Abstract
A member of the SF2 family of helicases, Escherichia coli RecQ is involved in the recombination and repair of double-stranded DNA breaks and single-stranded DNA (ssDNA) gaps. Although the unwinding activity of this helicase has been studied biochemically, the mechanism of translocation remains unclear. To this end, using ssDNA of varying lengths, the steady-state ATP hydrolysis activity of RecQ was analyzed. We find that the rate of ATP hydrolysis increases with DNA length, reaching a maximum specific activity of 38±2 ATP/RecQ/second. Analysis of the rate of ATP hydrolysis as a function of DNA length implies that the helicase has a processivity of 19±6 nucleotides on ssDNA, and that RecQ requires a minimal translocation site size of 10±1 nucleotides. Using the T4 phage encoded gene 32 protein (G32P), which binds ssDNA cooperatively, to decrease the lengths of ssDNA gaps available for translocation, we observe a decrease in the rate of ATP hydrolysis activity that is related to lattice occupancy. Analysis of the activity in terms of the average gap sizes available to RecQ on the ssDNA coated with G32P indicates that RecQ translocates on ssDNA on average 46±11 nucleotides before dissociating. Moreover, when bound to ssDNA, RecQ hydrolyzes ATP in a cooperative fashion, with a Hill coefficient of 2.1±0.6, suggesting that at least a dimer is required for translocation on ssDNA. We present a kinetic model for translocation by RecQ on ssDNA based on this characterization.
Helicases couple the hydrolysis of ATP to unidirectional movement on single-stranded DNA (ssDNA). Upon encountering double-stranded DNA (dsDNA), these ATP driven motors force the displacement of the opposite strand (1, 2), allowing essential metabolic processes such as DNA recombination, repair, and replication to proceed. Translocation on ssDNA also serves other biological roles such as displacing bound proteins to regulate pathways such as DNA recombination (3–5).
The RecQ helicase from E. coli is a Super-Family 2 (SF2) helicase involved in the repair and recombination of DNA (6, 7). This protein is the founding member of the RecQ protein family of helicases, which is a family of highly conserved motor proteins in bacteria and eukaryotes. recQ was identified as a gene that conferred resistance to thymine-less growth and was found to function in recombinational DNA repair by the RecF pathway (8). RecQ, in conjunction with RecJ, processes DNA at the site of a stalled replisome to allow daughter-strand gap repair and recombination-mediated restart of DNA replication (9). RecQ, a 3′ to 5′ helicase (10), and RecJ, a 5′ to 3′ exonuclease (11), can process double-strand breaks to produce 3′-terminated ssDNA (12). This ssDNA serves as the substrate for assembly of a RecA filament, which then finds homology in intact dsDNA and promotes pairing of the ssDNA to the homologous target.
RecQ has additional roles in DNA recombination and replication. RecQ can disrupt joint molecules both in vivo (13) and in vitro (12, 14). In addition, RecQ can function with Topoisomerase III (Topo III), a type I topoisomerase, to catenate and decatenate dsDNA (15, 16). This reaction can serve two potential functions: one is to dissolve double Holliday junctions formed during recombination (17–20), and the other is to decatenate converged replication forks (21).
In vitro, the RecQ helicase binds to and unwinds a variety of different DNA substrates (10, 14, 22, 23). DNA with an ssDNA tail, gapped DNA, blunt dsDNA and covalently closed dsDNA are all unwound by RecQ, indicating that the helicase can function on a variety of intermediates found in DNA metabolism. RecQ is one of the few helicases that can unwind covalently closed, circular DNA—showing that it does not require a DNA end to enter dsDNA (15, 24). The ssDNA binding protein (SSB) from E. coli interacts with RecQ and stimulates its helicase activity to the extent that RecQ can unwind plasmid-length DNA (21, 24, 25).
Initially, helicase assays performed with plasmid DNA suggested a nearly stoichiometric mechanism for unwinding dsDNA by RecQ (10, 22). In this mechanism, short patches of dsDNA are unwound by RecQ translocation over relatively short distances (24). However, unwinding of dsDNA is stimulated by SSB. In the presences of SSB, optimal unwinding requires 1 RecQ for every 30 base pairs, indicating that each helicase is capable of unwinding a region of DNA longer than its DNA binding site size (24, 26). Furthermore, experiments with dsDNA possessing a 3′-ssDNA tail show that RecQ alone can unwind dsDNA up to 25 base-pairs in length (27).
The translocation mechanism of RecQ, however, has not been studied in as great detail as the unwinding mechanism. Several assays, as well as models, exist for the study of translocation by helicases on ssDNA. Steady-state analysis of several helicases on ssDNA has revealed estimates of processivity, directionality, and sequence effects on translocation (28–30). Kinetic mechanisms of translocation can be elucidated from analysis of the steady-state ATP hydrolysis activity. To understand translocation by RecQ, we studied the steady-state behavior of its ssDNA-dependent ATP hydrolysis activity as a function of DNA length. We find that the activity of RecQ increases with longer lengths of ssDNA. Moreover, when studied on ssDNA that is coated with T4 gene 32 protein (G32P) to limit the size of ssDNA available for activity, ATP hydrolysis was reduced in a manner that is quantitatively consistent with RecQ translocation on the ssDNA gaps that were available. We present a model to describe the mechanism of translocation for RecQ.
EXPERIMENTAL PROCEDURES
Equations and Analysis
Equations 1 and 2 were fit using Prism v.5 (GraphPad Software) using a non-linear least squares (NLLS) fitting algorithm. Equation 3 was fit to the data using Scientist 3.0 (Micromath) by holding the parameters n, Kact, ω, and the DNA concentration fixed, while Vf and Kg were fit using NLLS. The numbers reported are the best fit value and the standard deviation for each parameter. The data are reported as the mean and standard deviation of 2–4 experimentally determined values.
DNA Substrates
All oligonucleotide substrates were purchased from Integrated DNA Technologies (IDT Coralville, IA) and purified by denaturing polyacrylamide gel electrophoresis (12%) using 8 M urea, followed by gel extraction, and then concentration by ethanol precipitation (31). The DNA concentrations were determined using the absorbance of thymidine at 267 nm and an extinction coefficient of 9,600 M−1 cm−1 (31). Poly dT was purchased from Amersham-Pharmacia, and had an average length of 312 nucleotides. An extinction coefficient of 8,520 M−1 cm−1 at 260 nm was used to determine the concentration of DNA in nucleotides (31). Plasmid DNA (pUC19) was purified by conventional alkaline-lysis followed by equilibrium ultracentrifugation in a CsCl-ethidium bromide gradient (31). Purified pUC19 was linearized with HindIII (New England BioLabs) for 1 hour at 37°C using the vendor’s recommended conditions, and purified by phenol extraction followed by ethanol precipitation. Agarose gel electrophoresis was used to verify that the DNA was completely digested by the restriction endonuclease. The DNA concentration was determined using an extinction coefficient of 6,600 M−1 cm−1 and measuring the absorbance at 260 nm (31).
Proteins
RecQ was purified as described (14). The concentration of RecQ was determined by measuring the absorbance at 280 nm and using an extinction coefficient of 1.48 × 104 M−1 cm−1 (14). G32P was purified as described (32). An extinction coefficient of 4.13 × 104 M−1 cm−1 was used to measure its concentration (32).
ATP hydrolysis assay
ATP hydrolysis was monitored continuously using a spectrophotometric method where pyruvate kinase couples the formation of ADP to the oxidation of NADH by lactate dehydrogenase (33). An HP8452 Spectrophotometer (Agilent Technologies) was used to measure the absorbance of NADH. Reactions were performed by adding 100 μL of reaction buffer consisting of 25 mM TrisOAc (pH 7.5), 1 mM Mg(OAc)2, 1 mM ATP, 1 mM phosphoenolpyruvate, 1 mM dithiothreitol, 25 units/mL pyruvate kinase, 25 units/mL lactose dehydrogenase, and 200 μM NADH unless otherwise noted to a quartz spectrophotometric cell (Starna Cells) at 37°. M13 ssDNA, poly dT, poly dA, or oligonucleotide DNA was added at the indicated concentration and incubated for 2 minutes in the reaction buffer. The reaction was started by adding RecQ protein to a final concentration of 100 nM. To measure the activity of RecQ using DNA coated with G32P, poly dT (2 μM) was first added to each cuvette. G32P was then added at the indicated binding density, which was calculated by using a site size of 7.5 nt and cooperativity of 1000 (34). After incubation for 2 minutes, RecQ (100 nM) was added to start the reaction. For the titrations with ATP, 100 nM RecQ and 0.3 μM dT30 (molecules) were added to a reaction buffer that did not contain ATP or Mg(OAc)2. To start the reaction, Mg(OAc)2 and then ATP was added to the solution in a 1:1 ratio at the indicated concentration. The slope of the linear region of each trace was calculated, and multiplied by a conversion factor of 1.02 × 10−4 μM−1 cm−1 to convert to units of nmoles (ATP)·s−1.
Electrophoretic mobility shift assays
Oligonucleotides were labeled with 32P using T4 polynucleotide kinase (New England Biolabs) at the 5′ end according to the manufacturers specifications. Unincorporated nucleotides were removed by a Micro-Spin G25 column (GE Healthcare). Binding of RecQ to short oligonucleotides (5 nM molecules) was carried out in a solution (15 μL) containing 25 mM TrisOAc pH 7.5, 1 mM dithiothreitol, and 1 mM Mg(OAc)2 with and without 1 mM ATPγS. RecQ (0–1000 nM monomer) was mixed with DNA for 5 minutes at 37°. The RecQ-DNA complexes were mixed with 3 μL of loading buffer (50% glycerol, 0.1% bromophenol-blue) and were quickly separated from free DNA using 6% (29:1 acrylamide:bisacrylamide ratio) polyacrylamide gel electrophoresis for dT52 and dT25, and 12% polyacrylamide gel electrophoresis for dT6 in TBE buffer (89 mM Tris-borate, 2 mM EDTA). Gels were dried on DE 81 paper (Whatman), exposed to a storage phosphor screen and scanned using a Storm imaging system (Molecular Dynamics). Quantification of free DNA at each concentration of RecQ was calculated using Image-QuaNT software (Version 5.2, G.E. Healthcare) and analyzed as described (35). The dissociation constant, Kd, for RecQ on each DNA substrate was determined by fitting the data to a one-site binding curve, , where Y is the fraction of DNA bound, Kd is the equilibrium dissociation constant, and Bmax is the maximum fraction of bound DNA. The value of Bmax was fixed to 1 (mol/mol).
RESULTS
Model that describes ATP hydrolysis by RecQ during translocation on ssDNA
A kinetic theory for the analysis of steady-state ATP hydrolysis by DNA translocases was elaborated by Young et al. (28). In this paper, several models were proposed that gave rise to characteristic dependencies on DNA length of the apparent affinity, or Km, (referred to as the Kact by Young et al.) and the maximum ATP hydrolysis rate. These models provide a useful framework for interpreting ATP hydrolysis and its relationship to the translocation of RecQ on ssDNA. As will be established experimentally below, the model that is depicted in Figure 1 (Scheme 1) is one that is applicable to RecQ. Free RecQ (E) has little or no ATP hydrolysis activity as compared to RecQ bound to ssDNA (E-DNAi where “i” indicates the position along the lattice and “n” is the length of ssDNA in nucleotides). Upon binding ssDNA with a rate constant k1, the helicase undergoes multiple rounds of ATP hydrolysis with rate, k, coupled to translocation. The enzyme moves in discrete steps with a forward rate constant, ki, for translocation. At each step, the helicase can also dissociate from internal DNA sites with a rate constant, k−1. Upon reaching the end of the lattice, the helicase ceases hydrolyzing ATP and dissociates with a rate constant, kd.
Scheme 1 can be condensed to Scheme 2, which collapses the translocation steps into a single species, E-DNA. In this simplified scheme, the apparent rate constant for translocation to the end of the ssDNA is represented by an average rate, kt. This average rate is derived by assuming an equal probability of RecQ binding along the length of ssDNA and averaging the rate constant ki over all bound species (28). The amount of ATP hydrolyzed by RecQ is directly proportional to the longevity of the E-DNA species, and hence, to the length of ssDNA. The results, which establish that the translocation of RecQ on ssDNA can be adequately described by the mechanism depicted in Scheme 2, follow.
The ATP hydrolysis activity of RecQ depends on the length of ssDNA
The rate of ATP hydrolysis by RecQ was measured as a function of DNA length using ssDNA that was composed solely of thymidine residues of length “n” in nucleotides (dTn). These substrates were used to prevent formation of DNA secondary structure. In Figure 2A, titrations using oligonucleotides of different lengths are shown. A hyperbolic dependence of the ATP hydrolysis rate on DNA concentration was observed. The data were fit to equation 1
(1) |
where Vmax is the maximal velocity of ATP hydrolysis, and Kact is the concentration of DNA at which the ATP hydrolysis activity is half of Vmax (28). The maximum velocity for ATP hydrolysis by RecQ increases as DNA length is increased (Figure 2A), however, the 6-mer oligonucleotide stimulated ATP hydrolysis poorly (Figure 2A, open diamonds). The dependence of the observed turnover number for ATP hydrolysis, kcat (Vmax/[RecQ]), and Kact on the length of DNA were plotted as a function of DNA length (Figures 2B and 2C, respectively). For substrates 12 nucleotides or longer, kcat increased in a hyperbolic fashion with DNA length; in contrast, Kact did not vary with DNA length above 12 nucleotides. The dependence of Vmax, but not Kact, on the DNA length is uniquely predicted by the kinetic model presented in Figure 1, which defines an ssDNA translocase that moves along DNA, hydrolyzing ATP with a uniform rate per step, until it reaches a DNA end whereupon it ceases ATP hydrolysis and dissociates with a distinct rate constant, kd (28). Consequently, the data in Figure 2B were fit to equation 2
(2) |
where Vf is the maximum specific activity; Kg the length of DNA at which the specific activity is one-half of Vf; n the length of the ssDNA substrate; and n0 is the minimum length of DNA for which stimulation of the ATP hydrolysis is observed. Equation 2 is a modification of the equation presented in Young and von Hippel, adding n0 to the equation to account for the minimum DNA length requirement for translocation. We added this parameter due to our observation that a 6-mer did not stimulate the ATP hydrolysis by RecQ; other helicases were also observed to require a minimum DNA length for translocation (36). Fitting of the data in Figure 2B to equation 2 yielded the values Vf = 38±2 s−1; Kg = 19±5 nucleotides; and n0 = 10±1 nucleotides (Table 1). This analysis reveals that after the minimum length of ~10 nts is exceeded, the midpoint for maximal stimulation of ATP hydrolysis by RecQ is ~19 nucleotides.
Table 1.
Substrate | Vf (s−1) | Kg (nucleotides) | n0 (nucleotides) |
---|---|---|---|
Oligonucleotides (dTn) | 38±2 | 19±5 | 10±1 |
G32P-Poly dT | 32±2 | 46±11 | -- |
The translocation parameters were determined from measurements of steady-state ATP hydrolysis on the indicated substrate. Values for Kg, Vf, and n0 were determined from a fit of equation 2 to the data in Figure 2 for dTn substrates, and from a fit of equation 3 to the data in Figure 5 for G32P-poly dT. All values reported are best fit values with the standard deviation from NLLS fitting
The ATP hydrolysis activity of RecQ shows little dependence on the DNA sequence but is cooperative with respect to ATP concentration
The experiments above measured ATP hydrolysis by RecQ using a homogenous DNA lattice. Normally, RecQ translocates and unwinds dsDNA with a heterogeneous base composition. To determine whether the activity of RecQ is dependent on DNA composition, we measured the steady-state parameters of RecQ using poly dT, poly dA, and M13 ssDNA. Figure 3 shows the titration data for each DNA substrate and the fits to equation 1 (solid curves). The values for each parameter are shown in Table 2. RecQ displays a larger Kact value for poly dA, and M13 ssDNA when compared with poly dT, showing that RecQ displays a modest compositional preference for DNA. The maximum rate of ATP hydrolysis, Vmax, was similar for poly dT, M13 ssDNA, and the dT-containing oligonucleotides; however, it increased slightly when poly dA was the substrate.
Table 2.
Substrate | Kact (μM nucleotides) | kcat (s−1) |
---|---|---|
Oligonucleotides (dTn) | 0.4±0.2 | 38±2 |
Poly dT | 0.14±0.02 | 32±1 |
M13 ssDNA | 0.27±0.04 | 38±2 |
Poly dA | 0.22±0.03 | 51±2 |
The parameters values for Kact and kcat were determined from a fit of equation 1 to the data in Figure 2 and Figure 3. For the DNA oligonucleotides, the Kact value reported is the average for all lengths above 12 nucleotides. All values reported are best fit values with the standard deviation from NLLS fitting.
We also examined the effect of the ATP concentration on ssDNA-dependent ATP hydrolysis by RecQ. Figure 4A shows the ATP hydrolysis activity of RecQ as a function of ATP concentration at a saturating concentration of dT30. The activity is sigmoidal with respect to the ATP concentration. The Hill equation was used to fit the data, and RecQ was determined to have an apparent Km of 51±4 μM, a kcat of 23±0.6 s−1, and a Hill coefficient of 2.1±0.3. The sigmoidal behavior of the ATP hydrolysis activity and the Hill coefficient implies that RecQ translocates as a dimer or larger on ssDNA.
Previously, the unwinding of dsDNA by RecQ was also seen to be cooperative in ATP concentration (with a Hill coefficient of 3.3 ± 0.3) implying that the unwinding species is a trimer or larger (24). We, therefore, tested whether the dsDNA-dependent ATP hydrolysis activity of RecQ also shows cooperative behavior with linear pUC19 dsDNA. In Figure 4B, it is clear that the rate of ATP hydrolysis by RecQ shows a sigmoidal dependence on ATP concentration, with Hill equation parameters of 116±5 μM for the Km; 19.0±0.6 s−1 for the kcat; and 5±1 for the Hill coefficient (solid curve). However, it is also evident from the fitting that although the curve passes through the data at the higher ATP concentration, it systematically deviates from the data at low ATP concentrations. Consequently, we also fit the ATP hydrolysis data to the Hill equation, while holding the Hill coefficient constant at 3, which is the value determined from the helicase assays. Such a constrained fit resulted in values of 114±9 μM for the Km and 19±0.7 s−1 for the kcat that are, within error, the same as for the unconstrained fit (Figure 4B, dotted curve), and it is evident that the dotted curve fits the data at low ATP concentration better than the solid line, but now deviates more at the higher ATP concentrations. Because of this systematic deviation, we cannot assign a Hill coefficient with certainty, but he closeness of the two fits using Hill coefficients of 3 and 5 indicates that a minimum of 3 to 5 monomers of RecQ are involved in the unwinding of dsDNA.
G32P blocks ATP hydrolysis by RecQ by limiting translocation on ssDNA
One drawback to the analysis of the ATP hydrolysis activity using short oligonucleotides is that the binding and hydrolysis activity of RecQ may be affected by the DNA ends. To see if the end effects of the short DNA substrates influence the activity of RecQ, we measured the ATP hydrolysis activity on a long ssDNA substrate (poly dT) coated with an ssDNA-binding protein. Provided that RecQ cannot displace the bound ssDNA-binding protein, an ssDNA-binding protein should block ssDNA binding sites and limit translocation, resulting in a decrease in the ATP hydrolysis activity (Figure 5A). We tested this possibility by using T4 phage-encoded gene 32 protein (G32P) because the average gap size and, thus, track length can be accurately calculated using the formalism of McGhee and von Hippel from its known equilibrium binding constants and cooperativity parameters (34, 37). Equation 3 describes the dependence of the ATP hydrolysis rate (V) on the concentration of DNA and ssDNA-binding protein (28).
(3) |
In equation 3, θ is the binding density (moles of ligand per moles of lattice divided by the site size of the enzyme); Vf is the maximum ATP hydrolysis activity; Kact is the concentration of DNA at which the velocity is one half of Vf; Kg is the length of DNA at which the ATP hydrolysis activity is half of Vf; and Gav is the average gap size. Gav is calculated using equation 4
(4) |
where θ is the binding density; ω is the cooperativity parameter; n is the site size of the single-strand DNA binding protein (in nucleotides) and R is given below.
Poly dT was incubated with increasing concentrations of G32P. With increasing binding density of G32P (θ), the ATP hydrolysis activity of RecQ decreased as shown in Figure 5B. The fact that that ATP hydrolysis by RecQ is decreased by 10-fold (32 to 3 s-1) when the binding density of the poly dT by G32P approaches saturation, implies that RecQ does not displace the bound G32P, consistent with an assumption of the model. The data were fit to equation 3, which determines the activity as a function of binding density. In the fits, the site size, n and cooperativity parameter, ω, were fixed using the values of 7.5 nucleotides and 1000 respectively, which were previously determined as the thermodynamic parameters describe the binding of G32P to poly dT (34). The non-linear least square fit of equation 3 is shown as a solid black curve, with corresponding parameters Vf and Kg of 32±2 s−1 and 46±11 nucleotides, respectively (Table 1). Additionally, for comparison, simulations are shown (dashed line) for the hypothetical cases of a translocase with a Kg (apparent processivity) of 10 nucleotides, 19 nucleotides, or 300 nucleotides. Given the assumptions and the many parameters involved, the best fit value for Kg determined by this independent procedure is quite close to that obtained from analysis of the ssDNA length-dependence of ATPase activity, although it is slightly larger.
RecQ does not bind short ssDNA
From the kinetic analysis, we observed that a 6-mer of ssDNA did not efficiently stimulate ATP hydrolysis; consequently, we wished to know whether the ATP hydrolysis activity of RecQ was not being activated by the 6-mer, or whether RecQ simply could not bind such a short oligonucleotide. To distinguish between these possibilities, we measured the affinity of RecQ for different oligonucleotide substrates using an electrophoretic mobility shift assay (Figure 6). We observed that although RecQ could bind and shift the mobility of these substrates, the complexes dissociated appreciably during electrophoresis; therefore, the free DNA in each lane was quantified (35). In the absence of ATP, we observed that RecQ binds to the longer oligonucleotide, dT52, with an apparent affinity (Kd = 170±10 nM) that is greater than for a shorter oligonucleotide, dT25, (Kd = 1000±100 nM), but that it did not bind to dT6 (Figure 6D–F). Addition of the non-hydrolysable ATP analog, adenosine 5′-O-(3-thio) triphosphate (ATPγS), (instead of ATP to permit an equilibrium measurement) did not detectably affect the already high apparent affinity for dT52 (Kd = 150±20 nM), but it did increase the affinity of RecQ for dT25 by 2.5-fold (Kd = 400±60 nM); there was still no detectable binding to dT6 (Figure 5A–C). The increase in the apparent affinity induced by ATPγS binding is consistent with the ~2-fold increase elicited by adenosine 5′-(beta, gamma-imido) triphosphate (AMPPNP) reported previously (26). Our results clearly show that RecQ does not bind a 6-mer with sufficient affinity to stimulate ATP hydrolysis.
DISCUSSION
Our analysis of the steady-state ssDNA-dependent ATP hydrolysis by RecQ is consistent with the translocation mechanism as depicted in Scheme 1. RecQ binds and translocates along the ssDNA, coupling ATP hydrolysis to each kinetic step. Upon reaching the end of the ssDNA, RecQ ceases to hydrolyze ATP, and then dissociates from the end with a distinct rate constant. This mechanism gives rise to the characteristic dependence of Vmax, but not Kact, on DNA length (28). In contrast, potential alternative mechanisms for translocation by RecQ that can be disregarded are distinguished by which of the two parameters, Vmax and Kact, depend on DNA length. If RecQ were to dissociate from the DNA end with the same rate constant as for dissociation from any internal site (i.e., k−1), then this mechanism would predict a decrease in Kact (i.e., an increase in apparent affinity) with increasing DNA length but no change in Vmax (28). On the other hand, if RecQ were to dissociate from the DNA end with a unique rate constant (i.e., kd) but, rather than ceasing ATP hydrolysis in this state it continued hydrolyzing ATP unproductively at the end, then such a mechanism would result in both Vmax and Kact being dependent on the DNA length (28, 30). Therefore, based on our observation that Vmax, but not Kact, is dependent on the length of DNA, we conclude that RecQ translocates via the mechanism depicted in Scheme 1.
The data and our analysis indicate that RecQ translocates with modest processivity. In deriving equation 2, the parameter Kg can be expressed as the rate constant for translocation and dissociation (28), as given by equation 5.
(5) |
Thus, Kg is proportional to the ratio of the translocation rate constant, ki, and the dissociation rate constant, k−1, providing an estimate for the processivity of RecQ. The value for Kg indicates that RecQ moves on average 19±6 nucleotides before dissociating from ssDNA. In addition, analysis of the ATP hydrolysis activity on G32P-coated ssDNA indicates that the helicase translocates 46±11 nucleotides before dissociating. This independent determination of the processivity is higher than the value determined from the titration with oligonucleotides. This difference in the values implies either that DNA ends may influence the binding to and translocation on ssDNA by RecQ or that dissociation from an ssDNA gap defined by bound G32P may be kinetically different than dissociation from an ssDNA end. All assumptions considered, the values are quite compatible, and they are similar to the value for the average number of nucleotides translocated by RecQ determined of 36±2 nucleotides determined from the pre-steady state kinetic experiments (38).
From the ssDNA length-dependence, we observed that stimulation of ATP hydrolysis activity of RecQ requires approximately 10 nucleotides. This value is in reasonable agreement with previous studies measuring ATP hydrolysis activity that showed RecQ bound to ssDNA with a site size of 6 nucleotides (24). In comparison, UvrD requires a length of 8 nucleotides for translocation, whereas PcrA requires only 5 nucleotides (39, 40). In our experiments, a 6-mer (dT6) slightly stimulated the ATP hydrolysis activity of RecQ. On the other hand, the 12-mer, dT12, stimulated ATP hydrolysis activity in a hyperbolic fashion. Electrophoretic mobility shift assays showed that RecQ binds shorter lengths of ssDNA poorly compared to longer ones: RecQ cannot bind dT6 either in the absence or presence of the non-hydrolysable ATP analogue ATPγS. The translocation site size of 10 nucleotides may reflect a minimum binding site size of the helicase on ssDNA (26). A similar translocation site size was determined for UvrD in kinetic studies (41). In seeming contradiction, pre-steady-steady translocation assays show that RecQ requires a minimum site of 34±4 nucleotides for translocation (38). But the electrophoretic mobility shift assays show that RecQ binds with a high apparent affinity (150–170 nM) to dT52 and that this affinity is unaffected by ATPγS. However, for dT25, the apparent affinity is much lower (~1 μM) in the absence of ATP, but in the presence of ATPγS, the apparent affinity increases to ~0.4 μM. These findings imply that in the pre-steady-state kinetic experiments, wherein RecQ is pre-mixed with ssDNA in the absence of ATP, the enzyme cannot bind to DNA shorter than 30 nucleotides and thus is quickly bound by quenching agent (heparin), rationalizing the kinetic observations.
The translocation processivity of RecQ (19–46 nucleotides) is low compared to the processivity of other helicases translocating on ssDNA, but it is also consistent with the amount of dsDNA unwound by RecQ under optimal stead-state conditions (30 base pairs per RecQ monomer) (24, 26). The superfamily 1 (SF1) helicases UvrD and PcrA translocate on average 700 and 300 nucleotides on ssDNA, respectively, before dissociating from ssDNA (41, 42). These values are ten-fold higher than the processivity of RecQ. On the other hand, the S. cerevisiae chromatin remodeling complex Isw2, a member of Superfamily 2, displays a processivity similar to that of RecQ (43). Isw2 was found to travel 20 nucleotides on ssDNA before dissociating. The similarity of the processivity of RecQ to another SF2 ssDNA translocase may reflect a structural and biochemical features shared by SF2, but not SF1, helicases. SF1 helicases bind ssDNA by making contacts with the phosphate backbone and individual base pairs (2, 44). On the other hand, SF2 helicases bind to ssDNA using primarily only the phosphate backbone.
Interestingly, the processivity of several SF2 translocases that translocate on dsDNA, rather than ssDNA, is very different when compared to RecQ. S. cerevisiae Rad54 and Tid1/Rdh54 are chromatin and protein-DNA remodeling complexes, and members of the SF2 superfamily. Rad54 translocates on average 10,000 base pairs, while Tid1 moves on average 5,000 base pairs, before dissociating from the dsDNA (45, 46). On the other hand, S. cerevisiae RSC, which is also remodels chromatin, has a processivity similar to RecQ, moving only 20 base pairs before dissociating (47). These examples underscore the mechanistic differences that arise between helicases within the same superfamily likely due to the role each protein plays in the cell.
We observed a Hill coefficient of 2.1±0.3 for the ATP hydrolysis stimulated by ssDNA, indicating that a minimum of 2 subunits of RecQ are involved in ssDNA translocation. In contrast, for dsDNA, the Hill coefficient is 3–5. Thus, the minimal size of RecQ for translocating on ssDNA is at least a dimer, whereas the minimal size for unwinding is at least a trimer and maybe even a pentamer or greater. Why oligomerization by a helicase is necessary for translocation ssDNA is unclear. The mechanism for translocation by Isw2 and RSC includes a slow step prior to steady-state ATP hydrolysis and movement (43, 47). A similar slow step is not observed with RecQ, indicating that binding to ssDNA and forming an oligomer is rapid and the kinetically slow step occurs during translocation (38). A dimer may be required to bind and translocate on ssDNA, while 3 dimers of RecQ may interact or coordinate to unwind dsDNA. Single-turnover experiments measuring the unwinding activity of RecQ on dsDNA substrates with an ssDNA tail show that while a monomer can unwind dsDNA, it cannot unwind more than 25 base pairs (27). These observations support our view that even though a monomer may be competent for DNA unwinding, an oligomeric form of RecQ is need for the efficient unwinding of longer tracts of dsDNA. Finally, these ideas derived, from ensemble data, are also consistent with recent single-molecule analysis of DNA unwinding by RecQ (48), further validating the general utility of the much simpler steady-state ensemble experiments.
Acknowledgments
We thank members of the Kowalczykowski laboratory for helpful comments, and especially Ichiro Amitani, James Graham, and Katsumi Morimatsu for their careful reading of this manuscript.
The abbreviations used are
- ATPγS
adenosine 5′-O-(3-thio)triphosphate
- AMPPNP
adenosine 5′-(beta, gamma-imido) triphosphate
- dsDNA
double-stranded DNA
- G32P
gene 32 protein
- SSB
single-stranded DNA binding protein
- ssDNA
single-stranded DNA
- Topo III
Topoisomerase III
Footnotes
This work was supported by National Institutes of Health grant GM41347 to S.C.K.; B.R. was supported in part by National Institutes of Health training grant T32-GM007377.
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