Importance of minor groove functional groups for the stability of DNA duplexes

Eight oligonucleotide duplexes have been prepared with four pairs of selected complementary pairs of native/analogue heterocyclic bases incorporated at a selected test site. The base pairs vary in the nature of their functionality in the minor groove. Each pair has a minor groove purine amino group present or absent, and correspondingly has a minor grove pyrimidine carbonyl present or absent. Loss of duplex stability is most notable when the minor groove pyrimidine carbonyl is absent although in other respects normal Watson-Crick hydrogen bonding is maintained in these sequences. These differences in stability are discussed in terms of possible variations in minor groove hydration.     

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.     

C-C-A-G-G-C-m5C-T-G-G. Helical fine structure, hydration, and comparison with C-C-A-G-G-C-C-T-G-G.

The self-complementary DNA duplex C-C-A-G-G-C-m5C-T-G-G has been refined against 1.75-A x-ray diffraction data to an R value of 17.4%. In the crystal of space group P6, 10-base pair DNA fragments with characteristic sequence-related fine structure stack end to end to form long antiparallel B-type double helices. As shown by a structure analysis at lower resolution (Heinemann, U., and Alings, C. (1991) EMBO J. 10, 35-43), the overall geometry of C-C-A-G-G-C-m5C-T-G-G is similar to that of the unmethylated analog C-C-A-G-G-C-C-T-G-G despite a different crystal environment. The present high resolution structure analysis permits a detailed comparison of the two duplexes and their hydration spheres. Helical parameters are significantly correlated between both molecules, with the exception of the base pair propeller. Sugar pucker and backbone torsion angles alpha, gamma, delta, and chi show similar mean values, but their individual values deviate significantly between duplexes. In contrast, torsion angles beta, epsilon, and zeta change along the strands of both duplexes in much the same way. The effect of single-site methylation on DNA conformation appears to be small and limited to the base pairs directly involved. Methylation tends to push base pairs toward the minor groove of the helix. A regular minor groove hydration pattern involves dual hydrogen bonding of water molecules to O-4' and base atoms of C-C-A-G-G-C-m5C-T-G-G.     

Structural principles of B-DNA grooves hydration in fibers as revealed by Monte Carlo simulations and X-ray diffraction

Being interested in possible effects of sequence-dependent hydration of B-DNA with mixed sequence in fibers, we performed a series of Monte Carlo calculations of hydration of polydeoxyribonucleotides in B form, considering all sequences with dinucleotide repeat. The computational results allow the ten base-stacking types to be classified in accordance with their primary hydration in the minor groove. As a rule, the minor groove is occupied by two water molecules per base pair in the depth of the groove, which are located nearly midway between the planes of successive base pairs and symmetrically according to the dyad there. The primary hydration of the major groove depends on the type of the given base pair. The coordinates of 3 water molecules per base pair in the depth of the major groove are determined by the type of this pair together with its position and orientation in the helix, and are practically independent on the adjacent base pairs. A/T-homopolymer tracts do not fit into this hydration pattern; the base pair edges are hydrated autonomously in both grooves. Analysis of the Li-B-DNA x-ray diffraction intensities reveals those two water positions in the minor groove. In the major groove, no electronic density peaks in sufficient distance from the base edges were found, thus confirming the absence of any helical invariance of primary hydration in this region. With the help of the rules proposed in this paper it is possible to position the water molecules of the first hydration shell in the grooves of canonical B-DNA for any given sequence.     

Minor groove hydration of DNA in aqueous solution: sequence-dependent next neighbor effect of the hydration lifetimes in d(TTAA)2 segments measured by NMR spectroscopy.

The hydration in the minor groove of double stranded DNA fragments containing the sequences 5'-dTTAAT, 5'-dTTAAC, 5'-dTTAAA and 5'-dTTAAG was investigated by studying the decanucleotide duplex d(GCATTAATGC)2 and the singly cross-linked decameric duplexes 5'-d(GCATTAACGC)-3'-linker-5'-d(GCGTTAATGC)-3' and 5'-d(GCCTTAAAGC)-3'-linker-5'-d(GCTTTAAGGC)-3' by NMR spectroscopy. The linker employed consisted of six ethyleneglycol units. The hydration water was detected by NOEs between water and DNA protons in NOESY and ROESY spectra. NOE-NOESY and ROE-NOESY experiments were used to filter out intense exchange cross-peaks and to observe water-DNA NOEs with sugar 1' protons. Positive NOESY cross-peaks corresponding to residence times longer than approximately 0.5 ns were observed for 2H resonances of the central adenine residues in the duplex containing the sequences 5'-dTTAAT and 5'-dTTAAC, but not in the duplex containing the sequences 5'-dTTAAA and 5'-dTTAAG. In all nucleotide sequences studied here, the hydration water in the minor groove is significantly more mobile at both ends of the AT-rich inner segments, as indicated by very weak or negative water-A 2H NOESY cross-peaks. No positive NOESY cross-peaks were detected with the G 1'H and C 1'H resonances, indicating that the minor groove hydration water near GC base pairs is kinetically less restrained than for AT-rich DNA segments. Kinetically stabilized minor groove hydration water was manifested by positive NOESY cross-peaks with both A 2H and 1'H signals of the 5'-dTTAA segment in d(GCATTAATGC)2. More rigid hydration water was detected near T4 in d(GCATTAATGC)2 as compared with 5'-d(GCATTAACGC)-3'-linker-5'-d(GCGTTAATGC)-3', although the sequences differ only in a single base pair. This illustrates the high sensitivity of water-DNA NOEs towards small conformational differences.     

Structure of the hydration shells of oligo(dA-dT).oligo(dA-dT) and oligo(dA).oligo(dT) tracts in B-type conformation on the basis of Monte Carlo calculations

Monte Carlo simulations [(N, V, T)-ensemble] were performed for the hydration shell of poly(dA-dT).poly(dA-dT) in canonical B form and for the hydration shell of poly(dA).poly(dT) in canonical B conformation and in a conformation with narrow minor groove, highly inclined bases, but with a nearly zero-inclined base pair plane (B' conformation). We introduced helical periodic boundary conditions with a rather small unit cell and a limited number of water molecules to reduce the dimensionality of the configuration space. The coordinates of local maxima of water density and the properties of one- and two-membered water bridges between polar groups of the DNA were obtained. The AT-alternating duplex hydration mirrors the dyad symmetry of polar group distribution. At the dApdT step, a water bridge between the two carbonyl oxygens O2 of thymines is formed as in the central base-pair step of Dickerson's dodecamer. In the major groove, 5-membered water chains along the tetranucleotide pattern d(TATA).d(TATA) are observed. The hydration geometry of poly(dA).poly(dT) in canonical B conformation is distinguished by autonomous primary hydration of the base-pair edges in both grooves. When this polymer adopts a conformation with highly inclined bases and narrow minor groove, the water density distribution in the minor groove is in excellent agreement with Dickerson's spine model. One local maximum per base pair of the first layer is located near the dyad axis between adjacent base pairs, and one local maximum per base pair in the second shell lies near the dyad axis of the base pair itself. The water bridge between the two strands formed within the first layer was observed with high probability. But the water molecules of the second layer do not have a statistically favored orientation necessary for bridging first layer waters. In the major groove, the hydration geometry of the (A.T) base-pair edge resembles the main features of the AT-pair hydration derived from other sequences for the canonical B form. The preference of the B' conformation for oligo(dA).oligo(dT) tracts may express the tendency to common hydration of base-pair edges of successive base pairs in the grooves of B-type DNA. The mean potential energy of hydration of canonical B-DNA was estimated to be -60 to -80 kJ/mole nucleotides in dependence on the (G.C) contents. Because of the small system size, this estimation is preliminary.     

Comparison of the conformation of an oligonucleotide containing a central G-T base pair with the non-mismatch sequence by proton NMR.

We have recorded NOESY spectra of two non-selfcomplementary undecanucleotide duplexes. From the observed NOEs we do not detect any significant distortion of the helix when a G-C pair is replaced by a G-T pair and the normal interresidue connectivities can be followed through the mismatch site. We conclude that the 2D spectra of the non-exchangeable protons do not allow differentiation between a wobble or rare tautomer form for the mismatch. NOE measurements in H2O, however, clearly show that the mismatch adopts a wobble structure and give information on the hydration in the minor groove for the G-T base pair which is embedded between two A-T base pairs in the sequence.     

Molecular recognition in noncovalent antitumor agent-DNA complexes: NMR studies of the base and sequence dependent recognition of the DNA minor groove by netropsin

We have investigated intermolecular interactions and conformational features of the netropsin complexes with d(G1-G2-A3-A4-T5-T6-C7-C8) duplex (AATT 8-mer) and the d(G1-G2-T3-A4-T5-A6-C7-C8) duplex (TATA 8-mer) by one and two-dimensional NMR studies in solution. We have assigned the amide, pyrrole and methylene protons of netropsin and the base and sugar H1' protons of the nucleic acid from an analysis of the nuclear Overhauser effect (NOESY) and correlated (COSY) spectra of the complex at 25 degrees C. The directionality of the observed distance-dependent NOEs demonstrates that the 8-mer helices remain right-handed and that the arrangement of concave and convex face protons of netropsin are retained in the complexes. The observed changes in NOE patterns and chemical shift changes on complex formation suggest small conformational changes in the nucleic acid at the AATT and TATA antibiotic binding sites and possibly the flanking G.C base pairs. We observe intermolecular NOEs between all three amide and both pyrrole protons on the concave face of the antibiotic and the minor groove adenosine H2 proton of the two central A4.T5 base pairs of the AATT 8-mer and TATA 8-mer duplexes. The concave face pyrrole protons of the antibiotic also exhibit NOEs to the sugar H1' protons of residues 5 and 6 in the AATT and TATA 8-mer complexes. We also detect intermolecular NOEs between the guanidino and propioamidino methylene protons at either end of netropsin and the adenosine H2 proton of the two flanking A3.T6 base pairs in the AATT 8-mer and T3.A6 base pairs in the TATA 8-mer duplexes. These studies establish a set of nine contacts between the concave face of the antibiotic and the minor groove AATT segment and TATA segment of the 8-mer duplexes in solution. The observed magnitude of the NOEs require that there be no intervening water molecules sandwiched between the concave face of the antibiotic and the minor groove of the DNA so that release of the minor groove spine of hydration is a prerequisite for netropsin complex formation. The observed differences in the netropsin amide proton chemical shifts in the AATT 8-mer and TATA 8-mer complexes suggest differences in the strength and/or type of intermolecular hydrogen bonds at the AATT and TATA binding sites.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effects of the minor groove pyrimidine nucleobase functional groups on the stability of duplex DNA: the impact of uncompensated minor groove amino groups

DNA sequences containing four types of analog nucleosides are described. All four are pyridine derivatives constructed as C-nucleosides so that they mimic the pyrimidine derivatives 2'-deoxyuridine, thymidine or 2'-deoxycytidine, but in all cases the analogs lack the corresponding O2-carbonyls that in duplex DNA are located in the minor groove. In place of the O2-carbonyl is a hydrogen atom, a polar fluorine atom, or a nonpolar methyl group. The described C-nucleosides have native-like bidentate Watson-Crick hydrogen-bonding faces and can form essentially normal W-C base pairs of varying stability with A or G. In each modified base pair, two inter-residue hydrogen bonds should be present. In spite of a common number of interstrand hydrogen bonds, the thermodynamic stabilities of the prepared duplexes, each containing two analog base pairs, vary dramatically. Most notably, base pairs containing uncompensated purine amino groups (those lacking a hydrogen-bonding partner) in the minor groove exhibit the most dramatic reductions in thermodynamic stability. Removal of such uncompensated amino groups results in increased duplex stability. Base pairs containing fluorine in the minor groove positioned adjacent to an amino group seem to enhance duplex stability marginally (relative to --H or --CH(3)), but there is little evidence to suggest that fluorine is an effective hydrogen-bonding partner in these systems. The presence of minor groove methyl groups results in the least stable duplexes in each series of sequences.     

The role of a minor groove spine of hydration in stabilizing poly(dA).poly(dT) against fluctuational interbase H-bond disruption in the premelting temperature regime.

Experimental estimates of the premelting Adenine-Thymine base pair opening probability for some B-DNA sequences are two orders of magnitude smaller than those of other B-DNA sequences. The AT pairs in the sequence with smaller open probability seem to be those that have a well defined spine of hydration in the minor groove. We show that this spine of hydration can significantly enhance the thermal stability of the base pairs to which they are attached. The effect of this spine of hydration coupled with the possible stabilization effect contributed from neighboring GC pairs can explain the differences in the observed AT pair opening probability for different AT containing B-DNA sequences.     

Close packing of helices 3 and 12 of 16 S rRNA is required for the normal ribosome function

The along-groove packing motif is a quasi-reciprocal arrangement of two RNA double helices in which a backbone of each helix is closely packed within the minor groove of the other helix. At the center of the inter-helix contact, a GU base pair in one helix packs against a Watson-Crick base pair in the other helix. Here, based on in vivo selection from a combinatorial gene library of 16 S rRNA and on functional characterization of the selected clones, we demonstrate that the normal ribosome performance requires that helices 3 and 12 be closely packed. In some clones the Watson-Crick and GU base pairs exchange in their positions between the two helices, which affects neither the quality of the helix packing, nor the ribosome function. On the other hand, perturbations in the close packing usually lead to a substantial drop in the ribosome activity. The functionality of the clones containing such perturbations may depend on the presence of particular elements in the vicinity of the area of contact between helices 3 and 12. Such cases do not exist in natural 16 S rRNA, and their selection enriches our knowledge of the constraints imposed on the structure of ribosomal RNA in functional ribosomes.     

Base interaction and conformation manifestations of repetitive nucleotide sequences

To understand why different nucleotide sequences prefer different double helical conformations and to predict conformational behaviour of definite sequences the base-base interaction energy in regular helices consisting of A:U, A:T, G:C and I:C (hypoxanthine-cytosine) base pairs was calculated. Interaction energy was assumed to be a function of eight conformational parameters: H, the distance between adjacent pairs along helix axes; tau, turn angle of one pair relative to the neighbouring one; angles between base planes in a pair (TW, propeller twist and BL, buckle) and position of pairs with respect to helix axes (D and SL, displacements in the plane normal to helix axes, and TL and RL, inclinations to this plane, tilt and roll, respectively). For H and tau characteristic of A- and B-families of nucleic acid conformations (2.5 A less than H less than or equal to 3.5 A, 30 degrees less than or equal to tau less than or equal to 45 degrees) the ranges of conformational parameters corresponding to energy values close to minimal ones (valleys) and correlations between conformational parameters were revealed. Valleys for different sequences largely coincide but have distinctive characteristics for each sequence. Reasons for base pair planarity distortion in double-stranded helices were considered. The calculations permit to account for A-phility of G:C sequences and B-phility for A:T sequences. The valley for I:C sequence branches. This corresponds to A:T-like behaviour in some cases and G:C-like in the others.     

Hydration of B-DNA: comparison between the water network around poly(dG).poly(dC) and poly(dG-dC).poly(dG-dC) on the basis of Monte Carlo computations

A computational method is elaborated for studying the water environment around regular polynucleotide duplexes; it allows rigorous structural information on the hydration shell of DNA to be obtained. The crucial aspect of this Monte Carlo simulation is the use of periodical boundary conditions. The output data consists of local maxima of water density in the space near the DNA molecule and the properties of one- and two-membered water bridges as function of pairs of polar groups of DNA. In the present paper the results for poly(dG).poly(dC) and poly(dG-dC).poly(dG-dC) are presented. The differences in their hydration shells are of a purely structural nature and are caused by the symmetry of the polar groups of the polymers under study, the symmetry being reflected by the hydration shell. The homopolymer duplex hydration shell mirrors the mononucleotide repeat. The water molecules contacting the polynucleotide in the minor groove are located nearly in the plane midway between the planes of successive base pairs. One water molecule per base pair forms a water bridge facing two polar groups of bases from adjacent base pairs and on different strands making a "spine"-like structure. In contrast, the major groove hydration is stabilized exclusively by two-membered water bridges; the water molecules deepest in the groove are concentrated near the plane of the corresponding base pair. The alternating polymer is characterized by a marked dyad symmetry of the hydration shell corresponding to the axis between two successive base pairs. The minor groove hydration of the dCpdG step resembles the characteristic features of the homopolymer, but the bridge between the O2 oxygens of the other base-stacking type is formed by two water molecules. The major groove hydration is characterized by high probability of one-membered water bridges and by localization of a water molecule on the dyad axis of the dGpdC step. The found structural elements are discussed as reasonable invariants of a dynamic hydration shell.     

Kinetics for exchange of imino protons in the d(C-G-C-G-A-A-T-T-C-G-C-G) double helix and in two similar helices that contain a G . T base pair, d(C-G-T-G-A-A-T-T-C-G-C-G), and an extra adenine, d(C-G-C-A-G-A-A-T-T-C-G-C-G)

The relaxation lifetimes of imino protons from individual base pairs were measured in (I) a perfect helix, d(C-G-C-G-A-A-T-T-C-G-C-G), (II) this helix with a G . C base pair replaced with a G . T base pair, d(C-G-T-G-A-A-T-T-C-G-C-G), and (III) the perfect helix with an extra adenine base in a mismatch, d(C-G-C-A-G-A-A-T-T-C-G-C-G). The lifetimes were measured by saturation recovery proton nuclear magnetic resonance experiments performed on the imino protons of these duplexes. The measured lifetimes of the imino protons were shown to correspond to chemical exchange lifetimes at higher temperatures and spin-lattice relaxation times at lower temperatures. Comparison of the lifetimes in these duplexes showed that the destabilizing effect of the G . T base pair in II affected the opening rate of only the nearest-neighbor base pairs. For helix III, the extra adenine affected the opening rates of all the base pairs in the helix and thus was a larger perturbation for opening of the base pairs than the G . T base pair. The temperature dependence of the exchange rates of the imino proton in the perfect helix gives values of 14-15 kcal/mol for activation energies of A . T imino protons. These relaxation rates were shown to correspond to exchange involving individual base pair opening in this helix, which means that one base-paired imino proton can exchange independent of the others. For the other two helices that contain perturbations, much larger activation energies for exchange of the imino protons were found, indicating that a cooperative transition involving exchange of at least several base pairs was the exchange mechanism of the imino protons. The effects of a perturbation in a helix on the exchange rates and the mechanisms for exchange of imino protons from oligonucleotide helices are discussed.     

Differential hydration of homopurine sequences relative to alternating purine/pyrimidine sequences.

The minor groove ligand distamycin A has been used to probe the relative hydration of the minor groove of eight synthetic polynucleotides of known sequence and composition. A combination of densimetric, calorimetric, and temperature-dependent spectroscopic techniques have been used to obtain complete thermodynamic profiles (delta Gzero, delta Hzero, delta Szero, and delta Vzero) for the association of distamycin A to all polymer duplexes. In 10 mM phosphate buffer, pH 7, binding of the drug to each of the polymeric duplexes resulted in characteristic negative changes in both the volume and enthalpy. Although the binding constants were found to be identical for pairs of isomer polynucleotides having identical compositions but different sequences, the values of delta Hzero, delta Szero, and delta Vzero of each such pair were remarkably different. The entropy changes were found to roughly parallel the volume changes; no such trend was seen between delta Hzero and delta Vzero. The data support the hypothesis that the volume changes observed for these systems reflect the coulombic-hydration contribution to the entropy. The heteropolymer duplexes generated much larger exothermic contributions, less favorable entropies and larger volume contractions than did the corresponding homopolymer duplexes of identical composition, and strongly suggest that polynucleotides with homopurine sequences are more hydrated than polynucleotides with alternating purine/pyrimidine sequences. In addition, it was found that duplexes containing guanine sharply reduced the affinity for the drug, also lowering the exothermicity but raising the entropy. This may be explained by the presence of an amino group in the minor groove that prevents hydrogen bonding. Substitution of the guanine with inosine reversed this trend in the thermodynamic properties. Furthermore, substitution of poly(dA) for poly(rA) in a duplex produced a similar reduction in the affinity, while raising the exothermic contribution and greatly reducing the favorable entropy effect in agreement with an apparent increase in the hydration state.     

Poly(amino2dA-dT) isomerizes into the unusual X-DNA double helix at physiological conditions inducing Z-DNA in poly (dG-methyl5dC)

It is demonstrated that a two-state conformational isomerization is induced in the poly(amino2-dA-dT) duplex by submillimolar concentrations of divalent magnesium cations in low-salt aqueous solution. The isomerization is fast and has a low degree of cooperativity. The resulting conformer is the unusual X-DNA double helix originally observed with poly(dA-dT) at very high concentrations of CsF. Interestingly, the X form is induced in poly(amino2dA-dT) under the physiological conditions when poly(dG-methyl5dC) assumes Z-DNA. The same conditions of stabilization are presumably connected with the fact, observed in previous phosphorus NMR studies, that Z- and X-DNA have similar polydinucleotide backbone architectures. Results presented in this work permit to specify base pair exocyclic groups responsible for the radically different conformational variability of the synthetic DNA molecules containing alternating purine-pyrimidine sequences of GC or AT base pairs.     

Influence of a fluorobenzene nucleobase analogue on the conformational flexibility of RNA studied by molecular dynamics simulations

Chemically modified bases are frequently used to stabilize nucleic acids, to study the driving forces for nucleic acid structure formation and to tune DNA and RNA hybridization conditions. In particular, fluorobenzene and fluorobenzimidazole base analogues can act as universal bases able to pair with any natural base and to stabilize RNA duplex formation. Although these base analogues are compatible with an A-form RNA geometry, little is known about the influence on the fine structure and conformational dynamics of RNA. In the present study, nano-second molecular dynamics (MD) simulations have been performed to characterize the dynamics of RNA duplexes containing a central 1'-deoxy-1'-(2,4-difluorophenyl)-beta-D-ribofuranose base pair or opposite to an adenine base. For comparison, RNA with a central uridine:adenine pair and a 1'-deoxy-1'-(phenyl)-beta-D-ribofuranose opposite to an adenine was also investigated. The MD simulations indicate a stable overall A-form geometry for the RNAs with base analogues. However, the presence of the base analogues caused a locally enhanced mobility of the central bases inducing mainly base pair shear and opening motions. No stable 'base-paired' geometry was found for the base analogue pair or the base analogue:adenine pairs, which explains in part the universal base character of these analogues. Instead, the conformational fluctuations of the base analogues lead to an enhanced accessibility of the bases in the major and minor grooves of the helix compared with a regular base pair.     

The double helix is dehydrated: evidence from the hydrolysis of acridinium ester-labeled probes

A highly chemiluminescent reporter molecule, acridinium ester (AE), was tethered to single-stranded oligonucleotide probes and hybridized to complementary as well as mismatched target sequences. When tethered to single-stranded probes, AE was readily hydrolyzed by water or hydroxide ion. In contrast, when hybridized to a complementary target, hydrolysis of the AE probe was markedly inhibited. Mismatches near AE eliminated the ability of the double helix to strongly inhibit AE hydrolysis. To establish the molecular basis for these remarkable hydrolysis properties of AE-labeled probes, the binding and hydrolysis mechanisms of AE-labeled probes were examined. When tethered to single- or double-stranded nucleic acids, hydrolysis of AE was found to proceed by generalized base catalysis in which a base abstracts a proton from water and the resulting hydroxide ion then hydrolyzes AE. Analysis of the hydrolysis rates of AE bound to DNA revealed that AE binds the minor groove of DNA and that its hydrolysis is inhibited by low water activity within the minor groove of the helix. Depending upon the sequence of the DNA, the water activity of the minor groove was estimated to be at least 2-4-fold lower than bulk solution. Hydrolysis measurements of AE tethered to RNA as well as RNA/DNA hybrids argued that the grooves of these double helices are also dehydrated relative to bulk solution. Remarkably, mismatched bases, regardless of their structure or sequence context, enhanced hydrolysis of AE by inducing hydration of the double helix that spread approximately five base pairs on either side of the mismatch.     

Double helix conformation, groove dimensions and ligand binding potential of a G/C stretch in B-DNA.

The self-complementary DNA fragment CCGGCGCCGG crystallizes in the rhombohedral space group R3 with unit cell parameters a = 54.07 A and c = 44.59 A. The structure has been determined by X-ray diffraction methods at 2.2 A resolution and refined to an R value of 16.7%. In the crystal, the decamer forms B-DNA double helices with characteristic groove dimensions: compared with B-DNA of random sequence, the minor groove is wide and deep and the major groove is rather shallow. Local base pair geometries and stacking patterns are within the range commonly observed in B-DNA crystal structures. The duplex bears no resemblance to A-form DNA as might have been expected for a sequence with only GC base pairs. The shallow major groove permits an unusual crystal packing pattern with several direct intermolecular hydrogen bonds between phosphate oxygens and cytosine amino groups. In addition, decameric duplexes form quasi-infinite double helices in the crystal by end-to-end stacking. The groove geometries and accessibilities of this molecule as observed in the crystal may be important for the mode of binding of both proteins and drug molecules to G/C stretches in DNA.     

Mediation of the A/B-DNA helix transition by G-tracts in the crystal structure of duplex CATGGGCCCATG

The crystal structure of the DNA dodecamer duplex CATGGGCCCATG lies on a structural continuum along the transition between A- and B-DNA. The dodecamer possesses the normal vector plot and inclination values typical of B-DNA, but has the crystal packing, helical twist, groove width, sugar pucker, slide and x-displacement values typical of A-DNA. The structure shows highly ordered water structures, such as a double spine of water molecules against each side of the major groove, stabilizing the GC base pairs in an A-like conformation. The different hydration of GC and AT base pairs provides a physical basis for solvent-dependent facilitation of the A↔B helix transition by GC base pairs. Crystal structures of CATGGGCCCATG and other A/B-DNA intermediates support a ‘slide first, roll later’ mechanism for the B→A helix transition. In the distribution of helical parameters in protein–DNA crystal structures, GpG base steps show A-like properties, reflecting their innate predisposition for the A conformation.