Two-dimensional proton nuclear magnetic resonance investigation of the synthetic deoxyribonucleic acid decamer d(ATATCGATAT)2

In this study two-dimensional NMR techniques (COSY and NOESY) have been used in conjunction with one-dimensional NMR results to complete the assignment of the proton NMR spectrum of the double-stranded DNA decamer, d(ATATCGATAT)2, and to obtain qualitative information about numerous interproton distances in this molecule and some limited information about conformational dynamics. COSY and NOESY measurements have been combined to systematically assign many of the resonances from the H1' and H2',2" sugar protons to specific nucleotides in the double helix. This method relies on the fact that sugar protons within a specific nucleotide are scalar coupled and that base protons (AH8, GH8, TH6, and CH6) in right-handed helices can interact simultaneously with their own H2',2" sugar protons and those of the adjacent (5'-3') nucleotide attached to its 5' side (i.e., XpA not ApX). A COSY experiment is used to identify sugar resonances within a residue whereas the NOESY experiment allows the neighboring sugar to be connected (linked). The CH5 and CH6 resonances in the spectrum can immediately be identified by the COSY experiment. The methyl protons of thymine residues exhibit strong through-space interbase interactions both with their own TH6 proton and with AH8 proton on the adjacent (5'-3') adenine residue. These interactions are used both to make assignments of the spectra and to establish that the thymine methyl groups are in close proximity to the AH8 protons of adjacent adenine residues [Feigon, J., Wright, J. M., Leupin, W., Denny, W. A., & Kearns, D. R. (1982) J. Am. Chem. Soc. 104, 5540].(ABSTRACT TRUNCATED AT 250 WORDS)     

One- and two-dimensional NMR studies on the conformation of DNA containing the oligo(dA)oligo(dT) tract.

The resonances of the imino protons and all of the non-exchangeable protons (except for H5'/H5') of d(CGCAAAAAAGCG)d(CGCTTTTTTGCG) have been assigned by means of one- and two-dimensional NMR spectroscopies. Qualitative analyses showed that the overall structure is of the B-form, but local conformational deviations exist. The NOEs between the imino protons of thymines and H2 of adenines suggest that the A-T base pairs are propeller-twisted to almost the same degree as in crystals. A remarkable chemical shift of H1' was observed for the residue located just before the oligo(dA)oligo(dT) tract, suggesting the presence of conformational discontinuity at the junctions between the oligo(dA)oligo(dT) tract and the other portions. Analyses of cross peaks in NOESY spectra between H2 of adenines and H1' of the 3'-neighbouring residues on the complementary strand revealed that the minor groove of the oligo(dA)oligo(dT) tract is narrow and compressed gradually, from 5' to 3', along the tract.     

Sequence-dependent recognition of DNA duplexes. Netropsin complexation to the AATT site of the d(G-G-A-A-T-T-C-C) duplex in aqueous solution

We have investigated intermolecular interactions and conformational features of the netropsin X d(G-G-A-A-T-T-C-C) complex by one- and two-dimensional NMR studies in aqueous solution. Netropsin removes the 2-fold symmetry of the d(G-G-A-A-T-T-C-C) duplex at the AATT binding site and to a lesser extent at adjacent dG X dC base pairs resulting in doubling of resonances for specific positions in the spectrum of the complex at 25 degrees C. We have assigned the amide, pyrrole, and CH2 protons of netropsin, and the base and sugar H1' protons of the nucleic acid from an analysis of the nuclear Overhauser effect (NOESY) and correlated (COSY) spectra of the complex at 25 degrees C. We observe intermolecular nuclear Overhauser effects (NOE) between all three amide and both pyrrole protons on the concave face of the antibiotic and the minor groove adenosine H2 proton of the two central A4 X T5 base pairs of the d(G1-G2-A3-A4-T5-T6-C7-C8) duplex. Weaker intermolecular NOEs are also observed between the pyrrole concave face protons and the sugar H1' protons of residues T5 and T6 in the AATT minor groove of the duplex. We also detect intermolecular NOEs between the guanidino CH2 protons at one end of netropsin and adenosine H2 proton of the two flanking A3 X T6 base pairs of the octanucleotide duplex. These studies establish a set of intermolecular contacts between the concave face of the antibiotic and the minor groove AATT segment of the d(G-G-A-A-T-T-C-C) duplex in solution. The magnitude of the NOEs require that there be no intervening water molecules sandwiched between the antibiotic and the DNA so that release of the minor groove spine of hydration is a prerequisite for netropsin complex formation.     

Study of the spatial structure of the duplex d(pTGTTTGGC) d(pCCAAAC)A in aqueous solution by methods of uni- and two-dimensional (1)H-NMR spectroscopy and organic molecular mechanics

Structure of the complementary complex d(pTGTTTGGC) d(pCCAAAC)A in the aqueous solution has been investigated by one- and two-dimensional 1H NMR spectroscopy. The resonances of nonexchangeable protons of bases as well as methyl and deoxyribose 1', 2'a, 2'b, 3' and 4' protons have been assigned by means of two-dimensional J-correlated spectroscopy (COSY) and two-dimensional nuclear Overhauser enhancement spectroscopy (NOESY). Using one-dimensional NOE measurements, 62 interproton distances (intranucleotide: (H6/H8)i--(H1')t, (H6/H8)i--(H2'a)i, (H1')i--(H2'a)i, (H1')i--(H2'b)i; internucleotide: (H6/H8)i--(H1')i-1, (H6/H8)i--(H2'a)i-1, (H6/H8)i--(H2'b)i-1, (H5/CH3)i--(H6/H8)i-1, (H5/CH3)i--(H2'a/H2'b)i-1) have been determined for nearest-neighbour protons. Spin-coupling constant values for some sugar protons have been obtained from COSY spectra. The restrained molecular mechanics calculations have yielded the possible solution structures of duplex fitting the experimental set of interproton distances and coupling constants.     

Minor groove hydration of DNA in aqueous solution: sequence-dependent next neighbor effect of the hydration lifetimes in d(TTAA)2 segments measured by NMR spectroscopy.

The hydration in the minor groove of double stranded DNA fragments containing the sequences 5'-dTTAAT, 5'-dTTAAC, 5'-dTTAAA and 5'-dTTAAG was investigated by studying the decanucleotide duplex d(GCATTAATGC)2 and the singly cross-linked decameric duplexes 5'-d(GCATTAACGC)-3'-linker-5'-d(GCGTTAATGC)-3' and 5'-d(GCCTTAAAGC)-3'-linker-5'-d(GCTTTAAGGC)-3' by NMR spectroscopy. The linker employed consisted of six ethyleneglycol units. The hydration water was detected by NOEs between water and DNA protons in NOESY and ROESY spectra. NOE-NOESY and ROE-NOESY experiments were used to filter out intense exchange cross-peaks and to observe water-DNA NOEs with sugar 1' protons. Positive NOESY cross-peaks corresponding to residence times longer than approximately 0.5 ns were observed for 2H resonances of the central adenine residues in the duplex containing the sequences 5'-dTTAAT and 5'-dTTAAC, but not in the duplex containing the sequences 5'-dTTAAA and 5'-dTTAAG. In all nucleotide sequences studied here, the hydration water in the minor groove is significantly more mobile at both ends of the AT-rich inner segments, as indicated by very weak or negative water-A 2H NOESY cross-peaks. No positive NOESY cross-peaks were detected with the G 1'H and C 1'H resonances, indicating that the minor groove hydration water near GC base pairs is kinetically less restrained than for AT-rich DNA segments. Kinetically stabilized minor groove hydration water was manifested by positive NOESY cross-peaks with both A 2H and 1'H signals of the 5'-dTTAA segment in d(GCATTAATGC)2. More rigid hydration water was detected near T4 in d(GCATTAATGC)2 as compared with 5'-d(GCATTAACGC)-3'-linker-5'-d(GCGTTAATGC)-3', although the sequences differ only in a single base pair. This illustrates the high sensitivity of water-DNA NOEs towards small conformational differences.     

Proton NMR studies on the covalently linked RNA-DNA hybrid r(GCG)d(TATACGC). Assignment of proton resonances by application of the nuclear Overhauser effect.

Proton NMR spectra of a covalently linked self-complementary RNA X DNA hybrid, r(GCG)-d(TATACGC), are recorded in H2O and D2O. Imino proton resonances as well as the non-exchangeable base and H-1' resonances are unambiguously assigned by means of nuclear. Overhauser effect measurements. Additional information was obtained by 31P NMR and circular dichroism spectra. The RNA parts in the duplex attain full conformational purity and adopt the usual A-RNA conformation. The DNA residues opposite the RNA tract do not adopt an A-type structure completely. Their respective sugar rings still appear to possess a certain conformational freedom. The same holds true for the central d(-TATA-) sequence which forms a DNA X DNA duplex. There appears to be a structural break in this part: the first two residues, T(4) and A(5), are clearly influenced by the adjacent RNA structure, whereas residues T(6) and A(7) behave quite similar to what usually is found in DNA duplexes in aqueous solution.     

Proton NMR study and conformational analysis of d(CGT), d(TCG) and d(CGTCG) in aqueous solution. The effect of a dangling thymidine and of a thymidine mismatch on DNA mini-duplexes

Proton NMR studies of d(CGT), d(TCG) and d(CGTCG) were carried out at 300 and 500 MHz. The temperature and concentration dependence of the chemical shifts of various resonances indicates duplex formation only in the cases of d(TCG) and d(CGTCG). It is concluded that d(TCG) forms a mini-duplex stabilized by a 5'-dangling thymine base. Thermodynamic parameters of the duplex-to-coil equilibrium of the d(TCG) duplex are: delta H0 = -22.3 kcal/mol and delta S0 = -70 cal/mol. K, which correspond to approximately 40% duplex formation at 0 degrees C in a 2 mM nucleotide solution. Comparison of these data with thermodynamic parameters given earlier [Borer, P.N., Dengler, B., Tinoco, I. and Uhlenbeck, O.C. (1974) J. Mol. Biol. 86, 843-853] leads to the conclusion that the dangling base stabilization observed here is approximately equivalent to the stabilization caused by one or two additional A . T base pairs. The chemical shift behaviour of various resonances in d(CGTCG) indicates duplex formation without looping out of the thymine bases. The T X T mismatch does not seem to disturb the helical structure to a large extent. Analysis of the vicinal proton-proton coupling constants of the three compounds yielded geometrical data for the sugar rings. The data are interpreted in terms of N and S pseudorotational ranges. It is shown that a distinct conformation-transmission effect is exerted by the guanosine residues in a 5'----3' direction.     

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.     

Sequential resonance assignments in 1H NMR spectra of oligonucleotides by two-dimensional NMR spectroscopy

A sequential assignment procedure is outlined, based on two-dimensional NOE ( NOESY ) and two-dimensional J-correlated spectroscopy ( COSY ), for assigning the nonexchangeable proton resonances in NMR spectra of oligonucleotides. As presented here the method is generally applicable to right-handed helical oligonucleotides of intermediate size. We applied it to a lac operator DNA fragment consisting of d( TGAGCGG ) and d( CCGCTCA ) and obtained complete assignments for the adenine H8, guanine H8, cytosine H6 and H5, thymine H6 and 5-methyl, and the deoxyribose H1', H2', H2", H3', and H4' resonances, as well as some H5', H5" (pairwise) assignments. These assignments are required for the analysis of two-dimensional NOE and J-coupling data in terms of the solution structure of oligonucleotides.     

High-resolution NMR study of a synthetic DNA-RNA hybrid dodecamer containing the consensus pribnow promoter sequence: d(CGTTATAATGCG).r(CGCAUUAUAACG)

The nonsymmetrical double-helical hybrid dodecamer d(CGTTATAATGCG).r(CGCAUUAUAACG) was synthesized with solid-phase phosphoramidite methods and studied by high-resolution 2D NMR. The imino protons were assigned by one-dimensional nuclear Overhauser methods. All the base protons and H1', H2', H2", H3', and H4' sugar protons of the DNA strand and the base protons, H1', H2', and most of the H3'-H4' protons of the RNA strand were assigned by 2D NMR techniques. The well-resolved spectra allowed a qualitative analysis of relative proton-proton distances in both strands of the dodecamer. The chemical shifts of the hybrid duplex were compared to those of the pure DNA double helix with the same sequence (Wemmer et al., 1984). The intrastrand and cross-strand NOEs from adenine H2 to H1' resonances of neighboring base pairs exhibited characteristic patterns that were very useful for checking the spectral assignments, and their highly nonsymmetric nature reveals that the conformations of the two strands are quite different. Detailed analysis of the NOESY and COSY spectra, as well as the chemical shift data, indicate that the RNA strand assumes a normal A-type conformation (C3'-endo) whereas the DNA strand is in the general S domain but not exactly in the normal C2'-endo conformation. The overall structure of this RNA-DNA duplex is different from that reported for hybrid duplexes in solution by other groups (Reid et al., 1983a; Gupta et al., 1985) and is closer to the C3'-endo-C2'-endo hybrid found in poly(dA).poly(dT) and poly(rU).poly(dA) in the fiber state (Arnott et al., 1983, 1986).     

Conformational microheterogeneity in a DNA double helix: structure of restriction endonuclease Bam H1 recognition site

Structural studies using 500 MHz 1H NMR spectroscopy on Bam H1 recognition site d(GGATCC)2 in solution at 19 degrees is reported. The resonances from the sugar ring and base protons have been assigned from the 2D-COSY and NOESY spectra. Analyses of the NOESY cross-peaks between the base protons H8/H6 and sugar protons H2'/H2", H3' reveal that the nucleotide units G2, A3 and C6 adopt (C3'-endo, chi = 200 degrees-220 degrees) conformation while G1, T4 and C5 exhibit (C2'-endo, chi = 240 degrees-260 degrees) conformation. NMR data clearly suggest that the two strands of d(GGATCC)2 are conformationally equivalent and there is a structural two-fold between the two A-T pairs. The above information and the NOESY data are used to generate a structural model of d(GGATCC)2. The important features are: (i) G1-G2 stack, the site of cleavage, shows an alternation in sugar pucker i.e. C2'-endo, C3'-endo as in a B-A junction, (ii) G2-A3 stack adopts a mini A-DNA, both the sugars being C3'-endo, (iii) A3-T4 stack, the site of two-fold, displays an A-B junction with alternation in sugar pucker as C3'-endo, C2'-endo, (iv) T4-C5 stack adopts a mini B-DNA both the sugars being C2'-endo and (v) C5-C6 stack exhibits a B-A junction with C2'-endo, C3'-endo sugar puckers. Thus, our studies demonstrate that conformational microheterogeneity with a structural two fold, is present in the Bam H1 recognition site.     

Conformational transitions in cytidine bulge-containing deoxytridecanucleotide duplexes: extra cytidine equilibrates between looped out (low temperature) and stacked (elevated temperature) conformations in solution

High-resolution homonuclear and heteronuclear two-dimensional NMR studies have been carried out on the self-complementary d(C-C-G-C-G-A-A-T-T-C-C-G-G) duplex (designated GCG 13-mer) in aqueous solution. This sequence contains an extra cytidine located between residues G3 and G4 on each strand of the duplex. The exchangeable and nonexchangeable proton resonances have been assigned from an analysis of two-dimensional nuclear Overhauser enhancement (NOESY) and correlated (COSY and relay COSY) spectra for the GCG 13-mer duplex in H2O and D2O solution. The extra cytidine at the bulge site (designated CX) results in more pronounced changes in the NOE distance connectivities for the G3-CX-G4 segment centered about the CX residue compared to the C9-C10 segment on the partner strand opposite the CX residue for the GCG 13-mer duplex at 25 degrees C. The cross-peak intensities in the short mixing time NOESY spectrum also establish that all glycosidic torsion angles including that of CX are anti in the GCG 13-mer duplex at 25 degrees C. The observed chemical shift changes for the CX base protons and the G3pCX phosphorus resonance with temperature between 0 and 40 degrees C demonstrate a temperature-dependent conformational equilibrium in the premelting transition region. The NOE and chemical shift parameters establish that the predominant conformation at low temperature (0 degree C) has the extra cytidine looped out of the helix with the flanking G3.C10 and G4.C9 base pairs stacked on each other. These results support conclusions based on earlier one-dimensional NMR studies of extra cytidine containing complementary duplexes in aqueous solution [Morden, K. M., Chu, Y. G., Martin, F. H., & Tinoco, I., Jr. (1983) Biochemistry 22, 5557-5563. Woodson, S. A., & Crothers, D. M. (1987) Biochemistry 26, 904-912]. By contrast, the chemical shift and NOE parameters demonstrate that the conformational equilibrium shifts toward a structure with a stacked extra cytidine on raising the temperature to 40 degrees C prior to the helix-coil melting transition. The most downfield shifted phosphorus resonance in the GCG 13-mer duplex has been assigned to the phosphate in the C2-G3 step, and this observation demonstrates that the perturbation in the phosphodiester backbone extends to regions removed from the (G3-CX-G4).(C9-C10) bulge site.     

NMR investigations of duplex stability of phosphorothioate and phosphorodithioate DNA analogues modified in both strands.

Duplex formation from the self-complementary 12mer d(CGCGAATTCGCG) (Dickerson dodecamer) in which all phosphodiester linkages were replaced by phosphorothioate or phosphorodithioate linkages was studied using variable-temperature 1H and 31P NMR spectroscopy. Melting temperatures of the dodecamer, measured spectrophotometrically, showed significant decrease upon sulfur substitution (Tm 49 degrees C for the phosphorothioate and 21 degrees C for the phosphorodithioate, compared with 68 degrees C for the unmodified oligomer, in 1 M salt). Hyperchromicity observed upon melting of the dithioate was surprisingly low. NOESY spectra of the monothioate showed a cross-peak pattern characteristic for a right-handed duplex. Imino proton resonances of the duplex, shown by the mono- and the dithioate, were similar to those of the parent compound. In spite of monophasic melting curves, temperature dependence of the imino proton resonances and phosphorus resonances of the phosphorodithioate indicated heterogeneity with respect to base-pairing, compatible with the presence of a hairpin loop. Relaxation times (T1) of the imino protons in the phosphorothioate, determined by the saturation recovery method, were considerably shorter than in the unmodified oligomer. Base-pair lifetimes in the unmodified Dickerson dodecamer, determined by catalyst-dependent changes in relaxation rates of imino protons, were in the range of 2-30 ms at 20 degrees C. Strongly reduced base-pair lifetimes were found in the phosphorothioate analogue.     

2D-NMR studies of the unnatural duplex alpha-d(TCTAAAC)-beta-d(AGATTTG).

The unnatural oligonucleotide alpha-d(TCTAAAC) was synthesized and was found more resistant towards endonucleases than its beta-analog. 2D-NMR experiments allowed the assignment of all non-exchangeable aromatic and sugar protons except for the overlapping 5' -5" resonances, as well as the exchangeable imino protons of the parallel hybrid duplex alpha-d (TCTAAAC)-beta-d(AGATTTG). NMR studies show that the strength of the association between the alpha-strand and the beta parallel strand is equivalent to that between their anti-parallel complementary beta-analogs beta-d(CAAATCT) and beta-d(AGATTTG). NOE data provide evidence that both duplexes form stable right-helical duplexes with an anti-conformation on the glycosyl linkages and a Watson-Crick pairing. NOESY and COSY spectra allowed us to determine that alpha and beta deoxyriboses adopt a 3' -exo conformation.     

1H NMR studies on the interaction between distamycin A and a symmetrical DNA dodecamer

High-resolution NMR techniques have been used to examine the structural and dynamical features of the interaction between distamycin A and the self-complementary DNA dodecamer duplex d-(CGCGAATTCGCG)2. The proton resonances of d(CGCGAATTCGCG)2 have been completely assigned by previous two-dimensional NMR studies [Hare, D. R., Wemmer, D. E., Chou, S. H., Drobny, G., & Reid, B. R. (1983) J. Mol. Biol. 171, 319-336]. Addition of the asymmetric drug molecule to the symmetric dodecamer leads to the formation of an asymmetric complex as evidenced by a doubling of DNA resonances over much of the spectrum. In two-dimensional exchange experiments, strong cross-peaks were observed between uncomplexed DNA and drug-bound DNA resonances, permitting direct assignment of many drug-bound DNA resonances from previously assigned free DNA resonances. Weaker exchange cross-peaks between formerly symmetry related DNA resonances indicate that the drug molecule flips head-to-tail on one duplex with half the frequency at which it leaves the DNA molecule completely. In experiments performed in H2O, nuclear Overhauser effects (NOEs) were observed from each drug amide proton to an adenine C2H and a pyrrole H3 ring proton. In two-dimensional nuclear Overhauser experiments performed on D2O solutions, strong intermolecular NOEs were observed between each of the three pyrrole H3 resonances of the drug and an adenine C2H resonance, with weaker NOEs observed between the drug H3 resonances and C1'H resonances. The combined NOE data allow us to position the distamycin A unambiguously on the DNA dodecamer, with the drug spanning the central AATT segment in the minor groove.     

Extra thymidine stacks into the d(CTGGTGCGG).d(CCGCCCAG) duplex. An NMR and model-building study.

NMR and model-building studies were carried out on the duplex d(CTGGTGCGG).d(CCGCCCAG), referred to as (9+8)-mer, which contains an unpaired thymidine residue. Resonances of the base and of several sugar protons of the (9+8)-mer were assigned by means of a NOESY experiment. Interresidue NOEs between dG(4) and dT(5) as well as between dT(5) and dG(6) provided evidence that the extra dT is stacked into the duplex. Thermodynamic analysis of the chemical shift vs temperature profiles yielded an average TmD value of 334 K and delta HD of -289 kJmol-1 for the duplex in equilibrium random-coil transition. The shapes of the shift profiles as well as the thermodynamic parameters obtained for the extra dT residue and its neighbours again indicate that the unpaired dT base is incorporated inside an otherwise intact duplex. This conclusion is further supported by (a) the observation of an imino-proton resonance of the unpaired dT; (b) the relatively small dispersion in 31P chemical shifts (approximately 0.5 ppm) for the (9+8)-mer, which indicates the absence of t/g or g/t combinations for the phosphate diester torsion angles alpha/zeta. An energy-minimized model of the (9+8)-mer, which fits the present collection of experimental data, is presented.     

Two-dimensional 1H and 31P NMR spectra of a decamer oligodeoxyribonucleotide duplex and a quinoxaline ((MeCys3, MeCys7]TANDEM) drug duplex complex

Assignment of the 1H and 31P NMR spectra of a decamer oligodeoxyribonucleotide duplex, d(CCCGATCGGG), and its quinoxaline ((MeCys3, MeCys7]TANDEM) drug duplex complex has been made by two-dimensional 1H-1H and heteronuclear 31P-1H correlated spectroscopy. The 31P chemical shifts of this 10 base pair oligonucleotide follow the general observation that the more internal the phosphate is located within the oligonucleotide sequence, the more upfield the 31P resonance occurs. While the 31P chemical shifts show sequence-specific variations, they also do not generally follow the Calladine "rules" previously demonstrated. 31P NMR also provides a convenient monitor of the phosphate ester backbone conformational changes upon binding of the drug to the duplex. Although the quinoxaline drug, [MeCys3, MeCys7]TANDEM, is generally expected to bind to duplex DNA by bis-intercalation, only small 31P chemical shift changes are observed upon binding the drug to duplex d(CCCGATCGGG). Additionally, only small perturbations in the 1H NMR and UV spectra are observed upon binding the drug to the decamer, although association of the drug stabilizes the duplex form relative to the other states. These results are consistent with a non-intercalative mode of association of the drug. Modeling and molecular mechanics energy minimization demonstrate that a novel structure in which the two quinoxaline rings of the drug binds in the minor groove of the duplex is possible.     

Study of the structure of the duplex (Phn-NH(CH2)2NH)pd(CCAAACA) .pd(TGTTTGGC) with covalently bound 10-(2-hydroxyethyl)phenazine in an aqueous solution by 2D-1H-NMR spectroscopy]

The spatial structure of duplex (Phn-NH(CH2)2NH)pd(CCAAACA).pd(TGTTTGGC) having a N-(2-oxyethyl)-phenazinium residue covalently linked with the 5'-terminal phosphate of the heptanucleotide was studied by means of one- and two-dimensional 1H-NMR spectroscopy. The resonances of phenazinium protons, ethylenediamine linker protons, as well as, oligonucleotide H5/H6/H8/CH3 base protons and H1',H2'a, H2'b, H3', H4' deoxyribose protons have been assigned by means of 1H-COSY, 1H-NOESY and 1H-13C-COSY. The presence of the phenazine residue in duplex causes an additional imino proton signal of the terminal (G-7).(C-1) base pair, suggesting a higher stability of the duplex (Phn-NH(CH2)2NH)pd(CCAAACA).pd(TGTTTGGC) as compared to the unmodified duplex pd(CCAAACA).pd(TGTTTGGC). Analysis of NOE interactions between protons of the dye and the oligonucleotides show the phenazinium polycyclic system to intercalate between G-7 and C-8 residues of the octanucleotide.     

Influence of N6-methylation of residue A(5) on the conformational behaviour of d(C-C-G-A-A-T-T-C-G-G) in solution studied by 1H-NMR spectroscopy. 2. The hairpin form

The solution conformations of the oligonucleotides d(C-C-G-A-A-T-T-C-G-G) and d(C-C-G-A-m6A-T-T-C-G-G) as a function of temperature and sample concentration were investigated by means of 1H-NMR spectroscopy. The NMR spectra revealed that, at certain combinations of temperature and low sample and salt concentration, both compounds exist as a B-DNA-type duplex slowly (on the 1H-NMR time scale) interconverting with a monomeric species. From chemical shift data and imino-proton spectra, it is concluded that the monomeric species consists of a mixture of a hairpin form in rapid equilibrium with the random-coil form. The double-helical stem of the hairpin is formed by the six terminal cytidine and guanine residues, whereas the four core residues, -A-(m6)A-T-T-, partake in the loop. Thermodynamic analysis of the chemical shift of the resonances of the monomeric species vs temperature profiles of the two decamers and mutual comparison of these profiles indicate the following: the influence of N6-methylation of residue A(5) upon the local structure of the hairpin must be small; methylation decreases the stability of the duplex relative to the monomeric species: the temperature at which the fraction duplex equals 0.5 was found to be 312 K for the parent compound and 305 K for the methylated decamer at 2 mM sample concentration; methylation does not significantly alter the stability of the hairpin form relative to the random coil form: the Tm of the hairp----n equilibrium random-coil equilibrium is 308 K for the parent compound and 306 K for the methylated decamer. A higher fraction hairpin-like structure for the N6-methylated compound is observed under identical conditions of temperature and sample concentration: at 300 K, 2 mM sample concentration, the fraction hairpin form is 0.12 for d(C-C-G-A-A-T-T-C-G-G) and 0.20 for d(C-C-G-A-m6A-T-T-C-G-G). This finding appears to be a consequence of the reduced stability of the methylated dimeric species relative to the monomeric species, and to depend upon the sodium-ion concentration: it becomes more pronounced under low-salt conditions.     

DNA structure in which an adenine-cytosine mismatch pair forms an integral part of the double helix

Extensive studies using one- and two-dimensional 1H NMR at 500 MHz revealed that the oligonucleotide d(CGCCGCAGC) in solution at 5 degrees C forms a double helix under conditions of high salt (500 mM in NaCl, 1 mM sodium phosphate), low pH (pH 4.5), and high DNA concentration (4 mM in duplex). The presence of very strong nuclear Overhauser effects (NOEs) from base H8/H6 to sugar H2',H2" and the absence of NOE from base H8/H6 to sugar H3' suggested that the oligomer under these solution conditions forms a right-handed B-DNA double helix. The following lines of experimental evidence were used to conclude that C4 and A7 form an integral part of the duplex: (i) the presence of a NOESY cross-peak involving H8 of A7 and H8 of G8, (ii) the presence of a two-dimensional NOE (NOESY) cross-peak between H6 of C3 and H6 of C4, (iii) base protons belonging to C4 and A7 forming a part of the H8/H6---H1' cross-connectivity route, and (iv) the pattern of H8/H6---H2',H2" NOESY cross-connectivity based upon a B-DNA model requiring that both C4 and A7 form an integral part of the duplex. The possibility of an A-C pair involving H bonds was also examined. Two possible structural models of the duplex at pH 4.5 are proposed: in one model A-C pairing involves two H bonds, and in the other A-C pairing involves a single H bond.