Reassessment of structural characteristics of the d(CGCG)2:actinomycin D complex from complete 1H and 31P NMR

Complexes formed between Actinomycin D (ActD) and the tetranucleotides d(AGCT)2 and d(CGCG)2 were studied in detail by one and two-dimensional 1H and 31P NMR. The 31P two dimensional chemical exchange experiment, at room temperature on saturated complexes (1:1), showed unambiguously that the asymmetrical phenoxazone ring binds to the unique GC site under the two possible orientations in the d(AGCT)2 tetranucleotide but adopts a single orientation in the d(CGCG)2 tetranucleotide. For the d(CGCG)2:Act D saturated complex, complete assignments of all protons and phosphorus signals of the two-nucleotide strands, as well as of the two cyclic pentapeptide chains has allowed us to study in details the conformational features of the complex from NOE and coupling constants analysis. The tetranucleotide remains in a right-handed duplex, but the sugar puckers are modified for residues at the intercalation site. A uniform C2' endo pucker is observed for residues on the strand facing the quinoid side of the phenoxazone ring while a C2' endo-C3-endo equilibrium about 60% of C2' endo is proposed for the two residues on the strand facing the benzenoid side of the phenoxazone ring. In contrast to previous studies on ActD-DNA interactions, we have been able to measure the 3J phosphorus-proton coupling constants at the intercalation site but also adjacent to it, showing that 31P chemical shifts are not simply related to the backbone conformation. Molecular mechanics calculations, using empirical distances deduced from NOE effects as restrained distances during minimizations, led to a model differing mainly from those previously published by orientation of the N methyl groups of both N-Methyl-Valines.     

An NMR investigation of the binding of the anticancer drug actinomycin D to oligodeoxyribonucleotides with isolated 5'd(GC)3' binding sites

Imino proton and 31P NMR studies were conducted on the binding of actinomycin D (ActD) to self-complementary oligodeoxyribonucleotides with one GC binding site [d(ATATGCATAT) (1), d-(ATACGCGTAT) (2), and d(ATATACGCGTATAT) (3)] and with two GC sites [d(ATGCATGCAT) (4)]. At R = 1 (molar ratio of ActD to oligomer duplex) ActD caused a doubling of the number of imino proton signals at, and adjacent to, the GC binding site of 1. One of the G.C base pair signals shifted upfield while the other shifted downfield. Both of the signals for the A.T base pairs adjacent to the binding site shifted downfield. All imino proton signals of 2 and the longer sequence, 3, shifted upfield on binding of ActD to the GC site, indicating a sequence-dependent change in base stacking on complex formation. For both 1 and 2 addition of ActD resulted in a similar pattern of three downfield 31P NMR signals. The two most downfield signals have chemical shift and temperature dependence which are characteristic of phosphate groups at isolated intercalation sites. At R = 1 the ActD complex with 4 has very complex spectra with both upfield and downfield A.T and G.C imino signals. All these data were consistent with two 1:1 complexes with the unsymmetrical phenoxazone ring adopting both of the two possible orientations.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

1H and 31P NMR investigations of actinomycin D binding selectivity with oligodeoxyribonucleotides containing multiple adjacent d(GC) sites

Imino proton and 31P NMR studies were conducted on the binding of actinomycin D (ActD) to self-complementary oligodeoxyribonucleotides with adjacent 5'-GC-3' sites. ActD showed very high specificity for binding to GC sites regardless of oligomer length and surrounding sequence. For a first class of duplexes with a central GCGC sequence, a mixture of 1:1 complexes was observed due to the two different orientations of the ActD phenoxazone ring system. Analysis of 1H chemical shifts suggested that the favored 1:1 complex had the benzenoid side of the phenoxazone ring over the G base in the central base pair of the GCGC sequence. This is the first case in which an unsymmetrical intercalator has been shown to bind to DNA in both possible orientations. A unique 2:1 complex, with significantly different 1H and 31P chemical shifts relative to those of the 1:1 complexes, was formed with these same oligomers, again with the benzenoid side of the ActD molecule over the G base of the central GC base pair. There is considerable anticooperativity to binding of the second ActD in a GCGC sequence. In titrations of oligomers with the GCGC sequence, only the two 1:1 complexes are found up to ratios of one ActD per oligomer. Increasing the ActD concentration, however, resulted in stoichiometric formation of the unique 2:1 adduct. Spectrophotometric binding studies indicated that the apparent binding equilibrium constant for a GC site adjacent to a bound site is reduced by approximately a factor of 20 relative to the ActD binding constant to an isolated GC site.     

Deoxyribose ring conformation of [d(GGTATACC)]2: an analysis of vicinal proton-proton coupling constants from two-dimensional proton nuclear magnetic resonance

Exchangeable and nonexchangeable protons of [d(GGTATACC)]2 in aqueous cacodylate solution were assigned from two-dimensional nuclear Overhausser effect (2D NOE) spectra. With phase-sensitive COSY and double quantum filtered COSY (DQF-COSY) experiments, the cross-peaks resulting from deoxyribose ring conformation sensitive proton-proton vicinal couplings, i.e., all 1'-2', 1'-2", 2'-3', and 3'-4' couplings and six from 2"-3' couplings, were observed. From the cross-peak fine structure, the 2',2" proton assignments can be confirmed; coupling constants J1'2' and J1'2" and sums of coupling constants involving H2' and H2" for all residues and H3' for C8 were obtained. The DISCO procedure [Kessler, H., Muller, A., & Oschkinat, H. (1985) Magn. Reson. Chem. 23, 844-852] was used to extract individual 1'-2' and 1'-2" coupling constants. The sum of coupling constants involving H1' or H3' was measured from the one-dimensional spectrum where signal overlap is not a problem. Analysis of the resulting coupling constants and sums of coupling constants, in the manner of Rinkel and Altona [Rinkel, L. J., & Altona, C. (1987) J. Biomol. Struct. Dyn. 4, 621-649], led to the following conclusion: C2'-endo deoxyribose ring conformation is predominant for every residue, but a significant amount of C3'-endo conformation may exist, ranging from 14% to 30%.     

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.     

NMR studies of echinomycin bisintercalation complexes with d(A1-C2-G3-T4) and d(T1-C2-G3-A4) duplexes in aqueous solution: sequence-dependent formation of Hoogsteen A1.T4 and Watson--Crick T1.A4 base pairs flanking the bisintercalation site

We report on two-dimensional proton NMR studies of echinomycin complexes with the self-complementary d(A1-C2-G3-T4) and d(T1-C2-G3-A4) duplexes in aqueous solution. The exchangeable and nonexchangeable antibiotic and nucleic acid protons in the 1 echinomycin per tetranucleotide duplex complexes have been assigned from analyses of scalar coupling and distance connectivities in two-dimensional data sets recorded in H2O and D2O solution. An analysis of the intermolecular NOE patterns for both complexes combined with large upfield imino proton and large downfield phosphorus complexation chemical shift changes demonstrates that the two quinoxaline chromophores of echinomycin bisintercalate into the minor groove surrounding the dC-dG step of each tetranucleotide duplex. Further, the quinoxaline rings selectively stack between A1 and C2 bases in the d(ACGT) complex and between T1 and C2 bases in the d(TCGA) complex. The intermolecular NOE patterns and the base and sugar proton chemical shifts for residues C2 and G3 are virtually identical for the d(ACGT) and d(TCGA) complexes. A change in sugar pucker from the C2'-endo range to the C3'-endo range is detected at C2 on formation of the d(ACGT) and d(TCGA) complexes. In addition, the sugar ring protons of C2 exhibit upfield shifts and a large 1 ppm separation between the H2' and H2" protons for both complexes. The L-Ala amide protons undergo large downfield complexation shifts consistent with their participation in intermolecular hydrogen bonds for both tetranucleotide complexes.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

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)     

The Effect of Crystal Packing on Oligonucleotide Double Helix Structure

Abstract

Complexes formed between Actinomycin D (ActD) and the tetranucleotides d(AGCT)2 and d(CGCG)₂ were studied in detail by one and two-dimensional ¹H and ³¹P NMR. The ³¹P two dimensional chemical exchange experiment, at room temperature on saturated complexes (1:1), showed unambiguously that the asymmetrical phenoxazone ring binds to the unique GC site under the two possible orientations in the d(AGCT)₂ tetranucleotide but adopts a single orientation in the d(CGCG)₂ tetranucleotide. For the d(CGCG)₂: Act D saturated complex, complete assignments of all protons and phosphorus signals of the two-nucleotide strands, as well as of the two cyclic pentapeptide chains has allowed us to study in details the conformational features of the complex from NOE and coupling constants analysis. The tetranucleotide remains in a right-handed duplex, but the sugar puckers are modified for residues at the intercalation site. A uniform C_2′ endo pucker is observed for residues on the strand facing the quinoid side of the phenoxazone ring while a C_2′ endo-C_3′ endo equilibrium about 60% of C_2′ endo is proposed for the two residues on the strand facing the benzenoid side of the phenoxazone ring. In contrast to previous studies on ActD-DNA interactions, we have been able to measure the ³J phosphorus-proton coupling constants at the intercalation site but also adjacent to it, showing that ³¹P chemical shifts are not simply related to the backbone conformation. Molecular mechanics calculations, using empirical distances deduced from NOE effects as restrained distances during minimizations, led to a model differing mainly from those previously published by orientation of the N methyl groups of both N-Methyl-Valines.     

Intercalation of the (1R,2S,3R,4S)-N6-[1-(1,2,3,4-tetrahydro-2,3,4-trihydroxybenz[a]anthracenyl)]-2'-deoxyadenosyl adduct in the N-ras codon 61 sequence: DNA sequence effects

The structure of the bay region (1R,2S,3R,4S)-N6-[1-(1,2,3,4-tetrahydro-2,3,4-trihydroxybenz[a]anthracenyl)]-2'-deoxyadenosyl adduct at X(7) of 5'-d(CGGACAXGAAG)-3'.5'-d(CTTCTTGTCCG)-3', incorporating codons 60, 61 (underlined), and 62 of the human N-ras protooncogene, was determined by NMR. This was the bay region benz[a]anthracene RSRS (61,3) adduct. The BA moiety intercalated above the 5'-face of the modified base pair. NOE connectivities between imino protons were disrupted at T16 and T17. Large chemical shifts at the lesion site were consistent with ring current shielding arising from the BA moiety. A large chemical shift dispersion was observed for the BA aromatic protons. An increased rise of 8.17 A was observed between base pairs A6 x T17 and X7 x T(16). The PAH moiety stacked with the purine ring of A6, the 5'-neighbor nucleotide. This resulted in buckling of the 5'-neighbor A6 x T17 base pair, evidenced by exchange broadening for the T17 imino resonance. It also interrupted sequential NOE connectivities between nucleotides C5 and A6. The A6 deoxyribose ring showed an increased percentage of the C3'-endo conformation. This differed from the bay region BA RSRS (61,2) adduct, in which the lesion was located at position X6 [Li, Z., Mao, H., Kim, H.-Y., Tamura, P. J., Harris, C. M., Harris, T. M., and Stone, M. P. (1999) Biochemistry 38, 2969-2981], but was similar to the benzo[a]pyrene BP SRSR (61,3) adduct [Zegar I. S., Chary, P., Jabil, R. J., Tamura, P. J., Johansen, T. N., Lloyd, R. S., Harris, C. M., Harris, T. M., and Stone, M. P. (1998) Biochemistry 37, 16516-16528]. The altered sugar pseudorotation at A6 appears to be common to both bay region BA RSRS (61,3) and BP SRSR (61,3) adducts. It could not be discerned if the C3'-endo conformation at A6 in the BA RSRS (61,3) adduct altered base pairing geometry at X7 x T16, as compared to the C2'-endo conformation. The structural studies suggest that the mutational spectrum of this adduct may be more complex than that of the BA RSRS (61,2) adduct.     

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).     

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 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.     

Solution conformation of a deoxynucleotide containing tandem G.A mismatched base pairs and 3'-overhanging ends in d(GTGAACTT)2.

We have used 31P and 1H NMR spectroscopy and circular dichroism to define the solution conformation of d(GTGAACTT)2 which contains tandem G.A mismatched base pairs and 3'-overhanging TT ends. Measurements of coupling constants and NOE intensities show that the sugar puckers of the nucleotides are predominantly in the south domain (i.e., near C2'-endo) and that the glycosidic torsion angles are anti. The sequential NOE intensities indicate the presence of a right-handed helix. Analysis of the 31P and 1H NMR spectra of the duplex shows that the tandem mismatch forms a block in which there are unusual backbone torsion angles (i.e., in the BII state), within an otherwise B-like structure. The chemical shift of the N1H of the mismatched guanosine and NOEs between the mismatched base pairs and their nearest neighbors are inconsistent with the imino pairing present in single A.G mismatches or in the X-ray structure of a tandem mismatch [Privé, G. G., et al. (1987) Science 238, 498-503] but the data are consistent with the amino pairing found by Li et al. (1991) [Li, Y., et al. (1991) Proc. Natl. Acad. Sci. U.S.A. 88, 26-30]. The strong base-base stacking both within the tandem G.A block and between the G.A mismatches and their other nearest neighbors offsets the intrinsic destabilizing effects of the mismatch. Further, the 3'-TT overhangs stack onto the ends of the helix and stabilize the duplex against fraying, which accounts for the observed increase in the melting temperature compared with the flush-ended duplex.     

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.     

High-resolution NMR studies of chimeric DNA-RNA-DNA duplexes, heteronomous base pairing, and continuous base stacking at junctions.

Two symmetrical DNA-RNA-DNA duplex chimeras, d(CGCG)r(AAUU)d(CGCG) (designated rAAUU) and d(CGCG)r(UAUA)d(CGCG) (designated rUAUA), and a nonsymmetrical chimeric duplex, d(CGTT)r(AUAA)d(TGCG)/d(CGCA)r(UUAU)d(A ACG) (designated rAUAA), as well as their pure DNA analogues, containing dU instead of T, have been synthesized by solid-phase phosphoramidite methods and studied by high-resolution NMR techniques. The 1D imino proton NOE spectra of these d-r-d chimeras indicate normal Watson-Crick hydrogen bonding and base stacking at the junction region. Preliminary qualitative NOESY, COSY, and chemical shift data suggest that the internal RNA segment contains C3'-endo (A-type) sugar conformations except for the first RNA residues (position 5 and 17) following the 3' end of the DNA block, which, unlike the other six ribonucleotides, exhibit detectable H1'-H2' J coupling. The nucleosides of the two flanking DNA segments appear to adopt a fairly normal C2'-endo B-DNA conformation except at the junction with the RNA blocks (residues 4 and 16), where the last DNA residue appears to adopt an intermediate sugar conformation. The DNA-RNA junction residues exhibit quite different COSY, chemical shift, and NOE behavior, but these effects do not appear to propagate into the DNA or RNA segments. The circular dichroism spectra of these d-r-d chimeras also display a mixture of characteristic A-type and B-type absorption bands. The data indicate that A-type and B-type conformations can coexist in a single short continuous nucleic acid duplex, but our results differ somewhat from previous theoretical model studies.     

Deoxyribose conformation in [d(GTATATAC)]2: evaluation of sugar pucker by simulation of double-quantum-filtered COSY cross-peaks

Exchangeable and nonexchangeable proton and phosphorus resonances (11.75 T) of [d(GTATATAC)]2 in aqueous solution were assigned by using proton two-dimensional nuclear Overhauser effect (2D NOE) spectra, homonuclear proton double-quantum-filtered COSY (2QF-COSY) spectra, proton spin-lattice relaxation time measurements, and 31P1H heteronuclear shift correlation spectra. Due to the large line widths, it was not possible to directly extract vicinal proton coupling constant values from any spectrum including ECOSY or 2QF-COSY. However, comparison of quantitative 2QF-COSY spectral simulations with experimental spectra enabled elucidation of coupling constants. The scope and limitations of this approach were explored by computation and by use of experimental data. It was found that proton line widths exhibit some variability from one residue to the next as well as from one proton to the next within a residue and the exact line width is critical to accurate evaluation of coupling constants. Experimental 2QF-COSY spectra were not consistent with a rigid deoxyribose conformation for any of the nucleotide residues. A classical two-state model, with rapid jumps between C2'-endo (pseudorotation angle P = 162 degrees) and C3'-endo (P = 9 degrees) conformations, was able to account for the spectral characteristics of terminal residue sugars: 60% C2'-endo and 40% C3'-endo. However, the 2QF-COSY cross-peaks from the -TATATA- core could be simulated only if the classical two-state model was altered such that the dominant conformer had a pseudorotation angle at 144 degrees instead of 162 degrees. In this case, the major conformer amounted to 80-85%. Alternatively, the spectral data were consistent with a three-state model in which C2'-endo and C3'-endo conformations had the largest and smallest populations, respectively, but a third conformer corresponding to C1'-exo (P = 126 degrees) was present, consistent with recent molecular dynamics calculations. This alternative yielded populations of 50% (P = 162 degrees), 35% (P = 126 degrees), and 15% (P = 9 degrees) for the -TATATA- sugars. The spectral results indicate little variation of sugar pucker between T and A. Small differences in cross-peak component intensities and characteristic spectral distortions, however, do suggest some unquantified variation. 31P1H heteronuclear chemical shift correlation spectra manifested alternating chemical shifts and coupling constants suggestive of phosphodiester backbone conformational differences between TA and AT junctions.     

NMR studies of an exocyclic 1,N2-propanodeoxyguanosine adduct (X) located opposite deoxyadenosine (A) in DNA duplexes at basic pH: simultaneous partial intercalation of X and A between stacked bases

The NMR parameters for the 1,N2-propanodeoxyguanosine (X) opposite deoxyadenosine positioned in the center of the complementary d(C1-A2-T3-G4-X5-G6-T7-A8-C9).d(G10-T11-A12-C13-A14-C15-A 16-T17-G18) X.A 9-mer duplex are pH dependent. A previous paper established protonated X5(syn).A14(anti) pairing in the X.A 9-mer duplex at pH 5.8 [Kouchakdjian, M., Marinelli, E., Gao, X., Johnson, F., Grollman, A., & Patel, D. J. (1989) Biochemistry 28, 5647-5657]; this paper focuses on the pairing alignment at the lesion site at pH 8.9. The observed NOEs between specific exocyclic CH2 protons and both the imino proton of G6 and the sugar H1' protons of C13 and A14 establish that X5 is positioned toward the G6.C13 base pair with the exocyclic ring directed between C13 and A14 on the partner strand. The observed NOE between the H2 proton of A14 and the imino proton of G4, but not G6, establishes that A14 at the lesion site is directed toward the G4.C15 base pair. NOEs are detected between all exocyclic CH2 protons of X5 and the H2 proton of A14, confirming that both X5 and A14 are directed toward the interior of the helix. The X5(anti).A14(anti) alignment at pH 8.9 is accommodated within the helix with retention of Watson-Crick pairing at flanking G4.C15 and G6.C13 base pairs. The energy-minimized conformation of the (G4-X5-G6).(C13-A14-C15) segment at pH 8.9 establishes that X5 and A14 are directed into the helix, partially stack on each other, and are not stabilized by intermolecular hydrogen bonds. The X5 base is partially intercalated between C13 and A14 on the unmodified strand, while A14 is partially intercalated between G4 and X5 on the modified strand. This results in a larger separation between the G4.C15 and G6.C13 base pairs flanking the lesion site in the basic pH conformation of the X.A 9-mer duplex. The midpoint of the transition between the protonated X5(syn).A14(anti) and X5(anti).A14(anti) conformations occurs at pH 7.6, establishing an unusually high pKa for protonation of the A14 ring opposite the X5 exocyclic adduct site. Thus, the interplay between hydrophobic and hydrogen-bonding contributions modulated by pH defines the alignment of 1,N2-propanodeoxyguanosine opposite deoxyadenosine in the interior of DNA helices.     

2'-deoxyribonolactone lesion in DNA: refined solution structure determined by nuclear magnetic resonance and molecular modeling

The solution conformation of the DNA duplex d(C1G2C3A4C5L6C7A8C9G10C11).d(G12C13G14T15G16T17G18T19G20C21G22 ) containing the 2'-deoxyribonolactone lesion (L6) in the middle of the sequence has been investigated by NMR spectroscopy and restrained molecular dynamics calculations. Interproton distances have been obtained by complete relaxation matrix analysis of the NOESY cross-peak intensities. These distances, along with torsion angles for sugar rings and additional data derived from canonical A- and B-DNA, have been used for structure refinement by restrained molecular dynamics (rMD). Six rMD simulations have been carried out starting from both regular A- and B-DNA forms. The pairwise rms deviations calculated for each refined structure are <1 A, indicating convergence to essentially the same geometry. The accuracy of the rMD structures has been assessed by complete relaxation matrix back-calculation. The average sixth-root residual index (Rx = 0.052 +/- 0.003) indicated that a good fit between experimental and calculated NOESY spectra has been achieved. Detailed analysis revealed a right-handed DNA conformation for the duplex in which both the T17 nucleotide opposite the abasic site and the lactone ring are located inside the helix. No kinking is observed for this molecule, even at the abasic site step. This structure is compared to that of the oligonucleotide with the identical sequence containing the stable tetrahydrofuran abasic site analogue that we reported previously [Coppel, Y., Berthet, N., Coulombeau, C., Coulombeau, Ce., Garcia, J., and Lhomme, J. (1997) Biochemistry 36, 4817-4830].