Solution structure of [d(ATGAGCGAATA)]2. Adjacent G:A mismatches stabilized by cross-strand base-stacking and BII phosphate groups.

The solution structure of a rather unusual B-form duplex [d(ATGAGCGAATA)]2 has been determined using two-dimensional nuclear magnetic resonance (2D-NMR) and distance geometry methods. This sequence forms a stable ten base-pair B-form duplex with 3' overhangs and two pairs of adjacent G:A mismatches paired via a sheared hydrogen-bonding scheme. All non-exchangeable protons, including the stereo-specific H-5'S/H-5'R of the 3G and 7G residues, were assigned by 2D-NMR. The phosphorus spectrum was assigned using heteronuclear correlation with H-3' and H-4' reasonances. The complete assignments reveal several unusual nuclear Overhauser enhancements (NOEs) and unusual chemical shifts for the neighboring G:A mismatch pairs and their adjacent nucleotides. Inter-proton distances were derived from time-dependent NOEs and used to generate initial structures, which were further refined by iterative back-calculation of the two-dimensional nuclear Overhauser enhancement spectra; 22 final structures were calculated from the refined distance bounds. All these final structures exhibit fully wound helical structures with small penalty values against the refined distance bounds and small pair-wise root-mean-square deviation values (typically 0.5 A to 0.9 A). The two helical strands exchange base stacking at both of the two G:A mismatch sites, resulting in base stacking down each side rather than down each strand of the twisted duplex. Very large twist angles (77 degrees) were found at the G:A mismatch steps. All the final structures were found to have BII phosphate conformations at the adjacent G:A mismatch sites, consistent with observed downfield 31P chemical shifts and Monte-Carlo conformational search results. Our results support the hypothesis that 31P chemical shifts are related to backbone torsion angles. These BII phosphate conformations in the adjacent G:A mismatch step suggest that hydrogen bonding of the G:A pair G-NH2 to a nearby phosphate oxygen atom is unlikely. The unusual structure of the duplex may be stabilized by strong interstrand base stacking as well as intrastrand stacking, as indicated by excellent base overlap within the mismatch stacks.     

Base pairing geometry in GA mismatches depends entirely on the neighboring sequence.

We have synthesized nine self-complementary DNA oligomers containing different flanking sequences adjacent to a pair of contiguous GA mismatches, and have used high resolution nuclear magnetic resonance (n.m.r.) to investigate the GpA phosphodiester backbone conformation and mismatch pairing schemes in these duplexes. We found dramatic effects of the flanking base pair on the hydrogen bonding and backbone conformation, which appear to be coupled. Thus the Ganti-Aanti base pairing scheme in a NAGATN sequence switches to a more stable sheared GA base pairing scheme in a NCGAGN or NTGAAN context, while no duplex is formed (or only GA bulges occur) when NAGATN is changed to NGGACN. Furthermore, the more stable sheared GA pairing in NPyGAPuN sequences is associated with a BII rather than BI backbone conformation for the phosphodiester between the adjacent mismatched GA pairs. The overall stability of these adjacent GA mismatches as measured by imino proton n.m.r. studies is Py-GA-Pu > A-GA-T > G-GA-C.     

Very stable mismatch duplexes: structural and thermodynamic studies on tandem G.A mismatches in DNA.

We have used ultraviolet melting techniques to compare the stability of several DNA duplexes containing tandem G.A mismatches to similar duplexes containing tandem A.G, I.A, and T.A base pairs. We have found that tandem G.A mismatches in 5'-Y-G-A-R-3' duplexes are more stable than their I.A counterparts and that they are sometimes more stable than tandem 5'-Y-T-A-R-3' sequences. This is not the case for tandem G.A mismatches in other base stacking environments, and it suggests that tandem G.A mismatches in 5'-Y-G-A-R-3' sequences have a unique configuration. In contrast to tandem 5'-G-A-3' mismatches, tandem 5'-A-G-3' mismatches were found to be unstable in all cases examined.     

Thermodynamics of RNA duplexes with tandem mismatches containing a uracil-uracil pair flanked by C.G/G.C or G.C/A.U closing base pairs

The thermodynamics governing the denaturation of RNA duplexes containing 8 bp and a central tandem mismatch or 10 bp were evaluated using UV absorbance melting curves. Each of the eight tandem mismatches that were examined had one U-U pair adjacent to another noncanonical base pair. They were examined in two different RNA duplex environments, one with the tandem mismatch closed by G.C base pairs and the other with G.C and A.U closing base pairs. The free energy increments (Delta Gdegrees(loop)) of the 2 x 2 loops were positive, and showed relatively small differences between the two closing base pair environments. Assuming temperature-independent enthalpy changes for the transitions, (Delta Gdegrees(loop)) for the 2 x 2 loops varied from 0.9 to 1.9 kcal/mol in 1 M Na(+) at 37 degrees C. Most values were within 0.8 kcal/mol of previously estimated values; however, a few sequences differed by 1.2-2.0 kcal/mol. Single strands employed to form the RNA duplexes exhibited small noncooperative absorbance increases with temperature or transitions indicative of partial self-complementary duplexes. One strand formed a partial self-complementary duplex that was more stable than the tandem mismatch duplexes it formed. Transitions of the RNA duplexes were analyzed using equations that included the coupled equilibrium of self-complementary duplex and non-self-complementary duplex denaturation. The average heat capacity change (DeltaC(p)) associated with the transitions of two RNA duplexes was estimated by plotting DeltaH degrees and DeltaS degrees evaluated at different strand concentrations as a function of T(m) and ln T(m), respectively. The average DeltaC(p) was 70 +/- 5 cal K(-)(1) (mol of base pairs)(-)(1). Consideration of this heat capacity change reduced the free energy of formation at 37 degrees C of the 10 bp control RNA duplexes by 0.3-0.6 kcal/mol, which may increase Delta Gdegrees(loop) values by similar amounts.     

DNA multiplex hybridization on microarrays and thermodynamic stability in solution: a direct comparison

Hybridization intensities of 30 distinct short duplex DNAs measured on spotted microarrays, were directly compared with thermodynamic stabilities measured in solution. DNA sequences were designed to promote formation of perfect match, or hybrid duplexes containing tandem mismatches. Thermodynamic parameters ΔH°, ΔS° and ΔG° of melting transitions in solution were evaluated directly using differential scanning calorimetry. Quantitative comparison with results from 63 multiplex microarray hybridization experiments provided a linear relationship for perfect match and most mismatch duplexes. Examination of outliers suggests that both duplex length and relative position of tandem mismatches could be important factors contributing to observed deviations from linearity. A detailed comparison of measured thermodynamic parameters with those calculated using the nearest-neighbor model was performed. Analysis revealed the nearest-neighbor model generally predicts mismatch duplexes to be less stable than experimentally observed. Results also show the relative stability of a tandem mismatch is highly dependent on the identity of the flanking Watson–Crick (w/c) base pairs. Thus, specifying the stability contribution of a tandem mismatch requires consideration of the sequence identity of at least four base pair units (tandem mismatch and flanking w/c base pairs). These observations underscore the need for rigorous evaluation of thermodynamic parameters describing tandem mismatch stability.     

Thermodynamic characterization of single mismatches found in naturally occurring RNA

Many naturally occurring RNA structures contain single mismatches. However, the algorithms currently used to predict RNA structure from sequence rely on a minimal set of data for single mismatches, most of which occur rather infrequently in nature. As a result, several approximations and assumptions are used to predict the stability of RNA duplexes containing the most common single mismatches. Therefore, the relative frequency of single mismatches was determined by compiling and searching a database of 955 RNA secondary structures. Thermodynamic parameters for duplex formation, derived from optical melting experiments, are reported for 28 oligoribonucleotides containing frequently occurring single mismatches. These data were then combined with previous data to construct a dataset of 64 single mismatches, including the 30 most common in the database. Because of this increase in experimental thermodynamic parameters for single mismatches that occur frequently in nature, more accurate free energy calculations have resulted. To improve the prediction of the thermodynamic parameters for duplexes containing single mismatches that have not been experimentally measured, single mismatch-specific nearest neighbor parameters were derived. The free energy of an RNA duplex containing a single mismatch that has not been thermodynamically characterized can be calculated by: DeltaG degrees 37,single mismatch = DeltaG degrees 37,mismatch nt + DeltaG degrees 37,mismatch-NN interaction + DeltaG degrees 37,AU/GU. Here, DeltaG degrees 37,mismatch is -0.4, -2.1, and -0.3 kcal/mol for A.G, G.G, and U.U mismatches, respectively; DeltaG degrees 37,mismatch-NN interaction is 0.7, -0.5, 0.4, -0.4, and -1.0 kcal/mol for 5'YRR3'/3'RRY5', 5'RYY3'/3'YYR5', 5'YYR3'/3'RYY5', 5'YRY3'/3'RYR5', and 5'RRY3'/3'YYR5' mismatch-nearest neighbor combinations, respectively, when A and G are categorized as purines (R) and C and U are categorized as pyrimidines (Y); and DeltaG degrees 37,AU/GU is a penalty of 1.2 kcal/mol for replacing a G-C base pair with either an A-U or G-U base pair. Similar predictive models were also derived for DeltaH degrees single mismatch and DeltaS degrees single mismatch. These new predictive models, in conjunction with the reported thermodynamics for frequently occurring single mismatches, should allow for more accurate calculations of the free energy of RNA duplexes containing single mismatches and, furthermore, allow for improved prediction of secondary structure from sequence.     

Synthesis of 2'-O-methyl-RNAs incorporating a 3-deazaguanine, and UV melting and computational studies on its hybridization properties

2'-O-methyl-RNAs incorporating 3-deazaguanine (c3G) were synthesized by use of N,N-diphenylcarbamoyl and N,N-dimethylaminomethylene as its base protecting groups to suppress sheared-type 5'-GA-3'/5'-GA-3' tandem mismatched base pairing which requires the N3 atom. These modified RNAs hybridized more weakly with the complementary and single mismatch-containing RNAs than the unmodified RNAs. The T(m) experiments were performed to clarify the effects of replacement of the fifth G with c(3)G on stabilization of 2'-O-methyl-(5'-CGGCGAGGAG-3')/5'-CUCCGAGCCG-3' and 2'-O-methyl-(5'-CGGGGACGAG-3')/5'-CUCGGACCCG-3'duplexes, which form sheared-type and face-to-face type 5'-GA-3'/5'-GA-3' tandem mismatched base pairs, respectively. Consequently, this replacement led to more pronounced destabilization of the former duplex that needs the N3 atom for the sheared-type base pair than the latter that does not need it for the face-to-face type base pair. A similar tendency was observed for 2'-O-methyl-RNA/DNA duplexes. These results suggest that the N3 atom of G plays an important role in stabilization of the canonical G/C base pair as well as the base discrimination and its loss suppressed formation of the undesired sheared-type mismatched base pair. Computational studies based on ab initio calculations suggest that the weaker hydrogen bonding ability and larger dipole moment of c3G can be the origin of the lower T(m).     

Influence of pH on the conformation and stability of mismatch base-pairs in DNA

A series of self-complementary dodecanucleotide duplexes containing two symmetrically disposed mismatches have been studied by pH-dependent, ultraviolet light melting techniques. The results indicate that A.C, and C.C mismatches are strongly stabilized by protonation and that the degree of stabilization of the A.C mismatch depends greatly on the flanking bases. In one case, a duplex containing two A.C mismatches is more stable than the native sequence below pH 5.5. The G.A mismatch displays conformational flexibility, with a protonated G(syn).A(anti) base-pair occurring in certain base stacking environments but not in others. The A.A and T.C mismatches are not stabilized at low pH. These solution studies correlate well with predictions based on X-ray crystallographic data.     

NMR studies of A.C mismatches in DNA dodecanucleotides at acidic pH. Wobble A(anti).C(anti) pair formation

Two-dimensional proton NMR studies were undertaken on the d(C-G-A-G-A-A-T-T-C-C-C-G) duplex (designated A.C 12-mer) where the A at the mismatch site is flanked by G residues and the d(C-G-C-G-A-A-T-T-C-A-C-G) duplex (designated C.A 12-mer) where the A at the mismatch site is flanked by C residues in an attempt to elucidate the role of flanking base pairs on the structure of the A.C mismatch. The exchangeable and nonexchangeable proton spectra of these two dodecanucleotides have been completely characterized by two-dimensional nuclear Overhauser enhancement (NOE) experiments in H2O and D2O solution at acidic pH. The NOE distance connectivities demonstrate that both A and C at the mismatch site are stacked into a right-handed helix between flanking G.C base pairs and exhibit anti-glycosidic torsion angles. The proton chemical shifts and NOE patterns are consistent with Wobble A.C pairing for the A.C 12-mer and C.A 12-mer duplexes in solution and demonstrate that the A.C mismatches introduce local conformational perturbations that do not extend to the central AATT segment. We detect that amino protons of adenosine (approximately 9.2 ppm) but not of cytidine at the A.C mismatch site in both duplexes on lowering the pH below 6.     

Stability and mismatch discrimination of locked nucleic acid-DNA duplexes

Locked nucleic acids (LNA; symbols of bases, +A, +C, +G, and +T) are introduced into chemically synthesized oligonucleotides to increase duplex stability and specificity. To understand these effects, we have determined thermodynamic parameters of consecutive LNA nucleotides. We present guidelines for the design of LNA oligonucleotides and introduce free online software that predicts the stability of any LNA duplex oligomer. Thermodynamic analysis shows that the single strand-duplex transition is characterized by a favorable enthalpic change and by an unfavorable loss of entropy. A single LNA modification confines the local conformation of nucleotides, causing a smaller, less unfavorable entropic loss when the single strand is restricted to the rigid duplex structure. Additional LNAs adjacent to the initial modification appear to enhance stacking and H-bonding interactions because they increase the enthalpic contributions to duplex stabilization. New nearest-neighbor parameters correctly forecast the positive and negative effects of LNAs on mismatch discrimination. Specificity is enhanced in a majority of sequences and is dependent on mismatch type and adjacent base pairs; the largest discriminatory boost occurs for the central +C·C mismatch within the +T+C+C sequence and the +A·G mismatch within the +T+A+G sequence. LNAs do not affect specificity in some sequences and even impair it for many +G·T and +C·A mismatches. The level of mismatch discrimination decreases the most for the central +G·T mismatch within the +G+G+C sequence and the +C·A mismatch within the +G+C+G sequence. We hypothesize that these discrimination changes are not unique features of LNAs but originate from the shift of the duplex conformation from B-form to A-form.     

Thermodynamics-structure relationship of single mismatches in RNA/DNA duplexes

Thermodynamics of 66 RNA/DNA duplexes containing single mismatches were measured by UV melting methods. Stability enhancements for rG. dT mismatches were the largest of all mismatches examined here, while rU.dG mismatches were not as stable. The methyl group on C5 of thymine enhanced the stability by 0.12 approximately 0.53 kcal mol(-)(1) depending on the identity of adjacent Watson-Crick base pairs, whereas the 2'-hydroxyl group in ribouridine stabilized the duplex by approximately 0.6 kcal mol(-)(1) regardless of the adjacent base pairs. Stabilities induced by the methyl group in thymine, the 2'-hydroxyl group of ribouridine, and an nucleotide exchange at rG.dT and rU.dG mismatches were found to be independent of each other. The order for the mismatch stabilities is rG.dT > rU. dG approximately rG.dG > rA.dG approximately rG.dA approximately rA. dC > rA.dA approximately rU.dT approximately rU.dC > rC.dA approximately rC.dT, although the identity of the adjacent base pairs slightly altered the order. The pH dependence stability and structural changes were suggested for the rA.dG but not for rG.dA mismatches. Comparisons of trinucleotide stabilities for G.T and G.U pairs in RNA, DNA, and RNA/DNA duplexes indicate that stable RNA/DNA mismatches exhibit a stability similar to RNA mismatches while unstable RNA/DNA mismatches show a stability similar to that of DNA mismatches. These results would be useful for the design of antisense oligonucleotides.     

Unusual duplex formation in purine rich oligodeoxyribonucleotides

The purine rich oligodeoxyribonucleotides 1C, d(ATGACGGAATA) and 2C, d(ATGAGCGAATA) alone exhibit highly cooperative melting transitions. Analysis of the concentration dependence of melting, and electrophoretic studies indicate that these oligomers can form an unusual purine rich offset double helix. The unusual duplex is predicted to contain four A.T, two G.C, and four G.A mismatch base pairs as well as a single A base stacked on the 3' end of each chain of the helix. Other possible models for the duplex are unlikely because they are predicted to contain many base pairs of low stability. Changing the central sequence to CGG or GGG should destabilize the duplex and this is observed. The unusual duplex of 2C is more stable than the duplex of 1C indicating that the stability of G.A base pairs is quite sensitive to the surrounding sequence. Addition of 1C and 2C to their complementary pyrimidine strands results in normal duplexes of similar stability. We feel that the unusual duplexes are significantly stabilized by the intrinsic stacking tendency of purine bases.     

NMR studies of G:A mismatches in oligodeoxyribonucleotide duplexes modelled after ribozymes.

The structures of two oligodeoxyribonucleotide duplexes, the base sequences of which were modelled after both a hammerhead ribozyme and a small metalloribozyme, were studied by NMR. Both duplexes contain adjacent G:A mismatches; one has a PyGAPu:PyGAPu sequence and the other a PyGAPy:PuGAPu sequence. It is concluded on the basis of many characteristic NOEs that in both duplexes G:A base pairs are formed in the unique 'sheared' form, where an amino proton instead of an imino proton of G is involved in the hydrogen bonding, and G and A bases are arranged 'side by side' instead of 'head to head'. A photo-CIDNP experiment, which gives unique and independent information on the solvent accessibility of nucleotide bases, also supports G:A base pairing rather than a bulged-out structure of G and A residues. This is the first demonstration that not only the PyGAPu:PyGAPu sequence but also the PyGAPy:PuGAPu sequence can form the unique sheared G:A base pairs. Taking the previous studies on G:A mismatches into account, the idea is suggested that a PyGA:GAPu sequence is a minimum and essential element for the formation of the sheared G:A base pairs. The sheared G:A base pairs in the PyGAPu:PyGAPu sequence are suggested to be more stable than those in the PyGAPy:PuGAPu sequence. This is explained rationally by the idea proposed above.     

Raman study of potential "antisense" drugs: nonamer oligonucleotide duplexes with a central mismatch as a model system for the binding selectivity evaluation

A set of four 9-mer oligonucleotide duplexes formed between the 5'-GCATNTCAC-3', N=A,C,T,G, and the 5'-GTGATATGC-3' complement has been proposed as a model system for the investigation of novel oligonucleotide analogues (candidates for antisense use) binding selectivity. Raman measurements were carried out on a set of natural DNA 9-mer in order to verify suitability of the model and to obtain reference spectral data. Difference Raman spectra between the mismatch and match duplexes obtained at 15 degrees C exhibited numerous spectral features sensitively indicating the structural changes. All the three mismatches only very weakly disturb the overall B-form conformation of the duplex. Significant structural changes that occurred at the mismatch site are reflected mainly by the neighboring thymidine Raman bands at 1377, 1650, and 1675 cm(-1). The intensity change of the two latter bands is almost the same for the T:G and the T:T mismatch while in the case of the T:C mismatch it is just opposite, demonstrating a very different arrangement of the mismatched pair.     

Conformational determinants of tandem GU mismatches in RNA: insights from molecular dynamics simulations and quantum mechanical calculations

Structure and energetic properties of base pair mismatches in duplex RNA have been the focus of numerous investigations due to their role in many important biological functions. Such efforts have contributed to the development of models for secondary structure prediction of RNA, including the nearest-neighbor model. In RNA duplexes containing GU mismatches, 5'-GU-3' tandem mismatches have a different thermodynamic stability than 5'-UG-3' mismatches. In addition, 5'-GU-3' mismatches in some sequence contexts do not follow the nearest-neighbor model for stability. To characterize the underlying atomic forces that determine the structural and thermodynamic properties of GU tandem mismatches, molecular dynamics (MD) simulations were performed on a series of 5'-GU-3' and 5'-UG-3' duplexes in different sequence contexts. Overall, the MD-derived structural models agree well with experimental data, including local deviations in base step helicoidal parameters in the region of the GU mismatches and the model where duplex stability is associated with the pattern of GU hydrogen bonding. Further analysis of the simulations, validated by data from quantum mechanical calculations, suggests that the experimentally observed differences in thermodynamic stability are dominated by GG interstrand followed by GU intrastrand base stacking interactions that dictate the one versus two hydrogen bonding scenarios for the GU pairs. In addition, the inability of 5'-GU-3' mismatches in different sequence contexts to all fit into the nearest-neighbor model is indicated to be associated with interactions of the central four base pairs with the surrounding base pairs. The results emphasize the role of GG and GU stacking interactions on the structure and thermodynamics of GU mismatches in RNA.     

Characterization of conformational features of DNA heteroduplexes containing aldehydic abasic sites

The DNA duplexes shown below, with D indicating deoxyribose aldehyde absic sites and numbering from 5' to 3', have been investigated by NMR. The 31P and 31P-1H correlation data indicate [formula: see text] that the backbones of these duplex DNAs are regular. One- and two-dimensional 1H NMR data indicate that the duplexes are right-handed and B-form. Conformational changes due to the presence of the abasic site extend to the two base pairs adjacent to the lesion site with the local conformation of the DNA being dependent on whether the abasic site is in the alpha or beta configuration. The aromatic base of residue A17 in the position opposite the abasic site is predominantly stacked in the helix as is G17 in the analogous sample. Imino lifetimes of the AT base pairs are much longer in samples with an abasic site than in those containing a Watson-Crick base pair. The conformational and dynamical properties of the duplex DNAs containing the naturally occurring aldehyde abasic site are different from those of duplex DNAs containing a variety of analogues of the abasic site.     

Structures of mismatched base pairs in DNA and their recognition by the Escherichia coli mismatch repair system.

The Escherichia coli mismatch repair system does not recognize and/or repair all mismatched base pairs with equal efficiency: whereas transition mismatches (G X T and A X C) are well repaired, the repair of some transversion mismatches (e.g. A X G or C X T) appears to depend on their position in heteroduplex DNA of phage lambda. Undecamers were synthesized and annealed to form heteroduplexes with a single base-pair mismatch in the centre and with the five base pairs flanking each side corresponding to either repaired or unrepaired heteroduplexes of lambda DNA. Nuclear magnetic resonance (n.m.r.) studies show that a G X A mismatch gives rise to an equilibrium between fully helical and a looped-out structure. In the unrepaired G X A mismatch duplex the latter predominates, while the helical structure is predominant in the case of repaired G X A and G X T mismatches. It appears that the E. coli mismatch repair enzymes recognize and repair intrahelical mismatched bases, but not the extrahelical bases in the looped-out structures.     

Effect of the oxidized guanosine lesions spiroiminodihydantoin and guanidinohydantoin on proofreading by Escherichia coli DNA polymerase I (Klenow fragment) in different sequence contexts

Oxidative damage to DNA by endogenous and exogenous reactive oxygen species has been directly linked to cancer, aging, and a variety of neurological disorders. The potential mutagenicity of the primary guanine oxidation product 8-oxo-7,8-dihydroguanine (Og) has been studied intensively, and much information is available about its miscoding potential in vitro and in vivo. Recently, a variety of DNA lesions have been identified as oxidation products of both guanine and 8-oxoguanine, among them spiroiminodihydantoin (Sp) and guanidinohydantoin (Gh). To address questions concerning the mutagenic potential of these secondary products of guanine oxidation, the effect of the lesions on proofreading by DNA polymerase was studied in vitro using the Klenow fragment of Escherichia coli polymerase I (Kf exo+). For the first time, k(cat)/K(m) values were obtained for proofreading of the X:N mismatches (X = Og, Gh, or Sp; N = A, G, or C). Proofreading studies of the terminal mismatches demonstrated the significance of the sequence context flanking the lesion on the 3' side. In addition, a sequence dependence was observed for Gh based on the identity of the base on the 5' side of the lesion providing evidence for a primer slippage mode if N was complementary to the 5' base. Internal mismatches were recognized by Kf exo+ resulting in the excision of the correct base pairs flanking mismatches from the 5' side. The absence of a sequence effect for the Gh- and Sp-containing duplexes can be attributed to the severe destabilization of the lesion-containing duplexes that promotes interaction with the exonuclease domain of the Klenow fragment.     

Crystal structure of an RNA octamer duplex r(CCCIUGGG)2 incorporating tandem I.U wobbles.

The crystal structure of the RNA octamer duplex r(CCCIUGGG)2has been elucidated at 2.5 A resolution. The crystals belong to the space group P21and have unit cell constants a = 33.44 A, b = 43.41 A, c = 49.39 A and beta = 104.7 degrees with three independent duplexes (duplexes 1-3) in the asymmetric unit. The structure was solved by the molecular replacement method and refined to an Rwork/Rfree of 0.185/0.243 using 3765 reflections between 8.0 and 2.5 A. This is the first report of an RNA crystal structure incorporating I.U wobbles and three molecules in the asymmetric unit. Duplex 1 displays a kink of 24 degrees between the mismatch sites, while duplexes 2 and 3 have two kinks each of 19 degrees and 27 degrees, and 24 degrees and 29 degrees, respectively, on either side of the tandem mismatches. At the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for all base pair steps, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectively. The tandem I.U wobbles show intrastrand purine-pyrimidine stacking but exhibit interstrand purine-purine stacking with the flanking C.G pairs. The three independent duplexes are stacked non-coaxially in a head-to-tail fashion to form infinite pseudo-continuous helical columns which form intercolumn hydrogen bonding interactions through the 2'-hydroxyl groups where the minor grooves come together.     

Base pair mismatches and carcinogen-modified bases in DNA: an NMR study of A.C and A.O4meT pairing in dodecanucleotide duplexes

Structural features of A.C mismatches and A.O4meT pairs in the interior of oligodeoxynucleotide duplexes have been investigated by high-resolution two-dimensional proton NMR spectroscopy on the self-complementary d(C-G-C-A-A-G-C-T-C-G-C-G) duplex (designated A.C 12-mer) and and the self-complementary d(C-G-C-A-A-G-C-T-O4meT-G-C-G) duplex (designated A.O4meT 12-mer) containing A.C and A.O4meT pairs at identical positions four base pairs in from either end of and A.O4meT pairs at identical positions four base pairs in from either end of the duplex. Proton NMR shows that there are similar pH-dependent changes in the structure in the A.C 12-mer and A.O4meT 12-mer duplexes. Our studies have focused on the low-pH (pH 5.5) conformation where high-quality two-dimensional NOESY data sets were collected from the exchangeable and nonexchangeable protons in these duplexes. The spectral parameters for the A.C 12-mer and the A.O4meT 12-mer duplexes were very similar, indicating that they must have similar structures at this pH in aqueous solution. Both structures are right-handed double helices with all the bases adopting the normal anti configuration about the glycosidic bond. The same atoms are involved in hydrogen-bond pairing for the A.C mismatch and the A.O4meT pair, and these pairs have a similar spatial relationship to flanking base pairs.(ABSTRACT TRUNCATED AT 250 WORDS)