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.     

Crystal structure of an RNA octamer duplex r(CCCIUGGG)2 incorporating tandem I.U wobbles.

The crystal structure of the RNA octamer duplex r(CCCIUGGG)2has been elucidated at 2.5 A resolution. The crystals belong to the space group P21and have unit cell constants a = 33.44 A, b = 43.41 A, c = 49.39 A and beta = 104.7 degrees with three independent duplexes (duplexes 1-3) in the asymmetric unit. The structure was solved by the molecular replacement method and refined to an Rwork/Rfree of 0.185/0.243 using 3765 reflections between 8.0 and 2.5 A. This is the first report of an RNA crystal structure incorporating I.U wobbles and three molecules in the asymmetric unit. Duplex 1 displays a kink of 24 degrees between the mismatch sites, while duplexes 2 and 3 have two kinks each of 19 degrees and 27 degrees, and 24 degrees and 29 degrees, respectively, on either side of the tandem mismatches. At the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for all base pair steps, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectively. The tandem I.U wobbles show intrastrand purine-pyrimidine stacking but exhibit interstrand purine-purine stacking with the flanking C.G pairs. The three independent duplexes are stacked non-coaxially in a head-to-tail fashion to form infinite pseudo-continuous helical columns which form intercolumn hydrogen bonding interactions through the 2'-hydroxyl groups where the minor grooves come together.     

NMR studies of pH-dependent conformational polymorphism of alternating (C-T)n sequences.

Alternating (C-T)n sequences are involved in the H-DNA structure associated with (GA)n.(CT)n sequences. Low pH values facilitate H-DNA formation. We have undertaken a detailed analysis of the structural consequences of the (C-T)n sequence as a function of pH. The structures of three DNA oligonucleotides, d(CT)4, d(TC)4 and d(TC)15, have been studied by NMR. We found that their conformations are polymorphic and pH dependent. There are at least three major conformational species: an antiparallel-stranded (APS) duplex with entirely C:T base pairs at pH 7, an antiparallel-stranded (APS) duplex with entirely C+:T base pairs at pH 3, and a possible parallel-stranded (PS) duplex with C+:C and T:T base pairs near pH 5. In the intermediate pH range, the APS duplex may have varying numbers of C+:T and C:T base pairs, and there may be a fast exchange going on between APS duplex species involving these two kinds of base pairs. However, the transition between the APS and PS duplexes is slow. Structural refinement of the two octamers, d(TC)4 and d(CT)4, at pH = 6.9 and pH = 3 using 2D-NOE data suggests that the molecules are likely in the duplex form at 5 degrees C. We lack evidence that the structure at pH 3 is a PS structure with T nucleotides residing in the exterior of the helix. Titration of the longer oligonucleotide, d(TC)15, showed a prominent pKa of approximately 6, approaching the value of 7.0 obtained from the titration of poly-(dC).     

Crystal structure of a B-DNA dodecamer containing inosine, d(CGCIAATTCGCG), at 2.4 A resolution and its comparison with other B-DNA dodecamers.

The crystal structure of the dodecamer, d(CGCIAATTCGCG), has been determined at 2.4 A resolution by molecular replacement, and refined to an R-factor of 0.174. The structure is isomorphous with that of the B-DNA dodecamer, d(CGCGAATTCGCG), in space group P2(1)2(1)2(1) with cell dimensions of a = 24.9, b = 40.4, and c = 66.4 A. The initial difference Fourier maps clearly indicated the presence of inosine instead of guanine. The structure was refined with 44 water molecules, and compared to the parent dodecamer. Overall the two structures are very similar, and the I:C forms Watson-Crick base pairs with similar hydrogen bond geometry to the G:C base pairs. The propeller twist angle is low for I4:C21 and relatively high for the I16:C9 base pair (-3.2 degrees compared to -23.0 degrees), and the buckle angles alter, probably due to differences in the contacts with symmetry related molecules in the crystal lattice. The central base pairs of d(CGCIAATTCGCG) show the large propeller twist angles, and the narrow minor groove that characterize A-tract DNA, although I:C base pairs cannot form the major groove bifurcated hydrogen bonds that are possible for A:T base pairs.     

Interaction between the Z-type DNA duplex and 1,3-propanediamine: crystal structure of d(CACGTG)2 at 1.2 A resolution

The crystal structure of a hexamer duplex d(CACGTG)(2) has been determined and refined to an R-factor of 18.3% using X-ray data up to 1.2 A resolution. The sequence crystallizes as a left-handed Z-form double helix with Watson-Crick base pairing. There is one hexamer duplex, a spermine molecule, 71 water molecules, and an unexpected diamine (Z-5, 1,3-propanediamine, C(3)H(10)N(2)) in the asymmetric unit. This is the high-resolution non-disordered structure of a Z-DNA hexamer containing two AT base pairs in the interior of a duplex with no modifications such as bromination or methylation on cytosine bases. This structure does not possess multivalent cations such as cobalt hexaammine that are known to stabilize Z-DNA. The overall duplex structure and its crystal interactions are similar to those of the pure-spermine form of the d(CGCGCG)(2) structure. The spine of hydration in the minor groove is intact except in the vicinity of the T5A8 base pair. The binding of the Z-5 molecule in the minor grove of the d(CACGTG)(2) duplex appears to have a profound effect in conferring stability to a Z-DNA conformation via electrostatic complementarity and hydrogen bonding interactions. The successive base stacking geometry in d(CACGTG)(2) is similar to the corresponding steps in d(CG)(3). These results suggest that specific polyamines such as Z-5 could serve as powerful inducers of Z-type conformation in unmodified DNA sequences with AT base pairs. This structure provides a molecular basis for stabilizing AT base pairs incorporated into an alternating d(CG) sequence.     

Structural variation in d(CTCTAGAG). Implications for protein-DNA interactions

Single-crystal X-ray diffraction techniques have been used to characterize the structure of the self-complementary DNA oligomer d(CTCTAGAG). The structure was refined to an R factor of 14.7% using data to 2.15-A resolution. The tetragonal unit cell, space group P4(3)2(1)2, has dimensions a = 42.53 and c = 24.33 A. The asymmetric unit consists of a single strand or four base pairs. Two strands, related by a crystallographic dyad axis, coil about each other to form a right-handed duplex. This octamer duplex has a mean helix rotation of 32 degrees, 11.3 base pairs per turn, an average rise of 3.1 A, C3'-endo furanose conformations, a shallow minor groove, and a deep major groove. Such averaged parameters suggest classification of the octamer as a member of the A-DNA family. However, the global parameters tend to mask variations in conformational parameters observed at the level of the base pairs. In particular, the central TpA (= TpA) step displays extensive interstrand purine-purine overlap and an unusual sugar-phosphate backbone conformation. These structural features may be directly related to certain sequence-specific protein-DNA interactions involving nucleases and repressors.     

Structural features and hydration of a dodecamer duplex containing two C.A mispairs.

X-ray diffraction techniques have been used to characterise the crystal and molecular structure of the deoxyoligomer d(C-G-C-A-A-A-T-T-C-G-C-G) at 2.5A resolution. The final R factor is 0.19 with the location of 78 solvent molecules. The oligomer crystallises in a B-DNA type conformation with two strands coiled about each other to produce a duplex. This double helix consists of four A.T and six G.C Watson-Crick base pairs and two C.A mispairs. The mismatched base pairs adopt a "wobble" type structure with the cytosine displaced laterally into the major groove, the adenine into the minor groove. We have proposed that the two close contacts observed in the C.A pairing represent two hydrogen bonds one of which results from protonation of adenine. The mispairs are accommodated in the double helix with small adjustments in the conformation of the sugar-phosphate backbone. Details of the backbone conformation, base stacking interactions, thermal parameters and the hydration are now presented and compared with those of the native oligomer d(C-G-C-G-A-A-T-T-C-G-C-G) and with variations of this sequence containing G.T and G.A mispairs.     

1H NMR study of the exchangeable protons of the duplex d(GCGTTGCG).d(CGCAACGC) containing a thymine photodimer.

A comparison is presented of the imino proton NMR spectra of the double stranded octamer d(GCGTTGCG).d(CGCAACGC) and the same octamer in which the two central thymine residues occur as a cis-syn thymine dimer. Except for the terminal base pairs all imino protons were detected and assigned in the NMR spectrum. The spectra show that in the thymine dimer duplex, contrary to common belief, all base pairs occur in a hydrogen bonded form, although the hydrogen bonds of the two central AT base pairs are substantially weakened. The melting temperature decreases about 13 degrees C on thymine dimer formation.     

Three-dimensional structure of d(GGGATCCC) in the crystalline state.

The structure of the self-complementary octamer d(GGGATCCC) has been analysed by single crystal X-ray diffraction methods at a nominal resolution of 2.5 A. With acceptable stereochemistry of the model the crystallographic R factor was 16.6% after restrained least-squares refinement. In the crystal, d(GGGATCCC) forms an A-DNA double helix with slightly varying conformation of the two strands. The average displacement of the base pairs from the helix axis is unusually large and is accompanied by pronounced sliding of the base pairs along their long axes at all dinucleotide steps except for the central AT. With 12 base pairs per complete turn the helix is considerably underwound. As observed with most oligodeoxyribonucleotides analysed by X-ray crystallography so far, the octamer displays reduced base pair tilt, increased rise per base pair and a more open major groove compared with canonical A-DNA. We propose that, based on these parameters, three A-helical sub-families may be defined; d(GGGATCCC) then is a representative of the class with intermediate tilt, rise, and major groove width.     

Structure and drug interactions of parallel-stranded DNA studied by infrared spectroscopy and fluorescence.

The infrared spectra of three different 25-mer parallel-stranded DNAs (ps-DNA) have been studied. We have used ps-DNAs containing either exclusively dA x dT base pairs or substitution with four dG x dC base pairs and have them compared with their antiparallel-stranded (aps) reference duplexes in a conventional B-DNA conformation. Significant differences have been found in the region of the thymine C = O stretching vibrations. The parallel-stranded duplexes showed characteristic marker bands for the C2 = O2 and C4 = O4 carbonyl stretching vibrations of thymine at 1685 cm-1 and 1668 cm-1, respectively, as compared to values of 1696 cm-1 and 1663 cm-1 for the antiparallel-stranded reference duplexes. The results confirm previous studies indicating that the secondary structure in parallel-stranded DNA is established by reversed Watson--Crick base pairing of dA x dT with hydrogen bonds between N6H...O2 and N1...HN3. The duplex structure of the ps-DNA is much more sensitive to dehydration than that of the aps-DNA. Interaction with three drugs known to bind in the minor groove of aps-DNA--netropsin, distamycin A and Hoechst 33258--induces shifts of the C = O stretching vibrations of ps-DNA even at low ratio of drug per DNA base pair. These results suggest a conformational change of the ps-DNA to optimize the DNA-drug interaction. As demonstrated by excimer fluorescence of strands labeled with pyrene at the 5'-end, the drugs induce dissociation of the ps-DNA duplex with subsequent formation of imperfectly matched aps-DNA to allow the more favorable drug binding to aps-DNA. Similarly, attempts to form a triple helix of the type d(T)n.d(A)n.d(T)n with ps-DNA failed and resulted in the dissociation of the ps-DNA duplex and reformation of a triple helix based upon an aps-DNA duplex core d(T)10.d(A)10.     

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.     

A parallel stranded linear DNA duplex incorporating dG.dC base pairs

DNA oligonucleotides with appropriately designed complementary sequences can form a duplex in which the two strands are paired in a parallel orientation and not in the conventional antiparallel double helix of B-DNA. All parallel stranded (ps) molecules reported to date have consisted exclusively of dA.dT base pairs. We have substituted four dA.dT base pairs of a 25-nt parallel stranded linear duplex (ps-D1.D2) with dG.dC base pairs. The two strands still adopt a duplex structure with the characteristic spectroscopic properties of the ps conformation but with a reduced thermodynamic stability. Thus, the melting temperature of the ps duplex with four dG.dC base pairs (ps-D5.D6) is 10-16 degrees C lower and the van't Hoff enthalpy difference delta HvH for the helix-coil transition is reduced by 20% (in NaCl) and 10% (in MgCl2) compared to that of ps-D1.D2. Based on energy minimizations of a ps-[d(T5GA5).d(A5CT5)] duplex using force field calculations we propose a model for the conformation of a trans dG.dC base pair in a ps helix.     

Circular dichroism spectra of DNA oligomers show that short interior stretches of C.C+ base pairs do not form in duplexes with A.T base pairs

Circular dichroism (CD) experiments were carried out on a series of DNA oligomers to determine if short internal stretches of protonated cytosine-cytosine (C.C+) base pairs could coexist with adenine-thymine (A.T) base pairs. (1) C.C+ base pairs did form in the absence of A.T base pairs in the individual oligomers d(AACC)5 and d(CCTT)5, as indicated by the appearance of a long-wavelength CD band centered at 282-284 nm, when the pH was lowered to 6 or 5 at 0.5 M Na+. A comparison of measured with calculated spectra showed that d(CCTT)5 at pH 5, 0.5 M Na+, 20 degrees C, likely adopted a structure with a central core of stacked C.C+ base pairs and looped-out thymines. Under the same conditions, it appeared that C.C+ base pairs also formed in d(AACC)5, but with the adenines remaining intrahelical. Each of these oligomers showed a cooperative transition for formation of C.C+ base pairs as the temperature was lowered, with C.C+ base pairs forming at a higher temperature in d(CCTT)5 than in d(AACC)5. A.T base formed in equimolar mixtures of d(AACC)5 plus d(CCTT)5 as monitored by an increase in the negative magnitude of the 250-nm CD band. However, a large increase did not appear at about 285 nm in CD spectra of the mixtures, showing that there were no stacked C.C+ base pairs in the d(AACC)5.d(CCTT)5 duplex even though they formed under the same conditions in the individual strands. Thus, in this duplex, A.T base pairs prevented the formation of neighboring internal C.C+ base pairs. (2) CD measurements were also made of d(A10C4T10).(ABSTRACT TRUNCATED AT 250 WORDS)     

The DNA sequence at echinomycin binding sites determines the structural changes induced by drug binding: NMR studies of echinomycin binding to [d(ACGTACGT)]2 and [d(TCGATCGA)]2

The complexes formed between the cyclic octadepsipeptide antibiotic echinomycin and the two DNA octamers [d(ACGTACGT)]2 and [d(TCGATCGA)]2 have been investigated by using one- and two-dimensional proton NMR spectroscopy techniques. The results obtained for the two complexes are compared to each other, to the crystal structures of related DNA-echinomycin complexes, and to enzymatic and chemical footprinting results. In the saturated complexes, two echinomycin molecules bind to each octamer by bisintercalation of the quinoxaline moieties on either side of each CpG step. Binding of echinomycin to the octamer [d(ACGTACGT)]2 is cooperative so that only the two-drug complex is observed at lower drug-DNA ratios, but binding to [d(TCGATCGA)]2 is not cooperative. At low temperatures, both the internal and terminal A.T base pairs adjacent to the binding site in the [d(ACGTACGT)]2-2 echinomycin complex are Hoogsteen base paired (Gilbert et al., 1989) as observed in related crystal structures. However, as the temperature is raised, the internal A.T Hoogsteen base pairs are destabilized and are observed to be exchanging between the Hoogsteen base-paired and an open (or Watson-Crick base-paired) state. In contrast, in the [d(TCGATCGA)]2-2 echinomycin complex, no A.T Hoogsteen base pairs are observed, the internal A.T base pairs appear to be stabilized by drug binding, and the structure of the complex does not change significantly from 0 to 45 degrees C. Thus, the structure and stability of the DNA in echinomycin-DNA complexes depends on the sequence at and adjacent to the binding site. While we conclude that no single structural change in the DNA can explain all of the footprinting results, unwinding of the DNA helix in the drug-DNA complexes appears to be an important factor while Hoogsteen base pair formation does not.     

Refined crystal structure of an octanucleotide duplex with G . T mismatched base-pairs

Single crystal X-ray diffraction techniques have been used to determine the structure of the DNA octamer d(G-G-G-G-C-T-C-C) at a resolution of 2.25 A. The asymmetric unit consists of two strands coiled about each other to produce an A-type DNA helix. The double helix contains six G . C Watson-Crick base-pairs and two G . T mismatched base-pairs. The mismatches adopt a "wobble" type structure in which both bases retain their major tautomer forms. The double helix is able to accommodate this G . T pairing with little distortion of the overall helical conformation. Crystals of this octamer melt at a substantially lower temperature than do those of a related octamer also containing two G . T base-pairs. We attribute this destabilization to disruption of the hydration network around the mismatch site combined with changes in intermolecular packing. Full details are given of conformational parameters, base stacking, intermolecular contacts and hydration involving 52 solvent molecules.     

Probing structural factors stabilizing antisense oligonucleotide duplexes: NMR studies of a DNA.DNA duplex containing a formacetal linkage.

The duplex formed by annealing the formacetal backbone modified dodecamer d-(CGCGTTOCH2OTTGCGC) to its complementary strand, d(GCGCAAAACGCG) (duplex I), has been studied by NMR techniques and analyzed with reference to its unmodified counterpart (duplex II). Comparison of parameters such as 2D cross-peak intensities, coupling constants, and spectral patterns indicates that structural perturbations caused by the incorporation of the formacetal linkage are minimal and localized to the central T4.A4 block. Duplex I adopts a B-type helical conformation with regular Watson-Crick base pairing and normal minor groove width. The methylene group is accommodated along the phosphate backbone in a conformation similar to that of the PO2 group found in the B-form DNA family. The central T6-T7 base pairs of duplex I melt simultaneously with the duplex, indicating a cooperative transition to single strands. Although the formacetal linkage affects global melting, as evidenced by a 3 degree C reduction in Tm for duplex I with respect to duplex II, the present study indicates that this is not the result of localized premelting at the formacetal site of duplex I but rather reflects the subtle interplay of several structural and energy factors which need to be further explored.     

Proton NMR study and conformational analysis of d(CGT), d(TCG) and d(CGTCG) in aqueous solution. The effect of a dangling thymidine and of a thymidine mismatch on DNA mini-duplexes

Proton NMR studies of d(CGT), d(TCG) and d(CGTCG) were carried out at 300 and 500 MHz. The temperature and concentration dependence of the chemical shifts of various resonances indicates duplex formation only in the cases of d(TCG) and d(CGTCG). It is concluded that d(TCG) forms a mini-duplex stabilized by a 5'-dangling thymine base. Thermodynamic parameters of the duplex-to-coil equilibrium of the d(TCG) duplex are: delta H0 = -22.3 kcal/mol and delta S0 = -70 cal/mol. K, which correspond to approximately 40% duplex formation at 0 degrees C in a 2 mM nucleotide solution. Comparison of these data with thermodynamic parameters given earlier [Borer, P.N., Dengler, B., Tinoco, I. and Uhlenbeck, O.C. (1974) J. Mol. Biol. 86, 843-853] leads to the conclusion that the dangling base stabilization observed here is approximately equivalent to the stabilization caused by one or two additional A . T base pairs. The chemical shift behaviour of various resonances in d(CGTCG) indicates duplex formation without looping out of the thymine bases. The T X T mismatch does not seem to disturb the helical structure to a large extent. Analysis of the vicinal proton-proton coupling constants of the three compounds yielded geometrical data for the sugar rings. The data are interpreted in terms of N and S pseudorotational ranges. It is shown that a distinct conformation-transmission effect is exerted by the guanosine residues in a 5'----3' direction.     

The crystal structure at 1.5 angstroms resolution of an RNA octamer duplex containing tandem G.U basepairs

The crystal structure of the RNA octamer, 5'-GGCGUGCC-3' has been determined from x-ray diffraction data to 1.5 angstroms resolution. In the crystal, this oligonucleotide forms five self-complementary double-helices in the asymmetric unit. Tandem 5'GU/3'UG basepairs comprise an internal loop in the middle of each duplex. The NMR structure of this octameric RNA sequence is also known, allowing comparison of the variation among the five crystallographic duplexes and the solution structure. The G.U pairs in the five duplexes of the crystal form two direct hydrogen bonds and are stabilized by water molecules that bridge between the base of guanine (N2) and the sugar (O2') of uracil. This contrasts with the NMR structure in which only one direct hydrogen bond is observed for the G.U pairs. The reduced stability of the r(CGUG)2 motif relative to the r(GGUC)2 motif may be explained by the lack of stacking of the uracil bases between the Watson-Crick and G.U pairs as observed in the crystal structure.