mutant protein is the same as for wild type. The biggest changes are localized in a peptide span over residues 60-65. The most striking behavior of the mutant protein is that at room temperature and neutral pH it exists in a state similar to the molten globular state that has been described for several proteins under mild denaturing conditions, but the mutant converts to a more ordered state at high pH and temperature.     

Refined crystal structure of troponin C from turkey skeletal muscle at 2.0 A resolution

The crystal structure of troponin C from turkey skeletal muscle has been refined at 2.0 A resolution (1 A = 0.1 nm). The resulting crystallographic R factor (R = sigma[[Fo[-[Fc[[/sigma[Fo[, where [Fo[ and [Fc[ are the observed and calculated structure factor amplitudes) is 0.155 for the 8054 reflections with intensities I greater than or equal to 2 sigma(I) within the 10 A to 2.0 A resolution range. With 66% of the residues in helical conformation, troponin C provides a good sample for helix analysis. The mean alpha-helix dihedral angles (phi, psi = -62 degrees, -42 degrees) agree with values observed for helical regions in other proteins. The helices are all curved and/or kinked. In particular, the 31 amino acid long inter-domain helix is smoothly curved, with a rather large radius of curvature of 137 A. Helix packing is different in the Ca2+-free domain (N-terminal) and the Ca2+-bound domain (C-terminal). The inter-helix angles for the two helix-loop-helix motifs in the regulatory domain are 133 degrees and 151 degrees, whereas the value for the two motifs in the C-terminal domain is 110 degrees, as observed in the EF-hands of parvalbumin. These differences affect the packing of the respective hydrophobic cores of each domain, in particular the disposition of aromatic rings. Pairwise arrangement of Ca2+-binding loops is common to both states, but the conformation is markedly different. Conversion of one to the other can be achieved by small cumulative changes of main-chain dihedral angles. The integrity of loop structure is maintained by numerous electrostatic interactions. Both salt bridges and carboxyl-carboxylate interactions are observed in TnC. There are more intramolecular (9) than intermolecular (1) salt bridges. Carboxyl-carboxylate interactions occur because the pH of the crystals is 5.0 and there is a multitude of aspartate and glutamate residues. One is intramolecular and four are intermolecular. Polar side-chain interactions occur more commonly with main-chain carbonyls and amides than with other polar side-chains. These interactions are mostly short range, and are similar to those observed in other proteins with one exception: negatively charged side-chains interact more frequently with main-chain carbonyl oxygen atoms. However, out of 19 such interactions, 10 involve oxygen atoms of the Ca2+ ligands. These unfavorable interactions are compensated by the favorable interactions with the Ca2+ ions and with main-chain amides. They are a trivial consequence of the tight fold of the Ca2+-binding loops.