Structural studies of DNA fragments: the G.T wobble base pair in A, B and Z DNA; the G.A base pair in B-DNA

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G.T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with O2 of T and O6 of G with N3 of T. The X-ray analyses establish that the G.T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G.A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

Tracts of A.T base pairs retard the electrophoretic mobility of short DNA duplexes.

An investigation of the mobility of short duplexes of DNA -octamers and decamers-on polyacrylamide gels is presented, showing that molecules containing less than one helical turn exhibit sequence dependent mobilities. Analysis of chains with different sequences indicates that any arrangement of two or more adjacent A.T base pairs causes a duplex to move more slowly than does any combination of isolated A.T pairs This behavior appears to be an intrinsic property of these sequences, since the anomaly persists in the absence of magnesium or presence of spermine and is not due to strand dissociation. In two decamers we studied, the position of A.T tracts within a duplex can be shown to influence mobility: the sequence GA4T4C associated with bending or curvature of the helix axis when ligated into polymers migrates more slowly than the corresponding sequence GT4A4C, polymers of which migrate as linear B DNA.     

Solution structure of a nitrous acid induced DNA interstrand cross-link

Nitrous acid is a mutagenic agent. It can induce interstrand cross-links in duplex DNA, preferentially at d(CpG) steps: two guanines on opposite strands are linked via a single shared exocyclic imino group. Recent synthetic advances have led to the production of large quantities of such structurally homogenous cross-linked duplex DNA. Here we present the high resolution solution structure of the cross-linked dodecamer [d(GCATCCGGATGC)]2 (the cross-linked guanines are underlined), determined by 2D NMR spectroscopy, distance geometry, restrained molecular dynamics and iterative NOE refinement. The cross-linked guanines form a nearly planar covalently linked 'G:G base pair' with only minor propeller twisting, while the cytidine bases of their normal base pairing partners have been flipped out of the helix and adopt well defined extrahelical positions in the minor groove. On the 5'-side of the cross-link, the minor groove is widened to accommodate these extrahelical bases, and the major groove becomes quite narrow at the cross-link. The cross-linked 'G:G base pair' is well stacked on the spatially adjacent C:G base pairs, particularly on the 3'-side guanines. In addition to providing the first structure of a nitrous acid cross-link in DNA, these studies could be of major importance to the understanding of the mechanisms of nitrous acid cross-linking and mutagenicity, as well as the mechanisms responsible for its repair in intracellular environments. It is also the shortest DNA cross-link structure to be described.     

Structural basis for proficient incorporation of dTTP opposite O6-methylguanine by human DNA polymerase iota

O(6)-methylguanine (O(6)-methylG) is highly mutagenic and is commonly found in DNA exposed to methylating agents, even physiological ones (e.g. S-adenosylmethionine). The efficiency of a truncated, catalytic DNA polymerase ι core enzyme was determined for nucleoside triphosphate incorporation opposite O(6)-methylG, using steady-state kinetic analyses. The results presented here corroborate previous work from this laboratory using full-length pol ι, which showed that dTTP incorporation occurs with high efficiency opposite O(6)-methylG. Misincorporation of dTTP opposite O(6)-methylG occurred with ～6-fold higher efficiency than incorporation of dCTP. Crystal structures of the truncated form of pol ι with O(6)-methylG as the template base and incoming dCTP or dTTP were solved and showed that O(6)-methylG is rotated into the syn conformation in the pol ι active site and that dTTP misincorporation by pol ι is the result of Hoogsteen base pairing with the adduct. Both dCTP and dTTP base paired with the Hoogsteen edge of O(6)-methylG. A single, short hydrogen bond formed between the N3 atom of dTTP and the N7 atom of O(6)-methylG. Protonation of the N3 atom of dCTP and bifurcation of the N3 hydrogen between the N7 and O(6) atoms of O(6)-methylG allow base pairing of the lesion with dCTP. We conclude that differences in the Hoogsteen hydrogen bonding between nucleotides is the main factor in the preferential selectivity of dTTP opposite O(6)-methylG by human pol ι, in contrast to the mispairing modes observed previously for O(6)-methylG in the structures of the model DNA polymerases Sulfolobus solfataricus Dpo4 and Bacillus stearothermophilus DNA polymerase I.     

Structural studies of the O6meG.C interaction in the d(C-G-C-G-A-A-T-T-C-O6meG-C-G) duplex

One- and two-dimensional nuclear magnetic resonance (NMR) experiments have been undertaken to investigate the conformation of the d(C1-G2-C3-G4-A5-A6-T7-T8-C9-O6meG10-C11-G12) self-complementary dodecanucleotide (henceforth called O6meG.C 12-mer), which contains C3.O6meG10 interactions in the interior of the helix. We observe intact base pairs at G2.C11 and G4.C9 on either side of the modification site at low temperature though these base pairs are kinetically destabilized in the O6meG.C 12-mer duplex compared to the G.C 12-mer duplex. One-dimensional nuclear Overhauser effects (NOEs) on the exchangeable imino protons demonstrate that the C3 and O6meG10 bases are stacked into the helix and act as spacers between the flanking G2.C11 and G4.C9 base pairs. The nonexchangeable base and H1', H2', H2', H3', and H4' protons have been completely assigned in the O6meG.C 12-mer duplex at 25 degrees C by two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) experiments. The observed NOEs and their directionality demonstrate that the O6meG.C 12-mer is a right-handed helix in which the O6meG10 and C3 bases maintain their anti conformation about the glycosidic bond at the modification site. The NOEs between the H8 of O6meG10 and the sugar protons of O6meG10 and adjacent C9 exhibit an altered pattern indicative of a small conformational change from a regular duplex in the C9-O6meG10 step of the O6meG.C 12-mer duplex. We propose a pairing scheme for the C3.O6meG10 interaction at the modification site. Three phosphorus resonances are shifted to low field of the normal spectral dispersion in the O6meG.C 12-mer phosphorus spectrum at low temperature, indicative of an altered phosphodiester backbone at the modification site. These NMR results are compared with the corresponding parameters in the G.C 12-mer, which contains Watson-Crick base pairs at the same position in the helix.     

Solution structure of DAPI selectively bound in the minor groove of a DNA T.T mismatch-containing site: NMR and molecular dynamics studies.

The solution structure of the complex between 4', 6-diamidino-2-phenylindole (DAPI) and DNA oligomer [d(GCGATTCGC)]2, containing a central T.T mismatch, has been characterized by combined use of proton one- and two-dimensional NMR spectroscopy, molecular mechanics and molecular dynamics computations including relaxation matrix refinement. The results show that the DAPI molecule binds in the minor groove of the central region 5'-ATT-3' of the DNA oligomer, which predominantly adopts a duplex structure with a global right-handed B-like conformation. In the final models of the complex, the DAPI molecule is located nearly isohelical with its NH indole proton oriented towards the DNA helix axis and forming a bifurcated hydrogen bond with the carbonyl O2 groups of a mismatched T5 and the T6 residue of the opposite strand. Mismatched thymines adopt a wobble base pair conformation and are found stacked between the flanking base pairs, inducing only minor local conformational changes in global duplex structure. In addition, no other binding mechanisms were observed, showing that minor groove binding of DAPI to the mismatch-containing site is favoured in comparison with any other previously reported interaction with G.C sequences.     

Chemical probes of the conformation of DNA modified by cis-diamminedichloroplatinum(II)

The purpose of this work was to analyze at the nucleotide level the distortions induced by the binding of cis-diamminedichloroplatinum(II) (cis-DDP) to DNA by means of chemical probes. In order to test the chemical probes, experiments were first carried out on two platinated oligonucleotides. It has been verified by circular dichroism and gel electrophoresis that the binding of cis-DDP to an AG or to a GTG site within a double-stranded oligonucleotide distorts the double helix. The anomalously slow electrophoretic mobility of the multimers of the platinated and ligated oligomers strongly suggests that the platinated oligonucleotides are bent. The reactivity of the oligonucleotide platinated at the GTG site with chloroacetaldehyde, diethyl pyrocarbonate, and osmium tetraoxide, respectively, suggests a local denaturation of the double helix. The 5'G residue and the T residue within the adduct are no longer paired, while the 3'G residue is paired. The double helix is more distorted (but not denatured) at the 5' side of the adduct than at the 3' side. In the case of the oligonucleotide platinated at the AG site, the double helix is also more distorted at the 5' side of the adduct than at the 3' side. The G residue within the adduct is paired. The reactivities of the chemical probes with six platinated DNA restriction fragments show that even at a relatively high level of platination only a few base pairs are unpaired but the double helix is largely distorted. No local denaturation has been detected at the GG sites separated from the nearest GG or AG sites by at least three bases pairs.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Structural studies of the O6meG.T interaction in the d(C-G-T-G-A-A-T-T-C-O6meG-C-G) duplex

High-resolution proton and phosphorus NMR studies are reported on the self-complementary d(C1-G2-T3-G4-A5-A6-T7-T8-C9-O6meG10-C11-G12) duplex (henceforth called O6meG.T 12-mer), which contains T3.O6meG10 interactions in the interior of the helix. The imino proton of T3 is observed at 9.0 ppm, exhibits a temperature-independent chemical shift in the premelting transition range, and broadens out at the same temperature as the imino proton of the adjacent G2.C11 toward the end of the helix at pH 6.8. We observed inter base pair nuclear Overhauser effects (NOEs) between the base protons at the T3.O6meG10 modification site and the protons of flanking G2.C11 and G4.C9 base pairs, indicative of the stacking of the T3 and O6meG10 bases into the helix. Two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) studies have permitted assignment of the base and sugar H1', H2', and H2' nonexchangeable protons in the O6meG.T 12-mer duplex. The observed NOEs demonstrate an anti conformation about all the glycosidic bonds, and their directionality supports formation of a right-handed helix in solution. The observed NOEs between the T3.O6meG10 interaction and the adjacent G2.C11 and G4.C9 base pairs at the modification site exhibit small departures from patterns for a regular helix in the O6.meG.T 12-mer duplex. The phosphorus resonances exhibit a 0.5 ppm spectral dispersion indicative of an unperturbed phosphodiester backbone for the O6meG.T 12-mer duplex. We propose a model for pairing of T3 and O6meG10 at the modification site in the O6meG.T 12-mer duplex.(ABSTRACT TRUNCATED AT 250 WORDS)     

A new model for DNA containing A.T and I.C base pairs.

DNA polymers containing exclusively A.T or I.C base pairs frequently exhibit D- or E-type X-ray diffraction patterns when dried. The distribution of intensities in fiber patterns appears to demand helical structures with 7 and 7.5 bp/turn, respectively, but it is not stereochemically possible to wind a right-handed antiparallel B-family helix this tightly. It is a simple matter, however, to build a left-handed helix with 7-7.5 bp/turn by incorporating Hoogsteen pairing into a Z helix framework. X-ray intensities calculated from this novel left-handed Hoogsteen model provide as reasonable a fit to the D-DNA diffraction pattern as do intensities calculated from previously proposed right-handed 8-fold models.     

The helical periodicity of DNA on the nucleosome

The precise number of base pairs per turn of the DNA double helix in the nucleosome core particle has been the subject of controversy. In this paper the positions of nuclease cutting sites are analysed in three dimensions. Using this midpoint of the DNA on the nucleosome dyad as origin, the cutting site locations measured along a strand of DNA are mapped onto models of the nucleosome core containing DNA of different helical periodicities. It is found that a helical periodicity of 10.5 base pairs per turn leads to cutting site positions which are sterically inaccessible. In contrast, a periodicity of 10.0 base pairs per turn leads to cutting site positions which are not only sterically sound, but which fall into a pattern such as would be expected when the access of the nuclease to the DNA is restricted by the presence of the histone core on one side and of the adjacent superhelical turn of DNA on the other. As proposed earlier by us (1), a value for the helical periodicity close to 10 base pairs per turn on the nucleosome, taken together with a periodicity close to 10.5 for DNA in solution - a value now established - resolves the so-called linkage number paradox.     

Synthesis and properties of defined DNA oligomers containing base mispairs involving 2-aminopurine.

DNA heptamers containing the mutagenic base analogue 2-aminopurine (AP) have been chemically synthesized and physically characterized. We report on the relative stabilities of base pairs between AP and each of the common DNA bases, as determined from heptamer duplex melts at 275 and 330 nm. Base pairs are ranked in order of decreasing stability: AP.T greater than AP.A greater than AP.C greater than AP.G. It is of interest that AP.A is more stable than AP.C even though DNA polymerase strongly favors the formation of AP.C over AP.A base pairs. Comparisons of melting profiles at 330 nm and 275 nm indicate that AP.T, AP.A, and AP.C base pairs are annealed in heptamer duplexes and melt 2-3 degrees prior to surrounding base pairs, whereas AP.G appears not to be annealed.     

Origin of DNA helical structure and its sequence dependence

Conformational analysis of DNA shows that the origin of the B-form double helix can be attributed in large part to the atomic charge pattern in the base pairs. The charge patterns favor specific helical stacking of the base pairs. Base pairs alone--without backbones--have a strong tendency to form helix, indicating that the backbones play a rather passive role in determining the basic helical structure of DNA. It is mainly the electrostatic interactions determined by the charge pattern on base pairs that stabilize a particular helical conformation. The charge pattern in the base pairs appears to be responsible for much of the sequence dependence of DNA conformation, rather than steric clashes.     

Thermodynamics of DNA duplexes with adjacent G.A mismatches.

The sequence 5'-d(ATGAGCGAAT) forms a very stable self-complementary duplex with four G.A mismatch base pairs (underlined) out of ten total base pairs [Li et al. (1991) Proc. Natl. Acad. Sci. U.S.A. 88, 26-30]. The conformation is in the general B-family and is stabilized by base-pair hydrogen bonding of an unusual type, by favorable base dipole orientations, and by extensive purine-purine stacking at the mismatched sites. We have synthesized 13 decamers with systematic variations in the sequence above to determine how the flanking sequences, the number of G.A mismatches, and the mismatch sequence order (5'-GA-3' or 5'-AG-3') affect the duplex stability. Changing A.T to G.C base pairs in sequences flanking the mismatches stabilizes the duplexes, but only to the extent observed with B-form DNA. The sequence 5'-pyrimidine-GA-purine-3', however, is considerably more stable than 5'-purine-GA-pyrimidine-3'. The most stable sequences with two pairs of adjacent G.A mismatches have thermodynamic parameters for duplex formation that are comparable to those for fully Watson-Crick base-paired duplexes. Similar sequences with single G.A pairs are much less stable than sequences with adjacent G.A mismatches. Reversing the mismatch order from 5'-GA-3' to 5'-AG-3' results in an oligomer that does not form a duplex. These results agree with predictions from the model derived from NMR and molecular mechanics and indicate that the sequence 5'-pyrimidine-GA-purine-3' forms a stable conformational unit that fits quite well into a B-form double helix.(ABSTRACT TRUNCATED AT 250 WORDS)     

Covalent carcinogenic lesions in DNA: NMR studies of O6-methylguanosine containing oligonucleotide duplexes

We report on proton and phosphorus high resolution NMR investigations of the self-complementary dodecanucleotide d(C1-G2-N3-G4-A5-A6-T7-T8-C9-O6meG10-C11-G12) duplexes (henceforth called O6 meG.N 12-mers), N = C, T, A and G, which contain N3.O6meG10 interactions in the interior of the helix. These sequences containing a single modified O6meG per strand were prepared by phosphoamidite synthesis and provide an excellent model for probing the structural basis for covalent carcinogenic lesions in DNA. Distance dependent nuclear Overhauser effect (NOE) measurements and line widths of imino protons demonstrate that the N3 and O6meG.10 bases stack into the duplex and are flanked by stable Watson-Crick base pairs at low temperature for all four O6meG.N 12-mer duplexes. The imino proton of T3 in the O6meG.T 12-mer and G3 in the O6meG.N 12-mer helix, which are associated with the modification site, resonate at unusually high field (8.5 to 9.0 ppm) compared to imino protons in Watson-Crick base pairs (12.5 to 14.5 ppm). The nonexchangeable base and sugar protons have been assigned from two dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) measurements on the O6meG.N 12-mer helices. The directionality of the distance dependent NOEs establish all O6meG.N duplexes to be right-handed helices in solution. The glycosidic torsion angles are in the anti range at the N3.O6meG10 modification site except for O6meG10 in the O6meG.G 12-mer duplex which adopts a syn configuration. This results in altered NOEs between the G3 (anti).O6meG10 (syn) pair and flanking G2.C11 and G4.C9 base pairs in the O6meG.G 12-mer duplex. We observe pattern reversal for cross peaks in the COSY spectrum linking the sugar H1' protons with the H2',2" protons at the G2 and O6meG10 residues in the O6meG.N 12-mer duplexes with the effect least pronounced for the O6meG.T 12-mer helix. The proton chemical shift and NOE data have been analyzed to identify regions of conformational perturbations associated with N3.O6meG10 modification sites in the O6meG.N 12-mer duplexes. The proton decoupled phosphorus spectrum of O6meG.T 12-mer duplex exhibits an unperturbed phosphodiester backbone in contrast to the phosphorus spectra of the O6meG.C 12-mer, O6meG.G 12-mer and O6meG.A 12-mer duplexes which exhibit phosphorus resonances dispersed over 2 ppm characteristic of altered phosphodiester backbones at the modification site. Tentative proposals are put forward for N3.O6meG10 pairing models based on the available NMR data and serve as a guide for the design of future experiments.     

Hydrogen and hydration of DNA and RNA oligonucleotides

In this paper, hydrogen bonding interaction and hydration in crystal structures of both DNA and RNA oligonucleotides are discussed. Their roles in the formation and stabilization of oligonucleotides have been covered. Details of the Watson-Crick base pairs G.C and A.U in DNA and RNA are illustrated. The geometry of the wobble (mismatched) G.U base pairs and the cis and almost trans conformations of the mismatched U.U base pairs in RNA is described. The difference in hydration of the Watson-Crick base pairs G.C, A.U and the wobble G.U in different sequences of codon-anticodon interaction in double helical molecules are indicative of the effect of hydration. The hydration patterns of the phosphate, the 2'-hydroxyl groups, the water bridges linking the phosphate group, N7 (purine) and N4 of Cs or O4 of Us in the major groove, the water bridges between the 2'-hydroxyl group and N3 (purine) and O2 (pyrimidine) in the minor groove are discussed.     

An NMR structural study of deaminated base pairs in DNA.

The structurally aberrant base pairs TG, UG and TI may occur in DNA as a consequence of deamination of 5-methylcytosine, cytosine and adenine respectively. Results of NMR spectroscopic studies are reported here for these deaminated base pairs in a model seven base pair long oligonucleotide duplex. We find that in all three cases, the DNA helix is a normal B form and both mispaired bases are intrahelical and hydrogen bonded with one another in a wobble geometry. Similarly, in all three cases, all sugars are found to be normal C2' endo in conformation. Symmetric structural perturbations are observed in the helix twist on the 3' side of the mispaired pyrimidine and on the 5' side of the mispaired purine. In all three cases, the amino group of the G residue on the 3' side of the mispaired pyrimidine shows hindered rotation. Although less thermodynamically stable than helices containing only Watson-Crick base pairs, these helices melt normally from the ends and not from the mispair outwards.     

Single base mismatches in DNA. Long- and short-range structure probed by analysis of axis trajectory and local chemical reactivity

We have devised a procedure to generate any single base mismatch in a constant sequence context, and have studied these from two points of view. (1) We have examined electrophoretic mobility of 458 base-pair fragments containing approximately centrally located single mismatches, in polyacrylamide gels, compared to fully matched DNA fragments. We found that no single mismatch caused a significant perturbation of gel mobility, and we conclude that all the mismatches may be accommodated within a helical geometry such that there is no alteration of the path of the helix axis in a straight DNA molecule. (2) We have studied all the single mismatches with respect to reactivity to a number of chemical probes. We found that: (a) No mispaired adenine bases are reactive to diethyl pyrocarbonate and are therefore not simply unpaired such that N-7 is exposed. (b) A number of mispaired thymine bases are reactive to osmium tetroxide, and cytosine bases to hydroxylamine. (c) Where crystal or nuclear magnetic resonance structures are available, the reactivity correlates with exposure of the pyrimidine 5,6 double bonds to attack in the major groove as a result of wobble base-pair formation. This is particularly clear for G.T and I.T base-pairs. (d) Reactivity of bases in mismatched pairs can be dependent on sequence context. (e) Reactivity of the C.C mismatch to hydroxylamine is suppressed at low pH, suggesting that a rearrangement of base-pairing occurs on protonation. The results overall are consistent with the formation of stacked intrahelical base-pairs wherever possible, resulting in no global distortion of the DNA structure, but specific enhancement of chemical reactivity in some cases.     

Breathing and bending fluctuations in DNA modeled by an open-base-pair kink coupled to axial compression

We develop a model designed to show that flexibility in the DNA molecule can arise from relatively improbable transient opening of base pairs. The axial direction changes at the site of an open base pair. The region between open base pairs is a double helix of hydrogen-bonded base pairs with a slightly decreased rise per residue and a slightly increased helical winding angle. An analysis of the model yields several testable predictions. For example, we predict probability 0.026 for a base pair to be open at 25°C, a value close to that measured by hydrogen-exchange experiments. Other predictions involve matters like the variation of persistence length with ionic strength and temperature, the variation of helical winding angle with temperature, and the kinetics of heat denaturation. An additional result of the analysis is an explanation of the high degree of local stiffness of the DNA molecule. Strong resistance to bending fluctuations is provided from two sources: increased polyelectrolyte repulsion among phosphate groups in the axially compressed stacks between open base pairs and the tendency of stacking forces to oppose opening of a base pair. Stacking forces, however, also support compression of the stacks between open base pairs, so that the net effect of stacking forces on elastic bending of DNA is small relative to the polyelectrolyte effect. If the ionic charges on the phosphate groups were absent, DNA would spontaneously fold, driven by the entropy gained when about 1% of its base pairs open.     

Parallel stranded DNA under scanning tunnelling microscope: the main characteristics of the double helix.

Using the scanning tunnelling microscopy we have directly observed the parallel stranded DNA of 43 bp in length, containing alternating AT-stretches. The double helix is right-handed and has the same width of each grooves equal to 17.4 A. The average pitch of the helical turn is about 34 A. The parallel double helix possesses no more than 8.6 bases per one turn. The diameter of the parallel stranded DNA molecule is 17-18 A. We conclude that in parallel DNA double helix the angle between N-glycoside bounds in trans-Crick-Watson base pairs is close to 180 degrees.