AT base pairs are less stable than GC base pairs in Z-DNA: The crystal structure of d(m5CGTAm5CG)

Two hexanucleoside pentaphosphates, 5-methyl and 5-bromo cytosine derivatives of d(CpGpTp-ApCpG) have been synthesized, crystallized, and their three-dimensional structure solved. They both form left-handed Z-DNA and the methylated derivative has been refined to 1.2 Å resolution. These are the first crystal Z-DNA structures that contain AT base pairs. The overall form of the molecule is very similar to that of the unmethylated or the fully methylated (dC-dG)₃ hexamer although there are slight changes in base stacking. However, significant differences are found in the hydration of the helical groove. When GC base pairs are present, the helical groove is systematically filled with two water molecules per base pair hydrogen bonded to the bases. Both of these water molecules are not seen in the electron density map in the segments of the helix containing AT base pairs, probably because of solvent disorder. This could be one of the features that makes AT base pairs form Z-DNA less readily than GC base pairs.     

Crystal structure of a Z-DNA fragment containing thymine/2-aminoadenine base pairs

The Z-DNA structure has been shown to form in two crystals made from self-complementary DNA hexamers d(CGTDCG) and d(CDCGTG) which contain thymine/2-aminoadenine (TD) base pairs. The latter structure has been solved and refined to 1.3 A resolution and it shows only small conformational changes due to the introduction of the TD base pairs in comparison with the structure of d(CG)3. Spectroscopic studies with these compounds demonstrate that DNA molecules containing 2-aminoadenine residues form Z-DNA slightly more easily than do those containing adenine nucleotides, but not as readily as the parent sequence containing only guanine-cytosine base pairs.     

Crystal structure of a Z-DNA hexamer d(CGCICG) at 1.7 A resolution: inosine.cytidine base-pairing, and comparison with other Z-DNA structures.

The crystal structure of the deoxyhexamer, d(CGCICG), has been determined and refined to a resolution of 1.7A. The DNA hexamer crystallises in space group P2(1)2(1)2(1) with unit cell dimensions of a = 18.412 +/- .017 A, b = 30.485 +/- .036A, and c = 43.318 +/- .024 A. The structure has been solved by rotation and translation searches and refined to an R-factor of 0.148 using 2678 unique reflections greater than 1.0 sigma (F) between 10.0-1.7 A resolution. Although the crystal parameters are similar to several previously reported Z-DNA hexamers, this inosine containing Z-DNA differs in the relative orientation, position, and crystal packing interactions compared to d(CGCGCG) DNA. Many of these differences in the inosine form of Z-DNA can be explained by crystal packing interactions, which are responsible for distortions of the duplex at different locations. The most noteworthy features of the inosine form of Z-DNA as a result of such distortions are: (1) sugar puckers for the inosines are of C4'-exo type, (2) all phosphates have the Zl conformation, and (3) narrower minor grove and compression along the helical axis compared to d(CGCGCG) DNA. In addition, the substitution of guanosine by inosine appears to have resulted in Watson-Crick type base-pairing between inosine and cytidine with a potential bifurcated hydrogen bond between inosine N1 and cytidine N3 (2.9 A) and O2 (3.3-3.A).     

Crystal structure of d(GCGAAAGCT) containing a parallel-stranded duplex with homo base pairs and an anti-parallel duplex with Watson-Crick base pairs

A DNA fragment d(GCGAAAGCT), known to adopt a stable mini-hairpin structure in solution, has been crystallized in the space group I4₁22 with the unit-cell dimensions a = b = 53.4 Å and c = 54.0 Å, and the crystal structure has been determined at 2.5 Å resolution. The four nucleotide residues CGAA of the first half of the oligomer form a parallel duplex with another half through the homo base pairs, C₂:C₂⁺ (singly-protonated between the Watson– Crick sites), G₃:G₃ (between the minor groove sites), A₄:A₄ (between the major groove sites) and A₅:A₅ (between the Watson–Crick sites). The two strands remaining in the half of the parallel duplex are split away in different directions, and they pair in an anti-parallel B-form duplex with the second half extending from a neighboring parallel duplex, so that an infinite column is formed in a head-to-tail fashion along the c-axis. It seems that a hexa-ammine cobalt cation supports such a branched and bent conformation of the oligomer. One end of the parallel duplex is stacked on the corresponding end of the adjacent parallel duplex; between them, the guanine base of the first residue is stacked on the fourth ribose of another duplex.     

The intrinsic structure and stability of out-of-alternation base pairs in Z-DNA.

Alternating pyrimidine-purine sequences typically form Z-DNA, with the pyrimidines in the anti and purines in the syn conformations. The observation that dC and dT nucleotides can also adopt the syn conformation (i.e. the nucleotides are out-of-alternation) extends the range of sequences that can convert to this left-handed form of DNA. Here, we study the effects of placing two adjacent d(G*C) base pairs as opposed to a single d(G*C) base pair or two d(A*T) base pairs out-of-alternation by comparing the structure of d(m5CGGCm5CG)2with the previously published structures of d(m5CGGGm5CG)*d(m5CGCCm5CG) and d(m5CGATm5CG)2. A high buckle and loss of stacking interactions are observed as intrinsic properties of the out-of-alternation base pairs regardless of sequence and the context of the dinucleotide. From solution titrations, we find that the destabilizing effect of out-of-alternation d(G*C) base pairs are identical whether these base pairs are adjacent or isolated. We can therefore conclude that it is these intrinsic distortions in the structure of the base pairs and not neighboring effects that account for the inability of out-of-alternation base pairs to adopt the left-handed Z conformation.     

Conformations in crystals and solutions of d(CACGTG), d(CCGCGG) and d(GGCGCC) studied by vibrational spectroscopy.

Crystals of self complementary DNA hexamers d(CACGTG), d(CCGCGG) and d(GGCGCC) were grown by vapour diffusion technique and studied by microRaman and microIR spectroscopies. The oligonucleotides were studied in parallel in solution by vibrational spectroscopy. A B- greater than Z transition was detected by Raman spectroscopy during the crystallization process for d(CACGTG). Vibrational spectroscopy shows that the d(GGCGCC) crystals adopt a B geometry. On the contrary the d(CCGCGG) sequence which is shown to be able to undergo in solution or in films quite easily the B- greater than Z transition, remains trapped in crystals in a geometry which may correspond to an intermediate conformation often proposed in models of the B- greater than Z transition. The crystals used in this study were characterized by X-ray diffraction. The unit cell and space group have been determined.     

Effects of 5-fluorouracil/guanine wobble base pairs in Z-DNA: molecular and crystal structure of d(CGCGFG).

The chemotherapeutic agent 5-fluorouracil is a DNA base analogue which is known to incorporate into DNA in vivo. We have solved the structure of the oligonucleotide d(CGCGFG), where F is 5-fluorouracil (5FU). The DNA hexamer crystallizes in the Z-DNA conformation at two pH values with the 5FU forming a wobble base pair with guanine in both crystal forms. No evidence of the enol or ionized form of 5FU is found under either condition. The crystals diffracted X-rays to a resolution of 1.5 A and their structures have been refined to R-factors of 20.0% and 17.2%, respectively, for the pH = 7.0 and pH = 9.0 forms. By comparing this structure to that of d(CGCGCG) and d(CGCGTG), we were able to demonstrate that the backbone conformation of d(CGCGFG) is similar to that of the archetypal Z-DNA. The two F-G wobble base pairs in the duplex are structurally similar to the T-G base pairs both with respect to the DNA helix itself and its interactions with solvent molecules. In both cases water molecules associated with the wobble base pairs bridge between the bases and stabilize the structure. The fluorine in the 5FU base is hydrophobic and is not hydrogen bonded to any solvent molecules.     

Energetics of Z-DNA formation in poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T).

The conformational change for the alternating purine-pyrimidine polydeoxyribonucleotides i.e. poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T) from a right-handed conformation at room temperature to the left-handed Z-DNA like double helix at elevated temperatures has been studied by UV spectroscopy, Raman spectroscopy, and by adiabatic differential scanning microcalorimetry (DSC) in the presence of Na+ and Mg2+ or Ni2+ respectively as counterions. The differential UV spectra reveal through a hyperchromic shift at around 280nm and a hypochromic shift at 260nm that a conformational change to the left-handed conformation occurs. The Raman spectra clearly show characteristic changes, a drastic decrease of the band at 680cm-1 and the appearance of a new band at 628cm-1, due to the change of the purine bases to the syn conformation upon inversion of the helix-handedness. The course of the transition as function of temperature can be followed quantitatively by plotting the change in the excess heat capacity vs. temperature. The transition enthalpy delta H for the B- to Z-DNA transition per mole base pairs (mbp) amounts to 2.0 +/- 0.2kcal for poly d(G-C), to 4.0 +/- 0.4kcal for poly d(A-T), and to 3.1 +/- 0.3kcal for poly d(A-C) poly d(G-T). The enthalpy change due to the Z-DNA to coil transitions (per mole base pairs) amounts to 11kcal for poly d(G-C), 10.5kcal for poly d(A-T) and 11.3kcal for poly d(A-C) poly d(G-T).     

Structure of a pleiomeric form of poly d(AT):poly d(AT)

A chemically simple polynucleotide duplex, poly d(AT):poly d(AT), has been trapped in a fibrous form with a complex helical secondary structure with a large (7.4 nm) axial repeat 24 nucleotides long. The motif which is repeated by the symmetry elements is a hexanucleotide in which two residues (both TpA) have the less common gauche minus conformation at C3'-O3' and consequently distinctive phosphate orientations. This reinforces earlier conclusions that PypPu nucleotides tend to have different shapes from PupPy nucleotides and that DNA surfaces may signal what base sequences lie beneath them. The morphological differences between this pleiomeric DNA polymer and closely-related, but more symmetrical allomorphs are just as great as those observed in short DNA fragments in crystals.     

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

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

"Asymmetric" opening reaction mechanism of Z-DNA base pairs: a hydrogen exchange study

With the tritium-Sephadex method, the hydrogen-exchange kinetics of the five NH protons of guanine and cytosine residues in Z-form poly(dG-dC) X poly (dG-dC) were measured as a function of temperature and catalyst concentration. Over the measured temperature range from 0 to 34 degrees C, two classes of protons with constant amplitudes are found. The three protons of the fast class, which were assigned to the guanine amino and imino protons, have an exchange half-time in the minute time range (at 20 degrees C the half-time is 2.5 min) and an activation energy of 18 kcal mol-1. Since these two types of protons exchange at the same rate in spite of their grossly different pK values, the exchange of these protons must be limited by the same nucleic acid conformational change. The two cytosine amino protons of the slow class are especially slow with exchange half-times in the hour time range (at 20 degrees C the exchange half-time is 1 h) and the activation energy is 20 kcal mol-1. The exchange of these two protons is not limited by some nucleic acid conformational change as shown by the marked exchange acceleration of these protons upon addition of 0.2 M imidazole. In addition, we have also reexamined the hydrogen-deuterium exchange kinetics of the amino protons of guanosine cyclic 2',3'-monophosphate by a spectral difference method using a stopped-flow spectrophotometer. The measured kinetic process is monophasic with a rate constant of 3 s-1 at 20 degrees C, which is in the same range as the predicted rate constant of the guanine amino protons.(ABSTRACT TRUNCATED AT 250 WORDS)     

Temperature-dependent molecular dynamics and restrained X-ray refinement simulations of a Z-DNA hexamer

Molecular dynamics simulations of the Z-DNA hexamer 5BrdC-dG-5BrdC-dG-5BrdC-dG were performed at several temperatures between 100 K and 300 K. Above 250 K, a strong sequence-dependent flexibility in the nucleic acid is observed, with the guanine sugar and the phosphate of GpC sequences much more mobile than the cytosine sugar and phosphate of CpG sequences. At 300 K, the hexamer is in dynamic equilibrium between several Z forms, including the crystallographically determined ZI and ZII forms. The local base-pair geometry, however, is not very variable, except for the roll of the base-pairs. The hexamer molecular dynamics trajectories have been used to test the restrained parameter crystallographic refinement model for nucleic acids. X-ray diffraction intensities corresponding to observed diffraction data were computed. The average structures obtained from the simulations were then refined against the calculated intensities, using a restrained least-squares program developed for nucleic acids in order to analyse the effects of the refinement model on the derived quantities. In general, the temperature dependence of the atomic fluctuations determined directly from the refined Debye-Waller factors is in reasonably good agreement with the results obtained by calculating the atomic fluctuations directly from the Z-DNA molecular dynamics trajectories. The agreement is best for refinement of temperature factors without restraints. At the highest temperature studied (300 K), the effect of the refinement on the most mobile atoms (phosphates) is to significantly reduce the mean-square atomic fluctuations estimated from the refined Debye-Waller factors below the actual values (less than (delta r)2 greater than congruent to 0.5 A2). Analysis of the temperature-dependence of the mean-square atomic fluctuations provides information concerning the conformational potential within which the atoms move. The calculated temperature-dependence and anharmonicity of the Z-DNA helix are compared with the results observed for proteins. The average structures from the simulations were refined against the experimental X-ray intensities. It is found that low-temperature molecular dynamics simulations provide a useful tool for optimizing the refinement of X-ray structures.     

Dissociation kinetics of 19 base paired oligonucleotide-DNA duplexes containing different single mismatched base pairs.

The dissociation kinetics of 19 base paired oligonucleotide-DNA duplex containing a various single mismatched base pair are studied on dried agarose gels. The kinetics of the dissociation are first order under our experimental conditions. The incorporation of a single mismatched base pair destabilizes the DNA duplexes to some extent, the amount depending on the nature of the mismatched base pair. G-T and G-A mismatches slightly destabilize a duplex, while A-A, T-T, C-T and C-A mismatches significantly destabilize it. The activation energy for the overall dissociation processes for these oligonucleotide-DNA duplexes containing 19 base pairs is 52 +/- 2 Kcal mol-1 as determined from the slope of Arrhenius plot.     

Intercalation of a Zn(II) complex containing ciprofloxacin drug between DNA base pairs

In this study, an attempt has been made to study the interaction of a Zn(II) complex containing an antibiotic drug, ciprofloxacin, with calf thymus DNA using spectroscopic methods. It was found that Zn(II) complex could bind with DNA via intercalation mode as evidenced by: hyperchromism in UV–Vis spectrum; these spectral characteristics suggest that the Zn(II) complex interacts with DNA most likely through a mode that involves a stacking interaction between the aromatic chromophore and the base pairs of DNA. DNA binding constant (K_b = 1.4 × 10⁴ M^?1) from spectrophotometric studies of the interaction of Zn(II) complex with DNA is comparable to those of some DNA intercalative polypyridyl Ru(II) complexes 1.0 ?4.8 × 10⁴ M^?1. CD study showed stabilization of the right-handed B form of DNA in the presence of Zn(II) complex as observed for the classical intercalator methylene blue. Thermodynamic parameters (ΔH < 0 and ΔS < 0) indicated that hydrogen bond and Van der Waals play main roles in this binding prose. Competitive fluorimetric studies with methylene blue (MB) dye have shown that Zn(II) complex exhibits the ability of this complex to displace with DNA-MB, indicating that it binds to DNA in strong competition with MB for the intercalation.     

Possible conformations of double-helical polynucleotides containing incorrect base pairs

Theoretical conformational analysis using classical potential functions has shown the possibility of incorporation of nucleotide mispairs with the bases in normal tautomeric forms into the DNA double helix. Incorrect purine-pyrimidine, purine-purine and pyrimidine-pyrimidine pairs can be incorporated into the double helix existing both in A- and B-conformations. The most energy favourable conformations of fragments containing a mispair have all the dihedral angles of the sugar-phosphate backbone within the limits characteristic of double helices consisting of Watson-Crick nucleotide pairs. Incorporation of mispairs is possible practically without the appearance of reduced interatomic contacts. Mutual position of bases in the incorporated mispair does not differ much from their position at the energy minimum of the corresponding isolated base pairs. Conformational parameters of irregular regions of double-stranded polynucleotides containing G:U, I:A, I:A* (syn) and U:C pairs are presented. Distortion of the sugar-phosphate backbone is the least upon incorporation of the G:U pair. Formation of mispairs in the processes of nucleic acid biosynthesis and spontaneous mutagenesis is discussed.     

Effect of base-pair sequence on the conformations and thermally induced transitions in oligodeoxyribonucleotides containing only AT base pairs

Tm curves, CD spectra, and kinetics results of the self-complementary DNA dodecamers d(A6T6), d(A3T3A3T3), d(A2T2A2T2A2T2), d(ATATATATATAT), and d(T6A6) demonstrate that the thermal transitions of these oligomers at low salt concentration involve a hairpin intermediate. At high salt concentrations (greater than 0.1 M Na+) only a duplex to denatured-strand transition appears to occur. The temperature and salt-concentration regions of the transitions are very sequence dependent. Alternating-type AT sequences have a lower duplex stability and a greater tendency to form hairpins than sequences containing more nonalternating AT base pairs. Of the two nonalternating sequences, d(T6A6) is significantly less stable than d(A6T6). Both oligomers have CD curves that are very similar to the unusual CD spectrum of poly(dA).poly(dT). The Raman spectra of these two oligomers are also quite similar, but at low temperature, small intensity differences in two backbone modes and three nucleoside vibrations are obtained. The hairpin to duplex transition for the AT dodecamers was examined by salt-jump kinetics measurements. The transition is faster than transitions for palindromic-sequence oligomers containing terminal GC base pairs. Stopped-flow kinetics studies indicate that the transition is second order and has a relatively low activation energy. The reaction rate increases with increasing ionic strength. These results are consistent with a three-step mechanism for the hairpin to duplex reaction: (i) fraying of the hairpin oligomers' terminal base pairs, (ii) a rate-determining bimolecular step involving formation of a cruciform-type intermediate from two hairpin oligomers with open terminal base pairs, and (iii) base-pair migration and formation in the intermediate to give the duplex.     

Parallel-stranded duplex DNA containing blocks of trans purine-purine and purine-pyrimidine base pairs.

A 30 base pair parallel-stranded (ps) duplex ps-L1.L2 composed of two adjoined purine-purine and purine-pyrimidine sequence blocks has been characterized thermodynamically and spectroscopically. The 5'-terminal 15 residues in both strands ('left-half') consisted of the alternating d(GA)7G sequence that forms a ps homoduplex secondary structure stabilized by d(G.G) and d(A.A) base pairs. The 3'-terminal 15 positions of the sequence ('right-half') were combinations of A and T with complementary reverse Watson-Crick d(A.T) base pairing between the two strands. The characteristics of the full length duplex were compared to those of the constituent left and right halves in order to determine the compatibility of the two ps helical forms. The thermal denaturation curves and hyperchromicity profiles of all three duplexes determined by UV absorption spectroscopy were characteristic of ps-DNA, in accordance with previous studies. The thermodynamic properties of the 30 bp duplex corresponded within experimental error to the linear combination of the two 15-mers. Thus, the Tm and delta HvH of ps-L1.L2 in 10 mM MgCl2, derived from analyses according to a statistical mechanical formulation for the helix-coil transition, were 43 degrees C and 569 kJ mol-1, compared to 21 degrees C, 315 kJ mol-1 (ps-F5.F6) and 22 degrees C, 236 kJ mol-1 (ps-GA15). The UV absorption and CD spectra of ps-L1.L2 and the individual 15-mer ps motifs were also compared quantitatively. The sums of the two constituent native spectra (left+right halves) accurately matched that of the 30 bp duplex, with only small deviations in the 195-215 nm (CD) and 220-240 nm (absorption) regions. Based on analysis by native gel electrophoresis, the sequences studied formed duplex structures exclusively; there were no indications of higher order species. Chemical modification with diethyl pyrocarbonate showed no hyperreactivity of the junctional bases, indicating a smooth transition between the two parallel-stranded conformations. We conclude that under given salt conditions, oligonucleotides with normal primary chemical structures can readily form a parallel-stranded double helix based on blocks of very disparate non-canonical purine-purine and purine-pyrimidine base pairs and without perceptible destabilization at the junction. There are biological implications of these findings in relation to genetic structure and expression.     

Characterization of imperfect DNA duplexes containing unpaired bases and non-Watson-Crick base pairs.

Synthetic duplex DNAs of repeating sequence, such as poly d(TTC).poly d(GAA), were separated into their individual single strands. The various single strands complexed not only, as expected, with their complementary strands, but also with other non-complementary strands. Characterization of such complexes with respect to stoichiometry, Tm values and the dependence of Tm on NaCl concentration showed that a variety of unusual structures could be inferred at physiological salt concentrations. These included extrahelical thymines, G.T oppositions, A.C oppositions and T.C oppositions.     

Preparation and properties of a nucleosomal particle containing 180 base pairs of DNA

If chromatin from chicken erythrocytes is enzymatically degraded in the presence of histone H5, nucleosomal DNA usually exceeds the size of 140 base pairs. Conditions are derived allowing the isolation of a 180 base pair particle which is subsequently characterized by histone binding and thermal denaturation studies. Association of H5 to such a particle is cooperative and occurs with a larger affinity than binding to specimens in the range of 140– 170 base pairs. Thermal denaduration studies show that some of the extra DNA participates in the main transition at 74°C (1 mm Na-cacodylate) indicating a tight binding to the histone core. Another part of the extra segment is loosely associated with the core but also distinct from free DNA.     

Unusual class of Alu sequences containing a potential Z-DNA segment.

A potential Z-DNA sequence, (dA-dC)9, has been found to replace the customary A-rich region in the middle of an Alu family member in the African green monkey genome. This Alu, bounded by imperfect direct repeats, also contains an unusual 3' end and may be a member of a large subfamily of such sequences.