Three-dimensional structure of the regular surface layer (HPI layer) of Deinococcus radiodurans

The low-resolution structure of the regular surface layer of Deinococcus radiodurans has been determined from negatively stained specimens by three-dimensional electron microscopy. The layer has P6 symmetry, a lattice constant of 18 nm and a thickness of 6.5 nm. Three-dimensional reconstruction was performed by a hybrid real space/Fourier space approach that incorporates partial compensation of lattice distortions: The model obtained is discussed in the light of independent information about the surface structure of this layer, derived from metal shadowing and surface relief reconstruction. While agreement is quite satisfactory for the apparently more rigid inner surface, the outer surface shows severe flattening effects. The structure of the HPI layer is compared with other bacterial surface layers using a classification scheme that is outlined in the Appendix.     

Three-dimensional structure of the surface protein layer (MW layer) of Bacillus brevis 47

The three-dimensional (3D) structure of one surface protein layer from Bacillus brevis 47, the middle wall (MW) layer, has been reconstructed from tilted-view electron micrographs after correlation averaging to a resolution of 2 nm. The MW layer has p6 symmetry with a center-to-center spacing of 18.3 nm and a minimum thickness of 5.5 nm. The reconstruction reveals a distinct domain structure: the heavier domain of six monomers jointly forms a massive core centered at the sixfold symmetry axis, and lighter domains interconnect adjacent unit cells. In addition, the larger domains collectively form a pore by making contact with each other towards the inner surface, while the smaller domains establish a second connectivity towards the outer surface of the S layer. The MW layer of B. brevis resembles the S layer of Acetogenium kivui in various aspects: they have very similar lattice parameters and highly reminiscent 3D structures; the pores penetrate through the whole core and appear to determine the porosity of the S layers.     

Domain structure of the Acetogenium kivui surface layer revealed by electron crystallography and sequence analysis.

The three-dimensional structure of the Acetogenium kivui surface layer (S-layer) has been determined to a resolution of 1.7 nm by electron crystallographic techniques. Two independent reconstructions were made from layers negatively stained with uranyl acetate and Na-phosphotungstate. The S-layer has p6 symmetry with a center-to-center spacing of approximately 19 nm. Within the layer, six monomers combine to form a ring-shaped core surrounded by a fenestrated rim and six spokes that point towards the axis of threefold symmetry and provide lateral connectivity to other hexamers in the layer. The structure of the A. kivui S-layer protein is very similar to that of the Bacillus brevis middle wall protein, with which it shares an N-terminal domain of homology. This domain is found in several other extracellular proteins, including the S-layer proteins from Bacillus sphaericus and Thermus thermophilus, Omp alpha from Thermotoga maritima, an alkaline cellulase from Bacillus strain KSM-635, and xylanases from Clostridium thermocellum and Thermoanaerobacter saccharolyticum, and may serve to anchor these proteins to the peptidoglycan. To our knowledge, this is the first example of a domain conserved in several S-layer proteins.     

Three-dimensional reconstruction of innermost chorion layer of Drosophila grimshawi and Drosophila melanogaster eggshell mutant fs(1)384.

A low-resolution three-dimensional structure of the crystalline innermost chorionic layer (ICL) of the Hawaiian species Drosophila grimshawi and the Drosophila melanogaster eggshell mutant fs(1)384 has been calculated from electron microscope images of tilted negatively stained specimens. The isolated ICL of Drosophila grimshawi is a three-layer structure, about 36 nm thick, whereas the ICL of Drosophila melanogaster eggshell mutant fs(1)384 is a single layer, about 12 nm thick. Each unit in both crystalline structures includes octamers made up of four heterodimers. Crosslinks between the structural elements, both within and between unit cells form an interconnecting network, apparently important in maintaining the integrity of the layer. A model which may account for the ICL self-assembly formation in vivo and the ICL observed lattice polymorphism is proposed, combining data from the three-dimensional reconstruction work and secondary structure features of the ICL component proteins s36 and s38.     

Three-dimensional structure of the tetragonal surface layer of Sporosarcina ureae.

The three-dimensional structure of the regular surface layer of Sporosarcina ureae has been determined to a resolution of 1.7 nm by electron microscopy and image reconstruction. The S-layer has p4 symmetry, a lattice constant of 12.9 nm, and a minimum thickness of 6.6 nm. The reconstruction reveals a distinct domain structure: a massive core, arms connecting adjacent unit cells, and spurs which make contact at the subsidiary fourfold symmetry axes. In the z-direction the domains appear to be arranged in three planes, creating two entirely different surface reliefs. The S-layer has a complex pattern of pores and gaps that are 2 to 3 nm wide. In addition, the secondary-structure composition has been determined by infrared spectroscopy: about 35% of the polypeptide appears to have a beta-structure conformation.     

Structural and chemical characterization of the S layer of a Pseudomonas-like bacterium.

Sections and freeze-fractured preparations showed an S layer on the surface of Pseudomonas-like strain EU2. Polyacrylamide gel electrophoresis of cell envelopes extracted with 1% sodium dodecyl sulfate (SDS) at room temperature showed three proteins (45K, 55K, and 110K). The 55K protein was identified as the S-layer protein. Incubation in 1.5 M guanidine hydrochloride removed the S layer from cell envelopes and dissociated the structure into subunits. The soluble 55K protein reassembled into planar sheets upon removal of the guanidine hydrochloride by dialysis. Electron microscopy and image processing indicated that these sheets had p4 symmetry in projection with a lattice constant of 13.2 +/- 0.1 nm (corresponding to 9.3 nm between adjacent fourfold axes). In some instances these reassemblies appeared to form small three-dimensional crystals which gave particularly clear views of the structure in projection because of the superimposition of information from a number of layers. A model is proposed with molecules having rounded lobes connected by a narrower linker region and joining at the lobes to form the fourfold axes of the array. The pattern superficially resembles those of other bacterial S layers, such as those of Aeromonas salmonicida, Aeromonas hydrophila, and Azotobacter vinelandii. Extraction of cell envelopes with 1% SDS at 50 degrees C released the 110K protein from the envelopes and removed an amorphous backing layer from the S layer. The 45K protein displayed heat-modifiable migration in SDS-polyacrylamide gel electrophoresis and was insoluble in SDS at 50 degrees C or in high concentrations of guanidine hydrochloride, suggesting that it was associated with the peptidoglycan.     

The tetragonal surface layer of Clostridium aceticum: three-dimensional structure and comparison with the hexagonal layer of Clostridium thermohydrosulfuricum

The regular surface layer (S-layer) of Clostridium aceticum has been isolated and the three-dimensional structure determined to a resolution of 2.0 nm from tilt series of negatively stained preparations. It has tetragonal symmetry with a lattice constant of 12 nm and a thickness of 6 nm; there are probably 4 protein monomers per unit cell. A large proportion of the protein is concentrated in massive "cores" at the major four-fold axes which are situated towards the inner surface of the layer. From these cores, delicate arms extend towards the minor four-fold axes, where secondary connectivity is established near the exterior surface. When viewed from the outside, each of the cores appears to have a large central depression, rather than a true "pore". Since this general pattern of mass distribution is shared by the hexagonal S-layer of Clostridium thermohydrosulfuricum, some consideration has been given to the possible evolutionary steps leading to changes in symmetry. From modelling experiments, it is evident that the change from four-fold to six-fold symmetry in this instance could be accomplished simply by the loss of a structural "domain" from the protomer.     

The three-dimensional structures of S-layers of two novel Eubacterium species isolated from inflammatory human processes

The three-dimensional structures of the crystalline surface layers of two species of Eubacteria have been determined by electron microscopy and computerized image processing. The S-layer of Eubacterium sp. ES4C has tetragonal symmetry, with a unit cell spacing of 10.6 nm and a thickness of 9.5 nm, while that of Eubacterium sp. AHN 990 has hexagonal symmetry a = b = 15.7 nm and a thickness of 13 nm. The resolutions in the reconstructions were 2.5 nm and 1.8 nm, respectively. The reconstruction of the S-layer of strain ES4C reveals a distinct domain structure: a major tetramer, arms connecting adjacent unit cells, and a minor tetramer. The S-layer of strain AHN 990, on the other hand, has a rather complex arrangement, centred around the six-fold axis.     

Three-dimensional structure of an open form of the surface layer from the fish pathogen Aeromonas salmonicida.

Cell-free culture supernatants of a lipopolysaccharide (LPS) O-polysaccharide-deficient, single-insertion transposon mutant of the tetragonal surface protein array (S layer)-containing fish pathogen Aeromonas salmonicida were examined by electron microscopy. Negative staining showed that the S layer was released as sheets of tetragonal material, indicating that although surface retention of assembled S layer requires the presence of wild-type LPS oligosaccharides, initial assembly of S-layer subunits into sheets does not require the presence of O-polysaccharide chains. The three-dimensional structure of the S layer was reconstructed from tilted micrographs of the released sheets. Horizontal sections through this reconstruction showed that the released sheets were composed of two identical S layers that were perfectly in register. The reconstructed layer had a lattice constant of 12.5 nm. At a resolution of 1.6 nm, the layer consisted of a major tetragon at one fourfold axis of symmetry and a minor tetragon at the second fourfold axis of symmetry. The core, composed of four of the major domains, contained a large depression and was located toward the inside of the layer. The minor tetragon provided connectivity within the layer and was located toward the outer surface of the layer. Projections through the double layer gave a type I (closed) pattern (M. Stewart, T. J. Beveridge, and T. J. Trust, J. Bacteriol. 166:120-127, 1986), yet projections through the single layer indicated that the type II (open) pattern was present. This open pattern was indistinguishable from that seen in S layer released from the surfaces of wild-type cells.     

Structure of light-harvesting chlorophyll a/b protein complex from plant photosynthetic membranes at 7 A resolution in projection

The structure of thin three-dimensional crystals of the light-harvesting chlorophyll a/b protein complex, an integral membrane protein from the photosynthetic membrane of chloroplasts, has been determined at 7 A (1 A = 0.1 nm) resolution in projection. The structure analysis was carried out by image processing of low-dose electron micrographs, and electron diffraction of thin three-dimensional crystals preserved in tannin. The three-dimensional crystals appeared to be stacks of two-dimensional crystals having p321 symmetry. Results of the image analysis indicated that the crystals were disordered, due to random translational displacement of stacked layers. This was established by a translation search routine that used the low-resolution projection of a single layer as a reference. The reference map was derived from the symmetrized average of two images that showed features consistent with the projected structure of negatively stained two-dimensional crystals. The phase shift resulting from the displacement of each layer was corrected. Phase shifts were then refined by minimizing the phase residual, bringing all layers to the same phase origin. Refined phases from different images were in agreement and reliable to 7 A resolution. A projection map was generated from the averaged phases and electron diffraction amplitudes. The map showed that the complex was a trimer composed of three protein monomers related by 3-fold symmetry. The projected density within the protein monomer suggested membrane-spanning alpha-helices roughly perpendicular to the crystal plane. The density in the centre and on the periphery of the trimeric complex was lower than that of the protein, indicating that this region contained low-density matter, such as lipids and antenna chlorophylls.     

Helical structure of unidirectionally shadowed metal replicas of cyanide hydratase from Gloeocercospora sorghi

The helical filaments of the cyanide hydratase from Gloeocercospora sorghi have been reconstructed in three dimensions from freeze dried, unidirectionally shadowed specimens using iterative real-space helical reconstruction. The average power spectrum of all selected images has three clear reflections on different layer lines. The reconstruction is complicated by the fact that three possible indexing schemes are possible and reconstructions using the starting symmetries based on each of these indexing schemes converge on three-dimensional volumes which appear plausible. Because only one side is visible in shadowed specimens, it is necessary to examine the phases from a single filament by cryo-electron microscopy in order to make an unequivocal assignment of the symmetry. Because of the novel nature of the reconstruction method used here, conventional cryo-EM methods were also used to determine a second reconstruction, allowing us to make comparisons between the two. The filament is shown to have a left-handed one-start helix with D(1) symmetry, 5.46 dimers per turn and a pitch of 7.15nm. The reconstruction suggests the presence of an interaction across the groove not previously seen in nitrilase helical fibres.     

Structural analysis of viral nucleocapsids by subtraction of partial projections

The nucleocapsid of flavivirus particles does not have a recognizable capsid structure when using icosahedral averaging for cryo-electron microscopy structure determinations. The apparent absence of a definitive capsid structure could be due to a lack of synchronization of the symmetry elements of the external glycoprotein layer with those of the core or because the nucleocapsid does not have the same structure within each particle. A technique has been developed to determine the structure of the capsid, and possibly also of the genome, for icosahedral viruses, such as flaviviruses, using cryo-electron microscopy. The method is applicable not only to the analyses of viral cores, but also to the missing structure of multi-component complexes due to symmetry mismatches. The density contributed by external glycoprotein and membrane layers, derived from previously determined three-dimensional icosahedrally averaged reconstructions, was subtracted from the raw images of the virus particles. The resultant difference images were then used for a three-dimensional reconstruction. After appropriate test data sets were constructed and tested, the procedure was applied to examine the nucleocapsids of flaviviruses, which showed that there is no distinct protein density surrounding the genome. Furthermore, there was no evidence of any icosahedral symmetry within the nucleocapsid core.     

The cell envelope of the hyperthermophilic archaebacterium Pyrobaculum organotrophum consists of two regularly arrayed protein layers: three-dimensional structure of the outer layer

The cell envelope of the hyperthermophilic sulphur-reducing archaebacterium Pyrobaculum organotrophum H10 was found to be composed of two distinct hexagonally arranged crystalline protein arrays. Electron microscopic analysis of freeze-etched cells and isolated envelopes in conjunction with image processing showed that the inner layer (lattice centre-to-centre spacing 27.9 nm) is essentially identical to the protein array of Pyrobaculum islandicum GEO3, a complex, rigid structure implicated in the maintenance of cell shape. The outer layer has clear p6 symmetry and a lattice spacing of 20.6 nm. Its three-dimensional structure was reconstructed from a negative stain tilt series of an intact double-layered envelope using Fourier filtration to separate the desired information from the other lattices present. The outer layer is a unique, porous network of blocklike dimers disposed around six-fold axes, and exhibits minimal asymmetry between its inner and outer faces. It appears to be rather loosely associated with the outer surface of the inner layer. In most H10 envelopes, the inner layer is orientated with one base vector exactly perpendicular to the long axis of the cell, so that the cylindrical portion is composed of a series of parallel cell-girdling hoops of hexameric morphological units. All the other known Pyrobaculum strains were found to have a GEO3-type envelope structure, consisting of a single rigid protein array and a fibrous capsule. Although H10 does not possess a capsule, fibrils appear to be sandwiched between the two protein layers.     

Negatively stained 50 S ribosomal subunits of Escherichia coli

Ribosomes are large nucleoproteins of approximately 3 X 10(6) Mr. In contrast to helical or spherical nucleoproteins (viruses) of similar size (which consist of several hundred small asymmetric units reproduced by symmetry), ribosomes are completely asymmetric; therefore, the amount of structural information (defined by the number of independent image elements) necessarily increases from about 10 to 20 to about 1000 to 2000 (at resolutions of the order of 2 nm). With present techniques, only stained single particles can be studied in the electron microscope. Our published work on the 30 S subunit and on the 50 S subunit has demonstrated that three-dimensional reconstructions of stained single particles show a great number of structural details that are reproducible if the particles have the same orientation. One of the main results of this paper is the final proof of this reproducibility from detailed comparisons of individual 50 S subunits and of independent averages over a few (3 to 5) particles in the kidney or crown orientation; in the latter case, even after a chemical modification. The 50 S subunit is non-uniformly stained along the optical axis. It displays a complicated, stain-filled channel-like structure, within which is approximately the partial volume expected for the RNA. The particle shows an irregular but reproducible boundary surface against the stain. At several sites, the channel structure protrudes to the surface. Since the secondary structure of the RNA is well known, one might try to locate it in the subunit after chemical identification of its surface contacts (the 3' end of 23 S RNA and the 3' end of the 5 S RNA have been localized). Most interesting is a groove on the surface, which might accommodate the mRNA.     

A two-exposure technique for ice-embedded samples successfully reconstructs the chlorocruorin pigment of Sabella spallanzanii at 2. 1 Nm resolution.

A technique for reconstructing ice-embedded macromolecules from electron micrographs taken at two specimen tilts (+/-23 degrees ) has been used to determine the structure of chlorocruorin isolated from the Polychaete annelid Sabella spallanzanii. Images of individual molecules were extracted in couples from two micrographs of the same field of view so each couple consists of two projections of the same molecule. One couple was used as a fixed reference for alignment. Different references yielded reconstructions with different orientations. These were merged to give a model against which the orientation of 1624 first-exposure images was refined to give a final reconstruction at 2.1 nm resolution. The structure of this hematic pigment, essentially the same as that for Lumbricus terrestris, is a bilayer structure with overall symmetry D6, containing six hollow groups per layer. A hollow group is formed by six globular masses and has approximate threefold symmetry. Other structural elements connect the two layers and the hollow groups in a layer. This non-globin material occupies about 15% of the total molecular volume. The results show that the double-exposure strategy, previously described by some of the authors and tested in computer simulations, performs well in real experiments and could be used to obtain preliminary reconstructions in a semiautomatic way.     

The structure of Photosystem I from the thermophilic cyanobacterium Synechococcus sp. determined by electron microscopy of two-dimensional crystals.

The structure of the Photosystem I (PS I) complex from the thermophilic cyanobacterium Synechococcus sp. has been investigated by electron microscopy and image analysis of two-dimensional crystals. Crystals were obtained from isolated PS I by removal of detergents with Bio-Beads. After negative staining, either single layers or two superimposed layers with a rotational different orientation were observed. The layers have a rectangular unit cell of 16.0 x 15.0 nm, which contains two PS I monomers. The monomers are arranged alternating up and down in each layer. For double-layer crystals, the images of the two layers could be separately processed by a combination of Fourier-peak-filtering and correlation averaging. Features in the two-dimensional plane can be seen with a resolution up to 1.5-1.8 nm. A model for the PS I structure was obtained by combining three-dimensional reconstructions from three tilt-series. The model shows an asymmetric PS I complex. On one side (presumably the stromal side) there is a 3 nm high ridge. This is most likely comprised of the psaC, psaD and psaE subunits. The other side (presumably the lumenal side) is rather flat, but in the center there is a 3 nm deep indentation, which possibly separates partly the two large subunits psaA and psaB.     

Three-dimensional structure of the HSV1 nucleocapsid

The three-dimensional structures of full and empty capsids of HSV1 were determined by computer analysis of low dose cryo-electron images of ice embedded capsids. The full capsid structure is organized into outer, intermediate, and inner structural layers. The empty capsid structure has only one layer which is indistinguishable from the outer layer of the full capsids. This layer is arranged according to T = 16 icosahedral symmetry. The intermediate layer of full capsids appears to lie on a T = 4 icosahedral lattice. The genomic DNA is located inside the T = 4 shell and is the component of the innermost layer of the full capsids. The outer and intermediate layers interact in such a way that the channels along their icosahedral two-fold axis coincide and form a direct pathway between the DNA and the environment outside the capsid.     

The innermost chorionic layer of Drosophila. I. The role of chorin octamers in the formation of a family of interdigitating crystalline plates

The innermost chorionic layer (ICL) within egg shells of Drosophila melanogaster is composed of thin, abutting three-dimensional crystalline plates which form a closed, membrane-like sheath. Collectively, the crystals within the sheath appear to form a family of related three-dimensional crystals in space group C222; however, specimens prepared for electron microscopy are actually two-dimensional crystals in c222. The projected structures of the negatively stained crystals have been studied by minimal dose electron microscopy employing image reconstruction methods. Thin sections indicate that unit cells within the ICL are composed of paired layers; top and bottom layers are related by centrally located 2-fold axes, aligned parallel to the surface of the ICL. The most probable structural unit of the crystals is a tetramer of chorin dimers with a point group symmetry of 222, which is denoted a chorin octamer. Projection maps were computed from average transforms of two-dimensional crystals for delta (the primitive unit cell angle) equal to 84 degrees, 90 degrees and 97 degrees (+/- 1.5 degrees). The maps indicate that the molecular transitions responsible for the observed family of crystals involve concerted intramolecular rearrangements about molecular 2-fold axes. The significance in vivo of the family of crystals within the ICL is not known; however, structural considerations suggest that the observed polymorphism may reflect one facet of an intrinsic bonding flexibility of the ICL octamer that may play a role in the formation of interplate junctions and the assembly of a continuous closed sheath. The ICL may therefore serve as a structural bridge between the vitelline membrane-wax layer and the endochondrial floor, allowing the larva to shed the inner egg shell layers during hatching.     

Fine structure of the fertilization membranes of sea urchin embryos

The fine structure of the fertilization membranes from S. purpuratus embryos has been studied with the electron microscope. Isolated membranes before and after their full development and membranes formed under the influence of 10⁻³% cystine have been observed. The membrane structure was found to be trilamella: a middle layer about 200 Å thick, which originally was the vitelline membrane, and about 175 Å thick peripheral layers organized by the “crystalline material” from the cortical granules. These surface layers were again found to be trilaminated structure composed of a monolayer of parallel, closely packed flat fibrils, about 160 Å wide and 75 Å thick, adhering on both sides to parallel, 40–50 Å thick filaments separated from each other by about 100 Å and intersecting with the fibrils by an angle of about 75 °.