Different packaging of DNA in the filamentous viruses Pf1 and Xf

Xf Virus DNA, like Pf1 DNA, is a single-stranded circular molecule and contains, within experimental error, the same number of nucleotides, 7400. This was unexpected since Pf1 virus is 2 μm long while Xf virus is only 1 μm long. The ratio of nucleotides to major coat protein subunits has been found to be nearly unity in Pf1 and nearly two in Xf, but it is not certain that the ratios have exactly integer values. Calculations give the average axial internucleotide separation in Pf1virus as 5.3 Å whereas in Xf virus, the calculated separation is only 2.6 Å. The protein subunits in both Pf1 and Xf have calculated axial separations close to 2.6 Å. The results provide a solution to a problem encountered in the interpretation of X-ray diffraction patterns of these viruses concerning the number of protein subunits per helical turn.     

Caulobacter crescentus bacteriophage phiCbK: structure and in vitro self-assembly of the tail

Electron micrographs of negatively stained and platinum-shadowed bacteriophage φCbK have been analyzed by optical diffraction and computer Fourier transformation. The results show that the phage tail is a helical “stacked disc” structure with an annular repeat of about 38 Å and with 3-fold rotational symmetry about the helix axis. Phage tails exhibited lateral and rotational flexibility and were found to possess variable helical parameters. The smaller angle of rotation about the helix axis between equivalent asymmetric units on adjacent discs measured from a number of tail images was found to have an average value of 41.5±0.9 °. Cross-sectional views of short tail fragments were obtained after sonication at 0 °C. These views confirmed the 3-fold symmetry of the 38 Å annular unit, which most probably consists of three identical subunits of the major tail protein. Formation of extended tail polymers, both linear and circular, was found to take place spontaneously in vitro after sonication. On the basis of these results, a low-resolution model for the tail helix is presented. The questions of head-tail symmetry mismatch in the phage and of tail length regulation are discussed.     

On the structure of agglutinated sheep red blood cell membranes

Specimens of isolated sheep red blood cell membranes are prepared by an agglutination technique in which membranes are stacked in regular arrays. X-ray diffraction patterns are recorded from such specimens which show meridional and equatorial diffraction phenomena. The meridional reflections correspond to single lamellar repeat periods of 160–186 Å. It is concluded that two asymmetric membranes are contained inthe elementary period. Lipid phases with preferentialyl oriented hydrocarbon chains are part of the membrane structure. The stacking of membranes is also demonstrated in the electron microscope. The X-ray scattering curve of intracellular hemoglobin of intact sheep red blood cells is recorded to a spacing of about 8 Å^?1. The broad diffraction rings of this scattering curve are replaced by a series of rather sharp rings, when the red blood cells are agglutinated and placed in a hypertonic medium. Both the presence of a functioning membrane and the agglutination appear to be essential for the full expression of this phenomenon.     

Crystal structure of (Gly-Pro-Hyp)(9) : implications for the collagen molecular model

Collagens have long been believed to adopt a triple‐stranded molecular structure with a 10/3 symmetry (ten triplet units in three turns) and an axial repeat of 29 Å. This belief even persisted after an alternative structure with a 7/2 symmetry (seven triplet units in two turns) with an axial repeat of 20 Å had been proposed. The uncertainty regarding the helical symmetry of collagens is attributed to inadequate X‐ray fiber diffraction data. Therefore, for better understanding of the collagen helix, single‐crystal analyses of peptides with simplified characteristic amino acid sequences and similar compositions to collagens have long been awaited. Here we report the crystal structure of (Gly‐Pro‐Hyp)₉ peptide at a resolution of 1.45 Å. The repeating unit of this peptide, Gly‐Pro‐Hyp, is the most typical sequence present in collagens, and it has been used as a basic repeating unit in fiber diffraction analyses of collagen. The (Gly‐Pro‐Hyp)₉ peptide adopts a triple‐stranded structure with an average helical symmetry close to the ideal 7/2 helical model for collagen. This observation strongly suggests that the average molecular structure of collagen is not the accepted Rich and Crick 10/3 helical model but is a 7/2 helical conformation. © 2012 Wiley Periodicals, Inc. Biopolymers 97: 607–616, 2012.     

Mass,length, composition and structure of the filamentous bacterial virus fd

Determinations by three independent methods gave an average of (14.6 ± 0.6) × 10⁶ daltons for the anhydrous mass of the filamentous bacterial virus fd; a determination of the mass per unit length by light scattering of the virus in solution gave 1560 ±60 daltons/Å; and three independent methods show that 12.0±O.2% of the virus mass is from the single-stranded circular DNA molecule. The data give an average axial distance of 3.82 ±0.15 Å between major coat protein subunits (5240 daltons each) for virus in solution. The DNA has an up strand and a down strand within the filament, and an average axial distance of 3.29 ± 0.14 Å between neighbouring nucleotides in a given strand is obtained from the data. There are 2.32 ±0.07 nucleotides per major coat protein subunit and hence each of the nucleotides cannot interact in the same way with subunits of coat protein. The results provide a basis for the interpretation of X-ray diffraction patterns of oriented fibers of the virus. The uncertainties cited above are 95% confidence limits.     

Filamentous Bacterial viruses

The filamentous bacterial virus is a simple and well-characterized model system for studying how genetic information is transformed into molecular machines. The viral DNA is a single-stranded circle coding for about 10 proteins. The major viral coat protein is largely α-helical, with about 46 amino acid residues. Several thousand identical copies of this protein in a helical array form a hollow cylindrical tube 1–2μ long, of outer diameter 60 Å and inner diameter 20 Å, with the twisted circular DNA extending down the core of the tube. Before assembly, the viral coat protein spans the cell membrane, and assembly involves extrusion of the coat from the membrane. X-ray fibre diffraction patterns of the Pf 1 species of virus at 4°C, oriented in a strong magnetic field, give three-dimensional data to 4 Å resolution. An electron density map calculated from native virus and a single iodine derivative, using the maximum entropy technique, shows a helix pitch of 5.9 Å. This may indicate a stretched A-helix, or it may indicate a partially 3₁₀ helix conformation, resulting from the fact that the coat protein is an integral membrane protein before assembly, and is still in the hydrophobic environment of other coat proteins after assembly.     

Different arrangements of protein subunits and single-stranded circular DNA in the filamentous bacterial viruses fd and Pf1

A single-stranded circular DNA molecule of 6690 ± 450 nucleotides accounts for 5.5 ± 0.3% of the mass of Pf1 virus. The remaining mass is contributed almost entirely by subunits of the major coat protein. A non-integral nucleotide to subunit ratio of 0.87 ± 0.05 is calculated from the DNA content, the average nucleotide mass (309), and the known mass of one protein subunit (4609). There are therefore 7690 ± 680 major coat protein subunits in the virus. The virus length determined by electron microscopy is 1960 ± 70 nm. The data give an average axial distance of 2.55 ± 0.24 Å between protein subunits in dry virus. Since there is an up strand and a down strand of the circular DNA within the virus filament, an axial distance between bases in a given strand of 5.9 ± 0.5 Å is calculated. Available X-ray data show that an axial repeat of 72 Å, or slightly less, would be expected for dry Pf1 virus (0% relative humidity). A structural model in which 27 protein subunits and 24 nucleotides are contained in this repeat would be consistent with our data. The DNA conformation and the subunit packing in Pf1 differ considerably from those in fd, even though both are filamentous viruses containing single-stranded circular DNA. The uncertainties cited are 95% confidence limits.     

Molecular organization of amyloid protofilament-like assembly of betabellin 15D: helical array of beta-sandwiches

Betabellin is a 32-residue peptide engineered to fold into a four-stranded antiparallel beta-sheet protein. Upon air oxidation, the betabellin peptides can fold and assemble into a disulfide-bridged homodimer, or beta-sandwich, of 64 residues. Recent biophysical and ultrastructural studies indicate that betabellin 15D (B15D) (a homodimer of HSLTAKIpkLTFSIAphTYTCAVpkYTAKVSH, where p = DPro, k = DLys, and h = DHis) forms unbranched, 35-A wide assemblies that resemble the protofilaments of amyloid fibers. In the present study, we have analyzed in detail the X-ray diffraction patterns of B15D prepared from acetonitrile. The fiber diffraction analysis indicated that the B15D fibril was composed of a double helix defined by the selection rule l = n + 7m (where l is even, and n and m are any integers), and having a 199-A period and pitch, 28-A rise per unit, and 10-A radius. This helical model is equivalent to a reverse-handed, single helix with half the period and defined by the selection rule l = -3n + 7m (where l is any integer). The asymmetric unit is the single B15D beta-sandwich molecule. These results suggest that the betabellin assembly that models the protofilaments of amyloid fibers is made up of discrete subunits on a helical array. Multiple intersheet hydrogen bonds in the axial direction and intersandwich polar interactions in the lateral direction stabilize the array.     

A Proposal For A Specific Double-Helical Structure In Which The Polynucleotide Strands Intercalate Instead of Forming Base-pairs

Abstract

Double helices, since the discovery of the DNA structure by Watson and Crick, represent the single most important secondary structural form of nucleic acids. The secondary structures of a variety of polynucleotide helices have now been well characterised with hydrogen- bonded base-pairs as building blocks. We wish to propose here the possibility, in a specific case, of a double stranded helical structure without any base-pair, but having a repeat unit of two nucleotides with their bases stacked through intercalation. The proposal comes from the initial models we have built for poly(dC) using the stacking patterns found in the crystal structures of 5′-dCMPNa₂ which crystallises in two forms depending on the degree of hydration. These structures have pairs of nucleotides with the cytosine rings partially overlapping and separated by 3.3Å. Using these as repeat units one could generate a model for poly(dC) with parallel strands, having a turn angle of 30° and a base separation of 6.6Å along each strand. Both right and left handed models with these parameters can be built in a smooth fashion without any obviously unreasonable stereochemical contacts. The helix diameter is about 13.5Å, much smaller than that of normal helices with base-pair repeats. The changes in the sugar-phosphate backbone conformation in the present models compared to normal duplexes only reflect the torsional flexibility available for extension of polynucleotide chains as manifested by the crystal structures of drug-inserted oligonucleotide complexes. Intercalation proposed here could have some structural relevance elsewhere, for instance to the base-mismatched regions on the double helix and the packing of noncomplementary single strands as found in the filamentous bacteriophage Pf1.     

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.     

Coat protein polymerization of alfalfa mosaic virus strain VRU

The association behaviour of the coat protein of alfalfa mosaic virus strain VRU was studied by sedimentation analysis and electron microscopy. The results of this study were compared with the data obtained from similar studies with the coat protein of strain 425 (Driedonks et al., 1977). In the depolymerized state VRU protein is likely a dinier of the 24,050 molecular weight polypeptide chain. The main association product is a tubular structure with a diameter of about 180 Å. The optimum conditions for the reaction were polyphosphate-containing buffer at pH 6·5. Optical diffraction analysis of negatively stained specimens revealed a helical arrangement of the protein subunits in these assemblies. The same type of reaction product was found when the association reaction was carried out in the presence of polynucleotides. The length of the VRU particles is abnormally long compared to other alfalfa mosaic virus strains. This phenomenon can be ascribed to the tendency of the protein to polymerize into tubular rather than spherical particles.     

Model for the capsid structure of alfalfa mosaic virus.

The coat protein of alfalfa mosaic virus is clustered in such a way as to avoid the 3 and 6-fold lattice positions of the hexagonal surface lattice. This results in a relatively open structure for the capsid, which is mainly caused by holes situated at the 6-fold positions and, to a minor extent, those present at the 3-fold lattice points. The evidence for this has been obtained by analysing electron micrographs of negatively stained virus particles by optical diffraction and digital image processing.     

Structures of Helical Plant Virus Ribonucleoproteins as Assessed by Tritium Planigraphy and Theoretical Modeling

This review considers the results of probing the structure of ribonucleoprotein particles of helical plant viruses by tritium planigraphy (TP). This method works by exposing macromolecular targets to a beam of tritium atoms and analyzing the tritium label distribution along the macromolecule length. The TP data combined with theoretical predictions made it possible to propose a structural model of the coat protein for the virions of potato viruses X (the type representative of potexviruses) and A (a potyvirus), which eluded X-ray diffraction analysis so far. TP revealed fine structural differences between the wild-type tobacco mosaic virus (strain U1) and its temperature-sensitive mutant with an altered coat protein and host specificity. The possibilities of using TP for studying the RNA–protein interactions in helical virus particles are discussed.     

An X-ray study of poly(L-prolyl-L-alpha-phenylglycyl-L-proline).

X-ray diffraction studies have been made on the polytripeptide poly(L -prolyl-L -α-phenylglycyl-L -proline). Its structure has been found to be helical, with a poly(L -proline) II conformation, packed in an orthorhombic lattice, space group P2₁2₁2, with a = 14.3 Å, b = 13.5 Å, and c = 9.4 Å.     

Helical arrays of Escherichia coli small ribosomal subunits produced in vitro.

In vitro conditions have been determined for obtaining ordered helical ribbons of small ribosomal subunits from Escherichia coli. These ribbons, suitable for study by three-dimensional reconstruction, are the first ordered arrays of ribosomes or ribosomal subunits to be produced in vitro.Although small ribosomal subunits remain in solution for extended periods (up to 6 months) during this procedure, their structural integrity, as assessed by acrylamide/agarose gel electrophoresis, by sucrose gradients, and by electron microscopy, is not significantly altered.Electron micrographs of ribbons of small subunits diffract to 60 Å resolution. Optical diffraction patterns suggest that adjacent subunits within helical ribbons are related by a 2-fold screw parallel to the long axis of the ribbon and the helical repeat distance measured from electron micrographs is 220 Å.     

Cross-Bridges and Periods in Insect Flight Muscle

The periodic structure of the cross-bridge lattice of glycerinatedLethocerus flight muscle has been studied in sections by electronmicroscopy, assisted by optical diffraction, and in unfixedfiber bundles by X-ray diffraction. Diffraction patterns exhibitfirst through ninth orders of 1166 Ä, virtually all ofwhich were found to arise from the lattice of cross-bridges.Diffraction and inspection show that "horizontal" cross-bridgesof relaxation become slanted in rigor, and may push actins towardthe M line in producing the increase in tension seen with theinduction of rigor. Myosin filaments contain unexpected structural features. Cross-bridgeorigins form opposed pairs repeating every 146 Ä; and rotating67.5 degrees with each repeat, thus defining twin, left-handed,helical tracks which require 1 turns (or 8 x 146 Ä) toestablish a meridional repeat of 1166 Ä. Each origin isdual and gives rise to two bridges; thus, the unit groupingof paired origins involves four bridges. One half-turn of themyosin helix requires 388 Ä, matching the actin helix exactlyin pitch. (Actin is, however, right-handed.) The resulting matchseems awkward azimuthally (sixteenfold myosin distributes bridgesto a sixfold envelope of actin filaments), but minimizes axialmismatching between subunits of the myosin and actin and lendscredence to the theory that all bridges may swing synchronouslyduring typical, low-amplitude, oscillatory contractions.     

Three-dimensional reconstruction of the flagellar hook from Caulobacter crescentus

The structure of the bacterial flagellar hook produced by a mutant of Caulobacter crescentus was studied by electron microscopy, optical diffraction, and digital image processing techniques. The helical surface lattice of the hook is defined by a single, right-handed genetic helix having a pitch of about 23 Å, an axial rise per subunit of 4 Å and an azimuthal angle between subunits of 64·5 °. The lattice is also characterized by intersecting families of 5-start, 6-start and long-pitch 11-start helices. These helical parameters are remarkably similar to those determined for the flagellar filaments from several strains of gram-negative bacteria. The technique of three-dimensional image reconstruction (DeRosier & Klug, 1968) was applied to nine of the better preserved specimens and the diffraction data from five of these were correlated and averaged and used to generate an average three-dimensional model of the hook. The pattern of density modulations in the three-dimensional model is suggestive of an elongated, curved shape for the hook subunit (100 Å × 25 Å × 25 Å). The subunits are situated in the lattice of the polyhook such that their long axes are tilted about 45 ° with respect to the hook axis. The subunits appear to make contact with each other along the 6-start helices at a radius of 80 Å and also along the 11-start helices at a radius of 65 Å. Few structural features are revealed at radii between 15 å and 45 Å and, therefore, we are unable to decide to what extent the hook subunits extend into this region. The most striking characteristic of the model is the presence of deep, broad, continuous 6-start helical grooves extending from an inner radius of about 50 Å to the perimeter of the particle at 105 Å radius. Normal hooks usually appear curved in electron micrographs and sometimes so are the mutant hooks; the prominent 6-start grooves appear to allow for bending with minimal distortion of matter in the outer regions of the hook. A round stain-filled channel about 25 Å in diameter runs down the center of the polyhook. Such a channel supports a model for flagellar assembly in which flagellin subunits travel through the interior of the flagellum to the growing distal end of the filament.     

Helical structure of Bordetella pertussis fimbriae.

The helical structures of Bordetella pertussis fimbriae of serotypes 2 and 6 were determined by optical diffraction analysis of electron micrographs of negatively stained paracrystalline bundles of purified fimbriae. The fimbrial structure is based on an axial repeat of 13 nm that contains five repeating units in two complete turns of a single-start helix. This structure was confirmed by direct measurements of mass per unit length for individual fimbriae performed by dark-field scanning transmission electron microscopy of unstained specimens. These data further established that the helically repeating unit is a monomer of fimbrial protein (Mr congruent to 22,000 for type 2 and Mr congruent to 21,500 for type 6). Radial density profiles calculated from the scanning transmission electron micrographs showed that the fimbria has peak density at its center, i.e., no axial channel, consistent with the results of conventional negative-staining electron microscopy. The radial profile gives an outermost diameter of approximately 7.5 nm, although the peripheral density is, on average, diffuse, allowing sufficient intercalation between adjacent fimbriae to give a center-to-center spacing of approximately 5.5 nm in the paracrystals. Despite serological and biochemical differences between type 2 and type 6 fimbriae, the packing arrangements of their fimbrial subunits are identical. From this observation, we infer that the respective subunits may have in common conserved regions whose packing dictates the helical geometry of the fimbria. It is plausible that a similar mechanism may underlie the phenomenon of phase variations in other systems of bacterial fimbriae.     

The structural relationship between the stacked disk and helical polymers of tobacco mosaic virus protein

An X-ray diffraction pattern from a well-oriented sol of the stacked disk rod aggregate of the protein of tobacco mosaic virus is presented. The helical parameters deduced from this are consistent with the stacked disk rod being a perturbed form of a stacked ring variant of the single helical polymer. Comparison of the intensity distributions in the X-ray diagrams of the two aggregates confirms their structural similarity.     

Conformation of the coat protein of filamentous bacteriophage Pf1 determined by neutron diffraction from magnetically oriented gels of specifically deuterated virions

The structure of filamentous bacteriophage Pf1 has been studied using neutron diffraction from magnetically oriented gels of native and valine-deuterated phage. Neutron diffraction intensities were measured to approximately 8 A resolution along the equator and first six layer-lines, and differences due to the deuterated valine residues were apparent. Analysis of equatorial data indicate that one valine residue is located at a radius of about 13 A, three are in the hydrophobic center of the protein coat at an average of about 22 A radius, and one is near the outer surface of the virion at about 28 A radius. Analysis of the three-dimensional data was initiated using the rod model for the alpha-helices of the coat protein derived from earlier X-ray diffraction studies. This model was refined against the neutron diffraction intensities from native phage to obtain a phase set that was used to calculate a difference map between the valine-deuterated and native phage. The difference map exhibits peaks that correspond to the positions of the five valine residues in the coat protein. From the amino acid sequence and the alpha-helical conformation of the coat protein, the five valine residues can be unambiguously assigned to the difference peaks. This assignment indicates that the two alpha-helices of the coat protein are parallel to one another, connected by a short stretch of non-helical peptide. The valine positions also indicate that the helical surface lattice of the phage particle is right-handed.