Literature DB >> 23763768

Revolution rather than rotation of AAA+ hexameric phi29 nanomotor for viral dsDNA packaging without coiling.

Chad Schwartz1, Gian Marco De Donatis, Hui Zhang, Huaming Fang, Peixuan Guo.   

Abstract

It has long been believed that the DNA-packaging motor of dsDNA viruses utilizes a rotation mechanism. Here we report a revolution rather than rotation mechanism for the bacteriophage phi29 DNA packaging motor. The phi29 motor contains six copies of the ATPase (Schwartz et al., this issue); ATP binding to one ATPase subunit stimulates the ATPase to adopt a conformation with a high affinity for dsDNA. ATP hydrolysis induces a new conformation with a lower affinity, thus transferring the dsDNA to an adjacent subunit by a power stroke. DNA revolves unidirectionally along the hexameric channel wall of the ATPase, but neither the dsDNA nor the ATPase itself rotates along its own axis. One ATP is hydrolyzed in each transitional step, and six ATPs are consumed for one helical turn of 360°. Transition of the same dsDNA chain along the channel wall, but at a location 60° different from the last contact, urges dsDNA to move forward 1.75 base pairs each step (10.5bp per turn/6ATP=1.75bp per ATP). Each connector subunit tilts with a left-handed orientation at a 30° angle in relation to its vertical axis that runs anti-parallel to the right-handed dsDNA helix, facilitating the one-way traffic of dsDNA. The connector channel has been shown to cause four steps of transition due to four positively charged lysine rings that make direct contact with the negatively charged DNA phosphate backbone. Translocation of dsDNA into the procapsid by revolution avoids the difficulties during rotation that are associated with DNA supercoiling. Since the revolution mechanism can apply to any stoichiometry, this motor mechanism might reconcile the stoichiometry discrepancy in many phage systems where the ATPase has been found as a tetramer, hexamer, or nonamer.
Copyright © 2013 The Authors. Published by Elsevier Inc. All rights reserved.

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Year:  2013        PMID: 23763768      PMCID: PMC3850062          DOI: 10.1016/j.virol.2013.04.019

Source DB:  PubMed          Journal:  Virology        ISSN: 0042-6822            Impact factor:   3.616


Introduction

The AAA+ (ATPases Associated with diverse cellular Activities) superfamily of proteins is a class of motor ATPases with a wide range of functions. Many members of this class of ATPases often fold into hexameric arrangements (Wang et al., 2011; Grainge et al., 2011; Kainov et al., 2008; Mastrangelo et al., 1989; Egelman et al., 1995; Niedenzu et al., 2001; Willows et al., 2004) and are involved in DNA translocation, tracking, and riding (Mueller-Cajar et al., 2011; Lowe et al., 2008; Parsons et al., 1995; Putnam et al., 2001; Iyer et al., 2004a). Despite their functional diversity, the common characteristic of this family is their ability to convert chemical energy obtained from the hydrolysis of the γ-phosphate bond of ATP into mechanical force, a process that usually involves a conformational change in the protein. This change of conformation generates both a loss of affinity for its substrate and a mechanical movement; which in turn is used to either make or break contacts between macromolecules, resulting in local or global protein unfolding, complex assembly or disassembly, or the translocation of DNA, RNA, proteins, or other macromolecules. These activities underlie processes critical to DNA repair, replication, recombination, chromosome segregation, DNA/RNA transportation, membrane sorting, cellular reorganization, and many others (Martin et al., 2005; Ammelburg et al., 2006; Grainge et al., 2007; Grainge, 2008; Lowe et al., 2008). Numerous biochemical and structural aspects of reactions catalyzed by AAA+ proteins have been elucidated, including those occurring during ATP hydrolysis. For instance, the crystal structure of the sliding clamp loader complex has revealed a spiral structure that strikingly correlates with the grooves of helical dsDNA, suggesting a simple explanation for how the loader/DNA helix interaction triggers ATP hydrolysis, and how DNA is released from the sliding clamp (McNally et al., 2010; Guenther et al., 1997). In both prokaryotic and eukaryotic cells, DNA needs to be transported from one cellular compartment to another. For example, during phage maturation, the genome of dsDNA viruses is translocated into preformed protein shells, termed procapsids (for review, see (Guo and Lee, 2007; Rao and Feiss, 2008; Zhang et al., 2012; Serwer, 2010)). This entropically unfavorable process is accomplished by a nanomotor that uses ATP as an energy source (Guo et al., 1987c; Chemla et al., 2005; Hwang et al., 1996; Sabanayagam et al., 2007; Schwartz et al., 2012; Lee et al., 2008; Shu and Guo, 2003a; Chen and Guo, 1997). The dsDNA packaging motor consists of a proteinaceous channel and two packaging molecules with which it carries out its activities. The larger packaging molecule serves as part of the ATPase complex, and the smaller is responsible for dsDNA binding and cleavage (Guo et al., 1987c, 1998). This model has now become well-established (Guo and Lee, 2007; Rao and Feiss, 2008; Zhang et al., 2012; Serwer, 2010). The bacterial virus phi29 motor involves an ATPase, gp16 (Guo et al., 1987c, 1987b; Huang and Guo, 2003a, 2003b; Lee and Guo, 2006; Lee et al., 2008; Ibarra et al., 2001; Grimes and Anderson, 1990) and a hexameric packaging RNA ring (Guo et al., 1987a, 1998; Shu et al., 2007; Zhang et al., accepted for publication). The connector consists of 12 copies of gp10 that creates a central channel that serves as a pathway for dsDNA translocation (Jimenez et al., 1986; Guasch et al., 2002; Badasso et al., 2000). The cellular components that show the strongest similarity to the viral DNA packaging motor include FtsK, an AAA+ DNA motor protein that transports DNA and separates intertwined chromosomes during cell division (Iyer et al., 2004b), and SpoIIIE (Demarre et al., 2013), an AAA+ protein responsible for transportation of DNA from a mother cell into the pre-spore during Bacillus subtilis sporulation (Bath et al., 2000). The ATPase of phi29, gp16, is similar to these families in both structure and function (Iyer et al., 2004b; Guo et al., 1998). Both the FtsK and SpoIIE DNA transportation systems rely on assembly of a hexameric machine. FtsK proteins contain three components: one for DNA translocation, one for controlling orientation of movement, and one for anchoring to the substrate (Demarre et al., 2013). Extensive studies suggest that FtsK may employ a “rotary inchworm” mechanism to transport DNA (Massey et al., 2006). The FtsK hexameric motor encircles dsDNA. During each cycle of ATP binding and hydrolysis within each FtsK subunit, one domain tightly binds the helix while another translocates along the DNA. This process causes translational movement, a mechanism that is repeated by the subsequent transfer of the helix to the next adjacent subunit (Massey et al., 2006). It was suggested that viral DNA packaging motors operate by a rotation mechanism involving a five-/six-fold mismatch structure (Hendrix, 1978). Many subsequent models have been proposed describing the packaging motor of dsDNA (Khan et al., 1995; Serwer, 2003; Astumian, 1997; Guo et al., 1998; Hendrix, 1978; Grimes and Anderson, 1997; Chen and Guo, 1997; Guasch et al., 2002; Hou et al., 2010; Morita et al., 1995b; Sabanayagam et al., 2007; Oram et al., 2008; Serwer, 2010; Shu et al., 2007; Maluf et al., 2006; Yu et al., 2010; Aathavan et al., 2009). The most well-studied bacteriophage phi29 DNA packaging motor was also the first constructed with purified components (Guo et al., 1986) and has been shown to consist of three major components that interact with each other in unison (Fig. 1) (Guo et al., 1987a, 1987c; Lee and Guo, 2006; Ibarra et al., 2001). An RNA component was discovered (Guo et al., 1987a) that was later determined to exist as a hexameric ring (Guo et al., 1998;Zhang et al., 1998). Based on the structure of the hexameric pRNA, it was proposed that the mechanism of the phi29 viral DNA packaging motor is similar to that used by other hexameric DNA tracking motors of the AAA+ family (Guo et al., 1998). The presence of hexameric folds in the motor has been revealed by biochemical analysis (Guo et al., 1998; Zhang et al., 1998; Hendrix, 1998); single molecule photobleaching (Shu et al., 2007); gold labeling imaged by EM (Xiao et al., 2008; Moll and Guo, 2007; Shu et al., 2007); nano-fabrication (Xiao et al., 2010); and RNA crystal structure (Zhang et al., accepted for publication).
Fig. 1

Depiction of structure and function of phi29 DNA-packaging motor. (A) Illustrated model of hexameric pRNA based on a crystal structure (Zhang et al., accepted for publication) and the 30° tilting of the channel subunits, relative to the central axis of the connector (pdb ID: 1H5W); (B) DsDNA showing the shift of 30° angle between two adjacent connector subunits; (C) Connector showing the change of 30° angle between two adjacent connector subunits; (D) AFM images of hexameric pRNA with 7-nt loops (Shu et al., 2013).

However, whether the RNA and ATPase are hexamers or pentamers is still debated. Other laboratories have reported the existence of five-fold symmetry (Chistol et al., 2012; Yu et al., 2010; Morais et al., 2008; Simpson et al., 2000; Ding et al., 2011; Harjes et al., 2012). Adherents of the pentamer model have also proposed variations to reconcile the pentamer and hexamer debate. One theory is that a pRNA hexamer is first assembled on the motor, after which one subunit leaves, resulting in a final pentamer state (Morais et al., 2001, 2008; Simpson et al., 2000). An alternative idea suggests that one subunit in the pentameric ring is inactive during each cycle while the other four subunits function sequentially during DNA packaging (Moffitt et al., 2009; Yu et al., 2010). In previous reports, we have shown that motor intermediates isolated during the active DNA packaging process also contain a hexameric pRNA (Shu et al., 2007). Furthermore, in this issue, we provide data to confirm that the ATPase motor is hexameric (Schwartz et al., this issue) and is a relative of the hexameric AAA+ DNA translocase. In this paper, we show that the motor mechanism of DNA translocation involves revolution, rather than a rotational mechanism that involves a coiling force.

Results

The structure of the hexameric motor

The essential components of the phi29 DNA packaging motor include the dodecameric connector and the ATPase gp16 geared by a ring of RNA. The crystal structure of the three-way junction (3WJ) of the pRNA (Shu et al., 2011), one of the motor components, has recently been solved (Zhang et al., accepted for publication) and the predicted hexameric pRNA ring structure has been confirmed (Zhang et al., 2013; Fig. 1A). AFM images revealed an elaborate, ring-shaped structure consisting of six distinct arms representing the six subunits of pRNA (Fig. 1D).

Sliding of gp16 out of dsDNA verified by addition of steric blocks to the end of dsDNA

When Cy3-dsDNA is mixed with eGFP-gp16, a transfer of energy from the donor fluorophore (eGFP) to the acceptor fluorophore (Cy3) is observed, indicating that the protein fluorophore is in close proximity to the dsDNA fluorophore. However, after addition of ATP, the Förster Resonance Energy Transfer (FRET) efficiency decreased significantly (Fig. 2), suggesting that the protein had dissociated from the DNA after ATP hydrolysis. We hypothesize that gp16 slides along DNA and then falls off upon reaching the end of the DNA. In contrast, binding of gp16 to dsDNA was significantly enhanced in the presence of non-hydrolyzable ATP analogue, γ-S-ATP, as shown by both gel shift and binding assays. To determine whether the reduced FRET signal is due to dissociation of eGFP-gp16 or a process by the protein moves along DNA, we exploited a streptavidin hindrance test (Fig. 3). The terminally biotinylated DNA was incubated with streptavidin, which should prevent gp16 sliding off the DNA, but not interfere with simple dissociation. Complexes of eGFP-gp16/DNA/γ-S-ATP complexes remain stable in the presence of ATP only when the terminally biotinylated Cy3 DNA was bound to streptavidin (lane 8, Fig. 3).
Fig. 2

FRET assay of fluorogenic ATPase and short dsDNA. eGFP-gp16 was incubated with Cy3-DNA and without ATP and excited at 480 nm. Energy transfer occurs between the two fluorophores, with light emission at ~560 nm, indicating that gp16 and DNA are in close proximity. Bar graph (top right) showing the FRET efficiency difference between the two samples.

Fig. 3

EMSA of eGFP-gp16 on terminally blocked short dsDNA. 40 bp Cy3-dsDNA, with biotin attached to each end, was incubated with eGFP-gp16, non-hydrolyzable γ-S-ATP, and streptavidin in different combinations. The complexes that were mixed at approximately a 6:1 molar ratio of protein:DNA were then electrophoresed through an agarose gel and scanned for Cy3 fluorescence of DNA and GFP fluorescence of gp16 (see Materials and Methods).

One defective monomer in the hexameric ATPase blocks function

The Walker A motif of AAA+ proteins is responsible for ATP binding, while the Walker B motif initiates ATP hydrolysis (Story and Steitz, 1992). Both motifs have been identified in phi29 gp16, previously (Guo et. al., 1987c) and (Schwartz et al., this issue). Since other ATPases have been shown to demonstrate cooperativity, the Hill constant for DNA-binding was evaluated using capillary electrophoresis (CE) to distinguish between a sequential or concerted action mechanisms. In order to help elucidate the mechanism of the DNA packaging motor, the number of copies of an inactive Walker B mutant within the hexameric ATPase required to block DNA packaging process was determined. The defective mutant was titrated with the active wild-type, were allowed to freely associate, and analyzed for DNA binding (see Materials and Methods). The minimum number (y) of mutant gp16 needed to block the packaging within the hexameric ring was predicted with the equation , where p and q represent the ratio of wildtype and Walker B mutant gp16, respectively, and p+q=1 (Fig. 4). Using this expanded binomial, each term represents a different mixed hexamer where the exponents of p and q, respectively indicate the number of wildtype and mutant monomer in each mixed hexamer. For example, the term indicates that the hexamer contains three wildtype and 3 three Walker B mutant monomers. Our empirical data almost perfectly overlapped with the theoretical curve corresponding to ‘y’ is equal to 1 (Fig. 4), suggesting that one inactive subunit in the hexamer abolishes motor activity.
Fig. 4

Binomial distribution assay to determine the minimum number (y) of defective eGFP-gp16 in the hexameric ring to block motor activity. Theoretical plot of percent Walker B mutant gp16 versus yield of infectious virions in in vitro phage assembly assays. Predictions were made with the equation as seen in the Materials and Methods.

Motor ATPase tightly clinches dsDNA after binding to ATP and subsequently pushes the dsDNA away after ATP hydrolysis

Similar to the AAA+ motor proteins that undergo conformational changes during their interaction with ATP and adopt two distinct states, the phi29 motor ATPase also exhibits a high or low affinity state for DNA. EMSA revealed that the affinity of gp16 for dsDNA increases in the presence of γ-S-ATP (Schwartz et al., 2012). We utilized a CE assay that allowed for direct quantification of the amount of DNA bound to gp16. At increasing concentrations of γ-S-ATP, the amount of bound DNA increased progressively, indicating that gp16 transitioned from a state in which binding to DNA was unfavorable to one in which binding was preferred (Fig. 5A). A regression plot of dissociation constant (K) for dsDNA versus concentration of γ-S-ATP indicated that the affinity of gp16 for substrate increased 40-fold with saturating amounts of γ-S-ATP (Fig. 5B). This significant increase strongly suggests that the species that binds to DNA is the gp16-ATP complex and the gp16 binds first to ATP and secondly to DNA, as also suggested previously (Schwartz et al., 2012). However, adding ADP, even at non-physiological conditions (up to 6 mM), failed to promote an increase in dsDNA-binding affinity (Fig. 5C). Furthermore, the amount of DNA bound to g16 was comparable to a condition where no nucleotide was added. These observations indicate that gp16 cycles through states of ATP binding/DNA loading and ATP hydrolysis/DNA release or pushing. This conclusion was further supported by the finding that addition of normal ATP to the gp16/DNA/γ-S-ATP complex promoted the departure of the dsDNA from the complex (Schwartz et al., this issue).
Fig. 5

One γ-S-ATP is sufficient to bind to one subunit of the gp16 hexamer and promote a high affinity state for dsDNA. Sequential binding of gp16 for dsDNA substrate involves γ-S-ATP substep. (A) The K for dsDNA at varying concentrations of γ-S-ATP. (B) The relative K of gp16 decreased 40-fold as the concentration of γ-S-ATP increased from 0 mM to 1 mM. (C) ADP, a derivative of ATP hydrolysis, was unable to promote binding and had the similar effect as no nucleotide addition. The hyperbolic curve (D) suggests a cooperativity factor of 1, indicating that one γ-S-ATP is sufficient to produce the high affinity state of gp16 for DNA. DNA releases from the complex DNA-gp16-γ-S-ATP mediated by ADP (E), forming a sigmoidal curve (F) with a cooperativity factor of 6 indicating that all six subunits of gp16 need to be bound to ADP to release DNA from the protein.

Only one molecule of ATP is sufficient to generate the high affinity state for DNA in the ring of the motor ATPase

Next, we sought the answer to how many nucleotides were required for gp16 to generate the high affinity state for dsDNA; in other words, how many subunits need to bind to ATP in order for the gp16 hexamer to stably associate to dsDNA. This information is useful in understanding how the hexameric complex of gp16 utilizes the substrate in order to generate unidirectional DNA translocation. AAA+ proteins are typically organized into a homo-oligomeric assembly where each component contains the recognition motifs required for binding of the substrate. In principle, one can imagine that each subunit can bind to the substrate independently from the others; however, such an arrangement can lead to futile cycles of ATP consumption. Two major configurations can be hypothesized to avoid the above described scenario. First, it may be possible that the binding sites for the substrate consist of the same recognition motifs in all the subunits, and in this case, all subunits can bind at the same time to the substrate. In this hypothetical situation, it is intuitive to imagine that a form of coordination among the subunits must also exist at the level of ATP hydrolysis, since the most effective mechanism of translocation would allow all subunits to hydrolyze at the same time corresponding to an exodus of the dsDNA substrate. The second possibility is that DNA is bound at any given time to only one subunit of the oligomer, and after the cycle of ATP hydrolysis is terminated in the specific subunit that binds DNA, the substrate is then passed to the next subunit in the high ATP affinity state in order to initiate another cycle of hydrolysis. To distinguish between these two scenarios, we analyzed the amount of DNA bound to gp16 by keeping the concentration of gp16 and DNA constant and varying the concentration of γ-S-ATP in the reaction mixture (Fig. 5D). If more than one γ-S-ATP per oligomer of gp16 is required to generate the high affinity state for DNA in the protein, the plot would show a cooperativity profile, with a Hill coefficient representing the amount of γ-S-ATP required to be bound to gp16. Our data exhibit no cooperativity in binding (Hill coefficient=1.5) indicating that not all of the subunits of gp16 are required to be bound to γ-S-ATP to stabilize binding to DNA. In principle, a Hill coefficient close to one indicates that only one γ-S-ATP-activated subunit in the oligomer is required for DNA binding or that the binding of DNA is progressively increased with the number of subunits that are bound to γ-S-ATP. To address this question, we performed an experiment similar to the CE assay described above. A complex of gp16-DNA was assembled in the presence of saturating γ-S-ATP. After the complex formed, increasing amounts of ADP were added in order to compete with γ-S-ATP for the active sites of gp16 and to ultimately promote DNA release. The reaction is remarkably cooperative (Fig. 5E, F). From the fractional inhibition plot we extrapolated a Hill coefficient close to 6, indicating that six molecules of ADP must be bound to gp16 before dsDNA is released from the protein. This indicates that only one ATP-bound subunit stably binds DNA and prevents ADP-mediated release. Furthermore, the data indicate that gp16 most likely binds to dsDNA at only one subunit per round of ATP hydrolysis. As mentioned above, a Hill coefficient close to one indicates that binding of DNA progressively increases with the number of subunits that are bound to γ-S-ATP. However, the 3.6-nm diameter of the motor channel, as measured from the crystal structure (Guasch et al., 2002; Badasso et al., 2000), suggests that only one dsDNA can be bound within the channel; indicating that dsDNA shifts to a neighboring gp16 subunit upon release of the first subunit. In combination with the finding that one Walker B mutant gp16 was found to be sufficient to block the motor for DNA packaging, these results support a model where the motor ATPase works sequentially, and upon ATP hydrolysis the subunit of the ATPase gp16 assumes a new conformation and pushes dsDNA away from the subunit and transfers it to an adjacent subunit (Fig. 7).
Fig. 7

Schematic of gp16 binding to DNA and mechanism of sequential revolution in translocating genomic DNA. The connector is a one way valve that allows dsDNA to move into the procapsid, but does not allow movement in the opposite direction. Gp16, which is bridged by pRNA to associate with the connector, provides the pushing force. The binding of ATP to one subunit stimulates gp16 to adopt a conformation with a higher affinity for dsDNA. ATP hydrolysis forces gp16 to assume a new conformation with a lower affinity for dsDNA, thus pushing dsDNA away from the subunit and transferring it to an adjacent subunit. DsDNA is translocated at a pace of 1.75 base pairs per transfer to the neighboring subunit and is bound at a location 60° different from the first subunit on the same phosphate backbone chain. Rotation of neither the hexameric ring nor the dsDNA is required since the dsDNA revolves around the diameter of the ATPase. In each transitional step, one ATP is hydrolyzed, and in one cycle, six ATPs are required to translocate dsDNA one helical turn of 360° (10.5 base pairs). An animation is available at http://nanobio.uky.edu/movie.html.

Mixed oligomer between wildtype and mutants display negative cooperativity and communication between the subunits of gp16 oligomer

The fact that dsDNA only binds to one gp16 subunit at a time suggests that gp16 undergoes cooperativity during translocation. To verify this hypothesis we analyzed ATPase activity by studying the effect on the oligomerization of gp16 when mutant subunits were introduced (Trottier and Guo, 1997; Chen et al., 1997). If we assume communication between the subunits of the ATPase, the effect on the ATPase activity mediated by one inactive subunit should be higher than the simple sum of the ATPase activity of the single subunit. When the ATPase activity was measured in the absence of dsDNA, increasing amounts of Walker B mutants added to the overall oligomer of gp16 failed to provide any significant effect on the rate of hydrolysis (Fig. 6A, C), suggesting that each subunit of gp16 is able to hydrolyze ATP independently. However, when saturating amounts of dsDNA were added to the reaction, we observed a strong negative cooperative effect with a profile that mostly overlapped with the one predicted for the case in which one single inactive subunit is able to inactivate a whole oligomer (Fig. 6B, D) using an equation derived from a binomial distribution inhibition assay (Trottier and Guo, 1997; Chen et al., 1997) (see also Fig. 4). The results suggest that in the presence of dsDNA, a rearrangement occurs within the subunits of gp16, enabling them to communicate and “sense” the nucleotide state of the neighboring subunit. The fact that dsDNA needs to be present in the reaction indicates that dsDNA binds to the inactive subunit during the catalytic cycle and remains bound to it, which generates a stalled ATP hydrolysis cycle. This observation supports the idea that only the subunit that is binding to the substrate at any given time is permitted to hydrolyze ATP, thus performing translocation while the other subunits are in a type of ‘stalled’ or ‘loaded’ state. The scenario suggests an extremely high level of coordination on protein function, which is likely the most efficient process to couple energy production with DNA translocation via ATP hydrolysis.
Fig. 6

ATPase inhibition assay by Walker B mutants reveals complete negative cooperativity. The inhibition ability of the Walker B mutants E119A and D118E/E119D was assayed by ATPase activity in the absence (left) and presence (right) of dsDNA. In the presence of DNA (right), the experimental data (solid line) overlapped with a theoretical curve indicating that one inactive subunit (dotted line) within the hexamer is able to completely block the activity of the hexameric gp16 and abolish ATPase activity, demonstrating negative cooperativity (see also Fig. 4). The dashed line is the theoretical curve where two inactive subunits are necessary for inhibition.

Direct observation of multiple ATPase gp16s lining up in queue along dsDNA as the initiation step in DNA packaging

The consensus idea from extensive investigation of viral packaging motors is that the ATPase binds to the procapsid to form a procapsid/ATPase complex as the first step of motor action (Fujisawa et al., 1991; Guo et al., 1987b; Koti et. al., 2008). To investigate the sequence of interaction between motor components during DNA packaging, a fluorescent Cy3-conjugated gp16 was used to visualize the protein. Interestingly, we found that the first step in DNA packaging was the binding of multiple gp16 queued along the dsDNA, as observed by both single molecule imaging (Fig. 8 Part I) and by binding affinity studies. Moreover, negatively stained electron microscopy images have been taken of a multimeric gp16 complex along long genomic DNA (Fig. 8 Part II), lending further support to our conclusions.
Fig. 8

Part I. Direct observation of ATPase complex queued and moving along dsDNA. Cy3 conjugated gp16 was incubated with (A, B, E) and without (D) dsDNA, tethered between two polylysine beads where (C, F) are magnified images of the framed regions of (B, E), respectively. (A–C) are overlapped pseudocolor images indicating the binding of Cy3-labeled gp16 along the To-Pro-3 stained dsDNA chain (Red: Cy3-gp16; Green: To-Pro-3 DNA). (G, H) The motion of the Cy3-gp16 spot was analyzed and a kymograph was produced to characterize the ATPase walking. (Actual motion videos can be found in the supplementary information and at http://nanobio.uky.edu/movie.html). Part II. Negatively stained transmission electron microscopy images of ATPase queued along dsDNA. gp16 was bound to non-specific dsDNA in queue. Part III. Recording of two Cy3-gp16/dsDNA complexes showing motionless gp16 spots in a buffer containing no ATP. (A) Sequential images of the recording. (B) Kymograph of the two spots.

DNA tightropes were constructed (Kad et al., 2010), that not only generated a straight DNA chain, but also lifted the DNA a few microns away from the surface of the slide within the sample chamber. Background fluorescence from non-specific binding of Cy3-gp16 to the surface of the slide is therefore eliminated when the focus of the imaging plane is on the DNA-bound Cy3-gp16 molecules. A string of multiple Cy3 spots representing Cy3-gp16 complexes are observed along the DNA chains (Fig. 8 Part I A–C, E, F). In the absence of DNA, a Cy3 signal was not observed between the polylysine beads (Fig. 8 Part I D), indicating that the queued Cy3 signals were truly from the multiple Cy3-gp16 bound to DNA. The results suggest that ATPase gp16 lines up in a queue along dsDNA at the initiation step in DNA packaging. These data are in accordance with another study where complexes of procapsid containing partially packaged dsDNA were isolated by sucrose sedimentation; conversion of the complexes to complete the DNA packaging process required the addition of ATPase gp16, but not pRNA (Shu and Guo, 2003b). The same publication also indicated that multiple gp16 molecules, but only a single hexameric pRNA, were required for packaging (Shu and Guo, 2003b). The motion of gp16 along the lifted dsDNA tightrope was observed by single molecule fluorescence imaging. Sequential images were taken after washing with different buffers to illustrate the displacement of Cy3-gp16 over time. When the sample was washed with a buffer, a total of 195 Cy3-gp16 spots were studied. In the absence of ATP, the vast majority of these Cy3-gp16 spots did not show any motion along the DNA chain. After 20 mM ATP was added to the washing buffer, active motion of eGFP-gp16 along the dsDNA was observed, as shown by the sequential images (Fig. 8 Part III A) and kymographs (Fig. 8 Part III B). Actual motion videos can be found in the supplementary information and at http://nanobio.uky.edu/movie.html. Terminases of viral DNA packaging motors bind to procapsids, although with an extremely low affinity and at low efficiency (Shibata et al., 1987; Morita et al., 1995b; Morita et al., 1995a; Guo et al., 1987b; Fujisawa et al., 1991; Lee and Guo, 2006). Our finding that gp16 first binds to dsDNA and then moves along dsDNA before reaching and binding to the procapsid is not in contradiction, rather a further refinement of the previous understanding. We hypothesize that gp16 contains two domains, one for dsDNA binding and one for connector/procapsid binding. In the absence of genomic DNA, gp16 binds to the procapsid, albeit with lower affinity. The key to understanding the sequence of interactions is based on the relative affinity of the protein for its substrate. Gp16 has a higher binding affinity for genomic DNA compared to that of the procapsid (Fig. 9). In the absence of dsDNA, gp16 and other terminases bind to the procapsid (Guo et al., 1987b). However, it is hypothesized that in the presence of genomic DNA, gp16 and other terminases prefer to bind to genomic DNA and track along it until reaching the packaging RNA and other motor components of the procapsid.
Fig. 9

Binding affinity of gp16 to dsDNA and procapsid/pRNA complex measured using sucrose sedimentation. Ratio of procapsid-bound and DNA-bound gp16 under different treatments where the percent of bound gp16 to total gp16 is expressed, showing gp16’s affinity to DNA is much greater than to procapsid/pRNA complex.

To test this hypothesis, we measured the interaction of ATPase gp16 with the procapsid (Fig. 9). Gp16 is sticky and binds to all kinds of substrate, including nonspecifically to the procapsid. No significant difference was observed during the formation of the procapsid/gp16 complex in the presence or absence of pRNA (Fig. 9), which has been reported to serve as the bridge for gp16 binding to procapsid (Lee and Guo, 2006), but gp16 exhibited substantially higher affinity for dsDNA than for procapsid/pRNA complex. Although the ATPase may contain both dsDNA and procapsid binding domains, we suggest it prefers to bind to the procapsid only after tracking along the genomic DNA; that is, gp16 prefers to bind to genomic DNA first before reaching the procapsid.

Translocation of dsDNA helix by revolution without involvement of coiling or tension force

It has been demonstrated that the connector acts as a one way valve (Schwartz et al., 2012; Fang et al., 2012; Jing et al., 2010), only allowing dsDNA to move into the procapsid, but not in the opposite direction. Gp16, which is bridged by hexameric pRNA to associate with the connector, is expected to be the pushing force (Fig. 10A). The binding of ATP to one subunit stimulates gp16 to adopt a conformation with high affinity for dsDNA, while ATP hydrolysis forces gp16 to assume a new conformation with lower affinity, thus shifting dsDNA away from the first subunit and transferring it to an adjacent subunit due to the higher affinity for the next subunit (Fig. 10). Since the contact of the connector with dsDNA chain is transferred from one point on the phosphate backbone to another, rotation of neither the hexameric ring nor the dsDNA is required. One ATP is hydrolyzed in each step, and six ATPs are consumed for one cycle to translocate dsDNA one helical turn of 360° (10.5 base pairs). The binding of gp16 to the same phosphate backbone chain, but at a location 60° different from the last subunit, causes dsDNA to move forward 1.75 base pairs (10.5 bp per turn/6 ATP=1.75 bp per ATP), in good agreement with the 2 bp/ATP(Guo et al., 1987c) or 1.8 bp/ATP previously quantified empirically (Morita et al., 1993).
Fig. 10

Mechanism of sequential revolution in translocating genomic DNA. Connector is a one way valve (Jing et. al., 2010) that allows dsDNA to move into the procapsid, but does not allow movement in the opposite direction. (A) Binding of ATP to one gp16 subunit stimulates it to adapt a conformation with higher affinity for dsDNA. ATP hydrolysis forces gp16 to assume a new conformation with lower affinity for dsDNA, thus pushing dsDNA away from this subunit and transferring it to an adjacent subunit. (B) Binding of gp16 to the same phosphate backbone chain, but at a location 60° different from last subunit urges dsDNA to move forward 1.75 base pairs. Since the dsDNA chain is transferred from one point on the phosphate backbone to another point, the rotation of the hexameric ring or the dsDNA is not required. (C) The revolution of dsDNA along the 12 subunits of the connector channel.

Translocation of dsDNA helix by revolution through the 30°-tilted connector subunits facilitated by anti-parallel displacement between the right-handed dsDNA helix and the left-handed connector channel subunits

The crystal structure of the connector revealed that all 12 subunits of the connector protein are tilted at a 30° relative to the DNA axis in a configuration opposite in handedness to the dsDNA helix during packaging, to form the channel (Guasch et al., 2002; Badasso et al., 2000). The structural relationship for the left-handed/right-handed anti-parallel displacement between the connector whirl and dsDNA helix can be visualized from an external viewpoint, in which dsDNA propels through the connector potentially making contact at every 30° subunit (Fig. 11). The left-handed/right-handed anti-parallel displacement argues against the rotation threading mechanism that requires the threads to be in the same direction to move. On the contrary, this arrangement greatly facilitates controlled single directional revolution motion; supporting the model that dsDNA revolves through the connector channel without producing a coiling or torsion force, and touching each of the 12 connector subunits in 12 discrete steps of 30° transitions. Since each change of 30° (360°/12=30°) during the advancement of the DNA helical pitch is compensated by the connector subunit 30° tilting (Fig. 11D), rotation of dsDNA is not necessary during translocation.
Fig. 11

DNA revolves and transports through 30° tilted connector subunits facilitated by anti-parallel helices between dsDNA helix and connector protein subunits. The anti-parallel configuration can be visualized in an external view (A) in which DNA revolves through the connector making contacts at every 30° subunit (B,C). A planar view is suggested (D) in which DNA is advanced and travels along the circular wall of the connector channel with no torsion or coiling force, through the connector channel, touching each subunit translating to 12 discrete steps of 30° revolving turns for each step.

Discussion

A rotation mechanism for viral DNA packaging has long been proposed (Hendrix, 1978) and has been well-regarded by the scientific community. However, studies in which the connector was covalently linked to the capsid protein have suggested that the connector does not rotate (Baumann et al., 2006; Maluf and Feiss, 2006). When the connector and the procapsid protein were fused to each other, rotation of the connector within the procapsid was not possible since motors were still active in packaging, implying that connector rotation is not necessary for DNA packaging. The lack of connector rotation was also shown by experiments combining the methods of single-molecule force spectroscopy with a polarization-sensitive single-molecule fluorescence trap (Hugel et al., 2007). Because the connector does not rotate, there is no reason to expect that gp16 would rotate since the gp16 ring is tightly bound to the pRNA ring (Lee and Guo, 2006) that is immobilized to the stationary connector. Single molecule studies by three separate labs using beads tethered to the end of the phi29 dsDNA have revealed that dsDNA still translocates into the procapsid even with such tethering (Shu et al., 2007; Chang et al., 2008; Moffitt et al., 2009; Yu et al., 2010). This data led to a mystery regarding the operation of the phi29 DNA translocation motor since it does not follow the classical rotational model. The finding that phi29 DNA packaging motor utilizes a revolution rather than a rotation mechanism is in good agreement with all data reported in the literature. The connector was recently shown to only allow unidirectional movement of dsDNA (Jing et al., 2010), and a model using a “push through a one-way valve” mechanism has been described (Schwartz et al., 2012; Fang et al., 2012) that is in accordance with the proposed ratchet (Serwer, 2003) and compression (Ray et al., 2010a, 2010b) models that explain how DNA is prevented from reversing out of the capsid during packaging (Black, 1989; Feiss and Rao, 2012; Casjens, 2011; Guo and Lee, 2007). The revolution mechanism is independent of any specific stoichiometry, thus motors with different oligomeric states can act similarly. This idea alleviates a current question that different phage packaging ATPases are found to be tetramers (Maluf et al., 2006; Feiss et al., 2010), hexamers (Guo et al., 1998; Schwartz et al., this issue; Shu et al., 2007), and nonamers (Roy et al., 2011).

Materials and methods

Cloning, mutagenesis and protein purification

The engineering of eGFP-gp16 and the purification of gp16 fusion protein have been reported previously (Lee et al., 2009). eGFP-gp16 mutants G27D, E119A, R146A, and D118E/E119D were cloned previously (Schwartz et al., this issue).

Measurement of gp16 ATPase activity

Enzymatic activity via fluorescence was described previously (Lee et al., 2008).

In vitro virion assembly assay

Purified in vitro components were mixed and subjected to virion assembly assay, as previously described (Lee and Guo, 1994).

Statistical analysis and data plotting

Most statistical analysis was performed using Sigmaplot 11. Determination of the Hill coefficient was obtained by nonlinear regression fitting of the experimental data to the following equation: , where E and Emax refer to the concentration of gp16/DNA complex, X is the concentration of ATP or ADP, Kapp is the apparent binding constant, and n is the Hill coefficient.

CE experiments to determine ratio of gp16 to bound dsDNA

CE (Capillary electrophoresis) experiments were performed on a Beckman MDQ system equipped with double fluorescent detectors (488 nm and 635 nm excitation). The capillary used was a bare borosilicate capillary 60 cm in total length with a 50 μm inner section. The method consisted of a 20 min separation at 30 KV normal polarity. Typical assay conditions contained an optimized buffer (Huang and Guo, 2003a, 2003b) of 50 mM Tris–HCl, 100 mM borate at pH 8.00, 5 mM MgCl2, 10% PEG 8000 (w/v), 0.5% acetone (v/v), 3 μM eGFP-gp16 monomer and variable amounts of ATP/ADP and DNA (Schwartz et al., this issue). Peaks were quantified and analyzed by Sigma Plot for DNA binding.

Sucrose gradient sedimentation of gp16/procapsid

Procapsids (1.6 mg/mL) were purified by opti-prep sedimentation, a sterile density gradient solution used in isolation of virus purification, and incubated with eGFP-gp16 (3 μM) and pRNA (62.5 ng/μL) at room temperature for 30 min. Samples were then loaded on top of a 5–20% sucrose gradient containing 50 mM NaCl, 25 mM Tris pH 8.0, 2% glycerol, 0.01% tween-20, 5 mM MgCl2, and 0.25 mM γ-S-ATP; 200 μL 60% sucrose was used as a cushion and were then sedimented at 35,000 rpm with a SW55 rotor for 4 h. After fractionation, the fluorescent signal was captured using a Synergy IV microplate reader.

Electrophoretic mobility shift assay (EMSA)

The engineering of eGFP-gp16 and the purification of gp16 fusion protein (Lee et al., 2009), as well as the gp16 and dsDNA binding assay (Schwartz et al., 2012), have been reported previously. Cy3- or Cy5-dsDNA (40 bp) was prepared by annealing two complementary DNA oligos containing Cy3 or Cy5 labels at their 5′ ends (IDT). The annealed product was purified from 10% polyacrylamide gel. The samples for EMSA assay were prepared in 20μl buffer A (20 mM Tris–HCl, 50 mM NaCl, 1.5% glycerol, 0.1 mM Mg2+). 1.78 μM eGFP-gp16 was mixed with 0.3 μM 40 bp Cy3-DNA at various conditions in the typical fashion. The samples were incubated at ambient temperature for 20 min and then loaded onto a 1% agarose gel (44.5 mM Tris borate) and electrophoresed at 8 V/cm for 1 h at 4 °C. The eGFP-gp16 and Cy3-DNA in the gel were analyzed by a fluorescent LightTools Whole Body Imager using 488 nm and 540 nm excitation wavelengths for GFP and Cy3, respectively.

Observation of gp16 motion

Double-stranded lambda DNA (48 kbp) was tethered between two polylysine coated 4 μm silica beads (Kad et al., 2010). The dsDNA was bound between beads by back-and-forth infusion of DNA over the beads for 10 min; binding occurred as a result of charge–charge interactions. The back and forth motion of DNA over the polylysine beads stretched the DNA taut and lifted the chain above the surface by the 4 μm silica beads as visualized under the microscope. The incident angle of the excitation beam in objective-type TIRF (total internal reflection fluorescence) was adjusted to a sub-critical angle in order to image the samples a few microns above the surface; this yields a low fluorescence background (Kad et al., 2010). To-Pro-3 was used to confirm the formation of the DNA tightropes. After the DNA tightrope was formed, a 30 μL mixture with a final concentration of 1 nM Cy3-gp16 with 100 nM unlabeled gp16 in buffer B (25 mM Tris, pH 6.1, 25 mM NaCl, 0.25 mM MgCl2) was infused into the sample chamber for binding to the stretched DNA. After 30 min incubation, 30 μL of a solution containing anti-photobleaching reagents (Shu et al., 2007) was infused into the chamber in order to prevent photobleaching of less photostable fluorophores and to detect binding. Movies were taken after the chamber was washed with buffer C (25 mM Tris, pH 8, 25 mM NaCl, 0.25 mM MgCl2). A comparison was made of washings with buffer C, with and without 20 mM ATP. Since the DNA has been fixed by charge interactions and the protein fixed by binding affinity to the tethered DNA, washing does not remove pertinent material. Sequential images were acquired with a 0.2 s exposure time at an interval of 0.22 s, with a laser of 532 nm for excitation. The movies were taken for about 8 min, or until the Cy3 fluorophores lost their fluorescence due to photobleaching. Image J software was utilized to generate kymographs to show the displacement of the Cy3-gp16 spots along the DNA chains.
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