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  • 1
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: We describe the crystal structure of an octameric DNA sequence, d(GGm5CCGGCC), at 2.25 Å resolution. The sequence contains one C5-methylated cytosine per DNA strand. This methylation corresponds to that utilized in vivo by the HaeIII restriction modification system. The present structure is compared to that of the unmethylated octamer solved previously as well as to other A-DNA crystal structures. It retains the characteristics seen in these other DNA molecules, i.e., reduced base-pair tilt angles and increased major groove width, indicating that the presence of the methyl groups does not drastically affect the A-DNA backbone conformation. The position of the methyl groups appears to block the major grove, thus preventing potential sequence-specific protein interactions. In addition, the presence of these hydrophobic substituents may enhance the overall stability of the A-DNA conformation.
    Additional Material: 9 Ill.
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  • 2
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Chemical shifts of base and H1′ protons of the single-stranded hexamers d(ATTACC) and d(GGTAAT), of the 1 : 1 mixtures of these complementary hexamers, and of the self-complementary dodecamer d(ATTACCGGTAAT) were measured at various temperatures in aqueous solution. Four different sample concentrations were used in the case of the dodecamer and of the mixture of the complementary hexamers; the individual hexamers were measured at two different DNA concentrations. Absorbance temperature profiles at five different NaCl concentrations were measured for the dodecamer in order to quantify the effect of the ionic strength on the duplex formation.Under suitable conditions of nucleotide concentration, temperature, and ionic strength, the dodecamer adopts either a B-DNA duplex or a hairpin-loop structure. Chemical shift vs temperature profiles, constructed for all samples, were used to obtain thermodynamic parameters either for the various stacking interactions in the single strands or for the duplex or the hairpin-loop formation. In the analysis of the duplex formation of the hexamers, a two-state approach appeared too simple, because systematic deviations were revealed. Therefore, a new three-state model (DUPSTAK) was developed. In order to investigate the magnitude of error arising from the use of the two-state approach in cases where the DUPSTAK model appears more appropriate, a series of test calculations was made. The magnitude of error in the enthalpy and in the entropy of duplex melting is found to depend linearly upon the actual melting temperature and not upon the individual ΔHOd and ΔSOd values.Thermodynamic analysis of the chemical shift vs temperature profiles in D2O solution (no added salt) yields an average Tmd value of 341 K (1M DNA) and ΔHOd of -121 kJ · mol-1 for the dimer/random-coil transition of the hexamer duplex d(ATTACC) · d(GGTAAT). For the duplex ⇄ random-coil transition of the 12-mer d(ATTACCGGTAAT) an average Tmd value of 336 K (1M DNA) and ΔHOd of -372 kJ · mol-1 are found. The hairpin/random-coil transition of d(ATTACCGGTAAT) is characterized by a rather large ΔHOh value, -130 kJ · mol-1, and an average Tmh value of 304 K.
    Additional Material: 9 Ill.
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  • 3
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: The left-handed Z-DNA structure of an araC-containing (where araC stands for arabinosylcytosine) hexamer, (araC-dG)3, has been solved by x-ray diffraction analysis at 1.3 A resolution. This hexamer was crystallized in the hexagonal P6522 (a = b = 17.96 Å, c = 43.22 Å) space group in which the hexamers have statistically disordered packing arrangement along the 65 screw axis, yet the crystals diffract x-rays to high resolution. Its structure has been refined by the constrained least square refinement to a final R factor of 0.287 using 737 [〉 3.0 σ(F)] observed reflections. The asymmetric unit of the unit cell contains only a dinucleotide, 5′-p(araC)p(dG). The overall conformation resembles that of the canonical Z-DNA, but with some differences in details. The O2′ hydroxyl groups of the araC residues form intramolecular hydrogen bonds with N2 of the 5′-guanine residues. In the deep groove of Z-DNA, these hydroxy groups replace the bridging water molecules that stabilize the guanine in the syn conformation. The results reinforce the earlier observation made by the structural analysis of another hexamer, d(CG[araC]GCG), with a mono-substitution of araC [M.-K. Teng, Y.-C. Liaw, G. A. van der Marel, J. H. van Boom, and A. H.-J. Wang (1989) Biochemistry, vol. 28, pp. 4923-4928]. These two structures show that araC residue can be incorporated readily into the Z structure and probably facilitates the B to Z transition, as supported by uv absorption spectroscopic studies in a number of araC-containing oligonucleotides. The potential biological roles of the araC-modified Z-DNA are discussed. © 1992 John Wiley & Sons, Inc.
    Additional Material: 6 Ill.
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  • 4
    ISSN: 0006-3525
    Keywords: DNA structures ; nucleic acids ; structure elucidation ; nmr spectroscopy ; molecular modeling ; Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: TheDNA sequences 5′-d(CGC-AC-GCG)-3′ (HPAC), 5′-d(CGC-AA-GCG)-3′ (HPAA), 5′-d(CGC-TC-GCG)-3′ (HPTC), and 5′-d(CGC-CT-GCG)-3′ (HPCT), were studied by means of nmr spectroscopy. At low DNA concentration and no added salt all four molecules adopt a minihairpin structure, containing three Watson-Crick base pairs and a two-residue loop. The structure of the HPAC hairpin is based on quantitative distance restraints, derived by a full relaxation matrix approach (iterative relaxation matrix approach), together with torsion angles obtained from coupling constant analysis. The loop folding is of the H1-family type, characterized by continuous 3′-5′ stacking of the loop bases on the duplex stem. The structure of the HPAA hairpin is similar to that of HPAC, but is more flexible and has a lower thermodynamic stability (Tm 326 K vs 320 K). According to “weakly” distance-constrained simulations in water on the HPAC minihairpin, the typical H1-family loop folding remains intact during the simulation. However, residue-based R factors of simulated nuclear Overhauser effect spectroscopy spectra, free molecular dynamics simulations in vacuo, and unusual chemical shift profiles indicate partial destacking of the loop bases at temperatures below the overall melting midpoint. The dynamic nature of the loop bases gives insight into the geometrical tolerances of stacking between bases in H1-family minihairpin loops. The HPTC and HPCT minihairpins, both containing a pyrimidine base at the first position in the loop, adopt a H2-family type folding, in which the first loop base is loosely bound in the minor groove and the second loop base is stacked upon the helix stem. The thermal stability for these two hairpins corresponds to 327-329 K, but depends on local base sequence. Preference for the type of folding depends on a single substitution from a pyrimidine (H2 family) to a purine (H1 family) at the first position of the miniloop and is explained by differences in base stacking energies, steric size, and the number of possible candidates for hydrogen bonds in the minor groove. In view of newly collected data, previous models of the H1-family and H2-family hairpins had to be revised and are now compatible with the reported HPTC and HPAC structures. The structural difference between the refined structure of HPAC and HPTC show that a conversion between H1-family and H2-family hairpins is geometrically possible by a simple pivot point rotation of 270° along two torsion angles, thereby swiveling the first loop base from a stacked position in a H1-family folding toward a position in the minor groove in a H2-family folding. The second loop residue subsequently shifts to the position of the first base in a concerted fashion. © 1998 John Wiley & Sons, Inc. Biopoly 46: 375-393, 1998
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  • 5
    ISSN: 0006-3525
    Keywords: Chemistry ; Polymer and Materials Science
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Both (dC-dG)4 and d(CGCATGCG) crystallize in hexagonal lattices and their three-dimensional structure has been solved by x-ray diffraction analysis. Both molecules are found to form Z-DNA, although the fine details of the structure cannot be visualized due to the statistical disordering of the molecules along the c-axis, which is brought about by the symmetry constraints of the space group. This represents the first time in which the unmodified dinucleotide sequences CpAp and TpGp have been found to form Z-DNA in a crystalline lattice.
    Additional Material: 1 Ill.
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