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Biophys J, January 2000, p. 373-384, Vol. 78, No. 1
Vollum Institute and Department of Microbiology, Oregon Health Sciences University, Portland, Oregon 97201-3098 USA
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ABSTRACT |
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We have used an in vitro system that mimics the assembly of immature Moloney murine leukemia virus (M-MuLV) particles to examine how viral structural (Gag) proteins oligomerize at membrane interfaces. Ordered arrays of histidine-tagged Moloney capsid protein (his-MoCA) were obtained on membrane bilayers composed of phosphatidylcholine (PC) and the nickel-chelating lipid 1,2-di-O-hexadecyl-sn-glycero-3-(1'-2"-R-hydroxy-3'N-(5-amino-1-carboxypentyl)iminodiacetic acid)propyl ether (DHGN). The membrane-bound arrays were analyzed by electron microscopy (EM) and atomic force microscopy (AFM). Two-dimensional projection images obtained by EM showed that bilayer-bound his-MoCA proteins formed cages surrounding different types of protein-free cage holes with similar cage holes spaced at 81.5-Å distances and distances between dissimilar cage holes of 45.5 Å. AFM images, showing topological features viewed near the membrane-proximal domain of the his-MoCA protein, revealed a cage network of only symmetrical hexamers spaced at 79-Å distances. These results are consistent with a model in which dimers constitute structural building blocks and where membrane-proximal and distal his-MoCA regions interact with different partners in membrane-bound arrays.
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INTRODUCTION |
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C-type retroviruses, such as the Moloney
murine leukemia virus (M-MuLV), represent a family of RNA viruses that
replicate through a DNA intermediate (Coffin et al., 1997
). They are
composed of cellular and viral components and are enveloped by
host-derived lipid membranes that contain proteins encoded by
retroviral env genes. The virus core is composed of
1000-5000 copies of the viral Gag proteins; 10-100 copies of
pol gene-encoded proteins, which include the viral protease,
reverse transcriptase, RNAse H, and integrase; two copies of the viral
RNA genome; and cellularly derived tRNAs that serve as primers during
reverse transcription (Coffin et al., 1997
). The assembly of C-type
retrovirus particles appears to occur at the plasma membranes of
infected cells and is directed by the Gag protein, which has been shown
to be necessary and sufficient for particle assembly. Most mammalian
retrovirus Gag proteins are synthesized as precursor polyproteins
(PrGag) and normally are cleaved into the mature
processed Gag proteins by the viral protease (PR) during or after
budding. Processing of PrGag results in a major
morphological change in virus particles, in which electron-dense
material adjacent to the periphery of the immature virion reorganizes
into the central and dense superstructure of the mature virus. For
M-MuLV, processing of PrGag yields the four
mature Gag proteins, matrix (MA), p12, capsid (CA), and nucleocapsid
(NC). While each mature Gag protein serves an essential function for
replication, several Gag domains are dispensable with regard to virus
particle assembly. For instance, deletion of p12 has been shown to be
compatible with particle assembly (Hansen and Barklis, 1995
). Moreover,
the only part of MA necessary for HIV or M-MuLV assembly appears to be
its membrane-binding myristate anchor (Wang et al., 1993
; Faecke et
al., 1993
; Barklis et al., 1997
). Furthermore, while the RNA-binding
retrovirus NC domains contribute to the efficiency of particle
formation (Campbell and Vogt, 1995
; Wills et al., 1994
), under some
circumstances they can be replaced in vivo (Zhang et al., 1995
), and
they are not essential to the formation of particle-like structures in vitro (Gross et al., 1998
; Von Schwedler et al., 1998
). This leaves the
capsid, or a portion of the CA domain, as central to the particle production process.
Although some Gag protein functions seem to be well defined,
the three-dimensional structures of retroviruses are not. A major obstacle has been the heterogeneity of naturally occurring virus particles. Nevertheless, researchers have determined the structures of
some Gag protein domains and their derivatives (Gitti et al., 1996
;
Gamble et al., 1996
; Hill et al., 1996
; DeGuzman et al., 1998
; Dememe
et al., 1994
; Fass et al., 1997
), and certain Gag domains can assemble
into rod- or sphere-shaped structures in vitro (Campbell and Vogt,
1995
; Von Schwedler et al., 1998
; Gross et al., 1998
). However, to
understand the mechanism of C-type retrovirus assembly, it is important
to analyze how Gag proteins organize on membranes, where virus particle
assembly occurs (Coffin et al., 1997
). One such analysis was an
electron microscopy (EM) study of HIV PrGag
proteins assembled at the plasma membranes of baculovirus
vector-infected cells (Nermut et al., 1994
). At low resolution (40-50
Å), the PrGag proteins appeared to form
cage-like structures beneath the membranes. In an effort to improve
upon Gag-membrane structure studies, we recently devised an in vitro
method for the analysis of Gag-membrane interactions (Barklis et al.,
1997
, 1998
). The approach, which is based on previous lipid monolayer
studies (Darst et al., 1991
; Uzgiris and Kornberg, 1983
), employs
histidine-tagged (his-tagged) Gag protein derivatives and a model
membrane consisting of egg phosphatidylcholine (PC) and the novel
nickel-chelating lipid 1,2-di-O-hexadecyl-sn-glycero-3-(1'-2"-R-hydroxy-3'-N-(5-amino-1-carboxypentaiminodiacetic acid) (DHGN) (see Fig. 1; Barklis et al.,
1997
). Using this system to produce samples for EM analysis, we have
found that membrane-bound HIV-1 capsid proteins formed hexamer-trimer
cages (Barklis et al., 1998
) consistent with previous lower resolution
studies (Nermut et al., 1994
), while M-MuLV capsid proteins formed
distinct hexamer-hexamer cages (Barklis et al., 1997
). To extend these
results, we have adapted our procedures to permit the imaging of lipid
bilayer-bound M-MuLV his-tagged capsid proteins (his MoCA) by both EM
and atomic force microscopy (AFM) in buffer solution (Binnig et al.,
1986
; Hansma and Hoh, 1994
; Muller et al., 1995
; Shao and Yang, 1995
; Brown et al., 1998
; Czajkowsky et al., 1998
; Fotiadis et al., 1998
;
Sato et al., 1998
). In agreement with monolayer findings, our EM
projections show that bilayer-bound his-MoCA forms a protein cage
surrounding different types of cage holes, in which similar cage holes
are spaced at 81.5-Å intervals, while dissimilar holes occur every
45-46 Å. AFM images, showing topological features, revealed a cage
network of only symmetrical hexamers spaced at 79-Å distances. Our
results are consistent with a model in which dimers constitute
structural building blocks and where membrane-proximal and distal
his-MoCA regions interact with different partners in membrane-bound
arrays.
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MATERIALS AND METHODS |
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Materials
Egg phosphatidylcholine (PC) was purchased from Avanti Polar
Lipids. DHGN was prepared by D. Thompson and charged with nickel as
described (Barklis et al., 1997
). Highly oriented pyrolytic graphite
(HOPG) and mica AFM substrates were from Digital Instruments (Santa
Barbara, CA) and Ted Pella, respectively, and carbon EM grids (300 mesh) were from Ted Pella. Water was filtered with a MilliQ
purification system.
Construction of the vector for bacterial expression of M-MuLV capsid protein
A M-MuLV capsid-coding region cassette was inserted into the
BamHI site of pET15B (Novagen). The cassette was constructed by polymerase chain reaction, generating a BamHI site at the
amino-terminus of the CA-coding region, and adding a BamHI
linker at the carboxy-terminal MscI site of this region. The
respective N- and C-terminal ends of the cassette are
GGAT/CCC, where the bold C is the M-MuLV viral nucleotide
1266 and TTG/GCGGATCC, where the bold G is viral nucleotide
2055. The plasmid pET15B-MoCA then was introduced into
Escherichia coli strain BL21(DE3)/pLys S (Novagen), and the bacteria was stored at
80°C in 50% glycerol.
Protein expression and purification
Cells of E. coli strain BL21(DE3)/pLys S containing
pET15B-MoCA were grown at 37°C in LB plus 15 mg/L chloramphenicol and 50 mg/L ampicillin to an OD600 of 0.7. Protein expression then was
induced by the addition of
isopropyl-
-D-thiogalactopyranoside (IPTG) 0.5 mM, and after 3 h of shaking at room temperature the bacteria were
harvested by centrifugation and stored at
80°C. For purification,
frozen bacterial pellets were resuspended in lysis buffer (50 mM sodium
phosphate, pH 7.8, 300 mM NaCl, 1 mM phenylmethylsulfonyl fluoride, 2 mM
-mercaptoethanol) and disrupted in a French press. Cellular
debris was removed by centrifugation (12,000 × g; 15 min; 4°C), and his-MoCA proteins were purified by two cycles of
nondenaturing affinity nickel-chelate chromatography, using a stepwise
gradient of imidazole (0, 10, and 250 mM in 50 mM sodium phosphate,
10% glycerol, 0.5 M NaCl, pH 7.8 for washes, pH 6.0 for elutions).
Fraction purities were assessed by a combination of Coomassie staining
and immunoblotting of electrophoretically separated proteins. Once
identified, pure fractions were desalted on Sephadex G-25 spin columns
equilibrated with 5 mM 3-(N-morpholino)propanesulfonic acid
(MOPS) (pH 7.8), 10% glycerol, and proteins were stored at
80°C.
Preparation of vesicles containing Ni2+-DHGN
Ni2+-DHGN (10 nmol) and egg
phosphatidylcholine (100 nmol) in chloroform solutions were mixed and
dried under a flux of nitrogen. The lipids then were fully dried under
vacuum and resuspended to 50 µM Ni2+-DHGN and
µM PC in 2× PNG buffer (200 µl) by sonication in an ultrasonic bath for 10 min. Vesicles were stored at 0-4°C for up to
2 weeks. Alternatively, and with similar success, vesicles were
prepared in 10 mM MOPS buffer (pH 7.8), 50 mM NaCl, by detergent dialysis techniques (Tauskela et al., 1992
).
Specimen preparation
The his-MoCA proteins (5 µl, 1-5 µg) were mixed gently with 5-µl vesicle suspensions, and drops were transferred onto 5-mm wells of depression well slides (no. 101005; Carlson Scientific). The slides then were placed into 150-mm petri plates humidified with a filter paper wetted with 2.5 ml water. Dishes were sealed tightly with parafilm strips before overnight incubations at 30°C. For EM analysis, arrays were transferred onto ultrathin, formvar-removed carbon grids (no. 1882-F; Ted Pella) by placing grids on top of the drops for 1 min. Samples then were processed by placing grids on top of 100-µl water drops for 30 s, wicking from the side, staining for 45 s on 50 µl 1.3% uranyl acetate (freshly diluted and filtered), followed by blotting and air drying. For AFM analysis, drops were deposited on freshly cleaved 3 mm × 3 mm highly oriented pyrolytic graphite or mica sheets. After 1 min, the samples were rinsed with water (three times 50 µl) and then maintained under a viewing buffer (20 mM TrisHCl, pH 8.0, 100 mM KCl).
Transmission electron microscopy
Electron microscopy was performed on a JEOL JEM1200EX operated at 100 kV (Portland VA Hospital). Low-dose photography was carried out at ambient temperature, using Kodak SO163 film. Searching was performed at a magnification of 5000×, and focusing and photography were at 40,000-60,000×.
Atomic force microscopy
After specimen adsorption, samples were mounted on an E-piezoscanner of an atomic force microscope equipped with a fluid cell (Nanoscope III; Digital Instruments, Santa Barbara, CA). Calibration of the scanner was carried out with mica as the substrate reference. Cantilevers with oxide-sharpened Si4N4 tips (purchased from Digital Instruments) were 200 µm long and had nominal spring constants of 0.06 N/m. Initial tip engagements were performed by setting the scan size to 0 nm to minimize sample deformation. Before the samples were scanned, the operating point of the servo system was set to forces below 1 nN.
Image processing
For EM images, micrographs 100315, 100316, 121215, and 121216 were digitized at 6.53 Å/pixel and converted to MRC format images r100315b, r100315c, r100316a, r100316c, r100316d, r100316e, r121215, and r121216 (Unwin and Henderson, 1975
; Baldwin et al., 1988
, Henderson
et al., 1990
). With the use of the ICE image analysis package (Schmid
et al., 1993
), real space images were Fourier transformed, and
diffraction patterns were indexed by hand. Lattices were refined and
unbent using the MRC-derived programs MMBOX and UNBEND (Baldwin et al.,
1988
, Henderson et al., 1990
; Schmid et al., 1993
). After these steps,
the calculated amplitude and phase (aph) files were edited manually to
remove all low signal-to-noise reflections of IQ > 5. The
acceptable reflections yielded resolutions extending to ~26 Å, and
the completeness of the data was ~70% (50% in the 37-25 Å resolution shell). The best space groups for amplitudes plus phases
(aph) files were determinated using the ALLSPACE program, using
hexagonally indexed diffraction patterns. (Note that p6 residuals were
aberrantly high when orthogonally indexed reflections were used as the
ALLSPACE input.) Merging of images and determination of phase residuals
were performed using unbent aph files and the program ORIGTILTB
(Henderson et al., 1990
). For all merges, the r100316b film was used as
the reference image. Reconstruction of a real image was done using the
programs CREATE TNF and FFTRANS. Files in MRC-format were then
converted to TIFF format.
For AFM, 300 nm × 300 nm images were acquired at a resolution of
512 pixel/line and were exported in TIFF formats. Images then were
converted to SPIDER format (Frank et al., 1988
) for real space
averaging steps. For averaging, raw images were Gausian low-pass
filtered, and 12 140.6 Å × 140.6 Å windows were picked and summed to
yield a cross-correlation reference. The reference then was used to
locate cross-correlation peaks using the SPIDER (Frank et al., 1988
)
operation CC, and 187.5 × 187.5 Å2 raw
image areas, representing the top 100 cross-correlation peaks, were
summed to give an average image. The quality of this image was
evaluated by halving the 100 image data set, averaging the half-sets,
and comparing the Fourier ring correlation (FRC) values between the
averages at different resolutions, using the SPIDER operation RFM
(Frank et al., 1988
).
Quantification of his-MoCA bound to vesicles
For isolation of MoCA-bound membranes, 200-µl mixtures
containing 25 µM his-MoCA and 250 µM PC:
Ni2+-DHGN 10:1 vesicles in PNG buffer, pH 8.3, were incubated overnight at 30°C and ultracentrifuged for 20 min at
165,000 × g (rotor Beckman TLS 55; 50,000 rpm) to
pellet membranes. Supernatants were carefully discarded to remove
unbound his-MoCA, and membranes were resuspended in 60 µl 10 mM MOPS
(pH 7.8), 50 mM NaCl (buffer A). As controls, two other incubations
were performed, with the omission of either the protein or the lipid
membranes. For quantification of his-MoCA bound to vesicles using the
mouse anti-CA monoclonal antibody Hy187 (Hansen et al., 1993
), two
10-µl aliquots of the previously prepared his-MoCA-bound membranes
were withdrawn and overlayed on the upper faces of two freshly cleaved
HOPG pucks (2 cm2) for 30 min, after which the
pucks were rinsed four times with buffer A (150 µl). One puck was
extracted directly with 40 µl 20 mM TrisHCl (pH 7.4), 150 mM NaCl, 1 mM EDTA, 0.1% sodium dodecyl sulfate (SDS), 1% Triton X-100, 0.5%
sodium deoxycholate (IPB buffer), and the other puck was incubated with
anti-CA (500 µl; 0.3 g/L in phosphate-buffered saline) for 30 min at
room temperature, rinsed, and extracted as decribed above. As controls,
10-µl aliquots of his-MoCA bound membranes and membranes alone were
incubated in solution with the anti-CA antibody (500 µl; 0.3 g/L) for
30 min, after which the antibody/his-MoCA/membrane complexes were pelleted by a second ultracentrifugation and were suspended in IPB
buffer. For protein analysis, samples were subjected to
SDS-polyacrylamide gel electrophoresis (SDS-PAGE), and gels were
electroblotted onto a nitrocellulose filter. Gag proteins were
immunodetected with the mouse anti-CA antibody Hy187, which was
revealed by using an alkaline phosphatase-conjugated anti-mouse
antibody at 1:12,550 dilution, followed by a color reaction (Hansen et
al., 1993
). The secondary antibody plus color reaction steps also
revealed nitrocellulose-bound anti-CA heavy and light chains from the
incubations described above.
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RESULTS |
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Preparation and analysis of lipid vesicles
Retrovirus particles have proved somewhat intractable to
structural analysis, as they are enveloped with a cellularly derived lipid bilayer and are heterogeneous in size and shape (Fuller et al.,
1997
; Yeager et al., 1998
). Because of this, we designed a method for
the analysis of how the major structural (Gag) proteins of the Moloney
murine leukemia virus (M-MuLV) organize on membranes in immature virus
particles (Barklis et al., 1997
). Briefly, N-terminally his-tagged Gag
protein derivatives assembled on monolayers containing the
nickel-chelating lipid DHGN can be lifted onto electron microscope grids and analyzed by transmission EM (see Fig. 1). This model system
is faithful in that in vitro assembly occurs on a membrane, with the
his-tag/DHGN interaction substituting for the membrane-anchoring function of a myristate group, which modifies the M-MuLV Gag protein amino-terminus in vivo (Rein et al., 1986
).
To complement EM analyses, we decided to adapt our system for analysis
of membrane-bound Gag proteins under buffer solution by AFM. Initially,
we attempted to transfer monolayers onto octadecyl-silanized mica and
glass substrates. Silanization was by octadecyltrichlorosilane treatment of cleaned glass or freshly cleaved mica surfaces (Egger et
al., 1990
). However, silanization of mica appeared incomplete, and
hydrophobic glass substrates were suboptimal for AFM as a consequence
of poor monolayer transfer and rapid loss of image quality during AFM
scanning with silicon nitride
(Si4N4) tips (data not shown).
As an alternative to monolayer lifts, and to mimic cellular plasma
membranes, we next opted to prepare
Ni2+-DHGN-containing lipid bilayers as Gag
protein assembly targets. Unilamellar vesicles were prepared by
sonication of dried lipids to final lipid concentrations of 500 µM PC
and 50 µM Ni2+-DHGN (see Materials and
Methods). Vesicles so prepared were processed by 4 h of adsorption
on freshly cleaved mica, followed by two gentle rinses with water and
then viewing buffer. Samples then were imaged under viewing buffer with
an oxide-sharpened Si4N4 tip at 2.0 Hz in contact mode (Fig. 2).
After 4 h of adsorption to mica, vesicles appeared to be intact
but heterogeneous in size, with diameters from 100 nm to 500 nm (Fig. 2
a). Heights ranged from 7.3 to 7.6 nm, with an occasional
measurement of approximately twice that height (Fig. 2 b, left
side). In this regard, because of strong elasticities observed for
these samples, it is noteworthy that imaging was only possible by
application of 5-10-nN forces. Given these high scan forces and
assuming a bilayer thickness of 4-5 nm (Simon and McIntosh, 1984
;
Sackmann, 1983
), our average apparent height of 7.5 nm is consistent
with those of flattened, unilamellar vesicles, while higher features
may result from the stacking of two vesicles. While 4-h preparations
appeared as flattened but elastic vesicles, after aging of
substrate-bound vesicle preparations overnight, AFM imaging could be
achieved with scan forces below 1 nN and lipids spread over areas of
200-1000 µm in diameter (Fig. 2 c). The heights of such
areas were relatively constant at 3.1 ± 0.2 nm (Fig. 2
d), within the expected range of lipid bilayers in a fluid
state and imaged by AFM (Mou et al., 1995
). These observations suggest
that initially substrate-bound vesicles converted to single bilayers
after overnight incubations and are consistent with previous observations (Mou et al., 1994
).
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EM imaging of bilayer-bound M-MuLV capsid protein two-dimensional arrays
As noted above, while lipid bilayers could be imaged conveniently
by AFM (Fig. 2), monolayer imaging gave poor results. Consequently, any
AFM images of membrane-bound proteins we hoped to obtain would have to
be compared with EM images of lipid bilayer-bound proteins, rather than
the monolayer-associated protein images obtained previously (Barklis et
al., 1997
). Because of this, we undertook the EM analysis of his-tagged
M-MuLV capsid (his-MoCA) proteins bound to lipid bilayers. To do so,
optimization experiments were undertaken. In agreement with previous
data (Barklis et al., 1997
), optimal conditions involved incubation in
50 mM sodium phosphate (pH 8.3), 5 mM sodium acetate, 10 mM imidazole,
250 mM NaCl, 20% glycerol (PNG buffer), using a PC:Ni-DHGN ratio of
10:1. We also observed that array formation was optimal
at a lipid-to-protein concentration ratio of 10:1 (250 µM
lipid:25 µM his-MoCA), slightly lower than the ratio predicted
assuming a lipid surface area of 70 Å2/molecule
(Schmitt et al., 1994
; Mingotaud et al., 1993
) versus 910 Å2/molecule for a his-MoCA monomer (Barklis et
al., 1997
).
Using the above conditions in overnight, 30°C incubations,
crystalline his-MoCA arrays made on vesicles were apparent by EM of
negatively stained samples. As shown in Fig.
3 a, vesicle incubations in
the presence of his-MoCA resulted in the appearance of large membranes
with extensive his-MoCA crystalline arrays, which were more obvious at
higher magnification (Fig. 3 b). A number of calculated diffraction patterns from such arrays were twinned, possibly resulting from arrays formed on opposite sides of a vesicle or from separate but
adjacent crystals. However, frequently untwinned patterns were
observed, as in Fig. 3 c. The diffraction patterns (Fig. 3
c) could be indexed in either a hexagonal (a* = b* = 0.0142 Å
1,
* = 60°) or
orthogonal (a* = 0.0123 Å
1,
b* = 0.0074 Å
1,
* = 90°)
fashion, with reflections (not visible in Fig. 3 c) out to
25.4 Å (orthogonal reflection 1, 5), similar to what we have obtained
with negatively stained monolayer arrays. Averaging of eight untwinned
diffraction patterns indexed in an orthogonal fashion yielded a mean
unit cell of a = 81.5 ± 0.3 Å, b = 135.3 ± 1.8 Å, and
= 89.1 ± 1.4°, while the
corresponding hexagonal unit cells were a = 81.2 ± 0.5 Å, b = 79.6 ± 1.7 Å,
= 117.9 ± 1.5° (see Table 1). As shown in Table
1, his-MoCA proteins formed arrays that were consistent with hexagonal
(p6) space group symmetry, giving an average phase residual of
18.1 ± 4.5° to 15-Å resolution. Phase residual values for
trigonal (p3) symmetry calculations were slightly better than those for
the p6 space group (13.5 ± 5.2 at 15-Å resolution; Table 1),
suggesting that it may be a more appropriate space group designation
for his-MoCA crystals; implications with regard to protein packing will
be discussed below (see Discussion).
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Comparison of calculated diffraction patterns of bilayer-bound
his-MoCA, assuming no symmetry constraints (p1), showed good agreement
between images, with phase residuals less than 30° at 26 Å or lower
(Table 1). Back-transformation of unbent, filtered diffraction patterns
resulted in 2D projection reconstructions, as shown in Fig.
4, A-C. As illustrated, the
M-MuLV capsid protein assembled into cage-like structures on
PC/Ni2+-DHGN bilayers. On inspection, there
appeared to be distinct types of protein-free cage holes
(dark), which were surrounded by six electron-dense
(white) units, apparently representing protein monomers.
Reconstructions showed two or three types of cage holes (numbered
in A-C). In all panels, the no. 1 cage holes appeared distinct,
as observed previously (Barklis et al., 1997
). However, it was unclear
whether the no. 2 and no. 3 holes were distinct, as predicted by p3
symmetry, or similar, consistent with p6 symmetry (see Discussion). In
any case, each cage hole was spaced 45.5 Å from its nearest-neighbor
cage holes, and spacings between putative distinct cage hole types
(Fig. 4, A-C, 1 to 1, 2 to 2, and 3 to 3) were
81.5 Å. These distances are consistent with those observed for M-MuLV
capsid proteins assembled on lipid monolayers (Barklis et al., 1997
),
as well as the apparent spacing of PrGag proteins in immature M-MuLV
particles (Yeager et al., 1998
).
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AFM imaging of his-MoCA bound to lipid bilayers
Based on our imaging of lipid membranes by AFM (Fig. 2), we opted
to image his-MoCA proteins on lipid bilayers. To do so, his-MoCA
proteins were incubated overnight at 30°C with
PC/Ni2+-DHGN vesicles, deposited on mica or
highly oriented pyrolytic graphite (HOPG), and imaged under 20 mM
TrisHCl, 200 mM KCl (pH 8.0). Scanning was performed in contact mode
with a Nanoscope III fluid cell, operated without the O-ring, employing
200-µm-long oxide-sharpened
Si4N4 tips, with nominal
spring constants of 0.06 N/m. After tip engagement, to locate membrane
areas, slow scans (2 Hz) were performed on 1-25
µm2 areas. As illustrated (Fig.
5 a), bilayer areas as large
as several hundred nanometers to microns were observed. In contrast to
bilayers composed only of lipid (Fig. 2 c), areas of
his-MoCA- bound bilayers (Fig. 5 a) revealed features as
tall as 8.5-10.6 nm, consistent with membrane heights of 3.0-4.0 nm
plus M-MuLV capsid protein heights of ~6 nm. Slight differences
between height measurements made on different dates may be related to
the utilization of different tips, which yielded different compression
forces on the membrane. At higher topologies, his-MoCA-bound membranes
(Fig. 5 c) showed patches of arrays, comprising apparent
0.33 ± 0.06 nm depressions spaced at ~8.0-nm intervals, and
calculated diffraction patterns (Fig. 5 d) demonstrated an
apparent sixfold symmetry (two reflections are obscured by the
y axis), corresponding to a unit cell of a = b = 7.9 nm,
= 60°.
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The his-MoCA arrays as imaged by AFM (Fig. 5) did not yield crystals
that were compatible with conventional 2D diffraction analysis.
However, it was possible to perform real space averaging operations
using the SPIDER suite of image reconstruction programs (Frank et al.,
1988
). To do so, 12 140.6 × 140.6 Å2
windows were added from low-pass filtered images to yield a
cross-correlation reference image, which was used to identify the top
100 cross-correlation peaks from his-MoCA AFM scans. After this step,
the corresponding 187.5 × 187.5 Å2 image
areas from unfiltered scans were added to give an averaged AFM image of
membrane-bound his-MoCA proteins. As illustrated (Fig.
6), the topology of the bilayer-bound
proteins shows a lattice of higher features surrounding shallow
depressions spaced at 7.9-nm distances, reminiscent of hole-to-hole
spacing between similar cage holes from EM micrographs (Fig. 4). The
quality of our AFM reconstruction was assessed by halving our data set,
generating two independent reconstructions, and comparing the averaged
images with each other by determination of Fourier ring correlation
(FRC) values. By this method, we found FRC values dropped from 0.93 (highly correlated) to 0.53 at 0.032 Å
1,
yielding a practical resolution limit of ~31 Å.
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Quantification of MoCA bound to membrane.
Although the above AFM results clearly showed the existence of a
cage-like lattice, it was unclear whether the lattice corresponded to
the protein or lipid sides of his-MoCA bound membranes. To disciminate
between these possibilities, we tested whether his-MoCA proteins (Fig.
7, lane 1) on substrate-bound
membranes were accessible to binding by the anti-MoCA monoclonal
antibody Hy187 (Fig. 7, lane 2; Hansen et al., 1993
). For
these experiments, we prepared PC/Ni2+-DHGN
vesicles and PC/Ni2+-DHGN vesicles with bound
his-MoCA proteins (his-MoCA vesicles). Not surprisingly, while 35-kDa
his-MoCA proteins in his-MoCA vesicles were pelleted by centrifugation
(Fig. 7, lane 3), free his-MoCA proteins were pelleted much
less efficiently (Fig. 7, lane 6). Also, as expected, the
50-kDa and 25-kDa heavy and light chains of the anti-MoCA antibody
bound well to his-MoCA containing vesicles (lane 4) but not
nearly as well to the naked PC/Ni2+-DHGN vesicles
(lane 5). Analysis of the orientation of his-MoCA proteins
on substrate-bound bilayers involved binding reactions on HOPG, which
served as a substrate for our AFM studies on his-MoCA arrays (Fig. 5).
Our procedure involved binding proteins or vesicles to HOPG,
postbinding steps with anti-MoCA, and detection of his-MoCA and
anti-MoCA proteins by electrophoresis and immunoblotting after release
from the HOPG substrate. As indicated in Fig. 7, the free his-MoCA
protein has some capacity for binding to HOPG by itself (lane
10), while his-MoCA vesicles appeared to bind quite efficiently to
HOPG (lane 9). Significantly, anti-MoCA, which bound well to his-MoCA vesicles in solution (lane 4), bound poorly to
substrate-bound his-MoCA vesicles (lane 9). Indeed, while
the amount of substrate-bound anti-MoCA in lane 9 exceeded the level of
direct anti-MoCA binding to HOPG (lane 11), it was
approximately equal to the amount that adhered to HOPG-bound
PC/Ni2+-DHGN vesicles (lane 12).
Furthermore, on a proportional basis, the amount of anti-moCA bound to
HOPG via his-MoCA vesicles (lane 9) appeared to be much
reduced relative to the level of anti-MoCA bound via free his-MoCA to
HOPG (lane 13). These results indicate that membrane-bound
his-MoCA proteins on AFM supports were not readily accessible to
antibody binding and thus imply that these retroviral Gag proteins were
sandwiched between PC/Ni2+ DHGN membranes and
HOPG substrates during AFM imaging.
|
| |
DISCUSSION |
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|
|
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Moloney murine leukemia virus, like its C-type retrovirus
conterparts, assembles at the plasma membranes of infected cells, and
the expression of the M-MuLV Gag polyprotein is sufficient for the
assembly of immature virus particles. Normally, during or after
budding, cleavage of the Gag proteins by the viral protease results in
a morphological change from an immature to a mature virus form (Coffin
et al., 1997
). Recent cryo-EM studies of immature retrovirus particles
have shown that Gag polyproteins associate to form paracrystalline
sheets, but the subsequently formed spherical virus shells apparently
lack icosahedral symmetry (Fuller et al., 1997
; Yeager et al., 1998
).
Unfortunately, natural retrovirus particle pleomorphism and
difficulties in preparation of homogeneous virus preparations have
hampered the analysis of immature and mature retrovirus particles
(Nermut et al., 1994
; Fuller et al., 1997
; Yeager et al., 1998
). To
circumvent the above difficulties, we designed a model system for the
study of the assembly of Gag proteins on the face of a lipid membrane
(Barklis et al., 1997
, 1998
). The approach employs a his-tagged
retrovirus capsid domain and membranes consisting of PC and a
nickel-chelating lipid, DHGN. Here, we have focused on the M-MuLV
capsid domain because it mediates critical Gag-Gag contacts, and it is
not sensitive to proteolysis.
As observed in monolayer experiments (Barklis et al., 1997
), his-tagged
Gag proteins formed regular arrays on
PC/Ni2+-DHGN vesicles (Fig. 3). Diffraction
analysis indicated that vesicle-bound his-MoCA proteins formed
consistent, 2D crystals (Table 1). Two-dimensional projection
reconstruction shows that the proteins formed cages composed of cage
holes spaced at 45-46-Å intervals (Fig. 4), in agreement with studies
on immature M-MuLV particles (Yeager et al., 1998
). The appearance of
reconstructions suggests that the no.1 holes in Fig. 4,
A-C, are hexagonally symmetrical, consistent with a p6
space group assignment. However, if slight differences in no. 2 and no.
3 holes are verified in future, higher resolution studies, the lower
symmetry p3 assignment may prove more appropriate.
Assuming a p6 packing arrangement, Fig. 8
A shows a model for M-MuLV capsid protein assembly at a
membrane. This model shows hexagonal and trigonal cage holes, each
surrounded by six CA monomers. Features of the model are that it
accounts for p6 symmetry, and head-to-head CA homodimers (Gamble et
al., 1997
; shown as hexagon pairs joined by no. 4-no. 4 interfaces)
and CA surfaces (idealized as numbers on hexagons) occupy constant
positions within the network. An alternative model, which allows for
three different types of cage holes, is shown in Fig. 8 B.
The model is compatible with p3 symmetry, but does not directly account
for the existence of head-to-head dimers (Gamble et al., 1997
);
requires that CA subdomains must fulfill two different roles (as where
hexagon no. 1 and no. 2 faces both form dimer interfaces and cage hole
edges); and presents an ambiguous assembly pathway.
|
In comparison with EM results, AFM analyses gave similar yet slightly
different results (Figs. 5 and 6). For AFM studies, we found that
his-MoCA-bound PC/Ni2+-DHGN vesicles adhered to
subtrates to yield image heights of 8.5-10.6 nm (Fig. 5), consistent
with a lipid bilayer height of 3.0-4.0 nm, plus a his-MoCA layer
height of ~6 nm. As demonstrated in Fig. 7, the his-MoCA layer
appeared inaccessible to antibody probing, supporting the notion that
his-MoCA proteins were sandwiched between bilayers and substrates
during AFM imaging. Our observations suggest that his-MoCA-decorated
vesicles adhered to supports by protein-substrate binding, followed by
vesicle breakage, and inside-up bilayer unrolling, a hypothesis that is
consistent with previous results (Mou et al., 1994
) and our own
observations with PC/Ni+2-DHGN vesicles (Fig. 2).
Although his-MoCA proteins appeared to be covered by bilayers during
AFM analyses, by using moderate (0.5 nN) force with low spring constant
(0.06 N/m) cantilevers it was possible to image membrane-bound arrays
under buffer (Fig. 5). Under these conditions, proteins would not be
expected to be imaged directly. Rather, bilayer regions supported by
proteins would appear as higher features, while membrane regions that
covered protein-free regions of his-MoCA cages could be deformed by tip forces, appearing as depressions. In contrast to EM results (Fig. 4),
we found that the membrane surfaces of his-MoCA arrays showed evidence
of only one type of cage hole. Specifically, shallow depressions of
0.33 ± 0.06 nm were observed to be spaced at 7.9-nm hole-to-hole distances (Figs. 5 and 6).
Because AFM images show surface topologies and EM images represent 2D
projections of electron densities, there are numerous ways in which AFM
and EM results can be reconciled. However, other observations reduce
the number of possible models. Notably, CA proteins are composed of two
domains (Fuller et al., 1997
; Yeager et al., 1998
; Gitti et al., 1996
),
and cage holes appear to be formed by hexamer rings (Barklis et al.,
1997
, Fig. 4). Given these results and making the assumption that AFM
cage hole positions correspond to one type of EM cage hole, models must
explain how one type of cage hole appears to be more electron dense
than the others, while two-thirds of the cage holes are supported well enough to resist deformation by AFM tips. One model that satisfies the
above restrictions is depicted in Fig. 8 C. As shown, each CA monomer is modeled as a hockey stick or golf club, with the club
ends adjacent to lipid monolayers. Club heads point away from one type
of cage hole (Fig. 8 C, 1, 2) and toward the other holes (an
example is shown in Fig. 8 C3). While the model obviously remains hypothetical, several of its implications are pertinent for
consideration. In particular, the two domains of CA monomers interact
most closely with different partners in membrane-bound arrays.
Moreover, while membrane-bound his-MoCA EM projections show cages with
two or three hexamer types (Figs. 4 and 8), our model, with slight
adjustment, is consistent with the hexamer-trimer cages that HIV capsid
proteins form on monolayers (Barklis et al., 1998
). Furthermore, the
arrangement shown implies that the cytoplasmic tails of M-MuLV envelope
protein trimers, which penetrate immature M-MuLV cores, would do so via
one type of cage hole, suggesting a maximum of one Env protein trimer
per six PrGag monomers. We are currently testing
these predictions and implications in vivo and in vitro.
| |
ACKNOWLEDGMENTS |
|---|
We thank Jason McDermott, Sonya Karanjia, and Doug Huseby for helpful discussions, and we are indebted to one of our manuscript reviewers, whose patient advice improved the accuracy and interpretation of our data.
This research was supported by a grant from the National Institutes of Health (5R01 GM 52914) to EB and fellowship support to GZ from the Association pour la Recherche sur le Cancer (ARC) and the Human Frontier Science Program Organization.
| |
FOOTNOTES |
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Received for publication 10 November 1998 and in final form 20 September 1999.
Address reprint requests to Dr. Eric Barklis, Vollum Institute and Department of Microbiology, Oregon Health Sciences University, 3181 S.W. Sam Jackson Park Road, Portland, OR 97201-3098. Tel.: 503-494-8098; Fax: 503-494-6862; E-mail: barklis{at}ohsu.edu.
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REFERENCES |
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Biophys J, January 2000, p. 373-384, Vol. 78, No. 1
© 2000 by the Biophysical Society 0006-3495/00/01/373/12 $2.00
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