Crystal structure of the lectin of Camptosema pedicellatum: implications of a conservative substitution at the hydrophobic subsite

Lectins have been used as models for studies of the molecular basis of protein-carbohydrate interaction and specificity by deciphering codes present in the glycan structures. The purpose of the present study was to purify and solve the complete primary and crystal structure of the lectin of Camptosema pedicellatum (CPL) complexed with 5-bromo-4-chloro-3-indolyl-α-d-mannose (X-Man) using tandem mass spectrometry. CPL was purified by single-step affinity chromatography. Mass spectrometry findings revealed that purified CPL features a combination of chains weighing 25,298 ± 2 (α-chain), 12,835 ± 2 (β-chain) and 12,481 ± 2 Da (γ-chain). The solved crystal structure of CPL features a conservative mutation in the hydrophobic subsite, a constituent of the carbohydrate recognition domain (CRD), indicating the relevance of hydrophobic interactions in the establishment of interactions with carbohydrates. The substitution and the analysis of the interactions with X-Man also revealed that the hydrophobic effect caused by a minor change in the hydrophobic subsite interferes in the formation of H-bonds due to the reorientation of the indolyl group in the CRD.     

Neutron crystallography, molecular dynamics, and quantum mechanics studies of the nature of hydrogen bonding in cellulose Ibeta

In the crystal structure of cellulose I beta, disordered hydrogen bonding can be represented by the average of two mutually exclusive hydrogen bonding schemes that have been designated A and B. An unanswered question is whether A and B interconvert dynamically, or whether they are static but present in different regions of the microfibril (giving temporally or a spatially averaged structures, respectively). We have used neutron crystallographic techniques to determine the occupancies of A and B at 295 and 15 K, quantum mechanical calculations to compare the energies of A and B, and molecular dynamics calculations to look at the stability of A. Microfibrils are found to have most chains arranged in a crystalline I beta structure with hydrogen bonding scheme A. Smaller regions of static disorder exist, perhaps at defects within or between crystalline domains in which the hydrogen bonding is complex but with certain features that are found in B.     

The crystal structure of Bombyx mori silk fibroin at the air–water interface

A new crystalline polymorph of Bombyx mori silk, which forms at the air–water interface, has been characterized. A previous study found this structure to be trigonal, and to be distinctly different than the two previously observed silk crystal structures, silk I and silk II. This new structure was named silk III. Identification of this new silk polymorph was based on evidence from transmission electron microscopy and electron diffraction, coupled with molecular modeling. In the current paper, additional data enables us to refine our model of the silk III structure. Some single crystal electron diffraction patterns indicate a deviation in symmetry away from a perfect trigonal unit cell to monoclinic unit cell. The detailed shape of the powder diffraction peaks also supports a monoclinic cell. The monoclinic crystal structure has an nonprimitive unit cell incorporating a slightly distorted hexagonal packing of silk molecular helices. The chains each assume a threefold helical conformation, resulting in a crystal structure similar to that observed for polyglycine II, but with some additional sheet-like packing features common to the threefold helical crystalline forms of many glycine-rich polypeptides. © 1997 John Wiley & Sons, Inc. Biopoly 42: 705–717, 1997     

Time-resolved X-ray diffraction study on poly[(R)-3-hydroxybutyrate] films during two-step-drawing: generation mechanism of planar zigzag structure

Uniaxially oriented films with high tensile strength were processed from ultrahigh-molecular-weight poly[(R)-3-hydroxybutyrate] (P(3HB)) by a method combining hot-drawing near the melting point of the polymer and two-step-drawing at room temperature. In a two-step-drawn and subsequently annealed film, P(3HB) molecular chains fall into two states: 2/1 helix (alpha-form) and planar zigzag (beta-form) conformations. The mechanism for generating the beta-form during two-step-drawing was investigated by time-resolved synchrotron wide- and small-angle X-ray scattering measurements (WAXD and SAXS), together with the measurement of stress-strain curves. It was found that the improvement of mechanical properties is due to not only the orientation of molecular chains but also the generation of the beta-form during the drawing. The crystal and molecular structures of the alpha-form remained unchanged until the yield point of the stress-strain curve. At the yield point, the long period obtained from SAXS doubled and a new reflection indicative of the beta-form was observed on the equatorial line in WAXD. The intensity of the reflection from the beta-form increased with an increase in the two-step-drawing ratio at room temperature. The SAXS pattern changed from a two-point reflection along the meridian to a cross pattern with streaking on the equatorial line, demonstrating the close alignment of shish-kebab structures. The reflection intensity, crystal orientation and crystal size of the alpha-form decreased during two-step-drawing. Based on these results, the beta-form is mainly introduced from the orientation of free molecular chains in the amorphous regions between alpha-form lamellar crystals, but the structural transformation of molecular chains also occurs from the alpha-form to the beta-form at the deformed lamellar crystals.     

Similarity between protein-protein and protein-carbohydrate interactions, revealed by two crystal structures of lectins from the roots of pokeweed

The roots of pokeweed (Phytolacca americana) are known to contain the lectins designated PL-A, PL-B, PL-C, PL-D1, and PL-D2. Of these lectins, the crystal structures of two PLs, the ligand-free PL-C and the complex of PL-D2 with tri-N-acetylchitotriose, have been determined at 1.8A resolution. The polypeptide chains of PL-C and PL-D2 form three and two repetitive chitin-binding domains, respectively. In the crystal structure of the PL-D2 complex, one trisaccharide molecule is shared mainly between two neighboring molecules related to each other by a crystallographic 2(1)-screw axis, and infinite helical chains of complexed molecules are generated by the sharing of ligand molecules. The crystal structure of PL-C reveals that the molecule is a dimer of two identical subunits, whose polypeptide chains are located in a head-to-tail fashion by a molecular 2-fold axis. Three putative carbohydrate-binding sites in each subunit are located in the dimer interface. The dimerization of PL-C is performed through the hydrophobic interactions between the carbohydrate-binding sites of the opposite domains in the dimer, leading to a distinct dimerization mode from that of wheat-germ agglutinin. Three aromatic residues in each carbohydrate-binding site of PL-C are involved in the dimerization. These residues correspond to the residues that interact mainly with the trisaccharide in the PL-D2 complex and appear to mimic the saccharide residues in the complex. Consequently, the present structure of the PL-C dimer has no room for accommodating carbohydrate. The quaternary structure of PL-C formed through these putative carbohydrate-binding residues may lead to the lack of hemagglutinating activity.     

Correlation between biological activity and binding energy in systems of integrin with cyclic RGD-containing binders: a QM/MM molecular dynamics study

We here report a combined quantum mechanical/molecular mechanical (QM/MM) molecular dynamics (MD) study on the binding interactions between the α(V)β(3) integrin and eight cyclic arginine-glycine-aspartate (RGD) containing peptides. The initial conformation of each peptide within the binding site of the integrin was determined by docking the ligand to the reactive site of the integrin crystal structure with the aid of docking software FRED. The subsequent QM/MM MD simulations of the complex structures show that these eight cyclic RGD-peptides have a generally similar interaction mode with the binding site of the integrin to the cyclo(RGDf-N[M]V) analog found in the crystal structure. Still, there are subtle differences in the interactions of peptide ligands with the integrin, which contribute to the different inhibition activities. The averaged QM/MM protein-ligand interaction energy (IE) is remarkably correlated to the biological activity of the ligand. The IE, as well as a three-variable model which is somewhat interpretable, thus can be used to predict the bioactivity of a new ligand quantitatively, at least within a family of analogs. The present study establishes a helpful protocol for advancing lead compounds to potent inhibitors.     

Structure of plant photosystem I revealed by theoretical modeling

Photosystem (PS) I is a large membrane protein complex vital for oxygenic photosynthesis, one of the most important biological processes on the planet. We present an "atomic" model of higher plant PSI, based on theoretical modeling using the recent 4.4 angstroms x-ray crystal structure of PSI from pea. Because of the lack of information on the amino acid side chains in the x-ray structural model and the high cofactor content in this system, novel modeling techniques were developed. Our model reveals some important structural features of plant PSI that were not visible in the crystal structure, and our model sheds light on the evolutionary relationship between plant and cyanobacterial PSI.     

A molecular mechanical study of the structure of poly(alpha-aminoisobutyric acid).

A molecular mechanical study has been carried out to determine the most favorable conformation of poly(Aib) both in solution and in the solid state. An energetic approach to the packing has been carried out by studying the stability of pairs of poly(Aib) chains. The study reveals a higher stability of a 3(10)-helix when forming part of a dimer whereas in isolated molecules the alpha-helix structure seems to be more stable depending on the length of the chain and dielectric constant of the environment.     

Three-dimensional structure of the complexes of ribonuclease A with 2',5'-CpA and 3',5'-d(CpA) in aqueous solution, as obtained by NMR and restrained molecular dynamics.

The three-dimensional structure of the complexes of ribonuclease A with cytidyl-2',5'-adenosine (2',5'-CpA) and deoxycytidyl-3',5'-deoxyadenosine [3',5'-d(CpA)] in aqueous solution has been determined by 1H NMR methods in combination with restrained molecular dynamics calculations. Twenty-three intermolecular NOE cross-corrections for the 3',5'-d(CpA) complex and 19 for the 2',5'-CpA, together with about 1,000 intramolecular NOEs assigned for each complex, were translated into distance constraints and used in the calculation. No significant changes in the global structure of the enzyme occur upon complex formation. The side chains of His 12, Thr 45, His 119, and the amide backbone group of Phe 120 are involved directly in the binding of the ligands at the active site. The conformation of the two bases is anti in the two complexes, but differs from the crystal structure in the conformation of the two sugar rings in 3',5'-d(CpA), shown to be in the S-type region, as deduced from an analysis of couplings between the ribose protons. His 119 is found in the two complexes in only one conformation, corresponding to position A in the free protein. Side chains of Asn 67, Gln 69, Asn 71, and Glu 111 from transient hydrogen bonds with the adenine base, showing the existence of a pronounced flexibility of these enzyme side chains at the binding site of the downstream adenine. All other general features on the structures coincide clearly with those observed in the crystal state.     

The effect of sunlight on the protein crystals from Bacillus thuringiensis var. kurstaki HD1 and NRD12: A Raman spectroscopic study

The Raman spectrum of the endotoxin crystals from Bacillus thuringiensis var. kurstaki NRD12 is found to resemble closely that for crystals of the strain kurstaki HD1 (P. R. Carey et al., 1986). Since the Raman data provide detailed molecular information on the crystal proteins, the protoxins of HD1 and NRD12 must be in similar conformations in their respective crystals. Estimation of the protoxin secondary structure in NRD12 crystals, using the amide III and amide I′ Raman spectral features, gave 57% unordered, 25% α-helix, and 18% β-structure. This is very similar to the result for HD1, as is the finding that the aromatic amino acid side chains of the NRD12 protoxin in the crystal appear to have widespread accessibility to water molecules. The effect of sunlight irradiation on dried NRD12 or HD1 crystals was studied by recording the Raman spectrum of the crystals before and after irradiation under a solar simulator whose spectral output is essentially identical to that of sunlight at the earth's surface. The only Raman spectral change detected following 40-hr irradiation was a 35% reduction of the intensity of features near 760 and 1555 cm⁻¹ due to tryptophan sidechains, indicating that irradiation brings about widespread destruction of indole residues. Control experiments using α-chymotrypsin, which has prominent tryptophan features in its Raman spectrum, show that the destruction of tryptophan is not brought about by the direct photolysis of the indole residues by the sunlight photons. Since silkworm bioassays on crystals of HD1 irradiated for 40 hr under the solar simulator or by natural sunlight showed that the crystals had become atoxic, the present results highlight the role of tryptophan destruction in sunlight-mediated crystal inactivation.     

Molecular structure of L-lysyl-L-alanyl-L-alanine: a tripeptide found in histone H1

The crystal structure of L -lysyl-L -alanyl-L -alanine hydrochloride has been determined by x-ray diffraction. The peptide is in zwitterionic form with the carboxylic group deprotonated, and with positive charges both in the amino terminal and ?-amino groups of lysine. Crystals are monoclinic, space group P2₁ and Z = 4, with two peptide molecules in the asymmetric unit, which show different conformations. While one molecule has torsional angles for the Lys-Ala peptide bond (φ₂, φ₂) in the β-pleated sheet region, the values for the other molecule are close to those for the α-helix. This molecular flexibility is of interest for the study of H1 histone, which contains this sequence repeated several times. The two lysine residues show fully extended side chains. Two methanol molecules and two acetonitrile molecules are also present in the unit cell. An extensive network of hydrogen bonds and ionic interactions stabilize the crystal structure.     

Solution structure of a hydrophobic analogue of the winter flounder antifreeze protein.

The solution structure of a synthetic mutant type I antifreeze protein (AFP I) was determined in aqueous solution at pH 7.0 using nuclear magnetic resonance (NMR) spectroscopy. The mutations comprised the replacement of the four Thr residues by Val and the introduction of two additional Lys-Glu salt bridges. The antifreeze activity of this mutant peptide, VVVV2KE, has been previously shown to be similar to that of the wild type protein, HPLC6 (defined here as TTTT). The solution structure reveals an alphahelix bent in the same direction as the more bent conformer of the published crystal structure of TTTT, while the side chain chi1 rotamers of VVVV2KE are similar to those of the straighter conformer in the crystal of TTTT. The Val side chains of VVVV2KE assume the same orientations as the Thr side chains of TTTT, confirming the conservative nature of this mutation. The combined data suggest that AFP I undergoes an equilibrium between straight and bent helices in solution, combined with independent equilibria between different side chain rotamers for some of the amino acid residues. The present study presents the first complete sequence-specific resonance assignments and the first complete solution structure determination by NMR of any AFP I protein.     

Structural and biochemical studies of the hedamycin type II polyketide ketoreductase (HedKR): molecular basis of stereo- and regiospecificities

Bacterial aromatic polyketides that include many antibiotic and antitumor therapeutics are biosynthesized by the type II polyketide synthase (PKS), which consists of 5-10 stand-alone enzymatic domains. Hedamycin, an antitumor antibiotic polyketide, is uniquely primed with a hexadienyl group generated by a type I PKS followed by coupling to a downstream type II PKS to biosynthesize a 24-carbon polyketide, whose C9 position is reduced by hedamycin type II ketoreductase (hedKR). HedKR is homologous to the actinorhodin KR (actKR), for which we have conducted extensive structural studies previously. How hedKR can accommodate a longer polyketide substrate than the actKR, and the molecular basis of its regio- and stereospecificities, is not well understood. Here we present a detailed study of hedKR that sheds light on its specificity. Sequence alignment of KRs predicts that hedKR is less active than actKR, with significant differences in substrate/inhibitor recognition. In vitro and in vivo assays of hedKR confirmed this hypothesis. The hedKR crystal structure further provides the molecular basis for the observed differences between hedKR and actKR in the recognition of substrates and inhibitors. Instead of the 94-PGG-96 motif observed in actKR, hedKR has the 92-NGG-94 motif, leading to S-dominant stereospecificity, whose molecular basis can be explained by the crystal structure. Together with mutations, assay results, docking simulations, and the hedKR crystal structure, a model for the observed regio- and stereospecificities is presented herein that elucidates how different type II KRs recognize substrates with different chain lengths, yet precisely reduce only the C9-carbonyl group. The molecular features of hedKR important for regio- and stereospecificities can potentially be applied to biosynthesize new polyketides via protein engineering that rationally controls polyketide ketoreduction.     

Structure refinement and diffuse streak scattering of silk (Bombyx mori).

Reexamination of the crystal structure of silk (Bombyx mori) was carried out by X-ray diffraction method. Four molecular chains are contained in the rectangular unit cell with parameters, a = 9.38 A, b = 9.49 A, and c (fiber axis) = 6.98 A, and the space group P2(1)-C(2)2. Silk assumes the statistical crystal structure, in which two antipolar-antiparallel sheet structures with different orientations statistically occupy a crystal site with the ratio 2:1. The molecular conformation is essentially the same pleated sheet structure as Marsh, Corey and Pauling proposed. However, the sheet structure formed by hydrogen bonds assumes the antipolar antiparallel structure different from that proposed by Marsh, Corey and Pauling, in which the methyl groups of alanine residues alternately point to both sides of the sheet structure along the hydrogen bonding direction. The crystalline region of silk is composed of stacking of two antipolar antiparallel sheet structures with different orientations.     

Structure of the molecular chaperone prefoldin: unique interaction of multiple coiled coil tentacles with unfolded proteins

Prefoldin (GimC) is a hexameric molecular chaperone complex built from two related classes of subunits and present in all eukaryotes and archaea. Prefoldin interacts with nascent polypeptide chains and, in vitro, can functionally substitute for the Hsp70 chaperone system in stabilizing non-native proteins for subsequent folding in the central cavity of a chaperonin. Here, we present the crystal structure and characterization of the prefoldin hexamer from the archaeum Methanobacterium thermoautotrophicum. Prefoldin has the appearance of a jellyfish: its body consists of a double beta barrel assembly with six long tentacle-like coiled coils protruding from it. The distal regions of the coiled coils expose hydrophobic patches and are required for multivalent binding of nonnative proteins.     

Hydrophobic Surface Patches on LolA of Pseudomonas aeruginosa Are Essential for Lipoprotein Binding

Many lipoproteins reside in the outer membrane (OM) of Gram-negative bacteria, and their biogenesis is dependent on the Lol (localization of lipoproteins) system. The periplasmic chaperone LolA accepts OM-destined lipoproteins that are released from the inner membrane by the LolCDE complex and transfers them to the OM receptor LolB. The exact nature of the LolA-lipoprotein complex is still unknown. The crystal structure of Escherichia coli LolA features an open β-barrel covered by α helices that together constitute a hydrophobic cavity, which would allow the binding of one acyl chain. However, OM lipoproteins contain three acyl chains, and the stoichiometry of the LolA-lipoprotein complex is 1:1. Here we present the crystal structure of Pseudomonas aeruginosa LolA that projects clear hydrophobic surface patches. Since these patches are large enough to accommodate acyl chains, their role in lipoprotein binding was investigated. Several LolA mutant proteins were created, and their functionality was assessed by studying their capacity to release lipoproteins produced in sphaeroplasts. Interruption of the largest hydrophobic patch completely destroyed the lipoprotein-releasing capacity of LolA, while interruption of smaller patches apparently reduced efficiency. Thus, the results show a new lipoprotein transport model that places (some of) the acyl chains on the hydrophobic surface patches.     

Mean geometry of the thiopeptide unit and conformational features of dithiopeptides and polythiopeptides

The mean geometry of the thiopeptide [Ca-N-C(=S)-Ca] unit has been derived from an analysis of X-ray crystal structure data, as well as MM2 and Gaussian 80/82 calculations. The conformational flexibilities of dithiopeptides with glycl- and alanyl-side chains have been investigated by molecular mechanics. Minimum energy conformations were examined using interactive computer graphics molecular modeling techniques. Alanyl-dithiopeptide substitution within an oligopeptide results in considerable restriction of conformational freedom whereas the effect is minimal for glycyl-dithiopeptide substitution. Polyglycyl-thiopeptide adopts a left-handed three or fourfold or right-handed threefold helical structure with favorable interchain C = S...H-N hydrogen bond interactions. A poly-L-alanyl-thiopeptide prefers a left-handed threefold poly-L-proline-like helical structure.     

Mechanical Network in Titin Immunoglobulin from Force Distribution Analysis

The role of mechanical force in cellular processes is increasingly revealed by single molecule experiments and simulations of force-induced transitions in proteins. How the applied force propagates within proteins determines their mechanical behavior yet remains largely unknown. We present a new method based on molecular dynamics simulations to disclose the distribution of strain in protein structures, here for the newly determined high-resolution crystal structure of I27, a titin immunoglobulin (IG) domain. We obtain a sparse, spatially connected, and highly anisotropic mechanical network. This allows us to detect load-bearing motifs composed of interstrand hydrogen bonds and hydrophobic core interactions, including parts distal to the site to which force was applied. The role of the force distribution pattern for mechanical stability is tested by in silico unfolding of I27 mutants. We then compare the observed force pattern to the sparse network of coevolved residues found in this family. We find a remarkable overlap, suggesting the force distribution to reflect constraints for the evolutionary design of mechanical resistance in the IG family. The force distribution analysis provides a molecular interpretation of coevolution and opens the road to the study of the mechanism of signal propagation in proteins in general.     

Conformational flexibility in the apolipoprotein E amino-terminal domain structure determined from three new crystal forms: implications for lipid binding

An amino-terminal fragment of human apolipoprotein E3 (residues 1-165) has been expressed and crystallized in three different crystal forms under similar crystallization conditions. One crystal form has nearly identical cell dimensions to the previously reported orthorhombic (P2(1)2(1)2(1)) crystal form of the amino-terminal 22 kDa fragment of apolipoprotein E (residues 1-191). A second orthorhombic crystal form (P2(1)2(1)2(1) with cell dimensions differing from the first form) and a trigonal (P3(1)21) crystal form were also characterized. The structures of the first orthorhombic and the trigonal form were determined by seleno-methionine multiwavelength anomalous dispersion, and the structure of the second orthorhombic form was determined by molecular replacement using the structure from the trigonal form as a search model. A combination of modern experimental and computational techniques provided high-quality electron-density maps, which revealed new features of the apolipoprotein E structure, including an unambiguously traced loop connecting helices 2 and 3 in the four-helix bundle and a number of multiconformation side chains. The three crystal forms contain a common intermolecular, antiparallel packing arrangement. The electrostatic complimentarity observed in this antiparallel packing resembles the interaction of apolipoprotein E with the monoclonal antibody 2E8 and the low density lipoprotein receptor. Superposition of the model structures from all three crystal forms reveals flexibility and pronounced kinks in helices near one end of the four-helix bundle. This mobility at one end of the molecule provides new insights into the structural changes in apolipoprotein E that occur with lipid association.