Crystalline structure of the gas vesicle wall from Anabaena flos-aquae.

The gas vesicles isolated from Anabaena flos-aquae have been studied by X-ray diffraction. Electron microscopy has previously shown that the gas vesicles are elongated shapes, with a thin wall having regular striations (ribs) at right-angles to the long axis. The X-ray diffraction pattern from a specimen of oriented, intact vesicles includes a number of sharp reflections which are attributed to regular structure in the plane of the wall. After correcting for the imperfect alignment of the long axes of the vesicles, the in-plane reflections are all seen to lie on a few, regularly spaced lines parallel to the long axis. This result shows for the first time that there are subunits regularly spaced along each rib, one subunit every 11 Å. The spacing of the in-plane reflections along each line is consistent with a rib periodicity of 46 Å. The 11 Å repeat, together with the 46 Å repeating distance from rib to rib and the average wall thickness of about 20 Å, define a volume for the subunit. Assuming a reasonable value for the density of the protein making up the wall, the molecular weight of the subunit indicated is about 8000 g/mol.The X-ray data also indicate that a large part of the protein is in the β-sheet conformation. In this structure there are parallel, or anti-parallel, polypeptide chains which are hydrogen-bonded to one another in a regular way to form a thin sheet. Assuming the wall contains β-sheet in two layers, one on top of the other and with the chains in each layer tilted at 35 ° to the long axis of the vesicle, we can explain a number of the X-ray observations: (1) oriented arcs with a Bragg spacing of 4.7 Å, which is the distance between the axes of neighbouring chains in each layer; (2) diffraction oriented in the direction of the chains at a spacing of 6 to 7 Å, which is the repeating distance of the dipeptide unit along the chain; (3) the 11 Å repeat, which is the repeating distance of pairs of chains along each rib; and (4) a broad band of diffraction at right-angles to the plane of the wall and centred at a spacing of 10 Å, which is a reasonable value for the distance between the mid-planes of the two sheets. Moreover, we can also find the remaining lattice parameter, the angle relating the centres of the subunits in neighbouring ribs. Thus the shortest line joining the centres makes an angle of 86 ° with the direction of the ribs.     

Solid-State NMR Evidence for Inequivalent GvpA Subunits in Gas Vesicles

Gas vesicles are organelles that provide buoyancy to the aquatic microorganisms that harbor them. The gas vesicle shell consists almost exclusively of the hydrophobic 70-residue gas vesicle protein A, arranged in an ordered array. Solid-state NMR spectra of intact collapsed gas vesicles from the cyanobacterium Anabaena flos-aquae show duplication of certain gas vesicle protein A resonances, indicating that specific sites experience at least two different local environments. Interpretation of these results in terms of an asymmetric dimer repeat unit can reconcile otherwise conflicting features of the primary, secondary, tertiary, and quaternary structures of the gas vesicle protein. In particular, the asymmetric dimer can explain how the hydrogen bonds in the β-sheet portion of the molecule can be oriented optimally for strength while promoting stabilizing aromatic and electrostatic side-chain interactions among highly conserved residues and creating a large hydrophobic surface suitable for preventing water condensation inside the vesicle.     

Average thickness of the gas vesicle wall in Anabaena flos-aquae.

The average thickness of the layer of protein which forms the wall of the gas vesicles in Anabaena flos-aquae was estimated from measurements of their density and geometry. The volume of the gas space in a purified gas vesicle suspension was determined from the contraction which occurred when the gas vesicles were collapsed by pressure. The volume of the protein in the same sample was calculated from its dry weight and density. From knowledge of the geometry of the average gas vesicle the thickness of the protein layer, 1.54 nm, was then calculated. By a similar method the thickness of the Microcystis gas vesicle wall, 1.62 nm, was calculated from data published by others. The average thickness of the protein layer is, as expected, slightly less than the stacking periodicity of collapsed gas vesicle walls indicated by X-ray diffraction studies.Anabaena gas vesicles with a mean length of 494 nm have an average density of 0.119 mg μl^?1 1 mg of protein is present in gas vesicles having a, total volume of 8.43 μl and a gas space of 7.67 μl. Suspensions of isolated gas vesicles with a gas space concentration of 1 μl ml^?1 give a pressure-sensitive optical density, E_1cm (500 nm) of 2.72, but gas vacuoles in cells give a smaller value.     

Solution Structure of the Lipoyl Domain of the 2-Oxoglutarate Dehydrogenase Complex fromAzotobacter vinelandii

The three-dimensional solution structure of the lipoyl domain of the 2-oxoglutarate dehydrogenase complex fromAzotobacter vinelandiihas been determined from nuclear magnetic resonance data by using distance geometry and dynamical simulated annealing refinement. The structure determination is based on a total of 580 experimentally derived distance constraints and 65 dihedral angle constraints. The solution structure is represented by an ensemble of 25 structures with an average root-mean-square deviation between the individual structures of the ensemble and the mean coordinates of 0.71 Å for backbone atoms and 1.08 Å for all heavy atoms. The overall fold of the lipoyl domain is that of a β-barrel-sandwich hybrid. It consists of two almost parallel four-stranded anti-parallel β-sheets formed around a well-defined hydrophobic core, with a central position of the single tryptophan 21. The lipoylation site, lysine 42, is found in a β-turn at the far end of one of the sheets, and is close in space to a solvent-exposed loop comprising residues 7 to 15. The lipoyl domain displays a remarkable internal symmetry that projects one β-sheet onto the other β-sheet after rotation of approximately 180° about a 2-fold rotational symmetry axis. There is close structural similarity between the structure of this 2-oxoglutarate dehydrogenase complex lipoyl domain and the structures of the lipoyl domains of pyruvate dehydrogenase complexes fromBacillus stearothermophilusandEscherichia coli, and conformational differences occur primarily in a solvent-exposed loop close in space to the lipoylation site. The lipoyl domain structure is discussed in relation to the process of molecular recognition of lipoyl domains by their parent 2-oxo acid dehydrogenase.     

Three-Dimensional Structure of Selenocosmia huwena Lectin-I (SHL-I) from the Venom of the Spider Selenocosmia huwena by 2D-NMR

The three-dimensional structure of native SHL-I, a lectin from the venom of the Chinese bird spider Selenocosmia huwena, has been determined from two-dimensional ¹H NMR spectroscopy recorded at 500 and 600 MHz. The best 10 structures have NOE violation <0.3 Å, dihedral violation <2 deg, and average root-mean-square differences of 0.85 + 0.06 Å over backbone atoms. The structure consists of a three-stranded antiparallel β-sheet and three turns. The three disulfide bridges and three-stranded antiparallel β-sheet form a inhibitor cystine knot motif which is adopted by several other small proteins, such as huwentoxin-I, ω-conotoxin, and gurmarin. The C-terminal fragment from Leu28 to Trp32 adopts two sets of conformations corresponding to the cis and trans conformations of Pro31. The structure of SHL-I also has high similarity with that of the N-terminus of hevein, a lectin from rubber-tree latex.     

Electron tunneling in proteins: role of the intervening medium

Analysis of electron-transfer (ET) kinetics data obtained from experiments on Ru-modified proteins (azurin, cytochrome c, myoglobin) and the bacterial photosynthetic reaction center reveals that distant donor-acceptor electronic couplings depend upon the secondary structure of the intervening polypeptide matrix. The β-sheet azurin structure efficiently and isotropically mediates coupling with an exponential distance-decay constant of 1.1?Å^–1. The experimentally derived distance-decay constant of 1.4?Å^–1 for long-range ET in myoglobin and the reaction center suggests that hydrogen-bond couplings are weaker through α helices than across β sheets. The donor-acceptor interactions of systems with comparable tunneling energies fall into two coupling zones: the β zone (bounded by distance-decay constants of 0.9?and 1.15 Å^–1) includes all the β-sheet (azurin) couplings and all but one coupling in cytochrome c; the α zone (boundaries: 1.25 and 1.6?Å^–1) includes less strongly coupled donor-acceptor pairs in myoglobin and the reaction center as well as a relatively weakly coupled pair in cytochrome c.     

Three-dimensional structure of actinoxanthin. III. A 4-Å resolution

The protein actinoxanthin (molecular weight 10,300) crystallizes in space group P2₁2₁2₁, with cell dimensions a = 30.9 Å, b = 48.8 Å, c = 64.1 Å, and z = 4. The three-dimensional structure of actinoxanthin at 4-Å resolution was determined by x-ray methods on the basis of experimental data from the native protein and five isomorphous derivatives. At the stage of solving the phase problem, the heavy atoms in the derivatives were located using direct methods. The actinoxanthin molecule can be described as an oblate ellipsoid with approximate dimensions 20 × 30 × 40 Å and consists of two different sizes of folded units separated by a well-defined cleft. The larger unit, including the N- and C-terminals of the protein chain, is characterized by a significant content of β-sheet structure. The smaller unit, containing two deca- and hexapeptide cycles closed by disulfide bonds, has a mainly irregular structure.     

5.5 Å crystallographic structure of penicillin β-lactamase and radius of gyration in solution

An electron density map of crystalline R-TEM Escherichia coli β-lactamase (penicillinase) has been calculated from X-ray diffraction data at 5.5 Å resolution with protein phases based on Friedel mates from a high-quality samarium derivative. The mean figure of merit for 854 independent reflections is 0.75. The monomeric molecule is slightly ellipsoidal and contains one and possibly two regions of α-helix which are 25 Å long. The Crystallographic search for the substrate binding site has so far been inconclusive. The radius of gyration of the enzyme in solution at pH 7 is 17.1 ± 1.0 Å from small-angle X-ray scattering measurements. This compares with 18.6 å calculated from the low-resolution electron density map of the molecule in the crystal.     

Molecular Basis for Immunity Protein Recognition of a Type VII Secretion System Exported Antibacterial Toxin

Gram-positive bacteria deploy the type VII secretion system (T7SS) to facilitate interactions between eukaryotic and prokaryotic cells. In recent work, we identified the TelC protein from Streptococcus intermedius as a T7SS-exported lipid II phosphatase that mediates interbacterial competition. TelC exerts toxicity in the inner wall zone of Gram-positive bacteria; however, intercellular intoxication of sister cells does not occur because they express the TipC immunity protein. In the present study, we sought to characterize the molecular basis of self-protection by TipC. Using sub-cellular localization and protease protection assays, we show that TipC is a membrane protein with an N-terminal transmembrane segment and a C-terminal TelC-inhibitory domain that protrudes into the inner wall zone. The 1.9-Å X-ray crystal structure of a non-protective TipC paralogue reveals that the soluble domain of TipC proteins adopts a crescent-shaped fold that is composed of three α-helices and a seven-stranded β-sheet. Subsequent homology-guided mutagenesis demonstrates that a concave surface formed by the predicted β-sheet of TipC is required for both its interaction with TelC and its TelC-inhibitory activity. S. intermedius cells lacking the tipC gene are susceptible to growth inhibition by TelC delivered between cells; however, we find that the growth of this strain is unaffected by endogenous or overexpressed TelC, although the toxin accumulates in culture supernatants. Together, these data indicate that the TelC-inhibitory activity of TipC is only required for intercellularly transferred TelC and that the T7SS apparatus transports TelC across the cell envelope in a single step, bypassing the cellular compartment in which it exerts toxicity en route.     

Crystallization,crystal structure analysis and molecular model of the third domain of Japanese quail ovomucoid,a Kazal type inhibitor

The third domain of Japanese quail ovomucoid, a Kazal type inhibitor, has been crystallized and its crystal structure determined at 2.5 Å resolution using multiple isomorphous replacement techniques. The asymmetric unit contains four molecules. In the crystal the molecules are arranged in two slightly different octamers with approximate D4 symmetry. The molecules are held together mainly by interactions of the N-terminal residues, which form a novel secondary structural element, a β-channel.The molecule is globular with approximate dimensions 35 Å × 27 Å × 19 Å. The secondary structural elements are a double-stranded anti-parallel β-sheet of residues Pro22 to Gly32 and an α-helix from Asn33 to Ser44. The reactive site Lys18-Asp19 is located in an exposed loop. It is close to Asn33 at the N terminus of the helical segment. The polypeptide chain folding of ovomucoid bears some resemblance to other inhibitors in the existence of an anti-parallel double strand following the reactive site loop.     

Conformational analysis of a snake neurotoxin by prediction from sequence, circular dichroism, and raman spectroscopy.

The secondary structure of the major neurotoxin from the sea snake Lapemis hardwickii was investigated by several methods of conformational analysis: structure prediction, circular dichroism, and laser Raman spectroscopy. From the primary structure, secondary structure prediction yielded two regions of β-sheet structure at residues 1–7 and 41–45. β-Turns were predicted at residues 14–17, 20–23, 30–33, 37–40, and 46–49. From the predictions, the toxin appears to be composed of approximately 20% β-sheet and 33% β-turn. The CD spectrum of the native toxin appears to be a hybrid of model spectra for β-sheet and β-turn proteins. The pH perturbation studies on the toxin observed by CD demonstrated that the toxin is a very stable molecule except at extremely high or low pH values. The Raman data indicated that the toxin contains both antiparallel β-sheet and β-turn structure. Using two methods of secondary structure quantitation from Raman spectra the molecule was calculated to contain 35% β-sheet from one method and 27% from the other. Overall, the various methods demonstrate that the toxin is composed of β-sheet and β-turn structure with little or no α-helix present. From the comparison of these different techniques appreciation can be gained for the necessity of several methods when identifying and quantitating secondary structure.     

Revisiting peptide amphiphilicity for membrane pore formation

It has previously been shown that an amphipathic de novo designed peptide made of 10 leucines and four phenylalanines substituted with crown ethers induces vesicle leakage without selectivity. To gain selectivity against negatively charged dimyristoylphosphatidylglycerol (DMPG) bilayers, one or two leucines of the peptide were substituted with positively charged residues at each position. All peptides induce significant calcein leakage of DMPG vesicles. However, some peptides do not induce significant leakage of zwitterionic dimyristoylphosphatidylcholine vesicles and are thus active against only bacterial model membranes. The intravesicular leakage is induced by pore formation instead of membrane micellization. Nonselective peptides are mostly helical, while selective peptides mainly adopt an intermolecular β-sheet structure. This study therefore demonstrates that the position of the lysine residues significantly influences the secondary structure and bilayer selectivity of an amphipathic 14-mer peptide, with β-sheet peptides being more selective than helical peptides.     

Structure of sarcoplasmic reticulum membranes at low resolution (17A)

Vesicles of fragmented sarcoplasmic reticulum membranes have been prepared and centrifuged into a multilayered form suitable for analysis by X-ray diffraction. X-ray diffraction has been recorded from a regular stacking of flattened vesicles in the presence of excess fluid. Discrete orders of a lamellar repeat distance ranging from 220 to 270 Å have been recorded. The diffraction data extend out to a minimum Bragg spacing of 33 Å. An electron density profile at a resolution of 17 Å has been derived using direct methods of structure analysis. The membrane has a bilayer construction (similar to nerve myelin and retina at low resolution) but the profile is markedly asymmetrical. The protein molecules are predominantly on the inside of the vesicle. A striking resemblance between the disc membranes in retina and the sarcoplasmic reticulum membranes has been noted and is described. X-ray diffraction has been recorded from the protein molecules in the surface of the sarcoplasmic reticulum membrane. The protein molecules are not in an ordered array but appear to have a liquid-like ordering. The observation that vesicles can be prepared in a suitable form for X-ray analysis has importance for membrane research for many different membranes form vesicles and it follows that these membranes can now be profitably studied by X-ray diffraction using a similar method.     

Analysis and prediction of the packing of α-helices against a β-sheet in the tertiary structure of globular proteins

The packing of α-helices and β-sheets in six $\text{α}\text{β}$ proteins (e.g. flavodoxin) has been analysed. The results provide the basis for a computer algorithm to predict the tertiary structure of an $\text{α}\text{β}$ protein from its amino acid sequence and actual assignment of secondary structure.The packing of an individual α-helix against a β-sheet generally involves two adjacent ± 4 rows of non-polar residues on the α-helix at the positions i, i + 4, i + 8, i + 1, i + 5, i + 9. The pattern of interacting β-sheet residues results from the twisted nature of the sheet surface and the attendant rotation of the side-chains. At a more detailed level, four of the α-helical residues (i + 1, i + 4, i + 5 and i + 8) form a diamond that surrounds one particular β-sheet residue, generally isoleucine, leucine or valine. In general, the α-helix sits 10 Å above the sheet and lies parallel to the strand direction.The prediction follows a combinational approach. First, a list of possible β-sheet structures (10⁶ to 10¹⁴) is constructed by the generation of all β-sheet topologies and β-strand alignments. This list is reduced by constraints on topology and the location of non-polar residues to mediate the sheet/helix packing, and then rank-ordered on the extent of hydrogen bonding. This algorithm was uniformly applied to 16 $\text{α}\text{β}$ domains in 13 proteins. For every structure, one member of the reduced list was close to the crystal structure; the root-mean-square deviation between equivalenced C^α atoms averaged 5.6 Å for 100 residues. For the $\text{α}\text{β}$ proteins with pure parallel β-sheets, the total number of structures comparable to or better than the native in terms of hydrogen bonds was between 1 and 148. For proteins with mixed β-sheets, the worst case is glyceraldehyde-3-phosphate dehydrogenase, where as many as 3800 structures would have to be sampled. The evolutionary significance of these results as well as the potential use of a combinatorial approach to the protein folding problem are discussed.     

Transverse location of the retinal chromophore of rhodopsin in rod outer segment disc membranes

Diffusion-enhanced fluorescence energy transfer was used to study the structure of photoreceptor membranes from bovine retinal rod outer segments. The fluorescent energy donor was Tb³⁺ chelated to dipicolinate and the acceptor was the 11-cis retinal chromophore of rhodopsin in vesicles made from disc membranes. The rapid-diffusion limit for energy transfer was attained in these experiments because of the long excited state lifetime of the terbium donor (~2 ms). Under these conditions, energy transfer is very sensitive to a, the distance of closest approach between the donor and acceptor (Thomas et al., 1978). Vesicles containing terbium dipicolinate in their inner aqueous space were prepared by sonicating disc membranes in the presence of this chelate and chromatographing this mixture on a gel filtration column. The sidedness of rhodopsin in these vesicles was the same as in native disc membranes. The transfer efficiency from terbium to retinal in this sample was 43%. For an R₀ value of 46.7 Å and an average vesicle diameter of 650 Å, this corresponds to an a value of 22 Å from the inner aqueous space of the vesicle. The distance of closest approach from the external aqueous space, determined by adding terbium dipicolinate to a suspension of already formed vesicles, was found to be 28 Å. These values of a show that the retinal chromophore is far from both aqueous surfaces of the disc membrane. Hence, the transverse location of the retinal chromophore is near the center of the hydrophobic core of the disc membrane. These findings suggest that conformational changes induced by photoisomerization are transmitted through a distance of at least 20 Å within rhodopsin to trigger subsequent events in visual excitation.     

The plasmalemmal vesicular system in striated muscle capillaries and in pericytes

By ultrathin serial sectioning of frog mesenteric capillaries it was recently demonstrated that the many apparently free vesicles in electron microscope (EM) sections of endothelial cells may be artefacts due to conventional (500–700 Å thick) sectioning (Frøkjaer-Jensen, 1980). The vesicles were found to be part of two sets of invaginations of the cell surfaces; one set connected to the lumen, the other to the interstitium. The present study extends this view to comprise the vesicle organization in frog striated muscle capillaries. By analysis of the three-dimensional organization of the plasmalemmal vesicles in 21 ultrathin serial sections (120–150 Å) of two muscle capillaries it is demonstrated that less than 1% of the about 70% apparently free vesicles seen in conventional thin sections of the same capillaries in fact represent truly free vesicular units. By analysis of 15 conventional EM cross-sections of capillaries from the frog cutaneous-pectoris muscle containing plasmaproteins in high concentration it is furthermore demonstrated that 48% of the total vesicle population connect to the lumen at the time of fixation. This organization of the vesicular system seems incompatible with the concept that macromolecules are transferred across the capillary wall by vesicular transport or by a series of fusions and fissions between individual cytoplasmic vesicles but is compatible with the notion that macromolecules exchange across capillary walls by means of passive processes such as diffusion and convection through rare ‘large pores’. The study emphasizes that any attempts to classify vesicles in conventional thin sections as ‘luminal’, ‘cytoplasmic’ and ‘abluminal’ is impossible and may lead to erroneous interpretations of vesicle involvement in transcapillary exchange of macromolecules. The rare occurrence of transendothelial channels compared to the number of vesicle invaginations suggests that the main function of the vesicular system relates to functions other than transport.     

Structural analyses and yeast production of the β-1,3-1,4-glucanase catalytic module encoded by the licB gene of Clostridium thermocellum

A thermophilic glycoside hydrolase family 16 (GH16) β-1,3-1,4-glucanase from Clostridium thermocellum (CtLic16A) holds great potentials in industrial applications due to its high specific activity and outstanding thermostability. In order to understand its molecular machinery, the crystal structure of CtLic16A was determined to 1.95 Å resolution. The enzyme folds into a classic GH16 β-jellyroll architecture which consists of two β-sheets atop each other, with the substrate-binding cleft lying on the concave side of the inner β-sheet. Two Bis–Tris propane molecules were found in the positive and negative substrate binding sites. Structural analysis suggests that the major differences between the CtLic16A and other GH16 β-1,3-1,4-glucanase structures occur at the protein exterior. Furthermore, the high catalytic efficacy and thermal profile of the CtLic16A are preserved in the enzyme produced in Pichia pastoris, encouraging its further commercial applications.     

Molecular Symmetry of the ClpP Component of the ATP-dependent Clp Protease,anEscherichia coliHomolog of 20 S Proteasome

The ClpP component Clp protease fromEscherichia colihas been crystallized and examined by X-ray crystallography and self-rotation function calculations. The crystal belongs to the monoclinic space groupP2₁with unit cell dimensions ofa=196.9 Å,b=104.3 Å,c=162.4 Å and β=98.3°. The X-ray diffraction pattern extends at least to 2.5 Å Bragg spacing when exposed to CuKα X-rays. Self-rotation function analyses indicate that the ClpP oligomer has 72-point group symmetry. This symmetry suggests that the ClpP oligomer is a tetradecamer, (ClpP)₁₄, consisting of two heptamers, (ClpP)₇stacked on top of each other in a head-to-head fashion. The measurement of crystal density indicates that two independent copies of the ClpP oligomers are present in the asymmetric unit, giving a crystal volume per protein mass (V_M) of 2.73 ų/Da and a solvent content of 54.9% (v/v). Self-rotation function calculations are consistent with the presence of two ClpP tetradecamers in the asymmetric unit. The Patterson function suggests that a translation ofx=0.5 andy=0.5 relates a pair of ClpP oligomers in one asymmetric unit to another pair in the other asymmetric unit. And the two independent tetradecamers in one asymmetric unit are related by a relative rotation of about 18° around the 7-fold axis.     

The Crystal Structure of Glutamine-binding Protein fromEscherichia coli

The crystal structure of the glutamine-binding protein (GlnBP) fromEscherichia coliin a ligand-free “open” conformational state has been determined by isomorphous replacement methods and refined to anR-value of 21.4% at 2.3 Å resolution. There are two molecules in the asymmetric unit, related by pseudo 4-fold screw symmetry. The refined model consists of 3587 non-hydrogen atoms from 440 residues (two monomers), and 159 water molecules. The structure has root-mean-square deviations of 0.013 Å from “deal” bond lengths and 1.5° from “ideal” bond angles.The GlnBP molecule has overall dimensions of approximately 60 Å × 40 Å × 35 Å and is made up of two domains (termed large and small), which exhibit a similar supersecondary structure, linked by two antiparallel β-strands. The small domain contains three α-helices and four parallel and one antiparallel β-strands. The large domain is similar to the small domain but contains two additional α-helices and three more short antiparallel β-strands. A comparison of the secondary structural motifs of GlnBP with those of other periplasmic binding proteins is discussed.A model of the “closed form” GlnBP-Gln complex has been proposed based on the crystal structures of the histidine-binding protein-His complex and “open form” GlnBP. This model has been successfully used as a search model in the crystal structure determination of the “closed form” GlnBP-Gln complex by molecular replacement methods. The model agrees remarkably well with the crystal structure of the Gln-GlnBP complex with root-mean-square deviation of 1.29 Å. Our study shows that, at least in our case, it is possible to predict one conformational state of a periplasmic binding protein from another conformational state of the protein. The glutamine-binding pockets of the model and the crystal structure are compared and the modeling technique is described.