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.     

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.     

Effect of a single 3''-methylene phosphonate linkage on the conformation of an A-DNA octamer double helix.

The three-dimensional structure of the self-complementary DNA octamer d(GCCCGpGGC) has been determined in the crystalline state using X-ray diffraction data to a nominal resolutoin of 2.12 measured from a very small crystal at DESY, Hamburg. The structure was refined with stereochemical restraints to an R value of 17.1%. d(GCCCGpGGC), containing one single 3'-methylene phosphonate linkage (denoted p), forms an A-DNA double helix with strict dyad symmetry, that is distinct from canonical A-DNA by a wide open major groove and a small average base-pair inclination against the helix axis. The conformation of the unmodified control d(GCCCGGGC) is known from an X-ray analysis of isomorphous crystals (Heinemann et al. (1987) Nucleic Acids Res. 15, 9531-9550). Comparison of the two structures reveals only minor conformational differences, most notably in the pucker of the reduced deoxyribose. It is suggested that oligonucleotides with charged 3'-methylene phosphonate groups may form stable duplexes with complementary DNA or RNA strands rendering them candidates for use as gene-regulatory antisense probes.     

Proton nuclear magnetic resonance investigations of the nucleation and propagation reactions associated with the helix-coil transition of d-ApTpGpCpApT in H2O solution.

The chemical shifts and line widths of the Watson-Crick ring NH resonances of the self-complementary duplex of d-ApTpGpCpApT have been monitored in the presence of 0.1 M phosphate at neutral pH in aqueous solution. While the resonance positions of the terminal and internal AT base pairs shift upfield and broaden as average resonances with increasing temperature (helix and coil exchange several times prior to exchange with water from the coil form), those of the central GC base pairs broaden in the absence of upfield shifts (exchange with water occurs each time helix converts to coil). The line-width changes at the AT base pairs monitor the lifetime of the coil state at these positions prior to exchange with water while the line-width changes at the GC base pairs monitor the lifetime of the helix prior to dissociation to strands. This permits the separation of the propagation reaction at the AT base pairs from the nucleation reaction at the GC base pairs during helix formation. The experimental data have been quantitatively analyzed to yield (at 20 degrees) a nucleation formation rate of approximately 10(3) sec-1 for the GC base pairs (bimolecular rate constant of approximately 6 times 10(6) l. mol-1 sec-1) and a dissociation rate of 6 times 10(2) sec-1 at these same base pairs (unimolecular dissociation to strands). The unimolecular propagation reactions at the terminal and terminal base pairs are associated with reaction rates greater than 10(4) sec-1. These values are consistent with a slow formation of a stable nucleus at the GC base pairs followed by a rapid propagation reaction at the AT base pairs. The line width of the (GC) central base pairs in the presence of phosphate is a direct measure of the lifetime of the total helix and yields an activation energy of 45 kcal for helix to coil conversion measured over a narrow temperature range. The exchange from the coil form with water is catalyzed by 0.1 M phosphate with a rate constant kHPO2-/4 = 0.2 times 10(6) 1. mol-1 sec-1.     

Chiral phosphorothioate analogues of B-DNA. The crystal structure of Rp-d[Gp(S)CpGp(S)CpGp(S)C]

The compound Rp-d[Gp(S)CpGp(S)CpGp(S)C], an analogue of the deoxyoligomer d(G-C)3, crystallizes in space group P2(1)2(1)2(1) with a = 34.90 A, b = 39.15 A and c = 20.64 A. The structure, which is not isomorphous with any previously determined deoxyoligonucleotide, was refined to an R factor of 14.5% at a resolution of 2.17 A, with 72 solvent molecules located. The two strands of the asymmetric unit form a right-handed double helix, which is a new example of a B-DNA conformation and brings to light an important and overlooked component of flexibility of the double helix. This flexibility is manifest in the alternation of the backbone conformation between two states, defined by the adjacent torsion angles epsilon and zeta, trans . gauche-(BI) and gauche-. trans (BII). BI is characteristic of classical of B-DNA and has an average C(1') to C(1') separation of 4.5 A. The corresponding separation for BII is 5.3 A. Each state is associated with a distinct phosphate orientation where the plane of the PO2 (or POS) group is alternately near horizontal or vertical with respect to the helix axis. The BI and BII conformations are out of phase on the two strands. As a consequence, on one strand purine-pyrimidine stacking is better than pyrimidine-purine, while the converse holds for the other strand. At each base-pair step, good and bad stacking alternate across the helix axis. The pattern of alternation is regular in the context of a fundamental dinucleotide repeat. Re-examination of the B-DNA dodecamer d(C-G-C-G-A-A-T-T-C-G-C-G) shows that the C-G-C-G regions contain the BI and BII conformations, and the associated dual phosphate orientation and asymmetric base stacking. Different mechanisms are used in the two structures to avoid clashes between guanine residues on opposite strands, a combination of lateral slide, tilt and helical twist in the present structure, and base roll, tilt and longitudinal slide (Calladine rules) in the dodecamer. The flexibility of the phosphate orientations demonstrated in this structure is important, since it offers a structural basis for protein-nucleic acid recognition.     

Unusual duplex formation in purine rich oligodeoxyribonucleotides

The purine rich oligodeoxyribonucleotides 1C, d(ATGACGGAATA) and 2C, d(ATGAGCGAATA) alone exhibit highly cooperative melting transitions. Analysis of the concentration dependence of melting, and electrophoretic studies indicate that these oligomers can form an unusual purine rich offset double helix. The unusual duplex is predicted to contain four A.T, two G.C, and four G.A mismatch base pairs as well as a single A base stacked on the 3' end of each chain of the helix. Other possible models for the duplex are unlikely because they are predicted to contain many base pairs of low stability. Changing the central sequence to CGG or GGG should destabilize the duplex and this is observed. The unusual duplex of 2C is more stable than the duplex of 1C indicating that the stability of G.A base pairs is quite sensitive to the surrounding sequence. Addition of 1C and 2C to their complementary pyrimidine strands results in normal duplexes of similar stability. We feel that the unusual duplexes are significantly stabilized by the intrinsic stacking tendency of purine bases.     

The crystal structure of an RNA oligomer incorporating tandem adenosine-inosine mismatches.

The X-ray crystallographic structure of the RNA duplex [r(CGCAIGCG)]2 has been refined to 2.5 A. It shows a symmetric internal loop of two non-Watson-Crick base pairs which form in the middle of the duplex. The tandem A-I/I-A pairs are related by a crystallographic two-fold axis. Both A(anti)-I(anti) mismatches are in a head-to-head conformation forming hydrogen bonds using the Watson-Crick positions. The octamer duplexes stack above one another in the cell forming a pseudo-infinite helix throughout the crystal. A hydrated calcium ion bridges between the 3'-terminal of one molecule and the backbone of another. The tandem A-I mismatches are incorporated with only minor distortion to the backbone. This is in contrast to the large helical perturbations often produced by sheared G-A pairs in RNA oligonucleotides.     

Interactions of quinoxaline antibiotic and DNA: the molecular structure of a triostin A-d(GCGTACGC) complex

The crystal structure of a DNA octamer d(GCGTACGC) complexed to an antitumor antibiotic, triostin A, has been solved and refined to 2.2 A resolution by x-ray diffraction analysis. The antibiotic molecule acts as a true bis intercalator surrounding the d(CpG) sequence at either end of the unwound right-handed DNA double helix. As previously observed in the structure of triostin A-d(CGTACG) complex (A.H.-J. Wang, et. al., Science, 225, 1115-1121 (1984)), the alanine amino acid residues of the drug molecule form sequence-specific hydrogen bonds to guanines in the minor groove. The two central A.T base pairs are in Hoogsteen configuration with adenine in the syn conformation. In addition, the two terminal G.C base pairs flanking the quinoxaline rings are also held together by Hoogsteen base pairing. This is the first observation in an oligonucleotide of. Hoogsteen G.C base pairs where the cytosine is protonated. The principal functional components of a bis-intercalative compound are discussed.     

The structure of guanosine-thymidine mismatches in B-DNA at 2.5-A resolution

The structure of the deoxyoligomer d(C-G-C-G-A-A-T-T-T-G-C-G) was determined at 2.5-A resolution by single crystal x-ray diffraction techniques. The final R factor is 18% with the location of 71 water molecules. The oligomer crystallizes in a B-DNA-type conformation, with two strands interacting to form a dodecamer duplex. The double helix consists of four A X T and six G X C Watson-Crick base pairs and two G X T mismatches. The G X T pairs adopt a "wobble" structure with the thymine projecting into the major groove and the guanine into the minor groove. The mispairs are accommodated in the normal double helix by small adjustments in the conformation of the sugar phosphate backbone. A comparison with the isomorphous parent compound containing only Watson-Crick base pairs shows that any changes in the structure induced by the presence of G X T mispairs are highly localized. The global conformation of the duplex is conserved. The G X T mismatch has already been studied by x-ray techniques in A and Z helices where similar results were found. The geometry of the mispair is essentially identical in all structures so far examined, irrespective of the DNA conformation. The hydration is also similar with solvent molecules bridging the functional groups of the bases via hydrogen bonds. Hydration may be an important factor in stabilizing G X T mismatches. A characteristic of Watson-Crick paired A X T and G X C bases is the pseudo 2-fold symmetry axis in the plane of the base pairs. The G X T wobble base pair is pronouncedly asymmetric. This asymmetry, coupled with the disposition of functional groups in the major and minor grooves, provides a number of features which may contribute to the recognition of the mismatch by repair enzymes.     

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.     

Solution conformation of an oligonucleotide containing a G.G mismatch determined by nuclear magnetic resonance and molecular mechanics.

We have determined by two-dimensional nuclear magnetic resonance studies and molecular mechanics calculations the three dimensional solution structure of the non-selfcomplementary oligonucleotide, d(GAGGAGGCACG). d(CGTGCGTCCTC) in which the central base pair is G.G. This is the first structural determination of a G.G mismatch in a oligonucleotide. Two dimensional nuclear magnetic resonance spectra show that the bases of the mismatched pair are stacked into the helix and that the helix adopts a classical B-DNA form. Spectra of the exchangeable protons show that the two guanosines are base paired via their imino protons. For the non-exchangeable protons and for some of the exchangeable protons nuclear Overhauser enhancement build up curves at short mixing times have been measured. These give 84 proton-proton distances which are sensitive to the helix conformation. One of the guanosines adopts a normal anti conformation while the other is syn or close to syn. All non-terminal sugars are C2' endo. These data sets were incorporated into the refinement of the oligonucleotide structure by molecular mechanics calculations. The G.G mismatch shows a symmetrical base pairing structure. Although the mismatch is very bulky many of its features are close to that of normal B-DNA. The mismatch induces a small lateral shift in the helix axis and the sum of the helical twist above and below the mismatch is close to that of B-DNA.     

A solid-state deuterium NMR investigation of conformation and order in magnetically oriented [d(CGCGAATTCGCG)]2

Solid-state deuterium NMR has been used to investigate the oriented liquid crystal phase of the hydrated oligonucleotide [d(CGCGAATTCGCG)]2. Previous investigations have shown that the helix axis is aligned perpendicular to the magnetic field, while at reduced temperatures motion about the helix axis is eliminated. Synthetic oligonucleotide samples incorporating different labeled nucleosides, [2"-2H]-2'-deoxyadenosine, [methyl-2H]thymidine, [8-2H]-2'-deoxyguanosine, and [8-2H]-2'-deoxyadenosine, permitted investigation of both the base and sugar conformation and ordering in the aligned phase. From line-shape analysis of the purine-labeled samples the orientation of the base C8 C-D bond with respect to the helix axis was determined to be theta = 90 degrees with a distribution of sigma total = 20 degrees, which is comparable to the orientation of theta = 90 degrees, sigma total = 15 degrees, with an oriented fraction P = 0.7 found for the C3 symmetry axis of the methyl-labeled dodecamer. The orientation of the sugar 2" C-D bond with respect to the helix axis is theta = 22 degrees with a distribution of sigma total = 15 degrees in agreement with the expected C2'-endo sugar conformation. The fraction of C3'-endo was also investigated and from analysis of line shape cannot exceed 20%. These results, though preliminary in nature, illustrate the application of this aligned phase for structural investigations.     

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.     

A cytosine . cytosine base paired parallel DNA double helix with thymine . thymine bulges

500 MHz 1H NMR studies using 2D-NOESY indicate that the oligonucleotide d(CTCTCT) at low pH forms a parallel double helix with cytosine . cytosine base pairs and thymine . thymine bulges. This unusual structure may explain the hypersensitivity of S1 nuclease at low pH towards supercoiled plasmids containing d(CT)n inserts.     

Crystal structure of the B-DNA hexamer d(CTCGAG): model for an A-to-B transition.

The crystal structure of the B-DNA hexamer d(CTCGAG) has been solved at 1.9 A resolution by iterative single isomorphous replacement, using the brominated derivative d(CG5BrCGAG), and refined to an R-factor of 18.6% for 120 nonhydrogen nucleic acid atoms and 32 water molecules. Although the central four base pairs form a typical B-form helix, several parameters suggest a transition to an A-like conformation at the termini. Based on this observation, a B-to-A transition was modeled, maintaining efficient base stacking across the junction. The wide minor groove (approximately 6.9 A) is reminiscent of that in the side-by-side double drug-DNA complexes and hosts a double spine of hydration. The global helix axes of the pseudo-continuous helices are at an acute angle of 60 degrees. The pseudocontinuous stacking is reinforced by the minor groove water structure extending between the two duplexes. The crossover point of two pairs of stacked duplexes is at the stacking junction, unlike that observed in the B-DNA decamers and dodecamers. This arrangement may have implications for the structure of a four-way DNA junction. The duplexes are arranged around a large (approximately 20 A diameter) channel centered on a 6(2) screw axis.     

cis-diamminedichloroplatinum(II) induced distortion of a single and double stranded deoxydecanucleosidenonaphosphate studied by nuclear magnetic resonance

The structural distortion of a single- and a double-stranded decadeoxynucleotide upon binding of cis-PtCl2(NH3)2 was studied by 1H-NMR. After selective platination of d(T-C-T-C-G-G-T-C-T-C) (I) at the central d(-GpG-) site (resulting in I-Pt), several non-exchangeable base protons as well as H1', H2', H2" and H3' protons could be assigned by means of conventional NMR double-resonance techniques. Addition of the complementary decamer strand to I and I-Pt yielded the double-stranded III and III-Pt, respectively. All non-exchangeable base, H1', and most of the H2' and H2" protons in the two double stranded compounds could be assigned using 2D-chemical shift correlation (COSY) and nuclear Overhauser enhancement (NOESY) techniques. The double stranded compound III appears to adopt a B-DNA like structure. Comparison of NOEs and proton-proton coupling constants in the d(-GpG-).cisPt part in I-Pt and III-Pt reveals that their structure displays large similarity. Significant chemical shift changes (i.e. larger than 0.1 ppm) between III and III-Pt are restricted to the central four base pairs. It follows that the outer three base pairs, located on either side of the central four base pairs in III-Pt are likely to adopt a regular B-DNA type helix. The observed large upfield and downfield chemical shifts in the d(-CpGpG-) part of III with respect to III-Pt can be rationalized by describing the distortion of the double helix as a kink. A discussion of the observed physical effects upon platination of a double-stranded oligonucleotide is presented.     

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.     

Crystal structure of a 14 bp RNA duplex with non-symmetrical tandem GxU wobble base pairs

Adjacent GxU wobble base pairs are frequently found in rRNA. Atomic structures of small RNA motifs help to provide a better understanding of the effects of various tandem mismatches on duplex structure and stability, thereby providing better rules for RNA structure prediction and validation. The crystal structure of an RNA duplex containing the sequence r(GGUAUUGC-GGUACC)2 has been solved at 2.1 A resolution using experimental phases. Novel refinement strategies were needed for building the correct solvent model. At present, this is the only short RNA duplex structure containing 5'-U-U-3'/3'-G-G-5' non-symmetric tandem GxU wobble base pairs. In the 14mer duplex, the six central base pairs are all displaced away from the helix axis, yielding significant changes in local backbone conformation, helix parameters and charge distribution that may provide specific recognition sites for biologically relevant ligand binding. The greatest deviations from A-form helix occur where the guanine of a wobble base pair stacks over a purine from the opposite strand. In this vicinity, the intra-strand phosphate distances increase significantly, and the major groove width increases up to 3 A. Structural comparisons with other short duplexes containing symmetrical tandem GxU or GxT wobble base pairs show that nearest-neighbor sequence dependencies govern helical twist and the occurrence of cross-strand purine stacks.     

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.     

Interactions of Quinoxaline Antibiotic and DNA.: The Molecular Structure of a Triostin A—d(GCGTACGC) Complex

Abstract

The crystal structure of a DNA. octamer d(GCGTA.CGC) complexed to an antitumor antibiotic, triostin A, has been solved and refined to 2.2 Å resolution by x-ray diffraction analysis. The antibiotic molecule acts as a true bis intercalator surrouding the d(CpG) sequence at either end of the unwound right-handed DNA. double helix. A.s previously observed in the structure of triostin A.—d(CGTA.CG) complex (A.H.-J. Wang, et. al., Science, 225,1115–1121 (1984)), the alanine amino acid residues of the drug molecule form sequence-specific hydrogen bonds to guanines in the minor groove. The two central A · T base pairs are in Hoogsteen configuration with adenine in the syn conformation. In addition, the two terminal G · C base pairs flanking the quinoxaline rings are also held together by Hoogsteen base pairing. This is the first observation in an oligonucleotide of. Hoogsteen G · C base pairs where the cytosine is protonated. The principal functional components of a bis-intercalative compound are discussed.