Crystallographic studies of the chicken gizzard G-actin X DNase I complex at 5A resolution

The structure of the chicken gizzard G-actin X DNase I complex has been determined at 5 A resolution by an X-ray diffraction method. Protein phases were computed by the multiple isomorphous replacement method using four heavy atom derivatives. The mean figure of merit was 0.65. Dimensions of the three molecular species, the complex, G-actin and DNase I, were determined based on the "cypress wood" models derived from the electron density map. The natures of the heavy atom binding sites are discussed in relation to the distinction between the two component molecules. The pattern of successive contacts between actin molecules observed in the present crystal seems unrelated to that found in F-actin.     

Three-dimensional structure of bovine pancreatic DNase I at 2.5 A resolution

The three-dimensional structure of bovine pancreatic deoxyribonuclease I (DNase I) has been determined at 2.5 A resolution by X-ray diffraction from single crystals. An atomic model was fitted into the electron density using a graphics display system. DNase I is an alpha, beta-protein with two 6-stranded beta-pleated sheets packed against each other forming the core of a 'sandwich'-type structure. The two predominantly anti-parallel beta-sheets are flanked by three longer alpha-helices and extensive loop regions. The carbohydrate side chain attached to Asn 18 is protruding by approximately 15 A from the otherwise compact molecule of approximate dimensions 45 A X 40 A. The binding site of CA2+-deoxythymidine-3',5'-biphosphate (Ca-pdTp) has been determined by difference Fourier techniques confirming biochemical results that the active centre is close to His 131. Ca-pdTp binds at the surface of the enzyme between the two beta-pleated sheets and seems to interact with several charged amino acid side chains. Active site geometry and folding pattern of DNase I are quite different from staphylococcal nuclease, the only other Ca2+-dependent deoxyribonuclease whose structure is known at high resolution. The electron density map indicates that two Ca2+ ions are bound to the enzyme under crystallization conditions.     

Crystallographic refinement and structure of ribulose-1,5-bisphosphate carboxylase from Rhodospirillum rubrum at 1.7 A resolution

The amino acid sequence of ribulose-1,5-bisphosphate carboxylase/oxygenase from Rhodospirillum rubrum has been fitted to the electron density maps. The resulting protein model has been refined to a nominal resolution of 1.7 A using the constrained-restrained least-squares refinement program of Sussman and the restrained least-squares refinement program of Hendrickson & Konnert. The crystallographic refinement, based on 76,452 reflections with F greater than sigma (F) in the resolution range 5.5 to 1.7 A resulted in a crystallographic R-factor of 18.0%. The asymmetric unit contains one dimeric ribulose-1,5-biphosphate carboxylase molecule, consisting of 869 amino acid residues and 736 water molecules. The geometry of the refined model is close to ideal, with root-mean-square deviations of 0.018 A in bond lengths and 2.7 degrees in bond angles. Two loop regions, comprising residues 54 to 63 and 324 to 335, and the last ten amino acid residues at the C terminus are disordered in our crystals. The expected trimodal distribution is obtained for the side-chain chi 1-angles with a marked preference for staggered conformation. The hydrogen-bonding pattern in the N-terminal beta-sheet and the parallel sheet in the beta/alpha-barrel is described. A number of hydrogen bonds and salt bridges are involved in domain-domain and subunit-subunit interactions. The subunit-subunit interface in the dimer covers an area of 2800 A2. Considerable deviations from the local 2-fold symmetry are found at both the N terminus (residues 2 to 5) and the C terminus (residues 422 to 457). Furthermore, loop 8 in the beta/alpha-barrel domain has a different conformation in the two subunits. A number of amino acid side-chains have different conformations in the two subunits. Most of these residues are located at the surface of the protein. An analysis of the individual temperature factors indicates a high mobility of the C-terminal region and for some of the loops at the active site. The positions and B-factors for 736 solvent sites have been refined (average B: 45.9 A2). Most of the solvent molecules are bound as clusters to the protein. The active site of the enzyme, especially the environment of the activator Lys191 in the non-activated enzyme is described. Crystallographic refinement at 1.7 A resolution clearly revealed the presence of a cis-proline at the active site. This residue is part of the highly conserved region Lys166-Pro167-Lys168.     

Crystal structure of yeast Cu,Zn superoxide dismutase. Crystallographic refinement at 2.5 A resolution.

The structure of Cu,Zn yeast superoxide dismutase has been determined to 2.5 A resolution. The enzyme crystallizes in the P2(1)2(1)2 space group with two dimeric enzyme molecules per asymmetric unit. The structure has been solved by molecular replacement techniques using the dimer of the bovine enzyme as the search model, and refined by molecular dynamics with crystallographic pseudo-energy terms, followed by conventional crystallographic restrained refinement. The R-factor for 32,088 unique reflections in the 10.0 to 2.5 A resolution range (98.2% of all possible reflections) is 0.158 for a model comprising two protein dimers and 516 bound solvent molecules, with a root-mean-square deviation of 0.016 A from the ideal bond lengths, and an average B-factor value of 29.9 A2. A dimeric molecule of the enzyme is composed of two identical subunits related by a non-crystallographic 2-fold axis. Each subunit (153 amino acid residues) has as its structural scaffolding a flattened antiparallel eight-stranded beta-barrel, plus three external loops. The overall three-dimensional structure is quite similar to the phylogenetically distant bovine superoxide dismutase (55% amino acid homology), the largest deviations can be observed in the regions of amino acid insertions. The major insertion site hosting residues Ser25A and Gly25B, occurs in the 2,3 beta-turn between strands 2b and 3c, resulting in the structural perturbations of the two neighbouring strands. The second insertion site, at the end of the 3c beta-strand in the wide Greek-key loop, hosts the Asn35A residue, having an evident effect on the structure of the loop and possibly on the neighbouring 5,4 beta-turn. The salt bridge Arg77-Asp99 and the disulphide bridge Cys55-Cys144 stabilize the loop regions containing the metal ligands. The stereochemistry of the two metal centres is conserved, with respect to the bovine enzyme. The Cu2+ ligands show an uneven distortion from a square plane, while Zn2+ co-ordination geometry is distorted tetrahedral. The imidazole ring of the His61 residue forms a bridge between Cu and Zn ions. A solvent peak compatible with a fifth ligand is observed 2.0 A away from the copper in the active site channel, which is filled by ordered water molecules that possibly contribute to the stability and function of the enzyme. The charged residues responsible for the electrostatic guidance of the substrate to the active site (Glu130, Glu131, Lys134 and Arg141) are fairly conserved in their positions, some of them showing different interactions in the four chains due to the intermolecular contacts between the dimers.(ABSTRACT TRUNCATED AT 400 WORDS)     

Three-dimensional structure of the complex of actin and DNase I at 4.5 A resolution.

The shape of an actin subunit has been derived from an improved 6 A map of the complex of rabbit skeletal muscle actin and bovine pancreatic DNase I obtained by X-ray crystallographic methods. The three-dimensional structure of DNase I determined independently at 2.5 A resolution was compared with the DNase I electron density in the actin:DNase map. The two structures are very similar at 6 A resolution thus leading to an unambiguous identification of actin as well as DNase I electron density. Furthermore the correct hand of the actin structure is determined from the DNase I atomic structure. The resolution of the actin structure was extended to 4.5 A by using a single heavy-atom derivative and the knowledge of the atomic coordinates of DNase I. The dimensions of an actin subunit are 67 A X 40 A X 37 A. It consists of a small and a large domain, the small domain containing the N terminus. Actin is an alpha,beta-protein with a beta-pleated sheet in each domain. These sheets are surrounded by several alpha-helices, comprising at least 40% of the structure. The phosphate peak of the adenine nucleotide is located between the two domains. The complex of actin and DNase I as found in solution (i.e., the actin:DNase I contacts which do not depend on crystal packing) was deduced from a comparison of monoclinic with orthorhombic crystals. Residues 44-46, 51, 52, 60-62 of DNase I are close to a loop region in the small domain of actin. At a distance of approximately 15 A there is a second contact in the large domain in which Glu13 of DNase I is involved. A possible binding region for myosin is discussed.     

Crystallographic structure of allosterically inhibited phosphofructokinase at 7 A resolution

The structure of the allosterically inhibited form of phosphofructokinase from Bacillus stearothermophilus has been determined by X-ray crystallography to 7 A resolution by molecular replacement using the known structure of the active state as a starting model. Comparing the inhibited state with the active state, the tetramer is twisted about its long axis such that one pair of subunits in the tetramer rotates relative to the other pair by about 8 degrees around one of the molecular dyad axes. This rotation partly closes the binding site for the co-operative substrate fructose-6-phosphate, explaining its weaker binding to this conformational state. Within the subunit, one domain rotates relative to the other by 4.5 degrees, which further closes the fructose-6-phosphate site, without closing the cleft between the domains of the same subunit: this motion causes little change to the catalytic site. This T-state model is consistent with the simple allosteric kinetic scheme in which the active and the inhibited conformations differ in their affinities for fructose-6-phosphate, but not in their catalytic rates. It does not explain the heterotropic allosteric effects.     

Crystallographic refinement of the three-dimensional structure of the FabD1.3-lysozyme complex at 2.5-A resolution.

The three-dimensional crystal structure of the complex between the Fab from the monoclonal anti-lysozyme antibody D1.3 and the antigen, hen egg white lysozyme, has been refined by crystallographic techniques using x-ray intensity data to 2.5-A resolution. The antibody contacts the antigen with residues from all its complementarity determining regions. Antigen residues 18-27 and 117-125 form a discontinuous antigenic determinant making hydrogen bonds and van der Waals interactions with the antibody. Water molecules at or near the antigen-antibody interface mediate some contacts between antigen and antibody. The fine specificity of antibody D1.3, which does not bind (K alpha less than 10(5) M-1) avian lysozymes where Gln121 in the amino acid sequence is occupied by His, can be explained on the basis of the refined model.     

Crystallographic structure of PNP from Mycobacterium tuberculosis at 1.9A resolution

Even being a bacterial purine nucleoside phosphorylase (PNP), which normally shows hexameric folding, the Mycobacterium tuberculosis PNP (MtPNP) resembles the mammalian trimeric structure. The crystal structure of the MtPNP apoenzyme was solved at 1.9 A resolution. The present work describes the first structure of MtPNP in complex with phosphate. In order to develop new insights into the rational drug design, conformational changes were profoundly analyzed and discussed. Comparisons over the binding sites were specially studied to improve the discussion about the selectivity of potential new drugs.     

Crystallographic structure of Rhodospirillum molischianum ferricytochrome c' at 2.5 A resolution

This paper describes the 2.5 Å crystallographic structure determination of ferricytochrome c′ from the photosynthetic bacterium Rhodospirillum molischianum. The molecule is a symmetric dimer, with each 128-residue polypeptide chain incorporating a covalently bound protoheme IX prosthetic group. The monomer is structurally organized as an array of four nearly parallel α-helices, which pack most closely at one end and thereafter spatially diverge to accommodate the heme prosthetic group. Although local features of the heme attachment pattern resemble those seen in cytochrome c, the heme iron in cytochrome c′ is pentaco-ordinate with a solvent-exposed histidine residue furnishing the single axial ligand to the heme iron.Subunit association in the dimeric molecule is principally stabilized by helix interactions, which are qualitatively similar to those occurring within each monomer. These interactions result in a dimer geometry that situates the exposed regions of both hemes on the same molecular surface.The structural basis for some of the physiochemical properties cytochrome c′ are examined and compared to those of other heme proteins of known structure.     

X-ray structure of the DNase I-d(GGTATACC)2 complex at 2.3 A resolution.

The crystal structure of a complex between DNase I and the self-complementary octamer duplex d(GGTATACC)2 has been solved using the molecular replacement method and refined to a crystallographic R-factor of 18.8% for all data between 6.0 and 2.3 A resolution. In contrast to the structure of the DNase I-d(GCGATCGC)2 complex solved previously, the DNA remains uncleaved in the crystal. The general architecture of the two complexes is highly similar. DNase I binds in the minor groove of a right-handed DNA duplex, and to the phosphate backbones on either side over five base-pairs, resulting in a widening of the minor groove and a concurrent bend of the DNA away from the bound enzyme. There is very little change in the structure of the DNase I on binding the substrate. Many other features of the interaction are conserved in the two complexes, in particular the stacking of a deoxyribose group of the DNA onto the side-chain of a tyrosine residue (Y76), which affects the DNA conformation and the binding of an arginine side-chain in the minor groove. Although the structures of the DNA molecules appear at first sight rather similar, detailed analysis reveals some differences that may explain the relative resistance of the d(GGTATACC)2 duplex to cleavage by DNase I: whilst some backbone parameters are characteristic of a B-conformation, the spatial orientation of the base-pairs in the d(GGTATACC)2 duplex is close to that generally observed in A-DNA. These results further support the hypothesis that the minor-groove width and depth and the intrinsic flexibility of DNA are the most important parameters affecting the interaction. The disposition of residues around the scissile phosphate group suggests that two histidine residues, H134 and H252, are involved in catalysis.     

X-ray crystal structure determination and refinement at 1.9 A resolution of isolectin I from the seeds of Lathyrus ochrus

Orthorhombic crystals of isolectin I (LOLI) from the seeds of Lathyrus ochrus were first obtained during the STS 29 space shuttle mission. Subsequently, isostructural crystals were also obtained in the laboratory. They belong to the space group P2(1)2(1)2, with cell dimensions a = 135.84 A, b = 63.12 A and c = 54.54 A with one functional entity, a dimer, in the asymmetric unit (Vm = 2.2 A3/Da). The three-dimensional structure of LOLI, which was solved by the molecular replacement method using a 3 A resolution model of pea lectin, has subsequently been refined by using crystallographic data between 8.0 A and 1.9 A resolution, coupled to molecular dynamics and energy minimization techniques. The conventional R-factor is 0.185 for Fo greater than 1 sigma(Fo). The final model includes 220 well-defined water molecules and has root-mean-square deviations from ideal bond distances and angles of 0.004 A and 3 degrees, respectively. Only slight conformation differences have been found between the two alpha beta monomers. The molecular structure of LOLI, the first to be determined from the genus Lathyrus, is very similar to those of concanavalin A, pea lectin and favin. Differences are confined to the loop regions and beta-chain termini. Comparison of equivalent C alpha atom positions between our final model and the pea lectin structure shows slight differences in the association of the two monomers, which are probably due to the different environments in the crystals. The root-mean-square deviation between C alpha atoms of LOLI and pea lectin is 0.40 A. The metal binding sites are very similar in pea lectin, concanavalin A and LOLI. The sugar-binding sites of LOLI are occupied by four well-ordered water molecules each. The cleavage site for one of the monomers is specially well defined in the final electron density map: the amino group of Glul (alpha) seems to form a salt bridge with the carboxylate group of the terminal Asn181 (beta). A detailed analysis of the difference in crystal packing contacts between pea lectin and LOLI shows that, as might be expected, several of the intermolecular interactions are mediated by residues that correspond to substitutions in the LOLI amino acid sequence.     

Structure of human lactoferrin: crystallographic structure analysis and refinement at 2.8 A resolution

The structure of human lactoferrin has been refined crystallographically at 2.8 A (1 A = 0.1 nm) resolution using restrained least squares methods. The starting model was derived from a 3.2 A map phased by multiple isomorphous replacement with solvent flattening. Rebuilding during refinement made extensive use of these experimental phases, in combination with phases calculated from the partial model. The present model, which includes 681 of the 691 amino acid residues, two Fe3+, and two CO3(2-), gives an R factor of 0.206 for 17,266 observed reflections between 10 and 2.8 A resolution, with a root-mean-square deviation from standard bond lengths of 0.03 A. As a result of the refinement, two single-residue insertions and one 13-residue deletion have been made in the amino acid sequence, and details of the secondary structure and tertiary interactions have been clarified. The two lobes of the molecule, representing the N-terminal and C-terminal halves, have very similar folding, with a root-mean-square deviation, after superposition, of 1.32 A for 285 out of 330 C alpha atoms; the only major differences being in surface loops. Each lobe is subdivided into two dissimilar alpha/beta domains, one based on a six-stranded mixed beta-sheet, the other on a five-stranded mixed beta-sheet, with the iron site in the interdomain cleft. The two iron sites appear identical at the present resolution. Each iron atom is coordinated to four protein ligands, 2 Tyr, 1 Asp, 1 His, and the specific Co3(2-), which appears to bind to iron in a bidentate mode. The anion occupies a pocket between the iron and two positively charged groups on the protein, an arginine side-chain and the N terminus of helix 5, and may serve to neutralize this positive charge prior to iron binding. A large internal cavity, beyond the Arg side-chain, may account for the binding of larger anions as substitutes for CO3(2-). Residues on the other side of the iron site, near the interdomain crossover strands could provide secondary anion binding sites, and may explain the greater acid-stability of iron binding by lactoferrin, compared with serum transferrin. Interdomain and interlobe interactions, the roles of charged side-chains, heavy-atom binding sites, and the construction of the metal site in relation to the binding of different metals are also discussed.     

Structure and refinement of penicillopepsin at 1.8 A resolution

Penicillopepsin, the aspartyl protease from the mould Penicillium janthinellum, has had its molecular structure refined by a restrained-parameter least-squares procedure at 1.8 Å resolution to a conventional R-factor of 0.136. The estimated co-ordinate accuracy for the majority of the 2363 atoms of the enzyme is better than 0.12 Å. The average atomic thermal vibration parameter, B, for the atoms of the enzyme is 14.5 Ų. One determining factor of this low average B value is the large central hydrophobic core, in which there are two prominent clusters of aromatic residues, one of nine, the other of seven residues. The N and C-terminal domains of penicillopepsin display an approximate 2-fold symmetry: 70 residue pairs are topologically equivalent, related by a rotation of 177 ° and a translation of 1.2 Å. The analysis of the secondary structural features of the molecule reveals non-linear hydrogen bonding. In penicillopepsin, there is no difference in the mean hydrogen-bond parameters for the elements of α-helix, parallel or antiparallel β-pleated sheet. The mean values for these structural elements are: NO, 2.90 Å; NHO, 1.95 Å; N?O, 160 °. The average hydrogen-bond parameters of the reverse β-turns and the 3₁₀ helices are distinctly different from the above values. The analysis of sidechain conformational angles χ¹ and χ² penicillopepsin and other enzyme structures refined in this laboratory shows much narrower distributions as compared with those compiled from unrefined protein structures. The close proximity of the carboxyl groups of Asp33 and Asp213 suggests that they share a proton in a tight hydrogen-bonded environment (Asp33OD2 to Asp213OD1 is 2.87 Å). There are several solvent molecules in the active site region and, in particular, O39 forms hydrogen-bonded interactions with both aspartate residues. The disposition of the two carboxyl groups suggests that neither is likely to be involved in a direct nucleophilic attack on the scissile bond of a substrate. The average atomic B-factors of the residues in this region of the molecule are between 5 and 8 Ų, confirming the proposal that conformational mobility of the active site residues has no role in the enzymatic mechanism. However, conformational mobility of neighbouring regions of the molecule e.g. the “flap” containing Tyr75, is verified by the high B-factors for those residues. The positions of 319 solvent sites per asymmetric unit have been selected from difference electron density maps and refined. Thirteen have been classified as internal, and several of these may have key roles during catalysis. The positively charged N^ζ atom of Lys304 forms hydrogen bonds to the carboxylate of Asp14 (internal ion pair) and to two internal water molecules O5 and O25. The protonated side-chain of Asp300 forms a hydrogen bond to Thr214O, 2.78 Å, and is the recipient of a hydrogen bond from a surface pocket water molecule O46. There is no possibility for direct interaction between Asp300 and Lys304 without large conformational changes of their environment. The intermolecular packing involves many protein-protein contacts (66 residues) with a large number of solvent molecules involved in bridging between polar residues at the contact surface. The penicillopepsin molecules resemble an approximate hexagonal close-packing of spheres with each molecule having 12 “nearest” neighbours.     

Protein structure refinement: Streptomyces griseus serine protease A at 1.8 A resolution.

The crystal structure of the bacterial serine protease from Streptomyces griseus (SGPA) has been refined at 1.8 Å resolution by a restrained parameter least-squares procedure (Konnert, 1976) to a conventional R factor of 0.139 for 12662 statistically significant reflections [I > 3σ(I)]. The number of variable parameters in the final model was 5912 which included positional and individual thermal parameters of the enzyme, and positions, B factors and occupancies of 175 solvent molecules. The algorithm used for this refinement allows for the simultaneous restraint on bond distances and distances related to interbond angles, the coplanarity of atoms in planar groups, the conservation of chirality of asymmetric centres, non-bonded contact distances, conformational torsional angles and individual isotropic temperature factors.The refined structure of SGPA differs from ideal bond lengths by an overall root-mean-square deviation of 0.02 Å; the corresponding value for angle distances is 0.038 Å. Comparison of the phase angles for the shell of data, 8.0 to 2.8 Å, between the multiple isomorphous replacement phases (Brayer et al., 1978a) and the refined phases, indicates an overall difference (r.m.s.) of 56.6 °. The average conformational angle of the peptide bond (ω) is 179.7 ° (root-mean-square deviation ± 2.5 °) for the 180 peptide bonds of SGPA. Of the 175 solvent molecules included during the course of the refinement, 22 with occupancies ranging from 1.00 to 0.38 are located in the active site and the substrate binding region. It was not until these water molecules were included in the refinement process that the active Ser195 adopted its final conformation (χ¹ = ?77 °). The resulting distance from O^γ of Ser195 to N^ε2 of His57 is 3.1 Å, which, when taken with the observed distortion from linearity (50 °), indicates a rather weak interaction.     

Refined crystal structure of deoxyhemoglobin S. I. Restrained least-squares refinement at 3.0-A resolution

The crystal structure of deoxyhemoglobin S has been refined at 3.0-A resolution using the Hendrickson-Konnert restrained least-squares method. Comparison with the structure of deoxyhemoglobin A reveals a hingelike movement of the beta-chain A helices, which are involved in molecular contacts, toward the EF corners of their respective subunits. This movement brings the amino termini of the beta-chains closer to the molecular dyad. The A helices remain alpha-helical throughout their entire lengths. No other major structural difference is found between deoxyhemoglobin A and deoxyhemoglobin S.     

X-ray structure and refinement of carbon-monoxy (Fe II)-myoglobin at 1.5 A resolution

The structure of carbon-monoxy (Fe II) myoglobin at 260 K has been solved at a resolution of 1.5 A by X-ray diffraction and a model refined against the X-ray data by restrained least-squares. The CO ligand is disordered and distorted from the linear conformation seen in model compounds. At least two conformations, with Fe--C--O angles of 140 degrees and 120 degrees, are required to model the system. The heme pocket is significantly larger than in deoxy-myoglobin because the distal residues have relaxed around the ligand; the largest displacement occurs for the distal histidine side-chain, which moves more than 1.4 A on ligand binding. The side-chain of Arg45 (CD3) is disordered and apparently exists in two equally populated conformations. One of these does not block the motion of the distal histidine out of the binding pocket, suggesting a mechanism for ligand entry. The heme group is planar (root-mean-square deviation from planarity is 0.08 A) with no doming of the pyrrole groups. The Fe--N epsilon 2 (His93) bond length is 2.2 A and the Fe--C bond length in the CO complex is 1.9 A. The iron is the least-squares plane of the heme, and this leads to the proximal histidine moving by 0.4 A relative to its position in deoxy-myoglobin. This shift correlates with a global structural change, with the proximal part of the molecule translated towards the heme plane.     

Crystallographic refinement of ricin to 2.5 A

The plant cytotoxin ricin consists of two disulfide-linked chains, each of about 30,000 daltons. An initial model based on a 2.8 A MIR electron density map has been refined against 2.5 A data using rounds of hand rebuilding coupled with either a restrained least squares algorithm or molecular dynamics (XPLOR). The last model (9) has an R factor of 21.6% and RMS deviations from standard bond lengths and angles of 0.021 A and 4.67 degrees, respectively. Refinement required several peptide segments in the original model to be adjusted translationally along the electron density. A wide range of lesser changes were also made. The RMS deviation of backbone atoms between the original and model 9 was 1.89 A. Molecular dynamics proved to be a very powerful refinement tool. However, tests showed that it could not replace human intervention in making adjustments such as local translations of the peptide chain. The R factor is not a completely satisfactory indicator of refinement progress; difference Fouriers, when observed carefully, may be a better monitor.     

Aplysia limacina myoglobin. Crystallographic analysis at 1.6 A resolution

The crystal structure of the ferric form of myoglobin from the mollusc Aplysia limacina has been refined at 1.6 A resolution, by restrained crystallographic refinement methods. The crystallographic R-factor is 0.19. The tertiary structure of the molecule conforms to the common globin fold, consisting of eight alpha-helices. The N-terminal helix A and helix G deviate significantly from linearity. The distal residue is recognized as Val63 (E7), which, however, does not contact the heme directly. Moreover the sixth (distal) co-ordination position of heme iron is not occupied by a water molecule at neutrality, i.e. below the acid-alkaline transition point of A. limacina myoglobin. The heme group sits in its crevice in the conventional orientation and no signs of heme isomerism are evident. The iron atom is 0.26 A out of the porphyrin plane, with a mean Fe-N (porphyrin) distance of 2.01 A. The co-ordination bond to the proximal histidine has a length of 2.05 A, and forms an angle of 4 degrees with the heme normal. A plane containing the imidazole ring of the proximal His intersects the heme at an angle of 29 degrees with the (porphyrin) 4N-2N direction. Inspection of the structure of pH 9.0 indicates that a hydroxyl ion is bound to the Fe sixth co-ordination position.