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D J DeRosier

Publications and source records attributed to D J DeRosier.

At least 19 recordsLinked to original sources

Non-helical perturbations of the flagellar filament: Salmonella typhimurium SJW117 at 9.6 A resolution.

Using a liquid-helium-cooled superconducting electron cryo-microscope, we obtained low-dose images of negatively stained preparations at 4 K and collected structural data to 1/9.6 -1 for flagellar filaments from the strain SJW117 of Salmonella typhimurium (serotype gt). The subunits of this left-handed, straight filament are non-helically perturbed in a pairwise manner. The perturbation corresponds to an alternating conformation in every other row of subunits. These are the 5-start rows and, necessarily, the resulting structure has a seam. The perturbation is not confined to the outside but extends into the structure. We separated the non-symmetric and symmetric parts of the structural data and generated a three-dimensional reconstruction from the latter. The resulting density map is a structure similar in domain organization to the left-handed filament of S. typhimurium SJW1660. Filtered images generated from the non-symmetric component show an ordered and polar structure. The nature of the perturbation was analyzed by model building using a sphere to represent the subunit at low resolution. A lateral shift of approximately 10 degrees mimics the perturbation.

Flagella

Reconstruction of symmetry deviations: a procedure to analyze partially decorated F-actin and other incomplete structures.

The absolute value of individual differences (AVID) procedure is a method to map variations within images arising from deviations in symmetry. We devised this procedure to analyze images of actin filaments decorated with actin-binding proteins (ABPs). In three-dimensional maps of such actin complexes, ABPs often appear weak (i.e. they have low density) relative to actin. Because the 3D map represents an average taken over equivalent positions in the helix, the final density at the position of the ABP represents an average of the densities at all ABP sites. If there is either incomplete binding or a conformational variability of the bound ABP, the average density will be lowered. By the same argument, the variation of density at these sites will be increased. The aim of the AVID procedure is to calculate the density variations within partially decorated filaments and thereby attempt to locate the bound protein. We tested the AVID procedure with model data and then applied it to electron micrographs of F-actin decorated with an actin-binding domain of fimbrin known as N375 [Hanein et al., J. Cell Biol. 139 (1997) 387-396]. The AVID maps have peaks at the site where N375 binds. Because it excludes the layer line data, the AVID procedure uses data that are independent of the data used for 3D reconstruction and difference mapping. It therefore provides an independent way to localize the bound subunit without the need for a map of undecorated actin. Moreover, the difficulties of scaling maps are minimized. This procedure could also be applied to structures with non-helical symmetry.

Actins

Evidence for a conformational change in actin induced by fimbrin (N375) binding.

Fimbrin belongs to a superfamily of actin cross-linking proteins that share a conserved 27-kD actin-binding domain. This domain contains a tandem duplication of a sequence that is homologous to calponin. Calponin homology (CH) domains not only cross-link actin filaments into bundles and networks, but they also bind intermediate filaments and some signal transduction proteins to the actin cytoskeleton. This fundamental role of CH domains as a widely used actin-binding domain underlines the necessity to understand their structural interaction with actin. Using electron cryomicroscopy, we have determined the three-dimensional structure of F-actin and F-actin decorated with the NH2-terminal CH domains of fimbrin (N375). In a difference map between actin filaments and N375-decorated actin, one end of N375 is bound to a concave surface formed between actin subdomains 1 and 2 on two neighboring actin monomers. In addition, a fit of the atomic model for the actin filament to the maps reveals the actin residues that line, the binding surface. The binding of N375 changes actin, which we interpret as a movement of subdomain 1 away from the bound N375. This change in actin structure may affect its affinity for other actin-binding proteins and may be part of the regulation of the cytoskeleton itself. Difference maps between actin and actin decorated with other proteins provides a way to look for novel structural changes in actin.

Actins

Analysis of a FliM-FliN flagellar switch fusion mutant of Salmonella typhimurium.

In the course of an analysis of the three genes encoding the flagellar motor switch, we isolated a paralyzed mutant whose defect proved to be a 4-bp deletion of the ribosome binding sequence of the fliN switch gene (V. M. Irikura, M. Kihara, S. Yamaguchi, H. Sockett, and R. M. Macnab, J. Bacteriol. 175:802-810,1993). This sequence lies just before the 3' end of the coding sequence of the upstream fliM switch gene, in the same operon. This mutant readily gave rise to pseudorevertants which, though much less motile than the wild type, did exhibit significant swarming. One such pseudorevertant was found to contain a compensating frameshift such that the fliM and fliN genes were placed in frame, coding for an essentially complete FliM-FliN protein fusion. Minicell analysis demonstrated that, as expected, the parental mutant synthesized an essentially full-length FliM protein but no detectable FliN. The pseudorevertant, in contrast, synthesized a protein with the predicted size for the FliM-FliN fusion protein and no detectable FliM or FliN. Immunoblotting of minicells with antibodies against FliM and FliN confirmed the identities of these various proteins. Immunoblotting of book-basal-body complexes from the wild-type strain gave a strong signal for the three switch proteins FliG, FliM, and FliN. Complexes from the FliM-FliN fusion mutant gave a strong signal for FliG but no signal for either FIiM or FliN; a moderately strong signal for the FliM-FliN fusion protein was seen with the anti-FliM antibody, and a weaker signal was seen with the anti-FliN antibody. The cytoplasmic C ring of the structure, which is seen consistently in electron microscopy of wild-type complexes and which is known to contain the FliM and FliN proteins, was much more labile in the FliM-FliN fusion mutant, giving a fragmented and variable appearance or being completely absent. Complementation data indicated that wild-type FliM had a mild dominant negative effect over the fusion protein, that wild-type FliN and the fusion protein work much better than the fusion protein alone, and that wild-type FliM and FliN together have no major positive or negative effect on the function of the fusion protein. We interpret these data to mean that the FliM-FliN fusion protein incorporates into structure but less stably than do the FliM and FliN proteins separately, that wild-type FliM tends to displace the fusion protein, and that wild-type FliN can supplement the FliN domain of the fusion protein without displacing the FliM domain. The data support, but do not prove, a model in which FliM and FliN in the wild-type switch complex are stationary with respect to each other.

Amino Acid Sequence

Structure of bacterial flagellar filaments at 11 A resolution: packing of the alpha-helices.

Recent advances in the analysis of electron micrographs of frozen, hydrated bacterial filaments have allowed us to average data from more than 150 images and to reconstruct the bacterial flagellar filament of Salmonella typhimurium at a resolution of approximately 11 A. In addition to the outermost features seen in earlier lower resolution maps of the filament, we find a pair of concentric tubes which surround a approximately A diameter channel at the center of the structure. The walls of these tubes are composed of rod-like features which we have interpreted as columns of individual alpha-helices stacked end-to-end. Each column runs approximately parallel to the helix axis. The wall of the innermost tube, at a radius of approximately 20 A, is formed from 11 such columns. The wall of the second tube is formed from 22 columns which occur alternately at radii of approximately 43 and approximately 47 A. The two concentric tubes are held apart by spacers. These are short, rod-like features, which run approximately parallel to the helix axis. We have interpreted these as additional alpha-helices. By symmetry, each flagellin monomer contributes an alpha-helix to the inner tube, two alpha-helices to the outer tube and a fourth alpha-helix to the spacer. We have tentatively assigned one type of alpha-helix in the outer tube to the approximately 30 C-terminal residues of flagellin while the remaining three alpha-helices are assigned to the approximately 70 N-terminal residues. This interpretation of the reconstruction is consistent with available biochemical, biophysical and amino acid sequence information. We also present details of improved methodology to extract and evaluate the original data and also to assess the statistical significance of features in the three-dimensional map.

Bacterial Proteins

Spinning tails.

The torque-generating, direction-reversing switch proteins of the bacterial flagellar rotary motor form a cytoplasmic extension of the bacterial flagellar basal body. 10 A maps, obtained by electron cryomicroscopy, of the bacterial filament reveal an unusual alpha domain which forms the protein-subunit export channel. The details of subunit export, assembly, and assembly-monitoring machinery are becoming clearer.

Bacterial Proteins

Isolation, characterization and structure of bacterial flagellar motors containing the switch complex.

A putative complex of the three switch proteins, FliG, FliM and FliN appears to be directly involved in torque generation and control of direction of rotation. We have developed a preparative procedure for flagellar motors that retains these proteins as evidenced by Western blots using anti-FliG, anti-FliM and anti-FliN antibodies. Immunogold labeling with these three antibodies shows that the three switch proteins are localized to the motor. Electron micrographs of frozen-hydrated preparations reveal a large, new component we have termed the "C ring complex" attached to the cytoplasmic face of the M ring. In a three-dimensional reconstruction of the cylindrically averaged structure, the M-S ring complex appears thicker and wider by the addition of extra material to the cytoplasmic surface of the M ring. In addition, extending into the cytoplasm from the thickened M ring is the C ring complex, a thin-walled cylinder having a length of 170 A and an outer diameter of 450 A compared to the 290 A diameter of the M ring. We provide evidence that the thickened M ring contains FliG and that the C ring complex may contain FliM and FliN. The large diameter of the C ring complex may permit interaction with the M ring and with the circlet of studs thought to be the MotA/MotB complex.

Bacterial Proteins

Electron diffraction of helical particles.

The development of low-dose electron cryo-microscopy has provided the means to see structural details to better than 10 A resolution in helical structures. The application of techniques of image analysis to micrographs can yield accurate phases, but not amplitudes with which to generate three-dimensional maps of the structure. Electron diffraction can provide reliable amplitudes, which can be combined with the phases from the images. In order to collect amplitude data, two problems have to be overcome: the pattern should be obtained from a large well ordered sample of particles, and the inelastic background should be properly subtracted. In this paper, we present three simple methods to produce rafts of helical particles. Using these methods we have obtained electron diffraction patterns from TMV (with data out to 0.28 nm), TMV protein stacked disks (with data out to 0.3 nm) and bacterial flagellar filaments (with data out to 0.5 nm). In addition, we describe the algorithms used to extract the amplitudes from the diffraction patterns.

Algorithms

Domain organization of the subunit of the Salmonella typhimurium flagellar hook.

The deduced amino acid sequences of the family of axial proteins of the bacterial flagellum possess N and C-terminal heptad repeats of hydrophobic amino acid residues, which suggests that these proteins all fold to form bundles of alpha-helices (e.g. coiled coils). There is evidence that flagellin, which is one of the axial proteins, has an axially oriented bundle of alpha-helices that gives rise to the inner, rod-shaped domains seen in electron density maps. We present evidence that a second member of the family, the hook subunit, also has such an axially oriented, rod-shaped domain. In three-dimensional reconstructions from electron micrographs of the helical hook of Salmonella typhimurium, the rod-shaped domain has a diameter of 18 A, which is that expected for a coiled coil. The corresponding domain in the flagellin subunit of the filament, however, is larger, having a diameter of 24 A suggesting a bundle of three or more alpha-helices. In addition to the rod-shaped domain, the hook has two other domains. At a radius of 55 A is the middle spheroidal domain about 25 A in diameter and at a radius of 75 A is the outer ellipsoidal domain about 20 A by 30 A by 40 A. The flagellin subunit also has a middle and an outer domain although they appear different from those of the hook. This is no doubt a result of the lack of any sequence similarity of the hook and flagellin subunits, apart from the N and C-terminal heptad repeats. Along the hook axis, there is a 25 A wide channel, which presumably serves in the export of hook and flagellin subunits in the assembly of the filament. There is a comparably sized channel in the filaments as deduced from electron micrographs. Thus, electron microscopy consistently finds a small channel, whereas in X-ray diffraction studies of the filament, the channel size appeared to be about 60 A. At a diameter of 60 A, the channel could pass the flagellin or hook subunit in its completely folded state, but if the channel is only 25 A in diameter, the subunit would have to be at least partially unfolded in order to pass through the channel.

Flagella

Size of the export channel in the flagellar filament of Salmonella typhimurium.

The size of the putative export channel in the bacterial flagellar filament appears small (25 A) in studies done by electron microscopy but large (60 A) in studies done by X-ray diffraction. We have undertaken additional studies by electron microscopy to examine some of the possible causes of the difference. A comparison of three-dimensional image reconstructions of native and reconstituted filaments rules out the presence or absence of flagellin monomers in the export channel as the source of the variation in apparent channel size. The channel seen in reconstructions from both kinds of filaments is 25 A in diameter. The difference in the previous studies is more probably a result of artifacts introduced in either the X-ray or the electron microscopical methodology. Comparisons of three-dimensional reconstructions from images of filaments embedded in various stains (anionic, cationic and neutral) and in ice, taken at a range of defocuses, rule out the two most likely sources of artifact in electron microscopy (i.e., staining artifacts and defocus phase contrast). Based on these studies we suggest that the channel seen in the image reconstructions is free of exported flagellin monomers, that its true diameter is about 25 A, and, therefore, that the flagellin monomer must be unfolded to pass along it.

Flagella

Conformational switching in the flagellar filament of Salmonella typhimurium.

The flagellar filament of the mutant Salmonella typhimurium strain SJW814 is straight, and has a right-handed twist like the filament of SJW1655. Three-dimensional reconstructions from electron micrographs of ice-embedded filaments reveal a flagellin subunit that has the same domain organization as that of SJW1655. Both show slight changes from the domain organization of the subunits from SJW1660, which possesses a straight, left-handed filament. This points to the possible role of changes in subunit conformation in the left-to-right-handed structural transition in filaments. Comparison of the left and right-handed filaments shows that the subunit's orientation and intersubunit bonding appear to change. The orientation of the subunit in the SJW814 filament is intermediate between that of SJW1655 and SJW1660. Its intermediate orientation may explain why the filaments of SJW1655 and SJW1660 are locked in one conformation, whereas the filament of SJW814 can be induced to switch by, for example, changes in pH and ionic strength.

Computer Graphics

Localization of the Salmonella typhimurium flagellar switch protein FliG to the cytoplasmic M-ring face of the basal body.

The direction of rotation of the bacterial flagellum is determined by the flagellar switch. We have localized FliG, one of the switch proteins of Salmonella typhimurium, to the cytoplasmic face of the M ring of the flagellar basal body. This localization was made possible by the discovery of two spontaneous mutants in which the fliF (M ring) and fliG (switch) genes were fused in-frame. In the first mutant, a deletion of 7 base pairs at the 3' end of fliF resulted in an essentially full-length fusion protein. In the second mutant, a larger deletion resulted in a fusion in which 56 amino acids from the carboxyl terminus of FliF and 94 amino acids from the amino terminus of FliG were lost. Both strains were motile and underwent switching; the first strain had a clockwise bias, and the second strain had a counterclockwise bias. Gel electrophoresis and immunoblotting of isolated hook-basal-body complexes verified that they contained the fusion proteins. Electron microscopy revealed additional mass at the cytoplasmic face of the M ring, which could be decorated with anti-FliG antibody. We conclude that the natural location for FliG is at the cytoplasmic face of the M ring and that the stoichiometric ratio between FliF and FliG in wild-type cells is probably 1:1.

Amino Acid Sequence

Mass determination and estimation of subunit stoichiometry of the bacterial hook-basal body flagellar complex of Salmonella typhimurium by scanning transmission electron microscopy.

The basal body, a part of the rotary motor of the bacterial flagellum, is a multiprotein assembly that consists of four rings (denoted M, S, P, and L) and an axial rod (denoted R). From analysis of scanning transmission electron microscopy images of hook-basal body preparations isolated from Salmonella typhimurium, we have determined the masses of the basal body and three of its subcomplexes. The mass of the basal body (i.e., the four rings and rod) is 4400 +/- 490 kDa (mean +/- SD; n = 54). The mass of the LPR subcomplex (i.e., L and P rings and the whole rod) is 2600 +/- 380 kDa (n = 55), that of the L and P rings and the distal part of the rod is 2100 +/- 320 kDa (n = 25), and the mass of the L and P ring subcomplex is 1700 +/- 260 kDa (n = 514). These results, together with the masses of the component proteins, indicate that the rings contain approximately 26 subunits each and that the mass of the rod is consistent with a composition of approximately 6 copies each of three of the rod proteins FlgB, FlgC, and FlgF and approximately 26 copies of FlgG as determined by Jones et al. [Jones, C. J., Macnab, R. M., Okino, H. & Aizawa, S.-I. (1990) J. Mol. Biol. 212, 377-387] using quantitative gel electrophoresis. The results of Jones et al., together with ours, account for all proteins in the basal body to within approximately 5% (or 200 kDa).

Bacterial Proteins

Substructure of the flagellar basal body of Salmonella typhimurium.

The Salmonella typhimurium basal body, a part of the flagellar rotary motor, consists of four rings (denoted M, S, P and L) and a coaxial rod. Using low-dose electron microscopy and image averaging methods on negatively stained and frozen-hydrated preparations, we examined whole basal body complexes and subcomplexes obtained by dissociation in acid. Dissociation occurs in steps, allowing us to obtain images of substructures lacking the M ring, lacking the M and S rings, and lacking the M and S rings and the proximal portion of the rod. We obtained images of the L and P ring subcomplex. The existence of a subcomplex missing only the M ring suggests either that the S and M rings derive from two different proteins, or that the M ring is a labile domain of a single protein, which makes up both rings. At the 25 to 30 A resolution of our averaged images, the L, P and S rings appear cylindrically symmetric. Images of the M ring show variability that may be due to differences in angular orientation of the grid, but equally could be due to structural variations. Three-dimensional reconstructions of these structures from the averaged images reveal the internal structure and spatial organization of these components.

Flagella