Structure of the anthramycin-d(ATGCAT)2 adduct from one- and two-dimensional proton NMR experiments in solution

One- and two-dimensional 400-MHz proton NMR experiments are used to examine the solution structure of the covalent adduct formed by the interaction of anthramycin methyl ether with the self-complementary deoxyoligonucleotide d(ATGCAT)2. The concentration dependence of chemical shifts and nuclear Overhauser enhancement (NOE) experiments are utilized to assign the adenine H2 protons within the minor groove for both free d(ATGCAT)2 and the adduct. These studies demonstrate that one of the four adenine H2 protons is in close proximity to the bound anthramycin and this results in its upfield shift of 0.3 ppm compared to the adenine H2 protons of the free duplex. Effects of the covalent attachment of anthramycin to the d(ATGCAT)2 duplex result in an increased shielding of selected deoxyribose protons located within the minor groove of the adduct, as demonstrated by two-dimensional autocorrelated (COSY) NMR techniques. Interactions between the protons of the covalently attached anthramycin and the d(ATGCAT)2 duplex are determined by utilizing two-dimensional NOE (NOESY) techniques. Analysis of these data reveals NOE cross-peaks between the anthramycin methyl, H6, and H7 protons with specific deoxyoligonucleotide protons within the minor groove, thus allowing the orientation of the drug within the minor groove to be determined. Nonselective inversion recovery (T1) relaxation experiments are used to probe the structural and dynamic properties of the anthramycin-d(ATGCAT)2 adduct. These data suggest that the binding of anthramycin alters the correlation time of the d(ATGCAT)2 duplex and stabilizes both of the internal A X T base pairs with respect to solvent exchange.(ABSTRACT TRUNCATED AT 250 WORDS)     

Intercalation of aflatoxin B1 in two oligodeoxynucleotide adducts: comparative 1H NMR analysis of d(ATCAFBGAT).d(ATCGAT) and d(ATAFBGCAT)2

8,9-Dihydro-8-(N7-guanyl-[d(ATCGAT)])-9-hydroxyaflatoxin B1.d(ATCGAT) and 8,9-dihydro-8-(N7-guanyl-[d(ATGCAT)])-9-hydroxyaflatoxin B1.8,9-dihydro-8-(N7-guanyl-[d(ATGCAT)])-9-hydroxyaflatoxin B1 were prepared by direct addition of afltoxin B1 8,9-epoxide to d(ATCGAT)2 and d(ATGCAT)2, respectively. In contrast to reaction of aflatoxin B1 8,9-epoxide with d(ATCGAT)2 which exhibits a limiting stoichiometry of 1:1 aflatoxin B1:d(ATCGAT)2 [Gopalakrishnan, S., Stone, M. P., & Harris, T. M. (1989) J. Am. Chem. Soc. 111, 7232-7239], reaction of aflatoxin B1 8,9-epoxide with d(ATGCAT)2 exhibits a limiting stoichiometry of 2:1 aflatoxin B1:d(ATGCAT)2. 1H NOE experiments, nonselective 1H T1 relaxation measurements, and 1H chemical shift perturbations demonstrate that in both modified oligodeoxynucleotides the aflatoxin moiety is intercalated above the 5'-face of the modified guanine. The oligodeoxynucleotides remain right-handed, and perturbation of the B-DNA structure is localized adjacent to the adducted guanine. Aflatoxin-oligodeoxynucleotide 1H NOEs are observed between aflatoxin and the 5'-neighbor base pair and include both the major groove and the minor groove. The aflatoxin methoxy and cyclopentenone ring protons face into the minor groove; the furofuran ring protons face into the major groove. No NOE is observed between the imino proton of the modified base pair and the imino proton of the 5'-neighbor base pair; sequential NOEs between nucleotide base and deoxyribose protons are interrupted in both oligodeoxynucleotide strands on the 5'-side of the modified guanine. The protons at C8 and C9 of the aflatoxin terminal furan ring exhibit slower spin-lattice relaxation as compared to other oligodeoxynucleotide protons, which supports the conclusion that they face into the major groove. Increased shielding is observed for aflatoxin protons; chemical shift perturbations of the oligodeoxynucleotide protons are confined to the immediate vicinity of the adducted base pair. The imidazole proton of the modified guanine exchanges with water and is observed at 9.75 ppm. The difference in reaction stoichiometry is consistent with an intercalated transition-state complex between aflatoxin B1 8,9-epoxide and B-DNA. Insertion of aflatoxin B1-8,9 epoxide above the 5'-face of guanine in d(ATCGAT)2 would prevent the binding of a second molecule of aflatoxin B1 8,9-epoxide. In contrast, two intercalation sites would be available with d(ATGCAT)2.(ABSTRACT TRUNCATED AT 400 WORDS)     

The conformation of the d(ACCCGGGT) duplex in aqueous solution

The nonexchangeable base and sugar protons of the octanucleotide d(ACCCGGGT)2 have been assigned using two dimensional homonuclear Hartmann-Hahn relayed spectroscopy (HOHAHA), double quantum filtered homonuclear correlation spectroscopy (DQFCOSY) and nuclear Overhauser spectroscopy (NOESY) in D2O at 12 degrees C. The observed NOE's between the base protons and their own H2' protons and between the base protons and the H2' protons of the 5' adjacent nucleotide and the observed coupling constants between the deoxyribose 1' and 2',2' protons indicate that this duplex assumes a right-handed B-type helix conformation in solution.     

Carcinogen-nucleic acid interactions: equilibrium binding studies of aflatoxin B1 with the oligodeoxynucleotide d(ATGCAT)2 and with plasmid pBR322 support intercalative association with the B-DNA helix

Equilibrium binding of aflatoxin B1 (AFB1) to the oligodeoxynucleotide d(ATGCAT)2 was examined by using 1H NMR. AFB1 binds to double-stranded d(ATGCAT)2 with an apparent binding constant of 3.7 x 10(3) M-1. The equilibrium is rapid on the NMR time scale; the observed 1H NMR spectrum represents the population-weighted average of the chemical shifts arising from the free and bound states of the oligodeoxynucleotide and the AFB1. The spectrum of d(ATGCAT)2 exhibits exchange broadening in the presence of AFB1, manifested as decreases in apparent T2 relaxation times for the d(ATGCAT)2 base protons. Upon binding to d(ATGCAT)2, the AFB1 signals are shifted upfield, indicative of increased shielding. The adenine H2 protons are also shifted upfield in the presence of the carcinogen. Small changes in chemical shift are observed for other d(ATGCAT)2 protons. A substantial decrease in the nonselective T1 relaxation time is observed for the adenine H2 protons in the presence of AFB1. Competition binding experiments in which the competing ligands actinomycin D, ethidium bromide, and spermidine were individually added to an AFB1-d(ATGCAT)2 equilibrium mixture showed that addition of 1 equiv of actinomycin D or 4 equiv of ethidium bromide was sufficient to displace bound AFB1 from d(ATGCAT)2. In contrast, the addition of spermidine did not result in the displacement of bound AFB1 molecules and may have slightly enhanced binding, presumably due to stabilization of the DNA duplex. 1H NOESY experiments confirmed that the overall conformation for the d(ATGCAT)2 duplex was right-handed both in the absence and in the presence of AFB1. Equilibrium binding of AFB1 to d(ATGCAT)2 is greatly diminished at higher temperatures at which the oligodeoxynucleotide is single-stranded.(ABSTRACT TRUNCATED AT 250 WORDS)     

Sequence-dependent conformations of DNA duplexes: the TATA segment of the d(G-G-T-A-T-A-C-C) duplex in aqueous solution

The base and sugar protons of the d(G-G-T-A-T-A-C-C) duplex have been assigned from two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) measurements in D₂O solution at 25°C. The nucleic acid protons have been assigned from NOEs between protons on adjacent bases on the same and partner strands, as well as from NOEs between the base protons and their own and 5′-flanking H1′, H2′, H2″, H3′, and H4′ sugar protons. These assignments are confirmed from coupling constant and NOE connectivities within the sugar protons of a given residue. Several of these NOEs exhibit directionality and demonstrate that the d(G-G-T-A-T-A-C-C) duplex is a right-handed helix. The relative magnitude of the NOEs between the base protons and the sugar H2′ protons of its own and 5′-flanking sugar demonstrate that the TATA segment of the d(G-G-T-A-T-A-C-C) duplex adopts a B-DNA type helix geometry in solution, in contrast to the previous observation of a A-type helix for the same octanucleotide duplex in the crystalline state.     

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.     

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)     

Solution structure of a trans-opened (10S)-dA adduct of (+)-(7S,8R,9S,10R)-7,8-dihydroxy-9,10-epoxy-7,8,9,10-tetrahydrobenzo[a]pyrene in a fully complementary DNA duplex: evidence for a major syn conformation

Two-dimensional NMR was used to determine the solution structure of an undecanucleotide duplex, d(CGGTCACGAGG).d(CCTCGTGACCG), in which (+)-(7S,8R,9S,10R)-7,8-dihydroxy-9,10-epoxy-7,8,9,10-tetrahydrobenzo[a]pyrene is covalently bonded to the exocyclic N(6)() amino group of the central deoxyadenosine, dA(6), through trans addition at C10 of the epoxide (to give a 10S adduct). The present study represents the first NMR structure of a benzo[a]pyrene (10S)-dA adduct in DNA with a complementary T opposite the modified dA. Exchangeable and nonexchangeable protons of the modified duplex were assigned by the use of TOCSY (in D(2)O) and NOESY spectra (in H(2)O and D(2)O). Sequential NOEs expected for a B-type DNA conformation with typical Watson-Crick base pairing are observed along the duplex, except at the lesion site. We observed a strong intraresidue NOE cross-peak between H1' and H8 of the modified dA(6). The sugar H2' and H2' ' of dC(5) lacked NOE cross-peaks with H8 of dA(6) but showed weak interactions with H2 of dA(6) instead. In addition, the chemical shift of the H8 proton (7.51 ppm) of dA(6) appears at a higher field than that of H2 (8.48 ppm). These NOE and chemical shift data for the dA(6) base protons are typical of a syn glycosidic bond at the modified base. Restrained molecular dynamics/energy minimization calculations show that the hydrocarbon is intercalated from the major groove on the 3'-side of the modified base between base pairs A(6)-T(17) and C(7)-G(16) and confirm the syn glycosidic angle (58 degrees ) of the modified dA(6). In the syn structure, a weak A-T hydrogen bond is possible between the N3-H proton of T(17) and N7 of dA(6) (at a distance of 3.11 A), whereas N1, the usual hydrogen bonding partner for N3-H of T when dA is in the anti conformation, is 6.31 A away from this proton. The 10(S)-dA modified DNA duplex remains in a right-handed helix, which bends in the direction of the aliphatic ring of BaP at about 42 degrees from the helical axis. ROESY experiments provided evidence for interconversion between the major, syn conformer and a minor, possibly anti, conformer.     

NMR structure of a parallel-stranded DNA duplex at atomic resolution

DNA dodecamers have been designed with two cytosines on each end and intervening A and T stretches, such that the oligomers have fully complementary A:T base pairs when aligned in the parallel orientation. Spectroscopic (UV, CD and IR), NMR and molecular dynamics studies have shown that oligomers having the sequences d(CCATAATTTACC) and d(CCTATTAAATCC) form a parallel-stranded duplex when dissolved at 1:1 stoichiometry in aqueous solution. This is due to the C:C⁺ clamps on either end and extensive mismatches in the antiparallel orientation. The structure is stable at neutral and acidic pH. At higher temperatures, the duplex melts into single strands in a highly cooperative fashion. All adenine, cytosine and thymine nucleotides adopt the anti conformation with respect to the glycosidic bond. The A:T base pairs form reverse Watson–Crick base pairs. The duplex shows base stacking and NOEs between the base protons T(H6)/A(H8) and the sugar protons (H1′/H2′/H2″) of the preceding nucleotide, as has been observed in antiparallel duplexes. However, no NOEs are observed between base protons H2/H6/H8 of sequential nucleotides, though such NOEs are observed between T(CH₃) and A(H8). A three-dimensional structure of the parallel-stranded duplex at atomic resolution has been obtained using molecular dynamics simulations under NMR constraints. The simulated structures have torsional angles very similar to those found in B-DNA duplexes, but the base stacking and helicoid parameters are significantly different.     

Sequence-dependent conformation of DNA duplexes. The AATT segment of the d(G-G-A-A-T-T-C-C) duplex in aqueous solution

The nonexchangeable base and sugar protons of the octanucleotide d(G-G-A-A-T-T-C-C) have been assigned by two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) methods in aqueous solution. The assignments are based on distance connectivities of less than 4.5 A established from NOE effects between base and sugar protons on the same strand and occasionally between strands, as well as, coupling connectivities within the protons on each sugar ring. We observe the NOEs to exhibit directionality and are consistent with the d(G-G-A-A-T-T-C-C) duplex adopting a right-handed helix in solution. The relative magnitude of the NOEs between base and sugar H2' protons of the same and 5'-adjacent sugars characterizes the AATT segment to the B-helix type in solution.     

NMR investigation of mithramycin A binding to d(ATGCAT)2: a comparative study with chromomycin A3

The binding of mithramycin A to the d(A1T2G3C4A5T6) duplex was investigated by 1H NMR and found to be similar to that of its analogue chromomycin A3. In the presence of Mg2+, mithramycin binds strongly to d(ATGCAT)2. On the basis of the two-dimensional NOESY spectrum, the complex formed possesses C2 symmetry at a stoichiometry of two drugs per duplex (2:1) and is in slow chemical exchange on the NMR time scale. NOESY experiments reveal contacts from the E-pyranose of mithramycin to the terminal and nonterminal adenine H2 proton of DNA and from the drug hydroxyl proton to both G3NH2 protons, C4H1' proton, and A5H1' proton. These data place the drug chromophore and E pyranose on the minor groove side of d(ATGCAT)2. NOE contacts from the A-, B-, C-, and D-pyranoses of mithramycin to several deoxyribose protons suggest that the A- and B-rings are oriented along the sugar-phosphate backbone of G3-C4, while the C- and D-rings are located along the sugar-phosphate backbone of A5-T6. These drug-DNA contacts are very similar to those found for chromomycin binding to d(ATGCAT)2. Unlike chromomycin, the NOESY spectrum of mithramycin at the molar ratio of one drug per duplex reveals several chemical exchange cross-peaks corresponding to the drug-free and drug-bound proton resonances. From the intensity of these cross-peaks and the corresponding diagonal peaks, the off-rate constant was estimated to be 0.4 s-1. These data suggest that the exchange rate of mithramycin binding to d(ATGCAT)2 is faster than that of chromomycin.     

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).     

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.     

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.     

NMR and computational characterization of mitomycin cross-linked to adjacent deoxyguanosines in the minor groove of the d(T-A-C-G-T-A).d(T-A-C-G-T-A) duplex

Two-dimensional homonuclear and heteronuclear NMR and minimized potential energy calculations have been combined to define the structure of the antitumor agent mitomycin C (MC) cross-linked to deoxyguanosines on adjacent base pairs in the d(T1-A2-C3-G4-T5-A6).d(T7-A8-C9-G10-T11-A12) duplex. The majority of the mitomycin and nucleic acid protons in the MC-X 6-mer complex have been assigned from through-bond and through-space two-dimensional proton NMR studies in aqueous solution at 5 and 20 degrees C. The C3.G10 and G4.C9 base pairs are intact at the cross-link site and stack on each other in the complex. The amino protons of G4 and G10 resonate at 9.36 and 8.87 ppm and exhibit slow exchange with solvent H2O. The NMR experimental data establish that the mitomycin is cross-linked to the DNA through the amino groups of G4 and G10 and is positioned in the minor groove. The conformation of the cross-link site is defined by a set of NOEs between the mitomycin H1" and H2" protons and the nucleic acid imino and amino protons of G4 and the H2 proton of A8 and another set of NOEs between the mitomycin geminal H10" protons and the nucleic acid imino and amino protons of G10 and the H2 proton of A2. Several phosphorus resonances of the d(T-A-C-G-T-A) duplex shift dramatically on mitomycin cross-link formation and have been assigned from proton-detected phosphorus-proton two-dimensional correlation experiments. The proton chemical shifts and NOEs establish fraying at the ends of the d(T-A-C-G-T-A) duplex, and this feature is retained on mitomycin cross-link formation. The base-base and base-sugar NOEs exhibit similar patterns for symmetry-related steps on the two nucleic acid strands in the MC-X 6-mer complex, while the proton and phosphorus chemical shifts are dramatically perturbed at the G10-T11 step on cross-link formation. The NMR distance constraints have been included in minimized potential energy computations on the MC-X 6-mer complex. These computations were undertaken with the nonplanar five-membered ring of mitomycin in each of two pucker orientations. The resulting low-energy structures MX1 and MX2 have the mitomycin cross-linked in a widened minor groove with the chromophore ring system in the vicinity of the G10-T11 step on one of the two strands in the duplex.(ABSTRACT TRUNCATED AT 400 WORDS)     

NMR and computational characterization of the N-(deoxyguanosin-8-yl)aminofluorene adduct [(AF)G] opposite adenosine in DNA: (AF)G[syn].A[anti] pair formation and its pH dependence

This paper reports on a combined two-dimensional NMR and energy minimization computational characterization of the conformation of the N-(deoxyguanosyl-8-yl)aminofluorene adduct [(AF)G] positioned across adenosine in a DNA oligomer duplex as a function of pH in aqueous solution. This study was undertaken on the d[C1-C2-A3-T4-C5-(AF)G6-C7-T8-A9-C10-C11].[G12-G13-T14 -A15-G16-A17-G18- A19-T20-G21-G22] complementary undecamer [(AF)G 11-mer duplex]. The modification of the single G6 on the pyrimidine-rich strand was accomplished by reaction of the oligonucleotide with N-acetoxy-2-(acetylamino)fluorene and subsequent deacetylation under alkaline conditions. The HPLC-purified modified strand was annealed with the unmodified purine-rich strand to generate the (AF)G 11-mer duplex. The exchangeable and nonexchangeable protons are well resolved and narrow in the NMR spectra of the (AF)G 11-mer duplex so that the base and the majority of sugar nucleic acid protons, as well as several aminofluorene ring protons, have been assigned following analysis of two-dimensional NOESY and COSY data sets at pH 6.9, 30 degrees C in H2O and D2O solution. The NOE distance constraints establish that the glycosidic torsion angle is syn at (AF)G6 and anti at A17, which results in the aminofluorene ring being positioned in the minor groove. A very large downfield shift is detected at the H2' sugar proton of (AF)G6 associated with the (AF)G6[syn].A17[anti] alignment in the (AF)G 11-mer duplex. The NMR parameters demonstrate formation of Watson-Crick C5.G18 and C7.G16 base pairs on either side of the (AF)G6[syn].A17[anti] modification site with the imino proton of G18 more stable to exchange than the imino proton of G16. Several nonexchangeable aminofluorene protons undergo large downfield shifts as do the imino and H8 protons of G16 on lowering of the pH from neutrality to acidic values for the (AF)G 11-mer duplex. Both the neutral and acidic pH conformations have been defined by assigning the NOE constraints in the [C5-(AF)G6-C7].[G16-A17-G18] segment centered about the modification site and incorporating them in distance constrained minimized potential energy calculations in torsion angle space with the DUPLEX program. A series of NOEs between the aminofluorene protons and the DNA sugar protons in the neutral pH conformation establish that the aminofluorene ring spans the minor groove and is directed toward the G16-A17-G18 sugar-phosphate backbone on the partner strand.(ABSTRACT TRUNCATED AT 400 WORDS)     

Preparation and characterization of oligonucleotides containing S-[2-(N7-guanyl)ethyl]glutathione.

S-[2-(N7-Guanyl)ethyl]glutathione is the major adduct derived from modification of DNA with 1,2-dibromoethane in biological systems and is postulated to be a mutagenic lesion [Humphreys, W. G., Kim, D.-H., Cmarik, J. L., Shimada, T., & Guengerich, F. P. (1990) Biochemistry 29, 10342-10350]. Oligonucleotides containing this modified base were prepared by treatment of oligonucleotides with S-(2-chloroethyl)glutathione and purified by chromatography. The self-complementary oligonucleotide d(ATGCAT), when thus modified at the single guanine, appeared to associate with itself as judged by UV measurements, but CD and NMR measurements indicated a lack of hybridization, with a decrease in the melting temperature of greater than 10 degrees C. The same lack of self-association was noted when d(ATGCAT) was modified to contain an N-acetyl-S-[2-(N7-guanyl)ethyl]cysteine methyl ester moiety. The oligomer d-(C1A2T3G4C5C6T7) was modified to contain a single S-[2-(N7-guanyl)ethyl]glutathione moiety at the central position, and UV, CD, and 1H NMR studies indicated that this oligomer hybridized to its normal complement d(A8G9G10C11A12T13G14), although the binding was considerably weakened by adduction (imino proton NMR spectroscopy in the presence of H2O indicated that the hydrogen bond signals seen in the oligomer were all broadened upon modification). All proton resonances were identified using two-dimensional 1H NMR spectroscopy. Adduct formation affected the chemical shifts of the base and 1', 2', and 2" protons of T3 and C5, the 2" proton of C6, and the 8 and 1' protons of C11, while little effect was observed on other protons. No cross-peaks were detected between the glutathione and oligomer moieties in two-dimensional nuclear Overhauser enhanced NMR studies. These results suggest that a rather local structural perturbation occurs in the DNA oligomer upon modification and that the glutathione moiety appears to be relatively unperturbed by its placement in the duplex. When the cytosine in the normal d(AGGCATG) complement to d-(CATGCCT) was changed to each of the other three potential bases at the central position, no hybridization with the oligomer d(CATGCCT) containing S-[2-(N7-guanyl)ethyl]glutathione was detected. We conclude that these N7-guanyl derivatives destabilize hybridization and that bases other than cytosine do not appear to show preferential thermodynamic bonding to these adducts, at least in the sequences examined to date.(ABSTRACT TRUNCATED AT 400 WORDS)     

Solution structure of the covalent sterigmatocystin-DNA adduct.

Sterigmatocystin and aflatoxin are potent mutagens that contaminate foodstuffs stored under conditions that permit fungal growth. These food mycotoxins can be metabolically activated to their epoxides, which subsequently form covalent adducts with DNA and can eventually induce tumor development. We have generated the sterigmatocystin-d(A1-A2-T3-G4-C5-A6-T7-T8) covalent adduct (two sterigmatocystins per duplex) by reacting sterigmatocystin-1,2-epoxide with the self-complementary d(A-A-T-G-C-A-T-T) duplex and determined its solution structure by the combined application of two-dimensional NMR experiments and molecular dynamics calculations. The self-complementary duplex retains its 2-fold symmetry following covalent adduct formation of sterigmatocystin at the N7 position of G4 residues on each strand of the duplex. The H8 proton of [ST]G4 exchanges rapidly with water and resonates at 9.58 ppm due to the presence of the positive charge on the guanine ring following adduct formation. We have assigned the exchangeable and nonexchangeable proton resonances of sterigmatocystin and the duplex in the covalent adduct and identified the intermolecular proton-proton NOEs that define the orientation and mode of binding of the mutagen to duplex DNA. The analysis was aided by intermolecular NOEs between the sterigmatocystin protons with both the major groove and minor groove protons of the DNA. The molecular dynamics calculations were aided by 180 intramolecular nucleic acid constraints, 16 intramolecular sterigmatocystin constraints, and 56 intermolecular distance constraints between sterigmatocystin and the nucleic acid protons in the adduct. The sterigmatocystin chromophore intercalates between the [ST]G4.C5 and T3.A6 base pairs and stacks predominantly over the modified guanine ring in the adduct duplex. The overall conformation of the DNA remains right-handed on adduct formation with unwinding of the helix, as well as widening of the minor groove. Parallel NMR studies on the sterigmatocystin-d(A1-A2-A3-G4-C5-T6-T7-T8) covalent adduct (two sterigmatocystins per duplex) provide supportive evidence that the mutagen covalently adducts the N7 position of G4 and its chromophore intercalates to the 5' side of the guanine and stacks over it. The present NMR-molecular dynamics studies that define a detailed structure for the sterigmatocystin-DNA adduct support key structural conclusions proposed previously on the basis of a qualitative analysis of NMR parameters for the adduct formed by the related food mutagen aflatoxin B1 and DNA [Gopalakrishnan, S., Harris, T. M., & Stone, M. P. (1990) Biochemistry 29, 10438-10448].     

Dynamics and binding mode of Hoechst 33258 to d(GTGGAATTCCAC)2 in the 1:1 solution complex as determined by two-dimensional 1H NMR.

We have investigated the interaction of the bisbenzimidazole derivative Hoechst 33258 with the self-complementary dodecadeoxynucleotide duplex d(GTGGAATTCCAC)2 using one-dimensional (1D) and two-dimensional (2D) proton nuclear magnetic resonance (1H NMR) spectroscopy. To monitor the extent of complex formation, we used the imino proton region of the 1D 1H NMR spectra acquired in H2O solution. These spectra show that the DNA duplex loses its inherent C2v symmetry upon addition of the drug, indicating that the two molecules form a kinetically stable complex on the NMR time scale (the lifetime of the complex has been measured to be around 450 ms). We obtained sequence-specific assignments for all protons of the ligand and most protons of each separate strand of the oligonucleotide duplex using a variety of homonuclear 2D 1H NMR experiments. The aromatic protons of the DNA strands, which are symmetrically related in the free duplex, exhibit exchange cross peaks in the complex. This indicates that the drug binds in two equivalent sites on the 12-mer, with an exchange rate constant of 2.2 +/- 0.2 s-1. Twenty-five intermolecular NOEs were identified, all involving adenine 2 and sugar 1' protons of the DNA and protons in all four residues of the ligand, indicating that Hoechst 33258 is located in the minor groove at the AATT site. Only protons along the same edge of the two benzimidazole moieties of the drug show NOEs to DNA protons at the bottom of the minor groove. Using molecular mechanics, we have generated a unique model of the complex using distance constraints derived from the intermolecular NOEs. We present, however, evidence that the piperazine group may adopt at least two locally different conformations when the drug is bound to this dodecanucleotide.     

Solid-phase synthesis and high-resolution NMR studies of two synthetic double-helical RNA dodecamers: r(CGCGAAUUCGCG) and r(CGCGUAUACGCG)

Ten-micromole solid-phase RNA synthesis has been successfully performed on an automated nucleic acid synthesizer with coupling efficiencies up to 99%, using the tert-butyldimethylsilyl group to protect the 2'-hydroxyl. The tert-butyldimethylsilyl group was easily removed by tetrabutylammonium fluoride under conditions in which virtually no 2'- to 3'-isomerization was found to occur. By use of this approach, the self-complementary RNA dodecamers r(CGCGAAUUCGCG) and r(CGCGUAUACGCG) were synthesized on an automated nucleic acid synthesizer, purified by TLC, and studied by high-resolution NMR. Imino protons were assigned from one-dimensional nuclear Overhauser effects. The nonexchangeable base, H1', and H2' protons were assigned by the sequential NOESY connectivity method. The NOE data from these two oligomers were analyzed qualitatively and compared to the ideal A- and B-type helix models of Arnott et al. (1972a,b). The internucleotide H6/H8 NOEs to the preceding H1' in r(CGCGUAUACGCG) were found to be sequence-dependent and probably reflect the roll angles between adjacent bases. The internucleotide H6/H8 to H2' NOEs of these oligomers correspond very well to an A-type conformation, but the interstrand adenine H2 NOEs to the following H1' were much stronger than those predicted from the fiber model. These srong interstrand NOEs can be rationalized by base pair slide to favor more interstrand base overlap, as predicted by Callidine and Drew (1984).