Neomycin, spermine and hexaamminecobalt (III) share common structural motifs in converting B- to A-DNA.

The (dG)n.(dC)n-containing 34mer DNA duplex [d(A2G15C15T2)]2 can be effectively converted from the B-DNA to the A-DNA conformation by neomycin, spermine and Co(NH3)6(3+). Conversion is demonstrated by a characteristic red shift in the circular dichroism spectra and dramatic NMR spectral changes in chemical shifts. Additional support comes from the substantially stronger CH6/GH8-H3'NOE intensities of the ligand-DNA complexes than those from the native DNA duplex. Such changes are consistent with a deoxyribose pucker transition from the predominate C2'-endo (S-type) to the C3'-endo (N-type). The changes for all three ligand-DNA complexes are identical, suggesting that those three complex cations share common structural motifs for the B- to A-DNA conversion. The A-DNA structure of the 4:1 complex of Co(NH3)6(3+)/d(ACCCGCGGGT) has been analyzed by NOE-restrained refinement. The structural basis of the transition may be related to the closeness of the two negatively charged sugar-phosphate backbones along the major groove in A-DNA, which can be effectively neutralized by the multivalent positively charged amine functions of these ligands. In addition, ligands like spermine or Co(NH3)6(3+) can adhere to guanine bases in the deep major groove of the double helix, as is evident from the significant direct NOE cross-peaks from the protons of Co(NH3)6(3+) to GH8, GH1 (imino) and CH4 (amino) protons. Our results point to future directions in preparing more potent derivatives of Co(NH3)6(3+) for RNA binding or the induction of A-DNA.     

Study of DNA-deltamethrin binding by voltammetry, competitive fluorescence, thermal denaturation, circular dichroism, and atomic force microscopy techniques

The interaction of deltamethrin (DM), a synthetic insecticide, with calf thymus DNA was studied. The cyclic voltammetric (CV) results revealed that DM has two irreversible cathodic peaks. The first peak (a) was devoted to reduction of -CN by 4 electrons and the second peak (b) was devoted to reduction of the -C = C- moiety by two electrons. By using non-linear regression analysis of CV data of peak (a), the binding constant, binding site size, and diffusion coefficient for free DM (D(f)) and DNA-DM (D(b)) were calculated as: 2.6 × 10(4), 1.6, 3.2 × 10(-4)Cm(2) S(-1), and 8.5 × 10(-6)Cm(2) S(-1), respectively. The thermal denaturation, competitive fluorescence, and AFM results revealed that the mode of interaction may be non-intercalative. Also the circular dichroism spectra showed that the conformation of CT DNA was converted from right-handed B-DNA to A-DNA due to the destacking of the adjacent guanine bases in pH 7.3 solution.     

Influence of counter-ions on the crystal structures of DNA decamers: binding of [Co(NH3)6]3+ and Ba2+ to A-DNA.

A-DNA is a stable alternative right-handed double helix that is favored by certain sequences (e.g., (dG)n.(dC)n) or under low humidity conditions. Earlier A-DNA structures of several DNA oligonucleotides and RNA.DNA chimeras have revealed some conformational variation that may be the result of sequence-dependent effects or crystal packing forces. In this study, four crystal structures of three decamer oligonucleotides, d(ACCGGCCGGT), d(ACCCGCGGGT), and r(GC)d(GTATACGC) in two crystal forms (either the P6(1)22 or the P2(1)2(1)2(1) space group) have been analyzed at high resolution to provide the molecular basis of the structural difference in an experimentally consistent manner. The study reveals that molecules crystallized in the same space group have a more similar A-DNA conformation, whereas the same molecule crystallized in different space groups has different (local) conformations. This suggests that even though the local structure is influenced by the crystal packing environments, the DNA molecule adjusts to adopt an overall conformation close to canonical A-DNA. For example, the six independent CpG steps in these four structures have different base-base stacking patterns, with their helical twist angles (omega) ranging from 28 degrees to 37 degrees. Our study further reveals the structural impact of different counter-ions on the A-DNA conformers. [Co(NH3)6]3+ has three unique A-DNA binding modes. One binds at the major groove side of a GpG step at the O6/N7 sites of guanine bases via hydrogen bonds. The other two modes involve the binding of ions to phosphates, either bridging across the narrow major groove or binding between two intra-strand adjacent phosphates. Those interactions may explain the recent spectroscopic and NMR observations that [Co(NH3)6]3+ is effective in inducing the B- to A-DNA transition for DNA with (G)n sequence. Interestingly, Ba2+ binds to the same O6/N7 sites on guanine by direct coordinations.     

Linear dichroism characteristics of ethidium-and proflavine-supercoiled DNA complexes

A flow linear dichroism technique is utilized to study the unwinding of supercoiled DNA induced by the binding of ethidium bromide (EB) and proflavine (PF) at different ratios r (drug added/DNA base). In the case of either EB or PF bound to linear calf thymus DNA, the reduced linear dichroism signals LD/A (LD: linear dichroism; A: absorbance, both measured at the same wavelength), determined at 258, and 520 or 462 nm (corresponding to contributions predominantly from the partially oriented DNA bases, intercalated EB, or PF, respectively) are nearly independent of drug concentration. In the case of supercoiled DNA, the magnitude of LD/A at 258 nm first increases to a maximum value near r = 0.04-0.05, and then decreases as r is increased further, mimicking the behavior of the sedimentation coefficients, viscosities, and gel electrophoresis patterns measured by other workers at similar values of r. However, LD/A at 520 nm, which is due to DNA-bound EB molecules, is constant within the range of r values of 0.02-0.06 in which the magnitude of LD/A determined at 258 nm due to the DNA bases exhibits a pronounced maximum. In contrast, in the case of PF, the magnitudes of LD/A determined at 258 or 462 nm are characterized by similar dependencies on r, both exhibiting pronounced maxima at r = 0.05; this parallel behavior is expected according to a simple intercalation model in which the DNA bases and drug molecules are stacked on top of one another, and in which both are oriented to similar extents in the flow gradient. The unexpected differences in the dependencies of (LD/A)258 and (LD/A)520 on r in the case of EB bound to supercoiled DNA, are attributed to differences in the net overall alignment of the EB molecules and DNA bases in the flow gradient. The magnitude of the LD signal at 258 nm reflects the overall degree of orientation of the supercoiled DNA molecules that, in turn, depends on their hydrodynamic shapes and sizes; the LD signals characterizing the bound EB molecules may reflect this orientation also, as well as the partial alignment of individual DNA segments containing bound EB molecules.(ABSTRACT TRUNCATED AT 400 WORDS)     

The complex of ethidium bromide with genomic DNA: structure analysis by polarized Raman spectroscopy

Structural properties of the complex formed between genomic DNA and the intercalating drug ethidium bromide (EtBr) have been determined by use of a Raman microscope equipped with near-infrared laser excitation. The polarized spectra, which were obtained from oriented fibers of the EtBr:DNA complex, are interpreted in terms of the relative orientations of the phenanthridinium ring of EtBr and bases of DNA. Quantification of structure parameters of EtBr and DNA in the complex were assessed using Raman tensors obtained from polarized Raman analyses of oriented specimens of EtBr (single crystal) and DNA (hydrated fiber). We find that the phenanthridinium plane is tilted by 35+/-5 degrees from the plane perpendicular to the fiber (DNA helix) axis. Assuming coplanarity of the phenanthridinium ring and its immediate base neighbors at the intercalation site, such bases would have a tilt angle closer to that of A-DNA (20 degrees) than to that of B-DNA (6 degrees). The average base tilt in stretches of DNA between intercalation sites remains that of B-DNA.     

Conformational variations in d(TGACGTCA) and its reverse sequence d(ACTGCAGT): a joint circular dichroism and nuclear magnetic resonance study

Circular dichroism (CD) and nuclear magnetic resonance (NMR) techniques have been used to characterize the structural properties of the two self-complementary DNA octamers d(TGACGTCA) (I) and d(ACTGCAGT) (II). These display as distinctive features reverse sequences and central steps CpG and GpC, respectively. CD experiments lead to B-form DNA spectra characterized by larger magnitude signals in the case of octamer (I). NMR COSY spectra indicate that in the two octamers all the residues are predominantly south, S, (2'-endo) sugar conformation. NMR NOESY spectra show most of the glycosidic angles confined in the range predicted for B-form DNA although important heterogeneity is noticed along the chains, more pronounced in the case of octamer (I). Both the increase of north, N, (3'-endo) sugar conformation and P (pseudorotation phase angle) deviation from its standard B-form DNA value (162 degrees) express local sequence dependent structure distortions, remarkably visible in CpG step of octamer (I) and agreeing with NOESY cross-peaks intensities. Results interpreted according to Calladine's rules indicate higher cross-chain strains in octamer (I) than in octamer (II). All together, we find evidence to support for octamer (I) in solution local structures with A-DNA properties likely dictated by the central CpG step. Such structures could be involved in the DNA recognition by proteins and anticancerous drugs.     

Conformational transition within the A-form of complementary nucleic acids in solution]

Circular dichroic spectra of A-DNA in 78% ethanol and of tRNA in water and ethanol solutions have been studied at different concentrations of NaCl. An increase in the Na+ concentration from 0.5.10(-4) M to 5.10(-4) M results in a shift of the positive CD band at 264 nm of the A-DNA to a longer wavelength, 272 nm. Simultaneously, the magnitude of the 210 nm band decreases. By contrast in the case of tRNA in water solution an increase in NaCl content results in straight opposite shifts of the CD spectra. This opposite behaviour is shown to the due to a difference in ions effects in water and water-ethanol solutions, since tRNA in the ethanol solution behaves in the same way as A-DNA does in 78% ethanol. We suppose that in aqueous solution in increase in the cation concentration would stabilize the helical conformations with progressively decreasing narrow groove, i. e. more wound. At a high concentration of ethanol (60--80%) the formation of specific complex between the hydrated cations and the double-stranded regions should be taken into consideration. Thus, the hydrated cations may insert into the deep groove exerting the opposite effect of unwinding.     

The B-A transition in superhelical DNA.

Relaxation of a DNA superhelical stress due to the B to A transition induced by trifluoroethanol has been studied by assessing the change of DNA orientation in a flow gradient. Using DNAs of different superhelical densities, a decrease in the winding angle during the B----A shift of DNA was found to be 1.5 degrees per base pair in solution. Accepting the winding angle for B-DNA in solution to be 34.1 degrees, that for A-DNA must have a value of 32.6 degrees which agrees with the X-ray data for A-DNA in the condensed state. The date obtained within the B-A transition interval make it possible to conclude that there is an increase in winding at each B/A junction, which is about 5 degrees per one junction.     

Base only binding of spermine in the deep groove of the A-DNA octamer d(GTGTACAC)

The crystal structure of a complex of spermine with the DNA octamer d(GTGTACAC) has been determined at 2.0-A resolution. The alternating sequence adopts an A-DNA conformation with a novel purine-purine extra-Watson-Crick hydrogen bond involving the central guanine G3 (G11) and adenine A13 (A5) in the deep groove. The oligocation spermine binds in the floor of the deep groove by interacting with the bases and assumes an S-shape. Its dyad is coincident with that of the DNA, reminiscent of repressor binding to B-DNA. The terminal and central ammonium groups of the top half of spermine form hydrogen-bonding interactions to the 5'-bases, GTG, of one strand; then the spermine winds across the groove to interact with the corresponding set of bases on the other strand. The methylene groups of spermine form a hydrophobic cluster with the methyl groups of the thymines and the O6 atoms of the guanines of the TGT sequences on either side of the dyad. The observed mode of binding of spermine to A-DNA can serve as a model for deep groove binding in RNA and DNA-RNA hybrids that show a propensity also for the A-conformation. It will be of interest to see if base binding of spermine to DNA is involved in the regulation of gene expression, since spermine and other oligocations are ubiquitous in cells and their concentration is coupled to stages in cell cycle.     

Matrix-method calculation of linear and circular dichroism spectra of nucleic acids and polynucleotides

Calculations of the optical properties (absorption, linear dichroism, circular dichroism, and anisotropic components of the CD) are presented for polynucleotides of random or regular sequence within the formalism of the matrix method using a set of parameters that includes only the ππ* transitions of the aromatic bases. Experimental solution spectra agree favorably with calculated CD spectra for A-RNA, A-DNA, and B-DNA, when coordinates derived from x-ray studies on fibers are used. Excessive hypochromicity is predicted when parameters intended to reproduce the vacuum-uv absorption of the chromophores are included in the calculations, but total elimination of these parameters leads to an insufficient hypochromicity for the long-wavelength absorption band. Using alternative conformations for DNA in low-salt aqueous solution did not improve the agreement between experimental and calculated spectra, but some features of the optical properties predicted for these variant structures suggest that the tilt of the bases with respect to the helical axis may be larger than that of the fiber B-form. In the case of polynucleotides with regular structure, which have been traditionally less easy to understand in terms of the standard nucleic acid conformations, a series of alternative structures has been examined. Unexpectedly, the calculated spectrum for the Z-DNA structure compares almost quantitatively with the experimental spectrum of poly(dGC·dGC) in low salt. This result, which confirms a recent report [Vasmel, H. & Greve, J. (1981) Biopolymers 20 , 1329–1332], is in contrast with the current identification of Z-DNA with the high-salt form of poly(dGC·dGC). Finally, the optical properties of single-stranded polyribonucleotides appear to be better explained when alternative structures [9₁-helix for poly(rA) and 6₁-helix for poly(rC)] are introduced instead of the A-RNA form.     

The extended and eccentric E-DNA structure induced by cytosine methylation or bromination

Cytosine methylation or bromination of the DNA sequence d(GGCGCC)2 is shown here to induce a novel extended and eccentric double helix, which we call E-DNA. Like B-DNA, E-DNA has a long helical rise and bases perpendicular to the helix axis. However, the 3'-endo sugar conformation gives the characteristic deep major groove and shallow minor groove of A-DNA. Also, if allowed to crystallize for a period of time longer than that yielding E-DNA, the methylated sequence forms standard A-DNA, suggesting that E-DNA is a kinetically trapped intermediate in the transition to A-DNA. Thus, the structures presented here chart a crystallographic pathway from B-DNA to A-DNA through the E-DNA intermediate in a single sequence. The E-DNA surface is highly accessible to solvent, with waters in the major groove sitting on exposed faces of the stacked nucleotides. We suggest that the geometry of the waters and the stacked base pairs would promote the spontaneous deamination of 5-methylcytosine in the transition mutation of dm5C-dG to dT-dA base pairs.     

Base tilt of DNA in various conformations from flow linear dichroism

We have measured the isotropic absorption (Aiso) and linear dichroism (LD) of Escherichia coli DNA in 0.01 M Na+ (10.4 base pairs per turn of B form), 5.5 M NH4F (10.2 base pairs per turn of B form), and 80% trifluoroethanol (A form) into the vacuum UV spectral region. The reduced dichroism spectrum (LD divided by Aiso) of DNA in the A conformation differed from those of the B conformations, demonstrating that LD is a sensitive method for distinguishing DNA conformation. The reduced dichroism spectra of the B conformations were similar, indicating little change in the orientation of the bases for DNA in high salt. The wavelength dependence of the reduced dichroism indicates that the angle between the base planes and the helix axis is less than 76 degrees for all three conformations of DNA.     

A note on sequence-dependence of DNA structure

A circular dichroism study was conducted on the solution structure of several different oligonucleotides, whose X-ray structures have been solved. It is suggested that in aqueous solution the oligonucleotides can form structures that maintain geometrical elements which are typical of B-DNA, A-DNA, and their intermediate forms. It is shown that 5'GGATGGGAG:5'CTCCCATCC, which forms an A-DNA helix in the crystal state (McCall et al. 1986), in aqueous solution maintains an A-DNA like structure at temperatures below 10 degrees C. At temperatures between 10 degrees C and 25 degrees C it shows a tendency to form an intermediate structure between A-DNA and B-DNA. Also, it is shown that TFE does not cause a transition from B-DNA to A-DNA helix in short DNA fragments, but instead disrupts the helix.     

Circular dichroism of flow-oriented nucleic acids. II. Comparison between observed and calculated spectra.

The ultraviolet circular dichroism (CD) of oriented DNA and RNA molecules is calculated by an extension of Johnson and Tinoco's theory [(1969) Biopolymers 7 , 727–749] for unoriented molecules. The calculations are carried out for molecular models of A-DNA, B-DNA, planar B-DNA, C-DNA, and RNA-11-α. The calculated curves are compared to measured spectra [(1975) J. Mol. Biol. 92 , 449–466] Chung and Holzwarth, for oriented solutions of DNA in buffer, DNA in 6 M LiCl or in ethylene glycol, and double-stranded viral RNA. The calculation, which considers only base–base interactions, predicts that the CD of B-DNA, measured with light propagating parallel to the helix axis, should be large and semiconservative, whereas the CD for light propagating perpendicular to the helix axis should be nonconservative. These predictions agree qualitatively with the experimental observations for DNA in buffer; agreement improves if one assumes the bases to be exactly perpendicular to the helix axis. For the other geometries, agreement is less satisfactory, but qualitative agreement with experiment is obtained and the signs of the specific CD spectra are in accord with observations.     

Binding of recA protein to Z-form DNA studied with circular and linear dichroism spectroscopy

Binding of RecA to poly(dG-m5dC) and poly(dG-dC) under B- and Z-form conditions was studied using circular dichroism (CD) and linear dichroism (LD). LD revealed a quantitative binding of RecA to Mg2+-induced Z-form poly(dG-m5dC) with a stoichiometry of 3.1 base pairs/RecA monomer, which is slightly larger than the 2.7 base pairs observed for the B-form. The LD spectra indicate a preferentially perpendicular orientation of DNA bases and a rather parallel orientation of the tryptophan residues relative to the fiber axis in both complexes. The association rate of RecA to Z-form DNA was found to be slower than to B-form. CD measurements showed that the polynucleotide conformation is retained upon RecA binding, and CD and LD confirm that RecA binds to both forms of DNA. The Mg2+-induced Z-form is shown to be retransformed into B-form, both in free and in RecA-complexed polynucleotides by addition of NaCl, whereas the B----Z transition cannot be induced by addition of Mg2+ when the polynucleotide is complexed with RecA. From this it is inferred that RecA does not stabilize the Z-conformation of the polynucleotide but that it can kinetically "freeze" the polynucleotide in its B-conformation. On all essential points, the same conclusions were also reached in a corresponding study of unmethylated poly(dG-dC) with the Z-form induced by Mn2+.     

Characterization of DNA structures by laser Raman spectroscopy

Oriented fibers drawn from aqueous gels of calf-thymus DNA were maintained at constant relative humidites of 75 and 92% to yield canonical A-DNA and B-DNA structures, respectively. Raman spectra of the two forms of DNA were recorded over the spectral range 300–4000 cm^?1. The authenticated DNA fibers were deuterated in hygrostatic cells containing D₂O at appropriate relative humidities, and the corresponding spectra of deuterated DNAs were also obtained. The spectra reveal all of the Raman scattering frequencies and intensities characteristic of A- and B-DNA structures in both nondeuterated and deuterated froms, as well as the frequencies and intensities of adsorbed solvent molecules from which the hydration content of DNA fibers can be calculated. Numerous conformation-sensitive vibrational modes of DNA bases and phosphate groups have been identified throughout the 300–1700-cm^?1 interval. Evidence has also been obtained for conformation sensitivity of deoxyribosyl CH stretching modes in the 2800–3000-cm^?1 region. Raman lines of both the backbone and the bases are proposed as convenient indicators of A- and B-DNA structures. The results are extended to Z-DNA models investigated previously. Some implications of these findings for the determination of DNA or RNA structure from Raman spectra of nucleoproteins and viruses are considered.     

Hydration and recognition of methylated CpG steps in DNA.

The analysis of the hydration pattern around methylated CpG steps in three high resolution (1.7, 2.15 and 2.2 A) crystal structures of A-DNA decamers reveals that the methyl groups of cytosine residues are well hydrated. In comparing the native structure with two structurally distinct forms of the decamer d(CCGCCGGCGG) fully methylated at its CpG steps, this study shows also that in certain structural and sequence contexts, the methylated cytosine base can be more hydrated that the unmodified one. These water molecules seem to be stabilized in front of the methyl group through the formation C-H...O interactions. In addition, these structures provide the first observation of magnesium cations bound to the major groove of A-DNA and reveal two distinct modes of metal binding in methylated and native duplexes. These findings suggest that methylated cytosine bases could be recognized by protein or DNA polar residues through their tightly bound water molecules.     

Crystal and solution structures of the B-DNA dodecamer d(CGCAAATTTGCG) probed by Raman spectroscopy: heterogeneity in the crystal structure does not persist in the solution structure

The self-complementary dodecamer d(CGCAAATTTGCG) crystallizes as a double helix of the B form and manifests a Raman spectrum with features not observed in Raman spectra of either DNA solutions or wet DNA fibers. A number of Raman bands are assigned to specific nucleoside sugar and phosphodiester conformations associated with this model B-DNA crystal structure. The Raman bands proposed as markers of the crystalline B-DNA structure are compared and contrasted with previously proposed markers of Z-DNA and A-DNA crystals. The results indicate that the three canonical forms of DNA can be readily distinguished by Raman spectroscopy. However, unlike Z-DNA and A-DNA, which retain their characteristic Raman fingerprints in aqueous solution, the B-DNA Raman spectrum is not completely conserved between crystal and solution states. The Raman spectra reveal greater heterogeneity of nucleoside conformations (sugar puckers) in the DNA molecules of the crystal structure than in those of the solution structure. The results are consistent with conversion of one-third of the dG residues from the C2'-endo/anti conformation in the solution structure to another conformation, deduced to be C1'-exo/anti, in the crystal. The dodecamer crystal also exhibits unusually broad Raman bands at 790 and 820 cm-1, associated with the geometry of the phosphodiester backbone and indicating a wider range of (alpha, zeta) backbone torsion angles in the crystal than in the solution structure. The results suggest that backbone torsion angles in the CGC and GCG sequences, which flank the central AAATTT sequence, are significantly different for crystal and solution structures, the former containing the greater diversity.(ABSTRACT TRUNCATED AT 250 WORDS)