X‐ray crystal structure of the N‐terminal region of Moloney murine leukemia virus integrase and its implications for viral DNA recognition

The retroviral integrase (IN) carries out the integration of a dsDNA copy of the viral genome into the host DNA, an essential step for viral replication. All IN proteins have three general domains, the N‐terminal domain (NTD), the catalytic core domain, and the C‐terminal domain. The NTD includes an HHCC zinc finger‐like motif, which is conserved in all retroviral IN proteins. Two crystal structures of Moloney murine leukemia virus (M‐MuLV) IN N‐terminal region (NTR) constructs that both include an N‐terminal extension domain (NED, residues 1–44) and an HHCC zinc‐finger NTD (residues 45–105), in two crystal forms are reported. The structures of IN NTR constructs encoding residues 1–105 (NTR_1–105) and 8–105 (NTR_8–105) were determined at 2.7 and 2.15 Å resolution, respectively and belong to different space groups. While both crystal forms have similar protomer structures, NTR_1–105 packs as a dimer and NTR_8–105 packs as a tetramer in the asymmetric unit. The structure of the NED consists of three anti‐parallel β‐strands and an α‐helix, similar to the NED of prototype foamy virus (PFV) IN. These three β‐strands form an extended β‐sheet with another β‐strand in the HHCC Zn²⁺ binding domain, which is a unique structural feature for the M‐MuLV IN. The HHCC Zn²⁺ binding domain structure is similar to that in HIV and PFV INs, with variations within the loop regions. Differences between the PFV and MLV IN NEDs localize at regions identified to interact with the PFV LTR and are compared with established biochemical and virological data for M‐MuLV. Proteins 2017; 85:647–656. © 2016 Wiley Periodicals, Inc.     

Crystal structure of the secreted protein HP1454 from the human pathogen Helicobacter pylori

HP1454 is a protein of 303 amino acids found in the extracellular milieu of Helicobacter pylori. The protein structure, crystallized in the orthorhombic C222₁ space group with one molecule per asymmetric unit, has been determined using the single‐wavelength anomalous dispersion method. HP1454 exhibits an elongated bent shape, composed of three distinct domains. Each domain possesses a fold already present in other structures: Domain I contains a three‐strand antiparallel β‐barrel flanked by a long α‐helix, Domain II is an anti‐parallel three‐helix bundle, and Domain III a β‐sheet flanked by two α‐helices. The overall assembly of the protein does not bear any similarity with known structures. Proteins 2014; 82:2868–2873. © 2014 Wiley Periodicals, Inc.     

Structural analysis of lysine‐4 methylated histone H3 proteins using synchrotron radiation circular dichroism spectroscopy

We report structural alterations of histone H3 proteins induced by lysine‐4 (K4) monomethylation, dimethylation, and trimethylation identified by using synchrotron radiation circular dichroism spectroscopy. Compared with unmethylated H3, monomethylation and dimethylation induced increases in α‐helix structures and decreases in β‐strand structures. In contrast, trimethylation decreased α‐helix content but increased β‐strand content. The structural differences among K4‐unmethylated/methylated H3 may allow epigenetic enzymes to discriminate the substrates both chemically and sterically.     

Comparison of the three‐dimensional structures of a humanized and a chimeric Fab of an anti‐γ‐interferon antibody

The objective of this work is to compare the three‐dimensional structures of “humanized” and mouse–human chimeric forms of a murine monoclonal antibody elicited against human γ‐interferon. It is also to provide structural explanations for the small differences in the affinities and biological interactions of the two molecules for this antigen. Antigen‐binding fragments (Fabs) were produced by papain hydrolysis of the antibodies and crystallized with polyethylene glycol (PEG) 8000 by nearly identical microseeding procedures. Their structures were solved by X‐ray analyses at 2.9 Å resolution, using molecular replacement methods and crystallographic refinement. Comparison of these structures revealed marked similarities in the light (L) chains and near identities of the constant (C) domains of the heavy (H) chains. However, the variable (V) domains of the heavy chains exhibited substantial differences in the conformations of all three complementarity‐determining regions (CDRs), and in their first framework segments (FR1). In FR1 of the humanized V_H, the substitution of serine for proline in position 7 allowed the N‐terminal segment (designated strand 4‐1) to be closely juxtaposed to an adjacent strand (4‐2) and form hydrogen bonds typical of an antiparallel β‐pleated sheet. The tightening of the humanized structure was relayed in such a way as to decrease the space available for the last portion of HFR1 and the first part of HCDR1. This compression led to the formation of an α‐helix involving residues 25–32. With fewer steric constraints, the corresponding segment in the chimeric Fab lengthened by at least 1 Å to a random coil which terminated in a single turn of 3₁₀ helix. In the humanized Fab, HCDR1, which is sandwiched between HCDR2 and HCDR3, significantly influenced the structures of both regions. HCDR2 was forced into a bent and twisted orientation different from that in the chimeric Fab, both at the crown of the loop (around proline H52a) and at its base. As in HCDR1, the last few residues of HCDR2 in the humanized Fab were compressed into a space‐saving α‐helix, contrasting with a more extended 3₁₀ helix in the chimeric form. HCDR3 in the humanized Fab was also adjusted in shape and topography. The observed similarities in the functional binding activities of the two molecules can be rationalized by limited induced fit adjustments in their structures on antigen binding. While not perfect replicas, the two structures are testimonials to the progress in making high affinity monoclonal antibodies safe for human use. Copyright © 1999 John Wiley & Sons, Ltd.     

A critical survey of average distances between catalytic carboxyl groups in glycoside hydrolases

Published X‐ray crystallographic structures for glycoside hydrolases (GHs) from 39 different families are surveyed according to some rigorous selection criteria, and the distances separating 208 pairs of catalytic carboxyl groups (20 α‐retaining, 87 β‐retaining, 38 α‐inverting, and 63 β‐inverting) are analyzed. First, the average of all four inter‐carboxyl O^…O distances for each pair is determined; second, the mean of all the pair‐averages within each GH family is determined; third, means are determined for groups of GH families. No significant differences are found for free structures compared with those complexed with a ligand in the active site of the enzyme, nor for α‐GHs as compared with β‐GHs. The mean and standard deviation (1σ) of the unimodal distribution of average O^…O distances for all families of inverting GHs is 8 ± 2Å, with a very wide range from 5Å (GH82) to nearly 13Å (GH46). The distribution of average O^…O distances for all families of retaining GHs appears to be bimodal: the means and standard deviations of the two groups are 4.8 ± 0.3Å and 6.4 ± 0.6Å. These average values are more representative, and more likely to be meaningful, than the often‐quoted literature values, which are based on a very small sample of structures. The newly‐updated average values proposed here may alter perceptions about what separations between catalytic residues are “normal” or “abnormal” for GHs. Proteins 2014; 82:1747–1755. © 2014 Wiley Periodicals, Inc.     

Using homology modeling to interrogate binding affinity in neutralization of ricin toxin by a family of single domain antibodies

In this report we investigated, within a group of closely related single domain camelid antibodies (V_HHs), the relationship between binding affinity and neutralizing activity as it pertains to ricin, a fast‐acting toxin and biothreat agent. The V1C7‐like V_HHs (V1C7, V2B9, V2E8, and V5C1) are similar in amino acid sequence, but differ in their binding affinities and toxin‐neutralizing activities. Using the X‐ray crystal structure of V1C7 in complex with ricin's enzymatic subunit (RTA) as a template, Rosetta‐based homology modeling coupled with energetic decomposition led us to predict that a single pairwise interaction between Arg29 on V5C1 and Glu67 on RTA was responsible for the difference in ricin toxin binding affinity between V1C7, a weak neutralizer, and V5C1, a moderate neutralizer. This prediction was borne out experimentally: substitution of Arg for Gly at position 29 enhanced V1C7's binding affinity for ricin, whereas the reverse (ie, Gly for Arg at position 29) diminished V5C1's binding affinity by >10 fold. As expected, the V5C1_R29G mutant was largely devoid of toxin‐neutralizing activity (TNA). However, the TNA of the V1C7_G29R mutant was not correspondingly improved, indicating that in the V1C7 family binding affinity alone does not account for differences in antibody function. V1C7 and V5C1, as well as their respective point mutants, recognized indistinguishable epitopes on RTA, at least at the level of sensitivity afforded by hydrogen‐deuterium mass spectrometry. The results of this study have implications for engineering therapeutic antibodies because they demonstrate that even subtle differences in epitope specificity can account for important differences in antibody function.     

Cover Caption: Organization of Actin Filaments

Plant actin depolymerizing factor (ADF) binds to both monomeric and filamentous actin, and plays a key role in the organization of the actin cytoskeleton. In this issue, Dong et al. (pp. 250–261) demonstrate that charged residues Arg98 and Lys100 of ADF1 are essential for both G‐ and F‐actin binding, and that basic residues on β‐strand 5 (K82/A) and α‐helix 4 (R135/A, R137/A) form another actin binding site for F‐actin.     

Revisiting the Ramachandran plot: hard-sphere repulsion, electrostatics, and H-bonding in the alpha-helix

What determines the shape of the allowed regions in the Ramachandran plot? Although Ramachandran explained these regions in terms of 1–4 hard‐sphere repulsions, there are discrepancies with the data where, in particular, the α_R, α_L, and β‐strand regions are diagonal. The α_R‐region also varies along the α‐helix where it is constrained at the center and the amino terminus but diffuse at the carboxyl terminus. By analyzing a high‐resolution database of protein structures, we find that certain 1–4 hard‐sphere repulsions in the standard steric map of Ramachandran do not affect the statistical distributions. By ignoring these steric clashes (N···H_i+1 and O_i?1···C), we identify a revised set of steric clashes (C^β···O, O_i?1···N_i+1, C^β···N_i+1, O_i?1···C^β, and O_i?1···O) that produce a better match with the data. We also find that the strictly forbidden region in the Ramachandran plot is excluded by multiple steric clashes, whereas the outlier region is excluded by only one significant steric clash. However, steric clashes alone do not account for the diagonal regions. Using electrostatics to analyze the conformational dependence of specific interatomic interactions, we find that the diagonal shape of the α_R and α_L‐regions also depends on the optimization of the N···H_i+1 and O_i?1···C interactions, and the diagonal β‐strand region is due to the alignment of the CO and NH dipoles. Finally, we reproduce the variation of the Ramachandran plot along the α‐helix in a simple model that uses only H‐bonding constraints. This allows us to rationalize the difference between the amino terminus and the carboxyl terminus of the α‐helix in terms of backbone entropy.     

Functional and structural studies of pullulanase from Anoxybacillus sp. LM18‐11

Pullulanase is a debranching enzyme that specifically hydrolyzes the α‐1,6 glycosidic linkage of α‐glucans, and has wide industrial applications. Here, we report structural and functional studies of a new thermostable pullulanase from Anoxybacillus sp. LM18‐11 (PulA). Based on the hydrolysis products, PulA was classified as a type I pullulanase. It showed maximum activity at 60°C and pH 6.0. Kinetic study showed that the specific activity and K_m for pullulan of PulA are 750 U mg^?1 and 16.4 μmol L^?1, respectively. PulA has a half‐life of 48 h at 60°C. The remarkable thermostability makes PulA valuable for industrial usage. To further investigate the mechanism of the enzyme, we solved the crystal structures of PulA and its complexes with maltotriose and maltotetraose at 1.75–2.22 Å resolution. The PulA structure comprises four domains (N1, N2, A, and C). A is the catalytic domain, in which three conserved catalytic residues were identified (D413, E442, and D526). Two molecules of oligosaccharides were seen in the catalytic A domain in a parallel binding mode. Interestingly, another two oligosaccharides molecules were found between the N1 domain and the loop between the third β‐strand and the third α‐helix in the A domain. Based on sequence alignment and the ligand binding pattern, the N1 domain is identified as a new type of carbohydrate‐binding motif and classified to the CBM68 family. The structure solved here is the first structure of pullulanase which has carbohydrate bound to the N1 domain. Proteins 2014; 82:1685–1693. © 2013 Wiley Periodicals, Inc.     

Basic conformers in β‐peptides

The conformation of oligomers of β‐amino acids of the general type Ac‐[β‐Xaa]_n‐NHMe (β‐Xaa = β‐Ala, β‐Aib, and β‐Abu; n = 1–4) was systematically examined at different levels of ab initio molecular orbital theory (HF/6‐31G*, HF/3‐21G). The solvent influence was considered employing two quantum‐mechanical self‐consistent reaction field models. The results show a wide variety of possibilities for the formation of characteristic elements of secondary structure in β‐peptides. Most of them can be derived from the monomer units of blocked β‐peptides with n = 1. The stability and geometries of the β‐peptide structures are considerably influenced by the side‐chain positions, by the configurations at the C^α‐ and C^β‐atoms of the β‐amino acid constituents, and especially by environmental effects. Structure peculiarities of β‐peptides, in particular those of various helix alternatives, are discussed in relation to typical elements of secondary structure in α‐peptides. © 1999 John Wiley & Sons, Inc. Biopoly 50: 167–184, 1999     

Virtual screening on an α‐helix to β‐strand switchable region of the FGFR2 extracellular domain revealed positive and negative modulators

The secondary structure of some protein segments may vary between α‐helix and β‐strand. To predict these switchable segments, we have developed an algorithm, Switch‐P, based solely on the protein sequence. This algorithm was used on the extracellular parts of FGF receptors. For FGFR2, it predicted that β4 and β5 strands of the third Ig‐like domain were highly switchable. These two strands possess a high number of somatic mutations associated with cancer. Analysis of PDB structures of FGF receptors confirmed the switchability prediction for β5. We thus evaluated if compound‐driven α‐helix/β‐strand switching of β5 could modulate FGFR2 signaling. We performed the virtual screening of a library containing 1.4 million of chemical compounds with two models of the third Ig‐like domain of FGFR2 showing different secondary structures for β5, and we selected 32 compounds. Experimental testing using proliferation assays with FGF7‐stimulated SNU‐16 cells and a FGFR2‐dependent Erk1/2 phosphorylation assay with FGFR2‐transfected L6 cells, revealed activators and inhibitors of FGFR2. Our method for the identification of switchable proteinic regions, associated with our virtual screening approach, provides an opportunity to discover new generation of drugs with under‐explored mechanism of action. Proteins 2014; 82:2982–2997. © 2014 Wiley Periodicals, Inc.     

Large‐scale analysis of secondary structure changes in proteins suggests a role for disorder‐to‐order transitions in nucleotide binding proteins

Conformational changes in proteins often involve secondary structure transitions. Such transitions can be divided into two types: disorder‐to‐order changes, in which a disordered segment acquires an ordered secondary structure (e.g., disorder to α‐helix, disorder to β‐strand), and order‐to‐order changes, where a segment switches from one ordered secondary structure to another (e.g., α‐helix to β‐strand, α‐helix to turn). In this study, we explore the distribution of these transitions in the proteome. Using a comprehensive, yet highly conservative method, we compared solved three‐dimensional structures of identical protein sequences, looking for differences in the secondary structures with which they were assigned. Protein chains in which such secondary structure transitions were detected, were classified into two sets according to the type of transition that is involved (disorder‐to‐order or order‐to‐order), allowing us to characterize each set by examining enrichment of gene ontology terms. The results reveal that the disorder‐to‐order set is significantly enriched with nucleotide binding proteins, whereas the order‐to‐order set is more diverse. Remarkably, further examination reveals that >22% of the purine nucleotide binding proteins include segments which undergo disorder‐to‐order transitions, suggesting that such transitions play an important role in this process. Proteins 2010. © 2009 Wiley‐Liss, Inc.     

BuildBeta—A system for automatically constructing beta sheets

We describe a method that can thoroughly sample a protein conformational space given the protein primary sequence of amino acids and secondary structure predictions. Specifically, we target proteins with β‐sheets because they are particularly challenging for ab initio protein structure prediction because of the complexity of sampling long‐range strand pairings. Using some basic packing principles, inverse kinematics (IK), and β‐pairing scores, this method creates all possible β‐sheet arrangements including those that have the correct packing of β‐strands. It uses the IK algorithms of ProteinShop to move α‐helices and β‐strands as rigid bodies by rotating the dihedral angles in the coil regions. Our results show that our approach produces structures that are within 4–6 Å RMSD of the native one regardless of the protein size and β‐sheet topology although this number may increase if the protein has long loops or complex α‐helical regions. Proteins 2010. © Published 2009 Wiley‐Liss, Inc.     

3(10)-Helix adjoining alpha-helix and beta-strand: sequence and structural features and their conservation

Does the amino acid use at the terminal positions of an α‐helix become altered depending on the context—more specifically, when there is an adjoining 3₁₀‐helix, and can a single helical cylinder encompass the resultant composite helix? An analysis of 138 and 107 cases of 3₁₀–α and α–3₁₀ composite helices, respectively, found in known protein structures indicate that the secondary structural element occurring first imposes its characteristics on the sequence of the structural element coming next. Thus, when preceded by a 3₁₀‐helix, the preference of proline to occur at the N1 position of an α‐helix is shifted to the N2 position, a typical characteristic of the C‐terminal capping of the 3₁₀‐helix. When an α‐ or a 3₁₀‐helix leads into a helix of the other type, there is a bend at the junction, especially for the 3₁₀–α composite, with the two junction residues facing inward and buried within the structure. Thus a single helical cylinder may not properly represent a composite helix, the bend providing a means for the tertiary structure to assume a globular shape, very much akin to what a proline‐induced kink does to an α‐helix. The tertiary structural context in which β–3₁₀ and 3₁₀–β composites occurs can be different, causing the angle between the secondary structural elements in the two cases to be different. Composites of 3₁₀‐helices and β‐strands are much more conserved among members in families of homologous structures than those between two types of helices; in many of the former instances, the 3₁₀‐helix constitutes the loops in β‐hairpin or β–β‐corner motifs. The overall fold of the chain may be more conserved than the actual identify of the secondary structure elements in a composite. © 2005 Wiley Periodicals, Inc. Biopolymers 78: 147–162, 2005 This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Solution NMR and molecular dynamics reveal a persistent alpha helix within the dynamic region of PsbQ from photosystem II of higher plants

The extrinsic proteins of photosystem II of higher plants and green algae PsbO, PsbP, PsbQ, and PsbR are essential for stable oxygen production in the oxygen evolving center. In the available X‐ray crystallographic structure of higher plant PsbQ residues S14‐Y33 are missing. Building on the backbone NMR assignment of PsbQ, which includes this “missing link”, we report the extended resonance assignment including side chain atoms. Based on nuclear Overhauser effect spectra a high resolution solution structure of PsbQ with a backbone RMSD of 0.81 Å was obtained from torsion angle dynamics. Within the N‐terminal residues 1–45 the solution structure deviates significantly from the X‐ray crystallographic one, while the four‐helix bundle core found previously is confirmed. A short α‐helix is observed in the solution structure at the location where a β‐strand had been proposed in the earlier crystallographic study. NMR relaxation data and unrestrained molecular dynamics simulations corroborate that the N‐terminal region behaves as a flexible tail with a persistent short local helical secondary structure, while no indications of forming a β‐strand are found. Proteins 2015; 83:1677–1686. © 2015 The Authors. Proteins: Structure, Function, and Bioinformatics Published by Wiley Periodicals, Inc.     

Helix‐sheet packing in proteins

The three‐dimensional structure of a protein is organized around the packing of its secondary structure elements. Although much is known about the packing geometry observed between α‐helices and between β‐sheets, there has been little progress on characterizing helix–sheet interactions. We present an analysis of the conformation of αβ₂ motifs in proteins, corresponding to all occurrences of helices in contact with two strands that are hydrogen bonded. The geometry of the αβ₂ motif is characterized by the azimuthal angle θ between the helix axis and an average vector representing the two strands, the elevation angle ψ between the helix axis and the plane containing the two strands, and the distance D between the helix and the strands. We observe that the helix tends to align to the two strands, with a preference for an antiparallel orientation if the two strands are parallel; this preference is diminished for other topologies of the β‐sheet. Side‐chain packing at the interface between the helix and the strands is mostly hydrophobic, with a preference for aliphatic amino acids in the strand and aromatic amino acids in the helix. From the knowledge of the geometry and amino acid propensities of αβ₂ motifs in proteins, we have derived different statistical potentials that are shown to be efficient in picking native‐like conformations among a set of non‐native conformations in well‐known decoy datasets. The information on the geometry of αβ₂ motifs as well as the related statistical potentials have applications in the field of protein structure prediction. Proteins 2010. © 2010 Wiley‐Liss, Inc.     

Exploring the free energy landscape of a model β‐hairpin peptide and its isoform

Secondary structural transitions from α‐helix to β‐sheet conformations are observed in several misfolding diseases including Alzheimer's and Parkinson's. Determining factors contributing favorably to the formation of each of these secondary structures is therefore essential to better understand these disease states. β‐hairpin peptides form basic components of anti‐parallel β‐sheets and are suitable model systems for characterizing the fundamental forces stabilizing β‐sheets in fibrillar structures. In this study, we explore the free energy landscape of the model β‐hairpin peptide GB1 and its E2 isoform that preferentially adopts α‐helical conformations at ambient conditions. Umbrella sampling simulations using all‐atom models and explicit solvent are performed over a large range of end‐to‐end distances. Our results show the strong preference of GB1 and the E2 isoform for β‐hairpin and α‐helical conformations, respectively, consistent with previous studies. We show that the unfolded states of GB1 are largely populated by misfolded β‐hairpin structures which differ from each other in the position of the β‐turn. We discuss the energetic factors contributing favorably to the formation of α‐helix and β‐hairpin conformations in these peptides and highlight the energetic role of hydrogen bonds and non‐bonded interactions. Proteins 2014; 82:2394–2402. © 2014 Wiley Periodicals, Inc.     

Inter‐subunit interaction of gastric H+,K+‐ATPase prevents reverse reaction of the transport cycle

The gastric H⁺,K⁺‐ATPase is an ATP‐driven proton pump responsible for generating a million‐fold proton gradient across the gastric membrane. We present the structure of gastric H⁺,K⁺‐ATPase at 6.5 Å resolution as determined by electron crystallography of two‐dimensional crystals. The structure shows the catalytic α‐subunit and the non‐catalytic β‐subunit in a pseudo‐E₂P conformation. Different from Na⁺,K⁺‐ATPase, the N‐terminal tail of the β‐subunit is in direct contact with the phosphorylation domain of the α‐subunit. This interaction may hold the phosphorylation domain in place, thus stabilizing the enzyme conformation and preventing the reverse reaction of the transport cycle. Indeed, truncation of the β‐subunit N‐terminus allowed the reverse reaction to occur. These results suggest that the β‐subunit N‐terminus prevents the reverse reaction from E₂P to E₁P, which is likely to be relevant for the generation of a large H⁺ gradient in vivo situation.     

Intermolecular versus intramolecular interactions of the vinculin binding site 33 of talin

The cytoskeletal proteins talin and vinculin are localized at cell‐matrix junctions and are key regulators of cell signaling, adhesion, and migration. Talin couples integrins via its FERM domain to F‐actin and is an important regulator of integrin activation and clustering. The 220 kDa talin rod domain comprises several four‐ and five‐helix bundles that harbor amphipathic α‐helical vinculin binding sites (VBSs). In its inactive state, the hydrophobic VBS residues involved in binding to vinculin are buried within these helix bundles, and the mechanical force emanating from bound integrin receptors is thought necessary for their release and binding to vinculin. The crystal structure of a four‐helix bundle of talin that harbors one of these VBSs, coined VBS33, was recently determined. Here we report the crystal structure of VBS33 in complex with vinculin at 2 Å resolution. Notably, comparison of the apo and vinculin bound structures shows that intermolecular interactions of the VBS33 α‐helix with vinculin are more extensive than the intramolecular interactions of the VBS33 within the talin four‐helix bundle.