‘Chargaff's Rules’ for Protein Folding: Stoichiometric Leitmotif Made Visible

Abstract

The complex between cobalt hexammine and decadeoxyoligomer d(CGTACGTACG) crystallizes into the space group P6₅ with unit cell constants a = b = 17.93Å, and c = 43.41Å. The molecules have the helix axis coincident with the crystal c-axis. The decamers stack on top of each other and form a quasi-continuous helix. The structure is disordered. The asymmetric unit is a dimer (pPyr-pPur)₂ with each base pair 60% of the time a C-G and 40% of the time a T-A. Restrainted least-squares refinement led to an R-factor of 25.5% for 506 observed reflections above the two-sigma level. The structure was found to have one strand in the Z_I-conformation and the other in the Z_II-conformation. The cobalt hexammine binds to two Z_II-chains of symmetrically related molecules. On one Z_II chain, two ammonia molecules of the cobalt hexammine bind to the N7 nitrogen and 06 oxygen atoms of the guanine bases and a third ammonia to the phosphate anionic oxygen atom of the preceding pyrimidine base, resulting in an “external” binding mode. On the other Z_II chain, one ammonia molecule of the cobalt hexammine binds only to the anionic oxygens of the phosphate group of the guanine bases, leading to an “internal” binding mode. Thus, the basis of the stabilization of Z-DNA by [Co(NH₃)₆]³⁺ is its binding to only guanine nucleotides. It is surmised that statistical disordering of deoxyoligonucleotide structures which take a Z conformation, depends on the length of the oligomer. That is to say, octamers and decamers (which cannot use an integral number of molecules for a 12 base pair repeat) form disordered structures whereas tetramers and hexamers form well ordered structures.     

Cobalt hexammine induced tautomeric shift in Z-DNA: the structure of d(CGCGCA)*d(TGCGCG) in two crystal forms

We report here the crystal structure of the DNA hexamer duplex d(CGCGCA).d(TGCGCG) at 1.71 Å resolution. The crystals, in orthorhombic space group, were grown in the presence of cobalt hexammine, a known inducer of the left-handed Z form of DNA. The interaction of this ion with the DNA helix results in a change of the adenine base from the common amino tautomeric form to the imino tautomer. Consequently the A:T base pair is disrupted from the normal Watson–Crick base pairing to a ‘wobble’ like base pairing. This change is accommodated easily within the helix, and the helical parameters are those expected for Z-DNA. When the cobalt hexammine concentration is decreased slightly in the crystallization conditions, the duplex crystallizes in a different, hexagonal space group, with two hexamer duplexes in the asymmetric unit. One of these is situated on a crystallographic 6-fold screw axis, leading to disorder. The tautomeric shift is not observed in this space group. We show that the change in inter-helix interactions that lead to the two different space groups probably arise from the small decrease in ion concentration, and consequently disordered positions for the ion.     

The interactions of ruthenium hexaammine with Z-DNA: crystal structure of a Ru(NH3)6+3 salt of d(CGCGCG) at 1.2 A resolution

A crystal of d(CGCGCG) in the Z-DNA lattice was soaked with ruthenium(III) hexaammine and its structure refined at 1.2 A resolution. Three unique metal complexes were found absorbed to each hexamer duplex. In addition, two symmetry-related binding sites were located, yielding a total of five ruthenium complexes bound to each d(CGCGCG) duplex. One unique site and its symmetry related site are nearly identical to the binding site of cobalt(III) hexaammine on Z-DNA. At that position, the metal complex bridges the convex surfaces of two adjacent Z-DNA strands by hydrogen bonds to the N7 and O6 functional groups of the guanine bases. The remaining three ruthenium three ruthenium(III) hexaammine binding sites are not present in the cobalt(III) hexaammine Z-DNA structure. Of these, two are related by symmetry and span the gap between the convex outer surface of one Z-DNA strand and the helical groove crevice of a neighboring strand. The third ruthenium site has no symmetry mate and involves interactions with only the deep groove. In this interaction, the metal complex hydrogen bonds to both the phosphate backbone and to a set of primary shell water molecules that extend the hydrogen bonding potential of the deep groove crevice out to the surface of the molecule. Solution studies comparing the circular dichroism spectra of low salt poly(dG-dC).poly(dG-dC) samples in the presence of ruthenium(III) and cobalt(III) hexammine show that the ruthenium complex does stabilize Z-DNA in solution, but not as effectively as the cobalt analogue. This suggests that some of the interactions available for the larger ruthenium complex may not be important for stabilization of the left-handed DNA conformation.     

Structural and electrostatic effects on binding of trivalent cations to double-stranded and single-stranded poly[d (AT)

We have measured the thermal melting profile for poly[d(AT)].poly[d(TA)] as a function of concentration of three trivalent cations: spermidine, me8spermidine, and hexammine cobalt(III). Using McGhee's (1976) theory of DNA melting in the presence of ligands, we have estimated association constants Kh, Kc and binding site sizes nh, nc for binding to double-helical (h) and single-stranded (c) polynucleotide. The results are as follows: (table; see text) The binding parameters for spermidine and hexammine cobalt(III) to double helical molecules agree fairly well with direct equilibrium dialysis measurements, and are in reasonable accord with predictions of counterion condensation theory. However, despite their identical charges, the three ligands bind to single-stranded DNA with quite different affinities. Estimates of the charge spacing of single-stranded DNA suggest that poly[d(AT)] is less elongated in the presence of spermidine and hexammine cobalt(III) than it is when complexed with me8spermidine.     

Covalent modification of guanine bases in double-stranded DNA. The 1.2-A Z-DNA structure of d(CGCGCG) in the presence of CuCl2

We have solved the single crystal structure to 1.2-A resolution of the Z-DNA sequence d(CGCGCG) soaked with copper(II) chloride. This structure allows us to elucidate the structural properties of copper in a model that mimics a physiologically relevant environment. A copper(II) cation was observed to form a covalent coordinate bond to N-7 of each guanine base along the hexamer duplex. The occurrence of copper bound at each site was dependent on the exposure of the bases and the packing of the hexamers in the crystal. The copper at the highest occupied site was observed to form a regular octahedral complex, with four water ligands in the equatorial plane and a fifth water along with N-7 of the purine base at the axial positions. All other copper complexes appear to be variations of this structure. By using the octahedral complex as the prototype for copper(II) binding to guanine bases in the Z-DNA crystal, model structures were built showing that duplex B-DNA can accommodate octahedral copper(II) complexes at the guanine bases as well as copper complexes bridged at adjacent guanine residues by a reactive dioxygen species. The increased susceptibility to oxidative DNA cleavage induced by copper(II) ions in solution of the bases located 5' to one or more adjacent guanine residues can thus be explained in terms of the cation and DNA structures described by these models.     

A theoretical model for the binding of cis-Pt(NH3)2(+2) to DNA

The binding of cis-Pt(NH3)2B1B2 to the bases B1 and B2, i.e., guanine (G), cytosine (C), adenine (A), and thymine (T), of DNA is studied theoretically. The components of the binding are analyzed and a model structure is proposed for the intrastrand binding to the dB1pdB2 sequence of a kinked double helical DNA. Quantum mechanical calculations of the ligand binding energy indicates that cis-Pt(NH3)2(+2) (cis-PDA) binds to N7(G), N3(C), O2(C), O6(G), N3(A), N7(A), O4(T) and O2(T) in order of decreasing binding energy. Conformational analysis provides structures of kinked DNA in which adjacent bases chelate to cis-PDA. Only bending toward the major groove allows the construction of acceptable square planar complexes. Examples are presented for kinks of -70 degrees and -40 degrees at the receptor site to orient the base pairs for ligand binding to B1 and B2 to form a nearly square planar complex. The energies for complex formation of cis-PDA to the various intra-strand base sites in double stranded DNA are estimated. At least 32 kcal/mole separates the energetically favorable dGpdG.cis-PDA chelate from the dCpdG.cis-PDA chelate. All other possible chelate structures are much higher in energy which correlates with their lack of observation in competition with the preferred dGpdG chelate. The second most favorable ligand energy occurs with N3(C). A novel binding site involving dC(N3)pdG(N7) is examined. Denaturation can result in an anti----syn rotation of C about its glycosidic bond to place N3(C) in the major groove for intrastrand binding in duplex DNA. This novel intrastrand dCpdG complex and the most favored dGpdG structure are illustrated with stereographic projections.     

Influence of counter-ions on the crystal structures of DNA decamers: binding of [Co(NH3)6]3+ and Ba2+ to A-DNA.

A-DNA is a stable alternative right-handed double helix that is favored by certain sequences (e.g., (dG)n.(dC)n) or under low humidity conditions. Earlier A-DNA structures of several DNA oligonucleotides and RNA.DNA chimeras have revealed some conformational variation that may be the result of sequence-dependent effects or crystal packing forces. In this study, four crystal structures of three decamer oligonucleotides, d(ACCGGCCGGT), d(ACCCGCGGGT), and r(GC)d(GTATACGC) in two crystal forms (either the P6(1)22 or the P2(1)2(1)2(1) space group) have been analyzed at high resolution to provide the molecular basis of the structural difference in an experimentally consistent manner. The study reveals that molecules crystallized in the same space group have a more similar A-DNA conformation, whereas the same molecule crystallized in different space groups has different (local) conformations. This suggests that even though the local structure is influenced by the crystal packing environments, the DNA molecule adjusts to adopt an overall conformation close to canonical A-DNA. For example, the six independent CpG steps in these four structures have different base-base stacking patterns, with their helical twist angles (omega) ranging from 28 degrees to 37 degrees. Our study further reveals the structural impact of different counter-ions on the A-DNA conformers. [Co(NH3)6]3+ has three unique A-DNA binding modes. One binds at the major groove side of a GpG step at the O6/N7 sites of guanine bases via hydrogen bonds. The other two modes involve the binding of ions to phosphates, either bridging across the narrow major groove or binding between two intra-strand adjacent phosphates. Those interactions may explain the recent spectroscopic and NMR observations that [Co(NH3)6]3+ is effective in inducing the B- to A-DNA transition for DNA with (G)n sequence. Interestingly, Ba2+ binds to the same O6/N7 sites on guanine by direct coordinations.     

Molecular biological analysis of sequence-specific DNA recognition and cleavage by metallobleomycins

The DNase I footprinting analysis shows binding sites of approximately two or three base pairs, in particular 5'-XGC sequences, for the green-colored Co(III) and fully oxidized Fe(III) complexes of bleomycin (BLM). In contrast to covalent attachment of guanine N-7 with aflatoxin B1 or dimethyl sulfate, the modification of guanine 2-amino group with anthramycin remarkably inhibits the DNA cleavages at 5'-GC and 5'-GT sites by the iron and cobalt complex systems of BLM. The present results strongly indicate that metallobleomycin binds in minor groove of B-DNA and that the 2-amino group of guanine adjacent to 5'-side of the cleaved pyrimidine base is one key element of specific 5'-GC or 5'-GT recognition by metallobleomycin. On the basis of these experimental data, possible binding mode of metallobleomycin in B-DNA helix has been proposed by computer-constructed model building.     

M.HhaI binds tightly to substrates containing mismatches at the target base.

The (cytosine-5) DNA methyltransferase M.HhaI causes its target cytosine base to be flipped completely out of the DNA helix upon binding. We have investigated the effects of replacing the target cytosine by other, mismatched bases, including adenine, guanine, thymine and uracil. We find that M.HhaI binds more tightly to such mismatched substrates and can even transfer a methyl group to uracil if a G:U mismatch is present. Other mismatched substrates in which the orphan guanine is changed exhibit similar behavior. Overall, the affinity of DNA binding correlates inversely with the stability of the target base pair, while the nature of the target base appears irrelevant for complex formation. The presence of a cofactor analog. S-adenosyl-L-homocysteine, greatly enhances the selectivity of the methyltransferase for cytosine at the target site. We propose that the DNA methyltransferases have evolved from mismatch binding proteins and that base flipping was, and still is, a key element in many DNA-enzyme interactions.     

Interactions of nucleic acids with distamycins. Binding of Dst-3 to d(CGTTTAAACG)2 and d(CGTACGTACG)2.

The binding between Distamycin 3 and the palindromic duplexes d(CGTTTAAACG)2 and d(CGTACGTACG)2 was investigated by two independent techniques: UV-Vis absorption in the Job's plot approach and Induced Circular Dichroism. Both decamers bind two molecules of peptide per duplex, with close overall affinities. This result indicates that a row of six A:T base pairs can accommodate two molecules of drug and that the minimal binding site of Distamycin 3 can consist of just two A:T base pairs.     

G . T base-pairs in a DNA helix: the crystal structure of d(G-G-G-G-T-C-C-C)

The synthetic deoxyoctanucleotide d(G-G-G-G-T-C-C-C) crystallizes as an A-type DNA double helix containing two adjacent G . T base-pair mismatches. The structure has been refined to an R-factor of 14% at 2.1 A resolution with 104 solvent molecules located. The two G . T mismatches adopt the "wobble" form of base-pairing. The mismatched bases are linked by a network of water molecules interacting with the exposed functional groups in both the major and minor grooves. The presence of two mispaired bases in the octamer has surprisingly little effect on the global structure of the helix or the backbone and glycosidic torsional angles. Base stacking around the mismatch is perturbed, but the central G-T step shows particularly good base overlap, which may contribute to the relatively high stability of this oligomer.     

1 A crystal structures of B-DNA reveal sequence-specific binding and groove-specific bending of DNA by magnesium and calcium

The 1 A resolution X-ray crystal structures of Mg(2+) and Ca(2+) salts of the B-DNA decamers CCAACGTTGG and CCAGCGCTGG reveal sequence-specific binding of Mg(2+) and Ca(2+) to the major and minor grooves of DNA, as well as non-specific binding to backbone phosphate oxygen atoms. Minor groove binding involves H-bond interactions between cross-strand DNA base atoms of adjacent base-pairs and the cations' water ligands. In the major groove the cations' water ligands can interact through H-bonds with O and N atoms from either one base or adjacent bases, and in addition the softer Ca(2+) can form polar covalent bonds bridging adjacent N7 and O6 atoms at GG bases. For reasons outlined earlier, localized monovalent cations are neither expected nor found.Ultra-high atomic resolution gives an unprecedented view of hydration in both grooves of DNA, permits an analysis of individual anisotropic displacement parameters, and reveals up to 22 divalent cations per DNA duplex. Each DNA helix is quite anisotropic, and alternate conformations, with motion in the direction of opening and closing the minor groove, are observed for the sugar-phosphate backbone. Taking into consideration the variability of experimental parameters and crystal packing environments among these four helices, and 24 other Mg(2+) and Ca(2+) bound B-DNA structures, we conclude that sequence-specific and strand-specific binding of Mg(2+) and Ca(2+) to the major groove causes DNA bending by base-roll compression towards the major groove, while sequence-specific binding of Mg(2+) and Ca(2+) in the minor groove has a negligible effect on helix curvature. The minor groove opens and closes to accommodate Mg(2+) and Ca(2+) without the necessity for significant bending of the overall helix.The program Shelxdna was written to facilitate refinement and analysis of X-ray crystal structures by Shelxl-97 and to plot and analyze one or more Curves and Freehelix output files.     

Sequence-dependent conformation of an A-DNA double helix. The crystal structure of the octamer d(G-G-T-A-T-A-C-C)

The crystal structures of the synthetic self-complementary octamer d(G-G-T-A-T-A-C-C) and its 5-bromouracil-containing analogue have been refined to R values of 20% and 14% at resolutions of 1.8 and 2.25 A, respectively. The molecules adopt and A-DNA type double-helical conformation, which is minimally affected by crystal forces. A detailed analysis of the structure shows a considerable influence of the nucleotide sequence on the base-pair stacking patterns. In particular, the electrostatic stacking interactions between adjacent guanine and thymine bases produce symmetric bending of the double helix and a major-groove widening. The sugar-phosphate backbone appears to be only slightly affected by the base sequence. The local variations in the base-pair orientation are brought about by correlated adjustments in the backbone torsion angles and the glycosidic orientation. Sequence-dependent conformational variations of the type observed here may contribute to the specificity of certain protein-DNA interactions.     

Structural characterization of d(CAACCCGTTG) and d(CAACGGGTTG) mini-hairpin loops by heteronuclear NMR: the effects of purines versus pyrimidines in DNA hairpins.

The DNA decamers, d(CAACCCGTTG) and d(CAACGGGTTG) were studied in solution by proton and heteronuclear NMR. Under appropriate conditions of pH, temperature, salt concentration and DNA concentration, both decamers form hairpin conformations with similar stabilities [Avizonis and Kearns (1995) Biopolymers, 35, 187-200]. Both decamers adopt mini-hairpin loops, where the first and last four nucleotides are involved in Watson-Crick hydrogen bonding and the central two nucleotides, CC or GG respectively, form the loop. Through the use of proton-proton, proton-phosphorus and natural abundance proton-carbon NMR experiments, backbone torsion angles (beta, gamma and epsilon), sugar puckers and interproton distances were measured. The nucleotides forming the loops of these decamers were found to stack upon one another in an L1 type of loop conformation. Both show gamma tr and unusual beta torsion angles in the loop-closing nucleotide G7, as expected for mini-hairpin loop formation. Our results indicate that the beta and epsilon torsion angles of the fifth and sixth nucleotides that form the loop and the loop-closing nucleotide G7 are not in the standard trans conformation as found in B-DNA. Although the loop structures calculated from NMR-derived constraints are not well defined, the stacking of the bases in the two different hairpins is different. This difference in the base stacking of the loop may provide an explanation as to why the cytosine-containing hairpin is thermodynamically more stable than the guanine-containing hairpin.     

Nitrogen-15 chemical shifts in AT (adenine-thymine) and CG (cytosine-guanine) nucleic acid base pairs

This paper presents ab initio (DFT) calculations of the 15N chemical shifts in AT (Adenine-Thymine) and CG (Cytosine-Guanine) nucleic acid base pairs. Calculations were done on 14 AT and 18 CG base pairs using experimental (X-ray) geometries obtained from several DNA decamers. The calculated chemical shifts are compared with the experimental values in the pure bases and subjected to statistical analysis to explore their sensitivity to the local geometry and pair helix parameters. The results indicate that the 15N chemical shifts, isotropic and principal components are quite sensitive to small changes in the geometry of the pairs, but they do not correlate well with the helix pair parameters. From the statistical analysis, several linear correlations between structural parameters and chemical shifts emerge. These relationships may serve as a foundation to extract information on molecular structure from 15N chemical shift measurements.     

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.     

Three-dimensional structure of a mutant ribonuclease T1 (Y45W) complexed with non-cognizable ribonucleotide, 2'AMP, and its comparison with a specific complex with 2'GMP.

The crystal structure of a mutant ribonuclease T1 (Y45W) complexed with a non-cognizable ribonucleotide, 2'AMP, has been determined and refined to an R-factor of 0.159 using X-ray diffraction data at 1.7 A resolution. A specific complex of the enzyme with 2'GMP was also determined and refined to an R-factor of 0.173 at 1.9 A resolution. The adenine base of 2'AMP was found at a base-binding site that is far apart from the guanine recognition site, where the guanine base of 2'GMP binds. The binding of the adenine base is mediated by a single hydrogen bond and stacking interaction of the base with the imidazole ring of His92. The mode of stacking of the adenine base with His92 is similar to the stacking of the guanine base observed in complexes of ribonuclease T1 with guanylyl-2',5'-guanosine, reported by Koepke et al., and two guanosine bases, reported by Lenz et al., and in the complex of barnase with d(GpC), reported by Baudet & Janin. These observations suggest that the site is non-specific for base binding. The phosphate group of 2'AMP is tightly locked at the catalytic site with seven hydrogen bonds to the enzyme in a similar manner to that of 2'GMP. In addition, two hydrogen bonds are formed between the sugar moiety of 2'AMP and the enzyme. The 2'AMP molecule adopts the anti conformation of the glycosidic bond and C-3'-exo sugar pucker, whereas 2'GMP is in the syn conformation with C-3'-endo-C'-2'-exo pucker. The mutation enhances the binding of 2'GMP with conformational changes of the sugar ring and displacement of the phosphate group towards the interior of the catalytic site from the corresponding position in the wild-type enzyme complex. Comparison of two crystal structures obtained provides a solution to the problem that non-cognizable nucleotides exhibit unexpectedly strong binding to the enzyme, compared with high specificity in nucleolytic activity. The results indicate that the discrimination of the guanine base from the other nucleotide bases at the guanine recognition site is more effective than that estimated from nucleotide-binding experiments so far.     

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).     

Thermodynamics of DNA binding and condensation: isothermal titration calorimetry and electrostatic mechanism

The thermodynamics of binding of the trivalent cations cobalt hexammine and spermidine to plasmid DNA was studied by isothermal titration calorimetry. Two stages were observed in the course of titration, the first attributed to cation binding and the second to DNA condensation. A standard calorimetric data analysis was extended by applying an electrostatic binding model, which accounted for most of the observed data. Both the binding and condensation reactions were entropically driven (TDeltaS approximately +10 kcal/mol cation) and enthalpically opposed (DeltaH approximately +1 kcal/mol cation). As predicted from their relative sizes, the binding constants of the cations were indistinguishable, but cobalt hexammine had a much greater DNA condensing capacity because it is more compact than spermidine. The dependence of both the free energy of cobalt hexammine binding and the critical cobalt hexammine concentration for DNA condensation on temperature and monovalent cation concentration followed the electrostatic model quite precisely. The heat capacity changes of both stages were positive, perhaps reflecting both the temperature dependence of the dielectric constant of water and the burial of polar surfaces. DNA condensation occurred when about 67 % of the DNA phosphate charge was neutralized by cobalt hexammine and 87 % by spermidine. During condensation, the remaining DNA charge was neutralized.     

Molecular structure of deoxycytidyl-3''-methylphosphonate (RP) 5''-deoxyguanidine, d[Cp(CH3)G]. A neutral dinucleotide with Watson-Crick base pairing and a right handed helical twist.

The crystal structure of d[Cp(CH3)G] has been determined as part of a project to study the mechanism of the B----Z transition in DNA. The asymmetric unit contains two dinucleotides and the equivalent of 7.5 water molecules, partially disordered over 12 definable positions. The two symmetry-independent dinucleotides form a duplex with Watson-Crick base-pairing and a right-handed helical sense. Comparison with previously determined structures of the B and A conformation showed that this duplex is closer to B than to A but significantly different from B. It corresponds to a stretched out helix with a 4 A rise per base pair and a helical twist of 32 degrees. This structure may serve as a model for the bending of DNA in certain situations. The configuration at the methyl phosphonate is RP, and a mechanism, based on this assignment, is presented for the B----Z transition in DNA.