The conformational variability of an adenosine.inosine base-pair in a synthetic DNA dodecamer.

A crystal structure analysis of the synthetic deoxydodecamer d(CGCAAATTIGCG) which contains two adenosine.inosine (A.I) mispairs has revealed that, in this sequence, the A.I base-pairs adopt a A(anti).I(syn) configuration. The refinement converged at R = 0.158 for 2004 reflections with F greater than or equal to 2 sigma(F) in the range 7.0-2.5A for a model consisting of the DNA duplex and 71 water molecules. A notable feature of the structure is the presence of an almost complete spine of hydration spanning the minor groove of the whole of the (AAATTI)2 core region of the duplex. pH-dependent ultraviolet melting studies have suggested that the base-pair observed in the crystal structure is, in fact, a protonated AH+ (anti).I(syn) species and that the A.I base-pairs in the sequence studied display the same conformational variability as A.G mispairs in the sequence d(CGCAAATTGGCG). The AH+(anti).I(syn) base-pair predominates below pH 6.5 and an A(anti).I(anti) mispair is the major species present between pH 6.5 and 8.0. The protonated base-pairs are held together by two hydrogen bonds one between N6(A) and O6(I) and the other between N1(A) and N7(I). This second hydrogen bond is a direct result of the protonation of the N1 of adenosine. The ultraviolet melting studies indicate that the A(anti).I(anti) base-pair is more stable than the A(anti).G(anti) base-pair but that the AH+(anti).I(syn) base pair is less stable than its AH+(anti).G(syn) analogue. Possible reasons for this observation are discussed.     

Crystal structure and stability of a DNA duplex containing A(anti).G(syn) base-pairs

The synthetic dodecanucleotide d(CGCAAATTGGCG) has been analysed by single-crystal X-ray diffraction techniques and the structure refined to R = 0.16 and 2.25 A resolution, with the location of 94 solvent molecules. The sequence crystallizes as a full turn of a B-DNA helix with ten Watson-Crick base-pairs and two adenine-guanine mispairs. The analysis clearly shows that the mismatches are of the form A(anti).G(syn). Thermal denaturation studies indicate that the stability of the duplex is strongly pH dependent, with a maximum at pH 5.0, suggesting that the base-pair is stabilized by protonation. Three different arrangements have been observed for base-pairs between guanine and adenine and it is likely that A.G mismatch conformation is strongly influenced by dipole-dipole interactions with adjacent base-pairs.     

Three-dimensional structures of bulge-containing DNA fragments.

The three-dimensional structure of a DNA tridecamer d(CGCAGAATTCGCG)2 containing bulged adenine bases was determined by single crystal X-ray diffraction methods, at 120 K, to 2.6 A resolution. The structure is a B-DNA type double helix with a single duplex in the asymmetric unit. One of the bulged adenine bases loops out from the double helix, while the other stacks in to it. This is in contrast to our preliminary finding, which indicated that both adenine bases were looped out. This revised model was confirmed by the use of a covalently bound heavy-atom derivative. The conformation of the looped-out bulge hardly disrupts base stacking interactions of the bases flanking it. This is achieved by the backbone making a "loop-the-loop" curve with the extra adenine flipping over with respect to the other nucleotides in the strand. The looped-out base intercalates into the stacked-in bulge site of a symmetrically related duplex. The looped-out and stacked-in bases form an A.A reversed Hoogsteen base-pair that stacks between the surrounding base-pairs, thus stabilizing both bulges. The double helix is frayed at one end with the two "melted" bases participating in intermolecular interactions. A related structure, of the same tridecamer, after soaking the crystals with proflavin, was determined to 3.2 A resolution. The main features of this B-DNA duplex are basically similar to the native tridecamer but differ in detail especially in the conformation of the bulged-out base. Accommodation of a large perturbation such as that described here with minimal disruption of the double helix shows both the flexibility and resiliency of the DNA molecule.     

Single base mismatches in DNA. Long- and short-range structure probed by analysis of axis trajectory and local chemical reactivity

We have devised a procedure to generate any single base mismatch in a constant sequence context, and have studied these from two points of view. (1) We have examined electrophoretic mobility of 458 base-pair fragments containing approximately centrally located single mismatches, in polyacrylamide gels, compared to fully matched DNA fragments. We found that no single mismatch caused a significant perturbation of gel mobility, and we conclude that all the mismatches may be accommodated within a helical geometry such that there is no alteration of the path of the helix axis in a straight DNA molecule. (2) We have studied all the single mismatches with respect to reactivity to a number of chemical probes. We found that: (a) No mispaired adenine bases are reactive to diethyl pyrocarbonate and are therefore not simply unpaired such that N-7 is exposed. (b) A number of mispaired thymine bases are reactive to osmium tetroxide, and cytosine bases to hydroxylamine. (c) Where crystal or nuclear magnetic resonance structures are available, the reactivity correlates with exposure of the pyrimidine 5,6 double bonds to attack in the major groove as a result of wobble base-pair formation. This is particularly clear for G.T and I.T base-pairs. (d) Reactivity of bases in mismatched pairs can be dependent on sequence context. (e) Reactivity of the C.C mismatch to hydroxylamine is suppressed at low pH, suggesting that a rearrangement of base-pairing occurs on protonation. The results overall are consistent with the formation of stacked intrahelical base-pairs wherever possible, resulting in no global distortion of the DNA structure, but specific enhancement of chemical reactivity in some cases.     

Sequence-dependent effects on DNA stability resulting from guanosine replacements by inosine.

The effect of replacing a G.C base-pair with an I.C base-pair on DNA stability was investigated for a related set of 14-mers. DNA melting analysis of the 14-mers was used to determine delta Hzero, delta Szero and delta G(zero)37 of the double to single stranded transition. All 14mers were shown to have B-DNA character by circular dichroism analysis. 14mers substituted with a single inosine in place of guanosine at different positions showed that consequences on DNA stability are sequence-dependent. Large changes in delta Hzero and delta Szero result when inosine is substituted within the trinucleotide sequence d(TCG).d(CGA) while substitution within d(TCC).d(GGA) causes minor changes in enthalpy and entropy. Moreover, some 14-mers with two inosine substitutions five base-pairs apart showed non-additive free energy changes for the double to single stranded transition. These results clearly indicate that the structural consequences of replacing a single guanosine with an inosine are transmitted over a significant distance.     

Structural features and hydration of d(C-G-C-G-A-A-T-T-A-G-C-G); a double helix containing two G.A mispairs

Single crystal X-ray diffraction techniques have been used to characterise the molecular structure of the title compound to 2.5A resolution. The structure consists of ten standard Watson-Crick base pairs and two G.A mismatched base pairs. The purine-purine mismatches have guanine in the usual anti orientation with respect to the sugar and adenine in syn orientation. There are two hydrogen bonds formed between the mismatch bases, N-1 and O-6 of guanine with N-7 and N-6 of adenine respectively. The bulky purine-purine mismatches are accommodated with minor perturbation of the sugar-phosphate backbone. There is a slight improvement in base pair overlap at the mismatch sites. Details of the backbone conformation, base stacking interactions and hydration are presented and compared with those of the parent compound d(C-G-C-G-A-A-T-T-C-G-C-G).     

Interaction between the replication origin and the initiator protein of the filamentous phage f1. Binding occurs in two steps

The replication initiator protein of bacteriophage f1 (gene II protein) binds to the phage origin and forms two complexes that are separable by polyacrylamide gel electrophoresis. Complex I is formed at low gene II protein concentrations, and shows protection from DNase I of about 25 base-pairs (from position +2 to +28 relative to the nicking site) at the center of the minimal origin sequence. Complex II is produced at higher concentrations of the protein, and has about 40 base-pairs (from -7 to +33) protected. On the basis of gel mobility, complex II appears to contain twice the amount of gene II protein as does complex I. The 40 base-pair sequence protected in complex II corresponds to the minimal origin sequence as determined by in-vivo analyses. The central 15 base-pair sequence (from +6 to +20) of the minimal origin consists of two repeats in inverted orientation. This sequence, when cloned into a plasmid, can form complex I, but not complex II. We call this 15 base-pair element the core binding sequence for gene II protein. Methylation interference with the formation of complex I by the wild-type origin indicates that gene II protein contacts six guanine residues located in a symmetric configuration within the core binding sequence. Formation of complex II requires, in addition to the core binding sequence, the adjacent ten base-pair sequence on the right containing a third homologous repeat. A methylation interference experiment performed on complex II indicates that gene II protein interacts homologously with the three repeats. In complex II, gene II protein protects from DNase I digestion not only ten base-pairs on the right but also ten base-pairs on the left of the sequence that is protected in complex I. Footprint analyses of various deletion mutants indicate that the left-most ten base-pairs are protected regardless of their sequence. The site of nicking by gene II protein is located within this region. A model is presented for the binding reaction involving both protein-DNA and protein-protein interactions.     

Stable sheared A.C pair in DNA hairpins

Single-residue d(Pu1NPu2) (Pu1.Pu2=G.A, G.G or A.A) hairpin loops can be stably closed by sheared purine.purine pairs. These special motifs have been found in several important biological systems. We now extend these loop-closing base-pairs to a sheared purine. pyrimidine (A.C) pair at a neutral pH condition. High-resolution NMR spectroscopy, distance geometry, and molecular dynamics methods were used to study d(GTACANCGTAC) oligomers. Numerous idiosyncratic nuclear Overhauser enhancements, especially those across the A.C base-pair between C4NH2left and right arrow AH1', C4NH2left and right arrow AH2, and CH5left and right arrow AH2 proton pairs, clearly define the novel sheared nature of the closing A.C base-pair. This novel base-pair is possibly present in several biological systems and in two single-stranded DNA aptamers selected from oligonucleotide libraries.     

Unique tertiary and neighbor interactions determine conservation patterns of Cis Watson-Crick A/G base-pairs

X-ray, phylogenetic and quantum chemical analysis of molecular interactions and conservation patterns of cis Watson-Crick (W.C.) A/G base-pairs in 16S rRNA, 23S rRNA and other molecules was carried out. In these base-pairs, the A and G nucleotides interact with their W.C. edges with glycosidic bonds oriented cis relative to each other. The base-pair is stabilised by two hydrogen bonds, the C1'-C1' distance is enlarged and the G(N2) amino group is left unpaired. Quantum chemical calculations show that, in the absence of other interactions, the unpaired amino group is substantially non-planar due to its partial sp(3) pyramidalization, while the whole base-pair is internally propeller twisted and very flexible. The unique molecular properties of the cis W.C. A/G base-pairs make them distinct from other base-pairs. They occur mostly at the ends of canonical helices, where they serve as interfaces between the helix and other motifs. The cis W.C. A/G base-pairs play crucial roles in natural RNA structures with salient sequence conservation patterns. The key contribution to conservation is provided by the unpaired G(N2) amino group that is involved in a wide range of tertiary and neighbor contacts in the crystal structures. Many of them are oriented out of the plane of the guanine base and utilize the partial sp(3) pyramidalization of the G(N2). There is a lack of A/G to G/A covariation, which, except for the G(N2) position, would be entirely isosteric. On the contrary, there is a rather frequent occurrence of G/A to G/U covariation, as the G/U wobble base-pair has an unpaired amino group in the same position as the cis W.C. G/A base-pair. The cis W.C. A/G base-pairs are not conserved when there is no tertiary or neighbor interaction. Obtaining the proper picture of the interactions and phylogenetic patterns of the cis W.C. A/G base-pairs requires a detailed analysis of the relation between the molecular structures and the energetics of interactions at a level of single H-bonds and contacts.     

N-6-(delta-2-isopentenyl) adenosine: hydrolysis by a mucleosidase isolated from Lactobacillus acidophilus cells.

A nucleosidase activity has been isolated from Lactobacillus acidophilus which rapidly hydrolyses N-6 (delta-2-isopentenyl) adenosine to its corresponding base, N-6(delta-2-isopentenyl) adenine. The activity can be distinguished from the spleen exzyme (EC. 2.4.2.1), a purine nucleoside transferase, on the basis of its substrate specificity, electrophoretic behavior, and nondependence on phosphate. The bacterial enzyme hydrolyzes both inosine and isopentenyl adenosine, giving Km values of 63.3muM and 177 muM respectively. The presence of this enzyme in bacteria counts for the rapid conversion of the parent nucleoside to isopentenyl adenine, which has been observed in these cells. The enzyme thus assumes importance as one of the catabolic activities available to the cell for metabolizing the cytokinin, N-6-(delta-2-isopentenyl) adenosine.     

Interaction of the antitumour antibiotic luzopeptin with the hexanucleotide duplex d(5''-GCATGC)2. One-dimensional and two-dimensional n.m.r. studies.

1H- and 31P-n.m.r. spectroscopy were used to characterize the solution structure of the 1:1 complex formed between the antitumour antibiotic luzopeptin and the self-complementary hexanucleotide d(5'-GCATGC)2. Eighteen nuclear Overhauser effects between antibiotic and nucleotide protons, together with ring-current-induced perturbations to base-pair and quinoline 1H resonances, define the position and orientation of the bound drug molecule. Luzopeptin binds in the minor groove of the DNA with full retention of dyad symmetry, its quinoline chromophores intercalating at the 5'-CpA and 5'-TpG steps and its depsipeptide ring spanning the central two A.T base-pairs. The chromophores stack principally on the adenine base with their carbocyclic rings pointing towards the deoxyribose of the cytosine. There is no evidence for Hoogsteen base-pairing in the complex, all glycosidic bond angles and sugar puckers being typical of B-DNA as found for the free hexanucleotide. The 'breathing' motions of the A.T and internal G.C base-pairs are substantially slowed in the complex compared with the free DNA, and the observation that two phosphate resonances are shifted downfield by at least 0.5 p.p.m. in the 31P-n.m.r. spectrum of the complex suggests pronounced local helix unwinding at the intercalation sites. The data are consistent with a model of the complex in which luzopeptin bisintercalates with its depsipeptide essentially in the conformation found in the crystal of the free antibiotic [Arnold & Clardy (1981) J. Am. Chem. Soc. 103, 1243-1244]. We postulate only one conformational change within the peptide ring, which involves rotation of the pyridazine-glycine amide group linkage by 90 degrees towards the DNA surface. This manoeuvre breaks the glycine-to-glycine transannular hydrogen bonds and enables the glycine NH groups to bond to the thymine O-2 atoms of the sandwiched A.T base-pairs. It also shortens the major axis of the depsipeptide so that the interchromophore distance is more suitable for spanning two base-pairs. The model further implies that the carboxy and hydroxy groups of the L-beta-hydroxyvaline residue are appropriately positioned for hydrogen-bonding to the 2-amino group of guanine and the O-2 atom of cytosine of the adjacent G.C base-pair.     

A self-consistent formulation for analysis and generation of non-uniform DNA structures

A fully self-consistent formulation is described here for the analysis and generation of base-pairs in non-uniform DNA structures, in terms of various local parameters. It is shown that the internal "wedge parameters" are mathematically related to the parameters describing the base-pair orientation with respect to an external helix axis. Hence any one set of three translation and three rotation parameters are necessary and sufficient to completely describe the relative orientation of the base-pairs comprising a step (or doublet). A general procedure is outlined for obtaining an average or global helix axis from the local helix axes for each step. A graphical representation of the local helix axes in the form of a polar plot is also shown and its application for estimating the curvature of oligonucleotide structures is illustrated, with examples of both A and B type structures.     

Analysis of local helix geometry in three B-DNA decamers and eight dodecamers

Local variations in B-DNA helix structure are compared among three decamers and eight dodecamers, which contain examples of all ten base-pair step types. All pairwise combinations of helix parameters are compared by linear regression analysis, in a search for internal relationships as well as correlations with base sequence. The primary conclusions are: (1) Three-center hydrogen bonds between base-pairs occur frequently in the major groove at C-C, C-A, A-A and A-C steps, but are less convincing at C-C and C-T steps in the minor groove. The requirements for large base-pair propeller are (1) that the base-pair should be A.T rather than G.C, and (2) that it be involved in a major groove three-center hydrogen bond with the following base-pair. Either condition alone is insufficient. Hence, a large propeller is expected at the leading base-pair of A-A and A-C steps, but not at A-T, T-A, C-A or C-C steps. (2) A systematic and quantitative linkage exists between helix variables twist, rise, cup and roll, of such strength that the rise between base-pairs can hardly be described as an independent variable at all. Two typical patterns of behavior are observed at steps from one base-pair to the next: high twist profile (HTP), characterized by high twist, low rise, positive cup and negative roll, and low twist profile (LTP), marked by low twist, high rise; negative cup and positive roll. Examples of HTP are steps G-C, G-A and Y-C-A-R, where Y is pyrimidine and R is purine. Examples of LTP steps are C-G, G-G, A-G and C-A steps other than Y-C-A-R. (3) The minor groove is especially narrow across the two base-pairs of the following steps: A-T, T-A, A-A and G-A. (4) In general, base step geometry cannot be correlated solely with the bases that define the step in question; the two flanking steps also must be taken into account. Hence, local helix structure must be studied in the context, not of two base-pairs: A-B, but of four: x-A-B-y. Calladine's rules, although too simple in detail, were correct in defining the length of sequence over which a given perturbation is expressed. Whereas ten different two-base steps are possible, allowing for the identity of complementary sequences, there are 136 different four-base steps. Only 33 of these 136 four-base steps are represented in the decamer and dodecamer structures solved to date, and hence it is premature to try to set up detailed structural algorithms. (5) The sugar-phosphate backbone chains of B-DNA place strong limits on sequence-induced structural variation, damping down most variables within four or five base-pairs, and preventing purine-purine anti-anti mismatches from causing bulges in the double helix. Hence, although short-range sequence-induced deformations (or deformability) are observed, long-range deformations propagated down the helix are not to be expected.     

A Self-Consistent Formulation for Analysis and Generation of Non-Uniform DNA Structures

Abstract

A fully self-consistent formulation is described here for the analysis and generation of base-pairs in non-uniform DNA structures, in terms of various local parameters. It is shown that the internal “wedge parameters” are mathematically related to the parameters describing the base-pair orientation with respect to an external helix axis. Hence any one set of three translation and three rotation parameters are necessary and sufficient to completely describe the relative orientation of the base-pairs comprising a step (or doublet). A general procedure is outlined for obtaining an average or global helix axis from the local helix axes for each step. A graphical representation of the local helix axes in the form of a polar plot is also shown and its application for estimating the curvature of oligonucleotide structures is illustrated, with examples of both A and B type structures.     

Structural Features and Hydration of d(C-G-C-G-A-A-T-T-A-G-C-G); a Double Helix Containing Two G.A Mispairs

Abstract

Single crystal X-ray diffraction techniques have been used to characterise the molecular structure of the title compound to 2.5Å resolution. The structure consists of ten standard Watson-Crick base pairs and two G.A mismatched base pairs. The purine-purine mismatches have guanine in the usual anti orientation with respect to the sugar and adenine in syn orientation. There are two hydrogen bonds formed between the mismatch bases, N-l and 0–6 of guanine with N-7 and N-6 of adenine respectively. The bulky purine-purine mismatches are accommodated with minor perturbation of the sugar-phosphate backbone. There is a slight improvement in base pair overlap at the mismatch sites. Details of the backbone conformation, base stacking interactions and hydration are presented and compared with those of the parent compound d(C-G-C-G-A-A-T-T-C-G-C-G).     

Orientation relaxation of DNA restriction fragments and the internal mobility of the double helix

The orientation relaxation of 15 DNA restriction fragments (43-4361 base-pairs) is characterized by measurements of linear dichroism using high electric field pulses. The off-field relaxation of fragments of 84 base-pairs or less can be described by single exponentials, which are related to the transverse rotational diffusion of the helix. Fragments of 95 base-pairs or greater exhibit an additional fast component with time constants around 100 ns for fragments of approx. 100 base-pairs, increasing with chain length to about 700 ns for a fragment with 258 base-pairs. The amplitude of this process increases from virtually zero at low fields (approximately equal to 10 kV) to a substantial limit contribution at high fields. According to these results, we suggest that electric fields induce stretching of the DNA fragments from a weakly bent to a more straight form and that the fast component reflects the internal mobility of the DNA chain. The slow off-field components of the orientation are discussed in terms of different models. The data up to helix lengths of about 400 base-pairs can be described by the 'weakly bending rod' model from Hearst using 3.4 A rise per base-pair and 13 A axial radius of the helix. Both the weakly bending rod according to Hearst and the 'wormlike chain' according to Hagerman and Zimm provide a persistence length of 500 A. The on-field relaxation is slower than the corresponding off-field process at low field strengths, but the on-field process is accelerated substantially at high electric fields. These observations are compared with model calculations of Schwarz.     

Production of Nucleic Acid-Related Substances by Fermentation Processes: XXXIII. Accumulation of Inosine by a Mutant of Brevibacterium ammoniagenes

Inosine-producing cultures were found among mutants resistant to 6-mercaptoguanine (6MG) derived from a 5'-inosinic acid (IMP)-producing strain, KY 13102, of Brevibacterium ammoniagenes. Inosine-producing ability was very frequent among the mutants resistant to a low concentration (10 to 50 mug/ml) of 6MG. The accumulation of inosine by strain KY 13714 was stimulated by a low concentration of adenine (25 mg/liter) but was depressed by high levels of adenine. The accumulation by strain KY 13714 was not inhibited by manganese ion but instead was stimulated by its excess, in contrast to IMP accumulation by KY 13102. Addition of hypoxanthine at an early stage of cultivation accelerated inosine accumulation. Furthermore, on addition of hypoxanthine and of a surface-activating agent after 48 hr of cultivation, the simultaneous accumulation of IMP and inosine was observed. A 9.3-mg amount of inosine per ml accumulated after 4 days of cultivation at 30 C. The inosine-producing mutant did not differ from the IMP-producing strain either in 5' purine nucleotide degradation or in IMP formation from hypoxanthine. However, it was found to be completely devoid of purine nucleoside-degrading activity. The conversion of IMP accumulation to inosine can be explained by the lack of nucleosidedegrading activity. The relationship between deficiency of nucleoside-degrading activity and resistance to low levels of 6MG is discussed, and a new mechanism for 6MG resistance is presented.     

Metabolism of Exogenous Purine Bases and Nucleosides by Salmonella typhimurium

Purine-requiring mutants of Salmonella typhimurium LT2 containing additional mutations in either adenosine deaminase or purine nucleoside phosphorylase have been constructed. From studies of the ability of these mutants to utilize different purine compounds as the sole source of purines, the following conclusions may be drawn. (i) S. typhimurium does not contain physiologically significant amounts of adenine deaminase and adenosine kinase activities. (ii) The presence of inosine and guanosine kinase activities in vivo was established, although the former activity appears to be of minor significance for inosine metabolism. (iii) The utilization of exogenous purine deoxyribonucleosides is entirely dependent on a functional purine nucleoside phosphorylase. (iv) The pathway by which exogenous adenine is converted to guanine nucleotides in the presence of histidine requires a functional purine nucleoside phosphorylase. Evidence is presented that this pathway involves the conversion of adenine to adenosine, followed by deamination to inosine and subsequent phosphorolysis to hypoxanthine. Hypoxanthine is then converted to inosine monophosphate by inosine monophosphate pyrophosphorylase. The rate-limiting step in this pathway is the synthesis of adenosine from adenine due to lack of endogenous ribose-l-phosphate.     

Base sequence and helix structure variation in B and A DNA

The observed propeller twist in base-pairs of crystalline double-helical DNA oligomers improves the stacking overlap along each individual helix strand. But, as proposed by Calladine, it also leads to clash or steric hindrance between purines at adjacent base-pairs on opposite strands of the helix. This clash can be relieved by: (1) decreasing the local helix twist angle between base-pairs; (2) opening up the roll angle between base-pairs on the side on which the clash occurs; (3) separating purines by sliding base-pairs along their long axes so that the purines are partially pulled out of the stack (leading to equal but opposite alterations in main-chain torsion angle delta at the two ends of the base-pair); and (4) flattening the propeller twist of the offending base-pairs. Simple sum functions, sigma 1 through sigma 4, are defined, by which the expected local variation in helix twist, base roll angle, torsion angle delta and propeller twist may be calculated from base sequence. All four functions are quite successful in predicting the behavior of B DNA. Only the helix twist and base roll functions are applicable to A DNA, and the helix twist function begins to fail for an A helical RNA/DNA hybrid. Within these limits, the sequence-derived sum functions match the observed helix parameter variation quite closely, with correlation coefficients greater than 0.900 in nearly all cases. Implications of this sequence-derived helix parameter variation for repressor-operator interactions are considered.     

Molecular mechanical studies of base-pair opening in d(CGCGC):d(GCGCG), dG5·dC5, d(TATAT):d(ATATA), and dA5·dT5 in the B and Z forms of DNA

Molecular mechanical energy refinement of double-helical pentanucleotide tetra-phosphates, d(CGCGC):d(GCGCG), dG₅·dC₅, d(TATAT):d(ATATA), and dA₅ ·dT₅ geometries, are presented in order to examine the energy required to open the Nl(purine) …? N3(pyrimidine) distance (base-pair opening) of a Watson-Crick base pair from its normal value of 3 Å to a value of 6 Å. The structural consequences of forcing base-pair opening is sequence dependent. For both dA₅ ·dT₅ and d(TATAT):d(ATATA), forcing the Nl (AdeKN3 (Thy) distance of the central base pair to a value of 6 Å slides the bases perpendicular to the helix axis forming a low-energy non-Watson-Crick base pair having an adenine amine hydrogen …? thymine carbonyl oxygen hydrogen bond. The two GC sequences behave differently from both AT sequences and differently from each other. Forcing the Nl(Gua) …? N3(Cyt) distance to 6 Å leads to unconventional structures in which hydrogen bonds are formed between the separated bases and the bases above or below them. These structures appear to be trapped in true local minima 6–10 kcal/mol higher in energy than the Watson-Crick structures. Preliminary simulations on d(CGCGC):d(GCGCG) in the Z geometry suggest the reason the Z form may be more refractory to proton exchange than the B form, consistent with experimental observations.