Caesium fluoride-induced changes in the c.d. spectra of synthetic DNA fragments

Ten DNA fragments containing self-complementary alternating sequences of adenine and thymine differing in length and the starting nucleotide were studied by c.d. spectroscopy. It was found that d(TATATATA) but not d(ATATATAT), d(TATATA), d(CTATATAG) or (dT-dA)20 isomerized into the unusual X-DNA double helix at molar concentrations of CsF in solution. But in contrast to poly(dA-dT), the octamer (dT-dA)4, isomerized very slowly, at relatively low CsF concentrations and the isomerization was strongly dependent on the octamer concentration. A model is proposed to account for the observed properties of the B-to-X isomerization on the oligomer level.     

Structure, dynamics, and thermodynamics of mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2

The structures and hydrogen exchange properties of the mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2 have been studied by high-resolution nuclear magnetic resonance. Both the adenine-adenine and thymine-thymine mismatches are intercalated in the duplexes. The structures of these self-complementary duplexes are symmetric, with the two strands in equivalent positions. The evidence indicates that these mismatches are not stably hydrogen bonded. The mismatched bases in both duplexes are in the anti conformation. The mismatched thymine nucleotide in d(CCCTGGG)2 is intercalated in the duplex with very little distortion of the bases or sugar-phosphate backbone. In contrast, the bases of the adenine-adenine mismatch in d(CCCAGGG)2 must tilt and push apart to reduce the overlap of the amino groups. The thermodynamic data show that the T-T mismatch is less destabilizing than the A-A mismatch when flanked by C-G base pairs in this sequence, in contrast to their approximately equal stabilities when flanked by A-T base pairs in the sequence d(CAAAXAAAG.CTTTYTTTG) where X and Y = A, C, G, and T [Aboul-ela, F., Koh, D., & Tinoco, I., Jr. (1985) Nucleic Acids Res. 13, 4811]. Although the mechanism cannot be determined conclusively from the limited data obtained, exchange of the imino protons with solvent in these destabilized heteroduplexes appears to occur by a cooperative mechanism in which half the helix dissociates.     

Alternating d(G-C)3 and d(C-G)3 hexanucleotides containing 7-deaza-2''-deoxyguanosine or 8-aza-7-deaza-2''-deoxyguanosine in place of dG.

The synthesis of alternating hexamers (8-13) derived from d(C-G)3 or d(G-C)3 but containing c7z8Gd (2) or c7Gd (3) instead of dG is described employing phosphoramidite-chemistry. Apart from the isobutyryl group the dimethylaminomethylene residue was used for the nucleobase-protection of 3. The methyl- and the cyanoethyl-phosphoramidites of 3 (5a-c) were synthesized. They were employed together with those of c7G or c7z8Gd in automated oligonucleotide synthesis. Tm-values as well as thermodynamic data of the oligomers 9, 10, 12, and 13 indicated that duplexes were destabilized if c7Gd replaced dG, whereas c7z8Gd stabilized the duplex structure. In contrast to d(C-G)3 which underwent salt-dependent B-Z transition, CD-spectra of oligomers containing c7Gd or c7z8Gd in place of dG showed retained B-conformation.     

Molecular dynamics simulation of the DNA triplex d(TC)5.d(GA)5.d(C+T)5.

A molecular dynamics simulation of the DNA triple helix d(TC)5.d(GA)5.d(C+T)5 is described (C+ represents a protonated cytosine residue). The simulation has been performed using the program AMBER 3.1 and includes counterions and explicit solvent under periodic boundary conditions. Both the dynamic and time-averaged behaviour of the system has been analysed. Considerable deviations from the fibre-diffraction model for DNA triple helix structure are observed, including the repuckering of the purine strand sugars that has been identified in some nuclear magnetic resonance (n.m.r.) studies. The simulation suggests that this conformational change may be driven by the possibility of improved interactions between the phosphate groups of this strand and both the solvent and counterions. Several examples of a particular conformational transition are observed, involving correlated changes in the backbone angles alpha and gamma. These transitions provide a possible explanation for some unusual n.m.r. data that have been reported. The structure of the triple helix major groove also suggests an explanation for the observed stabilization of DNA triplexes by polyvalent cations, and their ability to interact with drugs that bind in the minor groove of DNA duplexes.     

A comparison of the hairpin stability of the palindromic d(CGCG(A/T)4CGCG) oligonucleotides.

The palindromic deoxyribonucleotides 5'-CGCGA-TATCGCG-3' and 5'-CGCGTTAACGCG-3' have been characterized by 1H NMR spectroscopy. The NMR data identified both B-DNA duplex conformations and hairpin conformations, the latter with loop regions consisting of the four central nucleotides. The resonances of the various conformations were assigned by use of two-dimensional NMR methods. The relative stability of the various conformations was investigated as a function of temperature, ionic strength and nucleotide concentration. The duplexes were found to be stabilized at high ionic strength and at low temperature, while the hairpins were stabilized at low ionic strength and at medium temperature. The thermodynamics of the duplex-hairpin and the hairpin-random coil transitions were examined, and compared to the other two oligonucleotide in the palindromic d(CGCG(A/T)4CGCG) oligonucleotide family. The relative stabilities of the duplex conformations with respect to the random coil conformations are similar for the d(CGCGAATTCGCG), d(CGCGATATCGCG) and d(CGCGTATACGCG) oligonucleotides. The duplex conformation of d(CGCGTTAACGCG) is less stable. The hairpin of d(CGCGTTAACGCG) seems also to be less stable relative to the random coil conformation than in the case of the other oligonucleotides at an equal oligonucleotide concentration. A cruciform intermediate between the duplex and hairpin conformations is suggested to explain some discrepancies observed in this work in case of the d(CGCGTTAACGCG) oligonucleotide. This is similar to what has been reported for the d(CGCGTATACGCG) oligonucleotide.     

Nonionic analogs of oligonucleotide duplexes. Calculations using a molecular mechanics methods of the effect of configuration at the asymmetrical phosphorus atom in phosphonic and triester derivatives of d(TpCH3)6, d(TpOEt)6 on the structure and stability of their complexes with dA6

Molecular mechanical calculations of the optimal structure and relative stability of duplexes of dA6 with non-ionic oligonucleotide analogs of the methylphosphonate d(TpCH3)6 and phosphotriester d(TpOEt)6 have been carried out. Duplexes of dA6 and non-ionic oligonucleotide analogs with Rp enantiomeric configuration of modified phosphorous groups in d(TpCH3) and Sp in d(TpOEt) turned out to be more stable than those with second enantiomeric configurations Sp and Rp, respectively. The main factors of energetic selectivity between Sp and Rp stereoisomers have been found to be steric strains and electrostatic interaction between asymmetric modified phosphate groups and the d-ribose 5' end. NOE generated distances between protons of alkyl substitute and d-ribose H2", H3' have been analysed. The results of the calculations are in agreement with experimental observations.     

Water and ion binding around r(UpA)12 and d(TpA)12 oligomers--comparison with RNA and DNA (CpG)12 duplexes

The structural and dynamic properties of the water and ion first coordination shell of the r(A-U) and d(A-T) base-pairs embedded within the r(UpA)12 and d(TpA)12 duplexes are described on the basis of two 2.4 ns molecular dynamics simulations performed in a neutralizing aqueous environment with 0.25 M added KCl. The results are compared to previous molecular dynamics simulations of the r(CpG)12 and d(CpG)12 structures performed under similar conditions. It can be concluded that: (i) RNA helices are more rigid than DNA helices of identical sequence, as reflected by the fact that RNA duplexes keep their initial A-form shape while DNA duplexes adopt more sequence-specific shapes. (ii) Around these base-pairs, the water molecules occupy 21 to 22 well-defined hydration sites, some of which are partially occupied by potassium ions. (iii) These hydration sites are occupied by an average of 21.9, 21.0, 20.1, and 19.8 solvent molecules (water and ions) around the r(G=C), r(A-U), d(G=C), and d(A-T) pairs, respectively. (iv) From a dynamic point of view, the stability of the hydration shell is the strongest for the r(G=C) pairs and the weakest for the d(A-T) pairs. (v) For RNA, the observed long-lived hydration patterns are essentially non-sequence dependent and involve water bridges located in the deep groove and linking OR atoms of adjacent phosphate groups. Maximum lifetimes are close to 400 ps. (vi) In contrast, for DNA, long-lived hydration patterns are sequence dependent and located in the minor groove. For d(CpG)12, water bridges linking the (G)N3 and (C)O2 with the O4' atoms of adjacent nucleotides with 400 ps maximum lifetimes are characterized while no such bridges are observed for d(TpA)12. (vii) Potassium ions are observed to bind preferentially to deep/major groove atoms at RpY steps, essentially d(GpC), r(GpC), and r(ApU), by forming ion-bridges between electronegative atoms of adjacent base-pairs. On average, about half an ion is observed per base-pair. Positive ion-binding determinants are related to the proximity of two or more electronegative atoms. Negative binding determinants are associated with the electrostatic and steric hindrance due to the proximity of electropositive amino groups and neutral methyl groups. Potassium ions form only transient contacts with phosphate groups.     

Structure of d(CGCGAATTCGCG) in the presence of Ca(2+) ions.

The dodecamer d(CGCGAATTCGCG) was the first oligonucleotide to be crystallized as a B-DNA duplex. Its structure was analyzed in detail in the early 1980s. Here we show that, in the presence of Ca(2+), it crystallizes in a different way (R3 space group). The dodecamers form parallel columns of straight duplexes with ten base pairs in the B form. The terminal cytosines in each molecule are disordered, whereas the terminal guanines are placed in the minor groove of neighbor duplexes. The central GAATTC region is practically identical to that found in the classic structure of the same dodecamer crystallized in the P2(1)2(1)2(1) space group in the presence of Mg(2+) and spermine. Its structure is thus independent of the crystallization conditions which have been used.     

Complementary addressed alkylation of Escherichia coli 16S rRNA with 2',3'-O-[4-N-methyl-N-(2-chloroethyl)aminobenzylidene]m derivatives of oligodeoxyribonucleotides. IV. Determination of binding sites of 16S rRNA with benzylidene derivatives of d(pACCTTGTT)rA, d(pTTACGACT)rU, d(TTTGCTCCCC)rA

By site-directed alkylation of 16S rRNA with benzylidene derivatives of d(pACCTTGTT)rA (II), d(pTTACGACT)rU (III), d(pTTTGCTCCCC)rA (IV) (reagents (II)--(IV] followed by the RNase H treatment a number of 16S rRNA fragments have been obtained. Hybridisation of these fragments with restriction fragments of plasmid pKK 3535, containing operon rrnB of E. coli rRNAs, led to the identification of all reagents' binding sites in 16S rRNA. Good correlation is found between estimated stability of non-perfect 16S rRNA.oligodeoxyribonucleotide duplexes and the level of modification of this site with alkylating derivative of the same oligodeoxyribonucleotide. With high concentration of the reagents (II)--(IV) ((2-5) x 10(-5) M) the site-directed alkylation proceeds not only at the desired site but also at other sites corresponding to non-perfect duplexes between 16S rRNA and the reagents. It should be noted that the modification mainly occurs in the non-perfect duplexes, carrying mismatched bases at the termini. Influence of the secondary structure of 16S rRNA on the site-directed modification is discussed.     

Conformational changes in the oligonucleotide duplex d(GCGTTGCG) x d(CGCAACGC) induced by formation of a cis-syn thymine dimer. A two-dimensional NMR study

In order to obtain insight into the repair mechanism of DNA containing thymine photo-dimer, the conformation of the duplex d(GCGTTGCG) x d(CGCAACGC) with a thymine dimer incorporated has been studied by proton NMR and the results are compared with NMR data of the parent octamer. Two-dimensional nuclear Overhauser enhancement (2D NOE) spectroscopy and two-dimensional homonuclear Hartmann-Hahn spectroscopy have been applied to assign all the non-exchangeable base protons and most of the deoxyribose protons of both duplexes. From these experiments it is clear that indeed a cis-syn cyclobutane-type thymine photodimer is formed by the irradiation of this oligonucleotide with ultraviolet light. Comparison of 2D NOE spectra and the 1H chemical shifts of the damaged and the intact DNA duplexes reveals that formation of a thymine dimer induces small distortions of the B-DNA structure, the main conformational change occurring at the site of the thymine dimer.     

Kinetics for exchange of imino protons in the d(C-G-C-G-A-A-T-T-C-G-C-G) double helix and in two similar helices that contain a G . T base pair, d(C-G-T-G-A-A-T-T-C-G-C-G), and an extra adenine, d(C-G-C-A-G-A-A-T-T-C-G-C-G)

The relaxation lifetimes of imino protons from individual base pairs were measured in (I) a perfect helix, d(C-G-C-G-A-A-T-T-C-G-C-G), (II) this helix with a G . C base pair replaced with a G . T base pair, d(C-G-T-G-A-A-T-T-C-G-C-G), and (III) the perfect helix with an extra adenine base in a mismatch, d(C-G-C-A-G-A-A-T-T-C-G-C-G). The lifetimes were measured by saturation recovery proton nuclear magnetic resonance experiments performed on the imino protons of these duplexes. The measured lifetimes of the imino protons were shown to correspond to chemical exchange lifetimes at higher temperatures and spin-lattice relaxation times at lower temperatures. Comparison of the lifetimes in these duplexes showed that the destabilizing effect of the G . T base pair in II affected the opening rate of only the nearest-neighbor base pairs. For helix III, the extra adenine affected the opening rates of all the base pairs in the helix and thus was a larger perturbation for opening of the base pairs than the G . T base pair. The temperature dependence of the exchange rates of the imino proton in the perfect helix gives values of 14-15 kcal/mol for activation energies of A . T imino protons. These relaxation rates were shown to correspond to exchange involving individual base pair opening in this helix, which means that one base-paired imino proton can exchange independent of the others. For the other two helices that contain perturbations, much larger activation energies for exchange of the imino protons were found, indicating that a cooperative transition involving exchange of at least several base pairs was the exchange mechanism of the imino protons. The effects of a perturbation in a helix on the exchange rates and the mechanisms for exchange of imino protons from oligonucleotide helices are discussed.     

Influence of dA X dT and d(2aminoA) X dT base pairs on the B in equilibrium Z transition of DNA fragments. 1H-NMR study of d(C-G-C-A-m5C-G-T-G-m5C-G), d(m5C-G-C-A-m5C-G-T-G-C-G) and d(C-2aminoA-C-G-T-G)

The Helical structures of d(C-G-C-A-m5C-G-T-G-m5C-G), d(m5C-G-C-A-m5C-G-T-G-C-G) and d(C-2aminoA-C-G-T-G) were studied in aqueous solution at various salt concentrations and temperatures by 1H-NMR spectroscopy. In 0.1 M NaCl solution only the B form was evidenced for these DNA fragments whereas in 4 M NaCl both B and Z forms, in slow exchange on the NMR time scale, were observed. Under these conditions the Z form accounted for less than 60% of the decamer conformation; conversely d(C-G)3 hexamers containing methylated cytidines were predominantly in the Z form (greater than 90%) [Tran-Dinh et al. (1984) Biochemistry 23, 1362; Cavaillès et al. (1984) J. Biomol. Struct. Dyn. 1, 1347-1371]. On the other hand, d(C-2aminoA-C-G-T-G) in which the d(2aminoA) X dT base pair forms three hydrogen bonds, was found to adopt the Z conformation in 4M NaCl solution which was not the case for d(C-A-C-G-T-G) (unpublished results). The present study shows that the B in equilibrium Z transition in solution is highly sequence-dependent and that correlation exists between the stability of the duplexes (essentially governed by the number of hydrogen bonds between complementary bases) and their ability to adopt the Z conformation.     

Structure of poly d(A).poly d(T).

On the basis of the x-ray data from polycrystalline and well oriented fibers of the sodium salt of poly d(A).poly d(T) (Arnott et al, Nucl. Acids Res. 11, 4141-4155 (1983), a revised B'-DNA model incorporating B-like adenine and thymine strands is shown to give a much better x-ray agreement (R = 0.25) than the previously assigned model consisting of mixed sugar conformations in the two strands. The narrowing of the minor and the widening of the major grooves are promiscuous features of B'-DNA, which are common to all poly d(purine).poly d(pyrimidine) duplexes with two hydrogen bonded base-pairs and are in marked contrast with classical B-DNA. Due to modest propeller (-15 degrees), the cross strand diagonal hydrogen bonds (0.37 nm) in this duplex are not as strong as those in A,T-rich oligonucleotide crystal structures.     

Comparison of the solution and crystal conformations of (G + C)-rich fragments of DNA.

DNA fragments crystallize in an unpredictable manner, and relationships between their crystal and solution conformations still are not known. We have studied, using circular dichroism spectroscopy, solution conformations of (G + C)-rich DNA fragments, the crystal structures of which were solved in the laboratory of one of the present authors. In aqueous trifluorethanol (TFE) solutions, all of the examined oligonucleotides adopted the same type of double helix as in the crystal. Specifically, the dodecamer d(CCCCCGCGGGGG) crystalized as A-DNA and isomerized into A-DNA at high TFE concentrations. On the other hand, the hexamer d(CCGCGG) crystallized in Z-form containing tilted base pairs, and high TFE concentrations cooperatively transformed it into the same Z-form as adopted by the RNA hexamer r(CGCGCG), although d(CCGCGG) could isomerize into Z-DNA in the NaCl + NiCl2) aqueous solution. The fragments crystallizing as B-DNA remained B-DNA, regardless of the solution conditions, unless they denatured or aggregated. Effects on the oligonucleotide conformation of 2-methyl-2,4-pentanediol and other crystallization agents were also studied. 2-Methyl-2,4-pentanediol induced the same conformational transitions as TFE but, in addition, caused an oligonucleotide condensation that was also promoted by the other crystallization agents. The present results indicate that the crystal double helices of DNA are stable in aqueous TFE rather than aqueous solution.     

Crystal structure of the self-complementary 5''-purine start decamer d(GCACGCGTGC) in the A-DNA conformation. II.

The crystal structure of the alternating 5'-purine start decamer d(GCGCGCGCGC) was found to be in the left-handed Z-DNA conformation. Inasmuch as the A.T base pair is known to resist Z-DNA formation, we substituted A.T base pairs in the dyad-related positions of the decamer duplex. The alternating self-complementary decamer d(GCACGCGTGC) crystallizes in a different hexagonal space group, P6(1)22, with very different unit cell dimensions a = b = 38.97 and c = 77.34 A compared with the all-G.C alternating decamer. The A.T-containing decamer has one strand in the asymmetric unit, and because it is isomorphous to some other A-DNA decamers it was considered also to be right-handed. The structure was refined, starting with the atomic coordinates of the A-DNA decamer d(GCGGGCCCGC), by use of 2491 unique reflections out to 1.9-A resolution. The refinement converged to an R value of 18.6% for a total of 202 nucleotide atoms and 32 water molecules. This research further demonstrates that A.T base pairs not only resist the formation of Z-DNA but can also assist the formation of A-DNA by switching the helix handedness when the oligomer starts with a 5'-purine; also, the length of the inner Z-DNA stretch (d(CG)n) is reduced from an octamer to a tetramer. It may be noted that these oligonucleotide properties are in crystals and not necessarily in solutions.     

Binding of actinomycin D to single-stranded DNA of sequence motifs d(TGTCT(n)G) and d(TGT(n)GTCT)

Our recent binding studies with oligomers derived from base replacements on d(CGTCGTCG) had led to the finding that actinomycin D (ACTD) binds strongly to d(TGTCATTG) of apparent single-stranded conformation without GpC sequence. A fold-back binding model was speculated in which the planar phenoxazone inserts at the GTC site with a loop-out T base whereas the G base at the 3'-terminus folds back to form a basepair with the internal C and stacks on the opposite face of the chromophore. To provide a more concrete support for such a model, ACTD equilibrium binding studies were carried out and the results are reported herein on oligomers of sequence motifs d(TGTCT(n)G) and d(TGT(n)GTC). These oligomers are not expected to form dimeric duplexes and contain no canonical GpC sequences. It was found that ACTD binds strongly to d(TGTCTTTTG), d(TGTTTTGTC), and d(TGTTTTTGTC), all exhibiting 1:1 drug/strand binding stoichiometry. The fold-back binding model with displaced T base is further supported by the finding that appending TC and TCA at the 3'-terminus of d(TGTCTTTTG) results in oligomers that exhibit enhanced ACTD affinities, consequence of the added basepairing to facilitate the hairpin formation of d(TGTCTTTTGTC) and d(TGTCTTTTGTCA) in stabilizing the GTC/GTC binding site for juxtaposing the two G bases for easy stacking on both faces of the phenoxazone chromophore. Further support comes from the observation of considerable reduction in ACTD affinity when GTC is replaced by GTTC in an oligomer, in line with the reasoning that displacing two T bases to form a bulge for ACTD binding is more difficult than displacing a single base. Based on the elucidated binding principle of phenoxazone ring requiring its opposite faces to be stacked by the 3'-sides of two G bases for tight ACTD binding, several oligonucleotide sequences have been designed and found to bind well.     

Synthesis and physical characterization of DNA fragments containing N4-methylcytosine and 5-methylcytosine.

The synthesis of N4-methyl-2'-deoxycytidine and its fully protected mononucleotide, suitable for the oligonucleotide synthesis by phosphotriester method is described. A set of octanucleotides - d(CGCGCGCG), d(CG5mCGCGCG), d(CG4mCGCGCG) and dodecanucleotides - d(GGACCCGGGTCC), d(GGA5mCCCGGGTCC), d(GGA4mCCCGGGTCC) has been synthesized in a solution. Physical characterization of the oligonucleotide duplexes by means of UV and CD spectrometry provides the evidence that 4mC similarly to 5mC favours the B--greater than Z transition, although both of these methylated cytosines inhibit the B--greater than A conformational change. N4-Methylcytosine in contrast to 5-methylcytosine reduces the DNA double helix thermal stability.     

CD, absorption and thermodynamic analysis of repeating dinucleotide DNA, RNA and hybrid duplexes [d/r(AC)]12.[d/r(GT/U)]12 and the influence of phosphorothioate substitution.

Circular dichroism (CD) spectra and melting temperature (Tm) data for five duplexes containing phosphorothioate linkages were compared with data for four unmodified duplexes to assess the effect of phosphorothioate modification on the structure and stability of DNA. DNA and DNA.RNA duplexes. Nine duplexes were formed by mixing oligomers 24 nt long in 0.15 M K+(phosphate buffer), pH 7.0. Unmodified DNA.DNA and RNA.RNA duplexes were used as reference B-form and A-form structures. The CD spectra of the modified hybrids S-d(AC)12.r(GU)12 and r(AC)12.S-d(GT)12 differed from each other but were essentially the same as the spectra of the respective unmodified hybrids. They were more A-form than B-form in character. CD spectra of duplexes S-d(AC)12.d(GT)12 and d(AC)12.S-d(GT)12 were similar to that of d(AC)12.d(GT)12, except for a reduced long wavelength CD band. Sulfur modifications on both strands of the DNA duplex caused a pronounced effect on its CD spectrum. The order of thermal stability was: RNA.RNA > DNA.DNA > DNA.RNA > S-DNA.DNA > S-DNA. RNA > S-DNA.S-DNA. Phosphorothioation of one strand decreased the melting temperature by 7.8+/-0.6 degrees C, regardless of whether the substitution was in a hybrid or DNA duplex. Thermodynamic parameters were obtained from a multistate analysis of the thermal melting profiles. Interestingly, the destabilizing effect of the phosphorothioate substitution appears to arise from a difference in the entropy upon forming the DNA.DNA duplexes, while the destabilizing effect in the DNA.RNA hybrids appears to come from a difference in enthalpy.     

The structure and hydration of the A-DNA fragment d(GGGTACCC) at room temperature and low temperature.

The DNA fragment d(GGGTACCC) was crystallized as an A-DNA duplex in the hexagonal space group P6(1). The structure was analyzed at room temperature and low temperature (100K) at a resolution of 2.5 A. The helical conformations at the two temperatures are similar but the low-temperature structure is more economically hydrated than the room-temperature one. The structure of d(GGGTACCC) is compared to those of d(GGGTGCCC) and d(GGGCGCCC). This series of molecules, which consists of a mismatched duplex and its two Watson-Crick analogues, exhibits three conformational variants of the A-form of DNA, which are correlated with the specific intermolecular interactions observed in the various crystals. The largest differences in local conformation are displayed by the stacking geometries of the central pyrimidine-purine and the flanking purine-pyrimidine sites in each of the three duplexes. Stacking energy calculations performed on the crystal structures show that the mismatched duplex is destabilized with respect to each of the error-free duplexes, in accordance with helix-coil transition measurements.     

Crystal structure of the highly distorted chimeric decamer r(C)d(CGGCGCCG)r(G).spermine complex--spermine binding to phosphate only and minor groove tertiary base-pairing.

The crystal structure of the self-complementary chimeric decamer duplex r(C)d(CGGCGCCG)r(G), with RNA base pairs at both termini, has been solved at 1.9 A resolution by the molecular replacement method and refined to an R value of 0.145 for 2,314 reflections. The C3'-endo sugar puckers of the terminal riboses apparently drive the entire chimeric duplex into an A-DNA conformation, in contrast to the B-DNA conformation adopted by the all-deoxy decamer of the same sequence. Five symmetry related duplexes encapsulate a spermine molecule which interacts with ten phosphate groups, both directly and through water molecules to form multiple ionic and hydrogen bonding interactions. The spermine interaction severely bends the duplexes by 31 degrees into the major groove at the fourth base pair G(4).C(17), jolts it and slides the 'base plate' into the minor groove. This base pair, together with the adjacent base pair in the top half and the corresponding pseudo two-fold related base pairs in the bottom half, form four minor groove base-paired multiples with the terminal base pairs of two neighboring duplexes.