Characterization of divalent cation localization in the minor groove of the A(n)T(n) and T(n)A(n) DNA sequence elements by (1)H NMR spectroscopy and manganese(II)

The localization of Mn(2+) in A-tract DNA has been studied by (1)H NMR spectroscopy using a series of self-complementary dodecamer oligonucleotides that contain the sequence motifs A(n)(n) and T(n)A(n), where n = 2, 3, or 4. Mn(2+) localization in the minor groove is observed for all the sequences that have been studied, with the position and degree of localization being highly sequence-dependent. The site most favored for Mn(2+) localization in the minor groove is near the 5'-most ApA step for both the T(n)A(n) and the A(n)T(n) series. For the T(n)A(n) series, this results in two closely spaced symmetry-related Mn(2+) localization sites near the center of each duplex, while for the A(n)T(n) series, the two symmetry-related sites are separated by as much as one half-helical turn. The degree of Mn(2+) localization in the minor groove of the T(n)A(n) series decreases substantially as the AT sequence element is shortened from T(4)A(4) to T(2)A(2). The A(n)T(n) series also exhibits length-dependent Mn(2+) localization; however, the degree of minor groove occupancy by Mn(2+) is significantly less than that observed for the T(n)A(n) series. For both A(n)T(n) and T(n)A(n) sequences, the 3'-most AH2 resonance is the least broadened of the AH2 resonances. This is consistent with the observation that the minor groove of A-tract DNA narrows in the 5' to 3' direction, apparently becoming too narrow after two base pairs for the entry of a fully hydrated divalent cation. The results that are reported illustrate the delicate interplay that exists between DNA nucleotide sequence, minor groove width, and divalent cation localization. The proposed role of cation localization in helical axis bending by A-tracts is also discussed.     

A theoretical study of the structures of (Gly-Pro-Leu)n and (Gly-Leu-Pro)n

Theoretical conformation studies have been carried out for the polytripeptides (Gly-Pro-Leu)n and (Gly-Leu-Pro)n and the Fourier transforms of the structures have been calculated. X-ray powder patterns of these polymers had indicated that both these polymers take up coiled-coil triple-helical structures, but in the case of (Gly-Pro-Leu)n it was not clear whether the triple helix is formed by three parallel polypeptide chains or by a single chain folding back on itself (Scatturin et al 1975). Our studies show that both the polytripeptides can take up stereochemically satisfactory triple-helical structures with three parallel chains. There is also very good agreement between the calculated intensity distribution and that of the observed X-ray pattern, in each case.     

Stabilization of (dG-dC)n.(dG-dC)n in the Z conformation by a crosslinking reaction

(dG-dC)n.(dG-dC) was converted to the Z conformer by heating in the presence of Mn++n. Reaction of this preparation with the crosslinking reagent, DL-diepoxybutane (DEB), stabilized this conformer so that it retained its structure even when returned to conditions that favored reversion to the B conformation. Treatment of the crosslinked Z conformer with periodate caused scission of the crosslink, allowing reversion to the B conformer. Reaction of (dG-dC)n.(dG-dC)n in the B conformation with DEB did not prevent conversion to the Z conformer in 4M NaC1; dialysis of the high salt solution against low ionic strength buffer allowed return to the B conformer. The Z in equilibrium B transitions were followed by circular dichroism studies and immunochemical procedures. The results suggest the feasibility of stabilizing Z sequences of DNA in chromatin by crosslinking, so that they could then be identified after DNA isolation.     

Spectroscopic studies on acetylaminofluorene-modified (dT-dG)n . (dC-dA)n suggest a left-handed conformation

CD spectroscopy on the double-stranded strictly alternating dinucleotide polymer (dT-dG)n . (dC-dA)n partially modified by N-acetoxy-N-acetyl-2-aminofluorene suggests a left-handed conformation in concentrated NaCl solutions. Modification of the (dT-dG)n . (dC-dA)n polymer with acetylaminofluorene is required to promote formation of the left-handed helix since high salt concentrations and several other ionic conditions, which cause a similar transition for (dG-dC)n . (dG-dC)n, are ineffective. Furthermore, substitution of dC with 5-methyl dC in (dT-dG)n . (dC-dA)n does not facilitate formation of a left-handed helix, also in contrast to results found for (dG-dC)n . (dG-dC)n. A 62-base pair tract of almost perfectly alternating (dT-dG)n . (dC-dA)n from the 3'-side of the mouse kappa immunoglobulin gene modified with acetylaminofluorene undergoes the salt-induced transition to a left-handed helix when studied within a 140-base pair restriction fragment. High NaCl concentrations alone will not cause the transition for this 62-base pair tract in this fragment nor in the recombinant plasmid pRW777, which contains this fragment.     

Electrophoretic behavior of d(GGAAAAAAGG)n, d(CCAAAAAACC)n, and (CCAAAAAAGG)n and implications for a DNA bending model.

Double stranded multimers (C2A6C2)n, (C2A6G2)n and (G2A6G2)n were prepared from chemically synthesized oligonucleotides to study the influence of sequences flanking the An tract on the curvature of DNA. All these duplexes, including polypurine.polypyrimidine one, exhibit strong retardation in polyacrylamide gel which is indicative of pronounced DNA curvature. It has been proposed previously that among the bends at the boundary with the oligo(A) tract two types should be distinguished: 5'-bends and 3'-bends (Koo et al., 1986) This distinction was deduced from different relative mobilities of two specially designed sequences having phased 5'-bends and 3'-bends, respectively. Our data indicate that the substitutions of nucleotides at both 5' and 3' boundaries of A6 tract result in comparable changes in relative mobility. Therefore, for B-B' bends it is important to take into account not only whether they are at the 5' or 3' end of an oligo(dA) tract, but also the particular sequences at the boundaries of this tract.     

Raman Spectroscopy Study of the B-Z Transition in (dG-dC)n · (dG-dC)n and a DNA Restriction Fragment

Abstract

The B to Z conformational transition of (dG-dC)_n·(dG-dC)_n and a 157 bp DNA restriction fragment were followed using Raman spectroscopy. The 157 bp DNA has a 95 bp segment from the E. coli lactose operon sandwiched between 26 and 32 bp of (dC-dG) sequences. Raman spectra of the DNAs were obtained at varying sodium chloride concentrations through the region of the transition. A data analysis procedure was developed to subtract the background curves and quantify Raman vibrational bands. Profiles of relative intensity vs. sodium chloride concentration are shown for bands at 626, 682, 831–833 and 1093 cm^?1. Both (dG-dC)_n·(dG-dC)_n and the 157 bp DNA show changes in the guanine vibration at 682 cm^?1 and backbone band at 831–3 cm^?1 preceeding a highly cooperative change in the 1093 cm^?1 PO 7 vibration. This result indicates that there are at least two conformational steps in the B to Z conformational pathway.

We review the effect of the (dC-dG) portion of the 157 bp DNA on the 95 bp segment. Comparison of Raman spectra of the 157 bp DNA, the 95 bp fragment and (dG-dC)_n·(dG- dC)_n indicate that in 4.5 M NaC/the (dC-dG) segments are in a Z-conformation. Base stacking in the 95 bp portion of the 157 bp DNA appears to maintain a B-type conformation. However, a substantial portion of this region no longer has a B-type backbone vibration.     

Magnesium-dependent supercoiling-induced transition in (dG)n.(dC)n stretches and formation of a new G-structure by (dG)n strand.

Plasmids containing (dG)27.(dC)27 inserts (pPG27), (dG)37.(dC)37 inserts (pPG37), and (dG)24C(dG)21.(dC)24G(dC)21 inserts (pPG46C) were constructed for the study of structural transitions within (dG)n.(dC)n stretches. Two-dimensional gel electrophoresis has shown that a Mg2+-dependent supercoiling-induced structural transition takes place at pH 8 in plasmid pPG46C. The transition occurs at -0=0.06 and involves a supercoiling release corresponding to 5 superhelical turns. After denaturation of the restriction fragments containing (dG)n.(dC)n inserts, the strands do not renature completely and (dG)n-containing strand migrates in PAGE much faster than the (dC)n-containing one. Chemical modification experiments with the (dG)n-strand have revealed the periodic nature of the protection of guanines against dimethyl sulfate methylation. The (dG)n strand in the presence of Mg2+ forms complexes with the complementary (dC)n strand, which differ from the native duplex in mobility. We believe these effects to be due to the formation of an intrastrand structure within the (dG)n strand stabilized by G.G interactions (we called it G-structure), which in the presence of Mg2+ forms an interstrand complex. with the (dC)n strand.     

Conformational analysis of polytripeptides (Gly-Pro-Ala)n, (Gly-Ala-Hyp)n,and (Gly-Ala-Ala)n in connection with the problem of collagen structure

Conformational analysis of triple helics of a type of collagen was performed with typical collagen tripeptide sequences based on Gly-Pro-Ala, Gly-Ala-Hyp, and Gly-Ala-Ala. During energy minimization, the possibility of continual deformation of the pyrrolidine cycle was taken into account in order to achieve better accuracy in the resulting structure. The (Gly-Pro-Ala)_n structure is almost isomorphic to the (Gly-Pro-Hyp)_n structure obtained in the previous work [Tumanyan, V. G. & Esipova, N.G. (1982) Biopolymers 21 , 475–497]. For a collagen-type structure, the optimal conformation of (Gly-Ala-Hyp)_n tends to have a decreased unit twist (t = 15°), although the energy advantage with respect to the conformation with t = 45° is not so significant. A similar situation is observed for (Gly-Ala-Ala)_n. In this case, the energy decrease during unwinding to t = 15° from t = 45° is quite small. The conformations of (Gly-Ala-Hyp)_n and (Gly-Ala-Ala)_n with t = 15° exhibit a similarity with a triple complex of polyproline II helices—a noncoiled coil such as (Gly-Pro-Hyp)_n and (Gly-Pro-Ala)_n. A similar structure may be postulated for subcomponent cq1 of the first component of a human complement containing substantial Gly-X-Pro and Gly-X-Y tripeptide derivatives in the primary structure (X, Y = any amino acid). The results suggest that the observed helical symmetry of collagen (t = 36°) is a consequence of superposition of diffraction patterns (for sufficiently long segments) from various helices (t varies from ～15° for Gly-X-Hyp and Gly-X-Y to ～56° for Gly-Pro-Ala). For short alternating segments, some unification of different helical structures is possible.     

Length-dependent energetics of (CTG)n and (CAG)n trinucleotide repeats

Trinucleotide repeats are involved in a number of debilitating diseases such as myotonic dystrophy. Twelve to seventy-five base-long (CTG)_n oligodeoxynucleotides were analysed using a combination of biophysical [UV-absorbance, circular dichroism and differential scanning calorimetry (DSC)] and biochemical methods (non-denaturing gel electrophoresis and enzymatic footprinting). All oligomers formed stable intramolecular structures under near physiological conditions with a melting temperature that was only weakly dependent on oligomer length. Thermodynamic analysis of the denaturation process by UV-melting and calorimetric experiments revealed an unprecedented length-dependent discrepancy between the enthalpy values deduced from model-dependent (UV-melting) and model-independent (calorimetry) experiments. Evidence for non-zero molar heat capacity changes was also derived from the analysis of the Arrhenius plots and DSC profiles. Such behaviour is analysed in the framework of an intramolecular ‘branched-hairpin’ model, in which long CTG oligomers do not fold into a simple long hairpin–stem intramolecular structure, but allow the formation of several independent folding units of unequal stability. We demonstrate that, for sequences ranging from 12 to 25 CTG repeats, an intramolecular structure with two loops is formed which we will call ‘bis-hairpin’. Similar results were also found for CAG oligomers, suggesting that this observation may be extended to various trinucleotide repeats-containing sequences.     

Conformational change of the triple-helical structure. II. Conformation of (Pro-Pro-Gly)n and (Pro-Pro-Gly)n (Ala-Pro-Gly)m(Pro-Pro-Pro-Gly)n in an aqueous solution

Measurements of the molecular weight of (Pro-Pro-Gly)_n and (Pro-Pro-Gly)_n(Ala-Pro-Gly)_m(Pro-Pro-Gly)_n, which were synthesized by the solid-phase method, revealed that they formed a trimer in an aqueous solution, and dissociated into single-stranded chains on warming. Accompanying the transition, a large decrease of optical rotation was observed, like the collagen–gelatin transition. The shape of the trimeric molecule was rodlike, and the dimensions were 12 Å in diameter and 2.8 Å per residue in length, regardless of the length of Ala-Pro-Gly sequences in a peptide chain. The data indicate that both Pro-Pro-Gly sequences and Ala-Pro-Gly sequences from the triple-helical structure similar to that of collagen in aqueous solution. All optical rotational dispersion (ORD) curves of solutions of the peptides were represented by a single-term Drude equation, and the Drude constant λ_c was 200 nm for all peptides regardless of the length of Ala-Pro-Gly sequences. The resemblance between the helical structure formed by Pro-Pro-Gly sequences and that by Ala-Pro-Gly sequences was also suggested by the formation of the hybrid triple helix from two kinds of peptide chains with different lengths of Ala-Pro-Gly sequences.     

Informativeness of human (dC-dA)n.(dG-dT)n polymorphisms

Abundant human interspersed repetitive DNA sequences of the form (dC-dA)n.(dG-dT)n have been shown to exhibit length polymorphisms. Examination of over 100 human (dC-dA)n.(dG-dT)n sequences revealed that the sequences differed from each other both in numbers of repeats and in repeat sequence type. Using a set of precise classification rules, the sequences were divided into three categories: perfect repeat sequences without interruptions in the runs of CA or GT dinucleotides (64% of total), imperfect repeat sequences with one or more interruptions in the run of repeats (25%), and compound repeat sequences with adjacent tandem simple repeats of a different sequence (11%). Informativeness of (dC-dA)n.(dG-dT)n markers in the perfect sequence category was found to increase with increasing average numbers of repeats. PIC values ranged from 0 at about 10 or fewer repeats to above 0.8 for sequences with about 24 or more repeats. (dC-dA)n.(dG-dT)n polymorphisms in the imperfect sequence category showed lower informativeness than expected on the basis of the total numbers of repeats. The longest run of uninterrupted CA or GT repeats was found to be the best predictor of informativeness of (dC-dA)n.(dG-dT)n polymorphisms regardless of the repeat sequence category.     

UV-induced interstrand cross-linking of d(GT)n.d(CA)n is facilitated by a structural transition

Photochemical alterations following ultraviolet irradiation of the alternating copolymer d(GT)n.d(CA)n were studied. We found that in solution conditions which produced circular dichroism spectra compatible with B-form or A-form DNA, no interstrand cross-linking or photoproduct formation could be demonstrated. Zimmer et al. (Zimmer, C., Tymen, S., Marck, C., and Guschlbaumer, W. (1982) Nucleic Acids Res. 10, 1081-1091) and Vorlickova et al. (Vorlickova, M., Kypr, J., Sotkrova, S., Sponar, J. (1982) Nucleic Acids Res. 10, 1071-1080) have reported a number of solution conditions which produce a structural transition of this polymer characterized by a negative deviation of the circular dichroism spectrum in the region of 280 nm. The nature of this transition has not yet been elucidated. Following ultraviolet irradiation of d(GT)n.d(CA)n under two conditions which produce this transition (manganese solution or ethanol plus trace salts solution) we found ultraviolet dose-dependent interstrand cross-linking as well as dose-dependent formation of thymine-containing photoproduct. Interstrand cross-linking is demonstrated by two criteria: increase in polymer size as detected by alkaline agarose gel electrophoresis, and generation of intermediate density material in alkaline cesium sulfate isopycnic gradients. The thymine-containing photo-product was demonstrated by thin layer chromatography of acid hydrolysates of the polymer. The photo-product is at least partially photoreversible. These findings suggest that the geometry of the alternative conformation is such that pyrimidines from different strands are closely approximated, allowing for photodimerization.     

Raman spectroscopy study of the B-Z transition in (dG-dC)n.(dG-dC)n and a DNA restriction fragment

The B to Z conformational transition of (dG-dC)n.(dG-dC)n and a 157 bp DNA restriction fragment were followed using Raman spectroscopy. The 157 bp DNA has a 95 bp segment from the E. coli lactose operon sandwiched between 26 and 32 bp of (dC-dG) sequences. Raman spectra of the DNAs were obtained at varying sodium chloride concentrations through the region of the transition. A data analysis procedure was developed to subtract the background curves and quantify Raman vibrational bands. Profiles of relative intensity vs. sodium chloride concentration are shown for bands at 626, 682, 831-833 and 1093 cm-1. Both (dG-dC)n.(dG-dC)n and the 157 bp DNA show changes in the guanine vibration at 682 cm-1 and backbone band at 831-3 cm-1 preceding a highly cooperative change in the 1093 cm-1 PO2- vibration. This result indicates that there are at least two conformational steps in the B to Z conformational pathway. We review the effect of the (dC-dG) portion of the 157 bp DNA on the 95 bp segment. Comparison of Raman spectra of the 157 bp DNA, the 95 bp fragment and (dG-dC)n.(dG-dC)n indicate that in 4.5 M NaCl the (dC-dG) segments are in a Z-conformation. Base stacking in the 95 bp portion of the 157 bp DNA appears to maintain a B-type conformation. However, a substantial portion of this region no longer has a B-type backbone vibration.     

Diepoxybutane forms a monoadduct with B-form (dG-dC)n.(dG-dC)n and a crosslinked diadduct with the left-handed Z-form.

The characteristics of the reactions of DL-diepoxybutane (DEB) with (dG-dC)n.(dG-dC)n in the right-handed B-form or the left-handed Z-form were investigated. DEB does react with right-handed B-DNA since less salt is required to convert the modified B-form to Z-form than for the unmodified DNA. However, the product appears to be a monoadduct rather than the crosslinked diadduct formed with the Z-form. The modified B-form can be isolated, converted to a Z-form with l mM MnCl2, and then this activated complex further reacts intramolecularly to give the crosslinked Z-product. This modified Z-form cannot be reverted to the B-form unless the crosslink is cleaved with periodate. Only MnCl2, and to a lesser extent ZnCl2, was effective in facilitating the intramolecular conversion of the B-DNA monoadduct to the Z-DNA diadduct; lmM MgCl2 and 4M NaCl were ineffective suggesting that somewhat different types of modified left-handed conformations were generated by the different salts. DEB also cleaves DNA under our reaction conditions thus precluding studies with supercoiled recombinant plasmids harboring segments that adopt Z-structures.     

Variable (dG-dT)n.(dC-dA)n sequences in the porcine genome.

One of the more widely studied simple repeat sequences in the mammalian genome is the (dG-dT)n.(dC-dA)n dinucleotide repeat sequence. As these repeats are highly polymorphic and fairly evenly distributed in diverse mammalian genomes, they constitute a very powerful tool for genetic mapping in a wide variety of species. So far, the knowledge about repeat sequences in the porcine genome is sparse and only a few areas of this genome have been sequenced. We have isolated and characterized 108 porcine (dG-dT)n.(dC-dA)n sequences and studied the distribution of these, both by investigating random clones and by performing in situ hybridization. A remarkable correlation between humans and pigs was found with respect to the structure, to the number of repeat blocks, and to the chromosomal distribution.     

Comprehensive conformational analysis of (Gly-Pro-Pro)n and (Gly-Pro-Hyp)n related to collagen

A complete analysis of all possible conformations with correct hydrogen bonds of the collagen II type was performed on the basis of developed simultaneous equations. Using a unimodal search (by varying Ψ³), the energetically favorable structure was obtained. No other energetically satisfactory structural solutions are possible. The next aim was to obtain a precise model of the molecule. The program used includes a subroutine for continual deformation of the pyrrolidine rings. The set of parameters determining the structure consists of 14 independent variables (8 dihedral and 6 bond angles). As starting points for the energy optimization, conformations produced by scanning and some structures from previous work were used. The final structures (practically the same for both polymers) have helix parameters h = 0.285 nm and t = 52°, which are in excellent agreement with the 7/2 symmetry of diffraction data. The conformations of the pyrrolidine rings are of the B type, i.e., C₂-C^β-exo-C^γ-endo. For both polypeptides, the conformations of imino acids in position 3 of the triplet are the same; in position 2, however, they are slightly different. The difference in diffraction patterns for the 7/2 and 10/3 helices is discussed.     

Thermodynamics of base interaction in (A)n and (A.U)n

Using precision scanning microcalorimetry we studied (A)_n and (A·U)_n melting in highly diluted solutions (0.3 to 5.0 mm) with different Na⁺ activity. This permitted us to determine directly the thermodynamic functions of stacking interaction in (A)_n and base-pairing in (A·U)_n. For (A-A) stacking at (A)_n melting temperature we obtained ΔH^(A)n_m = 12.6 kJ mol^?1; ΔS^(A)n_m = 41 J K^?1 mol^?1. For A·U base-pairing at a standard temperature of 298 K and 0.1 m-Na⁺ we have: ΔH^(A·U) = 34 kJ mol^?1; ΔS^(A·U) = 102 J K^?1 mol^?1ΔG^(A·U) = ?3.5 kJ mol^?1.