Structure of a RecA-DNA complex from linear dichroism and small-angle neutron-scattering in flow-oriented solution

Small-angle neutron-scattering (SANS) and ultraviolet linear dichroism (l.d.) were measured on identical samples of a RecA-double-stranded (ds) DNA complex, including cofactor adenosine 5'-O-thiotriphosphate, which were aligned by flow in two equivalent Couette devices made of niobium and silica, transparent to neutrons and to ultraviolet light, respectively. The SANS anisotropy indicates a modest orientation of the RecA-dsDNA fiber with the helix axis parallel to the flow field. By correlation with the corresponding l.d. of the DNA at the same orientation conditions, it is inferred that the DNA bases have a local orientation that is approximately perpendicular to the helix axis. By comparison with the worse orientation in single-stranded DNA-RecA, this conclusion suggests that the dsDNA in its complex with RecA is not strand separated, and may be accommodated as an essentially unperturbed, straight double helix running along the RecA polymer fiber. The SANS anisotropy is also found to support the assignment of a subsidiary intensity maximum as originating from the pitch of a helical fiber.     

Linear dichroism study of RecA-DNA complexes. Structural evidence and binding stoichiometries

In the presence of RecA single-stranded DNA (ssDNA) is found to exhibit flow linear dichroism (LD). In the absence of the cofactor ATP gamma S, the LD is positive with a maximum at about 280 nm, whereas in the presence of the cofactor ATP gamma S there is still a positive long-wavelength band, but a negative LD contribution centered at 260 nm indicates an orientation of the DNA bases preferentially perpendicular to the fiber axis. For the complex between ssDNA and RecA without ATP gamma S, essentially all LD derives from the protein (tryptophane) subunits indicating a structure in which the tryptophanes are preferentially parallel to the fiber axis of the complex while the DNA bases remain essentially unoriented. The magnitude of the LD increases with the RecA/DNA ratio to a point corresponding to approximately three nucleotides per RecA and decreases thereafter with excess of DNA. This indicates that there are two modes of binding with different stoichiometries.     

Binding stoichiometry and structure of RecA-DNA complexes studied by flow linear dichroism and fluorescence spectroscopy. Evidence for multiple heterogeneous DNA co-ordination

The interaction between RecA and DNA (in the form of unmodified single-stranded DNA, fluorescent single-stranded DNA and double-stranded DNA) is studied with linear dichroism and fluorescence spectroscopy. RecA is found to form a complex with single-stranded DNA with a binding stoichiometry of about four nucleotides per RecA monomer, in which the DNA bases appear to have a random orientation. Addition of ATP gamma S (a non-hydrolyzable analog of ATP) reduces the stoichiometry to about three nucleotides per RecA and causes the DNA bases to adopt an orientation preferentially perpendicular to the fiber axis. This complex can incorporate an additional strand of single-stranded DNA or double-stranded DNA, yielding a total stoichiometry of six nucleotides or three nucleotides and three base-pairs, respectively, per RecA. RecA, in the presence of ATP gamma S, is also found to interact with double-stranded DNA, with a stoichiometry of about three base-pairs per RecA. In all studied complexes, the tryptophan residues in the RecA protein are oriented with their planes preferentially parallel to the fiber axis, whereas in complexes involving ATP gamma S the planes of the DNA bases are oriented preferentially perpendicular to the fiber. This virtually excludes the possibility that the tryptophan residues are intercalated in the DNA helix. On the basis of these results, a model for the research of homology in the RecA-mediated, strand-exchange reaction in the genetic recombination process is proposed.     

Fibers of RecA protein and complexes of RecA protein and single-stranded phi X174 DNA as visualized by negative-stain electron microscopy

Monomers of purified RecA protein polymerize into helical fibers whose pitch is 7.2 nm to 7.5 nm and whose diameter is 11 nm. Either short (approximately 0.2 micron), single fibers, or bundles of aligned, longer fibers, can be formed preferentially, by varying the Mg2+ concentration. When RecA protein is bound to circular, single-stranded phi X174 DNA it forms helical fibers of different classes of contour lengths, ranging from 0.98 micron, depending upon the conditions of assembly. Two different helical pitches are found, one of 9.3 nm when the incubation buffer contains, besides the obligatory Mg2+, either ATP gamma S or ATP accompanied by single-strand binding protein, and one of 5.5 nm when the latter additives are omitted. Preformed fibers of the compact type can be converted to open ones of 9.3 nm pitch upon addition of ATP gamma S, even after the removal of unbound RecA. All signs of helicity are obliterated upon glutaraldehyde cross-linking except in those fibers whose assembly has been mediated by ATP gamma S. RecA protein and single-strand binding protein are competitively bound to single-stranded DNA. Composite complexes, however, are not encountered unless ATP gamma S is present. Otherwise, segments of DNA that are coated by one or the other protein are seen as separate regions. When the assembly of complexes of single-stranded DNA and RecA is mediated by single-strand binding protein and ATP, the axial separation between successive bases is 0 X 42 nm, somewhat greater than the axial distance between bases in one strand of duplex DNA in the B form. It is proposed that the bases of the single-stranded DNA in the complex are located near its inner surface, and that base-pairing with double-stranded DNA takes place following invasion of the central cavity of the complex.     

The cofactor ATP in DNA-RecA complexes is not intercalated between DNA bases

In an attempt to understand the role of ATP as a cofactor at the interaction of the RecA protein with DNA, we have studied the orientation geometries of the cofactor analogs adenosine 5′-O-(3-thiotriphosphate) (ATPγS) and guanosine 5′-O-(3-thiotriphosphate) (GTPγS) in RecA-DNA complexes using flow linear dichroism spectroscopy. Both cofactors promote the formation of RecA-DNA complexes of similar structure as judged from similar orientations of DNA bases. The DNA orientation was probed through the dichroism of the long-wavelength absorption of a DNA analog, poly(dεA). In this way differences between the dichroic spectra of the ATPγS–RecA–DNA and GTPγS-RecA-DNA complexes, observed in the shorter-wavelength region, are related to orientation at variations of the cofactor chromophores. The results show that the guanine plane of GTPγS is oriented parallel with the principal axis of the complex in contrast to the more perpendicular orientation of the DNA bases. This observation directly excludes the possibility that the cofactor could be intercalated between the DNA bases. This observation directly excludes the possibility that the cofactor could be intercalated between the DNA bases. The orientation of the adenine base of ATPγS, which may be similar to that of guanine of GTPγS albeit not exactly the same, is also inconsistent with intercalation. The possibility that the cofactor bound to the protein could be intercalated in DNA had been speculated from the observation that some DNA intercalators can induce RecA binding to DNA in the absence of cofator. There are probably no direct interactions between the cofator and the DNA bases and the role of the cofactor is probably related to interaction with RecA and a modification of protein conformation.     

Binding of RecA protein to single-stranded nucleic acids: spectroscopic studies using fluorescent polynucleotides

Binding of the recA gene product from Escherichia coli to single-stranded polynucleotides has been investigated using poly(dA) that have been modified by chloroacetaldehyde to yield fluorescent 1,N6-ethenoadenine (epsilon A) bases. A strong enhancement of the fluorescent quantum yield of poly(d epsilon A) is induced upon RecA protein binding. A 4-fold increase is observed in the absence of ATP or ATP gamma S and a 7-fold increase in the presence of either nucleoside triphosphate. RecA protein can bind to poly(d epsilon A) in the absence of both Mg2+ ions and ATP (or ATP gamma S) but Mg2+ ions are required to observe RecA protein binding in the presence of ATP (or ATP gamma S) at pH 7.5. ATP binding to the RecA-poly(d epsilon A) complex induces a dissociation of RecA from the polynucleotide followed by re-binding of [RecA-ATP-Mg2+] ternary complex. Whereas ATP-induced dissociation of RecA-poly(d epsilon A) complexes is a fast process, the subsequent binding reaction of [RecA-ATP-Mg2+] is slow. A model is proposed whereby [RecA-ATP-Mg2+] binding to poly(d epsilon A) involves slow nucleation and elongation processes along the polynucleotide backbone. The nucleation reaction is shown to involve at least a trimer or a tetramer. Polymerization of the [RecA-ATP-Mg2+] ternary complex stops when the polynucleotide is entirely covered with 6 +/- 1 nucleotides per RecA monomer. ATP hydrolysis then induces a release of RecA-ADP complexes from the polynucleotide template.     

Cofactor-induced orientation of the DNA bases in single-stranded DNA complexed with RecA protein. A fluorescence anisotropy and time-decay study

The structure of the RecA-single-stranded DNA complex was investigated by studying the fluorescence emission of poly(deoxy-1,N6-ethenoadenylic acid (poly(d epsilon A)), a fluorescent derivative of poly(dA), under various viscosity conditions. The fluorescence intensity and average lifetime of poly(d epsilon A) are much smaller than those of nonpolymerized monoethenonucleotides (1,N6-ethenoadenosine 5'-triphosphate and 1,N6-ethenoadenine deoxyribose 5'-monophosphate) at low viscosity and reflect intramolecular base-base collisions in the polymer. They considerably increased upon RecA binding, both in the presence and absence of cofactor ATP or adenosine 5'-O-(3-thiotriphosphate). This increase, as well as the increase in fluorescence anisotropy upon RecA binding, was very similar to that which resulted from sucrose addition to free poly(d epsilon A). These observations point to a decrease in the mobility of DNA bases upon RecA binding. In the presence of cofactor, the fluorescence features became independent of viscosity. This strongly suggests the absence of base motion of significant amplitude on the time scale of the fluorescence lifetime (about 10 ns). In the absence of cofactor, however, these features remained sensitive to viscosity, implying residual local motions of the bases. Such cofactor-dependent rigid attachment of DNA bases to stiff phosphate backbone could facilitate the search for homology between two DNA molecules during recombination.     

Complexes of RecA protein in solution. A study by small angle neutron scattering

RecA complexes on DNA and self-polymers were analysed by small-angle neutron scattering in solution. By Guinier analysis at small angles and by model analysis of a subsidiary peak at wider angles, we find that the filaments fall into two groups: the DNA complex in the presence of ATP gamma S, an open helix with pitch 95 A, a cross-sectional radius of gyration of 33 A and a mass per length of about six RecA units per turn, which corresponds to the state of active enzyme; and the compact form (bound to single-stranded DNA in the absence of ATP, or binding ATP gamma S in the absence of DNA, or just the protein on its own), a helical structure with pitch 70 A, cross-sectional radius of gyration 40 A and mass per length about five RecA units per turn, which corresponds to the conditions of inactive enzyme. The results are discussed in the perspective of unifying previous conflicting structural results obtained by electron microscopy.     

Coordination and internal exchange of two DNA molecules in a RecA filament in the presence of hydrolysing ATP. Information on ATP-RecA-DNA structure from linear dichroism spectroscopy.

Solution structure of complexes between DNA and recombinase RecA from Escherchia coli, in the presence of the physiological cofactor ATP, is probed by flow linear dichroism (LD) spectroscopy. A problem of ADP accumulation which promotes dissociation of DNA-RecA is circumvented by using an ATP-regenerating system. The LD features indicate that the local structure of the complex is very similar to that found in the presence of the non-hydrolysable analog of ATP, adenosine-5'-O-[gamma-thio]triphosphate (ATP[gamma S]); the DNA bases are oriented with their planes preferentially perpendicular to the long axis of the filament, while the indole chromophores of the two tryptophan residues of RecA are rather parallel to this reference direction. A much smaller overall amplitude of the LD spectrum, compared to ATP[gamma S], is interpreted as a result of fast dissociation of RecA due to hydrolysis of ATP, producing transiently naked DNA regions which act like flexible joints, diminishing the macroscopic orientation of the RecA filaments. However, the ATP hydrolysis is not found to prevent simultaneous accommodation of two non-complementary DNA molecules in the RecA complex, as judged from the LD behaviour upon successive addition of two different polynucleotides or modified DNA strands. A notable difference from corresponding complexes formed with ATP[gamma S] is that, in the presence of ATP hydrolysis, the order in which the two DNA molecules have been added is insignificant as judged from virtually identical resulting structures; this observation indicates that exchange of DNA occurs between the two DNA accommodation sites within the RecA filament.     

Structural data suggest that the active and inactive forms of the RecA filament are not simply interconvertible.

We have used electron microscopy to examine the two major conformational states of the helical filament formed by the RecA protein of Escherichia coli. The compressed filament, formed in the absence of a nucleotide cofactor either as a self-polymer or on a single-stranded DNA molecule, is characterized in solution by about 6.1 subunits per turn of a 76 A pitch helix, and appears to be inactive with respect to all RecA activity. The active state of the filament, formed with ATP or an ATP analog on either a single or double-stranded DNA substrate, has about 6.2 subunits per turn of a 94 A pitch helix. Measurements of the contour length of RecA-covered single-stranded DNA circles in ice, formed in the absence of nucleotide cofactor, indicate that each RecA subunit binds five bases, in contrast to the three bases or base-pairs per subunit in the active state. The different stoichiometries of DNA binding suggests that the two polymeric forms are not interconvertible, as has been suggested on biochemical grounds. A three-dimensional reconstruction of the inactive state shows the same general features as the 83 A pitch filament present in the RecA crystal. This structural similarity and the fact that the crystal does not contain ATP or DNA suggests that the crystal structure is more similar to the compressed filament than the active, extended filament.     

Two forms of RecA-single-stranded DNA-adenosine 5'-O-(3-thiotriphosphate) complexes with different activities for cleavage of phage phi 80 cI repressor

The kinetics of cleavage of the phage phi 80 cI repressor by Escherichia coli RecA protein were studied. The rate of cleavage in the presence of single-stranded DNA (ssDNA) and either adenosine 5'-O-(3-thiotriphosphate) (ATP gamma S), ATP or dATP is very low in the first hour at 37 degrees C and then increases sharply as incubation continues. The initial rate of cleavage of the repressor is greatly increased by incubating the RecA protein with ssDNA prior to addition of ATP gamma S and the repressor. However, when ATP gamma S is present during preincubation of RecA protein with ssDNA, the stimulatory effect of preincubation is greatly reduced. This difference in the effect of preincubation in two different conditions can be explained by formation of RecA-ssDNA-ATP gamma S complexes with different activities for cleavage of the repressor. The active complex is formed by binding of ATP gamma S to a complex of RecA protein and ssDNA. However, when the RecA protein binds to ATP gamma S prior to its binding to ssDNA, the resulting complex has no or only very weak cleavage activity toward the repressor.     

Effects of the Escherichia coli SSB protein on the binding of Escherichia coli RecA protein to single-stranded DNA. Demonstration of competitive binding and the lack of a specific protein-protein interaction

The effect of the Escherichia coli single-stranded DNA binding (SSB) protein on the stability of complexes of E. coli RecA protein with single-stranded DNA has been investigated through direct DNA binding experiments. The effect of each protein on the binding of the other to single-stranded DNA, and the effect of SSB protein on the transfer rate of RecA protein from one single-stranded DNA molecule to another, were studied. The binding of SSB protein and RecA protein to single-stranded phage M13 DNA is found to be competitive and, therefore, mutually exclusive. In the absence of a nucleotide cofactor, SSB protein binds more tightly to single-stranded DNA than does RecA protein, whereas in the presence of ATP-gamma-S, RecA protein binds more tightly than SSB protein. In the presence of ATP, an intermediate result is obtained that depends on the type of DNA used, the temperature, and the magnesium ion concentration. When complexes of RecA protein, SSB protein and single-stranded M13 DNA are formed under conditions of slight molar excess of single-stranded DNA, no effect of RecA protein on the equilibrium stability of the SSB protein-single-stranded DNA complex is observed. Under similar conditions, SSB protein has no observed effect on the stability of the RecA protein-etheno M13 DNA complex. Finally, measurements of the rate of RecA protein transfer from RecA protein-single-stranded DNA complexes to competing single-stranded DNA show that there is no kinetic stabilization of the RecA protein-etheno M13 DNA complex by SSB protein, but that a tenfold stabilization is observed when single-stranded M13 DNA is used to form the complex. However, this apparent stabilizing effect of SSB protein can be mimicked by pre-incubation of the RecA protein-single-stranded M13 DNA complex in low magnesium ion concentration, suggesting that this effect of SSB protein is indirect and is mediated through changes in the secondary structure of the DNA. Since no direct effect of SSB protein is observed on either the equilibrium or dissociation properties of the RecA protein-single-stranded DNA complex, it is concluded that the likely effect of SSB protein in the strand assimilation reaction is on a slow step in the association of RecA protein with single-stranded DNA. Direct evidence for this conclusion is presented in the accompanying paper.     

Visualization of recA protein and its association with DNA: a priming effect of single-strand-binding protein

A stoichiometric interaction of RecA protein with single-stranded DNA promotes homologous pairing of the single strand with duplex DNA and subsequent polar formation of a heteroduplex joint. Escherichia coli single-strand-binding (SSB) protein augments these reactions. Electron microscopic observations suggest structural bases for these interactions. Without triphosphates or DNA, RecA protein forms short linear filaments. With added circular single-stranded DNA, it forms extended circular filaments as well as collapsed and aggregated complexes of protein and DNA. The extended circular filaments are stiff and regular in appearance, contrasting with the convoluted structure formed by SSB protein and single-stranded DNA. Together, these two proteins form mixed filaments, which mostly resemble the extended structures containing RecA protein; moreover, SSB protein accelerates formation of extended filaments more than 50-fold, increasing the yield of these structures at the expense of heterogeneous aggregates. Other observations further define the interactions of RecA protein with partially single-stranded DNA, and the effects of ATP gamma S on the tendency of RecA protein to form polymeric structures even in the absence of DNA.     

Conformational flexibility of RecA protein filament: transitions between compressed and stretched states

RecA protein is a central enzyme in homologous DNA recombination, repair and other forms of DNA metabolism in bacteria. It functions as a flexible helix-shaped filament bound on stretched single-stranded or double-stranded DNA in the presence of ATP. In this work, we present an atomic level model for conformational transitions of the RecA filament. The model describes small movements of the RecA N-terminal domain due to coordinated rotation of main chain dihedral angles of two amino acid residues (Psi/Lys23 and Phi/Gly24), while maintaining unchanged the RecA intersubunit interface. The model is able to reproduce a wide range of observed helix pitches in transitions between compressed and stretched conformations of the RecA filament. Predictions of the model are in agreement with Small Angle Neutron Scattering (SANS) measurements of the filament helix pitch in RecA::ADP-AlF(4) complex at various salt concentrations.     

Characterization of the DNA binding activity of stable RecA-DNA complexes. Interaction between the two DNA binding sites within RecA helical filaments

The DNA-binding, annealing and recombinational activities of purified RecA-DNA complexes stabilized by ATP gamma S (a slowly hydrolysable analog of ATP) are described. Electrophoretic analysis, DNase protection experiments and observations by electron microscopy suggest that saturated RecA complexes formed with single- or double-stranded DNA are able to accommodate an additional single strand of DNA with a stoichiometry of about one nucleotide of added single-stranded DNA per nucleotide or base-pair, respectively, of DNA resident in the complex. This strand uptake is independent of complementarity or homology between the added and resident DNA molecules. In the complex, the incoming and resident single-stranded DNA molecules are in close proximity as the two strands can anneal in case of their complementarity. Stable RecA complexes formed with single-stranded DNA bind double-stranded DNA efficiently when the added DNA is homologous to the complexed strand and then initiate a strand exchange reaction between the partner DNA molecules. Electron microscopy of the RecA-single-stranded DNA complexes associated with homologous double-stranded DNA suggests that a portion of duplex DNA is taken into the complex and placed in register with the resident single strand. Our experiments indicate that both DNA binding sites within RecA helical filaments can be occupied by either single- or double-stranded DNA. Presumably, the same first DNA binding site is used by RecA during its polymerization on single- or double-stranded DNA and the second DNA binding site becomes available for subsequent interaction of the protein-saturated complexes with naked DNA. The way by which additional DNA is taken into RecA-DNA complexes shows co-operative character and this helps to explain how topological problems are avoided during RecA-mediated homologous recombination.     

recA protein filaments bind two molecules of single-stranded DNA with off rates regulated by nucleotide cofactor

To probe the role of nucleotide cofactor in the binding of single-stranded DNA to recA protein, we have developed a sedimentation assay using 5'-labeled 32P-poly(dT).recA.poly(dT) complexes sediment quantitatively when centrifuged at 100,000 x g for 45 min, whereas free poly(dT) remains in the supernatant. In the presence of ATP, between 6 and 7 bases cosediment per recA monomer; but when ADP is present or in the absence of added nucleotide cofactor, only 3-3.5 bases/recA monomer cosediment. In competition experiments in which recA.32P-poly(dT) complexes are incubated with unlabeled poly(dT), we again find 3-3.5 bases of labeled poly(dT) cosedimenting per recA monomer when no nucleotide cofactor is present. However, when the same experiment is performed with ATP, only half of the expected 6-7 bases of labeled poly(dT) remain bound to the DNA, demonstrating that half of the poly(dT) in the complex exchanges rapidly with free poly(dT), whereas the other half equilibrates slowly, like poly(dT) in the absence of nucleotide. The rate of exchange of the second more tightly bound poly(dT) is accelerated when ADP is present. Our observations are rationalized by a model in which each recA protein helical filament binds two strands of poly(dT) with a stoichiometry of 3-3.5 bases/recA monomer/strand.     

Competitive Binding Between Unmodified and Etheno DNA Provides Information About Structure and Stoichiometry of RECA-DNA Complexes

Abstract

RecA is found to form three different complexes with single-stranded DNA with stoichiometries of 3, 6, and  9 nucleotides per RecA monomer. In the first two complexes the DNA bases are oriented preferentially perpendicular to the fiber axis of the complex. The second complex is shown to involve two different DNA strands.     

Structure of RecX protein complex with the presynaptic RecA filament: Molecular dynamics simulations and small angle neutron scattering

Using molecular modeling techniques we have built the full atomic structure and performed molecular dynamics simulations for the complexes formed by Escherichia coli RecX protein with a single-stranded oligonucleotide and with RecA presynaptic filament. Based on the modeling and SANS experimental data a sandwich-like filament structure formed two chains of RecX monomers bound to the opposite sides of the single stranded DNA is proposed for RecX::ssDNA complex. The model for RecX::RecA::ssDNA include RecX binding into the grove of RecA::ssDNA filament that occurs mainly via Coulomb interactions between RecX and ssDNA. Formation of RecX::RecA::ssDNA filaments in solution was confirmed by SANS measurements which were in agreement with the spectra computed from the molecular dynamics simulations.     

Purification and characterization of the human Rad51 protein, an analogue of E. coli RecA.

In bacteria, genetic recombination is catalysed by RecA protein, the product of the recA gene. A human gene that shares homology with Escherichia coli recA (and its yeast homologue RAD51) has been cloned from a testis cDNA library, and its 37 kDa product (hRad51) purified to homogeneity. The human Rad51 protein binds to single- and double-stranded DNA and exhibits DNA-dependent ATPase activity. Using a topological assay, we demonstrate that hRad51 underwinds duplex DNA, in a reaction dependent upon the presence of ATP or its non-hydrolysable analogue ATP gamma S. Complexes formed with single- and double-stranded DNA have been observed by electron microscopy following negative staining. With nicked duplex DNA, hRad51 forms helical nucleoprotein filaments which exhibit the striated appearance characteristic of RecA or yeast Rad51 filaments. Contour length measurements indicate that the DNA is underwound and extended within the nucleoprotein complex. In contrast to yeast Rad51 protein, human Rad51 forms filaments with single-stranded DNA in the presence of ATP/ATP gamma S. These resemble the inactive form of the RecA filament which is observed in the absence of a nucleotide cofactor.     

Effects of Escherichia coli SSB protein on the single-stranded DNA-dependent ATPase activity of Escherichia coli RecA protein: Evidence that SSB protein facilitates the binding of RecA protein to regions of secondary structure within single-stranded DNA

The effect that Escherichia coli single-stranded DNA binding (SSB) protein has on the single-stranded DNA-dependent ATPase activity of RecA protein is shown to depend upon a number of variables such as order of addition, magnesium concentration, temperature and the type of single-stranded DNA substrate used. When SSB protein is added to the DNA solution prior to the addition of RecA protein, a significant inhibition of ATPase activity is observed. Also, when SSB protein is added after the formation of a RecA protein-single-stranded DNA complex using either etheno M13 DNA, poly(dA) or poly(dT), or using single-stranded phage M13 DNA at lower temperature (25 °C) and magnesium chloride concentrations of 1 mm or 4 mm, a time-dependent inhibition of activity is observed. These results are consistent with the conclusion that SSB protein displaces the RecA protein from these DNA substrates, as described in the accompanying paper. However, if SSB protein is added last to complexes of RecA protein and single-stranded M13 DNA at elevated temperature (37 °C) and magnesium chloride concentrations of 4 mm or 10 mm, or to poly(dA) and poly(dT) that was renatured in the presence of RecA protein, no inhibition of ATPase activity is observed; in fact, a marked stimulation is observed for single-stranded M13 DNA. A similar effect is observed if the bacteriophage T4-coded gene 32 protein is substituted for SSB protein. The apparent stoichiometry of DNA (nucleotides) to RecA protein at the optimal ATPase activity for etheno M13 DNA, poly(dA) and poly(dT) is 6(±1) nucleotides per RecA protein monomer at 4 mm-MgCl₂ and 37 °C. Under the same conditions, the apparent stoichiometry obtained using single-stranded M13 DNA is 12 nucleotides per RecA protein monomer; however, the stoichiometry changes to 4.5 nucleotides per RecA protein monomer when SSB protein is added last. In addition, a stoichiometry of four nucleotides per RecA protein can be obtained with single-stranded M13 DNA in the absence of SSB protein if the reactions are carried out in 1 mm-MgCl₂. These data are consistent with the interpretation that secondary structure within the natural DNA substrate limits the accessibility of RecA protein to these regions. The role of SSB protein is to eliminate this secondary structure and allow RecA protein to bind to these previously inaccessible regions of the DNA. In addition, our results have disclosed an additional property of the RecA protein-single-stranded DNA complex: namely, in the presence of complementary base-pairing and at elevated temperatures and magnesium concentrations, a unique RecA protein-DNA complex forms that is resistant to inhibition by SSB protein.