Probing the DNA kink structure induced by the hyperthermophilic chromosomal protein Sac7d

Sac7d, a small, abundant, sequence-general DNA-binding protein from the hyperthermophilic archaeon Sulfolobus acidocaldarius, causes a single-step sharp kink in DNA (~60°) via the intercalation of both Val26 and Met29. These two amino acids were systematically changed in size to probe their effects on DNA kinking. Eight crystal structures of five Sac7d mutant–DNA complexes have been analyzed. The DNA-binding pattern of the V26A and M29A single mutants is similar to that of the wild-type, whereas the V26A/M29A protein binds DNA without side chain intercalation, resulting in a smaller overall bending (~50°). The M29F mutant inserts the Phe29 side chain orthogonally to the C2pG3 step without stacking with base pairs, inducing a sharp kink (~80°). In the V26F/M29F-GCGATCGC complex, Phe26 intercalates deeply into DNA bases by stacking with the G3 base, whereas Phe29 is stacked on the G15 deoxyribose, in a way similar to those used by the TATA box-binding proteins. All mutants have reduced DNA-stabilizing ability, as indicated by their lower T_m values. The DNA kink patterns caused by different combinations of hydrophobic side chains may be relevant in understanding the manner by which other minor groove-binding proteins interact with DNA.     

Dynamic Motions of the HIV-1 Frameshift Site RNA

The HIV-1 frameshift site (FS) plays a critical role in viral replication. During translation, the HIV-1 FS transitions from a 3-helix to a 2-helix junction RNA secondary structure. The 2-helix junction structure contains a GGA bulge, and purine-rich bulges are common motifs in RNA secondary structure. Here, we investigate the dynamics of the HIV-1 FS 2-helix junction RNA. Interhelical motions were studied under different ionic conditions using NMR order tensor analysis of residual dipolar couplings. In 150 mM potassium, the RNA adopts a 43°(±4°) interhelical bend angle (β) and displays large amplitude, anisotropic interhelical motions characterized by a 0.52(±0.04) internal generalized degree of order (GDO_int) and distinct order tensor asymmetries for its two helices (η = 0.26(±0.04) and 0.5(±0.1)). These motions are effectively quenched by addition of 2 mM magnesium (GDO_int = 0.87(±0.06)), which promotes a near-coaxial conformation (β = 15°(±6°)) of the two helices. Base stacking in the bulge was investigated using the fluorescent purine analog 2-aminopurine. These results indicate that magnesium stabilizes extrahelical conformations of the bulge nucleotides, thereby promoting coaxial stacking of helices. These results are highly similar to previous studies of the HIV transactivation response RNA, despite a complete lack of sequence similarity between the two RNAs. Thus, the conformational space of these RNAs is largely determined by the topology of their interhelical junctions.     

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.     

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.     

Visualization of diagnostic heteroduplex DNAs from cystic fibrosis deletion heterozygotes provides an estimate of the kinking of DNA by bulged bases.

Previous studies (Hsieh, C.-H., and Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837) of DNAs containing extra or bulged bases on one of the two strands of a duplex showed that they exhibit slower electrophoretic mobility than non-bulged DNAs, indicating that bulges create stiff kinks in the DNA. Here we paired a 97-base single-stranded DNA from the intact cystic fibrosis (CF) gene with a complementary 94-base strand containing a central 3-base deletion (delta F508), common to many CF patients. This produced a 94-base pair DNA with a central 3-base bulge. Visualization of these DNAs by electron microscopy showed that twice as many bulge-containing DNAs had a central kink as compared with the non-bulged controls. Examination of the distribution of kinking angles showed that the bulged population contained 5-7-fold more molecules with a central kink of 80 +/- 10 degrees than did the control molecules. When the 3-base bulge was replaced by a 3-base gap, the resulting duplex DNA showed central kinks with a somewhat lower frequency but greater range of kinking angles.     

Structure of the RNA claw of the DNA packaging motor of bacteriophage ?29

Bacteriophage DNA packaging motors translocate their genomic DNA into viral heads, compacting it to near-crystalline density. The Bacillus subtilis phage ϕ29 has a unique ring of RNA (pRNA) that is an essential component of its motor, serving as a scaffold for the packaging ATPase. Previously, deletion of a three-base bulge (18-CCA-20) in the pRNA A-helix was shown to abolish packaging activity. Here, we solved the structure of this crucial bulge by nuclear magnetic resonance (NMR) using a 27mer RNA fragment containing the bulge (27b). The bulge actually involves five nucleotides (17-UCCA-20 and A100), as U17 and A100 are not base paired as predicted. Mutational analysis showed these newly identified bulge residues are important for DNA packaging. The bulge introduces a 33–35° bend in the helical axis, and inter-helical motion around this bend appears to be restricted. A model of the functional 120b pRNA was generated using a 27b NMR structure and the crystal structure of the 66b prohead-binding domain. Fitting this model into a cryo-EM map generated a pentameric pRNA structure; five helices projecting from the pRNA ring resemble an RNA claw. Biochemical analysis suggested that this shape is important for coordinated motor action required for DNA translocation.     

Thermodynamic parameters for an expanded nearest-neighbor model for the formation of RNA duplexes with single nucleotide bulges

Thirty-four RNA duplexes containing single nucleotide bulges were optically melted, and the thermodynamic parameters deltaH degrees, deltaS degrees, deltaG degrees (37), and T(M) for each sequence were determined. Data from this study were combined with data from previous thermodynamic data [Longfellow, C. E., Kierzek, R., and Turner, D. H. (1990) Biochemistry 29, 278-85] to develop a model that will more accurately predict the free energy of an RNA duplex containing a single nucleotide bulge. Differences between purine and pyrimidine bulges as well as differences between Group I duplexes, those in which the bulge is not identical to either neighboring nucleotide, and Group II duplexes, those in which the bulge is identical to at least one neighboring nucleotide, were considered. The length of the duplex, non-nearest-neighbor effects, and bulge location were also examined. A model was developed which divides sequences into two groups: those with pyrimidine bulges and those with purine bulges. The proposed model for pyrimidine bulges predicts deltaG degrees (37,bulge) = 3.9 kcal/mol + 0.10deltaG degrees (37,nn) + beta, while the model for purine bulges predicts deltaG degrees (37,bulge) = 3.3 kcal/mol - 0.30deltaG degrees (37,nn) + beta, where beta has a value of 0.0 and -0.8 kcal/mol for Group I and Group II sequences, respectively, and deltaG degrees (37,nn) is the nearest-neighbor free energy of the base pairs surrounding the bulge. The conformation of bulge loops present in rRNA was examined. Three distinct families of structures were identified. The bulge loop was either extrahelical, intercalated, or in a "side-step" conformation.     

Fluorescence energy transfer analysis of DNA structures containing several bulges and their interaction with CAP

DNA molecules with three bulges separated by double-stranded helical sections of B-DNA were constructed to be used as substrates for DNA-protein binding assays. Fluorescence resonance energy transfer (FRET) between dye molecules attached to the 5'-ends of the DNA molecules is used to monitor the protein binding. The A5 bulge, which consists of five unpaired adenine nucleotides, alters the direction of the helical axis by approximately 80 to 90 at every bulge site. Computer molecular modeling facilitated a pre-selection of suitable helix lengths that bring the labeled ends of the three-bulge DNA molecules (60 to 70 base-pairs long) into close proximity. The FRET experiments verified that the labeled ends of the helices of these long molecules were indeed close. A series of FRET experiments was carried out with two A5 and two A7 bulge molecules. The relative positions of the bulges were varied along the central helical DNA sequence (between the bulges) in order to determine the relative angular juxtapositions of the outlying helical arms flanking the central helical region. The global structural features of the DNA molecules are manifested in the FRET data. The FRET experiments, especially those of the two-bulge series, could be interpreted remarkably well with molecular models based on the NMR structure of the A5 bulge. These models assume that the DNA molecules do not undergo large torsional conformational fluctuations at the bulge sites. The magnitude of the FRET efficiency attests to a relatively rigid structure for many of the long 5'-end-labeled molecules. The changes in the FRET efficiency of three-bulge structures containing the specific binding sequence of the catabolite activator protein (CAP) demonstrated significant deformation of the DNA upon binding of CAP. No direct interaction of CAP with the dyes was observed.     

Characterization of an RNA bulge structure by Fourier transform infrared spectroscopy

There may be several advantages associated with an antisense oligonucleotide that induces a bulged structure into its RNA target molecule. Many structures of RNA bulges are elucidated from single-stranded RNA models. However, a two-component system is the minimum requirement for a realistic antisense model. We have used Fourier transform infrared spectroscopy to investigate a single-stranded RNA oligonucleotide with known NMR solution structure, constructed to model a five nucleotide bulge, and its two-component oligonucleotide counterpart. The infrared spectra show A-helical base-paired stems and non-base-paired loops in both systems. The nucleosides are mainly in an anti-conformation. Both N-type and S-type of sugar puckers can be inferred from the infrared region sensitive to sugar conformations. The S-type of sugar pucker is likely to be associated with the nucleotides in the bulge. The FTIR results display an overall structural similarity between the two model systems.     

Crystal structure of an RNA duplex r(gugucgcac)(2) with uridine bulges.

The crystal structure of a nonamer RNA duplex with a uridine bulge in each strand, r(gugucgcac)(2), was determined at 1.4 A resolution. The structure was solved by multiple anomalous diffraction phasing method using a three-wavelength data set collected at the Advanced Protein Source and refined to a final R(work)/R(free) of 21.2 %/23.4 % with 33,271 independent reflections (Friedel pairs unmerged). The RNA duplex crystallized in the tetragonal space group P4(1)22 with two independent molecules in the asymmetric unit. The unit cell dimensions are a=b=47.18 A and c=80.04 A. The helical region of the nonamer adopts the A-form conformation. The uridine bulges assume similar conformations, with uracils flipping out and protruding into the minor groove. The presence of the bulge induces very large twist angles (approximately +50 degrees) between the base-pairs flanking the bulges while causing profound kinks in the helix axis at the bulges. This severe twist and the large kink in turn produces a very narrow major groove at the middle of the molecule. The ribose sugars of the guanosines before the bulges adopt the C2'-endo conformation while the rest, including the bulges, are in the C3'-endo conformation. The intrastrand phosphate-phosphate (P-P) distance of the phosphate groups flanking the bulges (approximately 4.4 A) are significantly shorter than the average P-P distance in the duplex (6.0 A). This short distance between the two phosphate groups brings the non-bridging oxygen atoms close to each other where a calcium ion is bound to each strand. The calcium ions in molecule 1 are well defined while the calcium ions in molecule 2 are disordered.     

Human Base Excision Repair Creates a Bias Toward ?1 Frameshift Mutations

Frameshift mutations are particularly deleterious to protein function and play a prominent role in carcinogenesis. Most commonly these mutations involve the insertion or omission of a single nucleotide by a DNA polymerase that slips on a damaged or undamaged template. The mismatch DNA repair pathway can repair these nascent polymerase errors. However, overexpression of enzymes of the base excision repair (BER) pathway is known to increase the frequency of frameshift mutations suggesting competition between these pathways. We have examined the fate of DNA containing single nucleotide bulges in human cell extracts and discovered that several deaminated or alkylated nucleotides are efficiently removed by BER. Because single nucleotide bulges are more highly exposed we anticipate that they would be highly susceptible to spontaneous DNA damage. As a model for this, we have shown that chloroacetaldehyde reacts more than 18-fold faster with an A-bulge than with a stable A·T base pair to create alkylated DNA adducts that can be removed by alkyladenine DNA glycosylase. Reconstitution of the BER pathway using purified components establishes that bulged DNA is efficiently processed. Single nucleotide deletion is predicted to repair +1 frameshift events, but to make −1 frameshift events permanent. Therefore, these findings suggest an additional factor contributing to the bias toward deletion mutations.     

Mechanism of DNA flexibility enhancement by HMGB proteins

The mechanism by which sequence non-specific DNA-binding proteins enhance DNA flexibility is studied by examining complexes of double-stranded DNA with the high mobility group type B proteins HMGB2 (Box A) and HMGB1 (Box A+B) using atomic force microscopy. DNA end-to-end distances and local DNA bend angle distributions are analyzed for protein complexes deposited on a mica surface. For HMGB2 (Box A) binding we find a mean induced DNA bend angle of 78°, with a standard error of 1.3° and a SD of 23°, while HMGB1 (Box A+B) binding gives a mean bend angle of 67°, with a standard error of 1.3° and a SD of 21°. These results are consistent with analysis of the observed global persistence length changes derived from end-to-end distance measurements, and with results of DNA-stretching experiments. The moderately broad distributions of bend angles induced by both proteins are inconsistent with either a static kink model, or a purely flexible hinge model for DNA distortion by protein binding. Therefore, the mechanism by which HMGB proteins enhance the flexibility of DNA must differ from that of the Escherichia coli HU protein, which in previous studies showed a flat angle distribution consistent with a flexible hinge model.     

Shallow Boomerang-shaped Influenza Hemagglutinin G13A Mutant Structure Promotes Leaky Membrane Fusion

Our previous studies showed that an angled boomerang-shaped structure of the influenza hemagglutinin (HA) fusion domain is critical for virus entry into host cells by membrane fusion. Because the acute angle of ∼105° of the wild-type fusion domain promotes efficient non-leaky membrane fusion, we asked whether different angles would still support fusion and thus facilitate virus entry. Here, we show that the G13A fusion domain mutant produces a new leaky fusion phenotype. The mutant fusion domain structure was solved by NMR spectroscopy in a lipid environment at fusion pH. The mutant adopted a boomerang structure similar to that of wild type but with a shallower kink angle of ∼150°. G13A perturbed the structure of model membranes to a lesser degree than wild type but to a greater degree than non-fusogenic fusion domain mutants. The strength of G13A binding to lipid bilayers was also intermediate between that of wild type and non-fusogenic mutants. These membrane interactions provide a clear link between structure and function of influenza fusion domains: an acute angle is required to promote clean non-leaky fusion suitable for virus entry presumably by interaction of the fusion domain with the transmembrane domain deep in the lipid bilayer. A shallower angle perturbs the bilayer of the target membrane so that it becomes leaky and unable to form a clean fusion pore. Mutants with no fixed boomerang angle interacted with bilayers weakly and did not promote any fusion or membrane perturbation.     

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.     

Predicting stability of DNA bulge at mononucleotide microsatellite

Mononucleotide microsatellites are clinically and forensically crucial DNA sequences due to their high mutability and abundance in the human genome. As a mutagenic intermediate of an indel in a microsatellite and a consequence of probe hybridization after such mutagenesis, a bulge with structural degeneracy sliding within a microsatellite is formed. Stability of such dynamic bulges, however, is still poorly understood despite their critical role in cancer genomics and neurological disease studies. In this paper, we have built a model that predicts the thermodynamics of a sliding bulge at a microsatellite. We first identified 40 common bulge states that can be assembled into any sliding bulges, and then characterized them with toehold exchange energy measurement and the partition function. Our model, which is the first to predict the free energy of sliding bulges with more than three repeats, can infer the stability penalty of a sliding bulge of any sequence and length with a median prediction error of 0.22 kcal/mol. Patterns from the prediction clearly explain landscapes of microsatellites observed in the literature, such as higher mutation rates of longer microsatellites and C/G microsatellites.     

Identification of DNA--cisplatin adducts in a blind trial of in situ scanning tunneling microscopy.

Scanning tunneling microscopy (STM) reveals nanometer scale details of hydrated DNA but the interpretation of the images is controversial because of substrate artifacts and the lack of a theory for image contrast. We demonstrate that we have overcome these problems by identifying five DNA samples by their STM images alone in a blinded trial. The samples were single-stranded and double-stranded DNA with and without covalent modification by the anti-tumor drug cisplatin. The cisplatin adducts were distinguished by substantial kinking at the drug binding site. The oligomers were 20 bases in length, which was too short to permit the kinking angle to be determined with precision. However, models with a 45 degree kink gave a better fit to the images of the duplex adducts than models with a 90 degrees kink. A variety of structures was observed for the single-stranded adducts.     

The Role of Mg(II) in DNA Cleavage Site Recognition in Group II Intron Ribozymes: SOLUTION STRUCTURE AND METAL ION BINDING SITES OF THE RNA·DNA COMPLEX*

Group II intron ribozymes catalyze the cleavage of (and their reinsertion into) DNA and RNA targets using a Mg²⁺-dependent reaction. The target is cleaved 3′ to the last nucleotide of intron binding site 1 (IBS1), one of three regions that form base pairs with the intron''s exon binding sites (EBS1 to -3). We solved the NMR solution structure of the d3′ hairpin of the Sc.ai5γ intron containing EBS1 in its 11-nucleotide loop in complex with the dIBS1 DNA 7-mer and compare it with the analogous RNA·RNA contact. The EBS1·dIBS1 helix is slightly flexible and non-symmetric. NMR data reveal two major groove binding sites for divalent metal ions at the EBS1·dIBS1 helix, and surface plasmon resonance experiments show that low concentrations of Mg²⁺ considerably enhance the affinity of dIBS1 for EBS1. Our results indicate that identification of both RNA and DNA IBS1 targets, presentation of the scissile bond, and stabilization of the structure by metal ions are governed by the overall structure of EBS1·dIBS1 and the surrounding loop nucleotides but are irrespective of different EBS1·(d)IBS1 geometries and interstrand affinities.     

Effects of single-base bulges on intercalator binding to small RNA and DNA hairpins and a ribosomal RNA fragment

The way in which a single-base bulge might affect the structure of an RNA helix has been examined by preparing a series of six RNA hairpins, all with seven base pairs and a four-nucleotide loop. Five of the hairpins have single-base bulges at different positions. The intercalating cleavage reagent (methidiumpropyl)-EDTA-Fe(II) [MPE-Fe(II)] binds preferentially at a CpG sequence in the helix lacking a bulge and in four of the five hairpins with bulges. Hairpins with a bulge one or two bases to the 3' side of the CpG sequence bind ethidium 4-5-fold more strongly than the others. V1 RNase, which is sensitive to RNA backbone conformation in helices, detects a conformational change in all of the helices when ethidium binds; the most dramatic changes, involving the entire hairpin stem, are in one of the two hairpins with enhanced ethidium affinity. Only a slight conformational change is detected in the hairpin lacking a bulge. A bulge adjacent to a CpG sequence in a 100-nucleotide ribosomal RNA fragment enhances MPE-Fe(II) binding by an order of magnitude. These results extend our previous observations of bulges at a single position in an RNA hairpin [White, S. A., & Draper, D.E. (1987) Nucleic Acids Res. 15, 4049] and show that (1) a structural change in an RNA helix may be propagated for several base pairs, (2) bulges tend to increase the number of conformations available to a helix, and (3) the effects observed in small RNA hairpins are relevant to larger RNAs with more extensive structure. A bulge in a DNA hairpin identical in sequence with the RNA hairpins does not enhance MPE-Fe(II) binding affinity, relative to a control DNA hairpin. The effects of bulges on ethidium intercalation are evidently modulated by helix structure.     

Recognition and incision of site-specifically modified C8 guanine adducts formed by 2-aminofluorene, N-acetyl-2-aminofluorene and 1-nitropyrene by UvrABC nuclease

Nucleotide excision repair plays a crucial role in removing many types of DNA adducts formed by UV light and chemical carcinogens. We have examined the interactions of Escherichia coli UvrABC nuclease proteins with three site-specific C8 guanine adducts formed by the carcinogens 2-aminofluorene (AF), N-acetyl-2-acetylaminofluorene (AAF) and 1-nitropyrene (1-NP) in a 50mer oligonucleotide. Similar to the AF and AAF adducts, the 1-NP-induced DNA adduct contains an aminopyrene (AP) moiety covalently linked to the C8 position of guanine. The dissociation constants for UvrA binding to AF–, AAF– and AP–DNA adducts, determined by gel mobility shift assay, are 33 ± 9, 8 ± 2 and 23 ± 9 nM, respectively, indicating that the AAF adduct is recognized much more efficiently than the other two. Incision by UvrABC nuclease showed that AAF–DNA was cleaved ~2-fold more efficiently than AF– or AP–DNA (AAF > AF ≈ AP), even though AP has the largest molecular size in this group. However, an opened DNA structure of six bases around the adduct increased the incision efficiency for AF–DNA (but not for AP–DNA), making it equivalent to that for AAF–DNA. These results are consistent with a model in which DNA damage recognition by the E.coli nucleotide excision repair system consists of two sequential steps. It includes recognition of helical distortion in duplex DNA followed by recognition of the type of nucleotide chemical modification in a single-stranded region. The difference in incision efficiency between AF– and AAF–DNA adducts in normal DNA sequence, therefore, is a consequence of their difference in inducing structural distortions in DNA. The results of this study are discussed in the light of NMR solution structures of these DNA adducts.