Solution structure of dAATAA and dAAUAA DNA bulges

The NMR structure analysis is described for two DNA molecules of identical stem sequences with a five base loop containing a pyrimidine, thymin or uracil, in between purines. These five unpaired nucleotides are bulged out and are known to induce a kink in the duplex structure. The dAATAA bulge DNA is kinked between the third and the fourth nucleotide. This contrasts with the previously studied dAAAAA bulge DNA where we found a kink between the fourth and fifth nucleotide. The total kinking angle is ~104° for the dAATAA bulge. The findings were supported by electrophoretic data and fluorescence resonance energy transfer measurements of a similar DNA molecule end-labeled by suitable fluorescent dyes. For the dAAUAA bulge the NMR data result in a similar structure as reported for the dAATAA bulge with a kinking angle of ~87°. The results are discussed in comparison with a rAAUAA RNA bulge found in a group I intron. Generally, the sequence-dependent structure of bulges is important to understand the role of DNA bulges in protein recognition.     

Effects of bulge composition and flanking sequence on the kinking of DNA by bulged bases

We recently showed that bulged bases kink duplex DNA, with the degree of kinking increasing in roughly equal increments as the number of bases in the bulge increases from one to four [Hsieh, C.-H., & Griffith, J.D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837]. Here we have examined the kinking of DNA by single A, C, G, or T bulges with different neighboring base pairs. Synthetic 30 base pair (bp) duplex DNAs containing 2 single-base bulges spaced by 10 bp were ligated head to tail, and their electrophoretic behavior in highly cross-linked gels was examined. All bulge-containing DNAs showed marked electrophoretic retardations as compared to non-bulge-containing DNA. Regardless of the sequence of the flanking base pairs, purine bulges produced greater retardations than pyrimidine bulges. Furthermore, C and T bulges produced the same retardations as did G and A bulges. Bulged DNA containing different flanking base pairs showed marked differences in electrophoretic mobility. For C-bulged DNA, the greatest retardations were observed with G.C neighbors, the least with T.A neighbors, and an intermediate amount with a mixture of neighboring base pairs. For A-bulged DNA, the retardations were greatest with G.C neighbors, less with T.A neighbors, even less with a mixture of neighboring base pairs, and finally least with C.G neighbors. Thus flanking base pairs affect C-bulged DNA and A-bulged DNA differently, and G.C and C.G flanking base pairs were seen to have very different effects. These results imply an important role of base stacking in determining how neighboring base pairs influence the kinking of DNA by a single-base bulge.     

Recognition of bulged DNA by a neocarzinostatin product via an induced fit mechanism

The binding of the wedge-shaped isostructural analogue of the biradical species of the chromphore of antitumor antibiotic neocarzinostatin to sequence-specific bulged DNAs results in alterations in ellipticity of the DNAs. Circular dichroism (CD) spectroscopic results suggest that the drug specifically recognizes bulges of DNA via a combination of conformational selection and induced fit, not by binding to a preorganized site. Analysis of circular dichroism spectra indicates that the degree of induced fit observed is primarily a consequence of optimising van der Waals contacts with the walls of the bulge cavity. The effective recognition of the bulge site on duplex DNA appears to depend to a significant extent on the bent groove space being flexible enough to be able to adopt the geometrically optimal conformation compatible with the wedge-shaped drug molecule, rather than involving 'lock and key' recognition. The spectroscopic results indicate a change of DNA conformation, consistent with an allosteric binding model. Spectroscopic studies with various bulged DNAs also reveal that the binding strength directly correlates with the stability of the bulge structures.     

Non-nearest-neighbor dependence of the stability for RNA bulge loops based on the complete set of group I single-nucleotide bulge loops

Fifty-nine RNA duplexes containing single-nucleotide bulge loops were optically melted in 1 M NaCl, and the thermodynamic parameters DeltaH degrees, DeltaS degrees, DeltaG 37 degrees, and TM for each sequence were determined. Sequences from this study were combined with sequences from previous studies [Longfellow, C. E., et al. (1990) Biochemistry 29, 278-285; Znosko, B. M., et al. (2002) Biochemistry 41, 10406-10417], thus examining all possible group I single-nucleotide bulge loop and nearest-neighbor sequence combinations. The free energy increments at 37 degrees C for the introduction of a group I single-nucleotide bulge loop range between 1.3 and 5.2 kcal/mol. The combined data were used to develop a model for predicting the free energy of a RNA duplex containing a single-nucleotide bulge. For bulge loops with adjacent Watson-Crick base pairs, neither the identity of the bulge nor the nearest-neighbor base pairs had an effect on the influence of the bulge loop on duplex stability. The proposed model for prediction of the stability of a duplex containing a bulged nucleotide was primarily affected by non-nearest-neighbor interactions. The destabilization of the duplex by the bulge was related to the stability of the stems adjacent to the bulge. Specifically, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. The stability of a duplex containing a bulged nucleotide adjacent to a wobble base pair also was primarily affected by non-nearest-neighbor interactions. Again, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. However, when one or both of the bulge nearest neighbors was a wobble base pair, the free energy increment for insertion of a bulge loop is dependent upon the position and orientation of the wobble base pair relative the bulged nucleotide. Bulge sequences of the type ((5'UBX)(3'GY)), ((5'GBG)(3'UU)) and ((5'UBU)(3'GG)) are less destabilizing by 0.6 kcal/mol, and bulge sequences of the type ((5'GBX)(3'UY)) and ((5'XBU)(3'YG)) are more destabilizing by 0.4 kcal/mol than bulge loops adjacent to Watson-Crick base pairs.     

DNA bending by the bulge defect

Comparative gel electrophoresis measurements were used to characterize DNA bending in molecules containing an extra adenosine on one strand, the so-called bulge defect. We used oligomers containing A6 tracts separated from the bulged base by varying numbers of nucleotides to determine the direction and magnitude of the bulge bend. Helix unwinding by the bulge was determined from the electrophoretic anomaly as a function of the size of the repeated monomers. We conclude that the bulge bend is 21 degrees +/- 3 degrees, primarily in the direction of tilt away from the bulged base. The total helical advance of the DNA at the bulge site is smaller than would be the case if the complementary T were present, corresponding to an unwinding by 25 degrees +/- 6 degrees. These values are in good agreement with the results of NMR and energy minimization studies of the bulged base in double-helical deoxyoligonucleotides [Woodson, S. A., & Crothers, D.M. (1988) Biochemistry 27, 3130-3141]     

Selective strand scission by intercalating drugs at DNA bulges

A bulge is an extra, unpaired nucleotide on one strand of a DNA double helix. This paper describes bulge-specific strand scission by the DNA intercalating/cleaving drugs neocarzinostatin chromophore (NCS-C), bleomycin (BLM), and methidiumpropyl-EDTA (MPE). For this study we have constructed a series of 5'-32P end labeled oligonucleotide duplexes that are identical except for the location of a bulge. In each successive duplex of the series, a bulge has been shifted stepwise up (from 5' to 3') one strand of the duplex. Similarly, in each successive duplex of the series, sites of bulge-specific scission and protection were observed to shift in a stepwise manner. The results show that throughout the series of bulged duplexes NCS-C causes specific scission at a site near a bulge, BLM causes specific scission at a site near a bulge, and MPE-Fe(II) causes specific scission centered around the bulge. In some sequences, NCS-C and BLM each cause bulge-specific scission at second sites. Further, bulged DNA shows sites of protection from NCS-C and BLM scission. The results are consistent with a model of bulged DNA with (1) a high-stability intercalation site at the bulge, (2) in some sequences, a second high-stability intercalation site adjacent to the first site, and (3) two sites of relatively unstable intercalation that flank the two stable intercalation sites. On the basis of our results, we propose a new model of the BLM/DNA complex with the site of intercalation on the 3' side (not in the center) of the dinucleotide that determines BLM binding specificity.(ABSTRACT TRUNCATED AT 250 WORDS)     

Analysis of the binding of p53 to DNAs containing mismatched and bulged bases

The tumor suppressor protein p53 modulates cellular response to DNA damage by a variety of mechanisms that may include direct recognition of some forms of primary DNA damage. Linear 49-base pair duplex DNAs were constructed containing all possible single-base mismatches as well as a 3-cytosine bulge. Filter binding and gel retardation assays revealed that the affinity of p53 for a number of these lesions was equal to or greater than that of the human mismatch repair complex, hMSH2-hMSH6, under the same binding conditions. However, other mismatches including G/T, which is bound strongly by hMSH2-hMSH6, were poorly recognized by p53. The general order of affinity of p53 was greatest for a 3-cytosine bulge followed by A/G and C/C mismatches, then C/T and G/T mismatches, and finally all the other mismatches.     

Kinking of RNA helices by bulged bases, and the structure of the human immunodeficiency virus transactivator response element.

We have used gel electrophoresis to show that the pyrimidine bulge of the HIV-1 TAR sequence causes a local bending of the helical axis. The TAR bulge caused a retardation in electrophoretic mobility in polyacrylamide gels. When this was placed adjacent to an additional bulged sequence in a linear RNA fragment, the mobility of the molecule varied sinusoidally with the spacing between the two bulges. Electrophoretic mobilities suggested that the TAR sequence context of the pyrimidine bulge causes a greater degree of axial kinking than in an equivalent randomly chosen sequence. Experiments in which an A5 bulge was progressively opposed by adenine bases inserted in the opposite strand showed that even a single opposed adenine markedly reduced electrophoretic mobility, i.e. axial bending, and two adenine bases reduced the mobility virtually to that of a normal duplex. We suggest that the pronounced kinking resulting from an unopposed bulge provides a particularly recognizable feature in RNA, and that this is the basis of the interaction between the HIV Tat protein and the TAR sequence.     

Crystal structure of an adenine bulge in the RNA chain of a DNA.RNA hybrid, d(CTCCTCTTC).r(gaagagagag)

Crystal structure of a DNA.RNA hybrid, d(CTCCTCTTC).r(gaagagagag), with an adenine bulge in the polypurine RNA strand was determined at 2.3 A resolution. The structure was solved by the molecular replacement method and refined to a final R-factor of 19.9% (Rfree 22.2%). The hybrid duplex crystallized in the space group I222 with unit cell dimensions, a = 46.66 A, b = 47.61 A and c = 54.05 A, and adopts the A-form conformation. All RNA and DNA sugars are in the C3'-endo conformation, the glycosyl angles in anti conformation and the majority of the C4'-C5' torsion angles in g+ except two trans angles, in conformity with the C3'-endo rigid nucleotide hypothesis. The adenine bulge is looped out and it is also in the anti C3'-endo conformation. The bulge is involved in a base-triple (C.g)*a interaction with the end base-pair (C9.g10) in the minor groove of a symmetry-related molecule. The 2' hydroxyl group of g15 is hydrogen bonded to O2P and O5' of g17, skipping the bulged adenine a16 and stabilizing the sugar-phosphate backbone of the hybrid. The hydrogen bonding and the backbone conformation at the bulged adenine site is very similar to that found in the crystal structure of a protein-RNA complex.     

Solution structure of a five-adenine bulge loop within a DNA duplex.

The three-dimensional solution structure of a DNA molecule of the sequence 5'-d(GCATCGAAAAAGCTACG)-3' paired with 5'-d(CGTAGCCGATGC)-3' containing a five-adenine bulge loop (dA(5)-bulge) between two double helical stems was determined by 2D (1)H and (31)P NMR, infrared, and Raman spectroscopy. The DNA in both stems adopt a classical B-form double helical structure with Watson-Crick base pairing and C2'-endo sugar conformation. In addition, the two dG/dC base pairs framing the dA(5)-bulge loop are formed and are stable at least up to 30 degrees C. The five adenine bases of the bulge loop are localized at intrahelical positions within the double helical stems. Stacking on the double helical stem is continued for the first four 5'-adenines in the bulge loop. The total rise (the height) of these four stacked adenines roughly equals the diameter of the double helical stem. The stacking interactions are broken between the last of these four 5'-adenines and the fifth loop adenine at the 3'-end. This 3'-adenine partially stacks on the other stem. The angle between the base planes of the two nonstacking adenines (A10 and A11) in the bulge loop reflects the kinking angle of the global DNA structure. The neighboring cytosines opposite the dA(5)-bulge (being parts of the bulge flanking base pairs) do not stack on one another. This disruption of stacking is characterized by a partial shearing of these bases, such that certain sequential NOEs for this base step are preserved. In the base step opposite the loop, an extraordinary hydrogen bond is observed between the phosphate backbone of the 5'-dC and the amino proton of the 3'-dC in about two-thirds of the conformers. This hydrogen bond probably contributes to stabilizing the global DNA structure. The dA(5)-bulge induces a local kink into the DNA molecule of about 73 degrees (+/-11 degrees ). This kinking angle and the mutual orientation of the two double helical stems agree well with results from fluorescence resonance energy transfer measurements of single- and double-bulge DNA molecules.     

Bulged adenosine influence on the RNA duplex conformation in solution

The RNA single bulge motif is an unpaired residue within a strand of several complementary base pairs. To gain insight into structural changes induced by the presence of the adenosine bulge on RNA duplex, the solution structures of RNA duplex containing a single adenine bulge (5'-GCAGAAGAGCG-3'/5'-CGCUCUCUGC-3') and a reference duplex with all Watson-Crick base pairs (5'-GCAGAGAGCG-3'/5'-CGCUCUCUGC-3') have been determined by NMR spectroscopy. The reference duplex structure is a regular right-handed helix with all of the attributes of an A-type helix. In the bulged duplex, single adenine bulge stacks into the helix, and the bulge region forms a well-defined structure. Both structures were analyzed by the use of calculated helical parameters. Distortions induced by the accommodation of unpaired residue into the helical structure propagate over the entire structure and are manifested as the reduced base pairs inclination and x-displacement. Intrahelical position of bulged adenine A5 is stabilized by efficient stacking with 5'-neighboring residues G4.     

Non-nearest-neighbor dependence of stability for group III RNA single nucleotide bulge loops

Thirty-five RNA duplexes containing single nucleotide bulge loops were optically melted and the thermodynamic parameters for each duplex determined. The bulge loops were of the group III variety, where the bulged nucleotide is either a AG/U or CU/G, leading to ambiguity to the exact position and identity of the bulge. All possible group III bulge loops with Watson–Crick nearest-neighbors were examined. The data were used to develop a model to predict the free energy of an RNA duplex containing a group III single nucleotide bulge loop. The destabilization of the duplex by the group III bulge could be modeled so that the bulge nucleotide leads to the formation of the Watson–Crick base pair rather than the wobble base pair. The destabilization of an RNA duplex caused by the insertion of a group III bulge is primarily dependent upon non-nearest-neighbor interactions and was shown to be dependent upon the stability of second least stable stem of the duplex. In-line structure probing of group III bulge loops embedded in a hairpin indicated that the bulged nucleotide is the one positioned further from the hairpin loop irrespective of whether the resulting stem formed a Watson–Crick or wobble base pair. Fourteen RNA hairpins containing group III bulge loops, either 3′ or 5′ of the hairpin loop, were optically melted and the thermodynamic parameters determined. The model developed to predict the influence of group III bulge loops on the stability of duplex formation was extended to predict the influence of bulge loops on hairpin stability.     

Solution structure of a trinucleotide A-T-A bulge loop within a DNA duplex.

We have synthesized an oligodeoxynucleotide duplex, d(G-C-A-T-C-G-A-T-A-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-C-G), with a three-base bulge loop (A-T-A) at a central site in the first strand. Nuclear Overhauser experiments (NOESY) in H2O indicate that the GC base pairs flanking the bulge loop are intact between 0 and 25 degrees C. Nuclear Overhauser effects in both H2O and D2O indicate that all bases within the bulge loop are stacked into the helix. These unpaired bases retain an anti conformation about their glycosidic bonds as they stack within the duplex. The absence of normal sequential connectivities between the two cytosine residues flanking the bulge site on the opposite strand indicates a disruption in the geometry of this base step upon insertion of the bulged bases into the helix. This conformational perturbation is more akin to a shearing apart of the bases, which laterally separates the two halves of the molecule, rather than the "wedge" model often invoked for single-base bulges. Using molecular dynamics calculations, with both NOE-derived proton-proton distances and relaxation matrix-calculated NOESY cross peak volumes as restraints, we have determined the solution structure of an A-T-A bulge loop within a DNA duplex. The bulged bases are stacked among themselves and with the guanine bases on either side of the loop. All three of the bulged bases are displaced by 2-3 A into the major groove, increasing the solvent accessibility of these residues. The ATA-bulge duplex is significantly kinked at the site of the lesion, in agreement with previously reported electron microscopy and gel retardation studies on bulge-containing duplexes [Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A 86, 4833-4837; Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840]. Bending occurs in a direction away from the bulge-containing strand, and we find a significant twist difference of 84 degrees between the two base pairs flanking the bulge loop site. This value represents 58% of the twist difference for base pairs four steps apart in B-DNA. These results suggest a structural mechanism for the bending of DNA induced by unpaired bases, as well as accounting for the effect bulge loops may have on the secondary and tertiary structures of nucleic acids.     

Specific binding of 2-amino-1,8-naphthyridine into a single guanine bulge as evidenced by photooxidation of GG doublet

Photoirradiation of 2-amino-1,8-naphthyridines in the presence of duplex DNA containing the GG doublet opposite a single bulge was examined. After hot piperidine treatment, DNA cleavage was observed preferentially at the GG opposite a single bulge. The cleavage efficiency was highly dependent on the nature of bulged base. The G cleavage at the GG opposite a single G bulge was exceptionally weak, suggesting an intercalative binding of 2-amino-1,8-naphthyridine chromophore into the GG step.     

Non-nearest-neighbor dependence of the stability for RNA group II single-nucleotide bulge loops

Thirty-one RNA duplexes containing single-nucleotide bulge loops were optically melted in 1 M NaCl, and the thermodynamic parameters ΔH°, ΔS°, ΔG°(37), and T(M) for each sequence were determined. The bulge loops were of the group II variety, where the bulged nucleotide is identical to one of its nearest neighbors, leading to ambiguity as to the exact position of the bulge. The data were used to develop a model to predict the free energy of an RNA duplex containing a single-nucleotide bulge. The destabilization of the duplex by the bulge was primarily related to the stability of the stems adjacent to the bulge. Specifically, there was a direct correlation between the destabilization of the duplex and the stability of the less stable duplex stem. Since there is an ambiguity of the bulge position for group II bulges, several different stem combinations are possible. The destabilization of group II bulge loops is similar to the destabilization of group I bulge loops, if the second least stable stem is used to predict the influence of the group II bulge. In-line structure probing of the group II bulge loop embedded in a hairpin indicates that the bulged nucleotide is the one positioned farther from the hairpin loop.     

Molecular design, chemical synthesis, and evaluation of cytosine-carbohydrate hybrids for selective recognition of a single guanine bulged duplex DNA

The designed cytosine-carbohydrate hybrid molecule selectively recognized and stabilized the bulged duplex DNA possessing the complementary bulged DNA base, guanine, while the nucleotide base itself did not exhibit any such ability. It was also found that the assistance of the carbohydrate to stabilize the interaction between the nucleotide base and the complementally bulge DNA base is very helpful for the selective recognition and stabilization of the single-bulged duplex DNA.     

Comparative NMR study of A(n)-bulge loops in DNA duplexes: intrahelical stacking of A, A-A, and A-A-A bulge loops.

We have prepared a series of deoxyoligonucleotide duplexes of the sequence d(G-C-A-T-C-G-X-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-G-C), in which X represents either one (A), two (A-A), or three (A-A-A) unpaired adenine basis. Using two-dimensional proton and phosphorus NMR spectroscopy, we have characterized conformational features of these bulge-loop duplexes in solution. We find that Watson-Crick hydrogen bonding is intact for all 12 base pairs, including the GC bases that flank the bulge loop. Observation of NOE connectivities in both H2O and D2O allows us to unambiguously localize all of the bulged adenine residues to intrahelical positions within the duplex. This is in contrast to an earlier model for multiple-base bulge loops in DNA [Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840], in which all but the most 5' bulged base are looped out into solution. We find that insertion of two or three bases into the duplex results in the disruption of specific sequential NOEs for the base step across from the bulge loop site on the opposite strand. This disruption is characterized by a partial shearing apart of these bases, such that certain sequential NOEs for this base step are preserved. We observe a downfield-shifted phosphorus resonance, which we assign in the A-A-A bulge duplex to the 3' side of the last bulged adenine residue. Proton and phosphorus chemical shift trends within the An-bulge duplex series indicate that there is an additive effect on the structural perturbations caused by additional unpaired bases within the bulge loop. This finding parallels previous observations [Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840; Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837] on the magnitude of the induced bending of DNA duplexes by multiple-base bulge loops.     

Solution structure of a wedge-shaped synthetic molecule at a two-base bulge site in DNA

The solution structure of the complex formed between an oligonucleotide containing a two-base bulge (5'-CACGCAGTTCGGAC.5'-GTCCGATGCGTG) and DDI, a designed synthetic agent, has been elucidated using high-resolution NMR spectroscopy and restrained molecular dynamic simulation. DDI, which has been found to modulate DNA strand slippage synthesis by DNA polymerase I [Kappen, L. S., Xi, Z., Jones, G. B., and Goldberg, I. H. (2003) Biochemistry 42, 2166-2173], is a wedge-shaped spirocyclic molecule whose aglycone structure closely resembles that of the natural product, NCSi-gb, which strongly binds to an oligonucleotide containing a two-base bulge. Changes in chemical shifts of the DNA upon complex formation and intermolecular NOEs between DDI and the bulged DNA duplex indicate that agent specifically binds to the bulge site of DNA. The benzindanone moiety of DDI intercalates via the minor groove into the G7-T8-T9.A20 pocket, which consists of a helical base pair and two unpaired bulge bases, stacking with the G7 and A20 bases. On the other hand, the dihydronaphthalenone and aminoglycoside moieties are positioned in the minor groove. The aminoglycoside, which is attached to spirocyclic ring, aligns along the A20T21G22 sequence of the nonbulged strand, while the dihydronaphthalenone, which is restrained by the spirocyclic structure, is positioned near the G7-T8-T9 bulge site. The aminoglycoside is closely aligned with the dihydronaphthalenone, preventing its intercalation into the bulge site. In the complex, the unpaired purine (G7) is intrahelical and stacks with the intercalating moiety of DDI, whereas the unpaired pyrimidine (T8) is extrahelical. The structure of the complex formed by binding of the synthetic agent to the two-base bulged DNA reveals a binding mode that differs in important details from that of the natural product, explaining the different binding specificity for the bulge sites of DNA. The structure of the DDI-bulged DNA complex provides insight into the structure-binding affinity relationship, providing a rational basis for the design of specific, high-affinity probes of the role of bulged nucleic acid structures in various biological processes.     

Thermodynamic characterization of deoxyribooligonucleotide duplexes containing bulges

Ultraviolet absorption techniques were used to study the thermodynamics of duplex formation for a DNA decamer, d(GCGAAAAGCG).d(CGCTTTTCGC), and a series of related duplexes, each of which contains a bulged base centered in the A.T tract. Thermodynamic parameters were obtained from nonlinear least-squares fits of the melting curves and the concentration dependences of the melting temperatures. Duplexes containing a localized single-base bulge were found to be 3.5-4.6 kcal/mol less stable than the decamer at 37 degrees C. These results indicate that both the identity of the bulged base and the strand in which it is located may influence the amount by which the duplex is destabilized. Bulged bases located in the T-strand, d(CGCTTYTTCGC), in position Y, were observed to be slightly more destabilizing than those located in the A-strand, d(GCGAAXAAGCG), in position X. Bulged purines may be more destabilizing than bulged pyrimidines.     

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.