Stable binding of recA protein to duplex DNA. Unraveling a paradox

recA protein binding to duplex DNA is a complicated, multistep process. The final product of this process is a stably bound complex of recA protein and extensively unwound double-stranded DNA. recA monomers within the complex hydrolyze ATP with an apparent kcat of approximately 19-22 min-1. Once the final binding state is achieved, binding and ATP hydrolysis by this complex becomes pH independent. The weak binding of recA protein to duplex DNA reported in previous studies does not, therefore, reflect an intrinsically unfavorable binding equilibrium. Instead, this apparent weak binding reflects a slow step in the association pathway. The rate-limiting step in this process involves the initiation rather than the propagation of DNA binding and unwinding. This step exhibits no dependence on recA protein concentration at pH 7.5. Extension or propagation of the recA filament is fast relative to the overall process. Initiation of binding is pH dependent and represents a prominent kinetic barrier at pH 7.5. ATP hydrolysis occurs only after the duplex DNA is unwound. The binding density of recA protein on double-stranded DNA is approximately one monomer/4 base pairs. A model for this process is presented. These results provide an explanation for several paradoxical observations about recA protein-promoted DNA strand exchange. In particular, they demonstrate that there is no thermodynamic requirement for dissociation of recA protein from the heteroduplex DNA product of strand exchange.     

Elongation of duplex DNA by recA protein

recA protein, which is essential for the recombination process in Escherichia coli, was incubated in the presence of 5′-γ-thiotriphosphate with circular plasmid pBR_βG containing small single-stranded gaps. Stable complexes were formed which appear in the electron microscope as fibres with a diameter about five times that of naked DNA. Complex formation appears to be a co-operative process whereby the average rise per base-pair with respect to the fibre axis increases from 3·39 ± 0·08 Å to 5·20 ± 0·18 Å. The elongation of DNA by about 50% is compatible with an unwinding of the double helix and an intercalating mode of binding of recA and/or 5′-γ-thiotriphosphate to DNA.     

Translocation of Escherichia coli recA protein from a single-stranded tail to contiguous duplex DNA

Duplex DNA with a contiguous single-stranded tail was nearly as effective as single-stranded DNA in acting as a cofactor for the ATPase activity of recA protein at neutral pH and concentrations of MgCl2 that support homologous pairing. The ATP hydrolysis reached a steady state rate that was proportional to the length of the duplex DNA attached to a short 5' single-stranded tail after a lag. Separation of the single-stranded tail from most of the duplex portion of the molecule by restriction enzyme cleavage led to a gradual decline in ATP hydrolysis. Measurement of the rate of hydrolysis as a function of DNA concentration for both tailed duplex DNA and single-stranded DNA cofactors indicated that the binding site size of recA protein on a duplex DNA lattice, about 4 base pairs, is similar to that on a single-stranded DNA lattice, about four nucleotides. The length of the lag phase preceding steady state hydrolysis depended on the DNA concentration, length of the duplex region, and the polarity of the single-stranded tail, but was comparatively independent of tail length for tails over 70 nucleotides in length. The lag was 5-10 times longer for 3' than for 5' single-stranded tailed duplex DNA molecules, whereas the steady state rates of hydrolysis were lower. These observations show that, after nucleation of a recA protein complex on the single-stranded tail, the protein samples the entire duplex region via an interaction that is labile and not strongly polarized.     

Dissociation pathway for recA nucleoprotein filaments formed on linear duplex DNA

recA protein forms stable filaments on duplex DNA at low pH. When the pH is shifted above 6.8, recA protein remains stably bound to nicked circular DNA, but not to linear DNA. Dissociation of recA protein from linear duplex DNA proceeds to a non-zero endpoint. The kinetics and final extent of dissociation vary with several experimental parameters. The instability on linear DNA is most readily explained by a progressive unidirectional dissociation of recA protein from one end of the filament. Dissociation of recA protein from random points in the filament is eliminated as a possible mechanism by several observations: (1) the requirement for a free end; (2) the inverse and linear dependence of the rate of dissociation on DNA length (at constant DNA base-pair concentration); and (3) the kinetics of exposure of a restriction endonuclease site in the middle of the DNA. Evidence against another possible mechanism, ATP-mediated translocation of the filament along the DNA, is provided by a novel effect of the non-hydrolyzable ATP analog, ATP gamma S, which generally induces recA protein to bind any DNA tightly and completely inhibits ATP hydrolysis. We find that very low, sub-saturating levels of ATP gamma S completely stabilize the filament, while most of the ATP hydrolysis continues. If these levels of ATP gamma S are introduced after dissociation has commenced, further dissociation is blocked, but re-association does not occur. These observations are inconsistent with movement of recA protein along DNA that is tightly coupled to ATP hydrolysis. The recA nucleoprotein filament is polar and the protein binds the two strands asymmetrically, polymerizing mainly in the 5' to 3' direction on the initiating strand of a single-stranded DNA tailed duplex molecule. A model consistent with these results is presented.     

The distribution of Escherichia coli recA protein bound to duplex DNA with single-stranded ends

A short single-stranded tail on one end of an otherwise duplex DNA molecule enables recA protein, in the presence of ATP and MgCl2, to form a complex with the DNA which extends into the duplex portion of the molecule. Nuclease protection studies at a concentration of MgCl2 which permits homologous pairing showed that cleavage by restriction endonucleases at sites throughout the duplex region was inhibited, whereas digestion by DNase I was not affected. These results indicate that recA protein binds to the duplex portion of tailed DNA allowing access by DNase I to a random sample of the many sites at which it cleaves, but providing limited protection of the relatively rare restriction sites. Electron microscopy revealed that the recA nucleoprotein complex with duplex DNA is indeed a segmented or interrupted filament that, with time, extends further from the single-stranded tail into the duplex region. recA protein binding extended into the duplex region more rapidly for duplexes with 5' tails than for those with 3' tails. These observations show that recA protein translocates from a single-stranded region into duplex DNA in the form of a segmented filament by a mechanism that is not strongly polarized.     

General mechanism for RecA protein binding to duplex DNA

RecA protein binding to duplex DNA occurs by a multi-step process. The tau analysis, originally developed to examine the binding of RNA polymerase to promoter DNA, is adapted here to study two kinetically distinguishable reaction segments of RecA-double stranded (ds) DNA complex formation in greater detail. One, which is probably a rapid preequilibrium in which RecA protein binds weakly to native dsDNA, is found to have the following properties: (1) a sensitivity to pH, involving a net release of approximately one proton; (2) a sensitivity to salts; (3) little or no dependence on temperature; (4) little or no dependence on DNA length. The second reaction segment, the rate-limiting nucleation of nucleoprotein filament formation accompanied by partial DNA unwinding, is found to have the following properties: (1) a sensitivity to pH, involving a net uptake of approximately three protons; (2) a sensitivity to salts; (3) a relatively large dependence on temperature, with an Arrhenius activation energy of 39 kcal mol(-1); (4) a sensitivity to DNA topology; (5) a dependence on DNA length. These results contribute to a general mechanism for RecA protein binding to duplex DNA, which can provide a rationale for the apparent preferential binding to altered DNA structures such as pyrimidine dimers and Z-DNA.     

Kinetic studies of recA protein binding to a fluorescent single-stranded polynucleotide

Fluorescence spectroscopy was used to investigate the binding of Escherichia coli recA protein to a single-stranded polynucleotide. Poly(deoxy-1,N6-ethenoadenylic acid) was prepared by reaction of chloroacetaldehyde with poly(deoxyadenylic acid). The fluorescence of poly(deoxy-1,N6-ethenoadenylic acid) was enhanced upon recA protein binding. The kinetics of the binding process were studied as a function of several parameters: ionic concentration (KCl and MgCl2), pH, nature of the nucleoside triphosphate [adenosine 5'-triphosphate or adenosine 5'-O-(gamma-thiotriphosphate)], protein and polynucleotide concentrations, polynucleotide chain length, and order of sequential additions. The observed kinetic curves exhibited a lag phase followed by a slow binding process characteristic of a nucleation-elongation mechanism with an additional slow step governing the rate of the association process. The lag phase reflecting the nucleation step was not observed when the protein was first bound to the polynucleotide before addition of adenosine 5'-triphosphate. Adenosine 5'-triphosphate induced a dissociation of the recA protein, which was immediately followed by binding of the recA-adenosine 5'-triphosphate-Mg2+ ternary complex. The origin of this "mnemonic effect" and of the different kinetic steps is discussed with respect to protein conformational changes and aggregation phenomena.     

Escherichia coli recA protein protects single-stranded DNA or gapped duplex DNA from degradation by RecBC DNase

RecA- mutants of Escherichia coli extensively degrade their DNA following UV irradiation. Most of this degradation is due to the recBC DNase, which suggests that the recA gene is involved in the control of recBC DNase in vivo. We have shown that purified recA protein inhibits the endonuclease and exonuclease activities of recBC DNase on single-stranded DNA. The extent of inhibition is dependent on the relative concentration of recA protein, recBC DNase, and the DNA substrate; inhibition is greatest when the concentrations of DNA and recBC DNase are low and the concentrations of recA protein is high. At fixed concentrations of recA protein and recBC DNase, inhibition is eliminated at high concentrations of DNA. In the presence of adenosine 5'-O-(3-thiotriphosphate), an ATP analog which stabilizes the binding of recA protein to both single- and double-stranded DNA, recA protein is a more potent inhibitor of the nuclease activities on single-stranded DNA and is a weak inhibitor of the exonuclease activity on double-stranded DNA. Inhibition of the latter is enhanced by oligodeoxynucleotides, which stimulate the binding of recA protein to double-stranded DNA. In the presence of adenosine 5'-O-(3-thiotriphosphate), recA protein also inhibits the action of exonuclease I on single-stranded DNA and of lambda exonuclease on double-stranded DNA. These observations are most consistent with the idea that recA protein protects DNA from recBC DNase by binding to DNA. RecA protein also blocks the endonucleolytic cleavage of gapped circular DNA by recBC DNase. Since both recA protein and recBC DNase have the ability under certain conditions to unwind duplex DNA and to displace strands, we looked for evidence that their combined action would enlarge gaps but found no extensive enlargement. D-loops, a putative intermediate in genetic recombination, are effectively protected against the action of recBC DNase by the E. coli single strand binding protein and by recA protein in the presence of adenosine 5'-O-(3-thiotriphosphate).     

Exchange of recA protein between adjacent recA protein-single-stranded DNA complexes

We have examined the exchange of recA protein between stable complexes formed with single-stranded DNA (ssDNA) and (a) other complexes and (b) a pool of free recA protein. We have also examined the relationship of ATP hydrolysis to these exchange reactions. Exchange was observed between two different recA X ssDNA complexes in the presence of ATP. Complete equilibration between two sets of complexes occurred with a t1/2 of 3-7 min under a set of conditions previously found to be optimal for recA protein-promoted DNA strand exchange. Approximately 200 ATPs were hydrolyzed for every detected migration of a recA monomer from one complex to another. This exchange occurred primarily between adjacent complexes, however. Little or no exchange was observed between recA X ssDNA complexes and the free recA protein pool, even after several hundred molecules of ATP had been hydrolyzed for every recA monomer present. ATP hydrolysis is not coupled to complete dissociation or association of recA protein from or with recA X ssDNA complexes under these conditions.     

Continuous association of Escherichia coli single-stranded DNA binding protein with stable complexes of recA protein and single-stranded DNA

The single-stranded DNA binding protein of Escherichia coli (SSB) stimulates recA protein promoted DNA strand exchange reactions by promoting and stabilizing the interaction between recA protein and single-stranded DNA (ssDNA). Utilizing the intrinsic tryptophan fluorescence of SSB, an ATP-dependent interaction has been detected between SSB and recA-ssDNA complexes. This interaction is continuous for periods exceeding 1 h under conditions that are optimal for DNA strand exchange. Our data suggest that this interaction does not involve significant displacement of recA protein in the complex by SSB when ATP is present. The properties of this interaction are consistent with the properties of SSB-stabilized recA-ssDNA complexes determined by other methods. The data are incompatible with models in which SSB is displaced after functioning transiently in the formation of recA-ssDNA complexes. A continuous association of SSB with recA-ssDNA complexes may therefore be an important feature of the mechanism by which SSB stimulates recA protein promoted reactions.     

Genetic recombination: recA protein promotes homologous pairing between duplex DNA molecules without strand unwinding.

The recA protein of Escherichia coli promotes pairing in vitro between covalent circular duplex DNA and homologous circular duplex DNA containing a single stranded region. We have used a filter binding assay to investigate the frequency of homologous pairing between gapped and intact duplex DNA when unwinding of the free 3' and 5' ends of the gapped molecules was blocked. In order to obtain DNA without free ends, the gapped DNA was treated with trimethylpsoralen and 360 nm light so as to introduce about 6 crosslinks per DNA molecule and the double stranded regions on either side of the gaps were then digested up to the first crosslinks with exonuclease III and lambda exonuclease. This treatment did not diminish the frequency of homologous pairing, an observation which is difficult to reconcile with models for recombination requiring strand unwinding before pairing.     

Stabilization of recA protein-ssDNA complexes by the single-stranded DNA binding protein of Escherichia coli

In vitro recombination reactions promoted by the recA protein of Escherichia coli are enhanced by the single-stranded DNA binding protein (SSB). SSB affects the assembly of the filamentous complexes between recA protein and ssDNA that are the active form of the recA protein. Here, we present evidence that SSB plays a complex role in maintaining the stability and activity of recA-ssDNA filaments. Results of ATPase, nuclease protection, and DNA strand exchange assays suggest that the continuous presence of SSB is required to maintain the stability of recA-ssDNA complexes under reaction conditions that support their recombination activity. We also report data that indicate that there is a functional distinction between the species of SSB present at 10 mM magnesium chloride, which enhances recA-ssDNA binding, and a species present at 1 mM magnesium chloride, which displaces recA protein from ssDNA. These results are discussed in the context of current models of SSB conformation and of SSB action in recombination activities of the recA protein.     

Analysis of the kinetic and equilibrium binding of Ku protein to DNA.

The loading of Ku onto a DNA end in a double-strand DNA break is thought to be one of the first steps in the non-homologous DNA end joining (NHEJ) pathway, giving it an essential role in the maintenance of genomic integrity. The binding of Ku to DNA is complicated since DNA can accommodate multiple Ku subunits, which can translocate on the DNA strand. Furthermore, Ku may exhibit cooperativity in the loading process. Therefore, simple one- to-one kinetic models are unable to adequately simulate the process. However, through the use of computer simulation and curve-fitting, we are able to provide a comprehensive mechanistic model and rate constants that closely approximate experimental data for DNA molecules that bind one, two, and three Ku molecules under both kinetic and equilibrium conditions. The model obtains a best fit with Ku having a roughly seven-fold preference to bind to DNA ends rather than internal positions and is consistent with Ku having a strong preference of which face of the protein loads onto the DNA end.     

Properties of the high-affinity single-stranded DNA binding state of the Escherichia coli recA protein

The properties of the high-affinity single-stranded DNA (ssDNA) binding state of Escherichia coli recA protein have been studied. We find that all of the nucleoside triphosphates that are hydrolyzed by recA protein induce a high-affinity ssDNA binding state. The effect of ATP binding to recA protein was partially separated from the ATP hydrolytic event by substituting calcium chloride for magnesium chloride in the binding buffer. Under these conditions, the rate of ATP hydrolysis is greatly inhibited. ATP increases the affinity of recA protein for ssDNA in a concentration-dependent manner in the presence of both calcium and magnesium chloride with apparent Kd values of 375 and 500 microM ATP, respectively. Under nonhydrolytic conditions, the molar ratio of ATP to ADP has an effect on the recA protein ssDNA binding affinity. Over an ATP/ADP molar ratio of 2-3, the affinity of recA protein for ssDNA shifts cooperatively from a low-to a high-affinity state.     

Active nucleoprotein filaments of single-stranded binding protein and recA protein on single-stranded DNA have a regular repeating structure.

When E. coli single-stranded DNA binding protein (SSB) coats single-stranded DNA (ssDNA) in the presence of 1 mM MgCl2 it inhibits the subsequent binding of recA protein, whereas SSB binding to ssDNA in 12 mM MgCl2 promotes the binding of recA protein. These two conditions correspond respectively to those which produce 'smooth' and 'beaded' forms of ssDNA-SSB filaments. By gel filtration and immunoprecipitation we observed active nucleoprotein filaments of recA protein and SSB on ssDNA that contained on average 1 monomer of recA protein per 4 nucleotides and 1 monomer of SSB per 20-22 nucleotides. Filaments in such a mixture, when digested with micrococcal nuclease produced a regular repeating pattern, approximately every 70-80 nucleotides, that differed from the pattern observed when only recA protein was bound to the ssDNA. We conclude that the beaded ssDNA-SSB nucleoprotein filament readily binds recA protein and forms an intermediate that is active in the formation of joint molecules and can retain substantially all of the SSB that was originally bound.     

Specific versus nonspecific binding of cationic PNAs to duplex DNA

Although peptide nucleic acids (PNAs) are neutral by themselves, they are usually appended with positively charged lysine residues to increase their solubility and binding affinity for nucleic acid targets. Thus obtained cationic PNAs very effectively interact with the designated duplex DNA targets in a sequence-specific manner forming strand-invasion complexes. We report on the study of the nonspecific effects in the kinetics of formation of sequence-specific PNA-DNA complexes. We find that in a typical range of salt concentrations used when working with strand-invading PNAs (10-20 mM NaCl) the PNA binding rates essentially do not depend on the presence of nontarget DNA in the reaction mixture. However, at lower salt concentrations (<10 mM NaCl), the rates of PNA binding to DNA targets are significantly slowed down by the excess of unrelated DNA. This effect of nontarget DNA arises from depleting the concentration of free PNA capable of interacting with DNA target due to adhesion of positively charged PNA molecules on the negatively charged DNA duplex. As expected, the nonspecific electrostatic effects are more pronounced for more charged PNAs. We propose a simple model quantitatively describing all major features of the observed phenomenon. This understanding is important for design of and manipulation with the DNA-binding polycationic ligands in general and PNA-based drugs in particular.     

Strand-specific binding of RPA and XPA to damaged duplex DNA

The nucleotide excision repair (NER) pathway is a major pathway used to repair bulky adduct DNA damage. Two proteins, xeroderma pigmentosum group A protein (XPA) and replication protein A (RPA), have been implicated in the role of DNA damage recognition in the NER pathway. The particular manner in which these two damage recognition proteins align themselves with respect to a damaged DNA site was assessed using photoreactive base analogues within specific DNA substrates to allow site-specific cross-linking of the damage recognition proteins. Results of these studies demonstrate that both RPA and XPA are in close proximity to the adduct as measured by cross-linking of each protein directly to the platinum moiety. Additional studies demonstrate that XPA contacts both the damaged and undamaged strands of the duplex DNA. Direct evidence is presented demonstrating preferential binding of RPA to the undamaged strand of a duplex damaged DNA molecule.     

Multi-random binding molecular interactions: a general kinetic model

A kinetic model is suggested to account for the interactions of several ligands with a target whose molecule possesses several independent equivalent receptor sites for each ligand (multiligand multisite model). To analyse the problem, we shall derive solutions for three elementary situations: (a) interactions of a ligand with a mono-receptor site target molecule (monosite model); (b) interactions of several ligands with a target whose molecule possesses one receptor site for each ligand involved (multiligand model); (c) interactions of a ligand with a target whose molecule possesses several receptor sites of the same kind for this ligand (multisite model). Throughout this study, every ligand molecule is assumed to offer one binding site to the target. The main implications of the corresponding analytical solutions are discussed from a molecular point of view. The results cover a great many well-known aspects of the molecular interactions in various fields such as enzymology, endocrinology, radio-immunology and saturation analysis. As suggested by the inhibition patterns obtained, this model may therefore provide a new point of view to interpret the relevant phenomena. Furthermore, a kinetic approach to the generalized mass action law can be deduced from this model, and experimental conditions in which the isotopic dilution law applies are examined.     

Thermodynamic analysis of monoclonal antibody binding to duplex DNA.

A technique based on fluorescence polarization (anisotropy) was used to measure the binding of antibodies to DNA under a variety of conditions. Fluorescein-labeled duplexes of 20 bp in length were employed as the standard because they are stable even at low ionic strength yet sufficiently short so that both arms of an IgG cannot bind to the same duplex. IgG Jel 274 binds duplexes in preference to single-stranded DNA; in 80 mM NaCl Kobs for (dG)20.(dC)20 is 4.1x10(7) M-1 compared with 6.4x10(5) M-1 for d(A5C10A5). There is little sequence specificity, but the interaction is very dependent on ionic strength. From plots of log Kobs against log[Na+] it was deduced that five or six ion pairs are involved in complex formation. At low ionic strength,Kobs is independent of temperature and complex formation is entropy driven with DeltaH degrees obs and DeltaC degrees p,obs both zero. In contrast, in 80 mM NaCl DeltaC degrees p,obs is -630 and -580 cal mol-1K-1 for [d(TG)]10.[d(CA)]10 and (dG)20.(dC)20 respectively. IgG Jel 241 also binds more tightly to duplexes than single-stranded DNA, but sequence preferences were apparent. The values for Kobs to [d(AT)]20 and [d(GC)]20 are 2.7x10(8) and 1.3x10(8) M-1 respectively compared with 5.7x10(6) M-1 for both (dA)20. (dT)20 and (dG)20.(dC)20. As with Jel 274, the binding of Jel 241 is very dependent on ionic strength and four or five ionic bonds are involved in complex formation with all the duplex DNAs which were tested. DeltaC degrees p,obs for Jel 241 binding to [d(AT)]20 was negative (-87 cal mol-1K-1) in 80 mM NaCl but was zero at high ionic strength (130 mM NaCl). Therefore, for duplex-specific DNA binding antibodies DeltaC degrees p,obs is dependent on [Na+] and a large negative value does not correlate with sequence-specific interactions.