B--Z conformational transition in d(CGCGCGTTAATT), d(CGCGCGTTAA) and d(CGCGCGTT)

Conformational studies on three DNA-oligomers (d(CGCGCGTTAATT), d(CGCGTTAA) and d(CGCGCGTT) in solution by circular dichroism spectroscopy are reported. In low salt solution, all three DNA oligomers exhibit a characteristic B-conformation. However, under the influence of high salt concentration i.e. 5M NaCl, the octamer d(CGCGCGTT) exhibits 'A' conformation whereas the decamer and dodecamer retain B-conformation. On addition of millimolar amount of NiCl2 to the 5M NaCl, solution of oligodeoxynucleotides a B-Z transition is observed in octamer, decamer and dodecamer. However, NiCl2 titrations show that mid point of transition for dodecamer is at 2.25 mM, for decamer is at 13 mM NiCl2 and for octamer is 17 mM at NiCl2. In 60% alcohol all three oligonucleotides remain in the B-conformation. The melting temperatures of oligonucleotides at various salt concentration are also reported. Thermodynamic parameters calculated by melting profile using a two state model show that dodecamer and decamer are most stable in their 5M NaCl, B-form. However, octamer is more stable in its Z form than that of its 'A' form.     

Energetics of Z-DNA formation in poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T).

The conformational change for the alternating purine-pyrimidine polydeoxyribonucleotides i.e. poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T) from a right-handed conformation at room temperature to the left-handed Z-DNA like double helix at elevated temperatures has been studied by UV spectroscopy, Raman spectroscopy, and by adiabatic differential scanning microcalorimetry (DSC) in the presence of Na+ and Mg2+ or Ni2+ respectively as counterions. The differential UV spectra reveal through a hyperchromic shift at around 280nm and a hypochromic shift at 260nm that a conformational change to the left-handed conformation occurs. The Raman spectra clearly show characteristic changes, a drastic decrease of the band at 680cm-1 and the appearance of a new band at 628cm-1, due to the change of the purine bases to the syn conformation upon inversion of the helix-handedness. The course of the transition as function of temperature can be followed quantitatively by plotting the change in the excess heat capacity vs. temperature. The transition enthalpy delta H for the B- to Z-DNA transition per mole base pairs (mbp) amounts to 2.0 +/- 0.2kcal for poly d(G-C), to 4.0 +/- 0.4kcal for poly d(A-T), and to 3.1 +/- 0.3kcal for poly d(A-C) poly d(G-T). The enthalpy change due to the Z-DNA to coil transitions (per mole base pairs) amounts to 11kcal for poly d(G-C), 10.5kcal for poly d(A-T) and 11.3kcal for poly d(A-C) poly d(G-T).     

Laser Photofootprinting of d(C)·d(G)·d(G) Intramolecular Triplex

Abstract

Supercoiling-induced structural transition of the d(C₂₄GC₂₁,) · d(G₂₁CG₂₄) sequence in plasmid DNA in the presence of Mg²⁺ at neutral pH results in alterations of efficiencies of not only single-quantum (pyrimidine[6–4]pyrimidone adducts) but also two-quantum (alkalisensitive lesions of dG residues) photomodifications of nucleoside residues within this sequence. The generation of both types of photoreactions was achieved by the application of high-intensity laser UV radiation (intensity ～ 10¹¹ W/m², pulse duration ～ 10^?8 s, λ= 266 nm) for irradiation of a plasmid DNA The modification extent sufficient for analysis of photoreaction efficiency distributions along both strands of the insert (photofootprinting) was obtained by the action of a single nanosecond pulse of laser UV radiation. The pattern of a laser photofootprinting is consistent with the d(C) · d(G) · d(G) triplex formation in the presence of Mg²⁺ within the insert and shows some details of this triplex structure.     

Molecular-Mechanical studies of the mismatched base analogs of d(CGCGAATTCGCG)2:d(CGTGAATTCGCG)2, d(CGAGAATTCGCG)2, d(CGCGAATTCACG)2, d(CGCGAATTCTCG)2, and d(CGCAGAATTCGCG)·d(CGCGAATTCGCG)

Molecular-mechanical simulations have been carried out on “mismatched base” analogs of the DNA double-helical structure d(CGCGAATTCGCG)₂, in which the base pairs CG at the 3 and 10 positions have been replaced by CA, AG, TC, and TG base pairs, as well as an insertion analog in which an extra adenine has been incorporated into one strand of the above structure between bases 3 and 4. The results of these simulations (calculated relative stabilities, structures, and nmr ring-current shifts) have been compared with calorimetric and nmr data. The calculated relative stabilities of the double-helical parent dodecamer and the various “wobble” base pairs qualitatively correlate with the experimental melting temperatures. The base-pairing structure for the GT wobble pair is in agreement with that previously determined from nmr experiments. For the GA base pair, the structure with both bases anti has a slightly more favorable energy from base pairing and stacking than a structure with non-Watson-Crick H-bonding with adenine syn, in agreement with nmr experiments. The CA wobble base is calculated to favor an adenine 6NH₂ …? cytosine N3 H-bond over cytosine 4NH₂ …? adenine N1, again, in agreement with nmr experiments. There is no definitive experimental data on the TC base pair, but the existence of (somewhat long and weak) H-bonds involving cytosine 4NH₂ …? thymine 4CO and cytosine N3 …? thymine HN3 seems reasonable. We find a structure in which the extra adenine base of the insertion analogs sits “inside” the double helix.     

Structure of poly d(A).poly d(T).

On the basis of the x-ray data from polycrystalline and well oriented fibers of the sodium salt of poly d(A).poly d(T) (Arnott et al, Nucl. Acids Res. 11, 4141-4155 (1983), a revised B'-DNA model incorporating B-like adenine and thymine strands is shown to give a much better x-ray agreement (R = 0.25) than the previously assigned model consisting of mixed sugar conformations in the two strands. The narrowing of the minor and the widening of the major grooves are promiscuous features of B'-DNA, which are common to all poly d(purine).poly d(pyrimidine) duplexes with two hydrogen bonded base-pairs and are in marked contrast with classical B-DNA. Due to modest propeller (-15 degrees), the cross strand diagonal hydrogen bonds (0.37 nm) in this duplex are not as strong as those in A,T-rich oligonucleotide crystal structures.     

Mercury-induced transitions between right-handed and putative left-handed forms of poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)]

Poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)], each dissolved in 0.1 M NaClO4, 5 mM cacodylic acid buffer, pH 6.8, experience inversion of their circular dichroism (CD) spectrum subsequent to the addition of Hg(ClO4)2. Let r identical to [Hg(ClO4)2]added/[DNA-P]. The spectrum of the right-handed form of poly[d(A-T).d(A-T)] turns into that of a seemingly left-handed structure at r greater than or equal to 0.05 while a similar transition is noted with poly[d(G-C).(G-C)] at r greater than or equal to 0.12. The spectral changes are highly cooperative in the long-wavelength region above 250 nm. At r = 1.0, the spectra of the two polymers are more or less mirror images of their CD at r = 0. While most CD bands experience red-shifts upon the addition of Hg(ClO4)2, there are some that are blue-shifted. The CD changes are totally reversible when Hg(II) is removed from the nucleic acids by the addition of a strong complexing agent such as NaCN. This demonstrates that mercury keeps all base pairs in register.     

Effects of poly[d(pGpT).d(pApC)] and poly[d(pCpG).d(pCpG)] repeats on homologous recombination in somatic cells.

Sequencing studies have shown that in somatic cells alternating runs of purines and pyrimidines are frequently associated with recombination crossover points. To test whether such sequences actually promote recombination, we have examined the effects of poly[d(pGpT).d(pApC)] and poly[d(pCpG).d(pCpG)] repeats on a homologous recombination event. The parental molecule used in this study, pSVLD, is capable of generating wild-type simian virus 40 DNA via recombination across two 751-base-pair regions of homology and has been described previously (Miller et al., Proc. Natl. Acad. Sci. USA 81:7534-7538, 1984). Single inserts of either a poly[d(pGpT).d(pApC)] repeat or a poly[d(pCpG).d(pCpG)] repeat were positioned adjacent to one region of homology in such a way that the recombination product, wild-type simian virus 40 DNA, could be formed only by recombination within the homologies and not by recombination across the alternating purine-pyrimidine repeats. We have found that upon transfection of test DNAs into simian cells, a poly[d(pCpG).d(pCpG)] repeat enhanced homologous recombination 10- to 15-fold, whereas a poly[d(pGpT).d(pApC)] repeat had less effect. These results are discussed in terms of the features of these repeats that might be responsible for promoting homologous recombination.     

Helix coil transitions of d (A)n·d(T)n,d(A-T)n·d(A-T)n,and d(A-A-T)n·d(A-T-T)n; evaluation of parameters governing DNA stability

The thermally induced helix-coil transitions of three A-T DNAs, d(A)_n·d(T)_n, d(A-T)_n·d(A-T)_n, and d(A-A-T)_n·d(A-T-T)_n, were studied. Experimental transition curves of the DNAs were analyzed using the loop entropy model of DNA melting. The calculation of the melting curve of d(A-A-T)_n·d(A-T-T)_n is presented using the integral equation formalism of Goel and Montroll. The aim of this work was to evaluate thermodynamic parameters which govern DNA stability and to test the theoretical model employed in the analysis. Our results show (1) an excellent over-all agreement between theory and experiment, (2) a loop entropy exponent k = 1.55 ± 0.05 provided the best fit to all the polymer transition curves, (3) the evaluated stacking free energies reflect the relative stability of the DNAs, and (4) the stacking energies of the ApA·TpT dimer evaluated from d(A)_n·d(T)_n and d(A-A-T)_n·d(A-T-T)_n differ. The last result is consistent with different conformations for the dimer in these two polymers.     

A novel Z-structure for poly d(GC).poly d(GC)

A novel zig-zag (Z) structure is proposed for poly d(GC).poly d(GC). The proposed model closely resembles the crystal structure of d(CG)₃.     

Actinomycin D binds strongly to d(CGACGACG) and d(CGTCGTCG)

Earlier calorimetric studies had indicated that despite the absence of a GpC sequence, the self-complementary octamer d(CGTCGACG) binds strongly to actinomycin D (ACTD) with high cooperativity and a 2:1 drug/duplex ratio. A subsequent optical spectral study with related oligomers led us to suggest that ACTD may likely stack at the G. C basepairs of the duplex termini. New findings are reported herein to indicate that despite the lack of complete self-complementarity, oligomers of d(CGXCGXCG) [X = A or T] motif exhibit unusually strong ACTD affinities with binding constants of roughly 2 x 10(7) M(-1) and binding densities of 1 drug molecule per strand. The ACTD binding affinity for the corresponding heteroduplex obtained by annealing these two oligomers is, however, considerably reduced. Although spectroscopic results with related oligomers obtained by removing, replacing, or appending bases at the termini appear to be consistent with the end-stacking model, capillary electrophoretic (CE) evidence provides additional insights into the binding mode. CE experiments with the self-complementary oligomers d(CGAGCTCG) and d(CGTCGACG) revealed contrasting migration patterns in the presence of ACTD, with mobility retardation and acceleration exhibited by the GpC- and non-GpC-containing octamers, respectively, whereas the X/X-mismatched d(CGXCGXCG) experienced retardation. These results, along with those of related oligomers, suggest that ACTD may in fact stack at the duplex stem end of a monomeric hairpin or at the 3'-end of dG as a single strand. The seemingly cooperative ACTD binding and the curved Scatchard plot for the self-complementary d(CGTCGACG) may thus be attributed to the drug-induced duplex denaturation resulting from strong binding to single strands of d(CGXCGYCG) motif. Detailed structural information on the ACTD-DNA complexes, however, must await further NMR investigations.     

Selection for thermodynamically stable DNA tetraloops using temperature gradient gel electrophoresis reveals four motifs: d(cGNNAg), d(cGNABg),d(cCNNGg), and d(gCNNGc)

Hairpins play important roles in the function of DNA, forming cruciforms and affecting processes such as replication and recombination. Temperature gradient gel electrophoresis (TGGE) and in vitro selection have been used to isolate thermodynamically stable DNA hairpins from a six-nucleotide random library. The TGGE-selection process was optimized such that known stable DNA tetraloops were recovered, and the selection appears to be exhaustive. In the selection, four families of exceptionally stable DNA loops were identified: d(cGNNAg), d(cGNABg), d(cCNNGg), and d(gCNNGc). (Lowercase denotes the closing base pair; N = A, C, G, or T; and B = C, G, or T.) It appears that the known stable d(cGNAg) triloop motif can be embedded into a tetraloop, with the extra nucleotide inserted into either the middle of the loop, d(cGNNAg), or at the 3'-end of the loop, d(cGNABg). For d(cGNNAg) and d(cGNABg), a CG closing base pair was strongly preferred over a GC, with DeltaDeltaG degrees (37) approximately 2 kcal/mol. Members of the two families, d(cCNNGg) and d(gCNNGc), are similar in stability. The loop sequences and closing base pairs identified for exceptionally stable DNA tetraloops show many similarities to those known for exceptionally stable RNA tetraloops. These data provide an expanded set of thermodynamic rules for the formation of tetraloops in DNA.     

Hydration of [d(CGC)r(aaa)d(TTTGCG)](2)

We have studied the hydration and dynamics of RNA C2'-OH in a DNA. RNA hybrid chimeric duplex [d(CGC)r(aaa)d(TTTGCG)](2). Long-lived water molecules with correlation time tau(c) larger than 0.3 ns were found close to the RNA adenine H2 and H1' protons in the hybrid segment. A possible long-lived water molecule was also detected close to the methyl group of 7T in the RNA-DNA junction but not to the other two thymine bases (8T and 9T). This result correlates with the structural studies that only DNA residue 7T in the RNA-DNA junction adopts an O4'-endo sugar conformation (intermediate between B-form and A-form), while the other DNA residues including 3C in the DNA-RNA junction, adopt C1'-exo or C2'-endo conformations (in the B-form domain). Based on the NOE cross-peak patterns, we have found that RNA C2'-OH tends to orient toward the O3' direction, forming a possible hydrogen bond with the 3'-phosphate group. The exchange rates for RNA C2'-OH were found to be around 5-20 s(-1), compared to 26.7(+/-13.8) s(-1) reported previously for the other DNA.RNA hybrid duplex. This slow exchange rate may be due to the narrow minor groove width of [d(CGC)r(aaa)d(TTTGCG)](2), which may trap the water molecules and restrict the dynamic motion of hydroxyl protons. The distinct hydration patterns of the RNA adenine H2 and H1' protons and the DNA 7T methyl group in the hybrid segment, as well as the orientation and dynamics of the RNA C2'-OH protons, may provide a molecular basis for further understanding the structure and recognition of DNA.RNA hybrid and chimeric duplexes.     

Conformations in crystals and solutions of d(CACGTG), d(CCGCGG) and d(GGCGCC) studied by vibrational spectroscopy.

Crystals of self complementary DNA hexamers d(CACGTG), d(CCGCGG) and d(GGCGCC) were grown by vapour diffusion technique and studied by microRaman and microIR spectroscopies. The oligonucleotides were studied in parallel in solution by vibrational spectroscopy. A B- greater than Z transition was detected by Raman spectroscopy during the crystallization process for d(CACGTG). Vibrational spectroscopy shows that the d(GGCGCC) crystals adopt a B geometry. On the contrary the d(CCGCGG) sequence which is shown to be able to undergo in solution or in films quite easily the B- greater than Z transition, remains trapped in crystals in a geometry which may correspond to an intermediate conformation often proposed in models of the B- greater than Z transition. The crystals used in this study were characterized by X-ray diffraction. The unit cell and space group have been determined.     

Energetics of the B-H transition in supercoiled DNA carrying d(CT)x.d(AG)x and d(C)n.d(G)n inserts.

We have studied the B-H transition in the d(AG)x inserts of varying length under superhelical stress. The new data and previously published results for the d(G)31 insert are treated within a phenomenological model of the B-H transition, making it possible to obtain, for the first time, the energy parameters of the B-H transition in the d(AG)x and d(G)n sequences.     

Structure of the beta-form of poly d(A).poly d(U)

The crystalline beta-form of the sodium salt of poly d(A).poly d(U) trapped in oriented fibers forms a Watson-Crick base-paired, 10(1) double-helix of pitch 3.2 nm. Two molecules are present in a monoclinic unit cell apparently isomorphous with beta-poly d(A).poly d(T). The two chains in each molecule both carry C2'-endo puckered furanose rings but are conformationally not identical. The orientations of the A:U base-pairs relative to the helix-axis are distinctly different from those in classical B-DNA and the overall morphology of the duplex in which they reside resembles that of the alpha-forms of poly (purine).poly (pyrimidine) DNA duplexes previously reported.     

Base tilt of poly[d(A)]-poly[d(T)] and poly[d(AT)]-poly[d(AT)] in solution determined by linear dichroism

We have measured the CD, isotropic absorption, and LD of poly[d(A)]–poly[d(T)] and poly[d(AT)]–poly[d(AT)] in the vacuum-uv spectral region. The reduced dichroism (LD divided by isotropic absorption) varied as a function of wavelength and was independent of shear gradient. Thus, the bases are not perpendicular to the helix axis in solution. Since the directions of the transition dipoles are known, the orientations of the bases in the polymers can be calculated from the reduced dichroism spectra. The results show that the base normals are tilted at angles greater than 25°, with respect to the helix axis, and thymine is tilted more than adenine for both polymers. The tilt axes of adenine and thymine are not parallel, indicating a large propeller twist. Space-filling models of poly[d(A)]–poly[d(T)] and poly[(AT)]–poly[d(AT)] are built based on our results, and the conformations of the two (A + T) polymers in solution are discussed.     

Enhanced stabilization of the triplexes d(C(+)-T)(6):d(A-G)(6);d(C-T)(6), d(T)(21):d(A)(21);d(T)(21) and poly r(U:AU) by water structure-making solutes

A variety of organic cations, cationic lipids, low molecular weight alcohols, sodium dodecylsulfate, trehalose, glycerol, low molecular weight polyethylene glycols, and DMSO were tested for their ability to modulate the stability of the triplexes d(C(+)-T)(6):d(A-G)(6);d(C-T)(6), d(T)(21):d(A)(21);d(T)(21), poly r(U:A U) and their respective core duplexes, d(A-G)(6);d(C-T)(6), d(A)(21);d(T)(21), poly r(A-U). Very substantial enhancement of triplex stability over that in a physiological salt buffer at pH 7 is obtained with different combinations of triplex and high concentrations of these additives, e.g. trimethylammonium chloride and d(C(+)-T)(6):d(A-G)(6);d(C-T)(6); 2-propanol and d(T)(21):d(A)(21);d(T)(21); ethanol and poly r(U:A;U). Triplex formation is even observed with a 1:1 strand mixture of d(A-G)(6) and d(C-T)(6) in the presence of dimethylammonium, tetramethylammonium, and tetraethylammonium-chloride, as well as methanol, ethanol, and 2-propanol. Triplex stability follows the water structure-making ability (and in some cases the duplex unwinding ability) of the organic cations, the low molecular weight alcohols and other neutral organic compounds, whereas water structure-breaking additives decrease triplex stability. These findings are consistent with those reported in the accompanying paper that triplex formation occurs with a net uptake of water. Since the findings suggest that third strand-binding is facilitated by unwinding of the target duplex, it is inferred that triplex formation may be enhanced by nucleic acid binding proteins operating similarly.     

Psi compaction of poly[d(AT)].poly[d(AT)]

The compaction of poly[d(A–T)] · poly[d(A–T)] by Co(III) is accompanied by the formation of ψ(+)- and ψ(-)-structures. The chirality of the ψ-structure depends on the Co(III) concentration, ionic strength, temperature, pH, and the chain length of the polymer. The two forms can be readily interconverted by manipulating these factors. Phase diagrams have been constructed that demonstrate the regions of stability of the enantiomers as a function of two variables, while other factors are held constant. At critical points in the phase diagram the two forms are in such unstable equilibrium that mechanical motion will cause ψ(+) ? ψ(-) interconversion. The formation of both ψ(+)- and ψ(-)-structures by the action of Co(III) on poly[d(A–T)] · poly[d(A–T)] contrasts markedly with the behavior of poly[d(G–C)] · poly[d(G–C)] in similar circumstances by forming only the ψ(+)-structure and that of native DNA to produce no ψ at all. Thus the base sequence is important in determining the structure of chirally associated DNA molecules.     

Electronic structure of DNA by DV-X alpha cluster calculations. I. d(GG).d(CC), d(CG)2, d(GC)2 A and B conformations

The electronic structure of d(GG).d(CC), d(CG)2, d(GC)2 which are stacked base pairs in the DNA double helix, are elucidated for both A and B conformations in detail by DV-X alpha cluster calculations. These three DNA double helix fragments are constructed from the same bases, G and C, but the electronic structure of the fragments for A and B conformations differs from each other characteristically. In particular, the electronic states of the O2 and O3 in phosphates differ drastically from each other, and might play a crucial role as recognition sites in various reaction processes concerning DNA. These differences are caused by the delicate differences in the admixture of the orbital components and the intra- and inter-bases interactions. Contour maps of the wavefunction of the HOMO and LUMO are compared among the stacking isomers.