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Subunit Folds and Maturation Pathway of a
dsRNA Virus Capsid
Article in Structure · July 2013
DOI: 10.1016/j.str.2013.06.007 · Source: PubMed
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Structure
Article
Subunit Folds and Maturation Pathway
of a dsRNA Virus Capsid
Daniel Nemecek,1,3,7 Evzen Boura,2,4,7 Weimin Wu,1 Naiqian Cheng,1 Pavel Plevka,3,5 Jian Qiao,6 Leonard Mindich,6
J. Bernard Heymann,1 James H. Hurley,2 and Alasdair C. Steven1,*
1National
Institute of Arthritis and Musculoskeletal and Skin Diseases
Institute of Diabetes and Digestive and Kidney Diseases
National Institutes of Health, 50 South Drive, Bethesda, MD 20892, USA
3Central European Institute of Technology, Masaryk University, Kamenice 5, 62500 Brno, Czech Republic
4Institute of Organic Chemistry and Biochemistry AS CR, v.v.i., Flemingovo nam. 2, 166 00 Prague 6, Czech Republic
5Department of Biological Sciences, Purdue University, 915 W. State Street, West Lafayette, IN 47907, USA
6Department of Microbiology, Public Health Research Institute Center, University of Medicine and Dentistry of New Jersey, 225 Warren Street,
Newark, NJ 07103, USA
7These authors contributed equally to this work
*Correspondence:
[email protected]
http://dx.doi.org/10.1016/j.str.2013.06.007
2National
SUMMARY
The cystovirus f6 shares several distinct features
with other double-stranded RNA (dsRNA) viruses,
including the human pathogen, rotavirus: segmented
genomes, nonequivalent packing of 120 subunits in
its icosahedral capsid, and capsids as compartments for transcription and replication. f6 assembles as a dodecahedral procapsid that undergoes
major conformational changes as it matures into
the spherical capsid. We determined the crystal
structure of the capsid protein, P1, revealing a flattened trapezoid subunit with an a-helical fold. We
also solved the procapsid with cryo-electron microscopy to comparable resolution. Fitting the crystal
structure into the procapsid disclosed substantial
conformational differences between the two P1 conformers. Maturation via two intermediate states involves remodeling on a similar scale, besides huge
rigid-body rotations. The capsid structure and its
stepwise maturation that is coupled to sequential
packaging of three RNA segments sets the cystoviruses apart from other dsRNA viruses as a dynamic
molecular machine.
INTRODUCTION
Double-stranded RNA viruses have a wide host range, including
animals, plants, fungi, and bacteria, but share a number of
distinct properties (Patton, 2008). Their genomes comprise multiple (up to 12) linear segments and are typically accommodated
in multiple nested protein shells (capsids). After cell entry, the
genome remains inside the innermost capsid that also houses
the viral RNA-dependent RNA polymerase. This particle functions as a replication machine or polymerase complex where
mRNAs are transcribed and secreted. Related particles, called
procapsids, are formed early in the assembly of next-generation
virions. They package single-stranded RNA (ssRNA) segments,
synthesize second strands, and finally transcribe. The overall
architecture of these inner capsids is similar in all doublestranded RNA (dsRNA) viruses, consisting of 120 copies of a
major capsid protein organized in a T = 1 icosahedral shell built
from 60 dimers of nonequivalent subunits. An important and still
unanswered question is: How is a single copy of each segment
selected and packaged?
High-resolution structures have been determined with X-ray
crystallography and cryo-electron microscopy (cryo-EM) for
the inner capsids of several dsRNA viruses, including several
reoviruses (Grimes et al., 1998; Nakagawa et al., 2003; Reinisch
et al., 2000), birnaviruses (Coulibaly et al., 2005), picobirnaviruses (Duquerroy et al., 2009), and totiviruses (Naitow et al.,
2002). Except for birnaviruses, the shell is formed by 60 dimers
of nonequivalent subunits, denoted A and B, an architecture
encountered in no other virus family. Twelve pentamers of
A-subunits are centered on the 5-fold vertices and 20 trimers
of B-subunits on the 3-fold axes. Although both subunits have
identical sequences and similar folds, they tend to differ somewhat in local features and radically in intersubunit interactions
(Grimes et al., 1998; Jäälinoja et al., 2007; Nakagawa et al.,
2003; Reinisch et al., 2000).
Cystoviridae are the only family of dsRNA viruses that infect
bacteria. They were also the first dsRNA viruses for which
reverse genetics has been developed (Mindich, 1999a, 1999b;
Olkkonen et al., 1990), an asset that commended them as a
model system for studying assembly and replication of dsRNA
viruses. In consequence, much biochemical and genetic data
have been collected concerning their replication cycle (Frilander
and Bamford, 1995; Mindich, 1999a; Poranen and Bamford,
2012).
Bacteriophage f6, the type member of the Cystoviridae,
initially assembles as an RNA-free procapsid with deeply recessed vertices, giving it a dodecahedral morphology (Butcher
et al., 1997). The procapsid accommodates the polymerase
(P2) and an accessory protein (P7), which has a regulatory function in assembly and RNA packaging (Poranen et al., 2008). P2 is
bound to the inner surface of the procapsid (Nemecek et al.,
2010; Sen et al., 2008) at sites close to the 3-fold axes that
Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved 1
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
Table 1. Crystallographic Statistics
Space Group
C 2221
Cell dimensions (Å)
a = 182.59
b = 278.85
c = 246.47
X-ray source
SER-CAT 22 ID
Wavelength (Å)
0.97899
Resolution (Å)
3.60 (3.66–3.60)
Total reflections
1,043,858
Unique reflections
66,561
I/s(I)
11.15 (2.04)
Data completeness (%)
91.07 (41.67)
Multiplicity
15.7 (2.3)
Rwork (%)
21.7
Rfree (%)
27.4
Rmerge (%)
19.2
Rmsd bond angle deviation ( )
1.41
Rmsd bond length deviation (Å)
0.008
Ramachandran favored (%)
95.0
Ramachandran outliers (%)
0.03
Number of non-hydrogen atoms
29,435
Rmsd, root-mean-square deviation.
overlap those occupied by P7 (Nemecek et al., 2012; Sun et al.,
2012). On the outer surface of the procapsid, hexamers of the
packaging NTPase (P4) overlie the 5-fold vertices (de Haas
et al., 1999; Pirttimaa et al., 2002).
Packaging of the three ssRNA segments proceeds in order
from the shortest segment (s, 2,948 nt) to the m-segment
(4,063 nt) and finally the l-segment (6,374 nt; Mindich, 1999a).
Packaging is accompanied by a major structural transformation
that yields the spherical mature capsid, with a net volume increase of 250%. It has been proposed (Mindich, 1999a) that
the transformation proceeds stepwise, sequentially exposing
binding sites for each RNA segment on the outer surface of the
maturing procapsid. A binding site for the s-segment has been
localized to the region between amino acids 98 and 155 of P1
by crosslinking (Qiao et al., 2003b). In support of this scenario,
two expansion intermediates have been observed (Nemecek
et al., 2011). The shell conformation also controls the activity of
the polymerase P2 that begins to synthesize second (minus)
RNA strands only after all three segments are packaged
(Frilander et al., 1992).
The present study has aimed to gain insight into the mechanisms that control assembly, maturation, and functioning
of the polymerase complex. To do so, we set out to crystallize
P1 and complemented this approach with cryo-EM and
image reconstruction of the procapsid. Both approaches
succeeded. Then by fitting the crystal structure into cryo-EM
density maps, we were able to characterize the structural
alterations undergone by P1 as it adapts to the P1A and P1B
conformations. Applying the same approach to earlier reconstructions of the mature capsid (Huiskonen et al., 2006) and
two expansion intermediates (Nemecek et al., 2011), we were
able to follow the molecular rearrangements that occurred
during maturation. From these models, we could identify
a positively charged cavity that is open on the procapsid
and likely to bind the s-segment but closed and therefore
inaccessible in the expansion intermediates and mature
capsid, observations consistent with the sequential packaging
hypothesis.
RESULTS
Crystallization of P1
Our initial crystallization trials with monomeric P1 produced
crystals but they diffracted only to 6 Å. Later, a mixture of
P1 and P7 yielded crystals diffracting to 3.6 Å. Because they
could not be separated from a film of denatured protein, we
were unable to determine whether they also contained P7.
Nevertheless, they sufficed to solve the structure of P1.
Because the self-rotation function suggested a pentamer in
the asymmetric unit, we used the P1 pentamer from an earlier
cryo-EM map at 7 Å resolution as a search model for molecular
replacement. Phases were extended to 3.6 Å, using noncrystallographic symmetry (Table 1). In the resulting density map (Figure S1A available online), the entire P1 subunit was well ordered
except for a few C-terminal residues and it was possible to
trace the whole Ca chain and almost all side chains (e.g., Figure S1B), apart from several flexible Arg and Lys residues. We
did not find any density attributable to P7 but cannot rule out
that P7 was present at low occupancy or in a disordered state
and somehow promoted P1 assembly into pentamers or stabilized a conformation that allowed the growth into well-ordered
crystals.
P1 Has an a-Helical Fold
The P1 subunit (Figure 1B) has a trapezoid shape with sides of
91 Å 3 73 Å. The thickness varies between 14 Å and 38 Å at
the edges, reaching 47 Å at the center. The structure is mostly
a-helical (46% of residues; Figures S1C and S1D), in agreement
with Raman spectroscopy data (Benevides et al., 2002) and
cryo-EM reconstructions at 7 Å resolution that resolved many
rod-like densities—putatively a helices—in both the procapsid
(Nemecek et al., 2012) and the nucleocapsid (Huiskonen et al.,
2006). We found no similar fold—and in particular, no similar
capsid protein fold—when using the DALI server (Holm and
Rosenström, 2010).
The N terminus forms a ‘‘latch’’ over two helices located in the
middle of the structure (blue in Figure 1B). This is followed by a
long loop connected to the ‘‘tip’’ region, featuring six a helices.
The next part is a set of four helices forming the ‘‘corner’’ of
the trapezoid. The central part of the polypeptide chain is
composed of long extended loops interspersed with a few helices. This region largely separates the N- and C-terminal thirds.
Finally, the C-terminal part starts with a two-strand b sheet forming a protruding hairpin (yellow in Figure 1B). This is followed by a
long helix-loop-helix (the ‘‘lever’’), three helices denoted the
‘‘anchor,’’ and the C-terminal helix and loop. These C-terminal
helices form an interface that maps to the P1B subunits in
the procapsid where a large ‘‘hinge’’ motion contributes to the
expansion of the shell (see below). The hinge region also interfaces the P1A to the P1B subunits around the rim of the P1A
pentamer (Figure 2A).
2 Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
Figure 1. Crystal Structure of P1
(A) Top and side views of the funnel-shaped P1 pentamer (the five subunits are in different colors).
(B) The P1 subunit (rainbow-colored from blue at the N terminus to red at the C terminus) has a trapezoid shape with four edges labeled I–IV. The long helix-turnhelix (in gold) forms a ‘‘lever’’ that rotates during maturation of the procapsid. Five copies of the ‘‘tip’’ line the axial channel through the pentamer. The ‘‘corner’’ of
one pentamer subunit fits against the ‘‘anchor’’ of a neighboring subunit.
See also Figure S1.
To describe the intersubunit interfaces in the procapsid
(below), we designate the four edges of the trapezoid as I–IV (Figure 1B). Only edges I and II are involved in intersubunit interactions in the crystallized pentamer (Figure 1A), and they show
good complementarity of positive and negative residues. The
buried surface at this interface is 9,248 Å2, suggesting a very
stable pentamer.
Expression of Quasi-Equivalence in the Procapsid
We determined the procapsid structure by cryo-EM to a resolution of 4.5 Å (Box 1). The features visualized, such as regular
helical grooves on a helices, separation of loops and b strands,
and densities for bulky side chains, validate the calculated resolution (Figure S2). With some discrepancies (see below), the
crystal P1 pentamer fits snugly into the P1A pentamer, and
the P1 monomer could be placed into the P1B-related density
without ambiguity. The molecular boundaries (Figure 2A) agree
with those inferred from previous cryo-EM maps of the nucleocapsid (Huiskonen et al., 2006) and the procapsid (Nemecek
et al., 2012). Each edge of the trapezoid forms two different interfaces with other P1 subunits. In the P1A pentamer, edges I
and II are apposed. Edge II in P1B fits across two edges from
different P1A subunits (one an edge III and the other an edge
IV). The P1B edges I and IV constitute the intratrimer interfaces
around the 3-fold axis. At the 2-fold axis, the apposing P1B edge
III meet to form the major hinge involved in expansion (see
below).
We performed flexible fitting of crystal P1 into the P1A density.
The quality of the density in the cryo-EM map gave confidence in
the reliability of the results. Overall there is good correspondence
but with significant differences that reflect adaptation of the protein conformation to the context of the procapsid. The largest difference is in the hinge region, where four helices (H24, H25, H28,
and H29) are rotated (by 18 ) to accommodate the adjacent
P1B in the procapsid (Figure 3B). The C-terminal helix is also
shifted, positioning the C terminus of P1A into a hydrophobic
groove in the neighboring P1B subunit.
In P1B, on the other hand, the hinge region and the C-terminal helix are essentially the same as those in crystal P1, as
are the loops and helices at the II–IV interface with the adjacent
P1B subunit. The most pronounced differences in P1B affect the
tip region at the interface with P1A (Figure 3C). Here, two helices are rotated through 27 and 9 , respectively, to accommodate displacement of loops at the P1A/P1B interface.
Changes in P1 during Capsid Maturation
Procapsid maturation during RNA packaging involves massive
conformational changes and accompanying changes in size
and shape (cf. Figures 3A and 3D). To determine the changes
in the conformations and interactions of P1A and P1B subunits,
we performed flexible fitting with crystal P1 into a nucleocapsid
map at 7.5 Å resolution (Electron Microscopy Data Bank [EMDB]
ID: emd1206; Huiskonen et al., 2006; Figures 3E and 3F). This
exercise showed that the principal mechanism has large-scale
Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved 3
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
Figure 2. Cryo-EM Reconstruction of the f6
Procapsid
(A) Segmentation of the outer surface viewed
along a 5-fold axis. The 12 inverted 5-fold vertices
are occupied by P1A pentamers (the five subunits
are in shades of blue) set in a dodecahedral frame
of 60 P1B subunits (red, except for the three subunits around one 3-fold axis, which are in shades
of yellow).
(B) Density for one a helix (left) and two b strands
with the corresponding atomic model (side chains
are shown for the a helix only, for clarity).
(C) Slices through the cryo-EM reconstruction
viewed along the 5-fold axis at 20 Å (left) and 40 Å
(right) from the procapsid center. Elongated
densities representing a helices that are approximately in-plane are indicated by arrows and
enlarged in the right panels. Scale bar: 100 Å.
See also Movie S2.
hinging movements around intersubunit interfaces (Figure 4).
The accompanying conformational changes, mainly affecting
P1B, are on the same order as those that distinguish procapsid
subunits from crystal P1. In P1A, the greatest change is in the
long b-hairpin and underlying helices of the anchor that tilt
through 20 (Figure 3E). Interactions with neighboring subunits
also change; e.g., the long helix-turn-helix (the lever) is no longer
connected to the neighboring P1B subunit by the Arg655 salt
bridge.
During expansion, adjacent P1B subunits rotate around a
‘‘pivot’’ axis connecting the 3-fold axes through the 2-fold axis
(Figures 4A and 4B). The planes of the two subunits meet at an
angle of 98 in the procapsid, changing to 148 in the nucleocapsid (Figures 4C and 4D). This movement results in much
larger buried surfaces for both subunits (50% increase for
P1B and 16% for P1A) and a better match of complementary
charged residues. At the intramolecular level, the lever shifts
away from the 2-fold icosahedral axis and is further tilted 25
within the subunit, pointing toward the b-hairpin in the apposing
P1B subunit (arrows in Figures 4C and 4D; Movie S2). Concomitantly, the hydrophobic C terminus is moved into the uncharged
groove in the opposing P1B subunit.
Staging Posts in the Expansion Reaction
We also had available two expansion intermediates at lower
resolution (18 Å; EMDB IDs: 5355 and 5357). With them, we performed rigid-body fitting, using the P1A and P1B conformations of
both the procapsid and the mature capsid. In both particles, the
best fits were obtained with P1A in its procapsid conformation
and P1B in its nucleocapsid conformation.
Figure 5 and Movie S3 show the sequence
of transitions, starting with the compact
procapsid and expanding to the almost
spherical mature capsid and a markedly
thinner P1 shell. The large change in the
hinge region occurs mainly in the first transition from the procapsid to expansion intermediate 1, which has the lowestenergy state of the P1 shell (not the fully
mature shell; Nemecek et al., 2011). Subsequent changes in
the expansion involve smaller rearrangements, mainly around
the hinge and tip regions.
DISCUSSION
Cystoviruses are of interest as dsRNA viruses that provide tractable experimental systems. The molecular composition and
assembly of the procapsid have been studied extensively, and
high-resolution structures have been determined for three of its
four proteins: the P2 RNA-dependent RNA polymerase of f6
(Butcher et al., 2001), the P4 packaging motor of f12 (Mancini
et al., 2004), and the P7 packaging facilitator of f12 (Eryilmaz
et al., 2008). Here we complete the ensemble with the structure
of P1 from f6 and show how the procapsid serves as a framework to which the other three proteins bind and how it transforms
during maturation.
We detected no similarity of the P1 fold with the known folds of
the capsid proteins of other dsRNA viruses. To the extent that the
capsid protein fold may be viewed as a hallmark of common
ancestry (Bamford et al., 2005), this distinction would suggest
that cystoviruses originated in a different lineage than other
dsRNA viruses. P1 does share with them the distinctive,
nonequivalent, 120-subunit capsid geometry but the in-plane
shapes of the subunit and of the pentamer of A-subunits, which
is quite pentagonal in the case of f6, are markedly different between the respective systems.
Another property that sets cystoviruses apart from other
dsRNA viruses is the large-scale conformational changes that
4 Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
would also suggest that the other dsRNA viruses select their
complements of segments for packaging by a different
mechanism.
Box 1. Single Particle Analysis: Statistics
Number of Micrographs
154
Number of particle images
28,194 (65% used)
Defocus range (mm)
1.3–3.2
FSC0.3 (Å)
3.9
FSC0.5 (Å)
4.4
occur during maturation. In this respect, they are more akin to
the capsids of tailed bacteriophages (Conway et al., 2001;
Gertsman et al., 2009; Lata et al., 2000) than to other dsRNA
viruses, although the respective folds (the HK97 archetype; Wikoff et al., 2000; in the case of tailed phages) and architecture
differ. (Tailed phages assume quasi-equivalent capsid geometries, and a variety of T-numbers; Dearborn et al., 2012; Duda
et al., 2006.) In the same vein, there is no evidence that the inner
capsids of other dsRNA viruses undergo comparable structural
changes. Insofar as these stepwise transitions of the maturing
f6 procapsid may afford a mechanism for selecting one copy
each of the three RNA segments—a proposition for which there
is supporting evidence but not yet a conclusive proof—this
Mapping Functional Sites on the P1 Lattice
Previous studies have identified the residues involved in the scissile sites on the procapsid for two proteases and in the epitope
for a monoclonal antibody (Qiao et al., 2003b). The procapsid
structure demonstrates the locations of these sites on its outer
surface (Figure 6; Figure S3), where they should be, for accessibility. As such, these observations help to validate the determined structure.
The other three proteins interact only with P1A: P2 and P7
bind on the inside of the procapsid (Katz et al., 2012; Nemecek
et al., 2012; Sen et al., 2008) and P4 on the outside (de Haas
et al., 1999; Pirttimaa et al., 2002). The overlapping footprints
of P2 and P7 cover the tip region of P1A. Crosslinking of the
s-segment and mutants that affect s-segment packaging (Qiao
et al., 2003a) also map to the tip (Figure 6), indicating this region
as the likely s-segment binding site. This region is exposed to the
exterior in P1B whereas it is covered by P4 hexamers in P1A (Figure 6A). Consequently, the s-segment most likely binds to P1B on
Figure 3. Conformational Changes between the Crystal, Procapsid, and Mature Capsid States of P1
(A) Cryo-EM reconstruction of the procapsid with subunits color-coded as in Figure 2A but viewed from a different angle.
(B) Differences between the P1A subunit in the procapsid (blue) and the P1 crystal structure (dark gray) are localized mainly to the hinge region (black arrows, white
arrow in A).
(C) Comparison of P1A (black) and P1B (red) in the procapsid, showing differences of similar magnitude to those in (B): black arrows point out features most
affected and additional differences at the tip (white arrow).
(D) Cryo-EM reconstruction of the nucleocapsid (EMD-1206; Huiskonen et al., 2006) segmented as in (A).
(E) Changes in the P1A structure on maturation (procapsid, blue; nucleocapsid, green) localize in the helices next to the hinge region (black arrows and white arrow
in C).
(F) Changes in the P1B structure on maturation (procapsid, red; nucleocapsid, yellow) involve the whole of edge III (black arrows) as well as the tip (white arrow).
Scale bar: 100 Å.
Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved 5
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
Figure 4. Transformation at the Hinge
(A) P1B subunits (red and yellow) are tightly connected to P1A subunits (blues) of the inverted
vertices in the procapsid. This shell contains cavities between the P1B and P1A subunits (arrows).
(B) In the nucleocapsid, the P1B subunits are
rotated so that the planes of these flat molecules
coincide with the tangential plane of the shell,
leaving no significant cavities between the subunits.
(C) Orientation of P1B subunits (red and yellow
ribbons) on either side of a 2-fold icosahedral axis
in the procapsid. The subunit planes are almost
perpendicular to each other, and their helix-turnhelix motifs are aligned with the 2-fold axis
(arrows).
(D) Corresponding representation of two P1B
subunits in the nucleocapsid. The two subunits are
now almost coplanar. (The views shown in C and D
are rotated around the 2-fold axis so that the
dihedral angles appear considerably larger.)
See also Movie S2.
the procapsid exterior, while the positively charged tips of P1A
interact with RNA that has translocated through the axial channel. The overlap with sites of mutants affected in m-segment
packaging (Qiao et al., 2003a) suggests some commonality in
the binding sites of the first two segments to be packaged.
The binding site for the s-segment has been mapped to the
polypeptide segment between Cys98 and Cys155 of P1 (Qiao
et al., 2003b). This segment is located near the tip (Figure 6). In
P1A, it lines the RNA-packaging channel at the 5-fold vertex. In
P1B, its residues are exposed on the procapsid surface near a
cavity between tilted P1B subunits at the periphery of the P1A
pentamer. The cavity, which is 60 Å from the 5-fold axis (Figure 5B), is positively charged with contributions from Arg104
and Lys105 on P1B and Arg523 on the neighboring P1B. Presumably, the negatively charged sugar-phosphate backbone of the
s-segment pac site (200 nucleotides near the 50 end of the ssRNA)
binds in this cavity. Subsequently, the cavity closes as the procapsid converts to the first expansion intermediate (Figure 5).
It is likely that the segment-binding sites involve more than one
molecule of P1 and are located some distance away from the P4
hexamers because deletion of 22 nucleotides in the s-sequence
50 to the pac sequence was able to prevent packaging but
Figure 5. Procapsid Expansion
(A) Cryo-EM reconstructions of three conformational states of the f6 capsid at 16 Å resolution.
(B and C) Models of a portion of capsid comprising
a pentamer of P1A subunits (blue, green) and
surrounding P1B subunits (red, yellow) subunits,
viewed from above (B) and from the side (C).
Expansion to intermediate 1 is the major transition
of the maturing capsid, achieved by rotation of P1B
subunits around an axis connecting the 3-fold
icosahedral axes (bar in A). This rotation appears
to stabilize the P1B/P1B interface at the 2-fold axis
(Figure 6) and seals gaps between P1A and P1B
subunits near the 3-fold axis (arrow). Further
expansion to intermediate 2 is achieved by outward movement of the P1A subunits. The final step
to the nucleocapsid state is accompanied by local
conformational changes in the P1A subunits that
correlate with increased outward curvature at the
5-fold axis. Scale bar: 50 Å.
See also Movie S3.
6 Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
Figure 6. Regions of P1 Interaction
(A) Regions of P1 interacting with the s-segment (green) and a monoclonal antibody (red) are shown for the P1A and P1B subunits, respectively, in the context of
the procapsid shell. The circle represents the area covered by the P4 hexamer.
(B) Locations of mutations in P1 affecting s- and m-segment binding (magenta) and packaging (orange) are shown for the P1A (cyan) and P1B (yellow) subunits.
The proteolytically susceptible sites for factor Xa and trypsin are also shown (black). The subunits are oriented as in the procapsid (A) and viewed from the outside.
See also Figure S3.
allowed binding and competition with normal binding and packaging (Qiao et al., 1997).
Mutations that Alter RNA Packaging also Affect the
Procapsid Conformation
Even small changes in the pac sequence have drastic effects
on RNA packaging. Point mutations in P1 can suppress pac
sequence mutations or, conversely, may prevent the wildtype RNA sequences from binding (Qiao et al., 2003b). The amino
acid replacements that eliminate s-segment binding (WR103VA,
R385A, and RR617AA) are located near edge II of P1 on the procapsid exterior (Figure S3A). These residues are not clustered
and the mutations probably act independently. Residue R196 is
located inside the P1 fold in the tip (Figure S3B) and the
RR617AA mutant probably disrupts interactions in the adjacent
s-segment binding site. Suppressors of the R196 mutation
(T316I and A402T) are not close to this site, implying that longrange allosteric effects are involved. Similarly, the suppressors
Y486C or Y486S map in different regions of P1 (Figure S3D). On
the other hand, suppressors of the Spac and Mpac mutants all
map close to the s-segment binding site, suggesting direct
interactions with it (Figures S3E and S3F). Moreover, they suggest that the binding sites for the s- and m- segments are close
together.
Conformations of P1 in the Procapsid: Implications
for Assembly
Attachment of P1B subunits around the rims of the P1A pentamers is accompanied by conformational changes at the P1A/P1B
interface. The lever in P1A is bent through 18 and interacts
with two adjacent P1B subunits. The adjacent C-terminal helix
in P1A is also affected, being bent toward the P1A /P1B interface,
with the hydrophobic C terminus inserted into a hydrophobic
pocket in P1B.
The conformation of P1B subunits in the procapsid is also
altered at the interface with P1A subunits at the tip. Loops and
helices are bent in this region to accommodate attachment to
helix bundles in P1A. However, the conformation of the P1B/
P1B interface at the 2-fold icosahedral axis corresponds to the
conformation in the crystal structure (Figure 3C). Although there
are complementary electrostatic interactions across this interface, the negatively charged tips of the levers come into proximity. The P1B subunits are relatively tilted against each other
by 90 , resulting in an interface with the neighboring subunits
that is 20% smaller compared with P1A in the procapsid (Figure 4). Similarly, the interfaces between P1B subunits around
the 3-fold icosahedral axis are relatively small and there are
appreciable cavities between the P1B subunits and the P1A
vertices (Figure 5B). These considerations suggest that P1B subunits may attach to preassembled P1A pentamers and connect
them into a dodecahedral shell in an overall conformation that
is suboptimal but is later optimized during maturation.
Conformations of P1A and P1B: Implications
for Maturation
In maturation, the conformation of P1A subunits changes mainly
in the hinge region, where the large b-hairpin and the underlying
helices bend through 20 . Also, loops at their interface with P1B
change to accommodate intersubunit interactions (Figure 3E).
As for P1B conformation, the entire subunit is affected, particularly in the hinge region. The lever is bent 26 from the icosahedral 2-fold axis, and its position is replaced by the C-terminal
helix (Figures 3F and 4D). This change accompanies a large
rigid-body rotation of P1B (Movie S2) that interlocks P1B subunits
around the 3-fold icosahedral axes and closes pre-existing
cavities between subunits. In this way, the buried surface area
per P1B subunit increases by 50% in the nucleocapsid and
becomes comparable to that of P1A.
Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved 7
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
Knowledge of the procapsid and nucleocapsid structures
illuminates numerous aspects of assembly, maturation, and
packaging. However, weighty issues remain. How does the
s-segment engage with P4, the packaging NTPase after attaching to its binding site? Do the P2 polymerase molecules remain in
place during maturation? How does their location affect transcription and replication? In particular, why is packaging of the
s-segment confined to a single copy when 60 binding sites are
distributed over the procapsid surface? Here, one possibility is
kinetics; i.e., binding of a single s-segment may be sufficient to
induce rapid conversion of the procapsid to the expansion intermediate 1 conformation, precluding further s-segment packaging (Nemecek et al., 2011).
EXPERIMENTAL PROCEDURES
Expression and Purification of P1 and P7 Subunits
Genes for expression of the full-length P1 and truncated P7 (residues 1–150)
subunits were extracted from plasmids pLM3572 and pLM3623, respectively,
and recloned into the first cassette of the pRSFD vector. The plasmids were
transformed into Escherichia coli BL21(DE3) Star cells and overexpressed
overnight at 20 C after induction with 0.5 mM isopropyl thiogalactoside
(IPTG) at optical density (OD) = 0.8. The proteins contained a C-terminal
His6-tag and were purified from the cell extract with affinity chromatography,
using Ni-NTA resin (QIAGEN). P1 was further purified with size-exclusion chromatography using a Superdex 200 column (GE Healthcare) equilibrated in
20 mM Tris, pH = 7.4, 75 mM NaCl, and 3 mM DTT buffer. The protein eluted
in two peaks corresponding to monomer and dimer. Fractions from the monomer peak were pooled and concentrated to 8 mg/ml, flash-frozen in liquid
nitrogen, and stored at 80 C. P7 was further purified using a Superdex 75 column (GE Healthcare) equilibrated in 10 mM Tris, pH = 7.4, 30 mM NaCl, 4 mM
DTT, and 1 mM EDTA buffer. P7-containing fractions were pooled, concentrated to 2.5 mg/ml, and stored at 80 C.
Crystallization, Data Collection, and Structure Determination
To obtain crystals that diffracted beyond 6 Å resolution, we used a P1:P7
mixture in a 2:1 molar ratio at a total concentration of 2 mg/ml. These crystals
were grown in hanging drops consisting of a 1:1 mixture of the protein and well
solution (100 HEPES, pH = 7.5, 180 mM calcium acetate, 10 mM EDTA, and
39% PEG 400) at 293 K. Data sets were collected from three crystals using
a MAR CCD detector at beamline 22-ID (Advanced Photon Source,
Argonne, IL) and merged in the program HKL2000 (Otwinowski and Minor,
1997), yielding a complete data set at 3.6 Å. The self-rotation function suggested a pentamer in the asymmetric unit and therefore we used a 7 Å EM
map of the P1A pentamer extracted from the wild-type procapsid (EMDB
code EMD-2341; Nemecek et al., 2012) as a search model for molecular
replacement. We found a good solution with LLG = 470 and Rfactor =
50.4%. Thereafter, the phases were extended to 3.6 Å resolution using noncrystallographic symmetry. The initial model was built by the program Buccaneer of the CCP4 package (Cowtan et al., 2011; Cowtan, 2012) and manually
refined using Phenix (Adams et al., 2010) and Coot (Emsley and Cowtan,
2004). The model was refined to Rwork = 21.7% and Rfree = 27.4% (Table 1).
Preparation and Purification of f6 Procapsids
Procapsids were produced in E. coli strain JM109 using the plasmid pLM687
(Mindich et al., 1994) to co-express wild-type P1, P2, P4, and P7 proteins (as
P1247 procapsids), then extracted and purified as described previously (Nemecek et al., 2011). Prior to experiments, the samples were transferred into
buffer P (10 mM potassium phosphate and 5 mM MgCl2, at pH 8.0) using
Zeba-midi buffer exchange columns with a 7-kDa cutoff (Thermo Scientific,
Rockford, IL).
Cryo-EM
Drops of f6 procapsids at 10 mg/ml protein concentration were applied to
glow-discharged C-flat grids (Protochips, Raleigh, NC), blotted, and plungefrozen in liquid ethane using a Vitrobot (FEI, Hillsboro, OR) that had been equil-
ibrated at 25 C and 90% humidity. The vitrified specimens were imaged at
47,0003 nominal magnification and 1.0–2.0 mm underfocus with the FEI Titan
Krios microscope at UCLA (courtesy of Dr. Z.H. Zhou and FEI). The
microscope was operated at 300 kV and micrographs were recorded on
SO163 Kodak film at 15 e/Å2 per exposure.
Image Processing
Micrographs were digitized using a Nikon Super Coolscan 9000ED at 4,000
dpi. Image processing was done with the EMAN1 package (Baker et al.,
2010; Ludtke, 2010; Ludtke et al., 1999; Wu et al., 2013) and Bsoft (Heymann
and Belnap 2007; Nemecek et al., 2012). The initial model was derived from the
previously determined procapsid map at 8 Å resolution (Nemecek et al.,
2012). An angular step size of 0.6 was used for global grid searches over
the asymmetric unit. Icosahedral reconstructions were calculated using
e2proc3d.py in EMAN2 and their resolution estimated by Fourier shell correlation between reconstructions from two half data sets at the 0.5 cut-off
(Figure S2).
Flexible Fitting of the P1 Structure into the Procapsid
Initially, the P1 crystal structure was rigid body-fitted into the procapsid map
filtered to 7 Å resolution, using Chimera (Goddard et al., 2005; Pettersen
et al., 2004). P1A and P1B were fitted independently, while the EM map was
rescaled from from 1.351 Å/pixel to 1.397 Å/pixel to maximize cross-correlation of the fits. Regions where the crystal structure deviated significantly
from the EM density were roughly adjusted in Coot (Emsley and Cowtan,
2004) and then the P1A and P1B structures were flexibly fitted using the
MDFF package (Trabuco et al., 2009). The fitted structures were further fitted
into the EM map of the procapsid filtered to 4 Å resolution together with all
neighboring subunits to avoid clashes at the P1A and P1B interfaces. Finally,
both structures were visually inspected and refined in Coot.
Flexible Fitting of P1 into the Nucleocapsid
Here, the cryo-EM map of the f6 nucleocapsid (EMDB ID: emd-1206; Huiskonen et al., 2006) was used. This map was rescaled and sharpened to match the
current cryo-EM map of the procapsid and band-pass-filtered to 7 Å resolution. As in the flexible fitting of P1 into the procapsid map, P1 was initially rigid
body-fitted into the map using Chimera and then manually adjusted in Coot.
The rod-like densities in the map corresponded well to the a helices of the
fitted P1 structure. We further refined the adjusted structures by flexible fitting
with MDFF. All subunits surrounding a given subunit (P1A or P1B) were included
in the fit.
Rigid Body-Fitting of P1 into the Expansion Intermediates
The P1A and P1B structures were transformed into EM density and band-passfiltered to 16 Å resolution using bsf in Bsoft (Heymann and Belnap, 2007) and
fitted into cryo-EM maps of the two expansion intermediates, using the symmetry-fitting algorithm in Chimera. The fit was done in two steps: initially,
P1A and P1B subunits were fitted into the asymmetric unit. Then, their positions
were refined, taking into account all symmetry-related P1A-P1B dimers in the
icosahedral shell. Several starting positions were tested and most solutions
converged to the same P1A and P1B orientations.
ACCESSION NUMBERS
The PDB accession numbers for the P1 crystal structure and the coordinates
for P1A and P1B obtained by flexible fitting of the crystal structure into the
reconstruction reported in this paper are 4K7H and 4BTG, respectively. The
EMDB accession number for the procapsid cryo-EM reconstruction reported
in this paper is 2364.
SUPPLEMENTAL INFORMATION
Supplemental Information includes three figures and three movies and can be
found with this article online at http://dx.doi.org/10.1016/j.str.2013.06.007.
8 Structure 21, 1–10, August 6, 2013 ª2013 Elsevier Ltd All rights reserved
Please cite this article in press as: Nemecek et al., Subunit Folds and Maturation Pathway of a dsRNA Virus Capsid, Structure (2013), http://dx.doi.org/
10.1016/j.str.2013.06.007
Structure
Atomic Model of f6 Maturation
ACKNOWLEDGMENTS
This work was supported by the intramural research programs of NIAMS and
NIDDK and by IATAP grants (to J.H.H. for E.B. and to A.C.S.) and by ASCR
(RVO: 61388963 to E.B.). Crystallographic data were collected at the Southeast Regional Collaborative Access Team 22-ID beamline at the Advanced
Photon Source, Argonne National Laboratory. Use of the Advanced Photon
Source was supported by the US Department of Energy, Office of Science,
Office of Basic Energy Sciences, under contract W-31-109-Eng-38.
Received: May 24, 2013
Revised: June 8, 2013
Accepted: June 14, 2013
Published: July 25, 2013
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