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.     

Parallel DNA double helices. II. Conformational analysis of regular helices having a second order axis of symmetry

Conformational analysis of double helices of DNA with parallel arranged sugar-phosphate chains connected by twofold symmetry has been performed. Homopolymers poly(dA).poly(dA), poly(dC).poly(dC), poly(dG).poly(dG) and poly(dT).poly(dT) were studied. For each of the homopolymers all variants of H-bond pairing were checked. The maps of closing of sugar-phosphate backbone were previously computed. By the optimization of potential energy the dihedral angles and helix parameters of relatively stable conformations of parallel stranded polynucleotides were calculated. The dependence of conformational energy on the nucleic base character and the base pair type were studied. Two main conformational regions for favourable "parallel" helix of polynucleotides were found. The former of these two regions coincide with the region of typical conformational parameters of B-DNA. On an average the conformational energy of "parallel" DNA is close to the energy of canonic "antiparallel" B-DNA.     

Anisotropic flexibility of DNA depends on the base sequence. Conformation calculations of double-stranded tetranucleotides AAAA:TTTT, (AATT)2, (TTAA)2, GGGG:CCCC, (GGCC)2, (CCGG)2

The bending flexibility of six tetramers was studied in an assumption that they were extended in the both directions by regular double helices. The bends of B-DNA in different directions were considered. The stiffness of the B-DNA double helix when bent into the both grooves proved to be less pronounced than in the perpendicular direction by the order of magnitude. Such an anisotropy is a feature of the sugar-phosphate backbone structure. The calculated fluctuations of the DNA bending along the dyad axis, 5-7 degrees, are in agreement with the experimental value of DNA persistence length. Anisotropy of the double helix is sequence-dependent: most easily bent into the minor groove are the tetramers with purine-pyrimidine dimer (RY) in the middle. In contrast, YR dinucleotides prefer bending into the major groove, moreover, they have an equilibrium bend of 6-12 degrees into this groove. The above inequality is caused by the stacking interaction of the bases. The bend in the central dimers is distributed to some extent between the adjacent links, though the main fraction of the bend remains within the central link. Variation of the sugar-phosphate geometry in the bent helix is unessential, so that DNA remains within the limits of the B-family of forms: namely, when the helical axis is bent by 20 degrees the backbone dihedral angles vary by no more than 15 degrees. The obtained results are in accord with the X-ray structure of B-DNA dodecamer; they further substantiate our earlier model of DNA wrapping in the nucleosome by means of "mini-kinks" separated by a half-pitch of the double helix, i.e. by 5-6 b. p. Sequence-dependent anisotropy of DNA presumably dictates the three-dimensional structure of DNA in solution as well. We have found that nonrandom allocation of YR dimers leads to the systematic bends in the equilibrium structure of certain DNA fragments. To the four "Calladine rules" two more can be added: the minor-groove steric clash of purines in the YR sequences are avoided by: (1) bending of the helix into the major groove; (2) increasing the distance between the base pairs (stretching the double helix).     

Solution structures of aminofluorene [AF]-stacked conformers of the syn [AF]-C8-dG adduct positioned opposite dC or dA at a template-primer junction.

A solution structural study has been undertaken on the aminofluorene-C8-dG ([AF]dG) adduct located at a single-strand-double-strand d(A1-A2-C3-[AF]G4-C5-T6-A7-C8-C9-A10-T11-C12-C13). d(G14-G15-A16-T17-G18-G19-T20- A21-G22-N23) 13/10-mer junction (N = C or A) using proton-proton distance restraints derived from NMR data in combination with intensity-based relaxation matrix refinement computations. This single-strand-double-strand junction models one arm of a replication fork composed of a 13-mer template strand which contains the [AF]dG modification site and a 10-mer primer strand which has been elongated up to the modified guanine with either its complementary dC partner or a dA mismatch. The solution structures establish that the duplex segment retains a minimally perturbed B-DNA conformation with Watson-Crick hydrogen-bonding retained up to the dC5.dG22 base pair. The guanine ring of the [AF]dG4 adduct adopts a syn glycosidic torsion angle and is displaced into the major groove when positioned opposite dC or dA residues. This base displacement of the modified guanine is accompanied by stacking of one face of the aminofluorene ring of [AF]dG4 with the dC5.dG22 base pair, while the other face of the aminofluorene ring is stacked with the purine ring of the nonadjacent dA2 residue. By contrast, the dC and dA residues opposite the junctional [AF]dG4 adduct site adopt distinctly different alignments. The dC23 residue positioned opposite the adduct site is looped out into the minor groove by the aminofluorene ring. The syn displaced orientation of the modified dG with stacking of the aminofluorene and the looped out position of the partner dC could be envisioned to cause polymerase stalling associated with subsequent misalignment leading to frameshift mutations in appropriate sequences. The dA23 residue positioned opposite the adduct site is positioned in the major groove with its purine ring aligned face down over the van der Waals surface of the major groove and its amino group directed toward the T6.A21 base pair. The Hoogsteen edge of the modified guanine of [AF]dG4 and the Watson-Crick edge of dA23 positioned opposite it are approximately coplanar and directed toward each other but are separated by twice the hydrogen-bonding distance required for pairing. This structure of [AF]dG opposite dA at a model template-primer junctional site can be compared with a previous structure of [AF]dG opposite dA within a fully paired duplex [Norman, D., Abuaf, P., Hingerty, B. E., Live, D. , Grunberger, D., Broyde, S., and Patel, D. J. (1989) Biochemistry 28, 7462-7476]. The alignment of the Hoogsteen edge of [AF]dG (syn) positioned opposite the Watson-Crick edge of dA (anti) has been observed for both systems with the separation greater in the case of the junctional alignment in the model template-primer system. However, the aminofluorene ring is positioned in the minor groove in the fully paired duplex while it stacks over the junctional base pair in the template-primer system. This suggests that the syn [AF]dG opposite dA junctional alignment can be readily incorporated within a duplex by a translation of this entity toward the minor groove.     

Solution structure of an O6-[4-oxo-4-(3-pyridyl)butyl]guanine adduct in an 11 mer DNA duplex: evidence for formation of a base triplex

The pyridyloxobutylating agents derived from metabolically activated tobacco-specific nitrosamines can covalently modify guanine bases in DNA at the O(6) position. The adduct formed, O(6)-[4-oxo-4-(3-pyridyl)butyl]guanine ([POB]dG), results in mutations that can lead to tumor formation, posing a significant cancer risk to humans exposed to tobacco smoke. A combined NMR-molecular mechanics computational approach was used to determine the solution structure of the [POB]dG adduct within an 11mer duplex sequence d(CCATAT-[POB]G-GCCC).d(GGGCCATATGG). In agreement with the NMR results, the POB ligand is located in the major groove, centered between the flanking 5'-side dT.dA and the 3'-side dG.dC base pairs and thus in the plane of the modified [POB]dG.dC base pair, which is displaced slightly into the minor groove. The modified base pair in the structure adopts wobble base pairing (hydrogen bonds between [POB]dG(N1) and dC(NH4) amino proton and between [POB]dG(NH2) amino proton and dC(N3)). A hydrogen bond appears to occur between the POB carbonyl oxygen and the partner dC's second amino proton. The modified guanine purine base, partner cytosine pyrimidine base, and POB pyridyl ring form a triplex via this unusual hydrogen-bonding pattern. The phosphodiester backbone twists at the lesion site, accounting for the unusual phosphorus chemical shift differences relative to those for the control DNA duplex. The helical distortions and wobble base pairing induced by the covalent binding of POB to the O(6)-position of dG help explain the significant decrease of 17.6 degrees C in melting temperature of the modified duplex relative to the unmodified control.     

Minor groove binding of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin to various duplex and triplex polynucleotides

The binding site and the geometry of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (CoTMPyP) complexed with double helical poly(dA).poly(dT) and poly(dG).poly(dC), and with triple helical poly(dA).[poly(dT)](2) and poly(dC).poly(dG).poly(dC)(+) were investigated by circular and linear dichroism (CD and LD). The appearance of monomeric positive CD at a low [porphyrin]/[DNA] ratio and bisignate CD at a high ratio of the CoTMPyP-poly(dA).poly(dT) complex is almost identical with its triplex counterpart. Similarity in the CD spectra was also observed for the CoTMPyP-poly(dG).poly(dC) and -poly(dC).poly(dG).poly(dC)(+) complex. This observation indicates that both monomeric binding and stacking of CoTMPyP to these polynucleotides occur at the minor groove. However, different binding geometry of CoTMPyP, when bind to AT- and GC-rich polynucleotide, was observed by LD spectrum. The difference in the binding geometry may be attributed to the difference in the interaction between polynucleotides and CoTMPyP: in the GC polynucleotide case, amine group protrude into the minor groove while it is not present in the AT polynucleotide.     

Molecular structure of an A-DNA decamer d(ACCGGCCGGT)

The molecular structure of the DNA decamer d(ACCGGCCGGT) has been solved and refined by single-crystal X-ray-diffraction analysis at 0.20 nm to a final R-factor of 18.0%. The decamer crystallizes as an A-DNA double helical fragment with unit-cell dimensions of a = b = 3.923 nm and c = 7.80 nm in the space group P6(1)22. The overall conformation of this A-DNA decamer is very similar to that of the fiber model for A-DNA which has a large average base-pair tilt and hence a wide and shallow minor groove. This structure is in contrast to that of several A-DNA octamers in which the molecules all have low base-pair-tilt angles (8-12 degrees) resulting in an appearance intermediate between B-DNA and A-DNA. The average helical parameters of this decamer are typical of A-DNA with 10.9 base pairs/turn of helix, an average helical twist angle of 33.1 degrees, and a base-pair-tilt angle of 18.2 degrees. However, the CpG step in this molecule has a low local-twist angle of 24.5 degrees, similar to that seen in other A-DNA oligomers, and therefore appears to be an intrinsic stacking pattern for this step. The molecules pack in the crystal using a recurring binding motif, namely, the terminal base pair of one helix abuts the surface of the shallow minor groove of another helix. In addition, the GC base pairs have large propeller-twist angles, unlike those found most other A-DNA structures.     

NMR studies of the exocyclic 1,N6-ethenodeoxyadenosine adduct (epsilon dA) opposite thymidine in a DNA duplex. Nonplanar alignment of epsilon dA(anti) and dT(anti) at the lesion site

Two-dimensional proton NMR studies are reported on the complementary d(C-A-T-G-T-G-T-A-C).d(G-T-A-C-epsilon A-C-A-T-G) nonanucleotide duplex (designated epsilon dA.dT 9-mer duplex) containing 1,N6-ethenodeoxyadenosine (epsilon dA), a carcinogen-DNA adduct, positioned opposite thymidine in the center of the helix. Our NMR studies have focused on the conformation of the epsilon dA.dT 9-mer duplex at neutral pH with emphasis on defining the alignment at the dT5.epsilon dA14 lesion site. The through-space NOE distance connectivities establish that both dT5 and epsilon dA14 adopt anti glycosidic torsion angles, are directed into the interior of the helix, and stack with flanking Watson-Crick dG4.dC15 and dG6.dC13 pairs. Furthermore, the d(G4-T5-G6).d(C13-epsilon A14-C15) trinucleotide segment centered about the dT5.epsilon dA14 lesion site adopts a right-handed helical conformation in solution. Energy minimization computations were undertaken starting from six different alignments of dT5(anti) and epsilon dA14(anti) at the lesion site and were guided by distance constraints defined by lower and upper bounds estimated from NOESY data sets on the epsilon dA.dT 9-mer duplex. Two families of energy-minimized structures were identified with the dT5 displaced toward either the flanking dG4.dC15 or the dG6.dC13 base pair. These structures can be differentiated on the basis of the observed NOEs from the imino proton of dT5 to the imino proton of dG4 but not dG6 and to the amino protons of dC15 but not dC13 that were not included in the constraints data set used in energy minimization. Our NMR data are consistent with a nonplanar alignment of epsilon dA14(anti) and dT5(anti) with dT5 displaced toward the flanking dG4.dC15 base pair within the d(G4-T5-G6).d(C13-epsilon A14-C15) segment of the epsilon dA.dT 9-mer duplex.     

High-resolution A-DNA crystal structures of d(AGGGGCCCCT). An A-DNA model of poly(dG) x poly(dC).

A-DNA conformation is favored by guanine-rich sequences, such as (dG)n x (dC)n, or under low-humidity conditions. Earlier A-DNA crystal structures revealed some conformational variations which may be the result of sequence-dependent effects and/or crystal packing forces. Here we report the high-resolution crystal structure of d(AGGGGCCCCT) in two crystal forms (either in the P212121 or the P6122 space group) to gain insights into the conformation and dynamics of the (dG)n x (dC)n sequence. The P212121 form has been analyzed using data to 1.1 A resolution by the anisotropic temperature factor refinement procedure of the SHELX97 program. Such analysis affords us with the detailed geometric, conformational and motional property of an A-DNA structure. The backbone torsional angles fall in a narrow range, except for the alpha/gamma angles which have two distinct combinations (gauche-/gauche+ or trans/trans). An A-DNA model of poly(dG) x poly(dC) has been constructed using the conformational parameters derived from the crystal structure of the P212121 form. In the crystal structure of the P6122 space group, the central eight base pairs of the decamer adopt A-DNA conformation with the two terminal nucleotides flipped out to form base pairs with the neighboring nucleotides. Comparison of the A-DNA structure of the same sequence from two different crystal forms, reinforced the conclusion that molecules crystallized in the same space group have a more similar conformation, whereas the same molecule crystallized in different space groups has different (local) conformations.     

Conformational sub-states in B-DNA.

Theoretical studies of the sequence-dependent conformation of B-DNA have been carried out using Jumna, a helicoidal co-ordinate minimization algorithm. The results obtained for a series of six oligomers with repetitive sequences show that, with the exception of the homopolymers (dA)n.(dT)n and (dG)n.(dC)n, all sequences can adopt a variety of conformations characterized by considerable changes in helicoidal parameters and also in sugar puckers which adopt C(2')-endo (falling into 2 classes) or, in the case of pyrimidine nucleotides, O(1')-endo forms. These studies lead to an improved understanding of the role of base sequence on DNA conformation and point to a number of interesting correlations between the various structural parameters describing the double helix.     

High propeller twist and unusual hydrogen bonding patterns from the MD simulation of (dG)6.(dC)6

A molecular dynamics (MD) study of (dG)6.(dC)6 including counter ions and 292 water molecules was made. The hydrogen bonding pattern and propeller twist angles for the mini-helix are reported as averages for times spanning 21-30, 31-40, 41-50, and 51-60 ps. The propeller twist angles range from 18 degrees to 38 degrees. Bifurcated and interstrand neighboring base (twisted) hydrogen bonding patterns were found.     

A demonstration of the intrinsic importance of stabilizing hydrophobic binding and non-covalent van der Waals contacts dominant in the non-covalent CC-1065/B-DNA binding

The comparative DNA binding properties and cytotoxic activity of CDPIn methyl esters (n = 1-5) vs. PDE-In methyl esters (n = 1-3) are detailed in studies which provide experimental evidence for the intrinsic importance of stabilizing hydrophobic binding and non-covalent van der Waals contacts dominant in the CC-1065/B-DNA minor groove binding. High affinity minor groove binding to DNA was established through: (1) the observation of CDPI3 binding (UV) but not unwinding of supercoiled DNA (phi 174 RFI DNA) thus excluding intercalative binding; (2) the observation of CDPI3 binding to T4 phage DNA (UV, delta Tm) in which the major groove is occluded by glycosylation thus excluding major groove binding; (3) the observation of salt (Na+) concentration independent high affinity CDPI3 binding to poly(dA . poly(dT) thus excluding simple electrostatic binding to the DNA phosphate backbone; and further inferred through (4) the observation of an intense induced dichroism (ICD, poly(dA) . poly(dT) and poly(dG) . poly(dC) [phi]23(358) = 24,000 and 23,500). This high affinity minor groove binding is sufficient to produce a potent cytotoxic effect.(ABSTRACT TRUNCATED AT 400 WORDS)     

NMR studies of the exocyclic 1,N6-ethenodeoxyadenosine adduct (epsilon dA) opposite deoxyguanosine in a DNA duplex. Epsilon dA(syn).dG(anti) pairing at the lesion site

Proton NMR studies are reported on the complementary d(C-A-T-G-G-G-T-A-C).d(G-T-A-C-epsilon A-C-A-T-G) nonanucleotide duplex (designated epsilon dA.dG 9-mer duplex), which contains exocyclic adduct 1,N6-ethenodeoxyadenosine positioned opposite deoxyguanosine in the center of the helix. The present study focuses on the alignment of dG5 and epsilon dA14 at the lesion site in the epsilon dA.dG 9-mer duplex at neutral pH. This alignment has been characterized by monitoring the NOEs originating from the NH1 proton of dG5 and the H2, H5, and H7/H8 protons of epsilon dA14 in the central d(G4-G5-G6).d(C13-epsilon A14-C15) trinucleotide segment of the epsilon dA.dG 9-mer duplex. These NOE patterns establish that epsilon dA14 adopts a syn glycosidic torsion angle that positions the exocyclic ring toward the major groove edge while all the other bases including dG5 adopt anti glycosidic torsion angles. We detect a set of intra- and interstrand NOEs between protons (exchangeable and nonexchangeable) on adjacent residues in the d(G4-G5-G6).d(C13-epsilon A14-C15) trinucleotide segment which establish formation of right-handed helical conformations on both strands and stacking of the dG5(anti).epsilon dA14(syn) pair between stable dG4.dC15 and dG6.dC13 pairs. The energy-minimized conformation of the central d(G4-G5-G6).d(C13-epsilon A14-C15) segment establishes that the dG5(anti).epsilon dA14(syn) alignment is stabilized by two hydrogen bonds from the NH1 and NH2-2 of dG5(anti) to N9 and N1 of epsilon dA14(syn), respectively.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Minor groove binding of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin to various duplex and triplex polynucleotides

The binding site and the geometry of Co(III)meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (CoTMPyP) complexed with double helical poly(dA)·poly(dT) and poly(dG)·poly(dC), and with triple helical poly(dA)·[poly(dT)]₂ and poly(dC)·poly(dG)·poly(dC)⁺ were investigated by circular and linear dichroism (CD and LD). The appearance of monomeric positive CD at a low [porphyrin]/[DNA] ratio and bisignate CD at a high ratio of the CoTMPyP-poly(dA)·poly(dT) complex is almost identical with its triplex counterpart. Similarity in the CD spectra was also observed for the CoTMPyP-poly(dG)·poly(dC) and -poly(dC)·poly(dG)·poly(dC)⁺ complex. This observation indicates that both monomeric binding and stacking of CoTMPyP to these polynucleotides occur at the minor groove. However, different binding geometry of CoTMPyP, when bind to AT- and GC-rich polynucleotide, was observed by LD spectrum. The difference in the binding geometry may be attributed to the difference in the interaction between polynucleotides and CoTMPyP: in the GC polynucleotide case, amine group protrude into the minor groove while it is not present in the AT polynucleotide.     

Solution structure of the N-(deoxyguanosin-8-yl)-1-aminopyrene ([AP]dG) adduct opposite dA in a DNA duplex.

Solution structural studies have been undertaken on the aminopyrene-C(8)-dG ([AP]dG) adduct in the d(C5-[AP]G6-C7). d(G16-A17-G18) sequence context in an 11-mer duplex with dA opposite [AP]dG, using proton-proton distance and intensity restraints derived from NMR data in combination with distance-restrained molecular mechanics and intensity-restrained relaxation matrix refinement calculations. The exchangeable and nonexchangeable protons of the aminopyrene and the nucleic acid were assigned following analysis of two-dimensional NMR data sets on the [AP]dG.dA 11-mer duplex in H2O and D2O solution. The broadening of several resonances within the d(G16-A17-G18) segment positioned opposite the [AP]dG6 lesion site resulted in weaker NOEs, involving these protons in the adduct duplex. Both proton and carbon NMR data are consistent with a syn glycosidic torsion angle for the [AP]dG6 residue in the adduct duplex. The aminopyrene ring of [AP]dG6 is intercalated into the DNA helix between intact Watson-Crick dC5.dG18 and dC7.dG16 base pairs and is in contact with dC5, dC7, dG16, dA17, and dG18 residues that form a hydrophobic pocket around it. The intercalated AP ring of [AP]dG6 stacks over the purine ring of dG16 and, to a lesser extent dG18, while the looped out deoxyguanosine ring of [AP]dG6 stacks over dC5 in the solution structure of the adduct duplex. The dA17 base opposite the adduct site is not looped out of the helix but rather participates in an in-plane platform with adjacent dG18 in some of the refined structures of the adduct duplex. The solution structures are quite different for the [AP]dG.dA 11-mer duplex containing the larger aminopyrene ring (reported in this study) relative to the previously published [AF]dG.dA 11-mer duplex containing the smaller aminofluorene ring (Norman et al., Biochemistry 28, 7462-7476, 1989) in the same sequence context. Both the modified syn guanine and the dA positioned opposite it are stacked into the helix with the aminofluorene chromophore displaced into the minor groove in the latter adduct duplex. By contrast, the aminopyrenyl ring participates in an intercalated base-displaced structure in the present study of the [AP]dG.dA 11-mer duplex and in a previously published study of the [AP]dG.dC 11-mer duplex (Mao et al., Biochemistry 35, 12659-12670, 1996). Such intercalated base-displaced structures without hydrogen bonding between the [AP]dG adduct and dC or mismatched dA residues positioned opposite it, if present at a replication fork, may cause polymerase stalling and formation of a slipped intermediate that could produce frameshift mutations, the most dominant mutagenic consequence of the [AP]dG lesion.     

Molecular structure of the netropsin-d(CGCGATATCGCG) complex: DNA conformation in an alternating AT segment

The molecular structure of the complex between a minor groove binding drug (netropsin) and the DNA dodecamer d(CGCGATATCGCG) has been solved and refined by single-crystal X-ray diffraction analysis to a final R factor of 20.0% to 2.4-A resolution. The crystal is similar to that of the other related dodecamers with unit cell dimensions of a = 25.48 A, b = 41.26 A, and c = 66.88 A in the space group P2(1)2(1)2(1). In the complex, netropsin binds to the central ATAT tetranucleotide segment in the narrow minor groove of the dodecamer B-DNA double helix as expected. However, in the structural refinement the drug is found to fit the electron density in two orientations equally well, suggesting the disordered model. This agrees with the results from solution studies (chemical footprinting and NMR) of the interactions between minor groove binding drugs (e.g., netropsin and distamycin A) and DNA. The stabilizing forces between drug and DNA are provided by a combination of ionic, van der Waals, and hydrogen-bonding interactions. No bifurcated hydrogen bond is found between netropsin and DNA in this complex due to the unique dispositions of the hydrogen-bond acceptors (N3 of adenine and O2 of thymine) on the floor of the DNA minor groove. Two of the four AT base pairs in the ATAT stretch have low propeller twist angles, even though the DNA has a narrow minor groove. Alternating helical twist angles are observed in the ATAT stretch with lower twist in the ApT steps than in the TpA step.     

The crystal structure of d(G-G-G-G-C-C-C-C). A model for poly(dG).poly(dC)

The structure of the DNA oligomer d(G-G-G-G-C-C-C-C) has been determined at a resolution of 2.5 A by single-crystal X-ray methods. There are two strands in the asymmetric unit, and these coil about each other to form a right-handed double-helix of the A-type with Watson-Crick hydrogen bonds between base-pairs. The helix has a shallow minor groove and a deep, water-filled major groove; almost all exposed functional groups on the DNA are hydrated, and 106 ordered solvent molecules have been found. The two d(G-G-G-G).d(C-C-C-C) segments in the octamer exhibit similar and uniform structures, but there is a slight discontinuity at the GpC step between them. A recurring feature of the structure is the overlap of adjacent guanine bases in each GpG step, with the five-membered ring of one guanine stacking on the six-membered ring of its neighbour. There is little or no overlap between adjacent cytosine rings. Conformational parameters for these GpG steps are compared with those from other single-crystal X-ray analyses. In general, GpG steps exhibit high slide, low roll and variable twist. Models for poly(dG).poly(dC) were generated by applying a simple rotation and translation to each of the unmodified d(G-G-G-G).d(C-C-C-C) units. Detailed features of these models are shown to be compatible with various assays of poly(dG).poly(dC) in solution, and are useful in understanding the polymorphic behaviour of this sequence under a variety of experimental conditions.     

Parallel double helices of DNA. Conformational analysis of regular helices with the second order symmetry axis

We have performed a conformational analysis of DNA double helices with parallel directed backbone strands connected with the second order symmetry axis being at the same time the helix axis. The calculations were made for homopolymers poly(dA).poly(dA), poly(dC).poly(dC), poly(dG) poly(dG), and poly(dT).poly(dT). All possible variants of hydrogen bonding of base pairs of the same name were studied for each polymer. The maps of backbone chain geometrical existence were constructed. Conformational and helical parameters corresponding to local minima of conformational energy of "parallel" DNA helices, calculated at atom-atom approximation, were determined. The dependence of conformational energy on the base pair and on the hydrogen bond type was analysed. Two major conformational advantageous for "parallel" DNA's do not depend much on the hydrogen-bonded base pair type were indicated. One of them coincided with the conformational region typical for "antiparallel" DNA, in particular for the B-form DNA. Conformational energy of "parallel" DNA depends on the base pair type and for the most part is similar to the conformational energy of "antiparallel" B-DNA.     

Conformational and model-building studies of the hairpin form of the mismatched DNA octamer d(m5C-G-m5C-G-T-G-m5C-G)

The hairpin form of the mismatched octamer d(m5C-G-m5C-G-T-G-m5C-G) was studied by means of NMR spectroscopy. In a companion study it is shown that the hairpin form of this DNA fragment consists of a structure with a stem of three Watson-Crick-type base pairs and a loop consisting of only two nucleotides. The non-exchangeable proton resonances were assigned by means of two-dimensional correlation spectroscopy and two-dimensional nuclear Overhauser effect spectroscopy. Proton-proton coupling constants were used for the conformational analysis of the deoxyribose ring and for some of the backbone torsion angles. From the two-dimensional NMR spectra and the coupling-constant analysis it is concluded that: (i) the stem of the hairpin exhibits B-DNA characteristics; (ii) the sugar rings are not conformationally pure, but display a certain amount of conformational flexibility; (iii) the stacking interaction in the stem of the hairpin is elongated from the 3'-side in a more or less regular fashion with the two loop nucleotides; (iv) at the 5'-side of the stem a stacking discontinuity occurs between the stem and the loop; (v) at the 5'-side of the stem the loop is closed by means of a sharp backbone turn which involves unusual gamma' and beta+ torsion angles in residue dG(6). The NMR results led to the construction of a hairpin-loop model which was energy-minimized by means of a molecular-mechanics program. The results clearly show that a DNA hairpin-loop structure in which the loop consists of only two nucleotides bridging the minor groove in a straightforward fashion, (i) causes no undue steric strain, and (ii) involves well-known conformational principles throughout the course of the backbone. The hairpin form of the title compound is compared with the hairpin form of d(A-T-C-C-T-A-T4-T-A-G-G-A-T), in which the central -T4- part forms a loop of four nucleotides. Both models display similarities as far as stacking interactions are concerned.