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Journal of Bacteriology, September 2002, p. 4868-4874, Vol. 184, No. 17
0021-9193/02/$04.00+0 DOI: 10.1128/JB.184.17.4868-4874.2002
Copyright © 2002, American Society for Microbiology. All Rights Reserved.
Department of Physiology & Biophysics, Boston University School of Medicine, Boston, Massachusetts 02118-2526,1 Department of Biochemistry & Molecular Genetics, University of Virginia, Charlottesville, Virginia 22908-07332
Received 15 March 2002/ Accepted 21 May 2002
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H. influenzae type b pili have structural and gene sequence similarities (4, 11, 13, 17) to pili described as class I (18) but not to those in the type IV pilus superfamily. In particular, strong sequence similarity is found between Hib pilins and pilins that comprise P-pili (13, 17). P-pili are expressed on the surface of uropathogenic Escherichia coli that cause pyelonephritis, urinary tract infections that involve the kidneys. Conversely, there is no significant sequence similarity between H. influenzae pilins and the type IV pilins involved in both twitching motility and bacterial adhesion, nor is there morphological similarity between the atomic structures of known pilins from E. coli (3, 23) and the type IV pilins from Neisseria gonorrhea (21) or Pseudomonas aeruginosa (14).
The structures of the adhesin subunits of type 1 pili and P-pili and a minor pilin of P-pili have been determined in complex with their periplasmic chaperone proteins: X-ray crystallography has been used to investigate the structures of FimH/FimC (3), PapG/PapD (6), and PapK/PapD (23). These pilins all contain subunits with an immunoglobulin-like fold and a donor strand complementation mechanism in which a beta strand donated from the chaperone fills the groove in the pilin subunit. In the modeled pilus filaments, it is a beta strand from the subsequent pilin monomer that inserts into the subunit groove (3, 23). Each of these pilins has sequence similarity with their respective major structural pilins (FimH with FimA, PapK with PapA) as well as similarity to HifA, the major structural pilin of the Hib pilus. The sequence similarities between HifA and PapK, in combination with morphological similarities of the helical filaments that comprise the pili, provide evidence for donor strand complementation of HifA, as seen in type 1 and P-pili (17). Structural information on the similarities and differences between assembled pili can be used to investigate the range of structural polymorphism that can be accommodated by this mechanism.
Immunologic cross-reactivity and sequence analysis are aiding our understanding of assembled pilus structures. Studies on the hydrophilicity of HifA were used to define three regions that were expected to be surface exposed and that might therefore constitute antigenic epitopes (8). Subsequently, it was shown that antibodies to 14- to 15-residue peptides of these regions do not react with assembled pili (10). Even strains of H. influenzae with 99% identity can be immunologically distinct, and researchers have constructed chimeras to enhance reactivity to conformational epitopes, thereby defining noncontiguous residues that are structurally associated (20). Studies such as these, in combination with sequence analyses that define variable regions of pilin subunits (4, 17), provide data for fitting known structures from homologous pilins into new structural data.
We present results from our studies of the structure of Hib pili with sequence analysis of the major structural pilin, HifA, and electron microscopy and image processing of the structure of Hib pili assembled into a helical filament. A comparison of the Hib pilus structure to that of P-pili elucidates significant structural differences within class I pili, a superfamily defined (18) by sequence similarity of the major structural pilins. Subunits in Hib pili appear to be oriented almost vertically along the filament axis, while subunits are oriented approximately horizontally in models of P-pili (23) and type 1 pili (3). Our data provide a basis for understanding bacterial strategies that facilitate survival of H. influenzae type b bacteria in the nasopharynx, preceding invasion of the human host and systemic disease.
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Sample preparation. Hib pili from H. influenzae strain Eagan were a generous gift from Joseph St. Geme III (Washington University School of Medicine, St. Louis, Mo.), purified as described previously (25). Briefly, H. influenzae was grown overnight in supplemented brain heart infusion broth at 37°C and then centrifuged to pellet the bacteria. Pili were sheared from the cell surface with a blender, and the bacterial cells were removed by centrifugation. Pili were purified by cycles of precipitation in ammonium sulfate and resuspension in 0.5 M Tris, pH 7. Final resuspension was in 50 mM Tris, pH 7.
Grids for transmission electron microscopy were made by adsorption of the sample onto carbon-coated grids for 3 min, washed with 8 drops of 50 mM Tris (pH 7), and stained with 1% uranyl acetate for 15 s. Samples were imaged with a Philips CM12 transmission electron microscope operated at 120 kV with a LaB6 filament. Images were recorded under minimal electron dose conditions at a magnification of x60,000 and digitized at 3.5 Å/pixel.
Image processing. Three-dimensional reconstructions of Hib pili were computed with single-particle data analysis (9) and the iterative helical real space reconstruction (IHRSR) method (7). After each cycle, the helical symmetry of the average structure was calculated and imposed, providing an improved reference particle for each subsequent iteration (7).
Specifically, overlapping lengths of Hib pili were masked from images of negatively stained sample for a total of approximately 165,000 subunits. The single-particle analysis program package SPIDER (9) was used to align each filament fragment to a reference particle, both rotationally and translationally. An initial reference particle comprising the P-pilus helical reconstruction (2) with 3.28 subunits per turn was not an appropriate starting model, as the iterative procedure did not converge to a stable solution for the Hib pilus structure.
Computed Fourier transforms of the best H. influenzae type b filament images were indexed, and found to have threefold symmetry (3.0 subunits per turn), with an approximately 300 Å repeat (data not shown). Therefore, a three-stranded rope model was constructed, and projections of this model perpendicular to the helical axis, computed every 5 degrees, were used as the initial references. Each particle was fit to the references with cross-correlation, and back projections were computed to produce an average structure. The helical symmetry of the result was computed and imposed, providing improved reference particles for each subsequent cycle of refinement. After 50 cycles, the structure had converged to a stable solution. Three back projection algorithms (SPIDER command bp3f or bp32, bprp, and the radon back projection algorithm written and generously provided by Michael Radermacher) were tested to ensure that the resultant reconstruction was reliable.
In the final reconstruction, approximately 145,000 subunits were retained. The resolution of the reconstruction is at least 19 Å, as calculated by splitting the data set in half and using a Fourier shell coefficient of 0.5 to determine self-similarity. If the less stringent criterion of the crossing point of the noise curve (noise factor 3) and the Fourier shell coefficient curve was used, the resolution would be estimated to be 12 Å. As a check for the validity of imposing threefold symmetry, data were analyzed with the P1 space group (no imposed symmetry), resulting in a reconstruction that again showed strong threefold symmetry (data not shown).
Images shown are of the resultant reconstructions computed with the SPIDER weighted back projection algorithm bp32f (9). Surface views in Fig. 4 were calculated with WEB (9). Electron density maps of the model H. influenzae type b filament were computed with Gaussian-weighted mass distributions from atomic coordinates of the minor P-pilin PapK (PDB 1PDK, chain B) (23). Isocontour surfaces of the reconstruction and of the model filament were computed with SITUS (28). Surface views in Fig. 6 are displayed with the visual molecular dynamics program (VMD) (15).
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FIG. 4. Results of three-dimensional reconstruction of Hib pili. (A) In projection, the central channel around the helical axis has a zigzag appearance along part of its length (arrow) and regions in which the central channel is indistinct (arrowhead), as is observed in electron micrographs of negatively stained Hib pili (see Fig. 2). (B) Cross section views show the threefold symmetry about the helical axis and a central channel straight up the filament axis. Cross-sections shown are spaced 2.7 Å apart. (C) Surface of the three-dimensional reconstruction of Hib pili. (D) For comparison, the surface of the three-dimensional reconstruction of P-pili; see also reference 2. Bar: 50 Å (A and B), 25 Å (C and D).
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FIG. 6. Three-dimensional reconstruction and model of Hib pilus. (A) Three-dimensional reconstruction computed from electron microscope data of H. influenzae type b pilus. Note the strong connections running along the left-handed three-start helix. The filament is 7 nm in diameter, with scalloped edges. (B) One model of the Hib pilus constructed from subunits of the homologous minor P-pilin PapK. The PapK structure was taken from PDB file 1PDK B (23) and placed on the Hib pilus helix. (C) An enlarged view of the three-dimensional reconstruction from the boxed region in A, with a cartoon of the PapK monomer included to illustrate the proposed position of the extra density of HifA compared to PapK. In our model, the extra 20% mass of HifA is seen as the surface-exposed region that extends furthest from the helical axis (arrow in C), corresponding to regions of highly variable amino acid sequence of the HifA subunit.
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The Hib pilus major subunit, HifA, is 20% larger than PapA, the major structural pilin in P-pili expressed on the surface of pyelonephritis-causing E. coli. Thus, alignment of the 196-amino-acid HifA sequence to the 163-amino-acid PapA sequence necessarily includes at least 33 amino acids in HifA with no corresponding amino acid in PapA. These amino acid "insertions" may be distributed randomly or may appear as a loop(s).
Automated sequence alignment of HifA/Eagan and HifA/M43p+ to PapA/J96 with ALIGN (22) predicted significantly different locations for the insertions of HifA amino acids with respect to PapA for each strain of H. influenzae despite the 82% identity and 95% homology between the two HifA sequences. As structural variations of this magnitude are extremely unlikely to occur in vivo from such highly homologous monomers, a manual alignment of the PapA sequence was completed to reconcile the preliminary sequence alignments. In addition, the new alignment was required to account for data available from published alignments of HifA/M43p+ with PapA/F7-2 (13) and of HifA/Eagan with PapK, a minor P pilin with 28% sequence identity and 55% similarity to PapA (17).
First, a shift of the PapA sequence HYTAVVKKSSAVG resulted in the correspondence of a HifA insert with the longest highly variable region in the HifA sequence. This shift reduced the sequence alignments from 23% identical and 61% similar to 22% identical and 57% similar, excluding the HifA inserts. Data from previous alignments of the major structural pilins of class I pili were used to indicate regions of conservation and of variability for predicted secondary structures in HifA (4, 13) and PapA (26). These data were also used as guidelines in our realignment of the HifA/Eagan and PapA/J96 pilin sequences (Fig. 1). Further minor modifications were made to the automated alignment to ensure that the sequence alignment was in best agreement with both the alignment of HifA/Eagan to PapK (17) and the alignment of HifA/M43p+ to PapA/P02972 (13).
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FIG. 1. Alignment of HifA and PapA after accounting for data from previous studies (10, 12, 13, 17, 20, 22, 26). HifA from two strains of H. influenzae, Eagan and M43p+, have 82% identity and 95% similarity or 76% identity and 91% similarity, excluding and including, respectively, the highly variable regions of HifA. HifA/Eagan (from H. influenzae) and PapA/J96 (from E. coli) have 21% identity and 58% similarity or 17% identity and 48% similarity, excluding and including, respectively, the amino acid insertions of HifA with respect to PapA. The alignment of HifA/Eagan and PapK/J96 of Krasan et al. (17) is included.
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Morphology of Hib pili. To determine the structure of Hib pili, purified pili were negatively stained and imaged by minimal-electron-dose transmission electron microscopy (Fig. 2). Hib pili did not demonstrate the extended stretches of extremely straight pilus seen in P-pili, but short stretches of reasonably straight segments were found (black arrow, Fig. 2A). The IHSRS method (7) only requires filaments to be approximately straight for the chosen box length, in this case 250 Å, rather than the greater than 1,500-Å-long filament segments required for a sufficient signal-to-noise ratio to use spline fitting and traditional helical reconstruction methods (5) on such a thin filament (70 Å diameter). Damaged pili were seen with apparent shear along their length (black arrowhead in Fig. 2B), and Hib pili did not exhibit the extensive unwinding of the helical filament seen in P-pili (1, 2).
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FIG. 2. Images of isolated, negatively stained H. influenzae type b pili. These pili are straight for short distances along the filament (black arrow in A). When damaged, Hib pili do not unwind into thin fibrillar structures but appear to be sheared perpendicular to the filament axis (black arrowhead in B). Along the length of the filament, there are regions in which a low-density channel is barely visible (white arrowhead) and regions in which the channel appears as a zigzag along the filament axis (white arrow). Bars: 100 Å (A and B), 50 Å (inset).
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FIG. 3. Images of Hib pili treated as single particles. (A) Filaments were selected and boxed as overlapping segments; shown are 36 of the 5,000 selected areas that were used in the data analysis. (B) The same 36 images after in-plane rotation and translational alignment to a reference particle. Bar, 100 Å.
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A central channel of approximately 20 Å in diameter is visible in the Hib reconstruction, straight up the filament axis. The straight channel was unexpected, as images of Hib pili often show low density with a zigzag appearance in the center of the filament (white arrow, Fig. 2A inset), as well as regions where the central low density is much less pronounced (white arrowhead, Fig. 2A inset). This variation in appearance along the filament length is due to the nature of transmission electron microscopy; images are a projection through the sample, with all planes of the object in focus; they are not a surface view. When such a projection image is calculated from the H. influenzae type b reconstruction, the zigzag and diffuse appearances of the central channel are both clearly apparent (white arrow and white arrowhead, respectively, in Fig. 4A). Similarly, our current results show that while only two strands are discernible at any time in a projection image (Fig. 4A), the filament comprises a three-start helix with threefold symmetry (Fig. 4B and 6). Connectivity of density in Hib pili is strongest along this three-start (Fig. 4C and 6). The outer edge of the filament has a scalloped appearance (Fig. 4C and 6). Thus, the measured diameter varies from 60 to 70 Å as the projected density narrows and widens along the length of the filament.
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242 Å. It was reported previously (25), based upon fast-freeze/deep-etch electron microscopy, that the Hib pilus contained a left-handed one-start and a right-handed two-start helix, with a crossover distance of 260 Å. How can these observations be reconciled with our current description of the Hib pilus structure? Shadowed samples provide a view of a surface-coated structure, whereas negatively stained samples provide a projection image through the protein density. The apparent one-start helix seen in shadowed images may be a visualization of the ring of density formed by filling the groove between each set of three subunits that comprise a unit cell. Three-dimensional reconstruction provides information about the protein density through the interior of a macromolecular assembly. Thus, at our current resolution of better than 20 Å, additional details are now available for a more complete understanding of the Hib pilus structure.
H. influenzae type b pili and P-pili are fundamentally similar; they are helical adhesive filaments extending from the outer cell membrane of pathogenic gram-negative bacteria. In both H. influenzae and E. coli, structural pilins are transported across the periplasm by chaperone proteins and exit via a homo-oligomeric usher protein that sits at the outer membrane. The pili each have lengths on the order of 1 µm and diameters of
70 Å (Fig. 4C and D). In addition, the major structural pilin for each pilus, HifA for Hib pili and PapA for P-pili, is expected to be structurally similar, and there is evidence for donor strand complementation based on morphological similarities of the pili and on sequence alignment between HifA and PapK, a minor structural P-pilin (17).
As seen in structures of filamentous phages, similar monomers assembled into filaments with different symmetry can produce dramatic alterations in functional properties. For example, a difference in the packing of the capsid proteins from Pf1 (19) versus Pf3 (27) produces phage that differ by a factor of 2.4 in their DNA-to-protein ratios. Despite their overall similarity in length and width, Hib pili and P-pili also have significant morphological differences. For example, Hib pili are not straight for extended stretches as are P-pili, necessitating the use of new image analysis methods (7). In addition, the amino acid sequence insertions in the HifA subunit compared with the PapA subunit must alter the resultant helical filament. That is, one cannot add mass to an object without changing it. By analogy, if a building supplier delivers bricks that are 20% larger than those sent previously, a house built with the new bricks cannot be structurally identical to one constructed with the older (smaller) bricks (Fig. 5).
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FIG. 5. Possible ways for a helix to accommodate a 20% increase in mass. (A) Initial rectangular "subunit," oriented approximately horizontally, with radius r and rise per subunit z. The helix is viewed after slicing it down the back and laying it flat on the page. (B) The subunit could increase in thickness, thereby increasing the filament radius, r. (C) The subunit could increase in height, increasing the rise per subunit, z. (D) As appears to occur in Hib pili compared with P-pili, the subunits could tip up, making space for the additional mass without increasing z or r; the number of subunits per turn is reduced.
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r, Fig. 5B). Data do not support this possibility, as both P-pili and Hib pili have diameters of
70 Å. Second, the cavity within the fiber could be reduced in size. Again, data do not support this possibility; the central channel in Hib pili is 20 Å in diameter, while that in P-pili has an elliptical cross-section, with major and minor axes of 25 and 15 Å, respectively, yielding an insufficient difference in volume (<7%). Third, the rise per subunit could increase (z +
z, Fig. 5C). This does occur; there is a 7.6-Å rise per subunit for P-pili, compared with a 9.0-Å rise per subunit for H. influenzae type b (calculated from a 26.9-Å rise per three subunits). This increase could be due to an increase in the height, along the helical axis, of each subunit. To calculate the expected change, the new height for a cylinder with constant diameter (70 Å) and central channel (20 Å) and an increased volume of 20% was determined. The increase in height would be from 24.9 Å in P-pili (2) to 29.1 Å in Hib pili. This does not fit the existing data, as the pitch in Hib is increased compared to P-pili, but only to 26.9 Å. Fourth, the subunits may tip up, creating a space for the extra mass to be inserted at the surface (shown in Fig. 5D). This possibility need not change the filament radius (r), the channel size, or the rise per subunit (z) and is consistent with our structural data. It is also consistent with biochemical and immunochemical data from other laboratories, which predict that the insertions of HifA occur at surface-exposed regions of high sequence variability (4, 13, 17). This predicted addition of mass at the pilus surface is also consistent with the results of our sequence alignment between the major structural pilins of Hib pili and P-pili, HifA/Eagan and PapA/J96, respectively. With biochemical, mutational, immunologic, and evolutionary data (4, 8, 10, 12, 13, 17, 20, 26), we have produced an alignment in which the absence of cross-reactivity of antibodies to HifA amino acids 62 to 72 and 97 to 102 (20) is correlated with insertion regions of HifA compared with PapA, and the extended hypervariable region defined by Krasan et al. (17) corresponds to the largest insertion region. This region is expected to be surface exposed. While it is not yet possible to define the boundaries between individual subunits in our reconstruction, our data suggest the location of the large HifA insert to be the mass extending farthest from the helical axis, as can be seen modeled in Fig. 6.
What are the structural consequences of Hib pili having threefold symmetry, with subunits oriented approximately vertically along the filament axis? Both Hib and P-pili have about 3 subunits per turn of their helix; Hib pili contain 3 subunits in each turn, and P-pili contain 3.28 subunits per turn. Thus, only Hib pili comprise a structure with threefold symmetry at all positions along the helical axis. An observed consequence of this difference in symmetry and differences between the pilin subunits (HifA compared to PapA) is that in P-pili the predominant interactions are along the one-start helix, forming a coil that can be unwound under stress. In Hib pili the predominant interactions are along each of three interwound helices. It is therefore not possible to unwind the Hib pilus into a comparable single fibrillar structure. The Hib filament can be described by imagining three elastic ropes wound about each other, each connected to the others by weak cross-bridges. If the cross-bridges begin to peel apart, separating one rope from the other two, that rope may bulge out but will not easily become a thin distinct fiber; this would require either that the damage be propagated all the way to the end of the filament or that the strand be severed, conditions that were not observed in images of thousands of Hib pili.
Overextension of the helical filament into thin fibrillae, as shown for P-pili (1, 2), was not observed in Hib pili. The comparative velocity of flow in each host environment provides a plausible argument for this structural difference. A cough or a sneeze can reach a velocity of 150 km/h, whereas urine flows at
0.002 km/h and mucociliary clearance occurs at
0.0005 km/h. Continued adherence of H. influenzae to the nasopharynx most likely occurs in niches about which there is no detailed information, whereas initial adherence may occur in exposed, relatively unprotected locations. The bacteria must then maintain contact long enough to create or locate a more protected environment. Consequently, while typical environmental velocities in the urinary tract and the nasopharynx differ by a factor of only about 10, intermittent coughs and sneezes may result in an extreme environment for H. influenzae to withstand. The precise shear pressures have not yet been calculated for these two environments, but it seems likely that an extended thin fiber 20 Å in diameter could not survive velocities 75,000 times greater than those experienced in the urinary tract.
We hypothesize that the combination of a three-stranded helix and orientation of the HifA subunits almost vertically along the helical axis provide the structural stability necessary for Hib pili to survive in the nasopharynx prior to invasion of host cells. Thus, while P-pili and Hib pili have an overall morphology of
70-Å-diameter helical filaments with a length on the order of 1 µm, the structure of each pilus type is specifically adapted to its local environmental niche.
This work was funded, in part, by NIH/NIGMS grants to E.B. and E.H.E. and a grant from the Medical Foundation to E.B.
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