Indirect readout of DNA sequence at the primary-kink site in the CAP-DNA complex: recognition of pyrimidine-purine and purine-purine steps

The catabolite activator protein (CAP) bends DNA in the CAP-DNA complex, typically introducing a sharp DNA kink, with a roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positions 6 and 7 of the DNA half-site, 5'-A1A2A3T4G5T6G7A8T9C10T11 -3' ("primary kink"). In previous work, we showed that CAP recognizes the nucleotide immediately 5' to the primary-kink site, T6, through an "indirect-readout" mechanism involving sequence effects on energetics of primary-kink formation. Here, to understand further this example of indirect readout, we have determined crystal structures of CAP-DNA complexes containing each possible nucleotide at position 6. The structures show that CAP can introduce a DNA kink at the primary-kink site with any nucleotide at position 6. The DNA kink is sharp with the consensus pyrimidine-purine step T6G7 and the non-consensus pyrimidine-purine step C6G7 (roll angles of approximately 42 degrees, twist angles of approximately 16 degrees ), but is much less sharp with the non-consensus purine-purine steps A6G7 and G6G7 (roll angles of approximately 20 degrees, twist angles of approximately 17 degrees). We infer that CAP discriminates between consensus and non-consensus pyrimidine-purine steps at positions 6-7 solely based on differences in the energetics of DNA deformation, but that CAP discriminates between the consensus pyrimidine-purine step and non-consensus purine-purine steps at positions 6-7 both based on differences in the energetics of DNA deformation and based on qualitative differences in DNA deformation. The structures further show that CAP can achieve a similar, approximately 46 degrees per DNA half-site, overall DNA bend through a sharp DNA kink, a less sharp DNA kink, or a smooth DNA bend. Analysis of these and other crystal structures of CAP-DNA complexes indicates that there is a large, approximately 28 degrees per DNA half-site, out-of-plane component of CAP-induced DNA bending in structures not constrained by end-to-end DNA lattice interactions and that lattice contacts involving CAP tend to involve residues in or near biologically functional surfaces.     

FLP protein of 2 mu circle plasmid of yeast induces multiple bends in the FLP recognition target site

The FLP recombinase of the 2 mu plasmid of Saccharomyces cerevisiae binds to a target containing three 13 base-pair symmetry elements called a, b and c. The symmetry elements b and c are in direct orientation while the a element is in inverted orientation with respect to b and c on the opposite side of an eight base-pair core region. Each symmetry element acts as a binding site for the FLP protein. The FLP protein can form three different complexes with the FLP recognition target (FRT site) according to the number of elements within the site that are occupied by the FLP protein. Binding of FLP to the FRT site induces DNA bending. We have measured the angles of bends caused by the binding of the FLP protein to full and partial FRT sites. We find that FLP induces three types of bend in the FRT-containing DNA. The type I bend is approximately 60 degrees and results from a molecule of FLP bound to one symmetry element. The type II bend is greater than 144 degrees and results from FLP molecules bound to symmetry elements a and b. The type III bend is approximately 65 degrees and results from FLP proteins bound to symmetry elements b and c. Certain FLP proteins that are defective in recombination can generate the type I and type III bends but are impaired in their ability to induce the type II bend. We discuss the role of bending in FLP-mediated recombination.     

Cre induces an asymmetric DNA bend in its target loxP site

Cre initiates recombination by preferentially exchanging the bottom strands of the loxP site to form a Holliday intermediate, which is then resolved on the top strands. We previously found that the scissile AT and GC base pairs immediately 5' to the scissile phosphodiester bonds are critical in determining this order of strand exchange. We report here that the scissile base pairs also influence the Cre-induced DNA bends, the position of which correlates with the initial site of strand exchange. The binding of one Cre molecule to a loxP site induces a approximately 35 degrees asymmetric bend adjacent to the scissile GC base pair. The binding of two Cre molecules to a loxP site induces a approximately 55 degrees asymmetric bend near the center of the spacer region with a slight bias toward the scissile A. Lys-86, which contacts the scissile nucleotides, is important for establishing the bend near the scissile GC base pair when one Cre molecule is bound but has little role in positioning the bend when two Cre molecules are bound to a loxP site. We present a model relating the position of the Cre-induced bends to the order of strand exchange in the Cre-catalyzed recombination reaction.     

HU binding to bent DNA: a fluorescence resonance energy transfer and anisotropy study

HU, an architectural DNA-binding protein, either stabilizes DNA in a bent conformation or induces a bend upon binding to give other proteins access to the DNA. In this study, HU binding affinity for a bent DNA sequence relative to a linear sequence was investigated using fluorescence anisotropy measurements. A static bend was achieved by the introduction of two phased A4T4 tracts in a 20 bp duplex. Binding affinity for 20 bp duplexes containing two phased A-tracts in either a 5'-3' or 3'-5' orientation was found to be almost 10-fold higher than HU binding to a random sequence 20 bp duplex (6.1 vs 0.68 microM(-1)). The fluorescence technique of resonance energy transfer was used to quantitatively determine the static bend of the DNA duplexes and the HU-induced bend. DNA molecules were 5'-end labeled with fluorescein as the donor or rhodamine as the acceptor. From the efficiency of energy transfer, the end-to-end distance of the DNA duplexes was calculated. The end-to-end distance relative to DNA contour length (R/R(C)) yields a bend angle for the A-tract duplex of 45 +/- 7 degrees in the absence of HU and 70 +/- 3 degrees in the presence of HU. The bend angle calculated for the T4A4 tract duplex was 62 +/- 4 degrees after binding two HU dimers. Fluorescence anisotropy measurements reveal that HU binds in a 1:1 stoichiometry to the A4T4 tract duplex but a 2:1 stoichiometry to the T4A4 tract and random sequence duplex. These findings suggest that HU binding and recognition of DNA may be governed by a structural mechanism.     

Bulge loops used to measure the helical twist of RNA in solution.

Bulge loops are commonly found in helical segments of cellular RNAs. When incorporated into long double-stranded RNAs, they may introduce points of flexibility or permanent bend that can be detected by the altered electrophoretic gel mobility of the RNA. We find that a single An or Un bulge loop near the middle of a long RNA helix significantly retards the RNA during polyacrylamide gel electrophoresis if n greater than or equal to 2. The mobility of an RNA containing two A2 bulges various periodically with the number of base pairs between the bulges. We interpret this to mean that A2 bulges varies periodically with the number of base pairs between the bulges. We interpret this to mean that Z2 bulges form torsionally stiff bends in the helix; the gel mobility reaches a minimum when the total helical twist between the bulges rotates the arms of the molecule into a cis conformation. The gel mobilities are proportional to the predicted end-to-end distance of the RNA if the average RNA helical repeat is 11.8 +/- 0.2 bp/turn and there is no helical twist (3 +/- 9 degrees) associated with the bulge (data obtained in 0.15 M Na+). Other sizes and sequences of bulges have very different effects on RNA helix conformation and flexibility. U2 bulges bend the helix to a much smaller degree than A2 bulges, while longer A or U bulge sequences probably allow bends of 90 degrees or more; all of these may be fairly flexible joints.(ABSTRACT TRUNCATED AT 250 WORDS)     

DNA bending induced by high mobility group proteins studied by fluorescence resonance energy transfer.

The HMG domains of the chromosomal high mobility group proteins homologous to the vertebrate HMG1 and HMG2 proteins preferentially recognize distorted DNA structures. DNA binding also induces a substantial bend. Using fluorescence resonance energy transfer (FRET), we have determined the changes in the end-to-end distance consequent on the binding of selected insect counterparts of HMG1 to two DNA fragments, one of 18 bp containing a single dA(2) bulge and a second of 27 bp with two dA(2) bulges. The observed changes are consistent with overall bend angles for the complex of the single HMG domain with one bulge and of two domains with two bulges of approximately 90-100 degrees and approximately 180-200 degrees, respectively. The former value contrasts with an inferred value of 150 degrees reported by Heyduk et al. (1) for the bend induced by a single domain. We also observe that the induced bend angle is unaffected by the presence of the C-terminal acidic region. The DNA bend of approximately 95 degrees observed in the HMG domain complexes is similar in magnitude to that induced by the TATA-binding protein (80 degrees), each monomeric unit of the integration host factor (80 degrees), and the LEF-1 HMG domain (107 degrees). We suggest this value may represent a steric limitation on the extent of DNA bending induced by a single DNA-binding motif.     

Tet repressor binding induced curvature of tet operator DNA.

Tet repressor dimer binds to two tet operator sites spaced by 30 bp in the Tn10 encoded tet regulatory DNA. The effect of repressor binding on the gel mobility of circular permutated DNA fragments containing either one or both operator sequences is reported. The EcoRI induced bending of DNA is used to compare the results with other protein binding induced structural perturbations of DNA. Tet repressor bends a DNA fragment with a single tet operator to an angle of 42 degrees +/- 7 degrees. The apparent bend angle of DNA fragments containing the tandem tet operator arrangement occupied by two Tet repressor dimers turns out to be 52 degrees +/- 9 degrees. These results are interpreted with respect to the end to end distances of the bent DNA fragments. They indicate that either the intervening tet regulatory DNA between the operators or the bound operator sequences themselves contain additional perturbations from the canonical B-DNA structure. This finding is discussed in the light of previously obtained results from CD, neutron scattering, and electrooptical studies.     

Bending of synthetic bacteriophage 434 operators by bacteriophage 434 proteins.

The extent of DNA bending induced by 434 repressor, its amino terminal DNA binding domain (R1-69), and 434 Cro was studied by gel shift assay. The results show that 434 repressor and R1-69 bend DNA to the same extent. 434 Cro-induced DNA bends are similar to those seen with the 434 repressor proteins. On approximately 265 base pair fragments, the cyclic AMP receptor protein of Escherichia coli (CRP) produces larger mobility shifts than does 434 repressor. This indicates that the 434 proteins bend DNA to a much smaller extent than does CRP. The effects of central operator sequence on intrinsic and 434 protein-induced DNA bending was also examined by gel shift assay. Two 434 operators having different central sequences and affinities for 434 proteins display no static bending. The amount of gel shift induced by 434 repressor on these operators is identical, showing that the 434 repressor bends operators with different central sequences to the same extent. Hence, mutations in the central region of the operator do not influence the bent structure of the unbound or bound operator.     

Indirect readout of DNA sequence at the primary-kink site in the CAP-DNA complex: alteration of DNA binding specificity through alteration of DNA kinking.

The catabolite activator protein (CAP) sharply bends DNA in the CAP-DNA complex, introducing a DNA kink, with a roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positions 6 and 7 of the DNA half-site, 5'-A(1)A(2)A(3)T(4)G(5)T(6)G(7)A(8)T(9)C(10)T(11)-3' ("primary kink"). CAP recognizes the base-pair immediately 5' to the primary-kink site, T:A(6), through an "indirect-readout" mechanism involving sequence effects on the energetics of primary-kink formation. CAP recognizes the base-pair immediately 3' to the primary-kink site, G:C(7), through a "direct-readout" mechanism involving formation of a hydrogen bond between Glu181 of CAP and G:C(7). Here, we report that substitution of the carboxylate side-chain of Glu181 of CAP by the one-methylene-group-shorter carboxylate side-chain of Asp changes DNA binding specificity at position 6 of the DNA half site, changing specificity for T:A(6) to specificity for C:G(6), and we report a crystallographic analysis defining the structural basis of the change in specificity. The Glu181-->Asp substitution eliminates the primary kink and thus eliminates indirect-readout-based specificity for T:A(6). The Glu181-->Asp substitution does not eliminate hydrogen-bond formation with G:C(7), and thus does not eliminate direct-readout-based specificity for G:C(7).     

On the use of phasing experiments to measure helical repeat and bulge loop-associated twist in RNA.

In a phasing experiment, two bends are introduced into a long duplex RNA or DNA and the number of base pairs between them varied. When electrophoresed in a gel, the set of molecules may show a periodic variation in mobility that contains information about the twist associated with the bends and the intervening helix. We show how a set of three phasing experiments can be used to extract this information, and apply it to an RNA helix bend at the bulge sequence A2. The bulge introduces a negative (left-handed) twist of approximately 30 degrees; at low temperatures, it is mostly confined to the 5' side of the bulge. The apparent helical repeat of random sequence RNA measured in these experiments was 10.2 +/- 0.1 base pairs, an unexpectedly low value. It is likely that moderate curvative of the RNA helix axis (30-40 degrees over 80 bp) has affected the measurement.     

Saturation mutagenesis of a DNA region of bend. Base steps other than ApA influence the bend

A 60 base-pair region of a simian virus 40 DNA fragment was mutagenized to determine base-pairs that are critical for the fragment to bend. The site-directed mutagenesis saturated this region with all possible single base-pair substitutions. The mobility of each mutated fragment was measured by polyacrylamide electrophoresis at 4 degrees C and at 65 degrees C to assess the degree of bend. Four conclusions can be drawn. First, interruptions within the A tracts and changes in the phasing of the A tracts alter the degree of bend. Second, G tracts phased at a half-helical turn from an A tract are additive to the bend. Third, guanine residues in a nearest-neighbor contact with the A tracts modify the bend. Fourth, some mutations that do not obviously relate to the A tracts also alter the DNA bend and suggest clearly that base steps other than ApA are involved in sequence-directed DNA bends.     

Negative staining of myosin molecules

A reproducible method has been developed for the negative staining of myosin molecules. The dimensions of stained molecules are in close agreement with those obtained by metal shadowing. Sharp bends in the tail, indicative of hinge regions, were observed at two positions 44 nm and 76 nm from the head-tail junction. The tail was often ill-defined at the position of the first (44 nm) bend. The bend positions may be sites of proteolytic cleavage that result in the production of long and short myosin subfragment S2. About half the molecules exhibited bending to various degrees at one or both of these positions, but cases where the tail folded back on itself in a 180 degrees bend were comparatively rare (approximately equal to 10%). However, in the absence of EGTA, a large fraction of the molecules (approximately equal to 80%) exhibited 180 degrees bends. A small region, approximately 20 nm long, at the tip of the tail often appears to be significantly different from the rest. The heads are about 19 nm long and roughly pear-shaped. Although sometimes straight, more often they show a pronounced curvature. Both senses of curvature were observed, but those curved in a clockwise manner were the most common, indicating preferential binding of one side of the head to the carbon substrate. An analysis of the different combinations of head shapes in individual molecules indicates that each head can rotate independently around its long axis. No preferred angle of orientation between the two heads in a molecule, or between either head and the tail could be found. Substructure has been observed within the heads.     

Determination of the extent of DNA bending by an adenine-thymine tract

We determined the magnitude of the bend induced in DNA by an adenine-thymine tract by measuring the rate of cyclization of DNA oligonucleotides containing phased A tracts. A series of linear multimers with 2-bp single-stranded ends, in which the (A.T)6 tracts are separated by CG2-3C sequences and are positioned 10 and 11 bp apart alternately, were prepared from 21 bp long synthetic duplexed deoxyoligonucleotides. The cyclization rates of the multimers (105-210 bp) and the bimolecular association rate of the 84 bp long multimer were measured in the presence of DNA ligase. From the rate constants of the cyclization and bimolecular association reactions, ring closure probabilities were obtained for the multimers. The systematically bent molecules were simulated by Monte Carlo methods, and the ring closure probabilities were calculated for a given set of junction bend angles. By comparing the calculated values of ring closure probabilities to experimental values and adjusting the junction bend angles to fit experimental values, the extent of bending at the junctions (or the extent of bending for an adenine tract) was determined. We conclude that an A6 tract bends the DNA helix by 17-21 degrees.     

The binding of cyclic AMP receptor protein to two lactose promoter sites is not cooperative in vitro.

The lactose promoter-operator region of Escherichia coli contains two binding sites for cyclic AMP receptor protein (CAP), two for the lactose repressor, and two for RNA polymerase. The high density of binding sites makes cooperative interactions between these proteins likely. In this study, we used the gel electrophoresis mobility shift assay and binding partition analysis techniques to determine whether the secondary CAP site influences the binding of CAP to the principal CAP site in the lactose promoter when both are present on a linear DNA molecule. Such an effect could occur through the formation of a bridged DNA-CAP-DNA structure, through the interaction of CAP molecules bound to each of the sites, or through allosteric effects caused by CAP-mediated DNA bending. We found, however, that the interaction of CAP with these sites was not cooperative, indicating that CAP sites 1 and 2 bind CAP in an independent manner.     

Identification of the DNA-binding domain of the FLP recombinase

We have subjected the FLP protein of the 2-micron plasmid to partial proteolysis by proteinase K and have found that FLP can be digested into two major proteinase K-resistant peptides of 21 and 13 kDa, respectively. The 21-kDa peptide contains a site-specific DNA-binding domain that binds to the FLP recognition target (FRT) site with an affinity similar to that observed for the native FLP protein. This peptide can induce DNA bending upon binding to a DNA fragment containing the FRT site, but the angle of the bend (approximately 24 degrees) is smaller in magnitude than that induced by the native FLP protein (60 degrees). The additional DNA bending induced by the interaction between two native FLP molecules bound to the FRT site is not observed with the 21-kDa DNA-binding peptide. Amino-terminal sequencing has been used to map this peptide to an internal region of FLP that begins at residue Leu-148. It is likely that the DNA-binding peptide includes the catalytic site of the FLP protein.     

Topological measurement of an A-tract bend angle: variation of duplex winding

The rotational variant method of Lutter et al. was developed to measure the bend angle induced when a protein binds to DNA. To measure the intrinsic bend conferred by a sequence of six adenine bases (an A6 tract), the method was modified by relaxing at high temperature to remove the bend. We describe here an alternative approach that involves unwinding the duplex DNA between adjacent bends in plasmids containing tandemly repeated blocks of A-tracts. This method measures the topological difference contributed by adjacent bends when they are in two different rotational settings, and therefore does not require reference to a straight state. The interbend DNA was unwound by use of the intercalator chloroquine, or, alternatively, by raising the temperature in the relaxation reaction. The effect of this unwinding is to change the pitch of the superhelix of the tandem repeats from which the bend angle is measured. The result is a bend angle value that is consistent with that measured using the bend-straightening version of the method. This version offers several advantages that complement the conventional bent versus straight approach.     

Indirect readout of DNA sequence at the primary-kink site in the CAP-DNA complex: DNA binding specificity based on energetics of DNA kinking.

The catabolite activator protein (CAP) makes no direct contact with the consensus base-pair T:A at position 6 of the DNA half-site 5'-A(1)A(2)A(3)T(4)G(5)T(6)G(7)A(8)T(9)C(10)T(11)-3' but, nevertheless, exhibits strong specificity for T:A at position 6. Binding of CAP results in formation of a sharp DNA kink, with a roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positions 6 and 7 of the DNA half-site. The consensus base-pair T:A at position 6 and the consensus base-pair G:C at position 7 form a T:A/G:C step, which is known to be associated with DNA flexibility. It has been proposed that specificity for T:A at position 6 is a consequence of formation of the DNA kink between positions 6 and 7, and of effects of the T:A(6)/G:C(7) step on the geometry of DNA kinking, or the energetics of DNA kinking. In this work, we determine crystallographic structures of CAP-DNA complexes having the consensus base-pair T:A at position 6 or the non-consensus base-pair C:G at position 6. We show that complexes containing T:A or C:G at position 6 exhibit similar overall DNA bend angles and local geometries of DNA kinking. We infer that indirect readout in this system does not involve differences in the geometry of DNA kinking but, rather, solely differences in the energetics of DNA kinking. We further infer that the main determinant of DNA conformation in this system is protein-DNA interaction, and not DNA sequence.