Solution structure of [d(GCGTATACGC)]2.

The solution structure of the alternating pyrimidine-purine DNA duplex [d(GCGTATACGC)]2 has been determined using two-dimensional nuclear magnetic resonance techniques and distance geometry methods. Backbone distance constraints derived from experimental nuclear Overhauser enhancement and J-coupling torsion angle constraints were required to adequately define the conformation of the inter-residue backbone linkages and to avoid underwinding of the duplex. The distance geometry structures were further refined by back-calculation of the two-dimensional nuclear Overhauser enhancement spectra to correct spin-diffusion distance errors. Fifteen final structures for [d(GCGTATACGC)]2 were generated from the refined experimental distance bounds. These structures all exhibit fully wound B-form geometry with small penalty values (< 1.5 A) against the distance bounds and small pair-wise root-mean-square deviation values (typically 0.6 A to 1.5 A). The final structures exhibit positive base-pair inclination with respect to the helix axis, a marked alternation in rise and twist, and are shorter and wider than classical fiber B-form DNA. The purines were found to adopt a sugar pucker close to the C-2'-endo conformation while pyrimidine sugars exhibited significantly lower pseudorotation phase angles in the C-1'-exo to C-2'-endo range. The minor groove cross-strand steric clashes at pyrimidine-purine steps that would exist in pure B-DNA are attenuated by an increased rise at these steps (and an increased roll angle at TpA steps). Concomitantly the backbone torsion angles of the pyrimidine moieties have larger gamma values, larger epsilon values, and smaller zeta values than the purines. The structures generated by distance geometry methods were also compared with those obtained from restrained molecular dynamics with empirical force-field potentials. The results indicate that the nuclear magnetic resonance/distance geometry approach alone is capable of elucidating most of the salient structural features of double-stranded helical nucleic acids in solution without resorting to empirical energy potentials and without using any structural assumptions from crystallographic data.     

Two-dimensional nuclear Overhauser enhancement investigation of the solution structure and dynamics of the DNA octamer [d(GGTATACC)]2

The resonances of nearly all 70 of the non-exchangeable protons of the duplex [d(GGTATACC)]2 in aqueous solution are assigned by proton two-dimensional nuclear Overhauser enhancement (2D NOE) spectra obtained in pure absorption phase at 500 MHz. Experimental and theoretical 2D NOE spectra are compared at each mixing time (100, 175, 250 and 400 ms) using two B-DNA structures: a standard B-form and an energy-minimized form. The GG and CC ends of the octamer duplex are well represented by the regular B-DNA structure. But large discrepancies from these models are observed for the 'TATA' box. All 2D NOE data are consistent with nanosecond correlation times, as indicated by non-selective proton spin-lattice relaxation times, but small variations in the correlation time are observed, suggesting that there are some local differences in mobility within the octamer duplex structure in solution.     

Solution structure of [d(A-T)5]2 via complete relaxation matrix analysis of two-dimensional nuclear Overhauser effect spectra and molecular mechanics calculations: evidence for a hydration tunnel

Pure absorption phase proton two-dimensional nuclear Overhauser effect (2D NOE) spectra at 500 MHz have been obtained for [d(5'ATATATATAT3')]2 in deuterium oxide solution at several mixing times. The 100 nonexchangeable proton resonances have been assigned. The experimental 2D NOE spectra were compared with theoretical spectra calculated by using the complete relaxation matrix analysis method [Keepers, J. W., & James, T. L. (1984) J. Magn. Reson. 57, 404-426] and x-ray diffraction determined molecular coordinates of A, B, alternating B, left-handed B, C, D, and wrinkled D forms of DNA and of energy-minimized structures calculated from the most promising X-ray crystal structures by using the molecular mechanics program AMBER, in which all hydrogens, counterions, and hydration water molecules were included. The analysis of all features of the 2D NOE spectra played an important role in extracting the promising structures, and it was concluded that the wrinkled D form yields the best fit for the 2D NOE data of the A-T decamer. The molecular mechanics calculation indicated that this model structure, whose minor groove is comparatively deep and narrow, may be energetically more stable than the B form for alternating d(A-T) DNA. Interesting features of the structure include possible intra- and interchain sugar-phosphate attractions and a hydration tunnel inside the minor groove capable of accommodating three types of water molecules that aid in helix stabilization via hydrogen bonding. Counterions (sodium) serve to reduce interchain phosphate-phosphate repulsive effects.     

Quantitative internuclear distancesvia two-dimensional nuclear magnetic resonance spectra: A test case and a DNA octamer duplex

Two-dimensional proton nuclear magnetic resonance nuclear Overhauser effect experiments have been performed at a series of mixing times on proflavine and on a DNA octamer duplex [d-(GGAATTCC)]₂ in solution. Using the complete matrix approach recently explored theoretically (Keepers and James, 1984), proton-proton internuclear distances were determined quantitatively for proflavine from the two-dimensional nuclear Overhauser effect results. Since proflavine is a rigid molecule with X-ray crystal structure determined, interproton distances obtained from the two-dimensional nuclear Overhauser effect experiments in solution can be compared with those for the crystalline compound agreement is better than 10 %. Experimental two-dimensional nuclear Overhauser effect spectral data for [d-(GGAATTCC)]₂ were analyzed by comparison with theoretical two-dimensional nuclear Overhauser effect spectra at each mixing time calculated using the complete 70 × 70 relaxation matrix. The theoretical spectra were calculated using two structures: a standard B-form DNA structure and an energy-minimized structure based on similarity of the octamer's six internal residues with those of [d-(CGCGAATTCGCG)]₂, for which the crystal structure has been determined. Neither the standard B-DNA nor the energy-minimized structure yield theoretical two-dimensional nuclear Overhauser effect spectra which accurately reproduce all experimental peak intensities. But many aspects of the experimental spectra can be represented by both the B-DNA and the energy-minimized structure. In general, the energy-minimized structure yields theoretical two-dimensional nuclear Overhauser effect spectra which mimic many, if not all, features of the experimental, spectra including structural characteristics at the purine-pyrimidine junction.     

Investigation of the solution structure of a DNA octamer [d(GGAATTCC)]2 using two-dimensional nuclear Overhauser enhancement spectroscopy

Proton two-dimensional nuclear Overhauser enhancement (2D NOE) spectra in the pure absorption phase were obtained at 500 MHz for [d(GGAATTCC)]2 in aqueous solution at a series of mixing times. The experimental data were analyzed by comparison with theoretical spectra calculated using the complete 70 X 70 relaxation matrix including all proton dipole-dipole interactions and spin diffusion [Keepers, J. W. & James, T. L. (1984) J. Magn. Reson. 57, 404-426]. The theoretical spectra at each mixing time were calculated using two structures: a standard B-form DNA structure and an energy-minimized structure based on the similarity of the six internal residues of the title octamer with those of the dodecamer [d(CGCGAATTCGCG)]2, for which the crystal structure has been determined. Neither the standard B-form nor the energy-minimized structure will yield theoretical 2D NOE spectra which accurately reproduce all peak intensities in the experimental spectra. However, many features of the experimental spectra can be represented by both the B-form and the energy-minimized structure. Sequence-dependent structural characteristics are manifest in the 2D NOE spectra, in particular at the purine-pyrimidine junction as noted previously in the crystal structure. On the whole, the energy-minimized structure appears to yield theoretical 2D NOE spectra which mimic many, if not all, aspects of the experimental spectra. All 2D NOE data were consistent with nanosecond correction times as implied by proton spin-lattice relaxation time measurements. But better fits of some of the 2D NOE data using small variations in an effective isotropic correlation time suggest that there may be some local variations in mobility within the octamer duplex structure in solution.     

Changes in drug 13C NMR chemical shifts as a tool for monitoring interactions with DNA

The antibiotic drug, netropsin, was complexed with the DNA oligonucleotide duplex [d(GGTATACC)]2 to monitor drug 13C NMR chemical shifts changes. The binding mode of netropsin to the minor groove of DNA is well-known, and served as a good model for evaluating the relative sensitivity of 13C chemical shifts to hydrogen bonding. Large downfield shifts were observed for four resonances of carbons that neighbor sites which are known to form hydrogen bond interactions with the DNA minor groove. Many of the remaining resonances of netropsin exhibit shielding or relatively smaller deshielding changes. Based on the model system presented here, large deshielding NMR shift changes of a ligand upon macromolecule binding can likely be attributed to hydrogen bond formation at nearby sites.     

Bh-DNA: variations of the poly[d(A)].poly[d(T)] structure within the framework of the fibre diffraction studies

A refinement of the recent results for poly[d(A)].poly[d(T)] (Alexeev et al., J. Biomol. Struct. Dyn. 4,989 (1987)) involving additional parameters of the base-pair structure and of the sugar-phosphate backbone expands the conformational potential of this polynucleotide of the B type to include the possibility of bifurcated hydrogen bonds of the kind recently discovered in crystalline deoxyoligonucleotide with lone d(A)n.d(T)n stretch (Nelson et al., Nature 330, 221 (1987)). Still, analysis of the available data and energy calculations do not seem to indicate that the bifurcated H-bonds are a crucial factor responsible for the anomalous structure of the d(A)n.d(T)n sequence. The unique structural properties of poly[d(A)].poly[d(T)] can hardly be explained without taking into account its interactions with the double-layer hydration spine in the minor groove. In view of the hydration mechanism stabilizing poly[d(A)].poly[d(T)] and of the polynucleotide's heteronomous prehistory (Arnott et al., Nucleic Acids Res. 11,4141 (1983)) we suggest that this B-type structure be called Bh.     

X-ray structure of the DNase I-d(GGTATACC)2 complex at 2.3 A resolution.

The crystal structure of a complex between DNase I and the self-complementary octamer duplex d(GGTATACC)2 has been solved using the molecular replacement method and refined to a crystallographic R-factor of 18.8% for all data between 6.0 and 2.3 A resolution. In contrast to the structure of the DNase I-d(GCGATCGC)2 complex solved previously, the DNA remains uncleaved in the crystal. The general architecture of the two complexes is highly similar. DNase I binds in the minor groove of a right-handed DNA duplex, and to the phosphate backbones on either side over five base-pairs, resulting in a widening of the minor groove and a concurrent bend of the DNA away from the bound enzyme. There is very little change in the structure of the DNase I on binding the substrate. Many other features of the interaction are conserved in the two complexes, in particular the stacking of a deoxyribose group of the DNA onto the side-chain of a tyrosine residue (Y76), which affects the DNA conformation and the binding of an arginine side-chain in the minor groove. Although the structures of the DNA molecules appear at first sight rather similar, detailed analysis reveals some differences that may explain the relative resistance of the d(GGTATACC)2 duplex to cleavage by DNase I: whilst some backbone parameters are characteristic of a B-conformation, the spatial orientation of the base-pairs in the d(GGTATACC)2 duplex is close to that generally observed in A-DNA. These results further support the hypothesis that the minor-groove width and depth and the intrinsic flexibility of DNA are the most important parameters affecting the interaction. The disposition of residues around the scissile phosphate group suggests that two histidine residues, H134 and H252, are involved in catalysis.     

Solution structure of the TnAn DNA duplex GCCGTTAACGCG containing the HpaI restriction site.

The solution structure of the self-complementary DNA duplex [d(GCCGTTAACGGC)]2, which contains the HpaI restriction site GTTAAC, has been elucidated by two-dimensional NMR, distance geometry (DG), and NOE back-calculation methods. Initial distance constraints were determined by polynomial fitting the two-spin initial NOE rates; backbone constraints from NOE and J-coupling observations (Kim et al., 1992) were included. RMSDs between initial-distance-refined structures derived from random-embedded DG, A-DNA, and B-DNA starting structures were all in the range 0.5-1.0 A, indicating good convergence properties of the algorithm, regardless of the starting structure. A semiautomatic back-calculation refinement procedure was developed and used to generate more refined structures for which the BKCALC-simulated NOE volumes matched the experimental data. The six final structures refined from various starting structures exhibit very good agreement with the experimental data (R values = 0.18) and converge well to within 0.8-A RMSD differences for the central 8 base pairs. The torsion and pseudorotation phase angles were found to be well determined by the data, and the local helical parameters for each base step converged quite well. The final structures show that the central T6-A7 step is somewhat underwound (twist angle ca. 29 degrees), with a large negative cup and a normal (wide) minor groove width, while the T5-T6 and A7-A8 steps have a partially narrowed minor groove.     

Raman spectroscopy study of the interaction between biogenic polyamines and an alternating AT oligodeoxyribonucleotide

The interaction between the 15-mer oligonucleotide d[A(TA)(7)].d[T(AT)(7)] and the three biogenic polyamines, putrescine, spermidine and spermine, under physiological conditions has been studied by Raman spectroscopy. Solutions containing 60 mM (phosphate) of the oligonucleotide and different polyamine concentrations ranging from 1 to 75 mM have been studied. Both natural and heavy water were used as solvents. Difference Raman spectra were computed by subtracting the sum of the separated component spectra from the experimental spectra of the complexes. The Raman data suggested that the interaction of biogenic polyamines with d[A(TA)(7)].d[T(AT)(7)] presents differences related with their sizes and electric charges. Preferential bindings through the oligonucleotide minor groove for putrescine and spermidine were proposed. Spermine would interact by both minor and major grooves, although interaction by the minor groove seems to be more favored. Main reactive sites were thymine-O2 and adenine-N3 atoms at the minor grooves and adenine-N7 and thymine-O4 at the major groove. Electrostatic attractions between the polyamine amino and oligonucleotide phosphodioxy groups were also proposed. Under our experimental conditions, no macromolecular effects on d[A(TA)(7)].d[T(AT)(7)] (changes on secondary or tertiary structures) were detected from Raman spectroscopy, contrary to what happened for GC sequences at the same experimental settings. This fact agrees with the role of the biogenic polyamines during the first steps of the macromolecular synthesis, which involve DNA opening in AT motifs.     

Hairpin Polyamides That use Parallel and Antiparallel Side-by-Side Peptide Motifs in Binding to DNA

Abstract

Pt-bis-netropsin is a synthetic sequence-specific DNA-binding ligand comprizing two netropsin-like fragments which are linked in a tail-to-tail manner via a cis-diammineplat-inum (II) residue. The CD studies and thermodynamic characterization of the DNA-binding properties exhibited by this compound reveal that it forms two types of complexes with poly[d(AT)]?poly[d(AT)] and DNA oligomers containing nucleotide sequences 5′-CC (TA)_nCC-3′, with n = 4, 5 and 6. The first type corresponds to the binding of Pt-bis-netropsin in the extended conformation and is characterized by the saturating ratio of one bound Pt-bis-netropsin molecule per 9 AT-base pairs. The second type of the complex corresponds to the binding of Pt-bis-netropsin to DNA in the folded hairpin form. The binding approaches saturation level when one Pt-bis-netropsin molecule is bound per four or five AT-base pairs. The hairpin form of Pt-bis-netropsin complex is built on the basis of parallel side-by-side peptide motif which is inserted in the minor DNA groove. The CD spectral profiles reflecting the binding of Pt-bis-netropsin in the hairpin form are different from those observed for binding of another bis-netropsin with the sequence Lys-Gly-Py-Py-Gly-Gly-Gly-Py-Py-Dp, where Py is a N-propylpyrrole amino acid residue and Dp is a dimethylaminopropylamino residue. The hairpin form of this bis-netropsin is formed on the basis of antiparallel side- by-side peptide motif. The CD spectra obtained for complexes of this polyamide in the hairpin form with poly[dAT)]?poly[d(AT)] exhibit positive CD band with a peak at 325 nm, whereas the CD spectral profiles for the second complex of Pt-bis-Nt with poly[d(AT)] ?poly[d(AT)] and short DNA oligomers have two intense positive CD bands near 290 nm and 328 nm. This reflects the fact that two bis-netropsins use different structural motifs on binding to DNA in the hairpin form.     

The crystal structure of the RNA/DNA hybrid r(GAAGAGAAGC). d(GCTTCTCTTC) shows significant differences to that found in solution.

The crystal structure of the RNA/DNA hybrid r(GAAGAGAAGC). d(GCTTCTCTTC) has been solved and refined at 2.5 A resolution. The refinement procedure converged at R = 0.181 for all reflections in the range 20.0-2.5 A. In the crystal, the RNA/DNA hybrid duplex has an A' conformation with all but one of the nucleotide sugar moieties adopting a C3'- endo (N) conformation. Both strands in the double helix adopt a global conformation close to the A-form and the width of the minor groove is typical of that found in the crystal structures of other A-form duplexes. However, differences are observed between the RNA and DNA strands that make up the hybrid at the local level. In the central portion of the duplex, the RNA strand has backbone alpha, beta and gamma torsion angles that alternate between the normal gauche -/ trans / gauche + conformation and an unusual trans / trans / trans conformation. Coupled with this so-called 'alpha/gamma flipping' of the backbone torsion angles, the distance between adjacent phosphorous atoms on the RNA strand systematically varies. Neither of these phenomena are observed on the DNA strand. The structure of the RNA/DNA hybrid presented here differs significantly from that found in solution for this and other sequences. Possible reasons for these differences and their implications for the current model of RNase H activity are discussed.     

Conformational and model-building studies of the hairpin form of the mismatched DNA octamer d(m5C-G-m5C-G-T-G-m5C-G)

The hairpin form of the mismatched octamer d(m5C-G-m5C-G-T-G-m5C-G) was studied by means of NMR spectroscopy. In a companion study it is shown that the hairpin form of this DNA fragment consists of a structure with a stem of three Watson-Crick-type base pairs and a loop consisting of only two nucleotides. The non-exchangeable proton resonances were assigned by means of two-dimensional correlation spectroscopy and two-dimensional nuclear Overhauser effect spectroscopy. Proton-proton coupling constants were used for the conformational analysis of the deoxyribose ring and for some of the backbone torsion angles. From the two-dimensional NMR spectra and the coupling-constant analysis it is concluded that: (i) the stem of the hairpin exhibits B-DNA characteristics; (ii) the sugar rings are not conformationally pure, but display a certain amount of conformational flexibility; (iii) the stacking interaction in the stem of the hairpin is elongated from the 3'-side in a more or less regular fashion with the two loop nucleotides; (iv) at the 5'-side of the stem a stacking discontinuity occurs between the stem and the loop; (v) at the 5'-side of the stem the loop is closed by means of a sharp backbone turn which involves unusual gamma' and beta+ torsion angles in residue dG(6). The NMR results led to the construction of a hairpin-loop model which was energy-minimized by means of a molecular-mechanics program. The results clearly show that a DNA hairpin-loop structure in which the loop consists of only two nucleotides bridging the minor groove in a straightforward fashion, (i) causes no undue steric strain, and (ii) involves well-known conformational principles throughout the course of the backbone. The hairpin form of the title compound is compared with the hairpin form of d(A-T-C-C-T-A-T4-T-A-G-G-A-T), in which the central -T4- part forms a loop of four nucleotides. Both models display similarities as far as stacking interactions are concerned.     

Binding of actinomycin D to [d(ATCGAT)]2: NMR evidence of multiple complexes

Actinomycin D (actD) binds to the oligonucleotide [d(ATCGAT)]2 with a hypochromatic and red-shifted visible absorbance band compared to free drug and a CD spectrum with double negative bands at 460 and 385 nm. These spectral features are similar to those of the actD-[d(ATGCAT)]2 complex, while actD-[d(AT)5]2 gives spectra similar to those of free drug. Upon dilution or raising the temperature, the spectral characteristics accompanying complex formation disappear in the actD-[(ATCGAT)]2 sample but remain in the actD-[d(ATGCAT)]2 complex under the same experimental conditions. These results suggest that (a) sequence-specific binding of actD occurs with [d(ATCGAT)]2 but not with [d(AT)5]2, (b) the binding is not as strong as with [d(ATGCAT)]2, and (c) actD binds [d(ATCGAT)]2 with the same mechanism as it binds [d(ATGCAT)]2, i.e., by intercalation. From NMR spectra of the actD-[d(ATCGAT)]2 complex, three types of signals can be detected below 20 degrees C, one major and two minor ones. At higher temperatures, exchange between the two minor ones becomes fast enough that only one type of minor signal was seen. Partial resonance assignments were made by using 2D nuclear Overhauser effect (NOE) and 2D homonuclear Hartmann-Hahn (HOHAHA) experiments. Proton chemical shift changes of the major complex are consistent with actD chromophore ring intercalation between hexamer base pairs. Data from NOE-detected dipolar interactions between actD and [d(ATCGAT)]2 protons were interpreted in terms of a major complex with the actD chromophore ring system intercalated at the CG position and minor complexes with the drug intercalated off center at the GA positions.(ABSTRACT TRUNCATED AT 250 WORDS)     

Bh-DNA: Variations of the Poly[d(A)] · Poly[d(T)] Structure within the Framework of the Fibre Diffraction Studies

Abstract

A refinement of the recent results for poly[d(A)] · poly[d(T)] (Alexeev et al., J. Biomol. Struct. Dyn. 4, 989 (1987)) involving additional parameters of the base-pair structure and of the sugar- phosphate backbone expands the conformational potential of this polynucleotide of the B type to include the possibility of bifurcated hydrogen bonds of the kind recently discovered in crystalline deoxyoligonucleotide with lone d(A)_n · d(T)_n stretch (Nelson et al., Nature 330, 221 (1987)).

Still, analysis of the available data and energy calculations do not seem to indicate that the bifurcated H-bonds are a crucial factor responsible for the anomalous structure of the d(A)_n · d(T)_n sequence. The unique structural properties of poly [d(A)] · poly[d(T)] can hardly be explained without taking into account its interactions with the double-layer hydration spine in the minor groove. In view of the hydration mechanism stabilizing poly [d(A)] · poly [d(T)] and of the polynucleotide's heteronomous prehistory (Arnott et al., Nucleic Acids Res. 11, 4141 (1983)) we suggest that this B-type structure be called B_h.     

Solution structure of the EcoRI DNA octamer containing 5-fluorouracil via restrained molecular dynamics using distance and torsion angle constraints extracted from NMR spectral simulations.

The self-complementary DNA octamer [d(GGAATUFCC)]2, containing the EcoRI recognition sequence with one of the thymines replaced by 5-fluorouracil (UF), was synthesized. Proton homonuclear two-dimensional nuclear Overhauser effect (2D NOE) and double-quantum-filtered correlation (2QF-COSY) spectra, as well as one-dimensional spectra at different temperatures, were recorded for the octamer. Consequently, all proton resonances were assigned. The thermally induced transition from the duplex to single strands has been followed, demonstrating the stability of the duplex containing 5-fluorouracil. Simulations of the 2QF-COSY cross-peaks by means of the programs SPHINX and LINSHA were compared with experimental data, establishing scalar coupling constants for the sugar ring protons and hence sugar pucker parameters. The deoxyribose rings exhibit a dynamic equilibrium of N- and S-type conformers with 75-95% populations of the latter. Two programs used for complete relaxation matrix analysis 2D NOE spectra, CORMA and MARDIGRAS, were modified to account for the influence of the fluorines on dipolar interactions in the proton system. Quantitative assessment of the 2D NOE cross-peak intensities for different mixing times, in conjunction with the program MARDIGRAS, gave a set of interproton distances for each mixing time. The largest and smallest values of each of the interproton distances were chosen as the upper and lower bounds for each distance constraint. The distance bounds define the size of a flat-well potential function term, incorporated into the AMBER force field, which was employed for restrained molecular dynamics calculations. Torsion angle constraints in the form of a flat-well potential were also constructed from the analysis of the sugar pucker data. Several restrained molecular dynamics runs of 35 ps were performed, utilizing 284 experimental distance and torsion angle constraints and two different starting structures, energy-minimized A- and B-DNA. Convergence to similar structures with a root-mean-square deviation of 1.2 A was achieved for the central hexamer of the octamer, starting from A- and B-DNA. The average structure from six different molecular dynamics runs was subjected to final restrained energy minimization. The resulting final structure was in good agreement with the structures derived from different molecular dynamics runs and showed a substantial improvement of the 2D NOE sixth-root residual index in comparison with classical and energy-minimized B-DNA. A detailed analysis of the conformation of the final structure and comparison with structures of similar sequences, obtained by different methods, were performed.     

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

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

Molecular structure of the netropsin-d(CGCGATATCGCG) complex: DNA conformation in an alternating AT segment

The molecular structure of the complex between a minor groove binding drug (netropsin) and the DNA dodecamer d(CGCGATATCGCG) has been solved and refined by single-crystal X-ray diffraction analysis to a final R factor of 20.0% to 2.4-A resolution. The crystal is similar to that of the other related dodecamers with unit cell dimensions of a = 25.48 A, b = 41.26 A, and c = 66.88 A in the space group P2(1)2(1)2(1). In the complex, netropsin binds to the central ATAT tetranucleotide segment in the narrow minor groove of the dodecamer B-DNA double helix as expected. However, in the structural refinement the drug is found to fit the electron density in two orientations equally well, suggesting the disordered model. This agrees with the results from solution studies (chemical footprinting and NMR) of the interactions between minor groove binding drugs (e.g., netropsin and distamycin A) and DNA. The stabilizing forces between drug and DNA are provided by a combination of ionic, van der Waals, and hydrogen-bonding interactions. No bifurcated hydrogen bond is found between netropsin and DNA in this complex due to the unique dispositions of the hydrogen-bond acceptors (N3 of adenine and O2 of thymine) on the floor of the DNA minor groove. Two of the four AT base pairs in the ATAT stretch have low propeller twist angles, even though the DNA has a narrow minor groove. Alternating helical twist angles are observed in the ATAT stretch with lower twist in the ApT steps than in the TpA step.     

Solution structure of a nitrous acid induced DNA interstrand cross-link

Nitrous acid is a mutagenic agent. It can induce interstrand cross-links in duplex DNA, preferentially at d(CpG) steps: two guanines on opposite strands are linked via a single shared exocyclic imino group. Recent synthetic advances have led to the production of large quantities of such structurally homogenous cross-linked duplex DNA. Here we present the high resolution solution structure of the cross-linked dodecamer [d(GCATCCGGATGC)]2 (the cross-linked guanines are underlined), determined by 2D NMR spectroscopy, distance geometry, restrained molecular dynamics and iterative NOE refinement. The cross-linked guanines form a nearly planar covalently linked 'G:G base pair' with only minor propeller twisting, while the cytidine bases of their normal base pairing partners have been flipped out of the helix and adopt well defined extrahelical positions in the minor groove. On the 5'-side of the cross-link, the minor groove is widened to accommodate these extrahelical bases, and the major groove becomes quite narrow at the cross-link. The cross-linked 'G:G base pair' is well stacked on the spatially adjacent C:G base pairs, particularly on the 3'-side guanines. In addition to providing the first structure of a nitrous acid cross-link in DNA, these studies could be of major importance to the understanding of the mechanisms of nitrous acid cross-linking and mutagenicity, as well as the mechanisms responsible for its repair in intracellular environments. It is also the shortest DNA cross-link structure to be described.     

Solution structure of the chromomycin-DNA complex

The structure of the chromomycin-DNA complex at the deoxyoctanucleotide duplex level has been determined from one- and two-dimensional proton NMR studies in Mg-containing aqueous solution. The NMR results demonstrate that the antitumor agent binds as a symmetrical dimer to the self-complementary d[T-T-G-G-C-C-A-A] duplex with retention of the 2-fold symmetry in the complex. A set of intermolecular nuclear Overhauser enhancements (NOEs) establishes that two chromomycin molecules in the dimer share the minor groove at the G-G-C-C.G-G-C-C segment in such a way that each hydrophilic edge of the chromophore is located next to the G-G.C-C half-site and each C-D-E trisaccharide chain extends toward the 3'-direction of the octanucleotide duplex. In addition, the A-B disaccharide segment and the hydrophilic side chain of the antitumor agent are directed toward the phosphate backbone. The observed changes in nucleic acid NOEs and coupling patterns on complex formation establish a transition to a wider and shallower minor groove at the central G-G-C-C.G-G-C-C segment required for accommodating the chromomycin dimer. The present demonstration that chromomycin binds as a dimer and switches the conformation of the DNA at its G.C-rich minor groove binding site provides new insights into antitumor agent design and the sequence specificity of antitumor agent-DNA recognition.