Hydration of [d(CGC)r(aaa)d(TTTGCG)](2)

We have studied the hydration and dynamics of RNA C2'-OH in a DNA. RNA hybrid chimeric duplex [d(CGC)r(aaa)d(TTTGCG)](2). Long-lived water molecules with correlation time tau(c) larger than 0.3 ns were found close to the RNA adenine H2 and H1' protons in the hybrid segment. A possible long-lived water molecule was also detected close to the methyl group of 7T in the RNA-DNA junction but not to the other two thymine bases (8T and 9T). This result correlates with the structural studies that only DNA residue 7T in the RNA-DNA junction adopts an O4'-endo sugar conformation (intermediate between B-form and A-form), while the other DNA residues including 3C in the DNA-RNA junction, adopt C1'-exo or C2'-endo conformations (in the B-form domain). Based on the NOE cross-peak patterns, we have found that RNA C2'-OH tends to orient toward the O3' direction, forming a possible hydrogen bond with the 3'-phosphate group. The exchange rates for RNA C2'-OH were found to be around 5-20 s(-1), compared to 26.7(+/-13.8) s(-1) reported previously for the other DNA.RNA hybrid duplex. This slow exchange rate may be due to the narrow minor groove width of [d(CGC)r(aaa)d(TTTGCG)](2), which may trap the water molecules and restrict the dynamic motion of hydroxyl protons. The distinct hydration patterns of the RNA adenine H2 and H1' protons and the DNA 7T methyl group in the hybrid segment, as well as the orientation and dynamics of the RNA C2'-OH protons, may provide a molecular basis for further understanding the structure and recognition of DNA.RNA hybrid and chimeric duplexes.     

The Solution Structure of [d(CGC)r(amamam)d(TTTGCG)]2

The solution structure and hydration of a DNARNA hybrid chimeric duplex [d(CGC)r(a_ma_ma_m)d(TTTGCG)]₂ in which the RNA adenines were substituted by 2-O-methylated riboadenines was determined using two-dimensional NMR, simulated annealing, and restrained molecular dynamics. Only DNA residue 7T in the 2-OMe-RNA DNA junction adopted an O4-endo sugar conformation, while the other DNA residues including 3C in the DNA 2-OMe-RNA junction, adopted C1-exo or C2-endo conformations. The observed NOE intensity of 2-O-methyl group to H1 proton of 4a_m at the DNA 2-OMe-RNA junction is much weaker than those of 5a_m and 6a_m. The 2-O-methyl group of 4a_m was found to orient towards the minor groove in the trans domain while the 2-O- methyl groups of 5a_m and 6a_m were found to be in the gauche (+) domain. In contrast to the long-lived water molecules found close to the RNA adenine H2 and H1 protons and the methyl group of 7T in the RNA-DNA junction of [d(CGC)r(aaa)d(TTTGCG)]₂, there were no long-lived water molecules found in [d(CGC)r(a_ma_ma_m)d(TTTGCG)]₂. This is probably due to the hydrophobic enviroment created by the 2-O-methylated riboadenines in the minor groove or due to the wider minor groove width in the middle of the structure. In addition, the 2-O-methylation of riboadenines in pure chimeric duplex increses its melting temperature from 48.5°C to 51.9°C. The characteristic structural features and hydration patterns of this chimeric duplex provide a molecular basis for further therapeutic applications of DNARNA hybrid and chimeric duplexes with 2-modified RNA residues.     

Crystal structure of 9-amino-N-[2-(4-morpholinyl)ethyl]-4-acridinecarboxamide bound to d(CGTACG)2: implications for structure–activity relationships of acridinecarboxamide topoisomerase poisons

The structure of the complex formed between d(CGTACG)₂ and 9-amino-N-[2-(4-morpholinyl)ethyl]-4-acridinecarboxamide, an inactive derivative of the antitumour agents N-[2-(dimethylamino)ethyl]acridine-4-carboxamide (DACA) and 9-amino-DACA, has been solved to a resolution of 1.8 Å using X-ray crystallography. The complex crystallises in the space group P6₄ and the final structure has an overall R factor of 21.9%. A drug molecule intercalates between each of the CpG dinucleotide steps with its side chain lying in the major groove, and its protonated morpholino nitrogen partially occupying positions close to the N7 and O6 atoms of guanine G2. The morpholino group is disordered, the major conformer adopting a twisted boat conformation that makes van der Waals contact with the O4 oxygen of thymine T3. A water molecule forms bridging hydrogen bonds between the 4-carboxamide NH and the phosphate group of guanine G2. Sugar rings are found in alternating C3′-exo/C2′-endo conformations except for cytosine C1 which is C3′-endo. Intercalation perturbs helix winding throughout the hexanucleotide compared with B-DNA, steps 1 and 2 being unwound by 10 and 8°, respectively, while the central TpA step is overwound by 11°. An additional drug molecule lies at the end of each DNA helix linking it to the next duplex to form a continuously stacked structure. The protonated morpholino nitrogen of this ‘end-stacked’ drug hydrogen bonds to the N7 atom of guanine G6, and its conformationally disordered morpholino ring forms a C–H···O hydrogen bond with the guanine O6 oxygen. In both drug molecules the 4-carboxamide group is internally hydrogen bonded to the protonated N10 atom of the acridine ring. We discuss our findings with respect to the potential role played by the interaction of the drug side chain and the topoisomerase II protein in the poisoning of topoisomerase activity by the acridinecarboxamides.     

Unusual intercalation of acridin-9-ylthiourea into the 5'-GA/TC DNA base step from the minor groove: implications for the covalent DNA adduct profile of a novel platinum-intercalator conjugate

The binding of the novel cytotoxic acridine derivative, 1-[2-(acridin-9-ylamino)ethyl]-1,3-dimethylthiourea (ACRAMTU) to various self-complementary oligonucleotide duplexes has been studied by combined high-resolution NMR spectroscopy/restrained molecular dynamics and equilibrium binding assays to establish the sequence and groove specificity of intercalation. The binding mode in the sequences d(GGACGTCC)₂ and d(GGAGCTCC)₂ was deduced from chemical shift changes and intermolecular NOEs between the ligand and the oligonucleotides. ACRAMTU intercalated into the 5′-CG/CG and 5′-GA/TC base steps, and penetration of the duplexes occurred from the minor groove. Intercalation of ACRAMTU in d(GGTACC)₂ occurs at the central TA/TA step, based on the absence of the internucleotide A4H8–T3H1′ and A4H8–T3H3′ cross-peaks in the 1:1 complex of this sequence. An energy- minimized AMBER model of the 1:2 complex, [d(GGAGCTCC)₂(ACRAMTU)₂], was generated, which was based on restricted molecular dynamics/ mechanics calculations using 108 NOE distance restraints (including 11 DNA–drug distances per ligand). Equilibrium dialysis experiments were performed using octamers containing various base steps present in the ‘NMR sequences’. The highest affinity for ACRAMTU was observed in d(TATAT ATA)₂, followed by d(CGCGCGCG)₂ and d(GAG ATCTC)₂. The binding levels for CG/CG and GA/TC were virtually the same. The unusual tolerance of the GA/TC intercalation site and the pronounced groove specificity of ACRAMTU play a significant role in the molecular recognition between the corresponding platinum conjugate, Pt-ACRAMTU, and DNA.     

Extrahelical cytosine bases in DNA duplexes containing d[GCC]n·d[GCC]n repeats: detection by a mechlorethamine crosslinking reaction

The cytosine–cytosine (C–C) pair is one of the least stable DNA mismatch pairs. The bases of the C–C mismatch are only weakly hydrogen bonded, and previous work has shown that, in certain sequence contexts, they can become unstacked from the core helix, and adopt an ‘extrahelical’ location. Here, using DNA duplexes with d[GCC]_n·d[GCC]_n fragments containing C–C mismatches in a 1,4 bp relationship, we show that cytosine bases of different formal mismatch pairs can be crosslinked by mechlorethamine. For example, in the duplex d[CTCTCGCCGCCGCCGTATC]·d[GATACGCCGCCGCCGAGAG], where underlined cytosine bases are present as the formal C–C mismatch pairs C₇–C₃₂, C₁₀–C₂₉ and C₁₃–C₂₆, we show that two mechlorethamine crosslinks form between C₁₃ and C₂₉ and between C₁₀ and C₃₂, in addition to crosslinks at C₇–C₃₂, C₁₀–C₂₉ and C₁₃–C₂₆ (we have reported previously the crosslinking of formal C–C pairs by mechlorethamine). We interpret the formation of the C₁₃–C₂₉ and C₁₀–C₃₂ crosslinks as evidence of an extrahelical location of the crosslinkable cytosines. Such extrahelical cytosine bases have been observed previously for a single C–C mismatch pair (in the so-called E-motif conformation). In the E-motif, the extrahelical cytosines are folded back towards the 5′-end of the duplex, consistent with our crosslinking data, and also consistent with the absence of C₇–C₂₉ and C₁₀–C₂₆ crosslinks in the current work. Hence, our data provide evidence for an extended E-motif DNA (eE-DNA) conformation in short d[GCC]_n·d[GCC]_n repeat fragments, and raise the possibility that such structures might occur in much longer d[GCC]_n·d[GCC]_n repeat tracts.     

Synthesis and crystal structure of an octamer RNA r(guguuuac)/r(guaggcac) with G.G/U.U tandem wobble base pairs: comparison with other tandem G.U pairs

We have determined the crystal structure of the RNA octamer duplex r(guguuuac)/r(guaggcac) with a tandem wobble pair, G·G/U·U (motif III), to compare it with U·G/G·U (motif I) and G·U/U·G (motif II) and to better understand their relative stabilities. The crystal belongs to the rhombohedral space group R3. The hexagonal unit cell dimensions are a = b = 41.92 Å, c = 56.41 Å, and γ = 120°, with one duplex in the asymmetric unit. The structure was solved by the molecular replacement method at 1.9 Å resolution and refined to a final R factor of 19.9% and R_free of 23.3% for 2862 reflections in the resolution range 10.0–1.9 Å with F ≥ 2σ(F). The final model contains 335 atoms for the RNA duplex and 30 water molecules. The A-RNA stacks in the familiar head-to-tail fashion forming a pseudo-continuous helix. The uridine bases of the tandem U·G pairs have slipped towards the minor groove relative to the guanine bases and the uridine O2 atoms form bifurcated hydrogen bonds with the N1 and N2 of guanines. The N2 of guanine and O2 of uridine do not bridge the ‘locked’ water molecule in the minor groove, as in motifs I and II, but are bridged by water molecules in the major groove. A comparison of base stacking stabilities of motif III with motifs I and II confirms the result of thermodynamic studies, motif I > motif III > motif II.     

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.     

Ensemble and single-molecule fluorescence spectroscopic study of the binding modes of the bis-benzimidazole derivative Hoechst 33258 with DNA

Ensemble and single-molecule fluorescence measurements of 2′-(4-hydroxyphenyl)-5-[5-(4-methylpiperazine-1-yl) benzimidazo-2-yl]-benzimidazole (H-258)– calf thymus (CT) DNA complexes at various [H-258]/[DNA bp] ratios were performed to elucidate the binding of H-258 with DNA. Upon binding to double-stranded CT DNA (CT ds DNA) at a [H-258]/[DNA bp] ratio of 0.05 the relative fluorescence quantum yield, Φ_f, of H-258 increases from 0.02 to 0.58. The fluorescence decay can be fitted almost by a mono-exponential model with a lifetime of ~3.6 ns. This indicates that H-258 binds almost quantitatively in the minor groove of DNA at low [H-258]/[DNA bp] ratios. With increasing [H-258]/[DNA bp] ratios, e.g. 0.15 and 0.20, the fluorescence quantum yield of H-258 decreases to 0.28 and 0.19, respectively. Fitting of the fluorescence decays measured for higher [H-258]/[DNA bp] ratios reveals the presence of additional shorter fluorescence lifetime components in the range of 0.5–2.0 ns. Our results suggest that H-258 partially intercalates in G:C sequences at higher [H-258]/[DNA bp] ratios reflected by a lifetime component of 1.5–2 ns. In addition, stacking or adsorption of H-258 molecules on DNA occurs at higher [H-258]/[DNA bp] ratios. These molecules exhibit a short fluorescence lifetime of ~500 ps and are more exposed to the aqueous environment. Fluorescence transients of the intensity and lifetime of single H-258 CT ds DNA demonstrate that weakly (unspecific) bound H-258 molecules exhibit a shorter fluorescence lifetime and a strongly reduced photostability.     

RNase H mediated cleavage of RNA by cyclohexene nucleic acid (CeNA)

Cyclohexene nucleic acid (CeNA) forms a duplex with RNA that is more stable than a DNA–RNA duplex (ΔT_m per modification: +2°C). A cyclohexenyl A nucleotide adopts a 3′-endo conformation when introduced in dsDNA. The neighbouring deoxynucleotide adopts an O4′-endo conformation. The CeNA:RNA duplex is cleaved by RNase H. The V_max and K_m of the cleavage reaction for CeNA:RNA and DNA:RNA is in the same range, although the k_cat value is about 600 times lower in the case of CeNA:RNA.     

Determination of DNA minor groove width in distamycin-DNA complexes by solid-state NMR

We have performed solid-state ³¹P-¹⁹F REDOR nuclear magnetic resonance (NMR) experiments to monitor changes in minor groove width of the oligonucleotide d(CGCAAA^2′FUTGGC)·d(GCCAAT(pS)TT GCG) (A₃T₂) upon binding of the drug distamycin A at different stoichiometries. In the hydrated solid-state sample, the minor groove width for the unbound DNA, measured as the ^2′FU7–pS19 inter-label distance, was 9.4 ± 0.7 Å, comparable to that found for similar A:T-rich DNAs. Binding of a single drug molecule is observed to cause a 2.4 Å decrease in groove width. Subsequent addition of a second drug molecule results in a larger conformational change, expanding this minor groove width to 13.6 Å, consistent with the results of a previous solution NMR study of the 2:1 complex. These ³¹P-¹⁹F REDOR results demonstrate the ability of solid-state NMR to measure distances of 7–14 Å in DNA–drug complexes and provide the first example of a direct spectroscopic measurement of minor groove width in nucleic acids.     

Complicated water orientations in the minor groove of the B-DNA decamer d(CCATTAATGG)2 observed by neutron diffraction measurements

It has long been suspected that the structure and function of a DNA duplex can be strongly dependent on its degree of hydration. By neutron diffraction experiments, we have succeeded in determining most of the hydrogen (H) and deuterium (D) atomic positions in the decameric d(CCATTAATGG)₂ duplex. Moreover, the D positions in 27 D₂O molecules have been determined. In particular, the complex water network in the minor groove has been observed in detail. By a combined structural analysis using 2.0 Å resolution X-ray and 3.0 Å resolution neutron data, it is clear that the spine of hydration is built up, not only by a simple hexagonal hydration pattern (as reported in earlier X-ray studies), but also by many other water bridges hydrogen-bonded to the DNA strands. The complexity of the hydration pattern in the minor groove is derived from an extraordinary variety of orientations displayed by the water molecules.     

A novel form of intercalation involving four DNA duplexes in an acridine-4-carboxamide complex of d(CGTACG)(2)

The structures of the complexes formed between 9-amino-[N-(2-dimethyl-amino)butyl]acridine-4-carboxamide and d(CG^5BrUACG)₂ and d(CGTACG)₂ have been solved by X-ray crystallography using MAD phasing methodology and refined to a resolution of 1.6 Å. The complexes crystallised in space group C222. An asymmetric unit in the brominated complex comprises two strands of DNA, one disordered drug molecule, two cobalt (II) ions and 19 water molecules (31 in the native complex). Asymmetric units in the native complex also contain a sodium ion. The structures exhibit novel features not previously observed in crystals of DNA/drug complexes. The DNA helices stack in continuous columns with their central 4 bp adopting a B-like motif. However, despite being a palindromic sequence, the terminal GC base pairs engage in quite different interactions. At one end of the duplex there is a CpG dinucleotide overlap modified by ligand intercalation and terminal cytosine exchange between symmetry-related duplexes. A novel intercalation complex is formed involving four DNA duplexes, four ligand molecules and two pairs of base tetrads. The other end of the DNA is frayed with the terminal guanine lying in the minor groove of the next duplex in the column. The structure is stabilised by guanine N7/cobalt (II) coordination. We discuss our findings with respect to the effects of packing forces on DNA crystal structure, and the potential effects of intercalating agents on biochemical processes involving DNA quadruplexes and strand exchanges. NDB accession numbers: DD0032 (brominated) and DD0033 (native).     

The crystal structure of an alternating RNA heptamer r(GUAUACA) forming a six base-paired duplex with 3'-end adenine overhangs

The crystal structure of an alternating RNA heptamer r(GUAUACA) has been determined to 2.0 Å resolution and refined to an R_work of 17.1% and R_free of 18.5% using 2797 reflections. The heptamer crystallized in the space group C222 with a unit cell of a = 25.74, b = 106.58, c = 30.26 Å and two independent strands in the asymmetric unit. Each heptamer forms a duplex with its symmetry-related strand and each duplex contains six Watson–Crick base pairs and 3′-end adenosine overhangs. Therefore, two kinds of duplex (duplex 1 and duplex 2) are formed. Duplexes 1 stack on each other forming a pseudo-continuous column, which is typical of the RNA packing mode, while duplex 2 is typical of A-DNA packing with its termini in abutting interactions. Overhang adenine residues stack within the duplexes with C3′-endo sugar pucker and C2′-endo sugar pucker in duplexes 1 and 2, respectively. A Na⁺ ion in the crystal lattice is water bridged to two N1 atoms of symmetry-related A7 bases.     

Solution structure of the hydroperoxide of Co(III) phleomycin complexed with d(CCAGGCCTGG)2: evidence for binding by partial intercalation

The bleomycins (BLMs) are natural products that in the presence of iron and oxygen bind to and cause single-strand and double-strand cleavage of DNA. The mode(s) of binding of the FeBLMs that leads to sequence-specific cleavage at pyrimidines 3′ to guanines and chemical-specific cleavage at the C-4′ H of the deoxyribose of the pyrimidine has remained controversial. 2D NMR studies using the hydroperoxide of CoBLM (HOO-CoBLM) have demonstrated that its bithiazole tail binds by partial intercalation to duplex DNA. Studies with ZnBLM demonstrate that the bithiazole tail binds in the minor groove. Phleomycins (PLMs) are BLM analogs in which the penultimate thiazolium ring of the bithiazole tail is reduced. The disruption of planarity of this ring and the similarities between FePLM- and FeBLM-mediated DNA cleavage have led Hecht and co-workers to conclude that a partial intercalative mode of binding is not feasible. The interaction of HOO-CoPLM with d(CCAGGCCTGG)₂ has therefore been investigated. Binding studies indicate a single site with a K_d of 16 µM, 100-fold greater than HOO-CoBLM for the same site. 2D NMR methods and molecular modeling using NMR-derived restraints have led to a structural model of HOO-CoPLM complexed to d(CCAGGCCTGG)₂. The model reveals a partial intercalative mode of binding and the basis for sequence specificity of binding and chemical specificity of cleavage. The importance of the bithiazoles and the partial intercalative mode of binding in the double-strand cleavage of DNA is discussed.     

Syntheses and structural studies of calix[4]arene-nucleoside and calix[4]arene-oligonucleotide hybrids

We have synthesized three types of calix[4]arene– nucleoside hybrid efficiently by amide bond formation between the amine functional groups of 1,3-diaminocalix[4]arene and the carboxyl groups of thymidine nucleoside derivatives. X-ray crystallography of a homocoupled calix[4]arene–nucleoside hybrid revealed an interesting hydrogen bonding pattern between thymine bases and the amide linkages. We designed the calix[4]arene–oligonucleotide hybrids (5′-AAAAGATATCAAXTTGATATCTTTT-3′, 5′-T₁₂-X-T₁₂-3′, and 5′-A₁₂-X-T₁₂-3′) to be V-shaped oligodeoxyribonucleotides and synthesized them by using a calix[4]arene–nucleoside hybrid (X) as a key building block. Thermal denaturation experiments, monitored by UV spectroscopy at 260 and 284 nm, and circular dichroism spectra of the calix[4]arene–oligonucleotide hybrids suggest that the modified oligonucleotides indeed adopt V-shaped conformations, making them suitable for use as building blocks in the construction of programmed oligonucleotide nanostructures.     

Incorporation of a cationic aminopropyl chain in DNA hairpins: thermodynamics and hydration

We report on the physicochemical effects resulting from incorporating a 5-(3-aminopropyl) side chain onto a 2′-deoxyuridine (dU) residue in a short DNA hairpin. A combination of spectroscopy, calorimetry, density and ultrasound techniques were used to investigate both the helix–coil transition of a set of hairpins with the following sequence: d(GCGACTTTTTGNCGC) [N = dU, deoxythymidine (dT) or 5-(3-aminopropyl)-2′-deoxyuridine (dU*)], and the interaction of each hairpin with Mg²⁺. All three molecules undergo two-state transitions with melting temperatures (T_M) independent of strand concentration that indicates their intramolecular hairpin formation. The unfolding of each hairpin takes place with similar T_M values of 64–66°C and similar thermodynamic profiles. The unfavorable unfolding free energies of 6.4–6.9 kcal/mol result from the typical compensation of unfavorable enthalpies, 36–39 kcal/mol, and favorable entropies of ~110 cal/mol. Furthermore, the stability of each hairpin increases as the salt concentration increases, the T_M-dependence on salt yielded slopes of 2.3–2.9°C, which correspond to counterion releases of 0.53 (dU and dT) and 0.44 (dU*) moles of Na⁺ per mole of hairpin. Absolute volumetric and compressibility measurements reveal that all three hairpins have similar hydration levels. The electrostatic interaction of Mg²⁺ with each hairpin yielded binding affinities in the order: dU > dT > dU*, and a similar release of 2–4 electrostricted water molecules. The main result is that the incorporation of the cationic 3-aminopropyl side chain in the major groove of the hairpin stem neutralizes some local negative charges yielding a hairpin molecule with lower charge density.     

Sequence-dependent variation in DNA minor groove width dictates orientational preference of Hoechst 33258 in A-tract recognition: solution NMR structure of the 2:1 complex with d(CTTTTGCAAAAG)(2)

The solution structure of the dodecamer duplex d(CTTTTGCAAAAG)₂ and its 2:1 complex with the bis-benzimidazole Hoechst 33258 has been investigated by NMR and NOE-restrained molecular dynamics (rMD) simulations. Drug molecules are bound in each of the two A-tracts with the bulky N-methylpiperazine ring of each drug located close to the central TG (CA) step, binding essentially to the narrow minor groove of each A-tract. MD simulations over 1 ns, using an explicit solvation model, reveal time-averaged sequence-dependent narrowing of the minor groove from the 3′-end towards the 5′-end of each TTTT sequence. Distinct junctions at the TpG (CpA) steps, characterised by large positive roll, low helical and propeller twists and rapid AT base pair opening rates, add to the widening of the groove at these sites and appear to account for the bound orientation of the two drug molecules with the N-methylpiperazine ring binding in the wider part of the groove close to the junctions. Comparisons between the free DNA structure and the 2:1 complex (heavy atom RMSD 1.55 Å) reveal that these sequence-dependent features persist in both structures. NMR studies of the sequence d(GAAAAGCTTTTC)₂, in which the A-tracts have been inverted with the elimination of the TpG junctions, results in loss of orientational specificity of Hoechst 33258 and formation of multiple bound species in solution, consistent with the drug binding in a number of different orientations.     

The solution structure of double helical arabino nucleic acids (ANA and 2��F-ANA): effect of arabinoses in duplex-hairpin interconversion

We report here the first structure of double helical arabino nucleic acid (ANA), the C2′-stereoisomer of RNA, and the 2′-fluoro-ANA analogue (2′F-ANA). A chimeric dodecamer based on the Dickerson sequence, containing a contiguous central segment of arabino nucleotides, flanked by two 2′-deoxy-2′F-ANA wings was studied. Our data show that this chimeric oligonucleotide can adopt two different structures of comparable thermal stabilities. One structure is a monomeric hairpin in which the stem is formed by base paired 2′F-ANA nucleotides and the loop by unpaired ANA nucleotides. The second structure is a bimolecular duplex, with all the nucleotides (2′F-ANA and ANA) forming Watson–Crick base pairs. The duplex structure is canonical B-form, with all arabinoses adopting a pure C2′-endo conformation. In the ANA:ANA segment, steric interactions involving the 2′-OH substituent provoke slight changes in the glycosidic angles and, therefore, in the ANA:ANA base pair geometry. These distortions are not present in the 2′F-ANA:2′F-ANA regions of the duplex, where the –OH substituent is replaced by a smaller fluorine atom. 2′F-ANA nucleotides adopt the C2′-endo sugar pucker and fit very well into the geometry of B-form duplex, allowing for favourable 2′F···H8 interactions. This interaction shares many features of pseudo-hydrogen bonds previously observed in 2′F-ANA:RNA hybrids and in single 2′F-ANA nucleotides.     

Synthesis and properties of 4'-ThioDNA: unexpected RNA-like behavior of 4'-ThioDNA

The synthesis and properties of fully modified 4′-thioDNAs, oligonucleotides consisting of 2′-deoxy-4′-thionucleosides, were examined. In addition to the known literature properties (preferable hybridization with RNA and resistance to endonuclease hydrolysis), we also observed higher resistance of 4′-thioDNA to 3′-exonuclease cleavage. Furthermore, we found that fully modified 4′-thioDNAs behaved like RNA molecules in their hybridization properties and structural aspect, at least in the case of the 4′-thioDNA duplex. This observation was confirmed by experiments using groove binders, in which a 4′-thioDNA duplex interacts with an RNA major groove binder, lividomycin A, but not with DNA groove binders, to give an increase in its thermal stability. Since a 4′-thioDNA duplex competitively inhibited the hydrolysis of an RNA duplex by RNase V₁, it was not only the physical properties but also this biological data suggested that a 4′-thioDNA duplex has an RNA-like structure.     

Hexamminecobalt(III)-induced condensation of calf thymus DNA: circular dichroism and hydration measurements

The interaction of hexamminecobalt(III), Co(NH₃)₆³⁺, with 160 and 3000–8000 bp length calf thymus DNA has been investigated by circular dichroism, acoustic and densimetric techniques. The acoustic titration curves of 160 bp DNA revealed three stages of interaction: (i) Co(NH₃)₆³⁺ binding up to the molar ratio [Co(NH₃)₆³⁺]/[P] = 0.25, prior to DNA condensation; (ii) a condensation process between [Co(NH₃)₆³⁺]/[P] = 0.25 and 0.30; and (iii) precipitation after [Co(NH₃)₆³⁺]/[P] = 0.3. In the case of 3000–8000 bp DNA only two processes were observed: (i) binding up to [Co(NH₃)₆³⁺]/[P] = 0.3; and (ii) precipitation after this point. In agreement with earlier observations, long DNA aggregates without changes in its B-form circular dichroism spectrum, while short DNA demonstrates a positive B→Ψ transition after [Co(NH₃)₆³⁺]/[P] = 0.25. From ultrasonic and densimetric measurements the effects of Co(NH₃)₆³⁺ binding on volume and compressibility have been obtained. The binding of Co(NH₃)₆³⁺ to both short and long DNA is characterized by similar changes in volume and compressibility calculated per mole Co(NH₃)₆³⁺: ΔV = 9 cm³ mol^–1 and Δκ = 33 × 10^–4 cm³ mol^–1 bar^–1. The positive sign of the parameters indicates dehydration, i.e. water release from Co(NH₃)₆³⁺ and the atomic groups of DNA. This extent of water displacement would be consistent with the formation of two direct, hydrogen bonded contacts between the cation and the phosphates of DNA.