The fine structure of myocytes in the sponges microciona prolifera (Ellis and Solander) and tedania ignis (Duchassaing and Michelotti)

Myocytes are long, fusiform cells found in the osculum and other contractile areas of many sponges. Myocytes in the oscular sphincter of Tedania ignis and the osculum and dermal membrane of Microciona prolifera were studied with light- and electron-microscopes to compare their structure to that of muscles. Salient points of similarity between myocytes and smooth muscles were their long, fusiform shape, their red color after staining with Mallory's triple stain, and the presence of filaments running longitudinally in the cytoplasm. Microciona myocytes have thick filaments of 150–250 Å diameter and thin filament of 50–70 Å diameter, and in transverse sections the thin filaments occasionally appear as a ring of dots around a thick filament. Longitudinal sections of Tedania myocytes show only one type of filament, which varies from 100 Å to 200–300 Å diameter in thick regions of the filament. Although transverse sections show light material around the dense filaments, a distinct pattern of thick and thin filaments is not seen in Tedania. Due to infrequent contacts between cells, the large extra-cellular space observed with the electron microscope (49% in Tedania, 57% in Microciona), and the absence of nerves, each myocyte probably acts as an independent contractile unit.     

Filamentous bacterial viruses. XI. Molecular architecture of the class II (Pf1, Xf) virion

The diffraction patterns of the Pf 1 and Xf strains of filamentous bacterial viruses (class II) can be interpreted in terms of a simple helix of protein subunits with 15Åpitch, having 22 units in five turns. The protein subunits are each elongated in an axial direction, and also slope radially, so as to overlap each other, giving an arrangement of subunits reminiscent of scales on a fish. The protein helix forms a tube with inner diameter about 20Åand outer diameter about 60Å. The single-stranded circular DNA is contained within this tube, with two DNA strands running the length of the tube.The diffraction patterns of fd, If 1 and IKe (class I) can be interpreted in terms of a perturbed version of the class II simple helix.     

X-ray diffraction and electron microscope studies on the structure of bacterial F pili.

F pili are hollow cylinders with 80 Å outer diameter and 20 Å inner diameter. Both X-ray fibre diffraction and optical diffraction of electron micrographs show a strong layer-line corresponding to a spacing of 32 Å, to which a J₄ Bessel function is assigned on the basis of the optical diffraction. X-ray diffraction patterns show near-meridional intensity on a layer-line corresponding to a spacing of 12.8 Å, to which a J₁ Bessel function is assigned. Mass per length measurements on unstained specimens in the scanning transmission electron microscope give 3000 daltons/Å, indicating that the 11,200 dalton pilin subunits are 3.7 Å apart along the axial direction of the pili. These observations show that the pilus structure can be represented as four coaxial helices of pitch 128 Å with the pilin subunits elongated and overlapping along the line of these helices. Each of these helices of subunits is translated axially with respect to its neighbour, to give a basic helix of 3.6 units per turn of 12.8 Å pitch. Radial electron density calculations indicate a 50 Å diameter girdle of hydrophobic amino acids between the inner and outer diameters of the protein shell. A molecular model of the structure at low resolution is presented.     

The structural basis for the intrinsic disorder of the actin filament: the "lateral slipping" model

Three-dimensional (3-D) helical reconstructions computed from electron micrographs of negatively stained dispersed F-actin filaments invariably revealed two uninterrupted columns of mass forming the "backbone" of the double-helical filament. The contact between neighboring subunits along the thus defined two long-pitch helical strands was spatially conserved and of high mass density, while the intersubunit contact between them was of lower mass density and varied among reconstructions. In contrast, phalloidinstabilized F-actin filaments displayed higher and spatially more conserved mass density between the two long-pitch helical strands, suggesting that this bicyclic hepta-peptide toxin strengthens the intersubunit contact between the two strands. Consistent with this distinct intersubunit bonding pattern, the two long-pitch helical strands of unstabilized filaments were sometimes observed separated from each other over a distance of two to six subunits, suggesting that the intrastrand intersubunit contact is also physically stronger than the interstrand contact. The resolution of the filament reconstructions, extending to 2.5 nm axially and radially, enabled us to reproducibly "cut out" the F-actin subunit which measured 5.5 nm axially by 6.0 nm tangentially by 3.2 nm radially. The subunit is distinctly polar with a massive "base" pointing towards the "barbed" end of the filament, and a slender "tip" defining its "pointed" end (i.e., relative to the "arrowhead" pattern revealed after stoichiometric decoration of the filaments with myosin subfragment 1). Concavities running approximately parallel to the filament axis both on the inner and outer face of the subunit define a distinct cleft separating the subunit into two domains of similar size: an inner domain confined to radii less than or equal to 2.5-nm forms the uninterrupted backbone of the two long-pitch helical strands, and an outer domain placed at radii of 2-5-nm protrudes radially and thus predominantly contributes to the outer part of the massive base. Quantitative evaluation of successive crossover spacings along individual F-actin filaments revealed the deviations from the mean repeat to be compensatory, i.e., short crossovers frequently followed long ones and vice versa. The variable crossover spacings and diameter of the F-actin filament together with the local unraveling of the two long-pitch helical strands are explained in terms of varying amounts of compensatory "lateral slipping" of the two strands past each other roughly perpendicular to the filament axis. This intrinsic disorder of the actin filament may enable the actin moiety to play a more active role in actin-myosin-based force generation than merely act as a rigid passive cable as has hitherto been assumed.     

Electron microscopy of the stacked disk aggregate of tobacco mosaic virus protein. I. Three-dimensional image reconstruction

The three-dimensional structure of the stacked disk aggregate of tobacco mosaic virus protein has been determined from “phase plate” electron micrographs to an effective resolution of about 12 Å. It is a long rod comprised of paired rings of protein (disks), the subunits of which have different conformations according to which ring they belong. The two subunit conformations are such that the rings come close together within a disk near the outer surface of the particle, but between disks on the inside. This property, interpreted on the basis of a polar packing of the subunits, was established from an earlier, lower resolution, study by Finch &; Klug (1971). The present study shows, in addition, that the pairing is contributed mainly by axial distortions of the subunits in one of the rings, the axial distortions of the subunits in the other being largely replaced at lower radii by a tilt or twist and, at higher radii, by a slew. The subunits in the latter ring appear to have a conformation similar to that of the protein molecules in the virus.     

The cryptophycin-tubulin ring structure indicates two points of curvature in the tubulin dimer

Cryptophycin-1 is the parent compound of a group of cyclic peptides with potent antineoplastic activity. Cryptophycins are thought to function by modulating the dynamic instability of spindle microtubules, and in vitro are known to bind in an equimolar ratio to the beta-tubulin subunit and to induce the formation of ring-like complexes. However, the detailed mechanisms whereby the cryptophycins interact with tubulin are not known. We have investigated the origin of the conformational changes in tubulin both biochemically and by electron microscopy and image analysis. Cryptophycin was found to protect both alpha- and beta-tubulin against proteolysis by trypsin, indicating conformational changes in specific regions of both subunits. The ring mass was determined to be approximately 0.81 MDa by sedimentation velocity combined with dynamic light scattering and by STEM, indicating a complex of eight alphabeta dimers. Statistical analysis of rings imaged by cryoelectron microscopy revealed 16-fold symmetry, corresponding to eight dimers. Computational averaging based on this symmetry yielded an image of a 24 nm diameter ring, at 2.6 nm resolution, that clearly distinguishes intradimer contacts from interdimer contacts, and allows discrimination of alpha-subunits from beta-subunits. Fitting of the tubulin dimer crystal structure into this projected density map indicates two points of curvature: a 13 degrees intradimer bend and a 32 degrees interdimer bend. We conclude that drug binding to one subunit (beta) results in two bends per dimer, affecting both subunits.     

Structures of the “open” and “closed” state of trypanosomal triosephosphate isomerase,as observed in a new crystal form: Implications for the reaction mechanism

The structure of trypanosomal triosephosphate isomerase (TIM)has been solved at a resolution of 2.1Å in a new crystal form grown at pH 8.8 from PEG6000. In this new crystal form (space group C2, cell dimensions 94.8 Å, 48.3 Å, 131.0 Å, 90.0°, 100.3°, 90.0°), TIM is present in a ligand-free state. The asymmetric unit consists of two TIM subunits. Each of these subunits is part of a dimer which is sitting on a crystallographic twofold axis, such that the crystal packing is formed from two TIM dimers in two distinct environments. The two constituent monomers of a given dimer are, therefore, crystallographically equivalent. In the ligand-free state of TIM in this crystal form, the two types of dimer are very similar in structure, with the flexible loops in the “Open” conformation. For one dimer (termed molecule-1), the flexible loop (loop-6) is involved in crystal contacts. Crystals of this type have been used in soaking experiments with 0.4 M ammonium sulphate (studied at 2.4 Å resolution), and with 40 μM phosphoglycolohydroxamate (studied at 2.5 Å resolution). It is found that transfer to 0.4 M ammonuum sulphate (equal to 80 times the Ki of sulphate for TIM), gives rise to significant sulphate binding at the active site of one dimer (termed molecule-2), and less significant binding at the active site of the other. In neither dimer does sulphate induce a “closed” conformation. In a mother liquor containing 40 μM phosphoglycolohydroxamate (equal to 10 times the Ki of phosphoglycolohydroxamate for TIM), an inhibitor molecule binds at the active site of only that dimer of which the flexible loop is free from crystal contacts (molecule-2). In this dimer, it induces a closed conformation. These three structures are compared and discussed with respect to the mode of binding of ligand in the active site as well as with respect to the conformational changes resulting from ligand binding. © 1993 Wiley-Liss, Inc.     

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.     

ON THE RELATIONSHIP OF BRAIN FILAMENTS TO MICROTUBULES1

Abstract— A method has been developed for the isolation of a previously undescribed fibrous protein from rat brain. The newly isolated material consists of bundles of tightly packed 70-80 Å diameter filaments. Based on studies employing degenerated rat optic nerve, it is proposed that these filaments correspond to the well-described astrocyte filaments observed in sectioned preparations of mammalian brain. The purified filaments are stable over a wide temperature range, are not disrupted by colchicine, and exhibit limited solubility in the absence of denaturants or detergents. In neutral SDS-polyacrylamide gel electrophoresis, the filament protein runs as a single band with an apparent molecular weight of 57,000 daltons. This preparation also migrates as a single band in alkaline urea gels, and as a well-resolved doublet on discontinuous SDS-urea gels. In all three electrophoretic systems, the filament subunits co-migrate with rat brain tubulin. Comparative peptide maps of the filament subunits and tubulin indicate a large degree of homology. Our results suggest that microtubules and astrocyte filaments are composed of the same or very similar protein subunits.     

X-ray microdiffraction reveals the orientation of cellulose microfibrils and the size of cellulose crystallites in single Norway spruce tracheids

The microfibril angle (MFA) distribution and the size of cellulose crystallites in isolated double cell walls of Norway spruce (Picea abies [L.] Karst.) tracheids were determined by synchrotron X-ray microdiffraction using the reflections 200 and 004. Samples were 25 μm thick longitudinal sections of earlywood from annual rings 6–18 of several stems. The asymmetric MFA distributions extended from ?20° to 90°. The mean MFA of tangential cell walls decreased from an average of 24° into 19° from the pith to the bark. The mode of the MFA distribution was about 10° smaller than the mean MFA. The standard deviation of the MFA distribution varied between 18° and 25°. The mean MFA and the mode of the MFA distribution were larger in radial than in tangential cell walls. MFA distributions of mature wood samples exhibited a separate small peak at around 90°. The average width and length of cellulose crystallites varied between 28.9–30.9 Å and 192–284 Å, respectively. Both increased slightly as a function of annual ring number from the pith up to the 15th annual ring. An irrigation–fertilisation treatment of some of the stems resulted in longer cellulose crystallites compared to the untreated stems.     

Metaphase chromosome structure: evidence for a radial loop model.

Electron micrographs of thin sections of metaphase chromosomes isolated from HeLa cells provide new insight into the higher-order arrangement of the nucleoprotein fiber. Micrographs obtained from chromosomes swollen by chelation of the divalent cation are particularly revealing. Under these conditions, chromosomes swell in width by a factor of about 4 and the basic, thick nucleoprotein fiber (200–300 Å) relaxes to the thin fiber (100 Å), which is probably a linear array of nucleosomes. Cross sections show a central area from which the fibers emerge in a radial fashion, often forming loops which are 3–4 μm long. Chromosomes fixed in the presence of 1 mM MgCl₂ are more compact, having an average chromatid diameter of about 1 μm, and consist of the thick (200–300 Å) fiber. Radial loops of about 0.6 μm can be observed frequently in these chromosomes, although the loops are more difficult to visualize due to the compactness of the structure and the material contaminating the periphery. Chromosomes isolated with the help of hexylene glycol are extremely compact (diameter about 0.6 μm) but quite free of cytoplasmic material. They consist of a 500 Å fiber that forms rather regular projections at the periphery. These projections appear to be loops of the thick fiber (200–300 Å), possibly shortened by twisting into a short supercoil. The chromatin loops observed in the intact chromosomes are thought to be structurally related to the DNA loops observed previously in the histone-depleted chromosomes (Paulson and Laemmli, 1977). In this paper, we discuss a model in which the nucleoprotein fiber is folded into loops which are arranged in the chromatid in radial fashion, in such a way that their bases become the central axis of the chromatid.     

Negative-stain electron microscopy of inside-out FtsZ rings reconstituted on artificial membrane tubules show ribbons of protofilaments

FtsZ, the primary cytoskeletal element of the Z ring, which constricts to divide bacteria, assembles into short, one-stranded filaments in vitro. These must be further assembled to make the Z ring in bacteria. Conventional electron microscopy (EM) has failed to image the Z ring or resolve its substructure. Here we describe a procedure that enabled us to image reconstructed, inside-out FtsZ rings by negative-stain EM, revealing the arrangement of filaments. We took advantage of a unique lipid that spontaneously forms 500 nm diameter tubules in solution. We optimized conditions for Z-ring assembly with fluorescence light microscopy and then prepared specimens for negative-stain EM. Reconstituted FtsZ rings, encircling the tubules, were clearly resolved. The rings appeared as ribbons of filaments packed side by side with virtually no space between neighboring filaments. The rings were separated by variable expanses of empty tubule as seen by light microscopy or EM. The width varied considerably from one ring to another, but each ring maintained a constant width around its circumference. The inside-out FtsZ rings moved back and forth along the tubules and exchanged subunits with solution, similarly to Z rings reconstituted outside or inside tubular liposomes. FtsZ from Escherichia coli and Mycobacterium tuberculosis assembled rings of similar structure, suggesting a universal structure across bacterial species. Previous models for the Z ring in bacteria have favored a structure of widely scattered filaments that are not in contact. The ribbon structure that we discovered here for reconstituted inside-out FtsZ rings provides what to our knowledge is new evidence that the Z ring in bacteria may involve lateral association of protofilaments.     

The organization and fine structure of the muscles of the scolex of the cysticercoid of Hymenolepis microstoma

The organization and fine structure of the muscles of the scolex of the cysticercoid of Hymenolepis microstoma are described. The contractile apparatus consists of thick (175–325 Å diameter × 1.4 μm) and thin (60–80 Å diameter × 1 μm) filaments. The thick filaments are occasionally attached to the thin filaments by cross bridges. The thin filaments are attached to the dense bodies or to a dense zone at the sarcolemma at muscle insertions. In contracted muscle the thick filaments appear as quasi-hexagonal arrays or in lines. Each thick filament is surrounded by an orbit of up to 12 thin filaments, which in turn may be shared by adjacent thick filaments. Thin filaments may be present in quasi-rectangular or hexagonal groupings indicating some low order degree of actin lattice. The fusiform dense bodies (1,500 Å × 900 Å), consisting of up to 25 discrete substructures, are distributed uniformly throughout the myofiber and/or attached to the sarcolemma at attachment plaques. The sarcoplasmic reticulum, consisting of a presumed anastomosing network of tubules is structurally connected to the sarcolemma by periodic deposits of electron opaque material. Sarcoplasmic extensions of the myofiber(s) contain the nucleus, Golgi complexes, rough endoplasmic reticulum, ribosomes, β-glycogen, mitochondria and membrane bound electron dense structures. Upon activation of the metacestode, groups of α-glycogen and enlargement of the rough endoplasmic reticulum were observed. Microtubules which were conspicuously absent from the sarcoplasm of the unactivated worms appeared adjacent to the myofibers in activated worms.     

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.     

Structure of the three-chain unit of the bovine epidermal keratin filament

The characteristic α-type X-ray diffraction pattern displayed by bovine epidermal keratin filaments can be ascribed to the presence of segments of triple-chain coiled coil α-helix in the repeating three-chain unit of the filaments.Limited proteolysis of filaments polymerized in vitro or a citrate-soluble protein derived from them with crystalline trypsin releases two types of α-helix-enriched particles which provide information on the structure of the three-chain unit. The smaller, particle 2, of molecular weight 42,500, α-helix content of 92% and dimensions of 180 Å × 20 Å, consists of three chains aligned side-by-side that presumably form a coiled coil. The high yields of particle 2 allow the conclusion that all of the α-helix of the epidermal keratin filament is present in the form of these discrete three-chain α-helical segments. The larger, particle 1, recovered during the earlier stages of digestion has a molecular weight of 100,000 to 110,000, α-helix content of 75%, average dimensions of 400 Å × 20 Å and also consists of three chains aligned side-by-side. It contains two α-helical segments corresponding to particle 2 which are located at the amino -terminal and carboxyl-terminal ends and are separated by a region of non-helix. Particle 1 contains all of the α-helix and therefore is the major portion of the three-chain unit of the keratin filament. The products resulting from reaction of intact filament subunits with N-bromosuccinimide suggest that particle 1 is formed during digestion by removal of regions of non-helix from each end of this unit.The structure of the three-chain unit of the bovine epidermal keratin filament may thus be viewed as three polypeptide subunits aligned side-by-side with two discrete coiled coil α-helical segments interspersed with regions of non-helix.     

Cofilin Changes the Twist of F-Actin: Implications for Actin Filament Dynamics and Cellular Function

Cofilin is an actin depolymerizing protein found widely distributed in animals and plants. We have used electron cryomicroscopy and helical reconstruction to identify its binding site on actin filaments. Cofilin binds filamentous (F)-actin cooperatively by bridging two longitudinally associated actin subunits. The binding site is centered axially at subdomain 2 of the lower actin subunit and radially at the cleft between subdomains 1 and 3 of the upper actin subunit. Our work has revealed a totally unexpected (and unique) property of cofilin, namely, its ability to change filament twist. As a consequence of this change in twist, filaments decorated with cofilin have much shorter ‘actin crossovers' (~75% of those normally observed in F-actin structures). Although their binding sites are distinct, cofilin and phalloidin do not bind simultaneously to F-actin. This is the first demonstration of a protein that excludes another actin-binding molecule by changing filament twist. Alteration of F-actin structure by cofilin/ADF appears to be a novel mechanism through which the actin cytoskeleton may be regulated or remodeled.     

Stages of tubulin assembly and disassembly studied by time-resolved synchrotron X-ray scattering

The structural transitions occurring during the assembly and disassembly of pig brain microtubule protein were investigated by time-resolved X-ray scattering using synchrotron radiation. The reactions were introduced by a slow temperature scan (2 deg.C/min) from 0 °C to 37 °C and back. Several structurally distinct states could be resolved during one cycle of assembly/disassembly. During the temperature rise, one observes four main phases: prenucleation events, microtubule nucleation, growth, and postassembly events.Heating from 0 °C to 22 °C results in a biphasic breakdown of rings and other aggregates, while the apparent mean diameter increases from 38 to 41 nm. Parallel time-resolved electron microscopic observations suggest that the initial solution contains several types of aggregates, mostly double concentric and single rings, but also rod-like particles, clusters of rings and other aggregates. All of these tend to break down with increasing temperature. Double concentric rings seem to dissociate into large and small single rings before both types of rings break down into protofilament fragments and tubulin subunits. From the breakdown products, associations of several protofilament fragments are formed, which are important for initiating microtubule nucleation. Assembly of nuclei begins around 22 °C. Microtubule elongation takes place between 25 and 30 °C. They grow mainly by addition of tubulin subunits but not via rings.During the reverse temperature scan, microtubules shorten by the release of subunits and/or small protofilament fragments from their ends. The degree of disassembly is strongly increased below 22 °C. Below about 10 °C rings are reformed, probably from the fragments, but their final number is much less than initially.Conditions that prevent microtubule nucleation such as GDP or Ca²⁺ also stabilize rings, even at 37 °C. Thus, rings are viewed as storage aggregates of tubulin and microtubule associated proteins, whose breakdown is a prerequisite for microtubule formation, and whose reformation is independent of microtubule breakdown.The midpoints of microtubule growth and breakdown differ by about 12 deg.C so that the system shows hysteresis-like behavior. It is dependent on microtubule formation and is not seen when the temperature is cycled below that required for nucleation. Thus, even during a slow temperature scan, microtubule assembly is kinetically limited by nucleation. By contrast, depolymerization proceeds close to equilibrium.The radius of gyration of the tubulin heterodimers is 3.1 nm. The weight average diameter of rings in cold solutions is 38 nm, that of microtubules is 24.5 nm.At radiation dose rates of about 100 rad/s. radiation damage is of minor importance, as judged by the criterion of polymerizability. Total doses of up to 500,000 rad can be applied.Some concepts of analyzing time-resolved X-ray scattering data are presented. They make use of the fact that the scattering intensities vary continuously both with scattering angle and time. Cross-correlation of different regions of the pattern, and comparison of their temperature derivatives, reveals structural transitions not seen by other techniques.     

Assembly architecture and DNA binding of the bacteriophage P22 terminase small subunit

Morphogenesis of bacteriophage P22 involves the packaging of double-stranded DNA into a preassembled procapsid. DNA is translocated by a powerful virally encoded molecular motor called terminase, which comprises large (gp2, 499 residues) and small (gp3, 162 residues) subunits. While gp2 contains the phosphohydrolase and endonuclease activities of terminase, the function of gp3 may be to regulate specific and nonspecific modes of DNA recognition as well as the enzymatic activities of gp2. Electron microscopy shows that wild-type gp3 self-assembles into a stable and monodisperse nonameric ring. A three-dimensional reconstruction at 18 Å resolution provides the first glimpse of P22 terminase architecture and implies two distinct modes of interaction with DNA—involving a central channel of 20 Å diameter and radial spikes separated by 34 Å. Electromobility shift assays indicate that the gp3 ring binds double-stranded DNA nonspecifically in vitro via electrostatic interactions between the positively charged C-terminus of gp3 (residues 143-152) and phosphates of the DNA backbone. Raman spectra show that nonameric rings formed by subunits truncated at residue 142 retain the subunit fold despite the loss of DNA-binding activity. Difference density maps between gp3 rings containing full-length and C-terminally truncated subunits are consistent with localization of residues 143-152 along the central channel of the nonameric ring. The results suggest a plausible molecular mechanism for gp3 function in DNA recognition and translocation.     

The structure of F-pili

Exchange of DNA between bacteria involves conjugative pili. While the prevailing view has been that F-pili are completely retracted before single-stranded DNA is passed from one cell to another, it has recently been reported that the F-pilus, in addition to establishing the contact between mating cells, serves as a channel for passing DNA between spatially separated cells during conjugation. The structure and function of F-pili are poorly understood. They are built from a single subunit having only 70 residues, and the small size of the subunit has made these filaments difficult to study. Here, we have applied electron cryo-microscopy and single-particle methods to solve the long-existing ambiguity in the packing geometry of F-pilin subunits. We show that the F-pilus has an entirely different symmetry from any of the known bacterial pili as well as any of the filamentous bacteriophages, which have been suggested to be structural homologs. Two subunit packing schemes were identified: one has stacked rings of four subunits axially spaced by ∼ 12.8 Å, while the other has a one-start helical symmetry with an axial rise of ∼ 3.5 Å per subunit and a pitch of ∼ 12.2 Å. Both structures have a central lumen of ∼ 30 Å diameter that is more than large enough to allow for the passage of single-stranded DNA. Remarkably, both schemes appear to coexist within the same filaments, in contrast to filamentous phages that have been described as belonging to one of two possible symmetry classes. For the segments composed of rings, the twist between adjacent rings is quite variable, while the segments having a one-start helix are in multiple states of both twist and extension. This coexistence of two very different symmetries is similar to what has recently been reported for an archaeal Methanococcus maripaludis pili filament and an archaeal Sulfolobus shibatae flagellar filament.     

Liesegang-like rings in fine needle aspirates of renal/perirenal hemorrhagic cysts

Periodic structures with equally spaced radial striations, identified as Liesegang-like rings, were encountered in fine needle aspirates of two patients' hemorrhagic renal/perirenal cysts. The patients, one 60 and the other 39 years old, had acute right-flank pain; both underwent nephrectomy. The ring structures ranged in size from 8 microns to 200 microns in diameter and had regularly striated double walls. Histochemical and immunoperoxidase tests for iron, calcium, mucopolysaccharides, amyloid, keratin and hemoglobin performed on the tissue sections of the resected specimens gave negative results. With electron microscopy, the ring structures of one of the cases displayed a fine fibrillary composition. Since these Liesegang-like structures may be mistaken for parasites or necrotic tissue, pathologists should be aware of them. To our knowledge, this is the first report of Liesegang-like rings in the cytology literature.