Nucleic Acids Research Advance Access originally published online on November 5, 2008
Nucleic Acids Research 2008 36(22):7059-7067; doi:10.1093/nar/gkn836
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Nucleic Acids Research, 2008, Vol. 36, No. 22 7059-7067
© 2008 The Author(s)
This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License (http://creativecommons.org/licenses/by-nc/2.0/uk/) which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.
Nucleic Acid Enzymes |
Reinitiated viral RNA-dependent RNA polymerase resumes replication at a reduced rate
1Kavli Institute of Nanoscience, Faculty of Applied Sciences, Delft University of Technology, Lorentzweg 1, 2628 CJ Delft, The Netherlands and 2Institute of Biotechnology and Department of Biological and Environmental Sciences, Viikki Biocenter, P.O. Box 56, 00014 University of Helsinki, Finland
*To whom correspondence should be addressed. Tel: +31 15 278 3219; Fax: +31 15 278 1202; Email: n.h.dekker{at}tudelft.nl
Received August 27, 2008. Accepted October 14, 2008.
| ABSTRACT |
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RNA-dependent RNA polymerases (RdRP) form an important class of enzymes that is responsible for genome replication and transcription in RNA viruses and involved in the regulation of RNA interference in plants and fungi. The RdRP kinetics have been extensively studied, but pausing, an important regulatory mechanism for RNA polymerases that has also been implicated in RNA recombination, has not been considered. Here, we report that RdRP experience a dramatic, long-lived decrease in its elongation rate when it is reinitiated following stalling. The rate decrease has an intriguingly weak temperature dependence, is independent of both the nucleotide concentration during stalling and the length of the RNA transcribed prior to stalling; however it is sensitive to RNA structure. This allows us to delineate the potential factors underlying this irreversible conversion of the elongation complex to a less active mode.
| INTRODUCTION |
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Template-directed polymerization of nucleotides (NTPs) is an essential process in all living entities. Accordingly, enzymes catalyzing these processes operate in both cellular organisms and in viruses. In RNA viruses, RNA-dependent RNA polymerases (RdRPs) are the essential catalytic components of the polymerization machinery. RdRPs are also encoded by numerous cellular organisms, where they initiate or amplify the regulatory mechanisms known as RNA silencing (1). The structure and reaction mechanisms of viral RdRPs display similarity with many other nucleic acid polymerases, but nonetheless incorporate subtle differences. For instance, viral RdRPs adopt the right hand-like conformation typical for numerous nucleic acid polymerases, but they display a distinct closed-hand conformation, rather than the more common open-hand structure (2,3).
Viral RdRPs are capable of carrying out two distinct reactions, replication and transcription. These reactions are completed in four steps: (i) template recognition and binding, (ii) initiation, (iii) elongation and (iv) termination. The binding of viral RdRPs to template RNA exhibits characteristically low binding constants (4,5), but binding may nonetheless be enhanced by specific nucleotide sequences and/or RNA secondary structures (6,7). During initiation and elongation, viral RdRPs perform a nucleotidyl transfer reaction to polymerize the complementary RNA strand (8). While RNA or protein primers may be required for initiation, most RdRPs initiate RNA synthesis de novo (3).
To date, the kinetic studies of viral RdRP mechanism have neglected the effect of viral RdRP stalling. Partial RNA products isolated from poliovirus- and tobacco mosaic virus-infected cells suggest that the RdRP indeed frequently stalls, leading to compromised processivity during RNA elongation in vivo (9). It has been suggested that viral RdRP pausing could be brought about by specific RNA sequences and secondary structures (9), and is likely a prerequisite for viral RNA recombination (10,11). Furthermore, rational drug design against viral RdRPs could benefit from the analysis of stalled viral RdRPs (12). Finally, while stalling of viral RdRPs has been utilized to separate the elongation and initiation stages of the replication and transcription reactions (13), the consequences of stalling on the elongation rates have not been examined.
To quantitatively study the effect of stalling on the kinetics of viral RdRPs, we have used the RdRP from bacteriophage
6 (
6 RdRP) as a model system (Figure 1A).
6 RdRP catalyzes primer-independent de novo RNA synthesis on single-stranded RNA (ssRNA) and double-stranded RNA (dsRNA) templates and elongates with high processivity (14). During replication, the single-stranded sense RNA strand [(+)RNA] serves as the template for conversion to a dsRNA genome (Figure 1B). In contrast, during transcription, the (–)RNA strand within the dsRNA genome serves as the template for a new (+)RNA strand, which leaves the original (+)RNA strand as a single-stranded by-product (Figure 1C). In both processes,
6 RdRP initiates exclusively at the free 3'-end of the template strand, which enters the
6 RdRP through the template tunnel leading from the polymerase surface to the active site in the center of the enzyme structure (Figure 1A). By contrast, internal initiation of the elongation complex is not thought to occur (Supplementary Figure S1) (15).
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Here, we measure the rate of RNA elongation by
6 RdRP and demonstrate that while it is possible to reinitiate the polymerase following stalling induced by nucleotide deprivation, the resulting elongation rate is drastically and irreversibly reduced. This was quantified by measuring the elongation rate of the reinitiated complex using gel electrophoresis. Neither the NTP concentration nor the length of the RNA synthesized prior to stalling had an effect on the rate reduction following reinitiation. We attribute the reduction in the elongation rate to a transition to a sub-optimal conformational state of the elongation complex, brought about by stalling, and demonstrate that the conversion to the sub-optimal conformational state depends on the structure of the RNA template. In addition to the potential biological importance of the stalling, in vitro studies of polymerases have used stalling to measure elongation rates (13,16–18). In light of our findings, it is important to design the experimental setup in a way that a possible reduction in the elongation rate due to stalling is taken into account. | MATERIALS AND METHODS |
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Purification of the recombinant RdRP from bacteriophage
6The NdeI–EcoRI restriction fragment from pEM2 plasmid (14) was transferred into a pET-28a(+) vector (Novagen, USA). The resultant plasmid pAA5 was propagated in Escherichia coli BL21(DE3) (19).
6 RdRP was expressed as previously described (14), except for 25 µg/ml kanamycin. The cells were harvested and resuspended in 50 mM Tris–HCl (pH 8.0), 300 mM NaCl, 1 mM imidazole and disrupted. The supernatant was loaded onto a Ni-NTA affinity column (Qiagen, Valencia, CA, USA). After two successive washes with imidazole buffers (10 mM and 20 mM),
6 RdRP was eluted in 50 mM Tris–HCl (pH 8.0), 300 mM NaCl, 250 mM imidazole. Further purification was done using HiTrapTM Heparin HP and Q HP columns (GE Healthcare, USA).
6 RdRP was eluted with a linear NaCl gradient (from 0.1 M–1 M NaCl) in 50 mM Tris–HCl (pH 8.0), 0.1 mM EDTA. The purified protein was stored in the elution buffer (containing 300 mM NaCl) at 4°C.
Preparation of RNA molecules
ssRNAs were obtained via in vitro run-off transcription using PCR-amplified sections of the pBB10 plasmid (20) as described previously (primers listed in Table S1) (21). To favor terminal incorporation of cytidine into the 3'-end of the transcripts used as templates for
6 RdRP, the transcription mixtures were supplemented with 20 mM CTP.
dsRNA molecules were obtained by hybridizing complementary ssRNAs in 0.5 x SSC (Promega, Madison, WI, USA) using a gradual-cool temperature program (21). dsRNA template for transcription reactions was obtained by hybridizing three RNA molecules (4 kb RNA, 1.3 kb RNA and 4 kb main RNA) in a molar ratio of 1:1:1. Alternatively, a molar ratio of 1:4 was used in hybridizations between longer and shorter complementary ssRNA molecules for calibration of the electrophoretic mobilities. All hybridized RNAs were purified as described in (21).
A kinetic study of elongation by reinitiation of stalled
6 RdRP
The elongation rate of
6 RdRP was typically assayed in a reaction mixture containing 80 nM RNA template, 2.6 µM
6 RdRP, 50 mM HEPES pH 7.9, 20 mM ammonium acetate, 5 mM MgCl2, 2 mM MnCl2, 0.1 mM EDTA pH 8.0, 0.1% Triton X-100, 5% (v/v) SuperaseIn, and 2.5 mM of each nucleotide. A 10-fold lower enzyme to RNA template ratio was tested and shown to have no effect on the kinetics of the reinitiated reaction (data not shown). Prior to the reactions, RNA was heat-denatured by incubation at 65°C for 15 min, followed by fast cooling to 4°C. The stalled reactions were initiated using only three NTPs (ATP, CTP, and GTP). The unstalled reactions were incubated in the absence of NTPs for the same time period. After 15 min incubation at temperature T1, the temperatures of the stalled and unstalled reactions were changed to temperature T2, and left to equilibrate for 5 min. The stalled
6ECs were reinitiated by adding UTP, and the unstalled reactions were initiated by the addition of all four NTPs. Aliquots were taken at different time points after the addition of missing nucleotides, mixed with EDTA to 45 mM final concentration, and placed on ice. The products were analyzed using 0.75% or 1.5% agarose gels for the transcription and replication reactions, respectively. The agarose gels were preloaded at 2 V/cm for 15 min, and the electrophoresis was carried out at 5 V/cm at 4°C. The reaction products were visualized with ethidium bromide staining. The electrophoretic mobilities of the RNA replication intermediates were compared to a 2-log DNA ladder calibrated using a series of RNA hybrids (Supplementary Data and Figure S2). For experiments including a heparin trap (13), 9 mg/ml heparin (Sigma-Aldrich, St. Louis, MO, USA) was added after the stalling reactions, and the reactions were incubated at 22°C for 5 min prior to the addition of UTP.
| RESULTS |
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Reinitiated
6EC replicates with a reduced rateIn replication, a
6 RdRP elongation complex (
6EC) can be stalled in vitro using a limited selection of NTPs and a template molecule in which the 3'-terminal region is devoid of one or more of the nucleotides (Figure 2A; for proof of stalling on short oligos, see Supplementary Data and Figure S3). Elongation can then be reinitiated by the addition of the missing NTP(s), yielding an entirely double-stranded product. To study the effect of stalling on the rate of
6 RdRP replication, we selected a 4193 nt long replication template (4 kb ssRNA) in which the first occurrence of adenine was 50 nt from the 3'-end. The stalled
6EC exhibited an electrophoretic mobility indistinguishable from that of free 4 kb ssRNA (Supplementary Figure S4). Following stalling and reinitiation by UTP addition, aliquots were collected at successive time points and analyzed on agarose gel (Figure 2B). After reinitiation, a fraction of the replication template retained the electrophoretic mobility of free 4 kb ssRNA (Supplementary Figure 2B, lanes 2–10), which corresponds to either free 4 kb ssRNA or to inactive stalled
6EC. The electrophoretic mobility of successfully reinitiated
6ECs decreased with time as
6 RdRP progressed along the 4 kb ssRNA (Figure 2B, lanes 2–10). Notably, the band corresponding to the reinitiated
6ECs stayed well-defined, suggesting that the stalled
6ECs reinitiated in a synchronized manner. Termination of the replication reaction was detected by a stabilization of the electrophoretic mobility of the reinitiated
6ECs (data not shown). This occurred between 30 min and 60 min after reinitiation, from which we deduce an overall kelong between 1.2 and 2.3 nt·s–1. (For the discussion of the measured rates please see Supplementary Data).
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A control experiment was carried out to measure the overall replication polymerization rate (kpoly) of unstalled
6 RdRP under identical reaction conditions (Figure 2C). To measure kpoly, the 4 kb ssRNA was first incubated with
6 RdRP for the same duration as above, but in the absence of NTPs. Subsequently, all four NTPs were simultaneously added and aliquots were taken at successive time points. At time zero, only free 4 kb ssRNA could be detected (Figure 2C, lane 1). In contrast to the reinitiated
6ECs, at later times distinct bands could only be detected for the free 4 kb ssRNA and the final replication product (4 kb dsRNA) (Figure 2C, lanes 2–10), consistent with an unsynchronized population of
6ECs in this experiment. The first appearance of 4 kb dsRNA product occurred 6 min after the addition of NTPs (Figure 2C, Lane 4), corresponding to a minimal kpoly of 12 nt s–1. Surprisingly, the observed kpoly is at least six-fold higher than kelong, despite the fact that kpoly is a composite of kelong and the rates of accompanying initial stages of replication (e.g.
6 RdRP binding and initiation of
6EC). This suggests that the randomly-initiated
6EC elongates considerably faster than the reinitiated
6EC.
An accurate determination of kelong and kpoly
To support this initial observation, we obtained a more quantitative determination of kelong and kpoly in the case of reinitiated and randomly initiated
6ECs, respectively. We converted the electrophoretic mobilities of the elongation intermediates of reinitiated
6EC to a number of replicated nucleotides by using a calibration curve relating the two quantities (Supplementary Data and Figure S2). We converted only the earlier time points in Figure 2B, because the decreasing differences in the electrophoretic mobilities in the later reaction stages precluded an accurate determination of the number of replicated nucleotides. The results show that the number of replicated nucleotides after reinitiation increased linearly with time, indicating that the reinitiated
6EC exhibited a constant kelong (Figure 3A, red points). kelong was deduced from the slope of the linear fit (Figure 3A, solid red line) and averaged 2 ± 1 nt s–1 (mean and standard deviation determined from six experiments).
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Independently, we determined an improved estimate for kpoly for randomly-initiated
6RdRP replication, by extrapolating the data to the minimum time
necessary for the conversion of a single 4 kb ssRNA to its 4 kb dsRNA product, as previously reported (14). For example, to extract the value of
from the data in Figure 2D, the normalized intensity of the band corresponding to 4 kb dsRNA was plotted as a function of polymerization time, and the experimental points were fitted to a straight line (Figure 3B, solid red line). The x-intercept of the linear fit yielded
= 287 ± 42 s, which corresponds to kpoly = 15 ± 3 nt s–1 (mean and standard deviation deduced from three experiments). These more accurate values of kelong and kpoly thus establish that the elongation rate of randomly-initiated
6EC exceeds that of reinitiated
6EC by nearly an order of magnitude.
kelong of the reinitiated
6EC is independent of temperature
To gain insight into the mechanisms underlying the observed rate reduction, we compared the temperature dependence of kelong and kpoly. To measure the temperature dependence of kelong, we first stalled
6EC at temperature T1 for 15 min, equilibrated for 5 min at temperature T2, and reinitiated the
6EC (Figure 2A). We first fixed T1 at 22°C and varied T2 (16°C, 22°C, or 30°C) (Supplementary Figure S5). Using calibration described above, we found that the number of replicated nucleotides by the reinitiated
6ECs increased linearly with time for all three T2 (Figure 3A, green, red and blue solid lines correspond to T2 = 16°C, T2 = 22°C, and T2 = 30°C, respectively). Surprisingly, we found kelong to be independent of T2 (kelong of 2 ± 1 nt s–1 for all three T2). The experiment was then repeated at different T1 (16°C and 30°C) (Supplementary Figure S5). Here, too, we found that kelong remained constant during replication and was unaffected by changes in T1. Furthermore, the data reveals that kelong is independent of T1. In summary, we can conclude that over the range tested, kelong of the reinitiated
6EC is independent of temperature.
For comparison, we applied the same temperature variation to the unstalled enzyme. As above, three different values of T1 and T2 were tested (16°C, 22°C, and 30°C for both T1 and T2) (Supplementary Figure S6). kpoly was determined by measuring
as in Figure 2D. At fixed T1 = 22°C, we found that kpoly increased with increasing T2, from 9 ± 4 nt s–1 at T2 = 16°C, to 15 ± 3 nt s–1 at T2 = 22°C, and finally to 43 ± 14 nt s–1 at T2 = 30°C (mean and standard deviation deduced from three experiments). No detectable changes in the measured kpoly were observed when T1 was changed to 16°C or 30°C (Supplementary Figure S6). A comparison of kelong and kpoly is revealing: first, kpoly is consistently greater than kelong over the entire temperature range probed (Figure 3C): the rate reduction is not a particularity of experiments performed at room temperature; in addition, in contrast to the temperature-insensitive kelong, the polymerization rate kpoly of randomly-initiated
6EC showed significant dependence on T2 (Figure 3C), from which we deduced an activation free energy for the rate-determining step of 24 kBT by fitting the data to an Arrhenius equation (solid line in Figure 3C).
kelong is insensitive to the nucleotide concentration during stalling and to the length of elongated RNA prior to stalling
To relate the observed differences between the kinetic profiles of reinitiated and randomly-initiated
6ECs to specific regions of
6RdRP structure, we investigated a number of factors that could affect the interactions within the
6EC. These experiments were performed at a fixed T1 and T2 of 22°C.
To determine whether the NTP concentration during stalling affected the rate of the reinitiated
6ECs, we varied it from 0–2.5 mM per NTP. The stalled
6ECs were reinitiated by the addition of a mixture of all four NTPs to bring the final concentration of each NTP after reinitiation to 2.5 mM, as above. Aliquots were collected at 4 min and 8 min after reinitiation and loaded on agarose gel (Supplementary Figure S7A). In the complete absence of NTPs during stalling, only the products of randomly-initiated
6ECs were detected, as expected (Figure 4A). As the NTP concentration during the stalling stage was increased from 0.2 mM to 0.6 mM, this remained the case: only the products of randomly-initiated replication were present, and no detectable slow population of reinitiated
6EC was observed (Figure 4A top, circles). However, once the NTP concentration exceeded 0.8 mM, the products of randomly-initiated replication were no longer observed; instead the slowly-migrating, distinct bands of elongation intermediates attributable to reinitiated
6ECs appeared (Figure 4A top, triangles). Concentrations of reinitiated
6ECs increased as the NTP concentration during stalling was further increased to 1.4 mM, but beyond 1.4 mM no further increase was detected. We note that little variation was observed between the electrophoretic mobilities of the reinitiated
6EC, indicating similar kelong (Supplementary Figure S7A).
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Finally, to absolutely confirm that the bands detected below 0.8 mM NTP concentration during stalling were indeed the products of randomly-initiated replication, the experiments were repeated in the presence of heparin following stalling (Supplementary Figure S7B). Heparin is known to inactivate free (i.e. unstalled) RNA polymerase (13), and can thus prevent random initiation after stalling. We indeed observed the products of randomly-initiated replication either entirely disappeared or were greatly reduced in the presence of heparin (Figure 4A bottom, circles). In contrast, the presence of heparin did not reduce the concentration of the reinitiated
6ECs; however, it decreased the nucleotide concentration during stalling at which successfully reinitiated
6ECs were detected (Figure 4A bottom, triangles). We can thus conclude that NTP concentration during the stalling stage affects the likelihood of forming stalled
6ECs, leaving the subsequent dynamics as captured by kelong entirely unaffected.
The site at which the
6EC stalls on the template strand determines the length of the dsRNA protruding from the
6 RdRP product tunnel (Figure 1B). To investigate the effect of the dsRNA length on the kelong of reinitiated
6EC, we synthesized replication templates with a stalling site at the third or seventh nucleotide. These replication templates were designed to stall
6EC in the presence of three NTPs (i.e. ATP, CTP, and GTP) and reinitiate by the addition of UTP, as in the case of 4 kb ssRNA. On all these templates, the number of replicated nucleotide increased linearly with the elongation time (Figure 4B), as observed previously. Similarly, the observed kelong were measured to be 2 ± 1 nt s–1 in all instances (mean and standard deviation deduced from three experiments). Thus, we find the dynamics of the reinitiated
6EC to be insensitive to the length of the elongated RNA prior stalling.
Kinetics of the reinitiated elongation complex during
6 RdRP transcription
Different secondary structures of replication and transcription templates may interact differently with
6 RdRP within the stalled
6ECs (Figure 1), as RNA secondary structure elements located in viral RNAs have been shown to regulate RdRP polymerization (22,23). To test the role of template secondary structure on
6EC kinetics after reinitiation, a 4 kb long transcription template was designed with a 50 nt long single-stranded sequence devoid of adenine at the 3'-end of the transcribed strand (Figure 5A). The design of the transcription template included a nick solely to facilitate separation of the template from the product on gel. After
6EC stalling and introduction of the missing UTP,
6EC can reinitiate yielding a branched elongation intermediates. At the end of transcription, a completely double-stranded 3 kb dsRNA (Product A) and partially double-stranded RNA (Product B) remained.
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Similarly to the above study of
6RdRP replication, we measured kelong of the reinitiated
6EC and kpoly of randomly initiated
6EC during transcription. First, kelong on the transcription template after reinitiation was assayed at three different T2 (16°C, 22°C or 30°C). The elongation intermediates could be readily observed and displayed a decreased electrophoretic mobility compared to the free transcription template or the stalled
6EC as a result of their higher molecular weight and branched structure (Supplementary Figure 5B). The electrophoretic mobility of Product A corresponds well to that of 2876 bp long dsRNA, and the electrophoretic mobility of Product B agrees with the value predicted by the previously constructed calibration curves of RNA hybrids (Supplementary Figure S2C). As in the replication reaction, an appreciable fraction of the transcription template binds
6 RdRP, stalls the
6EC, and enables the synchronized reinitiation of the stalled
6EC after UTP addition, as judged from the well-defined bands corresponding to the elongation intermediates (Figure 5B, lane 2). In these transcription experiments, the more complex structure of the elongation intermediates prevented determination of kelong from the electrophoretic mobilities of the reaction intermediates. Rather, kelong was determined by dividing the length of the transcribed template by the typical time required to complete transcription. This time was approximated by measuring the mid-point between time t1, when the Product A band was first detected, and time t2, when the intensity of the elongation intermediate was observed to decrease. We report that kelong during transcription was comparable to kelong during replication at the lowest T2 (1.6 ± 1.0 nt s–1 at T2 = 16°C) but increased somewhat at higher T2 (4.6 ± 1.5 nt s–1 at T2 = 22°C) and 5.6 ± 1.3 nt s–1 at T2 = 30°C (red circles in Figure 5D) (mean and standard deviation deduced from three experiments).
We then investigated the kinetics of transcription by randomly-initiated
6EC. In the transcription reaction with the unstalled
6EC, the transcription products could readily be observed (Figure 5C). However, no elongation intermediates were detected, due to a lack of synchrony in the population of
6ECs. We plotted the intensity of the Product A band as a function of the polymerization time and fitted the experimental points to a line. The
values obtained were used to determine kpoly as above. At T1 = 22°C, the kpoly obtained for the randomly-initiated transcription was 5 ± 2 nt s–1 at T2 = 16°C, kpoly = 12 ± 2 nt s–1 at T2 = 22°C, and kpoly = 11 ± 2 nt s–1 at T2 = 30°C (black squares in Figure 5D). We thus observe that the values of kelong are again consistently slower than the values of kpoly of the randomly-initiated
6 RdRP. However, the observed differences are less pronounced than in the case of the replication reaction. In addition, in transcription, the kelong and kpoly display similar temperature sensitivities, in contrast to the replication reaction, where considerable differences in the temperature trends were observed.
| DISCUSSION |
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We have established that a reinitiated
6EC displays a decreased kelong compared to a randomly-initiated
6EC. The reduced kelong of the reinitiated
6EC remained constant during the replication of at least the first 2.5 kb of the 4 kb ssRNA replication template (Figure 3A). Furthermore, our estimate of the time point at which replication of 4 kb ssRNA was complete (Figure 2B) yielded an overall elongation rate between 1.2 nt s–1 and 2.3 nt s–1, in a good agreement with the rate determined for the replication of the first 2.5 kb via fitting the electrophoretic mobilities of the replication intermediate (2 ± 1nt s–1). Thus, the reinitiated
6EC elongates with a reduced rate throughout the template, from which we conclude that the conversion undergone by
6EC during the stalling step is irreversible.
This irreversible conversion to the inhibited
6EC state must be promoted during stalling, as the initial stages prior to
6EC stalling proceeded similarly in both stalled and unstalled reactions. An upper limit for the time needed for the conversion to the inhibited
6EC state could be deduced from the shortest time required to observe a synchronized population of reinitiated
6ECs (2 min at T1 = 22°C; Supplementary Figure S8). Analysis of the temperature dependence of the reinitiated and randomly-initiated
6EC showed considerably different behaviour for the two complexes (Figure 3C). The kinetics of a randomly-initiated
6EC could be described well within an Arrhenius model and yielded activation energy of 24 kBT for polymerization. In contrast, the kinetics of a reinitiated
6EC showed little temperature dependence of the elongation rates, implying that the conversion event during the stalling step may be insensitive to temperature. The irreversible conversion was similarly insensitive to both the NTP concentration during stalling and the length of the replicated template before stalling (Figure 4).
It is interesting to consider the possible nature of this irreversible conversion. A comparison of replication and transcription revealed that inhibition of the reinitiated
6EC was appreciably greater with single- than double-stranded templates (Figures 3 and 5). This suggests that the template type has an effect on the conversion to the inhibited
6EC state. This may be akin to the regulation of activity observed for other nucleic acid polymerases via either specific (e.g. RNA hairpin-protein) or nonspecific (e.g. electrostatic, hydrophobic) interactions (24–26). The interactions between
6 RdRP and its template that are responsible for the conversion to the inhibited state do not appear to be related to a particular RNA secondary structure, as the template strands were denatured prior to stalling and were thus most likely present as an ensemble of different RNA folds stable under the applied reaction conditions. The fact that replication is affected more than transcription may suggest the nature of the nonspecific interactions involved (e.g. hydrophobic interactions promoted by the exposed bases of ssRNA). However, the fact that replication is affected more than transcription may also implicate other nonspecific interactions that occur with a higher probability in the case of ssRNA template simply as a consequence of its lower persistence length, which gives rise to a lower radius of gyration (27) and thus a higher local concentration of the template at the enzyme surface. Nonspecific RNA-
6 RdRP interactions may cause the template RNA to interfere with the different tunnels in the enzyme and impair their proper functioning (e.g. they might limit exchange of free NTPs in the NTP channel, exit of the dsRNA in the product tunnel, or entry of the template strand in the template tunnel), resulting in a decrease in the overall elongation rates. Alternatively, RNA-
6 RdRP interactions could trigger conformational changes within the
6RdRP that result in suboptimal reaction rates.
It is evident that complex enzymes such as
6 RdRPs are regulated through multiple mechanisms, and their sum total dictates both the enzyme rates. It is thus intriguing that even a simple stalling event can lead to considerable changes in enzyme dynamics. It remains to be seen whether the reduction in elongation rate after stalling is a general property of viral RdRPs. The arrest of the elongation complex could be biologically relevant during the viral life cycle, in which RNA replication and transcription are highly regulated (28). In addition, it could affect the frequency of RNA recombination and thus the adaptation of RNA viruses to their environment (10,11). More technically, many experiments have applied stalling protocols to measure elongation rates of polymerases (13,16–18). As shown here for
6 RdRP, these measurements may provide inaccurate values, in the absence of confirmation that the enzyme is unaffected by stalling. For example, when T7 RNA polymerase (T7 RNAP) was stalled and subsequently reinitiated, the resulting elongation rate was as low as 2 nt s–1 as judged from a study by Ferrari and co-workers (17). By contrast, unstalled T7 RNAP exhibited elongation rates that range from 40–400 nt s–1 (29–31). Finally, polymerases may not be the only enzymes whose activity can be regulated via stalling. For instance, Kowalczykowski and co-workers recently showed that RecBCD helicase switches lead motors in response to the stalling at a specific DNA sequence, similarly resulting in a rate reduction of motor translocation (32).
| SUPPLEMENTARY DATA |
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Supplementary Data are available at NAR Online.
| FUNDING |
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Nanoned, The Netherlands Organization for Scientific Research, and the European Science Foundation (grants to N.H.D.); the Finish Center of Excellence Program 2006-2011 (1213467 to D.H.B.), the Academy of Finland and Nanotechnology (700036 to D.H.B.); Helsinki Graduate School of Biotechnology and Molecular Biology (funding of A.P.A.). Funding for open access charge: The Netherlands Organization for Scientific Research.
Conflict of interest statement. None declared.
| ACKNOWLEDGEMENTS |
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We thank W. Kamping and R. Tarkiainen for their experimental work and R. Tuma for fruitful discussions.
| Footnotes |
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Present address: Andrea Candelli, Department of Physics and Astronomy, Vrije Universiteit, 1081 HV Amsterdam, The Netherlands
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