Structural insights into the effect of hydration and ions on A-tract DNA: a molecular dynamics study

DNA structure is known to be sensitive to hydration and ionic environment. To explore the dynamics, hydration, and ion binding features of A-tract sequences, a 7-ns Molecular dynamics (MD) study has been performed on the dodecamer d(CGCAAATTTGCG)(2). The results suggest that the intrusion of Na(+) ion into the minor groove is a rare event and the structure of this dodecamer is not very sensitive to the location of the sodium ions. The prolonged MD simulation successfully leads to the formation of sequence dependent hydration patterns in the minor groove, often called spine of hydration near the A-rich region and ribbon of hydration near the GC regions. Such sequence dependent differences in the hydration patterns have been seen earlier in the high resolution crystal structure of the Drew-Dickerson sequence, but not reported for the medium resolution structures (2.0 approximately 3.0 A). Several water molecules are also seen in the major groove of the MD simulated structure, though they are not highly ordered over the extended MD. The characteristic narrowing of the minor groove in the A-tract region is seen to precede the formation of the spine of hydration. Finally, the occurrence of cross-strand C2-H2.O2 hydrogen bonds in the minor groove of A-tract sequences is confirmed. These are found to occur even before the narrowing of the minor groove, indicating that such interactions are an intrinsic feature of A-tract sequences.     

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.     

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

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

An NMR study of d(CTACTGCTTTAG).d(CTAAAGCAGTAG) showing hydration water molecules in the minor groove of a TpA step

The hydration properties of the non-palindromic duplex d(CTACTGCTTTAG). d(CTAAAGCAGTAG) were investigated by NMR spectroscopy. The oligonucleotide possesses a heterogeneous B-DNA structure. The H2(n)-H1'(m+1) distances reflect a minor groove narrowing within the TTT/AAA segment (approximately 3.9A) and a sudden widening at the T10:A15 base-pair (approximately 5.3A), the standard B-DNA distance being approximately 5A. The facing T10pA11 and T14pA15 steps at the end of the TTTA/AAAT segment have completely different behaviors. Only A15 ending the AAA run displays NMR features comparable to those shown by adenines of TpA steps occupying the central position of TnAn (n> or =2) segments. These involve particular chemical shifts and line broadening of the H2 and H8 protons. Positive NOESY cross-peaks were measured between the water protons and the H2 protons of A15, A16 and A17 reflecting the occurrence of hydration water molecules with residence times longer than 500 picoseconds along the minor groove of the TTT/AAA segment. In contrast no water molecules with long residence times were observed neither for A3, A20 and A23 nor for A11 ending the 5'TTTA run. We confirm thus that the binding of water molecules with long residence time to adenine residues correlates with the minor groove narrowing. In contrast, the widening of the minor groove at the A11:T14 base-pair ending the TTTA/TAAA segment, likely associated to a high negative propeller twist value at this base-pair, prevents the binding of a water molecule with long residence time to A11 but not to A15 of the preceding T10:A15 base-pair. Thus, in our non-palindromic oligonucleotide the water molecules bind differently to A11 and A15 although both adenines are part of a TpA step. The slower motions occurring at A15 compared to A11 are also well explained by the present results.     

Structural comparison of the B-DNA dodecamers d(CGCGTTAACGCG) and d(CGCGAATTCGCG) with T2A2 and A2T2 tracts.

The x-ray structure of the deoxy oligonucleotide dodecamer d(CGCGTTAACGCG) recently determined in our laboratory shows that the helical parameters of the central TTAA segment are significantly different compared to the central AATT in d(CGCGAATTCGCG). The roll in the central TA step of the T2A2 dodecamer opens towards the minor groove while the AT step of the A2T2 dodecamer opens towards the major groove. Also, the roll angles at the steps 4 and 8 (GT and AC in T2A2) and (GA and TC in A2T2) are in opposite directions. The high cup and helical twist angles at the central base-pair of T2A2 decreases the base stacking interactions compared to A2T2. Tilt angles within the tetranucleotide segments TTAA and AATT have opposite signs. In spite of the local differences caused by the sequence inversion (TTAA----AATT), the two dodecamers exhibit similar overall bending. The top third is more bent than the bottom third relative to the central segment. This asymmetric bending in the two dodecamers is mainly due to crystal packing interactions.     

Sequence structure of human nucleosome DNA

Positional distributions of various dinucleotides in experimentally derived human nucleosome DNA sequences are analyzed. Nucleosome positioning in this species is found to depend largely on GG and CC dinucleotides periodically distributed along the nucleosome DNA sequence, with the period of 10.4 bases. The GG and CC dinucleotides oscillate counterphase, i.e., their respective preferred positions are shifted about a half-period from one another, as it was observed earlier for AA and TT dinucleotides. Other purine-purine and pyrimidine-pyrimidine dinucleotides (RR and YY) display the same periodical and counterphase pattern. The dominance of oscillating GG and CC dinucleotides in human nucleosomes and the contribution of AG(CT), GA(TC), and AA(TT) suggest a general nucleosome DNA sequence pattern - counterphase oscillation of RR and YY dinucleotides. AA and TT dinucleotides, commonly accepted as major players, are only weak contributors in the case of human nucleosomes.     

Quantitative structure of a complex between a minor-groove-specific drug and a bent DNA decamer duplex: use of 2D NMR data and NOESY constrained energy minimization

Two-dimensional nuclear magnetic resonance (2D NMR) studies on d(GA4T4C)2 and d(GT4A4C)2 [Sarma, M.H., et al. (1988) Biochemistry 27, 3423-3432; Gupta G., et al. (1988) Biochemistry 27, 7909-7919] showed that A.T pairs are propeller twisted. As a result, A/T tracts form a straight rigid structural block with an array of bifurcated inter base pair H bonds in the major groove. It was demonstrated (previous paper) that replacement of methyl group by hydrogen (changing from T to U) in the major groove does not disrupt the array of bifurcated H bonds in the major groove. In this article, we summarize results of 2D NMR and molecular mechanic studies on the effect of a minor-groove-binding A.T-specific drug on the structure d(GA4T4C)2. A distamycin analogue (Dst2) was used for this study. It is shown that Dst2 binds to the minor groove of d(GA4T4C)2 mainly driven by van der Waals interaction between A.T pairs and the drug; as a consequence, an array of bifurcated H bonds can be formed in the minor groove between amide/amino protons of Dst2 and A.T pairs of DNA. NOESY data suggest that Dst2 predominantly binds at the central 5 A.T pairs. NOESY data also reveal that, upon drug binding, d(GA4T4C)2 does not undergo any significant change in conformation from the free state; i.e., propeller-twisted A.T pairs are still present in DNA and hence the array of bifurcated H bonds must be preserved in the major groove. NOESY data for the A5-T6 sequence also indicate that there is little change in junction stereochemistry upon drug binding.     

The crystal structure of the octamer [r(guauaca)dC]2 with six Watson-Crick base-pairs and two 3' overhang residues

The crystal structure of an alternating RNA octamer, r(guauaca)dC (RNA bases are in lower case while the only DNA base is in upper case), with two 3' overhang residues one of them a terminal deoxycytosine and the other a ribose adenine, has been determined at 2.2 A resolution. The refined structure has an Rwork 18.6% and Rfree 26.8%. There are two independent duplexes (molecules I and II) in the asymmetric unit cell, a = 24.95, b = 45.25 and c = 73.67 A, with space group P2(1)2(1)2(1). Instead of forming a blunt end duplex with two a+.c mispairs and six Watson-Crick base-pairs, the strands in the duplex slide towards the 3' direction forming a two-base overhang (radC) and a six Watson-Crick base-paired duplex. The duplexes are bent (molecule I, 20 degrees; molecule II, 25 degrees) and stack head-to-head to form a right-handed superhelix. The overhang residues are looped out and the penultimate adenines of the two residues at the top end (A15) are anti and at the bottom (A7) end are syn. The syn adenine bases form minor groove A*(G.C) base triples with C8-H...N2 hydrogen bonds. The anti adenine in molecule II also forms a triple and a different C2-H...N3 hydrogen bond, while the other anti adenine in molecule I does not, it stacks on the looped out overhang base dC. The 3' terminal deoxycytosines form two stacked hemiprotonated trans d(C.C)+ base-pairs and the pseudo dyad related molecules form four consecutive deoxyribose and ribose zipper hydrogen bonds in the minor groove.     

Solution structure of a trinucleotide A-T-A bulge loop within a DNA duplex.

We have synthesized an oligodeoxynucleotide duplex, d(G-C-A-T-C-G-A-T-A-G-C-T-A-C-G).d(C-G-T-A-G-C-C-G-A-T-C-G), with a three-base bulge loop (A-T-A) at a central site in the first strand. Nuclear Overhauser experiments (NOESY) in H2O indicate that the GC base pairs flanking the bulge loop are intact between 0 and 25 degrees C. Nuclear Overhauser effects in both H2O and D2O indicate that all bases within the bulge loop are stacked into the helix. These unpaired bases retain an anti conformation about their glycosidic bonds as they stack within the duplex. The absence of normal sequential connectivities between the two cytosine residues flanking the bulge site on the opposite strand indicates a disruption in the geometry of this base step upon insertion of the bulged bases into the helix. This conformational perturbation is more akin to a shearing apart of the bases, which laterally separates the two halves of the molecule, rather than the "wedge" model often invoked for single-base bulges. Using molecular dynamics calculations, with both NOE-derived proton-proton distances and relaxation matrix-calculated NOESY cross peak volumes as restraints, we have determined the solution structure of an A-T-A bulge loop within a DNA duplex. The bulged bases are stacked among themselves and with the guanine bases on either side of the loop. All three of the bulged bases are displaced by 2-3 A into the major groove, increasing the solvent accessibility of these residues. The ATA-bulge duplex is significantly kinked at the site of the lesion, in agreement with previously reported electron microscopy and gel retardation studies on bulge-containing duplexes [Hsieh, C.-H., & Griffith, J. D. (1989) Proc. Natl. Acad. Sci. U.S.A 86, 4833-4837; Bhattacharyya, A., & Lilley, D. M. J. (1989) Nucleic Acids Res. 17, 6821-6840]. Bending occurs in a direction away from the bulge-containing strand, and we find a significant twist difference of 84 degrees between the two base pairs flanking the bulge loop site. This value represents 58% of the twist difference for base pairs four steps apart in B-DNA. These results suggest a structural mechanism for the bending of DNA induced by unpaired bases, as well as accounting for the effect bulge loops may have on the secondary and tertiary structures of nucleic acids.     

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.     

Preferred positions of AA and TT dinucleotides in aligned nucleosomal DNA sequences.

Multiple alignment of 118 nucleosomal DNA sequences by maximizing simultaneously match of AA dinucleotides and match of TT dinucleotides results in a pattern of the dinucleotide distributions which is characteristic of the nucleosomal DNA sequences. The AA dinucleotides are found to be distributed symmetrically relative to the TT dinucleotide distribution, around the middle point of the nucleosomal DNA sequence. The distances between major peaks of the distributions are multiples of about 10.4 bases. The peaks of the TT distribution are shifted by 6 bases downstream from the peaks of the AA distribution.     

A DNA hairpin with a single residue loop closed by a strongly distorted Watson-Crick G x C base-pair

Our previous NMR and modeling studies have shown that the single-stranded 19mer oligonucleotides d(AGCTTATC-ATC-GATAA GCT) -ATC- and d(AGCTTATC-GAT-GATAAGCT) -GAT- encompassing the strongest topoisomerase II cleavage site in pBR322 DNA could form stable hairpin structures. A new sheared base-pair, the pyrimidine-purine C x A, was found to close the single base -ATC- loop, while -GAT- displayed a flexible loop of three/five residues with no stabilizing interactions. Now we report a structural study on -GAC-, an analog of -GAT-, derived through the substitution of the loop residue T by C. The results obtained from NMR, non-denaturing PAGE, UV-melting, circular dichroism experiments and restrained molecular dynamics indicate that -GAC- adopts a hairpin structure folded through a single residue loop. In the -GAC- hairpin the direction of the G9 sugar is reversed relative to the C8 sugar, thus pushing the backbone of the loop into the major groove. The G9 x C11 base-pair closing the loop is thus neither a sheared base-pair nor a regular Watson-Crick one. Although G9 and C11 are paired through hydrogen bonds of Watson-Crick type, the base-pair is not planar but rather adopts a wedge-shaped geometry with the two bases stacked on top of each other in the minor groove. The distortion decreases the sugar C1'-C1' distance between the paired G9 and C11, to 8 A versus 11 A in the standard B-DNA. The A10 residue at the center of the loop interacts with the G9 x C11 base-pair, and seems to contribute to the extra thermal stability displayed by -GAC- compared to -GAT-. Test calculations allowed us to identify the experimental NOEs critical for inducing the distorted G.C Watson-Crick base-pair. The preference of -GAC- for a hairpin structure rather than a duplex is confirmed by the diffusion constant values obtained from pulse-field gradient NMR experiments. All together, the results illustrate the high degree of plasticity of single-stranded DNAs which can accommodate a variety of turn-loops to fold up on themselves.     

A-form conformational motifs in ligand-bound DNA structures

Recognition and biochemical processing of DNA requires that proteins and other ligands are able to distinguish their DNA binding sites from other parts of the molecule. In addition to the direct recognition elements embedded in the linear sequence of bases (i.e. hydrogen bonding sites), these molecular agents seemingly sense and/or induce an "indirect" conformational response in the DNA base-pairs that facilitates close intermolecular fitting. As part of an effort to decipher this sequence-dependent structural code, we have analyzed the extent of B-->A conformational conversion at individual base-pair steps in protein and drug-bound DNA crystal complexes. We take advantage of a novel structural parameter, the position of the phosphorus atom in the dimer reference frame, as well as other documented measures of local helical structure, e.g. torsion angles, base-pair step parameters. Our analysis pinpoints ligand-induced conformational changes that are difficult to detect from the global perspective used in other studies of DNA structure. The collective data provide new structural details on the conformational pathway connecting A and B-form DNA and illustrate how both proteins and drugs take advantage of the intrinsic conformational mechanics of the double helix. Significantly, the base-pair steps which exhibit pure A-DNA conformations in the crystal complexes follow the scale of A-forming tendencies exhibited by synthetic oligonucleotides in solution and the known polymorphism of synthetic DNA fibers. Moreover, most crystallographic examples of complete B-to-A deformations occur in complexes of DNA with enzymes that perform cutting or sealing operations at the (O3'-P) phosphodiester linkage. The B-->A transformation selectively exposes sugar-phosphate atoms, such as the 3'-oxygen atom, ordinarily buried within the chain backbone for enzymatic attack. The forced remodeling of DNA to the A-form also provides a mechanism for smoothly bending the double helix, for controlling the widths of the major and minor grooves, and for accessing the minor groove edges of individual base-pairs.     

Dependence of the hydration shell structure in the minor groove of the DNA double helix on the groove width as revealed by Monte Carlo simulation.

The hydration shell of several conformations of the polynucleotides poly(dA).poly(dT), poly(dA).poly(dU), and poly(dA-dI).poly(dT-dC) has been simulated using the Monte Carlo method (Metropolis sampling). Calculations have shown that the structure of the hydration shell of the minor groove greatly depends on its width. In conformations with a narrowed minor groove, the first layer of the hydration shell of this groove has only one molecule per nucleotide pair that forms H bonds with purine N3 of one pair and pyrimidine O2 of the next pair. The second layer of the hydration shell of such conformations contains molecules that form H bonds between two adjacent molecules of the first layer. The probability of formation of hydration spine is about 20% while the bridges of the first layer are formed with a probability of about 70%. In the first layer of the minor groove of the B-DNA conformation with wide minor groove there are approximately two water molecules per base pair that form H bonds with purine N3 or pyrimidine O2 and with the sugar ring oxygen of the adjacent nucleotide. The probability of simultaneous H bonding of a water molecule with N3 (or O2) and O of sugar ring is about 30%. The results of simulation suggest that hydration spine proposed for the narrowed minor groove of oligonucleotide crystals [H. R. Drew, and R. E. Dickerson (1981) Journal of Molecular Biology, Vol. 151, pp. 535-556] can be formed in fibers of poly(dA).poly(dT), poly(dA).poly(dU), and poly(dA-dI).poly(dT-dC) as well as in DNA fragments of these sequences in solution.(ABSTRACT TRUNCATED AT 250 WORDS)     

Free energy and structural pathways of base flipping in a DNA GCGC containing sequence

Structural distortions of DNA are essential for its biological function due to the genetic information of DNA not being physically accessible in the duplex state. Base flipping is one of the simplest structural distortions of DNA and may represent an initial event in strand separation required to access the genetic code. Flipping is also utilized by DNA-modifying and repair enzymes to access specific bases. It is typically thought that base flipping (or base-pair opening) occurs via the major groove whereas minor groove flipping is only possible when mediated by DNA-binding proteins. Here, umbrella sampling with a novel center-of-mass pseudodihedral reaction coordinate was used to calculate the individual potentials of mean force (PMF) for flipping of the Watson-Crick (WC) paired C and G bases in the CCATGCGCTGAC DNA dodecamer. The novel reaction coordinate allowed explicit investigation of the complete flipping process via both the minor and major groove pathways. The minor and major groove barriers to flipping are similar for C base flipping while the major groove barrier is slightly lower for G base flipping. Minor groove flipping requires distortion of the WC partner while the flipping base pulls away from its partner during major groove flipping. The flipped states are represented by relatively flat free energy surfaces, with a small, local minimum observed for the flipped G base. Conserved patterns of phosphodiester backbone dihedral distortions during flipping indicate their essential role in the flipping process. During flipping, the target base tracks along the respective grooves, leading to hydrogen-bonding interactions with neighboring base-pairs. Such hydrogen-bonding interactions with the neighboring sequence suggest a novel mechanism of sequence dependence in DNA dynamics.     

Crystallographic study of one turn of G/C-rich B-DNA

The DNA decamer d(CCAGGCCTGG) has been studied by X-ray crystallography. At a nominal resolution of 1.6 A, the structure was refined to R = 16.9% using stereochemical restraints. The oligodeoxyribonucleotide forms a straight B-DNA double helix with crystallographic dyad symmetry and ten base-pairs per turn. In the crystal lattice, DNA fragments stack end-to-end along the c-axis to form continuous double helices. The overall helical structure and, notably, the groove dimensions of the decamer are more similar to standard, fiber diffraction-determined B-DNA than A-tract DNA. A unique stacking geometry is observed at the CA/TG base-pair step, where an increased rotation about the helix axis and a sliding motion of the base-pairs along their long axes leads to a superposition of the base rings with neighboring carbonyl and amino functions. Three-center (bifurcated) hydrogen bonds are possible at the CC/GG base-pair steps of the decamer. In their common sequence elements, d(CCAGGCCTGG) and the related G.A mismatch decamer d(CCAAGATTGG) show very similar three-dimensional structures, except that d(CCAGGCCTGG) appears to have a less regularly hydrated minor groove. The paucity of minor groove hydration in the center of the decamer may be a general feature of G/C-rich DNA and explain its relative instability in the B-form of DNA.     

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.     

Netropsin specifically recognizes one of the two conformationally equivalent strands of poly(dA).poly(dT). One dimensional NMR study at 500 MHz involving NOE transfer between netropsin and DNA protons

Recent observations that the heteronomous structural model for poly(dA).poly(dT) is not found in solution and that in this DNA, the two strands are conformationally equivalent (J. Biomole. Str. Dyns. 2, 1057 (1985], has added a new dimension to the structural dynamics of DNA-netropsin complex. Does the antibiotic somehow distinguish between the two strands and specifically interact with only one of the conformationally equivalent strands? Model-building studies suggest that netropsin can either bind to the dA-strand in the minor groove such that H-bonds are formed between the imino protons N4-H, N6-H, N8-H of netropsin and N3 atoms of A or can bind to the dT-strand in the minor groove and form H-bonds between the imino-protons N4-H, N6-H, N8-H of netropsin and O2 atoms of T. If netropsin binds to the dA-strand, AH2 atoms of poly(dA).poly(dT) would be in closer proximity to the imino protons N4-H, N6-H, N8-H and pyrrole ring protons C5-H, C11-H of netropsin than they would be, if netropsin binds to the dT-strand. In order to distinguish these possibilities experiments were conducted which involved NOE energy transfer between netropsin and DNA protons in the drug-DNA complex. Difference NOE spectra of netropsin-poly(dA).poly(dT) complex in which AH2 was irradiated indicate that dominant NOEs were observed at the imino and pyrrole ring protons of netropsin. When the netropsin pyrrole ring protons were irradiated, the magnetization transfer was at AH2 of DNA. These observations suggest that netropsin binds to the dA-strand of poly(dA).poly(dT) even though dA/dT strands are conformationally equivalent.     

Sequence structure of hidden 10.4-base repeat in the nucleosomes of C. elegans

By measuring prevailing distances between YY, YR, RR, and RY dinucleotides in the large database of the nucleosome DNA fragments from C. elegans, the consensus sequence structure of the nucleosome DNA repeat of C. elegans was reconstructed: (YYYYYRRRRR)n. An actual period was estimated to be 10.4 bases. The pattern is fully consistent with the nucleosome DNA patterns of other eukaryotes, as established earlier, and, thus, the YYYYYRRRRR repeat can be considered as consensus nucleosome DNA sequence repeat across eukaryotic species. Similar distance analysis for [A, T] dinucleotides suggested the related pattern (TTTYTARAAA)n where the TT and AA dinucleotides display rather out of phase behavior, contrary to the "AA or TT" in-phase periodicity, considered in some publications. A weak 5-base periodicity in the distribution of TA dinucleotides was detected.