Tetraplex Formation of d(GGGGGTTTTT): 1H NMR Study in Solution

Abstract

The oligonucleotide d(G₅T₅) can in principle form a fully matched duplex with G · T pairing and/or a tetraplex. Non-denaturing gel electrophoresis, circular dichroism and NMR experiments show that the tetraplex is exclusively formed by this oligomer in solution. In the presence of its complementary strand d(A₅C₅) at low temperature, d(G₅T₅) forms the tetraplex over the normally expected Watson-Crick duplex. However, when d(G₅T₅) and d(A₅C₅) are mixed together in equimolar amounts and heated for several minutes at 85°C, and then allowed to cool, the product was essentially the Watson-Crick duplex. The lack of resolution in the 500 MHz ¹H NMR spectra and the presence of extensive spin diffusion do not allow us to derive a quantitative structure for the tetraplex from the NMR data. However, we find good qualitative agreement between the NOESY and MINSY data and a theoretically derived stereochemically sound structure in which the G's and T's are part of a parallel tetraplex.     

Guanine tetraplex formation by short DNA fragments containing runs of guanine and cytosine.

Using CD spectroscopy, guanine tetraplex formation was studied with short DNA fragments in which cytosine residues were systematically added to runs of guanine either at the 5' or 3' ends. Potassium cations induced the G-tetraplex more easily with fragments having the guanine run at the 5' end, which is just an opposite tendency to what was reported for (G+T) oligonucleotides. However, the present (G+C) fragments simultaneously adopted other conformers that complicated the analysis. We demonstrate that repeated freezing/thawing, performed at low ionic strength, is a suitable method to exclusively stabilize the tetraplex in the (G+C) DNA fragments. In contrast to KCl, the repeated freeze/thaw cycles better stabilized the tetraplex with fragments having the guanine run on the 3' end. The tendency of guanine blocks to generate the tetraplex destabilized the d(G5).d(C5) duplex whose strands dissociated, giving rise to a stable tetraplex of (dG5) and single-stranded (dC5). In contrast to d(G3C3) and d(G5C5), repeated freezing/thawing induced the tetraplex even with the self-complementary d(C3G3) or d(C5G5); hence the latter oligonucleotides preferred the tetraplex to the apparently very stable duplex. The tetraplexes only included guanine blocks while the 5' end cytosines interfered neither with the tetraplex formation nor the tetraplex structure.     

NMR studies of a DNA containing 8-hydroxydeoxyguanosine.

The effects of hydroxylation at the C8 of a deoxyguanosine residue in DNA were studied by NMR analysis of a self-complementary dodecanucleotide, d(C1-G2-C3-oh8G4-A5-A6-T7-T8-C9-G10-C11-G12), which has an 8-hydroxy-2'-deoxyguanosine (oh8dG) residue at the 4th position. NMR data indicate that the 8-hydroxyguanine (oh8G) base takes a 6,8-diketo tautomeric form and is base-paired to C with Watson-Crick type hydrogen bonds in a B-form structure. The thermal stability of the duplex is reduced, but the overall structure is much the same as that of the unmodified d(CGCGAATTCGCG) duplex. The structural changes caused by 8-hydroxylation of the deoxyguanosine, if any, are localized near the modification site.     

Non-Watson-Crick structures in oligodeoxynucleotides: self-association of d(TpCpGpA) stabilized at acidic pH

The 1H NMR spectrum of the tetradeoxynucleotide d(TpCpGpA) was examined as a function of temperature, pH, and concentration. At pH 7 and above the solution conformation for this oligodeoxynucleotide appears to be a mixture of random coil and Watson-Crick duplex. At 25 degrees C, a pH titration of d(TpCpGpA) shows that distinct conformational changes occur as the pH is lowered below 7.0. These conformational changes are reversible upon readjusting the pH to neutrality, indicating the presence of a pH-dependent set of conformational equilibria. At 25 degrees C, the various conformational states in the mixture are in rapid exchange on the NMR time scale. Examination of the titration curve shows the presence of distinct conformational states at pH greater than 7, and between pH 4 and pH 5. At pH less than 4, a third conformational state is present. When the pH titration is repeated at 5 degrees C, the conformational equilibria are in slow exchange on the NMR time scale; distinct signals from each conformational state are observable. The stable conformational state present between pH 4 and pH 5 represents an ordered conformation of d(TpCpGpA) which dissociates to a less ordered structure upon raising the temperature. This ordered conformation does not result from an intramolecular rearrangement, as is shown by by spectra obtained by varying oligodeoxynucleotide concentration at constant pH. The ordered conformation differs from the Watson-Crick helix, as is shown from nuclear Overhauser enhancement experiments, as well as chemical shift data. An ordered conformation for d(TpCpGpA) was previously reported [Reid, D. G., Salisbury, S. A., Brown, T., & Williams, D. H. (1985) Biochemistry 24, 4325-4332].(ABSTRACT TRUNCATED AT 250 WORDS)     

Circular dichroism spectra of DNA quadruplexes [d(G(5)T(5))](4) as formed with G(4) and T(4) tetrads and [d(G(5)T(5)). d(A(5)C(5))]2 as formed with Watson-Crick-like (G-C)(2) and (T-A)(2) tetrads

We utilize electrophoresis and find that a thermally treated equimolar mixture of the oligonucleotide d(G(5)T(5)) and its complementary oligonucleotide d(A(5)C(5)) exhibits either two bands or a single band in one lane, depending on the conditions of the incubation solutions. The thermally treated d(G(5)T(5)) solution loaded in a different lane exhibits a single band of the parallel quadruplex [d(G(5)T(5))](4), which is composed of homocyclic hydrogen-bonded G(4) and T(4) tetrads previously proposed. For the thermally treated equimolar mixture of d(G(5)T(5)) and d(A(5)C(5)), the fast band is assigned to a Watson-Crick d(G(5)T(5)). d(A(5)C(5)) duplex, so that the slow band with the same low mobility as that of [d(G(5)T(5))](4) may be assigned to either [d(G(5)T(5))](4) itself or a [d(G(5)T(5)). d(A(5)C(5))](2) quadruplex. If the latter compound is true, this may be the antiparallel quadruplex composed of the heterocyclic hydrogen-bonded G-C-G-C and T-A-T-A tetrads proposed previously. After removing these three bands for the duplex and two kinds of hypothetical quadruplexes, we electrophoretically elute the corresponding compounds in the same electrophoresis buffer using an electroeluter. The eluted compounds are ascertained to be stable by electrophoresis. The circular dichroism (CD) and UV absorption spectra measured for the three isolated compounds are found to be clearly different. For the electrophoretic elution of the hypothetical [d(G(5)T(5))](4) quadruplex, the result of the molecularity of n = 4 obtained from the CD melting curve analysis provides further support for the formation of the parallel [d(G(5)T(5))](4) quadruplex already proposed. For the thermally treated equimolar mixture of d(G(5)T(5)) and d(C(5)A(5)), the fast band with a molecularity of n = 2 corresponds to the Watson-Crick duplex, d(G(5)T(5)). d(A(5)C(5)). The slow band with a molecularity of n = 4 indicates the antiparallel quadruplex [d(G(5)T(5)). d(A(5)C(5))](2), whose observed CD and UV spectra are different from those of [d(G(5)T(5))](4). By electrophoresis, after reannealing the eluted compound [d(G(5)T(5)). d(A(5)C(5))](2), a distinct photograph showing the band splitting of this quadruplex band into the lower duplex and upper quadruplex bands is not possible; but by a transilluminator, we occasionally observe this band splitting with the naked eye. The linear response polarizability tensor calculations for the thus determined structures of the [d(G(5)T(5))](4) quadruplex, the McGavin-like [d(G(5)T(5)). d(A(5)C(5))](2) quadruplex, and the Watson-Crick d(G(5)T(5)). d(A(5)C(5)) duplex are found to qualitatively predict the observed CD and UV spectra.     

Crystallographic characterization of an exocyclic DNA adduct: 3,N4-etheno-2'-deoxycytidine in the dodecamer 5'-CGCGAATTepsilonCGCG-3'

Exocyclic DNA adducts are formed from metabolites of chemical carcinogens and have also been detected as endogenous lesions in human DNA. The exocyclic adduct 3,N(4)-etheno-2'-deoxycytidine (epsilon dC), positioned opposite deoxyguanosine in the B-form duplex of the dodecanucleotide d(CGCGAATTepsilonCGCG), has been crystallographically characterized at 1.8A resolution. This self-complementary oligomer crystallizes in space group P3(2)12, containing a single strand in the asymmetric unit. The crystal structure was solved by isomorphous replacement with the corresponding unmodified dodecamer structure. Exposure of both structures to identical crystal packing forces allows a detailed investigation of the influence of the exocyclic base adduct on the overall helical structure and local geometry. Structural changes are limited to the epsilon C:G and adjacent T:A and G:C base-pairs. The standard Watson-Crick base-pairing scheme, retained in the T:A and G:C base-pairs, is blocked by the etheno bridge in the epsilon C:G pair. In its place, a hydrogen bond involving O2 of epsilon C and N1 of G is present. Comparison with an epsilon dC-containing NMR structure confirms the general conformation reported for epsilon C:G, including the hydrogen bonding features. Superposition with the crystal structure of a DNA duplex containing a T:G wobble pair shows similar structural changes imposed by both mismatches. Evaluation of the hydration shell of the duplex with bond valence calculations reveals two sodium ions in the crystal.     

Circular dichroism spectroscopy reveals invariant conformation of guanine runs in DNA

We demonstrate that the characteristic circular dichroism (CD) features of the parallel-stranded DNA tetraplex of d(G4), especially the strong band at 260 nm, are characteristic for the B and A forms of the antiparallel duplex of d(C4G4). Hence, this band evidently originates from intrastrand guanine-guanine stacking, which is therefore very similar in the duplex and tetraplex DNA. In addition, the same type of the CD spectrum is provided by the ordered single strand of d(GA)10. This observation suggests that the ordered single strand of d(GA)10 is stabilized by a core of guanines stacked like in the parallel tetraplex. This view is used to start the modeling of the molecular structure of the ordered d(GA)10 single strand. Our studies suggest that guanine itself is strong enough to stabilize various secondary structures of DNA, which is a property relevant to thinking about the origin and evolution of molecular replicators.     

Wobble dG X dT pairing in right-handed DNA: solution conformation of the d(C-G-T-G-A-A-T-T-C-G-C-G) duplex deduced from distance geometry analysis of nuclear Overhauser effect spectra

We report below on features of the three-dimensional structure of the d(C-G-T-G-A-A-T-T-C-G-C-G) self-complementary duplex (designated 12-mer GT) containing symmetrical G X T mismatches in the interior of the helix. The majority of the base and sugar protons in the 12-mer GT duplex were assigned by two-dimensional nuclear Overhauser effect (NOESY) spectra in H2O and D2O solution. A set of 92 short (less than 4.5-A) proton-proton distances defined by lower and upper bounds for one symmetrical half of the 12-mer GT duplex were estimated from NOESY data sets recorded as a function of mixing time. These experimental distances combined with nucleotide bond length parameters were embedded into Cartesian space; several trial structures were refined to minimize bond geometry and van der Waals and chirality error. Confidence in this approach is based on the similarity of the refined structures for the solution conformation of the 12-mer GT duplex. The G and T bases pair through two imino-carbonyl hydrogen bonds, and stacking is maintained between the G X T wobble pair and adjacent Watson-Crick G X C pairs. The experimental distance information is restricted to base and sugar protons, and hence structural features such as base pair overlap, glycosidic torsion angles, and sugar pucker are well-defined by this combination of NMR and distance geometry methods. By contrast, we are unable to define the torsion angles about the bonds C3'-O3'-P-O5'-C5'-C4' in the backbone of the nucleic acid.     

The structure of guanosine-thymidine mismatches in B-DNA at 2.5-A resolution

The structure of the deoxyoligomer d(C-G-C-G-A-A-T-T-T-G-C-G) was determined at 2.5-A resolution by single crystal x-ray diffraction techniques. The final R factor is 18% with the location of 71 water molecules. The oligomer crystallizes in a B-DNA-type conformation, with two strands interacting to form a dodecamer duplex. The double helix consists of four A X T and six G X C Watson-Crick base pairs and two G X T mismatches. The G X T pairs adopt a "wobble" structure with the thymine projecting into the major groove and the guanine into the minor groove. The mispairs are accommodated in the normal double helix by small adjustments in the conformation of the sugar phosphate backbone. A comparison with the isomorphous parent compound containing only Watson-Crick base pairs shows that any changes in the structure induced by the presence of G X T mispairs are highly localized. The global conformation of the duplex is conserved. The G X T mismatch has already been studied by x-ray techniques in A and Z helices where similar results were found. The geometry of the mispair is essentially identical in all structures so far examined, irrespective of the DNA conformation. The hydration is also similar with solvent molecules bridging the functional groups of the bases via hydrogen bonds. Hydration may be an important factor in stabilizing G X T mismatches. A characteristic of Watson-Crick paired A X T and G X C bases is the pseudo 2-fold symmetry axis in the plane of the base pairs. The G X T wobble base pair is pronouncedly asymmetric. This asymmetry, coupled with the disposition of functional groups in the major and minor grooves, provides a number of features which may contribute to the recognition of the mismatch by repair enzymes.     

Thermodynamics of triple helix formation: spectrophotometric studies on the d(A)10.2d(T)10 and d(C+3T4C+3).d(G3A4G3).d(C3T4C3) triple helices.

We have stabilized the d(A)10.2d(T)10 and d(C+LT4C+3).d(G3A4G3).d(C3T4C3) triple helices with either NaCl or MgCl2 at pH 5.5. UV mixing curves demonstrate a 1:2 stoichiometry of purine to pyrimidine strands under the appropriate conditions of pH and ionic strength. Circular dichroic titrations suggest a possible sequence-independent spectral signature for triplex formation. Thermal denaturation profiles indicate the initial loss of the third strand followed by dissociation of the underlying duplex with increasing temperature. Depending on the base sequence and ionic conditions, the binding affinity of the third strand for the duplex at 25 degrees C is two to five orders of magnitude lower than that of the two strands forming the duplex. Thermodynamic parameters for triplex formation were determined for both sequences in the presence of 50 mM MgCl2 and/or 2.0 M NaCl. Hoogsteen base pairs are 0.22-0.64 kcal/mole less stable than Watson-Crick base pairs, depending on ionic conditions and base composition. C+.G and T.A Hoogsteen base pairs appear to have similar stability in the presence of Mg2+ ions at low pH.     

Solution structure of the luzopeptin-DNA complex.

The luzopeptin-d(C-A-T-G) complex (1 drug/duplex) has been generated in aqueous solution and its structure characterized by a combined application of two-dimensional NMR experiments and molecular dynamics calculations. One equivalent of luzopeptin binds to the self-complementary tetranucleotide duplex with the 2-fold symmetry of the antitumor agent and the DNA oligomer retained on complex formation. We have assigned the exchangeable and nonexchangeable proton resonances of luzopeptin and the d(C-A-T-G) duplex in the complex and identified the intermolecular proton-proton NOEs that define the alignment of the antitumor agent at its binding site in duplex DNA. The analysis was greatly aided by a large number of intermolecular NOEs involving exchangeable protons on both the luzopeptin and the DNA in the complex. The molecular dynamics calculations were guided by 140 intramolecular nucleic acid distance constraints, 74 intramolecular luzopeptin distance constraints, and 96 intermolecular distance constraints between luzopeptin and the nucleic acid protons in the complex. The quinoline rings of luzopeptin bisintercalate at d(C-A).d(T-G) steps in the d(C-A-T-G) duplex and sandwich two Watson-Crick A.T base pairs between the bisintercalation site. The long axis of the quinoline rings are collinear with the long axis of the flanking Watson-Crick C1.G4 and A2.T3 base pairs such that the OCH3-6 group is directed toward the C1-A2 step and the OH-3 group is directed toward the T3-G4 step in the complex. The quinoline chromophore stacks with purines on both strands, with the quinoline A ring stacked on A2 and the quinoline B ring stacked on G4 in the complex. The C1.G4 and A2.T3 base pairs that flank the intercalation sites are parallel to each other with partial overlap of T3 and G4 in the T3-G4 step but no overlap of C1 and A2 in the C1-A2 step in the complex. The cyclic depsipeptide ring of luzopeptin is positioned in the minor groove of the d(C-A-T-G) duplex with the oligopeptide and oligonucleotide chains running antiparallel to each other. The cyclic depsipeptide backbone of luzopeptin exhibits cis peptide bonds at Pyr-Gly and Gly-Sar steps in the luzopeptin-d(C-A-T-G) complex in solution, in contrast to all trans peptide bonds for free luzopeptin in the crystalline state.(ABSTRACT TRUNCATED AT 400 WORDS)     

Nearest-neighbor thermodynamics and NMR of DNA sequences with internal A.A, C.C, G.G, and T.T mismatches

Thermodynamic measurements are reported for 51 DNA duplexes with A.A, C.C, G.G, and T.T single mismatches in all possible Watson-Crick contexts. These measurements were used to test the applicability of the nearest-neighbor model and to calculate the 16 unique nearest-neighbor parameters for the 4 single like with like base mismatches next to a Watson-Crick pair. The observed trend in stabilities of mismatches at 37 degrees C is G.G > T.T approximately A.A > C.C. The observed stability trend for the closing Watson-Crick pair on the 5' side of the mismatch is G.C >/= C.G >/= A.T >/= T.A. The mismatch contribution to duplex stability ranges from -2.22 kcal/mol for GGC.GGC to +2.66 kcal/mol for ACT.ACT. The mismatch nearest-neighbor parameters predict the measured thermodynamics with average deviations of DeltaG degrees 37 = 3.3%, DeltaH degrees = 7. 4%, DeltaS degrees = 8.1%, and TM = 1.1 degrees C. The imino proton region of 1-D NMR spectra shows that G.G and T.T mismatches form hydrogen-bonded structures that vary depending on the Watson-Crick context. The data reported here combined with our previous work provide for the first time a complete set of thermodynamic parameters for molecular recognition of DNA by DNA with or without single internal mismatches. The results are useful for primer design and understanding the mechanism of triplet repeat diseases.     

Theoretical study of the geometrical arrangement of GT and GA wobble pairs in two short duplexes, Proton NMR chemical shifts and interaction energy calculations

NMR shielding constants are calculated for the base protons of duplexes formed by the dodecamer d(CGTGAATTCGCG) and the decamer d(CCAAGATTGG). A good agreement with experimental data is obtained for B-DNA helices in which the wobble GT and GA pairs are in the plane of the corresponding GC pairs of the parent duplexes formed by d(CGCGAATTCGCG) and d(CCAAGCTTGG), if the glycosyl bonds of T and G or A and G are symmetrical with respect to the dyad axis of the Watson-Crick GC pair. Interaction energy calculations show that this type of geometrical arrangement, which implies a distortion of the ribonphosphate backbone of both strands of the duplexes are more stable than those in which only one strand has its conformation modified by the presence of the wobble pair. For the duplex containing the GA pair, NMR chemical shifts as well as interaction energy computations favour the Watson-Crick hydrogen bonding scheme. The variation of the different contributions (intrastrand, interstrand, pair-pair) to the interaction energy between the bases of the duplexes, with the geometrical arrangement of the wobble pairs, is reported.     

A DNA hairpin with a single residue loop closed by a strongly distorted Watson-Crick G x C base-pair

Our previous NMR and modeling studies have shown that the single-stranded 19mer oligonucleotides d(AGCTTATC-ATC-GATAA GCT) -ATC- and d(AGCTTATC-GAT-GATAAGCT) -GAT- encompassing the strongest topoisomerase II cleavage site in pBR322 DNA could form stable hairpin structures. A new sheared base-pair, the pyrimidine-purine C x A, was found to close the single base -ATC- loop, while -GAT- displayed a flexible loop of three/five residues with no stabilizing interactions. Now we report a structural study on -GAC-, an analog of -GAT-, derived through the substitution of the loop residue T by C. The results obtained from NMR, non-denaturing PAGE, UV-melting, circular dichroism experiments and restrained molecular dynamics indicate that -GAC- adopts a hairpin structure folded through a single residue loop. In the -GAC- hairpin the direction of the G9 sugar is reversed relative to the C8 sugar, thus pushing the backbone of the loop into the major groove. The G9 x C11 base-pair closing the loop is thus neither a sheared base-pair nor a regular Watson-Crick one. Although G9 and C11 are paired through hydrogen bonds of Watson-Crick type, the base-pair is not planar but rather adopts a wedge-shaped geometry with the two bases stacked on top of each other in the minor groove. The distortion decreases the sugar C1'-C1' distance between the paired G9 and C11, to 8 A versus 11 A in the standard B-DNA. The A10 residue at the center of the loop interacts with the G9 x C11 base-pair, and seems to contribute to the extra thermal stability displayed by -GAC- compared to -GAT-. Test calculations allowed us to identify the experimental NOEs critical for inducing the distorted G.C Watson-Crick base-pair. The preference of -GAC- for a hairpin structure rather than a duplex is confirmed by the diffusion constant values obtained from pulse-field gradient NMR experiments. All together, the results illustrate the high degree of plasticity of single-stranded DNAs which can accommodate a variety of turn-loops to fold up on themselves.     

Proton NMR studies of 5'-d-(TC)(3) (CT)(3) (AG)(3)-3'--a paperclip triplex: the structural relevance of turns

In this study, we present the results of structural analysis of an 18-mer DNA 5'-T(1)C(2)T(3)C(4)T(5)C(6)C(7)T(8)C(9)T(10)C(11)T(12)A(13)G(14)A(15)G(16)A(17)G(18)-3' by proton nuclear magnetic resonance (NMR) spectroscopy and molecular modeling. The NMR data are consistent with characteristics for triple helical structures of DNA: downfield shifting of resonance signals, typical for the H3(+) resonances of Hoogsteen-paired cytosines; pH dependence of these H3(+) resonance; and observed nuclear Overhauser effects consistent with Hoogsteen and Watson-Crick basepairing. A three-dimensional model for the triplex is developed based on data obtained from two-dimensional NMR studies and molecular modeling. We find that this DNA forms an intramolecular "paperclip" pyrimidine-purine-pyrimidine triple helix. The central triads resemble typical Hoogsteen and Watson-Crick basepairing. The triads at each end region can be viewed as hairpin turns stabilized by a third base. One of these turns is comprised of a hairpin turn in the Watson-Crick basepairing portion of the 18-mer with the third base coming from the Hoogsteen pairing strand. The other turn is comprised of two bases from the continuous pyrimidine portion of the 18-mer, stabilized by a hydrogen-bond from a purine. This "triad" has well defined structure as indicated by the number of nuclear Overhauser effects and is shown to play a critical role in stabilizing triplex formation of the internal triads.     

The first example of a Hoogsteen base-paired DNA duplex in dynamic equilibrium with a Watson-Crick base-paired duplex--a structural (NMR), kinetic and thermodynamic study.

A single-point substitution of the O4' oxygen by a CH2 group at the sugar residue of A6 (i.e. 2'-deoxyaristeromycin moiety) in a self-complementary DNA duplex, 5'-d(C1G2C3G4A5A6T7T8C9G10C11G12)2(-3), has been shown to steer the fully Watson-Crick basepaired DNA duplex (1A), akin to the native counterpart, to a doubly A6:T7 Hoogsteen basepaired (1B) B-type DNA duplex, resulting in a dynamic equilibrium of (1A)<==>(1B): Keq = k1/k(-1) = 0.56+/-0.08. The dynamic conversion of the fully Watson-Crick basepaired (1A) to the partly Hoogsteen basepaired (1B) structure is marginally kinetically and thermodynamically disfavoured [k1 (298K) = 3.9 0.8 sec(-1); deltaHdegrees++ = 164+/-14 kJ/mol; -TdeltaS degrees++ (298K) = -92 kJ/mol giving a deltaG degrees++ 298 of 72 kJ/mol. Ea (k1) = 167 14 kJ/mol] compared to the reverse conversion of the Hoogsteen (1B) to the Watson-Crick (1A) structure [k-1 (298K) = 7.0 0.6 sec-1, deltaH degrees++ = 153 13 kJ/mol; -TdeltaSdegrees++ (298K) = -82 kJ/mol giving a deltaGdegrees++(298) of 71 kJ/mol. Ea (k-1) = 155 13 kJ/mol]. Acomparison of deltaGdegrees++(298) of the forward (k1) and backward (k-1) conversions, (1A)<==>(1B), shows that there is ca 1 kJ/mol preference for the Watson-Crick (1A) over the double Hoogsteen basepaired (1B) DNA duplex, thus giving an equilibrium ratio of almost 2:1 in favour of the fully Watson-Crick basepaired duplex. The chemical environments of the two interconverting DNA duplexes are very different as evident from their widely separated sets of chemical shifts connected by temperature-dependent exchange peaks in the NOESY and ROESY spectra. The fully Watson-Crick basepaired structure (1A) is based on a total of 127 intra, 97 inter and 17 cross-strand distance constraints per strand, whereas the double A6:T7 Hoogsteen basepaired (1B) structure is based on 114 intra, 92 inter and 15 cross-strand distance constraints, giving an average of 22 and 20 NOE distance constraints per residue and strand, respectively. In addition, 55 NMR-derived backbone dihedral constraints per strand were used for both structures. The main effect of the Hoogsteen basepairs in (1B) on the overall structure is a narrowing of the minor groove and a corresponding widening of the major groove. The Hoogsteen basepairing at the central A6:T7 basepairs in (1B) has enforced a syn conformation on the glycosyl torsion of the 2'-deoxyaristeromycin moiety, A6, as a result of substitution of the endocyclic 4'-oxygen in the natural sugar with a methylene group in A6. A comparison of the Watson-Crick basepaired duplex (1A) to the Hoogsteen basepaired duplex (1B) shows that only a few changes, mainly in alpha, sigma and gamma torsions, in the sugar-phosphate backbone seem to be necessary to accommodate the Hoogsteen basepair.     

NMR studies of the exocyclic 1,N6-ethenodeoxyadenosine adduct (epsilon dA) opposite thymidine in a DNA duplex. Nonplanar alignment of epsilon dA(anti) and dT(anti) at the lesion site

Two-dimensional proton NMR studies are reported on the complementary d(C-A-T-G-T-G-T-A-C).d(G-T-A-C-epsilon A-C-A-T-G) nonanucleotide duplex (designated epsilon dA.dT 9-mer duplex) containing 1,N6-ethenodeoxyadenosine (epsilon dA), a carcinogen-DNA adduct, positioned opposite thymidine in the center of the helix. Our NMR studies have focused on the conformation of the epsilon dA.dT 9-mer duplex at neutral pH with emphasis on defining the alignment at the dT5.epsilon dA14 lesion site. The through-space NOE distance connectivities establish that both dT5 and epsilon dA14 adopt anti glycosidic torsion angles, are directed into the interior of the helix, and stack with flanking Watson-Crick dG4.dC15 and dG6.dC13 pairs. Furthermore, the d(G4-T5-G6).d(C13-epsilon A14-C15) trinucleotide segment centered about the dT5.epsilon dA14 lesion site adopts a right-handed helical conformation in solution. Energy minimization computations were undertaken starting from six different alignments of dT5(anti) and epsilon dA14(anti) at the lesion site and were guided by distance constraints defined by lower and upper bounds estimated from NOESY data sets on the epsilon dA.dT 9-mer duplex. Two families of energy-minimized structures were identified with the dT5 displaced toward either the flanking dG4.dC15 or the dG6.dC13 base pair. These structures can be differentiated on the basis of the observed NOEs from the imino proton of dT5 to the imino proton of dG4 but not dG6 and to the amino protons of dC15 but not dC13 that were not included in the constraints data set used in energy minimization. Our NMR data are consistent with a nonplanar alignment of epsilon dA14(anti) and dT5(anti) with dT5 displaced toward the flanking dG4.dC15 base pair within the d(G4-T5-G6).d(C13-epsilon A14-C15) segment of the epsilon dA.dT 9-mer duplex.     

NMR studies of abasic sites in DNA duplexes: deoxyadenosine stacks into the helix opposite the cyclic analogue of 2-deoxyribose

Proton and phosphorus NMR studies are reported for the complementary d(C-A-T-G-A-G-T-A-C).d(G-T-A-C-F-C-A-T-G) nonanucleotide duplex (designated APF 9-mer duplex) which contains a stable abasic site analogue, F, in the center of the helix. This oligodeoxynucleotide contains a modified tetrahydrofuran moiety, isosteric with 2-deoxyribofuranose, which serves as a structural analogue of a natural apurinic/apyrimidinic site [Takeshita, M., Chang, C.N., Johnson, F., Will, S., & Grollman, A.P. (1987) J. Biol. Chem. 262, 10171-10179]. Exchangeable and nonexchangeable base and sugar protons, including those located at the abasic site, have been assigned in the complementary APF 9-mer duplex by recording and analyzing two-dimensional phase-sensitive NOESY data sets in H2O and D2O solution at low temperature (0 degrees C). These studies indicate that A5 inserts into the helix opposite the abasic site F14 and stacks with flanking G4.C15 and G6.C13 Watson-Crick base pairs. Base-sugar proton NOE connectivities were measured through G4-A5-G6 on the unmodified strand and between the base protons of C15 and the sugar protons of the 5'-flanking residue F14 on the modified strand. These studies establish that all glycosidic torsion angles are anti and that the helix is right-handed at and adjacent to the abasic site in the APF 9-mer duplex. Two of the 16 phosphodiester groups exhibit phosphorus resonances outside the normal spectral dispersion indicative of altered torsion angles at two of the phosphate groups in the backbone of the APF 9-mer duplex.     

Proton NMR and optical spectroscopic studies on the DNA triplex formed by d-A-(G-A)7-G and d-C-(T-C)7-T.

Triplex and duplex formation of two deoxyribohexadecamers d-A-(G-A)-G (a) and d-C-(T-C)-T (b) have been studied by UV, CD, fluorescence, and proton NMR spectroscopy. Optical studies of a and b at dilute concentrations (microM range) yielded results similar to those seen for polymers of the same sequence, indicating that these hexadecamers have properties similar to the polymers in regard to triplex formation. The CD spectra of concentrated NMR samples (mM range) are similar to those observed at optical concentrations at both low and high pH, making possible a correlation between CD and NMR studies. In NMR spectra, two imido NH-N hydrogen bonded resonance envelopes at 12.6 and 13.7 ppm indicate that only the duplex conformation is present at pH greater than 7.7. Four new NH-N hydrogen-bonded resonance envelopes at 12.7, 13.5, 14.2, and 14.9 ppm are observed under acidic conditions (pH 5.6) and the two original NH-N resonances gradually disappear as the pH is lowered. Assignment of these four peaks to Watson-Crick G.C. Hoogsteen T.A Watson-Crick A.T, and Hoogsteen C+.G hydrogen-bonded imidos, respectively, confirm the formation of triple-stranded DNA NMR results also show that triplex is more stable than duplex at the same salt condition and that triplex melts to single strands directly without going through a duplex intermediate. However, in the melting studies, a structural change within the triple-stranded complex is evident at temperatures significantly below the major helix-to-coil transition. These studies demonstrate the feasibility of using NMR spectroscopy and oligonucleotide model compounds a and b for the study of DNA triplex formation.