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Journal of Bacteriology, August 2004, p . 5052-5061, Vol . 186,
No . 15
Three-Dimensional Electron Microscopic Imaging of Membrane Invaginations in
Escherichia coli Overproducing the Chemotaxis Receptor Tsr
Jonathan Lefman,1,
Peijun Zhang,1,
Teruhisa Hirai,1 Robert M . Weis,1,2 Jemma Juliani,1
Donald Bliss,1 Martin Kessel,1 Erik Bos,3 Peter
J . Peters,3 and Sriram Subramaniam1*
Laboratory of Cell Biology, National Cancer Institute, National Institutes of
Health, Bethesda, Maryland 20817,1 Department of Chemistry,
University of Massachusetts, Amherst, Massachusetts 01003,2 Division
of Tumor Biology, The Netherlands Cancer Institute, Amsterdam, The Netherlands3
Received 24 December 2003/ Accepted 30 March 2004
Electron tomography is a powerful method for determining the
three-dimensional structures of large macromolecular assemblies, such
as cells, organelles, and multiprotein complexes, when
crystallographic averaging methods are not applicable . Here we used
electron tomographic imaging to determine the molecular architecture
of Escherichia coli cells engineered to overproduce the
bacterial chemotaxis receptor Tsr . Tomograms constructed from fixed,
cryosectioned cells revealed that overproduction of Tsr led to
formation of an extended internal membrane network composed of stacks
and extended tubular structures . We present an interpretation of the
tomogram in terms of the packing arrangement of Tsr using constraints
derived from previous X-ray and electron-crystallographic studies of
receptor clusters . Our results imply that the interaction between the
cytoplasmic ends of Tsr is likely to stabilize the presence of the
membrane networks in cells overproducing Tsr . We propose that
membrane invaginations that are potentially capable of supporting
axial interactions between receptor clusters in apposing membranes
could also be present in wild-type E . coli and that such
receptor aggregates could play an important role in signal
transduction during bacterial chemotaxis .
Over the last three decades, methods for three-dimensional reconstruction
of objects (5) imaged with an electron microscope have
been used to determine the structures of a variety of biological
assemblies by two types of approaches . One approach, which has
been used extensively in analyses of large macromolecular assemblies,
involves three-dimensional reconstruction of a structure by averaging
images recorded from several identical copies oriented randomly
relative to the electron beam (11, 31) .
The other approach, which has been used for reconstruction of objects
that cannot be easily averaged, such as whole cells, involves
tomographic reconstruction by combining projection images of an
object recorded with an electron microscope over a range of tilt
angles (4) . Electron tomography is therefore a
potentially powerful tool for three-dimensional imaging of the
spatial arrangement of proteins that make up complex and dynamic
assemblies, such as those involved in bacterial chemotaxis .
At least 12 proteins act in concert to convert the signal of
ligand binding at the periplasmic end of a chemotaxis receptor into
rotation of the flagellar motor (6, 27) .
The principal protein components at the input end include one of the
chemotaxis receptors (Tsr, Tar, Trg, Tap, or Aer), and the
cytoplasmic signaling proteins CheA and CheW, which are thought to
form a noncovalent complex with the chemotaxis receptors . Knowledge
of the structure and spatial arrangement of the chemotaxis receptors
is therefore fundamental to understanding the structural biology
of signaling . X-ray crystallographic studies of the periplasmic
fragments of the aspartate receptor fragments have revealed the
dimeric organization of the ligand binding domain, in which the
ligand binding pocket is located at the dimer interface (20) .
Structural studies of a cytoplasmic fragment of the related Tsr
receptor have shown that it also forms a dimer of extended
coiled-coil hairpins (13) . The cytoplasmic fragments pack in
the three-dimensional crystals used for X-ray crystallographic
analysis as trimers of dimers, and this has led to a proposal by Kim
et al . (14) that such an arrangement may also be
representative of full-length receptors in cell membranes . Figure
1a shows the spatial arrangement of the periplasmic
and cytoplasmic domains in the context of an atomic model for the
full-length receptor (14) that includes plausible
structures for the transmembrane region and the linker region between
the membrane domain and the cytoplasmic domain .
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FIG . 1 . (a) Structural model for the full-length Tsr dimer based on
structures of the periplasmic and cytoplasmic domains, adapted from the
work of Kim et al . (14) . (b and c) Projection images
of thin (70-nm) sections of fixed specimens of either wild-type E .
coli (b) or an E . coli Tsr-overexpressing strain
(HCB721/pHSe5.tsrQEQE) induced with 1 mM isopropyl-ß-D-thiogalactopyranoside
(IPTG) (c) . Scale bars = 0.5 µm . (d) Higher magnification of cells
overproducing Tsr . Scale bar = 50 nm . The dark spots in the images are
from 10-nm gold-conjugated protein A used to locate Tsr.
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Ultrastructural studies of bacterial cells in combination with
immunoelectron microscopy have revealed that chemotaxis receptors, as
well as CheA and CheW, are predominantly localized to the poles of
the cells (18, 25) . Although biochemical
studies have implicated the involvement of extended interactions
among receptor subunits in the membrane during signaling (1)
and many computational models for clustering have been proposed (19,
24), there is only limited direct structural
evidence that such interactions occur under physiological conditions .
Approaches such as electron tomography provide tools which can be
used to begin to unravel the molecular arrangement of these protein
components in the cell because of the potential for integrating
structural information from X-ray crystallography with the
lower-resolution data obtained from electron microscopic imaging . As
a first step in this direction, we obtained three-dimensional images
of the assemblies and networks formed in cells by overexpression of
the full-length chemotaxis receptor Tsr . Projection images recorded
from negatively stained membrane extracts obtained from cells have
shown that Tsr is organized in receptor arrays that have the
appearance of either zipper-like or micelle-like entities (32) .
The novel feature of these assemblies was the evidence that there are
direct interactions between Tsr molecules both in the plane of the
membrane and in the axial direction involving the cytoplasmic
domains . In this study, we extended this analysis into the third
dimension with a description of the overall architecture of cells
engineered to overproduce Tsr . The three-dimensional structural
analyses demonstrated that the receptor arrays form an extended
membrane network that extends into the cytoplasm, resulting in the
formation of extended sheets and tubules, which are converted into
the zippered and rounded assemblies seen in the isolated membrane
extracts . We also describe similar analyses performed with wild-type
cells to evaluate the presence of local invaginations in the
cytoplasmic membrane .
Fixation and embedding of cells. Escherichia coli strain
RP437 was used as the control for wild-type experiments . Plasmids
pHSe5.tsrQQQQ and pHSe5.tsrQEQE were used to
produce Tsr in HCB721 cells, which do not express the chemotaxis-related
proteins Tar, Tsr, Trg, Tap, CheA, CheW, CheR, and CheB, as
described previously (32) . Harvested cells were fixed at room
temperature for 2.5 h in a mixture of 2% paraformaldehyde and
0.2% glutaraldehyde in the presence of 60 mM piperazine-N,N'-bis(2-ethanesulfonic
acid) (PIPES), 50 mM HEPES (pH 6.9), 4 mM MgCl2, and 20 mM
EGTA . The fixed cells were collected by centrifugation and
resuspended in prewarmed 0.1 M phosphate buffer containing 12%
gelatin . After the cell-containing gelatin pellets were solidified on
ice, they were cut into 1-mm cubes and incubated with a solution
containing 2.3 M sucrose and 0.1 M sodium phosphate buffer (pH
7.4) . Cubes of gelatin were frozen on the surfaces of aluminum pins
by plunging them into liquid nitrogen and were sectioned with a
cryoultramicrotome at –120°C . Labeling with anti-Tsr antibody (which
specifically reacts with the conserved signaling domain) and protein
A-gold and subsequent embedding in methyl cellulose with uranyl
acetate with reagents were carried out as described previously (22) .
Electron microscopy. The projection images shown in Fig.
1 were recorded with a Gatan 2K charge-coupled
device camera mounted on a Tecnai 12 electron microscope (FEI
Corporation, Hillsboro, Oreg.) equipped with an LaB6
filament operating at 120 kV . For tomography, a series of images were
recorded at room temperature with the aid of a Gatan 2K
charge-coupled device (magnification,
x47,500)
by tilting the specimen from –70° to 70° in increments of
0.5° in a Tecnai F30 microscope equipped with a field emission gun
tip operating at 300 kV . Images were recorded at underfocus values
that were between 2 and 3 µm along the tilt axis . A back-projection
algorithm, as implemented in the IMOD reconstruction package (15),
was used to convert the information present in the series of tilted
projection images into three-dimensional density maps .
Preparation of Tween 80-extracted membranes. Membrane
preparations (16) isolated on sucrose gradients were
typically incubated with Tween 80 at a protein/Tween 80 molar
ratio of 0.004 for about 4 h as described previously (32) .
Segmentation and rendering. The tomogram was segmented in
the environment of the program Amira (TGS Inc., San Diego, Calif.) by
marking all regions in the volume where the bilayer (white lines in
the slice) could be visualized clearly in three dimensions . An
isosurface was created by tracing the path of the bilayer in each
slice of the tomogram . Structural models of the two types of receptor
assemblies shown in Fig . 3d and e were docked onto the
isosurface by using the program 3dsmax (DISCREET, Montreal, Quebec,
Canada) . The coordinates for the receptor dimer were the coordinates
in the model described by Kim et al . (14) and kindly
provided by Sung-Hou Kim . Starting from the model of the dimer, a
variety of plausible arrangements for higher-order arrangements, such
as the trimer of dimers shown in Fig . 3d and e, were
then generated by using the electron microscopic images as a guide .
One set of the plausible arrangements is shown in Fig .
3 .
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FIG . 3 . (a to c) Negatively stained electron micrographs obtained from a
Tween 80 extract of cells expressing Tsr . The extract preserved the
overall appearance of the membrane morphologies in the tomogram, and the
images show in more detail the organization of the zippered structures
in cross section (a) and top view (b), as well as rounded vesicular
structures (c) . Scale bars = 50 nm . (d) Molecular model for packing in
the zippered regions based on the atomic model for the structure of Tsr
shown in Fig . 1a and the electron crystallographic
analysis of the crystalline regions (32) . The packing
in the crystalline areas of the membrane (b) roughly corresponds to a
lattice with the following constants: a,
75
Å; b,
75
Å; and
,
60° .
The cross-sectional area of each unit in the crystal is
5,000
Å2, which can accommodate at most three Tsr dimers, based on
the presence of four helices per Tsr monomer at the wider, periplasmic
end of the receptor (20) and the known values of
about 180 Å2 that characterize the cross-sectional areas of
helices in well-packed two-dimensional crystalline arrays (12) .
The array shown is one of many possible arrangements of the three dimers
and is presented primarily to provide an indication of the density of
receptor packing in the membrane . The white regions at the center of the
zippered structure in panel a are interpreted as high-density regions
where the cytoplasmic ends of the Tsr trimer are presumed to be
interdigitated . The depth of the interdigitation is consistent with the
proportional width of this region in the micrograph in panel a . The
average internal spacing of the zippered structures in tomographic
slices such as the slice shown in Fig . 2c is 31.5 +
2.5 nm (averaged over 26 separate measurements) . This compares well with
the value for the same internal spacing in these negatively stained
specimens (31.3 ± 0.6 nm [averaged over 10 measurements], as reported by
Weis et al . [32]) . (e) Molecular model for packing in
the vesicular regions (sectional view) . The outer white ring of the
circular structure in panel c is interpreted as the surface of the
membrane region enclosing the volume, and the less clear inner ring is
interpreted as a high-density region where the cytoplasmic ends of Tsr
come together.
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We carried out a three-dimensional structural analysis of E . coli
cells engineered to overexpress the 60-kDa membrane protein Tsr (16)
in order to explore whether the novel assemblies observed in membrane
preparations isolated from disrupted cells (32)
could also be detected in intact cells and imaged . Immunolabeling of
fixed cryosections of wild-type E . coli (Fig . 1b)
showed that Tsr was predominantly located at the polar region(s) of
the cells, which is consistent with previously reported data (18) .
In contrast, in cells overproducing Tsr, the receptor was located
throughout the periphery and in some interior regions of the cell
(Fig . 1c) . In all areas where the immunolabel appeared
to be localized to the interior of the cell, there was evidence
of membranous material, implying that the high level of Tsr resulted
in extension of the membrane so that it was no longer confined to the
periphery of the cell . A closer examination of a region of the cell
displaying invaginations (Fig . 1d) confirmed that
the immunolabel, which was directed against the C-terminal region of
Tsr, was localized primarily to the interior portions of the zippered
regions .
In order to investigate the three-dimensional structure of the
cells overproducing Tsr, we recorded a series of projection images by
tilting the specimen relative to the electron beam, typically over a
range of ±70° (Fig . 2a) . The images were then
combined by using weighted back-projection methods to reconstruct the
three-dimensional structure . Representative slices from an electron
tomogram constructed from images such as those shown in Fig.
2a are shown in Fig . 2b and c . These
slices provide a glimpse of the extensive internal organization
of the membranes and the improved clarity relative to the projection
images . The slice in Fig . 2b is close to the upper edge of the
section on the grid and shows extensive labeling of Tsr, as
expected . The slice in Fig . 2c is from an interior region of
the section, and the absence of immunolabeling reflects the
lack of penetration of the anti-Tsr antibody and/or the protein
A-gold conjugates into the section . An MPEG movie of the tomogram is
available at
http://hrem.nci.nih.gov/Lefman_et_al_J.Bact_2004/E.coli_tomogram .
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FIG . 2 . (a) Selected projection images (recorded at tilt angles of 0°,
35°, and 70°) from a 250-nm-thick section obtained from cells
overproducing Tsr . (b and c) Slices from an electron tomogram
constructed by using a series of tilted images from –70° to 70° at tilt
intervals of 0.5° . The slice in panel b is from a region closer to the
surface of the section, while the slice in panel c is from an interior
region that is not accessible to the protein A-gold particles . Bars,
0.17 µm (b and c) . (d) Computed Fourier transform from a region in the
x-y slice of the tomogram, showing Thon rings at a
resolution of 15 Å–1 in the x-y plane
(indicated by the arrow) . The region of the slice used to calculate the
transform contains a flagellar filament whose helical structure is
responsible for producing the elongated spots in the transform in the
horizontal direction . (e) Transform in the x-z plane from
a similar-size region, showing the expected missing wedge due to the
absence of data between tilt angles of 70° and 90° and Thon rings at a
resolution of
22
Å–1 (indicated by the arrow) . The edge of the transform in
panels d and e is at 13 Å–1.
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A measure of the quality of both the collected data and the
reconstruction procedure was obtained from analysis of a small region
extracted from the central region of the tomogram used to obtain the
images shown in Fig . 2 . The Fourier transforms
(Fig . 2d and e) computed from individual horizontal (x-y)
and vertical (x-z) slices in the tomogram showed that
there were well-defined Thon rings (30) . The first
zero crossing of the contrast transfer function was at
40
Å–1, and the spacing of the rings matched the values
expected for the defocus values used ( 2.6-µm
underfocus along the tilt axis) . The overall contrast in the slice
arises primarily from the presence of the uranyl acetate used for
staining . However, the intrinsic resolution limit in a given slice of
the tomogram relevant for detection of molecular structures is
expected to be limited by the damage that occurred during specimen
preparation and by the radiation-induced damage that occurs upon
illumination of the specimen . For these reasons, the tomograms were
not corrected for the effects of the contrast transfer function .
Inspection of the tomographic slice in Fig . 2c suggests
that the internal volume is laced with an extensive network of
twisted sheet-like features that have the appearance of stacked
layers in certain regions and rounded features that appear to be
vesicular in cross section in other regions . From their location and
continuity with the cytoplasmic membrane, it is clear that the white
lines defining the boundaries of the stacks and the rounded
structures represent the bilayer membrane . The formation of these
structures is a consequence of invaginations of the surface of the
cytoplasmic membrane in response to the high level of expression of
Tsr . The uniformity of the spacing between the membrane layers (there
was <5% variation across the length of an individual stretch)
in the stacks is consistent with the idea that the membrane network
is stabilized by specific interactions between protein components in
the bilayer membrane . Since these extended stacks and rounded
structures were not observed in either wild-type E . coli or
control cells not expressing Tsr, the simplest explanation is that
they are formed in response to the high concentration of Tsr in the
membrane and are stabilized by interactions between Tsr molecules
located in adjacent bilayer membranes .
Further structural insights into the molecular organization of the
membrane stacks were developed from analyses of membrane extracts
obtained from lysed cells (32) . Tsr represents about
90% of the polypeptide present in these membrane extracts (16) .
Micrographs (Fig . 3a to c) obtained from negatively
stained membrane specimens treated with small amounts of the
detergent Tween 80 (at molar ratios of 1:250) indicated that there
was a rich variety of connected membranous morphologies (see the
legend to Fig . 3 for details of the dimensions), with
the principal components being represented by (i) zipper-like
features (Fig . 3a) with dimensions matching those
observed for the cross sections of the sheet-like regions detected in
the tomogram, (ii) small crystalline arrays (Fig . 3b)
with pseudohexagonal ordering, and (iii) rounded structures (Fig.
3c) which had a micellar appearance in the
projection images and had a radius of curvature similar to that
observed for the rounded structures in the tomogram . Previous
electron crystallographic analyses (32) have suggested
that the packing of the small crystalline patches in the plane
is consistent with an arrangement in which the repeating unit has
three Tsr dimers with a packing density of approximately 200 Å2/helix .
The overall appearance of these structures is thus similar to the
appearance of structures seen in cells, although the detergent
treatment may have resulted in a slight enhancement of the packing
density of protein in the membranes .
The constraints for receptor packing in the isolated membrane
preparations suggest how the interactions between Tsr cytoplasmic
domains from two adjacent bilayers could lead to the formation of a
pair of stacked membranes whose appearance (Fig . 3d) could
correspond to that of a sheet (membrane stack) in a tomogram
(Fig . 2c) and a zipper (Fig . 3a) or
quasicrystalline array (Fig . 3b) in a projection
view . Similarly, it is possible to derive a plausible molecular model
for the rounded structures (Fig . 3e) in which the
lengths of the cytoplasmic domain of Tsr are well-matched with the
experimentally measured radii in the electron micrographs (Fig.
3c) and with packing densities of the cytoplasmic
ends of Tsr in its interior comparable to the densities observed in
the zipper-like structures . Construction of plausible models for
these assemblies allowed placement of the assemblies into the
tomographic volume, thereby providing a powerful tool for
interpreting the large amount of information contained in the
tomogram at the molecular level (Fig . 4) .
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FIG . 4 . (a) Segmented representation of a small region from a cellular
tomogram . (b) Slice of the tomogram . The region indicated by the box
(width, 230 nm) corresponds to a slice in the region that was segmented .
Aside from the interaction between the cytoplasmic domains (yellow) in
apposing bilayers, a complementary interaction between the periplasmic
domains (blue) also appears to be likely . The uniformity in spacing
between the rounded vesicular region and the invaginated membrane
surrounded by it suggests that the entire membrane network is stabilized
by interactions at both ends of the receptor . The segmented region is
composed of two sets of stacked membranes . The lower membrane sheet is
wrapped around a tubular invagination (see panel 4 in Fig .
5 for a schematic representation of the geometry) . The segmentation
was carried out to be faithful to the density in the tomogram and is
therefore noisy, as seen, for example, in the patchy appearance of the
rounded end of the tubular invagination.
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What is the mechanism underlying the formation of these structures?
In wild-type E . coli, the surface area covered by the cytoplasmic
membrane is adequate to accommodate normal levels of expressed
membrane proteins and lipids . In the cells overproducing Tsr, as the
Tsr levels began to exceed the amount of membrane proteins normally
present in the cell, the membrane invaginates in order to accommodate
the excess protein (Fig . 5, panels 1 and 2) .
Evidence for these intermediate stages is clearly present in other
regions of the tomographic slice shown in Fig . 2c . The
interaction between the invaginated membranes can thus lead to
the formation of two kinds of stacking interactions (Fig .
5, panels 3 and 4) depending on whether they involve the
periplasmic side (narrower spacing) or the cytoplasmic side (wider
spacing) . The interactions at the periplasmic domain may help
accommodate the unique packing interaction between complementary
curved surfaces (i.e., between the rounded ends at the ends of two
separately invaginated regions) . As shown in Fig . 5,
panel 5, these interdigitated surfaces can sometimes suggest the
presence of free-standing vesicular regions in a given slice .
However, all such regions inspected by tomography were found to
represent fortuitous cross sections of tubular invaginations arising
from a different plane of the membrane .
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FIG . 5 . Schematic illustration of the formation of membrane networks
such as the network shown in Fig . 3 . (Panel 1)
Cytoplasmic membrane of wild-type cell or overproducing cell when the
levels of Tsr expression are not very high . (Panel 2) Invaginations of
the cytoplasmic membrane at different regions to accommodate the
increased levels of Tsr by increasing the ratio of membrane surface to
cytoplasmic volume . (Panel 3) Formation of two kinds of interactions
between proximal invaginated membranes . The interactions between the
cytoplasmic domains (yellow) in adjacent membranes lead to a zipper-like
structure with wider spacing (about 270 Å), while the interactions
between the periplasmic domains lead to the zipper-like structure with
narrower spacing (about 150 Å) . Note that the diagram is drawn so that
it indicates that not all regions of the membrane are part of the
zippered structures . (Panel 4) The rounded regions at the ends of the
invaginations are occasionally large enough to accommodate an
invagination from a different region of the membrane, as shown by the
rounded tubule beginning to emerge from the backside . (Panel 5) The
secondary invagination can become large enough that its growth is
limited by the boundaries of other surrounding membranes . A
cross-sectional view through such a region would have the appearance of
a free-standing vesicular region . This diagram corresponds to the
tomogram shown in Fig . 4b (rotated clockwise about
70°).
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Are the modes of interaction which we observed in cells overproducing
Tsr relevant to chemotaxis receptors in wild-type cells? While the
resolution of electron tomograms is not adequate at present to detect
individual Tsr dimers in wild-type cells, we reasoned that a
prerequisite for the formation of axially interacting receptor
clusters would be local curvature variations in the cytoplasmic
membrane which might be detectable in tomograms . Tomograms recorded
from wild-type cells (RP437) indeed showed the presence of small
local invaginations, as indicated in two representative slices shown
in Fig . 6 . These invaginations were about five
times more abundant in the polar regions of the cell, and their
overall frequency of occurrence was low; fewer than 10 such
invaginations were typically observed in tomograms of 1,000-Å-thick
slices of wild-type cells . This is not surprising since the level of
expression of Tsr in the overproducing strain is
2
orders of magnitude higher than the combined levels of expression of
all chemotaxis receptors in wild-type E . coli . The dimensions
of some of the invaginations (Fig . 6a) appear to be
too small to accommodate the zippered assemblies, such as those shown
in Fig . 4, or the receptor-CheA-CheW complexes
observed in vitro by mixing purified components (10) .
However, other invaginations (Fig . 6b) resulted in
membrane geometries that were, in principle, long enough to
accommodate such a longitudinal receptor-transducer assembly .
Invaginations such as those seen in wild-type cells were also
observed in control cells (HCB721) lacking chemotaxis receptors,
indicating that chemoreceptors are not required in the formation of
these invaginations . At present, it is not possible to establish
whether some of the invaginations in wild-type cells contain axially
interacting clusters of chemoreceptors . We also cannot exclude the
possibility that the invaginations in the wild-type cells were an
artifact induced by chemical fixation . Nevertheless, we think that it
is conceivable that the initial formation of the different shapes
could be an intrinsic property of the cytoplasmic membrane that
is preferential to polar regions of the such cells . Once they are
formed, such invaginations could provide a structural context for
axial interaction signaling between receptors which may already be
clustered (1) in the plane of the membrane . Structural
analyses of cells fixed by rapid freezing instead of chemical
methods, as well as resolution improvements in tomography, are likely
to provide a greater understanding of the structure and arrangement
of chemoreceptor assemblies in bacterial cells .
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FIG . 6 . Representative slices from tomograms of sections obtained from
wild-type cells processed in the same way that the strain overproducing
Tsr was processed . Invaginations in the cytoplasmic membrane are evident
in both tomograms . The invagination in panel a appears to be too small
to accommodate an axially interacting cluster of chemotaxis receptors,
while the invagination in panel b has the potential to accommodate such
an interdigitated receptor cluster at the locations indicated by the
arrow (width,
50
nm) . Scale bars = 50 nm.
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It is instructive to identify specific features revealed by the
tomographic analysis that are not evident in projection images
recorded from isolated membrane assemblies . One of the goals of the
tomographic studies was to understand the nature of membrane
continuity in the cells overproducing Tsr . Two-dimensional images do
not allow determination of whether the striations and rounded regions
observed in images such as those in Fig . 3a to c
result from free or connected entities in the cell . Our tomographic
analysis revealed that in all cases examined, the invaginations
showed evidence of physical continuity with the cytoplasmic membrane .
An illustration of the insight gained by this approach is shown in
Fig . 5, panel 5, which suggests how a series of
sectional views alone could lead to an incorrect interpretation .
Another new insight from the tomography analysis is the
identification of a well-preserved shorter spacing corresponding to
the face-to-face interactions between the periplasmic sides of the
membrane (Fig . 4) . This interaction, which is presumably
weaker than the interdigitating interaction on the cytoplasmic
side, was an unexpected finding and explains how a three-dimensional
network of membranes could be stabilized in the cell by combining the
cytoplasmic and periplasmic pairs of interactions . Finally, it is
important to note that there is significant improvement in resolution
in a tomographic slice compared to the resolution in a projection
image . For example, the image in Fig . 2c, which
corresponds to a 1.4-nm-thick computational slice, shows more
structural detail than one would expect from a conventional thin
section that is 30 to 50 nm thick .
The accumulation of membrane-rich structures as a result of
overproduction of membrane proteins has been documented previously
for both prokaryotic cells (3) and eukaryotic cells (2) .
There are also examples of membrane deposits that have been found
naturally, such as the deposits found in certain cyanobacteria
(23) . Nevertheless, the observation of these extended
structures provides an interesting view of the effects of
overexpression of membrane proteins in a bacterial cell . It is very
likely that high levels of expression of a membrane protein may be
required before invaginations form, but it is equally possible
that high levels of expression can be sustained in this case because
of the stabilization of the membrane by the interactions which we
describe here . The receptor arrangements reflect the intrinsic
tendency of Tsr to associate, and extension of these studies to
analysis of cells overproducing Tsr, CheA, and CheW is likely to
provide further insights into the organization of receptor-transducer
assemblies in chemotaxis .
The presence of the invaginations in wild-type cells could provide
a new dimension to considerations of the molecular mechanism of
receptor signaling . The propensity of Tsr to interact axially
suggests that the interactions might stabilize the formation of
complexes of CheA and CheW with the receptor in which these signaling
proteins bind at the junction of the two cytoplasmic tail regions .
Such an arrangement has indeed been experimentally observed in
mixtures prepared from purified CheA, CheW, and a Tar receptor in
which the transmembrane region was replaced by a stretch of mostly
nonpolar residues (10) . What is especially
striking is that the combined length ( 30
nm) of the apposing cytoplasmic portions in the pair of axially
interacting receptors in this ternary complex is essentially the same
as the length observed in the zippered Tsr assemblies reported here
(Fig . 3) which did not contain either CheA or CheW .
It is therefore reasonable to suppose that the type of interaction
observed here in the cells overproducing Tsr in the absence of CheA
and CheW may also be relevant to signaling in wild-type bacteria .
In cells that lack expression of chemotaxis receptors, CheA and
CheW do not localize to the poles, while in cells with normal levels
of chemotaxis receptors but without CheA and CheW the extent of polar
localization of receptors is considerably reduced (17) .
The idea that invaginations near the polar regions may provide a
mechanism for the selective clustering of an assembly of
chemoreceptors, CheA, and CheW is fully consistent with these
findings .
The zippered and rounded assemblies that we describe here have
some parallels to structural features observed in eukaryotic cells .
Weak homotypic interactions between cytoplasmic domains of membrane
proteins expressed in the endoplasmic reticulum are known to induce
the formation of membrane stacks known as crystalloid (33)
or organized smooth (26) endoplasmic reticulum .
All eukaryotic cells also have molecular machinery that is capable of
triggering the conversion of flat regions of membrane into rounded
structures that can be used for transporting soluble and
membrane-bound components . At least four eukaryotic proteins have
been identified that can induce changes in membrane curvature:
dynamin (28), amphiphysin (29), endophilin
(7), and epsin (8) . Furthermore,
the recruitment of clathrin to membranes via epsin (8)
or Ap180 (9) can trigger bud formation, an event that precedes
vesicle formation . The novel aspect of our work is the discovery
that when suitable protein-protein interactions are present,
phenomena strongly resembling curvature induction and tubulation (21)
may be mimicked even in a simple prokaryotic model system . The
rounded regions in the cell appear to be poised for release as small
vesicles, but they stay attached in the absence of a mechanism such
as detergent addition (Fig . 2c) or an energy source
that triggers their release . We expect that the methods used here to
reveal the organization of the bacterial membrane networks will be
directly applicable to imaging similar structures in eukaryotic cells
and that the strategy of combining tomographic, electron, and X-ray
crystallographic approaches can be a tool that is generally
applicable for constructing plausible three-dimensional models for
protein networks in cells at molecular resolution .
We thank Anas Chalah for assistance with preparation of membranes and
Stanton Lee for generous assistance with recording tomograms .
This work was supported by the intramural program at the National
Cancer Institute .
* Corresponding author . Mailing address: Laboratory of Cell
Biology, National Cancer Institute, National Institutes of Health, Bethesda, MD
20817 . Phone: (301) 594-2062 . Fax: (301) 480-3834 . E-mail: ss1@nih.gov .
J.L . and P.Z . contributed equally to this work .
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