X-ray structure determination and comparison of two crystal forms of a variant (Asn115Arg) of the alkaline protease from Bacillus alcalophilus refined at 1.85 A resolution.

The X-ray structure determination, refinement and comparison of two crystal forms of a variant (Asn115Arg) of the alkaline protease from Bacillus alcalophilus is described. Under identical conditions crystals were obtained in the orthorhombic space group P2(1)2(1)2(1) (form I) and the rhombohedral space group R32 (form II). For both space groups the structures of the protease were solved by molecular replacement and refined at 1.85 A resolution. The final R-factors are 17.9% and 17.1% for form I and form II, respectively. The root-mean-square deviation between the two forms is 0.48 A and 0.86 A for main-chain and side-chain atoms, respectively. Due to differences in crystal lattice contacts and packing, the structures of the two crystal forms differ in intermolecular interaction affecting the local conformation of three flexible polypeptide sequences (Ser50-Glu55, Ser99-Gly102, Gly258-Ser259) at the surface of the protein. While the two overall structures are very similar, the differences are significantly larger than the errors inherent in the structure determination. As expected, the differences in the temperature factors in form I and II are correlated with the solvent accessibility of the corresponding amino acid residues. In form II, two symmetry-related substrate binding sites face each other, forming a tight intermolecular interaction. Some residues contributing to this intermolecular interaction are also found to be involved in the formation of the complex between subtilisin Carlsberg and the proteinaceous inhibitor eglin C. This demonstrates that the two symmetry-related molecules interact with each other at the same molecular surface area that is used for binding of substrates and inhibitors.     

X-ray structural evidence for a local helix-loop transition in alpha-lactalbumin.

The three-dimensional structure of human alpha-lactalbumin for two crystal forms has been determined by x-ray analysis. One crystal (the form LT) was obtained at pH 4.2 and room temperature, while the other crystal (the form HT) was grown at pH 6.5 and 37 degrees C. The backbone structure for Lys1-Ile95 residues is almost conserved between the two structures as indicated by the root mean square difference of 0.30 A for the superposition of equivalent C alpha atoms. The calcium ion is surrounded by seven oxygen atoms of three carboxyl groups, two carbonyl groups, and two water molecules, which form a distorted pentagonal bipyramid in both structures. A large difference in polypeptide folding is found in the region of Leu96-Leu123 residues. Especially in the region of Trp104-Cys111 residues, a distorted alpha-helix is observed in the form HT while a loop structure is formed in the other crystal. The fact that the crystals of both forms appeared in the same batch at pH 6.5 and room temperature indicates that the human alpha-lactalbumin structure is highly fluctuated in solution and the folding and unfolding of the alpha-helix of Trp104-Cys111 residues are in equilibrium. Since the crystal of the form HT exclusively appeared around the physiological temperature, the structure of this form can be considered as the native structure. The partially unfolded structure in the form LT indicates that the local denaturation occurs even at room temperature.     

Side-necked turtle (Pleurodira, Chelonia, reptilia) hemoglobin: cDNA-derived primary structures and X-ray crystal structures of Hb A

Red blood cells of yellow-spotted river turtles (Podocnemis unifilis, Pleurodira, Chelonia, REPTILIA) have two hemoglobin (Hb) components, Hb A and Hb D. We purified the hemoglobin component homologous to amniote (reptiles, birds, and mammals) adult Hb A which comprises two identical α(A) -globin polypeptides and two identical β-globin polypeptides. To establish the crystal structure of Podocnemis Hb A, we first determined the globin primary structures using cDNA nucleotide sequencing with the assistance of protein sequencing. The purified Podocnemis Hb A produced a different form of crystal for each of the two different buffer systems used: form A, tetragonal crystals (space group, P4?2?2), produced under neutral pH (pH 7-8) conditions; and form B, hexagonal crystals (space group, P6?22), produced under high alkaline pH (pH 11-13) conditions. Single crystals of the two forms were examined by Raman microscopy with an excitation of 532 nm, indicating their structural differences. The crystal structures of the two forms were constructed by X-ray crystallographic diffraction at a resolution of 2.20 ? for form A and 2.35 ? for form B. The differences of the tertiary and quaternary structures of the two forms were marginal; however, one clear difference was found in helix structure. When comparing Podocnemis Hb A with Hb A from specimens in other taxa, such as Anser indicus (birds) and Homo sapiens (mammals) by SHELXPRO, the root mean square deviation (RMSD) between the corresponding Cα atoms of the two globins does not exceed 2.0 ?. These low values indicate the crystal structures resemble each other. Our data on X-ray crystal structures and Raman spectra not only reveal the first findings on the two crystal forms of Podocnemis unifilis Hb A but also provide the first refined models for reptilian adult Hb A.     

Structure and internal mobility of proteins: a molecular dynamics study of hen egg white lysozyme

The structure and internal motions of the protein hen egg white lysozyme are studied by analysis of simulation and experimental data. A molecular dynamics simulation and an energy minimization of the protein in vacuum have been made and the results compared with high-resolution structures and temperature factors of hen egg white lysozyme in two different crystal forms and of the homologous protein human lysozyme. The structures obtained from molecular dynamics and energy minimization have root-mean-square deviations for backbone atoms of 2.3 Å and 1.1–1.3 Å, respectively, relative to the crystal structures; the different crystal structures have root-mean-square deviations of 0.73–0.81 Å for the backbone atoms. In comparing the backbone dihedral angles, the difference between the dynamics and the crystal structure on which it is based is the same as that between any two crystal structures. The internal fluctuations of atomic positions calculated from the molecular dynamics trajectory agree well with the temperature factors from the three structures. Simulation and crystal results both show that there are large motions for residues involved in exposed turns of the backbone chain, relatively smaller motions for residues involved in the middle of helices or β-sheet structures, and relatively small motions of residues near disulfide bridges. Also, both the simulation and crystal data show that side-chain atoms have larger fluctuations than main-chain atoms. Moreover, the regions that have large deviations among the x-ray crystal structures, which indicates flexibility, are found to have large fluctuations in the simulation.     

Modeling the structure of Pyrococcus furiosus rubredoxin by homology to other X-ray structures.

The three-dimensional structure of rubredoxin from the hyperthermophilic archaebacterium, Pyrococcus furiosus, has been modeled from the X-ray crystal structures of three homologous proteins from Clostridium pasteurianum, Desulfovibrio gigas, and Desulfovibrio vulgaris. All three homology models are similar. When comparing the positions of all heavy atoms and essential hydrogen atoms to the recently solved crystal structure (Day, M. W., et al., 1992, Protein Sci. 1, 1494-1507) of the same protein, the homology model differ from the X-ray structure by 2.09 A root mean square (RMS). The X-ray and the zinc-substituted NMR structures (Blake, P. R., et al., 1992b, Protein Sci. 1, 1508-1521) show a similar level of difference (2.05 A RMS). On average, the homology models are closer to the X-ray structure than to the NMR structures (2.09 vs. 2.42 A RMS).     

Atomic resolution structures of oxidized [4Fe-4S] ferredoxin from Bacillus thermoproteolyticus in two crystal forms: systematic distortion of [4Fe-4S] cluster in the protein

Diffraction data of two crystal forms (forms I and II) of [4Fe-4S] ferredoxin from Bacillus thermoproteolyticus have been collected to 0.92 A and 1.00 A resolutions, respectively, at 100 K using synchrotron radiation. Anisotropic temperature factors were introduced for all non-hydrogen atoms in the refinement with SHELX-97, in which stereochemical restraints were applied to the protein chain but not to the [4Fe-4S] cluster. The final crystallographic R-factors are 9.8 % for 7.0-0.92 A resolution data of the form I and 11.2 % for the 13.3-1.0 A resolution data of the form II. Many hydrogen atoms as well as multiple conformations for several side-chains have been identified. The present refinement has revised the conformations of several peptide bonds and side-chains assigned previously at 2.3 A resolution; the largest correction was that the main-chain of Pro1 and the side-chain of Lys2 were changed by rotating the C(alpha)-C bond of Lys2. Although the overall structures in the two crystal forms are very similar, conformational differences are observed in the two residues at the middle (Glu29 and Asp30) and the C-terminal residues, which have large temperature factors. The [4Fe-4S] cluster is a distorted cube with non-planar rhombic faces. Slight but significant compression of the four Fe-S bonds along one direction is observed in both crystal forms, and results in the D(2d) symmetry of the cluster. The compressed direction of the cluster relative to the protein is conserved in the two crystal forms and consistent with that in one of the clusters in Clostridium acidurici ferredoxin.     

Cyclic diguanylic acid behaves as a host molecule for planar intercalators

Cyclic ribodiguanylic acid, c-(GpGp), is the endogenous effector regulator of cellulose synthase. Its three-dimensional structure from two different crystal forms (tetragonal and trigonal) has been determined by X-ray diffraction analysis at 1 A resolution. In both crystal forms, two independent c-(GpGp) molecules associate with each other to form a self-intercalated dimer. A hydrated cobalt ion is found to coordinate to two N7 atoms of adjacent guanines, forcing these two guanines to destack with a large dihedral angle (32 degrees), in the dimer of the tetragonal form. This metal coordination mechanism may be relevant to that of the anticancer drug cisplatin. Moreover, c-(GpGp) exhibits unusual spectral properties not seen in any other cyclic dinucleotide. It interacts with planar organic intercalator molecules in ways similar to double helical DNA. We propose a cage-like model consisting of a tetrameric c-(GpGp) aggregate in which a large cavity ('host') is generated to afford a binding site for certain planar intercalators ('guests').     

Hydration of oligonucleotides in crystals

The solvent molecules found around crystallized oligonucleotides after X-ray refinement are analysed in terms of interaction sites to bases, phosphates and sugars in the three main forms of nucleic acid structures, the A-form, the B-form and the Z-form. The average numbers of contacts to nucleic acid atoms made by solvent molecules are identical in the three forms, but it appears that the average number of contacts solvent molecules make with each other depends on the resolution of the structure. The phosphate anionic oxygen atoms are the most hydrated, while the O(3′) and O(5′) backbone atoms and the ring oxygen atom O(4′) are the least hydrated. Among the hydrophilic atoms of the bases, there is a modulation of the relative water affinities with the nucleic acid form. Numerous hydration sites are such that water molecules can bridge hydrophilic atoms of the same residue, of adjacent residues on the same strand, of distant residues on the two strands, or belonging to symmetry-related residues. Through the helical periodicity of the nucleic acid structure, those bridges can lead to regular and striking hydration networks involving several water molecules and characteristic of the nucleic acid form. Solvent dynamics, as seen by temperature factor versus occupancy plots, seems intimately related to nucleic acid structure and dynamics, since they depend on hydration sites around the nucleic acids.     

Crystal structure of the reduced form of p-hydroxybenzoate hydroxylase refined at 2.3 A resolution.

The crystal structure of the reduced form of the enzyme p-hydroxybenzoate hydroxylase from Pseudomonas fluorescens, complexed with its substrate p-hydroxybenzoate, has been obtained by protein X-ray crystallography. Crystals of the reduced form were prepared by soaking crystals of the oxidized enzyme-substrate complex in deaerated mother liquor containing 300-400 mM NADPH. A rapid bleaching of the crystals indicated the reduction of the enzyme-bound FAD by NADPH. This was confirmed by single crystal spectroscopy. X-ray data to 2.3 A were collected on oscillation films using a rotating anode generator as an X-ray source. After data processing and reduction, restrained least squares refinement using the 1.9 A structure of the oxidized enzyme-substrate complex as a starting model, yielded a crystallographic R-factor of 14.8% for 11,394 reflections. The final model of the reduced complex contains 3,098 protein atoms, the FAD molecule, the substrate p-hydroxybenzoate and 322 solvent molecules. The structures of the oxidized and reduced forms of the enzyme-substrate complex were found to be very similar. The root-mean-square discrepancy for all atoms between both structures was 0.38 A. The flavin ring is almost completely planar in the final model, although it was allowed to bend or twist during refinement. The observed angle between the benzene and the pyrimidine ring is 2 degrees. This value should be compared with observed values of 10 degrees for the oxidized enzyme-substrate complex and 19 degrees for the enzyme-product complex. The position of the substrate is virtually unaltered with respect to its position in the oxidized enzyme. No trace of a bound NADP+ or NADPH molecule was found.     

Structure of desheptapeptide (B24–B30) insulin in a new crystal form

The structure of desheptapeptide (B24–B30) insulin (DHPI) in a new crystal form (form B) has been determined and refined to 0.2 nm resolution. The crystals were obtained under the same crystallization condition as previously reported crystal form (form A). The overall structures of the two crystal forms are similar but obvious differences can be observed in crystal packing and local conformation. The crystal structures of the two forms show that the two independent molecules in an asymmetric unit from a DHPI dimer, and the dimer formation buries more than 18.20 and 16.95 nm² of solvent accessible surfaces for form A and form B DHPI, respectively, the largest among insulin and insulin analogs ever reported. Close examination at crystal packing shows that the dimer-forming surface of DHPI, namely Surface II, is normally present in the association of insulin and insulin analogs in their crystal structures. The results demonstrate that Surface II is crucially important for the formation of two crystal forms under the same crystallization condition.     

Crystal structure of the trigonal form of bovine beta-lactoglobulin and of its complex with retinol at 2.5 A resolution

The structure of the trigonal crystal form of bovine beta-lactoglobulin has been determined by X-ray diffraction methods. An electron density map, calculated with phases obtained by the multiple isomorphous replacement method, served as a starting point for alternate cycles of model building and restrained least-squares refinement. The model of the molecule fitted to the initial Fourier map was the one built for the orthorhombic crystal form of beta-lactoglobulin, solved at 2.8 A resolution (1 A = 0.1 nm). The final R factor for 1456 atoms (1276 non-hydrogen protein atoms and 180 solvent atoms) is 0.22, including 5245 reflections from 6.0 to 2.5 A. The molecule shows significant differences in the two crystal forms mentioned, mainly due to different packing. In the trigonal form, the species crystallized does not appear to be dimeric, but a linear polymer with tight intermolecular contacts. A difference electron density map between the complex of beta-lactoglobulin with retinol and the native protein shows no significant peaks in the cavity which, in the similar retinol-binding protein, binds the chromophore. Instead, differences are found at a surface pocket, which is limited almost completely by hydrophobic residues.     

Structure of desheptapeptide (B24-B30) insulin in a new crystal form

The structure of desheptapeptide (B24-B30) insulin (DHPI) in a new crystal form (form B) has been determined and refined to 0.2 nm resolution. The crystals were obtained under the same crystallization condition as previously reported crystal form (form A). The overall structures of the two crystal forms are similar but obvious differences can be observed in crystal packing and local conformation. The crystal structures of the two forms show that the two independent molecules in an asymmetric unit from a DHPI dimer, and the dimer formation buries more than 18.20 and 16.95 nm~2 of solvent accessible surfaces for form A and form B DHPI, respectively, the largest among insulin and insulin analogs ever reported. Close examination at crystal packing shows that the dimer-forming surface of DHPI, namely Surface Ⅱ, is normally present in the association of insulin and insulin analogs in their crystal structures. The results demonstrate that Surface Ⅱ is crucially important for the formation of two crystal form     

Ordered water structure around a B-DNA dodecamer: A quantitative study

The crystal structure of the double-helical B-DNA dodecamer of sequence C-G-C-G-A-A-T-T-C-G-C-G has been solved and refined independently in three forms: (1) the parent sequence at room temperature; (2) the same sequence at 16 K; and (3) the 9-bromo variant C-G-C-G-A-A-T-T^BrC-G-C-G at 7 °C in 60% (v/v) 2-methyl-2.4-pentanediol. The latter two structures show extensive hydration along the phosphate backbone, a feature that was invisible in the native structure because of high temperature factors (indicating thermal or static disorder) of the backbone atoms. Sixty-five solvent peaks are associated with the phosphate backbone, or an average of three per phosphate group. Nineteen other molecules form a first shell of hydration to base edge N and O atoms within the major groove, and 36 more are found in upper hydration layers. The latter tend to occur in strings or clusters spanning the major groove from one phosphate group to another. A single spermine molecule also spans the major groove. In the minor groove, the zig-zag spine of hydration that we believe to be principally responsible for stabilizing the B form of DNA is found in all three structures. Upper level hydration in the minor groove is relatively sparse, and consists mainly of strings of water molecules extending across the groove, with few contacts to the spine below. Sugar O-1′ atoms are closely associated with water molecules, but these are chiefly molecules in the spine, so the association may reflect the geometry of the minor groove rather than any intrinsic attraction of O-1′ atoms for hydration. The phosphate O-3′ and O-5′ atoms within the backbone chain are least hydrated of all, although no physical or steric impediment seems to exist that would deny access to these oxygen atoms by water molecules.     

Solvent structure in crystals of trypsin determined by X-ray and neutron diffraction.

The solvent structure in orthorhombic crystals of bovine trypsin has been independently determined by X-ray diffraction to 1.35 A resolution and by neutron diffraction to 2.1 A resolution. A consensus model of the water molecule positions was obtained using oxygen positions identified in the electron density map determined by X-ray diffraction, which were verified by comparison to D2O-H2O difference neutron scattering density. Six of 184 water molecules in the X-ray structure, all with B-factors greater than 50 A2, were found to be spurious after comparison with neutron results. Roughly two-thirds of the water of hydration expected from thermodynamic data for proteins was localized by neutron diffraction; approximately one-half of the water of hydration was located by X-ray diffraction. Polar regions of the protein are well hydrated, and significant D2O-H2O difference density is seen for a small number of water molecules in a second shell of hydration. Hydrogen bond lengths and angles calculated from unconstrained refinement of water positions are distributed about values typically seen in small molecule structures. Solvent models found in seven other bovine trypsin and trypsinogen and rat trypsin structures determined by X-ray diffraction were compared. Internal water molecules are well conserved in all trypsin structures including anionic rat trypsin, which is 65% homologous to bovine trypsin. Of the 22 conserved waters in trypsin, 19 were also found in trypsinogen, suggesting that they are located in regions of the apoprotein that are structurally conserved in the transition to the mature protein. Seven waters were displaced upon activation of trypsinogen. Water structure at crystal contacts is not generally conserved in different crystal forms. Three groups of integral structural water molecules are highly conserved in all solvent structures, including a spline of water molecules inserted between two beta-strands, which may resemble an intermediate in the formation of beta sheets during the folding of a protein.     

High-resolution structures of scytalone dehydratase-inhibitor complexes crystallized at physiological pH

Scytalone dehydratase is a molecular target of inhibitor design efforts aimed at preventing the fungal disease caused by Magnaporthe grisea. A method for cocrystallization of enzyme with inhibitors at neutral pH has produced several crystal structures of enzyme-inhibitor complexes at resolutions ranging from 1.5 to 2.2 A. Four high resolution structures of different enzyme-inhibitor complexes are described. In contrast to the original X-ray structure of the enzyme, the four new structures have well-defined electron density for the loop region comprising residues 115-119 and a different conformation between residues 154 and 160. The structure of the enzyme complex with an aminoquinazoline inhibitor showed that the inhibitor is in a position to form a hydrogen bond with the amide of the Asn131 side chain and with two water molecules in a fashion similar to the salicylamide inhibitor in the original structure, thus confirming design principles. The aminoquinazoline structure also allows for a more confident assignment of donors and acceptors in the hydrogen bonding network. The structures of the enzyme complexes with two dichlorocyclopropane carboxamide inhibitors showed the two chlorine atoms nearly in plane with the amide side chain of Asn131. The positions of Phe53 and Phe158 are significantly altered in the new structures in comparison to the two structures obtained from crystals grown at acidic pH. The multiple structures help define the mobility of active site amino acids critical for catalysis and inhibitor binding.     

High-resolution solution structure of reduced French bean plastocyanin and comparison with the crystal structure of poplar plastocyanin

The three-dimensional solution structure of reduced (CuI) plastocyanin from French bean leaves has been determined by distance geometry and restrained molecular dynamics methods using constraints obtained from 1H n.m.r. (nuclear magnetic resonance) spectroscopy. A total of 1244 experimental constraints were used, including 1120 distance constraints, 103 dihedral angle constraints and 21 hydrogen bond constraints. Stereospecific assignments were made for 26 methylene groups and the methyls of 11 valines. Additional constraints on copper co-ordination were included in the restrained dynamics calculations. The structures are well defined with average atomic root-mean-square deviations from the mean of 0.45 A for all backbone heavy atoms and 1.08 A for side-chain heavy atoms. French bean plastocyanin adopts a beta-sandwich structure in solution that is similar to the X-ray structure of reduced poplar plastocyanin; the average atomic root-mean-square difference between 16 n.m.r. structures and the X-ray structure is 0.76 A for all backbone heavy atoms. The conformations of the side-chains that constitute the hydrophobic core of French bean plastocyanin are very well defined. Of 47 conserved residues that populate a single chi 1 angle in solution, 43 have the same rotamer in the X-ray structure. Many surface side-chains adopt highly preferred conformations in solution, although the 3J alpha beta coupling constants often indicate some degree of conformational averaging. Some surface side-chains are disordered in both the solution and crystal structures of plastocyanin. There is a striking correlation between measures of side-chain disorder in solution and side-chain temperature factors in the X-ray structure. Side-chains that form a distinctive acidic surface region, believed to be important in binding other electron transfer proteins, appear to be disordered. Fifty backbone amide protons form hydrogen bonds to carbonyls in more than 60% of the n.m.r. structures; 45 of these amide protons exchange slowly with solvent deuterons. Ten hydrogen bonds are formed between side-chain and backbone atoms, eight of which are correlated with decreased proton exchange. Of the 60 hydrogen bonds formed in French bean plastocyanin, 56 occur in the X-ray structure of the poplar protein; two of the missing hydrogen bonds are absent as a result of mutations. It appears that molecular dynamics refinement of highly constrained n.m.r. structures allows accurate prediction of the pattern of hydrogen bonding.     

Application of molecular dynamics with interproton distance restraints to three-dimensional protein structure determination. A model study of crambin

The applicability of restrained molecular dynamics for the determination of three-dimensional protein structures on the basis of short interproton distances (less than 4 A) that can be realistically determined from nuclear magnetic resonance measurements in solution is assessed. The model system used is the 1.2 A resolution crystal structure of the 46 residue protein crambin, from which a set of 240 approximate distance restraints, divided into three ranges (2.5 +/- 0.5, 3.0+0.5(-1.0) and 4 +/- 1 A), is derived. This interproton distance set comprises 159 short-range ([i-j] less than or equal to 5) and 56 ([i-j] greater than 5) long-range inter-residue distances and 25 intra-residue distances. Restrained molecular dynamics are carried out using a number of different protocols starting from two initial structures: a completely extended beta-strand; and an extended structure with two alpha-helices in the same positions as in the crystal structure (residues 7 to 19, and 23 to 30) and all other residues in the form of extended beta-strands. The root-mean-square (r.m.s.) atomic differences between these two initial structures and the crystal structure are 43 A and 23 A, respectively. It is shown that, provided protocols are used that permit the secondary structure elements to form at least partially prior to folding into a tertiary structure, convergence to the correct final structure, both globally and locally, is achieved. The r.m.s. atomic differences between the converged restrained dynamics structures and the crystal structure range from 1.5 to 2.2 A for the backbone atoms and from 2.0 to 2.8 A for all atoms. The r.m.s. atomic difference between the X-ray structure and the structure obtained by first averaging the co-ordinates of the converged restrained dynamics structures is even smaller: 1.0 A for the backbone atoms and 1.6 A for all atoms. These results provide a measure with which to judge future experimental results on proteins whose crystal structures are unknown. In addition, from an examination of the dynamics trajectories, it is shown that the convergence pathways followed by the various simulations are different.     

Comparison of the refined crystal structures of two wheat germ isolectins

The crystal structures of two closely related members of the multigene family of wheat lectins (isolectins 1 and 2) have been compared. These isolectins differ at five sequence positions, one being located in the saccharide binding site modulating ligand affinity. Crystals of the two isolectins are closely isomorphous (space group C2). The atomic models are based on structure refinement at 1.8 A resolution in the case of isolectin 2 (WGA2) and 2.0 A resolution in the case of isolectin 1 (WGA1). Refinement results for WGA1, recently completed with a crystallographic R-factor of 16.5% (Fo greater than 3 sigma (Fo)), are presented. Examination of a difference Fourier map, [FWGA2-FWGA1], at 2.0 A resolution and direct superposition of the two models indicated an overall close match of the two structures. Local differences are observed in the region of residues 44 to 69, where three sequence differences occur, and at highly mobile external residues on the surface. The average positional discrepancy (root-mean-square delta r) for corresponding protein atoms in the two crystal structures is 0.64 A for independent protomer I and 0.61 A for protomer II (0.29 A and 0.30 A for main-chain atoms). The mean atomic temperature factors are very similar 20.9 versus 22.0 A2). Regions of high flexibility coincide in the two isolectin structures. Of the 210 water sites identified in WGA1, 144 have corresponding positions in WGA2. A set of 51 well-ordered sites was found to be identical in the two independent environments in both structures, and was considered to be important for structure stabilization. Both of the unique sugar binding sites superimpose very closely, exhibiting root-mean-square positional differences ranging from 0.29 A to 0.42 A. The side-chains of the critical tyrosine residues, Tyr73 (P-site) and Tyr159 (S-site), superimpose best, while other highly flexible aromatic groups (Tyr64 and Trp150) and several water sites display large differences in position (0.5 to 1.0 A) and high temperature factors. The aromatic side-chains of Tyr66 in WGA1 and His66 in WGA2 are oriented similarly.     

The structure of 2Zn pig insulin crystals at 1.5 A resolution

The paper describes the arrangement of the atoms within rhombohedral crystals of 2Zn pig insulin as seen in electron density maps calculated from X-ray data extending to 1.5 A (1 A = 10(-10) m = 10(-1) nm) at room temperature and refined to R = 0.153. The unit cell contains 2 zinc ions, 6 insulin molecules and about 3 x 283 water molecules. The atoms in the protein molecules appear well defined, 7 of the 102 side chains in the asymmetric unit have been assigned alternative disordered positions. The electron density over the water molecules has been interpreted in terms of 349 sites, 217 weighted 1.0, 126 weighted 0.5, 5 at 0.33 and 1 at 0.25 giving ca. 282 molecules. The positions and contacts of all the residues belonging to the two A and B chains of the asymmetric unit are shown first and then details of their arrangement in the two insulin molecules, 1 and 2, which are different. The formation from these molecules of a compact dimer and the further aggregation of three dimers to form a hexamer around two zinc ions, follows. It appears that in the packing of the hexamers in the crystal there are conflicting influences; too-close contacts between histidine B5 residues in neighbouring hexamers are probably responsible for movements of atoms at the beginning of the A chain of one of the two molecules of the dimer that initiate movements in other parts, particularly near the end of the B chain. At every stage of the building of the protein structure, residues to chains of definite conformation, molecules, dimers, hexamers and crystals, we can trace the effect of the packing of like groups to like, aliphatic groups together, aromatic groups together, hydrogen-bonded structures, positive and negative ions. Between the protein molecules, the water is distributed in cavities and channels that are continuous throughout the crystals. More than half the water molecules appear directly hydrogen bonded to protein atoms. These are generally in contact with other water molecules in chains and rings of increasing disorder, corresponding with their movement through the crystals. Within the established crystal structure we survey next the distribution of hydrogen bonds within the protein molecules and between water and protein and water and water; all but eight of the active atoms in the protein form at least one hydrogen bond.(ABSTRACT TRUNCATED AT 400 WORDS)