Structures of bacterial flagellar motors from two FliF-FliG gene fusion mutants.

Flagella purified from Salmonella enterica serovar Typhimurium contain FliG, FliM, and FliN, cytoplasmic proteins that are important in torque generation and switching, and FliF, a transmembrane structural protein. The motor portion of the flagellum (the basal body complex) has a cytoplasmic C ring and a transmembrane M ring. Incubation of purified basal bodies at pH 4.5 removed FliM and FliN but not FliG or FliF. These basal bodies lacked C rings but had intact M rings, suggesting that FliM and FliN are part of the C ring but not a detectable part of the M ring. Incubation of basal bodies at pH 2.5 removed FliG, FliM, and FliN but not FliF. These basal bodies lacked the C ring, and the cytoplasmic face of the M ring was altered, suggesting that FliG makes up at least part of the cytoplasmic face of the M ring. Further insights into FliG were obtained from cells expressing a fusion protein of FliF and FliG. Flagella from these mutants still rotated but cells were not chemotactic. One mutant is a full-length fusion of FliF and FliG; the second mutant has a deletion lacking the last 56 residues of FliF and the first 94 residues of FliG. In the former, C rings appeared complete, but a portion of the M ring was shifted to higher radius. The C-ring-M-ring interaction appeared to be altered. In basal bodies with the fusion-deletion protein, the C ring was smaller in diameter, and one of its domains occupied space vacated by missing portions of FliF and FliG.

Evidence for cleft closure in actomyosin upon ADP release.

Structural insights into the interaction of smooth muscle myosin with actin have been provided by computer-based fitting of crystal structures into three-dimensional reconstructions obtained by electron cryomicroscopy, and by mapping of structural and dynamic changes in the actomyosin complex. The actomyosin structures determined in the presence and absence of MgADP differ significantly from each other, and from all crystallographic structures of unbound myosin. Coupled to a complex movement ( approximately 34 A) of the light chain binding domain upon MgADP release, we observed a approximately 9 degrees rotation of the myosin motor domain relative to the actin filament, and a closure of the cleft that divides the actin binding region of the myosin head. Cleft closure is achieved by a movement of the upper 50 kDa region, while parts of the lower 50 kDa region are stabilized through strong interactions with actin. This model supports a mechanism in which binding of MgATP at the active site opens the cleft and disrupts the interface, thereby releasing myosin from actin.

The bacterial flagellar cap as the rotary promoter of flagellin self-assembly.

The growth of the bacterial flagellar filament occurs at its distal end by self-assembly of flagellin transported from the cytoplasm through the narrow central channel. The cap at the growing end is essential for its growth, remaining stably attached while permitting the flagellin insertion. In order to understand the assembly mechanism, we used electron microscopy to study the structures of the cap-filament complex and isolated cap dimer. Five leg-like anchor domains of the pentameric cap flexibly adjusted their conformations to keep just one flagellin binding site open, indicating a cap rotation mechanism to promote the flagellin self-assembly. This represents one of the most dynamic movements in protein structures.

Correction of high-resolution data for curvature of the Ewald sphere.

At sufficiently high resolution, which depends on the wavelength of the electrons, the thickness of the sample exceeds the depth of field of the microscope. At this resolution, pairs of beams scattered at symmetric angles about the incident beam are no longer related by Friedel's law; that is, the Fourier coefficients that describe their amplitudes and phases are no longer complex conjugates of each other. Under these conditions, the Fourier coefficients extracted from the image are linear combinations of independent (as opposed to Friedel related) Fourier coefficients corresponding to the three-dimensional (3-D) structure. In order to regenerate the 3-D scattering density, the Fourier coefficients corresponding to the structure have to be recovered from the Fourier coefficients of each image. The requirement for different views of the structure in order to collect a full 3-D data set remains. Computer simulations are used to determine at what resolution, voltage and specimen thickness the extracted coefficients differ significantly from the Fourier coefficients needed for the 3-D structure. This paper presents the theory that describes this situation. It reminds us that the problem can be treated by considering the curvature of the Ewald sphere or equivalently by considering that different layers within the structure are imaged with different amounts of defocus. The paper presents several methods to extract the Fourier coefficients needed for a 3-D reconstruction. The simplest of the methods is to take images with different amounts of defocus. For helical structures, however, only one image is needed.

Rotational symmetry of the C ring and a mechanism for the flagellar rotary motor.

FliG, FliM, and FliN, key proteins for torque generation, are located in two rings. The first protein is in the M ring and the last two are in the C ring. The rotational symmetries of the C and M rings have been determined to be about 34 (this paper) and 26 (previous work), respectively. The mechanism proposed here depends on the symmetry mismatch between the rings: the C ring extends 34 levers, of which 26 can bind to the 26 equivalent sites on the M ring. The remaining 8 levers bind to proton-pore complexes (studs) to form 8 torque generators. Movement results from the swapping of stud-bound levers with M ring-bound levers. The model predicts that both the M and C rings rotate in the same direction but at different speeds.

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.

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.

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.

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.

Image analysis of helical objects: the Brandeis Helical Package.

Although the fundamental steps in Fourier-based image analysis of electron micrographs of helical structures have not changed significantly since the techniques were developed 30 years ago, there have been developments which aid both the analysis itself and the interpretation of results. Increases in computational resources have allowed the automation of many of the repetitive steps in image processing. We describe here a set of computer programs which have been developed at Brandeis University over the past 10 or more years. These programs, referred to as the Brandeis Helical Package, are designed to operate independently of each other with a simple and more uniform protocol for the flow of information between them. The programs are now easier to understand and to use and therefore represent a good tool for the analysis of helical structures.

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.

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.

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.

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.

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.