Structure and stability of the consecutive stereoregulated chiral phosphorothioate DNA duplex

The duplex structures of the stereoregulated phosphorothioate DNAs, [R(p),R(p)]- and [S(p),S(p)]-[d(GC(ps)T(ps)ACG)] (ps, phosphorothioate; PS-DNA), with their complementary RNA have been investigated by combined use of (1)H NMR and restrained molecular dynamics calculation. Compared to those obtained for the unmodified duplex structures (PO-DNA.RNA), the NOE cross-peak intensities are virtually identical for the PS-DNA.RNA hybrid duplexes. The structural analysis on the basis of the NOE restraints reveals that all of the three DNA.RNA duplexes take a A-form conformation and that there is no significant difference in the base stacking for the DNA.RNA hybrid duplexes. On the other hand, the NOE cross-peak intensities of the protons around the central T(ps)A step of the PS-DNA.DNA duplexes are apparently different from those of PO-DNA. DNA. The chemical shifts of H8/6 and H1' at the T(ps)A step are also largely different among PS-DNA.DNAs and PO-DNA.DNA, suggesting that the DNA.DNA structure is readily changed by the introduction of the phosphorothioate groups to the central T(p)A step. The structure calculations indicate that all of these DNA.DNA duplexes are B-form although there exist some small differences in helical parameters between the [R(p),R(p)]- and [S(p),S(p)]PS-DNA.DNA duplexes. The melting temperatures (T(m)) were determined for all of the duplexes by plotting the chemical shift change of isolated peaks as a function of temperature. For the PS-DNA.RNA hybrid duplexes, the [S(p),S(p)] isomer is less stable than the [R(p),R(p)] isomer while this trend is reversed for the PS-DNA.DNA duplexes. Consequently, although the PS-DNA.RNA duplexes take the similar A-form structure, the duplex stability is different between PS-DNA.RNA duplexes. The stability of the DNA.RNA duplexes may not be governed by the A-form structure itself but by some other factors such as the hydration around the phosphorothioate backbone, although the T(m) difference of the DNA.DNA duplexes could be explained by the structural factor.     

NMR studies of abasic sites in DNA duplexes: deoxyadenosine stacks into the helix opposite acyclic lesions

Proton and phosphorus NMR studies are reported for two complementary nonanucleotide duplexes containing acyclic abasic sites. The first duplex, d(C-A-T-G-A-G-T-A-C).d(G-T-A-C-P-C-A-T-G), contains an acyclic propanyl moiety, P, located opposite a deoxyadenosine at the center of the helix (designated APP 9-mer duplex). The second duplex, d(C-A-T-G-A-G-T-A-C).d(G-T-A-C-E-C-A-T-G), contains a similarly located acyclic ethanyl moiety, E (designated APE 9-mer duplex). The ethanyl moiety is one carbon shorter than the natural carbon-phosphodiester backbone of a single nucleotide unit of DNA. The majority of the exchangeable and nonexchangeable base and sugar protons in both the APP 9-mer and APE 9-mer duplexes, including those at the abasic site, have been assigned by recording and analyzing two-dimensional phase-sensitive NOESY data sets in H2O and D2O solution between -5 and 5 degrees C. These spectroscopic observations establish that A5 inserts into the helix opposite the abasic site (P14 and E14) and stacks between the flanking G4.C15 and G6.C13 Watson-Crick base pairs in both the APP 9-mer and APE 9-mer duplexes. The helix is right-handed at and adjacent to the abasic site, and all glycosidic torsion angles are anti in both 9-mer duplexes. Proton NMR parameters for the APP 9-mer and APE 9-mer duplexes are similar to those reported previously for the APF 9-mer duplex (F = furan) in which a cyclic analogue of deoxyribose was embedded in an otherwise identical DNA sequence [Kalnik, M. W., Chang, C. N., Grollman, A. P., & Patel, D. J. (1988) Biochemistry 27, 924-931]. These proton NMR experiments demonstrate that the structures at abasic sites are very similar whether the five-membered ring is open or closed or whether the phosphodiester backbone is shortened by one carbon atom. Phosphorus spectra of the APP 9-mer and APE 9-mer duplexes (5 degrees C) indicate that the backbone conformation is similarly perturbed at three phosphodiester backbone torsion angles. These same torsion angles are also distorted in the APF 9-mer but assume a different conformation than those in the APP 9-mer and APE 9-mer duplexes.     

Impact of the C1' configuration of abasic sites on DNA duplex structure

Naturally occurring abasic sites in DNA exist as an equilibrium mixture of the aldehyde, the hydrated aldehyde, and the hemiacetal forms (dominant). The influence of the configuration of the C1' hydroxyl group of the hemiacetal form on duplex structure and abasic site repair has been examined using novel carbocyclic analogues. Both the alpha- and beta-forms of this novel abasic site were introduced into oligomeric DNA using the standard DMT-phosphoramidite approach in an automated solid-phase synthesizer. Solution structures of the d(CGTACXCATGC).d(GCATGAGTACG) duplex (where X is the alpha- or beta-anomer of the carbocyclic abasic site analogue) were determined by NMR spectroscopy and restrained molecular dynamics simulations. The structures were only minimally perturbed by the presence of either anomer of the abasic site. All residues adopted an anti conformation, and Watson-Crick alignments were observed on all base pairs of the duplexes. At the lesion site, the abasic residues and their partner adenines showed increased dynamic behavior but adopted intrahelical positions in the final refined structures. Incision of duplexes having the alpha- or beta-anomer of the carbocyclic abasic site by human AP endonuclease showed that the enzyme recognizes both configurations of the lesion and nicks the DNA backbone with similar efficiency. Our results challenge the suggestion that Ape1 is stereoselective and imply a plasticity at the active site of the enzyme for accommodating either anomer of the lesion.     

NMR evidence for syn-anti interconversion of a trans opened (10R)-dA adduct of benzo[a]pyrene (7S,8R)-diol (9R,10S)-epoxide in a DNA duplex

2D NMR has been used to examine the structure and dynamics of a 12-mer DNA duplex, d(T(1)A(2)G(3)T(4)C(5)A(6)A(7)G(8)G(9)G(10)C(11)A(12))-d(T(13)G(14)C( 15)C(16)C(17)T(18)T(19)G(20)A(21)C(22)T(23)A(24)), containing a 10R adduct at dA(7) that corresponds to trans addition of the N(6)-amino group of dA(7) to (-)-(7S,8R,9R,10S)-7,8-dihydroxy-9, 10-epoxy-7,8,9,10-tetrahydrobenzo[a]pyrene [(-)-(S,R,R,S)-BP DE-2]. This DNA duplex contains the base sequence for the major dA mutational hot spot in the HPRT gene when Chinese hamster V79 cells are given low doses of the highly carcinogenic (+)-(R,S,S,R)-BP DE-2 enantiomer. NOE data indicate that the hydrocarbon is intercalated on the 5'-side of the modified base as has been seen previously for other oligonucleotides containing BP DE-2 (10R)-dA adducts. 2D chemical exchange-only experiments indicate dynamic behavior near the intercalation site especially at the 10R adducted dA, such that this base interconverts between the normal anti conformation and a less populated syn conformation. Ab initio molecular orbital chemical shift calculations of nucleotide and dinucleotide fragments in the syn and anti conformations support these conclusions. Although this DNA duplex containing a 10R dA adduct exhibits conformational flexibility as described, it is nevertheless more conformationally stable than the corresponding 10S adducted duplex corresponding to trans opening of the carcinogenic isomer (+)-(R,S,S, R)-BP DE-2, which was too dynamic to permit NMR structure determination. UV and imino proton NMR spectral observations indicated pronounced differences between these two diastereomeric 12-mer duplexes, consistent with conformational disorder at the adduct site and/or an equilibrium with a nonintercalated orientation of the hydrocarbon in the duplex containing the 10S adduct. The existence of conformational flexibility around adducts may be related to the occurrence of multiple mutagenic outcomes resulting from a single DE adduct.     

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

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

Computation of nitroxide-nitroxide distances in spin-labeled DNA duplexes

Nanometer distances in nucleic acids can be measured by EPR using two 1-oxyl-2,2,5,5-tetramethylpyrroline radicals, with each label attached via a methylene group to a phosphorothioate-substituted backbone position as one of two phosphorothioate diastereomers (R(P) and S(P)). Correlating the internitroxide distance to the geometry of the parent molecule requires computational analysis of the label conformers. Here, we report sixteen 4-ns MD simulations on a DNA duplex d(CTACTGCTTTAG) .d(CTAAAGCAGTAG) with label pairs at C7/C19, T5/A17, and T2/T14, respectively. For each labeled duplex, four simulations were performed with S(P)/S(P), R(P)/R(P), S(P)/R(P), and R(P)/S(P) labels, with initial all trans label conformations. Another set of four simulations was performed for the 7/19-labeled duplex using a different label starting conformation. The average internitroxide distance r(MD) was within 0.2 A for the two sets of simulations for the 7/19-labeled duplex, indicating sufficient sampling of conformational space. For all three labeled duplexes studied, r(MD) agreed with experimental values, as well as with average distances obtained from an efficient conformer search algorithm (NASNOX). The simulations also showed that the labels have conformational preferences determined by the linker chemistry and label-DNA interactions. These results establish computational algorithms that allow use of the 1-oxyl-2,2,5,5-tetramethylpyrroline label for mapping global structures of nucleic acids.     

Structure of hybrid backbone methylphosphonate DNA heteroduplexes: effect of R and S stereochemistry.

Methyl phosphonate oligonucleotides have been used as antisense and antigene agents. Substitution of a methyl group for oxygen in the phosphate ester backbone introduces a new chiral center. Significant differences in physical properties and hybridization abilities are observed between the R(p) and S(p) diastereomers. Chirally pure methylphosphonate deoxyribooligonucleotides were synthesized, and the solution structures of duplexes formed between a single strand heptanucleotide methylphosphonate, d(Cp(Me)Cp(Me)Ap(Me)Ap(Me)Ap(Me)Cp(Me)A), hybridized to a complementary octanucleotide, d(TpGpTpTpTpGpGpC), were studied by NMR spectroscopy. Stereochemistry at the methylphosphonate center for the heptanucleotide was either RpRpRpRpRpRp (R(p) stereoisomer) or RpRpRpSpRpRp (S(p) stereoisomer, although only one of the six methylphosphonate centers has the S(p) stereochemistry). The results show that the methylphosphonate strands in the heteroduplexes exhibit increased dynamics relative to the DNA strand. Substitution of one chiral center from R(p) to S(p) has a profound effect on the hybridization ability of the methylphosphonate strand. Sugars in the phosphodiester strand exhibit C(2)(') endo sugar puckering while the sugars in the methyl phosphonate strand exhibit an intermediate C(4)(') endo puckering. Bases are well stacked on each other throughout the duplex. The hybridization of the methylphosphonate strand does not perturb the structure of the complementary DNA strand in the hetero duplexes. The sugar residue 5' to the S(p) chiral center shows A-form sugar puckering, with a C(3)(')-endo conformation. Minor groove width in the R(p) stereoisomer is considerably wider, particularly at the R(p) vs S(p) site and is attributed to either steric interactions across the minor groove or poorer metal ion coordination within the minor groove.     

The solution conformation of a carbocyclic analog of the Dickerson-Drew dodecamer: comparison with its own X-ray structure and that of the NMR structure of the native counterpart

The NMR conformation of a carbocyclic analog of the Dickerson-Drew dodecamer [d(CGC-GAAT*T*CGCG)]2 containing 6'-alpha-Me carbocyclic thymidines (T*) has been determined and compared with that of its X-ray structure. The solution structure of the 6'-alpha-Me carbocyclic thymidine modified duplex has also been compared with the solution structure of the corresponding unmodified Dickerson-Drew duplex solved by us under the same experimental conditions. The NMR structures have been based on 24 experimental distance and torsion constraints per residue for [d(CGCGAAT*T*CGCG)]2 (1) and on 21 constraints per residue for the natural counterpart. In general, both final NMR structures are more close to the B-type DNA. The cyclopentane moieties of the carbocyclic thymidine residues adopt C1'-exo B-DNA type puckers (the phase angles P = 136-139 degrees and the puckering amplitudes psi = 36-37 degrees) that are close to their previously published crystal C1'-exo or C2'-endo puckers. The main differences between the two NMR structures are for beta(T*8) and epsilon, xi(T*7) backbone torsions (27-50 degrees ), for basepair twist for the 7-8 and 8-9 basepair steps (5-6 degrees), tilt for the 8-9 step (7 degrees), roll for the 7-8 step (7 degrees), shift for the 7-8 step (0.9A) and slide for the 9-10 step (0.6A). The relatively small deviations of helical structure parameters lead to structural isomorphism of these duplexes in aqueous solutions (atomic RMSD = 1.0A). The difference of the minor groove widths (less than 0.7A) in the core part of the modified duplex in comparison with the native one is much smaller than the difference between the X-ray structures of these duplexes. A detailed comparison of NMR and X-ray structure parameters showed significant monotonic differences (0.9-2.5A) for all basepair slides in both duplexes. Deviations between NMR and X-ray structure parameters for the modified duplex were also found for basepair tilt of the 4-5 step (13 degrees), rolls for the 8-9 and 10-11 steps (16 and 19 degrees), twist of the 3-4 step (8 degrees) and shift of the 9-10 step (0.9A).     

Backbone-base inclination as a fundamental determinant of nucleic acid self- and cross-pairing

The crystal structure of the duplex formed by oligo(2',3'-dideoxy-beta-d-glucopyranosyl)nucleotides (homo-DNA) revealed strongly inclined backbone and base-pair axes [Egli,M., Pallan,P.S., Pattanayek,R., Wilds,C.J., Lubini,P., Minasov,G., Dobler,M., Leumann,C.J. and Eschenmoser,A. (2006) Crystal structure of homo-DNA and nature's choice of pentose over hexose in the genetic system. J. Am. Chem. Soc., 128, 10847-10856]. This inclination is easily perceived because homo-DNA exhibits only a modest helical twist. Conversely, the tight coiling of strands conceals that the backbone-base inclinations for A- (DNA and RNA) and B-form (DNA) duplexes differ considerably. We have defined a parameter eta(B) that corresponds to the local inclination between sugar-phosphate backbone and base plane in nucleic acid strands. Here, we show its biological significance as a predictive measure for the relative strand polarities (antiparallel, aps, or parallel, ps) in duplexes of DNA, RNA and artificial nucleic acid pairing systems. The potential of formation of ps duplexes between complementary 16-mers with eight A and U(T) residues each was investigated with DNA, RNA, 2'-O-methylated RNA, homo-DNA and p-RNA, the ribopyranosyl isomer of RNA. The thermodynamic stabilities of the corresponding aps duplexes were also measured. As shown previously, DNA is capable of forming both ps and aps duplexes. However, all other tested systems are unable to form stable ps duplexes with reverse Watson-Crick (rWC) base pairs. This observation illustrates the handicap encountered by nucleic acid systems with inclinations eta(B) that differ significantly from 0 degrees to form a ps rWC paired duplex. Accordingly, RNA with a backbone-base inclination of -30 degrees , pairs strictly in an aps fashion. On the other hand, the more or less perpendicular orientation of backbone and bases in DNA allows it to adopt a ps rWC paired duplex. In addition to providing a rationalization of relative strand polarity with nucleic acids, the backbone-base inclination parameter is also a determinant of cross-pairing. Thus, systems with strongly deviating eta(B) angles will not pair with each other. Nucleic acid pairing systems with significant backbone-base inclinations can also be expected to display different stabilities depending on which terminus carries unpaired nucleotides. The negative inclination of RNA is consistent with the higher stability of duplexes with 3'- compared to those with 5'-dangling ends.     

A molecular dynamics study of the effect of G.T mispairs on the conformation of DNA in solution

The effect of G.T mispair incorporation into a double-helical environment was examined by molecular dynamics simulation. The 60-ps simulations performed on the two hexanucleotide duplexes d (G3C3)2 and d(G3TC2)2 included 10 Na+ counterions and first hydration shell waters. The resulting backbone torsional angle trajectories were analyzed to select time spans representative of conformational domains. The average backbone angles and helical parameters of the last time span for both duplexes are reported. During the simulation the hexamers retained B-type DNA structures that differed from typical A- or B-DNA forms. The overall helical structures for the two duplexes are vary similar. The presence of G.T mispairs did not alter the overall helical structure of the oligonucleotide duplex. Large propeller twist and buckle angles were obtained for both duplexes. The purine/pyrimidine crossover step showed a large decrease in propeller twist in the normal duplex but not in the mismatch duplex. Upon the formation of wobble mispairs in the mismatched duplex, the guanines moved into the minor groove and the thymines moved into the major groove. This helped prevent purine/purine clash and created a deformation in the relative orientation of the glycosidic bonds. It also exposed the free O4 of the thymines in the major groove and N2 of the guanines in the minor groove to interactions with solvent and counterions. These factors seemed to contribute to the apparently higher rigidity of the mismatched duplex during the simulation.     

Effects of GA mismatches on the structure and thermodynamics of RNA internal loops

UV melting, CD and NMR studies indicate rGCGAGCG and rGCAGGCG from unusually stable duplexes of type a and b. The observed delta G degree 37's in 1 M NaCl are -6.7 and -6.3 kcal/mol, respectively. For the related duplex, c, delta G degree 37 is -4.2 kcal/mol. The predicted delta G degree 37 from nearest-neighbor parameters (formula; see text) for all three duplexes is -4.7 kcal/mol (Freier, S.M., Kierzek, R., Jaeger, J.A., Sugimoto, N., Caruthers, M.H., Neilson, T., & Turner, D.H. (1986) Proc. Natl. Acad. Sci. U.S.A. 83, 9373-9377). The results suggest a special interaction in the duplexes containing GA mismatches. Presumably, this is hydrogen bonding between G and A. While the thermodynamics for (rGCGAGCG)2 and (rGCAGGCG)2 are similar, CD and the imino region of the proton NMR spectra indicate their structures are different. In particular, (rGCAGGCG)2 exhibits a CD spectrum typical of A-form geometry with a weak negative band at 280 nm. In contrast, the CD spectrum for (rGCGAGCG)2 has an intense positive band at 285 nm. The NMR spectrum of (rGCAGGCG)2 has a resonance corresponding to a hydrogen-bonded GA mismatch, while for (rGCGAGCG)2 no hydrogen-bonded imino proton is observed for the mismatch. The glycosidic torsion angles of the bases in the GA mismatches of (rGCAGGCG)2 and (rCGCAGGCG)2 are anti. Duplexes of type d, where X is A, G, or U, are more stable than e, and the stability differences are similar to those (formula; see text) observed for f versus g. Thus, 3'-dangling ends in this system make contributions to duplex stability that are similar to contributions observed with fully paired duplexes.     

Assignments of 31P NMR resonances in oligodeoxyribonucleotides: origin of sequence-specific variations in the deoxyribose phosphate backbone conformation and the 31P chemical shifts of double-helical nucleic acids

It is now possible to unambiguously assign all 31P resonances in the 31P NMR spectra of oligonucleotides by either two-dimensional NMR techniques or site-specific 17O labeling of the phosphoryl groups. Assignment of 31P signals in tetradecamer duplexes, (dTGTGAGCGCTCACA)2, (dTAT-GAGCGCTCATA)2, (dTCTGAGCGCTCAGA)2, and (dTGTGTGCGCACACA)2, and the dodecamer duplex d(CGTGAATTCGCG)2 containing one base-pair mismatch, combined with additional assignments in the literature, has allowed an analysis of the origin of the sequence-specific variation in 31P chemical shifts of DNA. The 31P chemical shifts of duplex B-DNA phosphates correlate reasonably well with some aspects of the Dickerson/Calladine sum function for variation in the helical twist of the oligonucleotides. Correlations between experimentally measured P-O and C-O torsional angles and results from molecular mechanics energy minimization calculations show that these results are consistent with the hypothesis that sequence-specific variations in 31P chemical shifts are attributable to sequence-specific changes in the deoxyribose phosphate backbone. The major structural variation responsible for these 31P shift perturbations appears to be P-O and C-O backbone torsional angles which respond to changes in the local helical structure. Furthermore, 31P chemical shifts and JH3'-P coupling constants both indicate that these backbone torsional angle variations are more permissive at the ends of the double helix than in the middle. Thus 31P NMR spectroscopy and molecular mechanics energy minimization calculations appear to be able to support sequence-specific structural variations along the backbone of the DNA in solution.     

Structural effect of the anticancer agent 6-thioguanine on duplex DNA

The incorporation of 6-thioguanine (S6G) into DNA is an essential step in the cytotoxic activity of thiopurines. However, the structural effects of this substitution on duplex DNA have not been fully characterized. Here, we present the solution structures of DNA duplexes containing S6G opposite thymine (S6G·T) and opposite cytosine (S6G·C), solved by high-resolution NMR spectroscopy and restrained molecular dynamics. The data indicate that both duplexes adopt right-handed helical conformations with all Watson–Crick hydrogen bonding in place. The S6G·T structures exhibit a wobble-type base pairing at the lesion site, with thymine shifted toward the major groove and S6G displaced toward the minor groove. Aside from the lesion site, the helices, including the flanking base pairs, are not highly perturbed by the presence of the lesion. Surprisingly, thermal dependence experiments suggest greater stability in the S6G-T mismatch than the S6G-C base pair.     

1H NMR assignment and melting temperature study of cis-syn and trans-syn thymine dimer containing duplexes of d(CGTATTATGC).d(GCATAATACG)

The preparation and spectroscopic characterization of duplex decamers containing site-specific cis-syn and trans-syn thymine dimers are described. Three duplex decamers, d(CGTATTATGC).d(GCATAATACG), d(CGTAT[c,s]TATGC).d(GCATAATACG), and d(CGTAT[t,s]TATGC).d(GCATAATACG), were prepared by solid-phase phosphoramidite synthesis utilizing cis-syn and trans-syn cyclobutane thymine dimer building blocks (Taylor et al., 1987; Taylor & Brockie, 1988). NMR spectra (500 MHz 2D 1H and 202 MHz 1D 31P) were obtained in "100%" D2O at 10 degrees C, and 1D exchangeable 1H spectra were obtained in 10% D2O at 10 degrees C. 1H NMR assignments for H5, H6, H8, CH3, H1', H2', and H2" were made on the basis of standard sequential NOE assignment strategies and verified in part by DQF COSY data. Comparison of the chemical shift data suggests that the helix structure is perturbed more to the 3'-side of the cis-syn dimer and more to the 5'-side of the trans-syn dimer. Thermodynamic parameters for the helix in equilibrium coil equilibrium were obtained by two-state, all or none, analysis of the melting behavior of the duplexes. Analysis of the temperature dependence of the T5CH3 1H NMR signal gave delta H = 44 +/- 4 kcal and delta S = 132 +/- 13 eu for the trans-syn duplex. Analysis of the concentration and temperature dependence of UV spectra gave delta H = 64 +/- 6 kcal and delta S = 178 +/- 18 eu for the parent duplex and delta H = 66 +/- 7 kcal and delta S = 189 +/- 19 eu for cis-syn duplex. It was concluded that photodimerization of the dTpdT unit to give the cis-syn product causes little perturbation of the DNA whereas dimerization to give the trans-syn product causes much greater perturbation, possibly in the form of a kink or dislocation at the 5'-side of the dimer.     

NMR structure of an antisense DNA.RNA hybrid duplex containing a 3'-CH(2)N(CH(3))-O-5' or an MMI backbone linker.

The solution structure of an antisense DNA.RNA hybrid duplex, d(CGCGTT-MMI-TTGCGC).r(GCGCAAAACGCG) (designated R4), containing an MMI backbone linker [3'-CH(2)N(CH(3))-O5'], is elucidated. The structural details of the MMI linker, its structural effects on the neighboring residues, and the molecular basis of the MMI effects are examined. The lipophilic N-methyl group of MMI is peripheral to the helix, assuming a conformation that is most stable with regard to the N-O torsion angle. The MMI linker promotes a 3'-endo conformation for the sugar moieties at both 3'- and 5'-adjacent positions and a backbone kink involving distant residues along the 3'-direction. Comparison of R4 with other analogous hybrid duplexes previously studied in this laboratory reveals a new family of low-energy helical conformations that can be accommodated in stable duplexes and a common feature of C3'-modified sugars for adopting a C3'-endo pucker. The results of these studies emphasize the interplay of several factors that govern the formation of stable hybrid duplexes and provide a basis for the understanding of the biological role of the MMI modifications, which are important building blocks for a family of promising chimeric antisense oligonucleotides.     

Oligonucleotides with conjugated dihydropyrroloindole tripeptides: base composition and backbone effects on hybridization.

The ability of conjugated minor groove binding (MGB) residues to stabilize nucleic acid duplexes was investigated by synthesis of oligonucleotides bearing a tethered dihydropyrroloindole tripeptide (CDPI3). Duplexes bearing one or more of these conjugated MGBs were varied by base composition (AT- or GC-rich oligonucleotides), backbone modifications (phosphodiester DNA, 2'-O-methyl phosphodiester RNA or phosphorothioate DNA) and site of attachment of the MGB moiety (5'- or 3'-end of either duplex strand). Melting temperatures of the duplexes were determined. The conjugated CDPI3 residue enhanced the stability of virtually all duplexes studied. The extent of stabilization was backbone and sequence dependent and reached a maximum value of 40-49 degrees C for d(pT)8. d(pA)8. Duplexes with a phosphorothioate DNA backbone responded similarly on CDPI3 conjugation, although they were less stable than analogous phosphodiesters. Modest stabilization was obtained for duplexes with a 2'-O-methyl RNA backbone. The conjugated CDPI3 residue stabilized GC-rich DNA duplexes, albeit to a lesser extent than for AT-rich duplexes of the same length.     

Binding of nucleic acids to E. coli RNase HI observed by NMR and CD spectroscopy.

To clarify the mechanism by which the RNA portion of a DNA/RNA hybrid is specifically hydrolyzed by ribonuclease H (RNase H), the binding of a DNA/RNA hybrid, a DNA/DNA duplex, or an RNA/RNA duplex to RNase HI from Escherichia coli was investigated by 1H-15N heteronuclear NMR. Chemical shift changes of backbone amide resonances were monitored while the substrate, a hybrid 9-mer duplex, a DNA/DNA 12-mer duplex, or an RNA/RNA 12-mer duplex was titrated. The amino acid residues affected by the addition of each 12-mer duplex were almost identical to those affected by the substrate hybrid binding, and resided close to the active site of the enzyme. The results reveal that all the duplexes, hybrid-, DNA-, and RNA-duplex, bind to the enzyme. From the linewidth analysis of the resonance peaks, it was found that the exchange rates for the binding were different between the hybrid and the other duplexes. The NMR and CD data suggest that conformational changes occur in the enzyme and the hybrid duplex upon binding.     

The DNA phosphate backbone is not involved in catalysis of the duocarmycin and CC-1065 DNA alkylation reaction

The rates of DNA alkylation were established for the reaction of (+)-duocarmycin SA (1) with the native duplex d(G(1)TCAATTAGTC(11))*d(G(12)ACTAATTGAC(22)), an 11 bp deoxyoligonucleotide that contains a single high-affinity alkylation site that has been structurally characterized at exquisite resolution, and modified duplexes in which the four backbone phosphates proximal to the C4 carbonyl of bound 1 were replaced with methylphosphonates. All were found to react at comparable rates establishing that these backbone phosphates do not participate in catalysis of the DNA alkylation reaction.     

HU protein employs similar mechanisms of minor-groove recognition in binding to different B-DNA sites: demonstration by Raman spectroscopy

The sequence isomers d(CGCAAATTTGCG) and d(TCAAGGCCTTGA) form self-complementary duplexes that present distinct targets for binding of the homodimeric architectural protein HU of Bacillus stearothermophilus (HUBst). Raman spectroscopy shows that although each duplex structure is of the B-DNA type, there are subtle conformational dissimilarities between them, involving torsion angles of the phosphodiester backbone and the arrangements of stacked bases. Each DNA duplex forms a stable stoichiometric (1:1) complex with HUBst, in which the structure of the HUBst dimer is largely conserved. However, the Raman signature of each DNA duplex is perturbed significantly and similarly with HUBst binding, as reflected in marker bands assigned to localized vibrations of the phosphodiester moieties and base residues. The spectral perturbations identify a reorganization of the DNA backbone and partial unstacking of bases with HUBst binding, which is consistent with non-sequence-specific minor-groove recognition. Prominent among the HUBst-induced perturbations of B-DNA are a conversion of approximately one-third of the alpha/beta/gamma torsions from the canonical g(-)/t/g(+) conformation to an alternative conformation, an equivalent conversion of deoxyadenosyl moieties from the C2'-endo/anti to the C3'-endo/anti conformation, and appreciable unstacking of purines. The results imply that each solution complex is characterized by structural perturbations extending throughout the 12-bp sequence. Comparison with previously studied protein/DNA complexes suggests that binding of HUBst bends DNA by approximately 70 degrees.     

Conformational transitions in thymidine bulge-containing deoxytridecanucleotide duplexes. Role of flanking sequence and temperature in modulating the equilibrium between looped out and stacked thymidine bulge states

Structural features at extra thymidine bulge sites in DNA duplexes have been elucidated from a two-dimensional NMR analysis of through-bond and through-space connectivities in the otherwise self-complementary d(C-C-G-T-G-A-A-T-T-C-C-G-G) (GTG 13-mer) and d(C-C-G-G-A-A-T-T-C-T-C-G-G) (CTC 13-mer) duplexes in aqueous solution. These studies establish that the extra thymidine flanked by guanosines in the GTG 13-mer duplex is in a conformational equilibrium between looped out and stacked states. The looped-out state is favored at low temperature (0 degrees C), whereas the equilibrium shifts in favor of the stacked state at elevated temperatures (35 degrees C) prior to the onset of the duplex-strand transition. By contrast, the extra thymidine flanked by cytidines in the CTC 13-mer duplex is looped out independent of temperature in the duplex state. Our results demonstrate that temperature and flanking sequence modulate the equilibrium between looped-out and stacked conformations of single base thymidine bulges in DNA oligomer duplexes.