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PubMed1989

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.

DNA↗
PubMed1989

Prediction of DNA structure from sequence: a build-up technique.

A build-up technique has been devised that permits prediction of DNA structure from sequence. No experimental information is employed other than the force field parameters. This strategy for dealing with the multiple minimum problem requires a supercomputer to make the necessary global searches. The number of energy minimization trials that were made for each of the 16 deoxydinucleoside monophosphate conformational building blocks of DNA was 1944. As a test case, the minimum energy conformations of d(GpC) and d(CpG) to 5.5 kcal/mole were then combined to generate energy-minimized structures for d(CpGpC). The number of trials that were made for d(CpGpC) was 3752. Minima for this single-stranded trimer to 15 kcal/mole were then employed to search for minimum energy conformations of the duplex d(CpGpC).d(GpCpG). The number of starting conformations that were utilized at this stage was 1514. The lowest energy duplex had a Z-II-DNA conformation, followed by a B-DNA form at 1.2 kcal/mole. The A- and Z-I-forms as well as many novel Watson-Crick base-paired structures were found at higher energy. Finally, energy-minimized structures of d(CG)6.d(CG)6 in Z-II and B-DNA conformations were computed using torsion angles from the analogous duplex trimer minima.

Base Sequence↗
PubMed1989

Vibrational free energy, entropy, and temperature factors of DNA calculated by a helix lattice approach.

The vibrational contribution to the free energy, entropy, and the temperature factors of the different atoms in the unit cell are calculated using the method of helix lattice dynamics for the DNA homopolymer poly(dG.poly(dC) in the B conformation. These results are compared to other theoretical calculations and the temperature (B) factors are compared to experiment as well. The problems encountered in using small molecule approximations to describe B factors in DNA like long chain molecules are discussed and a corrected estimate of the temperature factors are presented. Significant differences are found between the different theoretical approaches as reflected in the results of temperature factor calculations.

Amino Acid Sequence↗
PubMed1990

Structural and electrostatic effects on binding of trivalent cations to double-stranded and single-stranded poly[d (AT)].

We have measured the thermal melting profile for poly[d(AT)].poly[d(TA)] as a function of concentration of three trivalent cations: spermidine, me8spermidine, and hexammine cobalt(III). Using McGhee's (1976) theory of DNA melting in the presence of ligands, we have estimated association constants Kh, Kc and binding site sizes nh, nc for binding to double-helical (h) and single-stranded (c) polynucleotide. The results are as follows: (table; see text) The binding parameters for spermidine and hexammine cobalt(III) to double helical molecules agree fairly well with direct equilibrium dialysis measurements, and are in reasonable accord with predictions of counterion condensation theory. However, despite their identical charges, the three ligands bind to single-stranded DNA with quite different affinities. Estimates of the charge spacing of single-stranded DNA suggest that poly[d(AT)] is less elongated in the presence of spermidine and hexammine cobalt(III) than it is when complexed with me8spermidine.

Binding Sites↗
PubMedDate not supplied

Delta V0 of the Na(+)-induced B-Z transition of poly[d(G-C)] is positive.

The equilibrium between the right- and left-handed conformations of poly[d(G-C)] in aqueous NaCl shifts towards the right-handed (B) form with increasing pressure. The optical density at 290 and 260 nm was determined at 50 and 180 MPa for solutions in which approximately equal amounts of the two conformations were present at 0.1 MPa (atmospheric pressure). Interpretation of the observed changes in terms of a two-state unimolecular reaction mechanism results in an average molar reaction volume (delta V0) equal to 26 cm3 mol-1 at 22 degrees C; that is, the partial molar volume of B form poly[d(G-C)] is smaller than that of the left-handed (Z) form. Based upon the thermodynamics of ion-pair formation in polar solvents, it is proposed that the positive delta V0 reflects a favorable entropy change for the reaction toward the Z conformation. The larger entropy change of the Z form may derive from the release of water molecules from the hydration spheres of the cation and the poly[d(G-C)] due to the formation of ionic interactions with the Z conformer. The delta V0 of the transition is similar in sign and magnitude to the calculated molar volume change of the interaction of Na+ with H2PO4- in water.

Nucleic Acid Conformation↗
PubMedDate not supplied

Excimer fluorescence of (+)-anti-benzo (a)pyrene diol epoxide covalently bound to poly(dG-dC): structural implications.

Fluorescence of (+)-anti-benzo(a)pyrene diol epoxide [(+)-anti-BPDE] covalently bound to poly(dG-dC) has been studied with steady-state and time-resolved techniques. Extensive formation of excimers is found, even at small (0.008) BPDE/nucleotide ratios. This indicates favored covalent binding to bases close to already modified guanines. Both fluorescence excitation spectra and lifetime measurements reveal two populations of (+)-anti-BPDE adducts: one that can form excimers and one that cannot. Three excimer lifetimes (4.5, 29, and 83 ns) are observed. Differently shifted monomer and excimer excitation spectra are discussed in terms of pyrene-pyrene exciton interactions, consistent with a distance shorter than 7 A between the excimer-forming BPDE chromophores.

7,8-Dihydro-7,8-dihydroxybenzo(a)pyrene 9,10-oxide↗
PubMed1990

Anomalously slow electrophoretic mobilities of DNA restriction fragments in polyacrylamide gels are not eliminated by increasing the gel pore size.

The effect of gel pore size on the anomalous mobility of certain curved DNA restriction fragments in polyacrylamide gels was studied by comparing the electrophoretic mobilities of normal and anomalous fragments in gels of varying composition but constant acrylamide concentration. Molecular weight ladders were prepared from two 147 base pair G-C rich restriction fragments, called 12A (anomalous) and 12B (normal), obtained from the MspI digestion of plasmid pBR322. The electrophoretic mobilities of multimers of the two fragments increasingly diverged with increasing molecular weight. The anomalous mobility of fragment 12A was essentially independent of gel pore size, regardless of whether the pore size was varied by increasing the acrylamide concentration at constant cross-linker concentration or by increasing the cross-linker concentration at constant acrylamide concentration. The anomalous mobility of higher multimers of fragment 12A decreased with increasing gel pore size when the pore size was varied by changing the gel concentration. However, when the gel pore size was changed by varying the cross-linker concentration at constant acrylamide concentration, the anomalous mobility of higher multimers of fragment 12A went through a maximum and then decreased as the pore size was increased. Copolymerizing acrylamide with high molecular weight linear polyacrylamides had no effect on the anomalous mobility of the 12A multimer ladder, even though the apparent absolute mobilities of all fragments increased markedly. Only by incorporating charged residues into the gel matrix or by copolymerizing acrylamide with the intercalator ethidium bromide could the difference in mobility between the 12A and 12B multimer ladders be substantially reduced or eliminated. Similar results were observed with a molecular weight ladder containing 78 base pair repeats of the bending locus of kinetoplast DNA. These results suggest that pore size alone is not responsible for the anomalously slow migration of curved DNA molecules in polyacrylamide gels.

Base Sequence↗
PubMed1990

Dielectric study on hydration of B-, A-, and Z-DNA.

Dielectric relaxation peak due to bound water was found around 100 MHz in poly(dG-dC).poly(dG-dC) and calf thymus DNA in water-ethanol mixtures with NaCl buffer. Relaxation time and strength show a transition for poly(dG-dC).poly(dG-dC) at an ethanol composition Cw = 0.45 (w/w) where the structural transition from B- to Z-DNA takes place. It has been suggested that the transition is caused by removal of the bound water molecules preferentially from the phosphate groups. If the bound water molecules are removed equally from the phosphate groups and the grooves, the structural transition from B to A takes place. By analogy with hydration of tropocollagen, it was found that 19 water molecules per one nucleotide are at least necessary to keep B-DNA. Thirteen molecules are bound to A-DNA and 9 molecules to Z-DNA. Stringlike multimers are proposed as available structures of the bound water.

Animals↗
PubMed1991

Zinc ion-DNA polymer interactions.

The adjacent GN7-M-GN7 cross-linking and adjacent G-M-G sandwich-complex models for DNA metal ion binding were evaluated both with native DNAs differing in GC content as well as with the synthetic polymers poly [(dGdC)]2, poly[(dAdT)]2, and poly[(dAdC)(dGdT)]. The effect of Zn2+ was studied in depth, and limited studies were also performed with Co2+ and Mg2+. The results were compared to the extensive information available on Cu2+ binding to native DNAs and poly[(dAdT)]2. At high ratios of metal/base (R), Zn2+ caused all native DNAs to denature with the same melting temperature Tm, approximately 61 degrees C. A similar pattern was reported previously for Cu2+, but the typical Tm was approximately 35 degrees C. The extent of renaturation on cooling DNAs denatured in the presence of Zn2+ increased with GC content, as reported previously for Cu2+. These results, together with previously reported similarities, strongly indicate that the DNA binding characteristics of the two cations are similar. By comparison of the Tm values and hyperchromicity changes monitored at 260 and 282 nm, it is clear that, during thermal denaturation in the presence of Zn2+, both AT and GC regions were denatured, even at high R. The Tm vs R profile for the native DNAs was typical. The rise at low R and subsequent decrease at high R were inversely and directly related, respectively, to GC content. Except for poly[(dAdT)]2, where Tm increased with R, the other synthetic polymers exhibited the increase/decrease pattern. Poly[(dAdC)(dGdT)] gave a Tm value at high R of 54 degrees C. In the absence of Zn2+, this polymer exhibited little hypochromicity on cooling of denatured polymer. However, in the presence of Zn2+, nearly complete hypochromicity was observed, although the midpoint of the cooling curve was lower than the Tm value by approximately 15 degrees C at R = 10. These characteristics were similar to those with native DNAs, although viscosity and CD studies suggested that the "renatured" polymer was not identical to the unheated polymer. Furthermore, addition of Zn2+ after denaturation nearly completely reversed the absorption increase. This finding contrasts with those for native DNAs, where the Zn2+ must be present during denaturation in order to reverse the absorption increase nearly completely on cooling. With some caveats, poly[(dAdC)(dGdT)] appears to be a good model for native DNAs since its properties, including CD and uv changes on addition of Zn2+ to premelted and melted polymer, parallel those of the native polymers.(ABSTRACT TRUNCATED AT 400 WORDS)

Animals↗
PubMed1991

Effect of basic oligopeptides on the B-Z transition of poly(dG-dC). poly(dG-dC) in water-methanol solutions.

The effect of basic oligopeptides (Lys-Ala-Ala)n (n = 1-5, 10) and (Lys-Leu-Ala)n (n = 1-4) on the B-Z transition of poly(dG-dC).poly(dG-dC) in water-methanol solutions was investigated using CD and uv spectroscopy. In the absence of peptides, the concentration of methanol at the midpoint of the B-Z transition is 64% at 25 degrees C. The transition is temperature dependent and the B conformation is preferred at higher temperatures. All peptides tested shift the midpoint of the B-Z transition to lower concentrations of methanol. For shorter peptides this effect increases with an increasing number of monomeric units, showing the importance of the number of positive charges in the peptide molecule. Al conditions of low methanol content, the trimer and tetramer of the (Lys-Leu-Ala)n series have a greater effect on the B-Z transition than the corresponding oligomers of the (Lys-Ala-Ala)n series. This indicates an important influence of the presence of hydrophobic groups in the peptide side chains on the binding. In the presence of peptides, the B-Z transition is also temperature dependent and the B conformation is preferred at higher temperatures. The addition of peptides results in an increase of the transition midpoint and of the transition width. These parameters were used for the calculation of the transition enthalpy delta HB-Z in 65% methanol, which is -1.15 +/- 0.25 kcal/base pair. Since the van't Hoff enthalpy delta HVH calculated from the temperature dependence of the B-Z transition in the absence of peptides is -130 kcal/mol, the length of the cooperative unit is about 110 base pairs. The results suggest that the mechanism of Z-DNA induction is similar but not identical with that involved in the action of metal cations in aqueous solution.

Amino Acid Sequence↗
PubMed1991

Comparison of the bis-intercalating complexes formed between either ditercalinium or a flexible analogue and d(CpGpCpG)2 or d(TpTpCpGpCpGpApA)2 minihelices: 1H- and 31P-NMR analyses.

The 400-MHz 1H- and 162-MHz 31P-nmr have been used to study complexes constituted by (a) the d(TpTpCpGpCpGpApA)2 or the d(CpGpCpG)2 self-complementary oligonucleotides and (b) two bifunctional 7H-pyrido [4,3-c] carbazole dimer drugs, the antitumoral ditercalinium (NSC 366241), a dimer with a rigid bis-piperidine linking chain and its pharmacologically inactive analogue, a dimer with a flexible spermine-like linking chain. Nearly all proton and phosphorus signals have been assigned by two-dimensional (2D) nmr (correlated spectroscopy, homonuclear Hartmann-Hahn, nuclear Overhauser enhancement spectroscopy, 2D 31P (1H) heteronuclear correlated spectroscopy and 31P-31P chemical exchange experiments). Both drugs bis-intercalate into the two CpG sites. The complexes show small differences in the position of the 7H-pyrido [4,3-c] carbazole ring into the intercalation site and possibly in the ribose-phosphate backbone deformation. However, the inactive analogue exhibits a longer residence lifetime in octanucleotide than the ditercalinium does. All these results are discussed in terms of differences in dimer activities.

Base Sequence↗
PubMed1991

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)

Base Sequence↗
PubMed1991

Distance-dependent dielectric constants and their application to double-helical DNA.

Detailed studies of structures of biological macromolecules, even in simplified models, involve many costly and time-consuming calculations. Any thorough methods require sampling of an extremely large conformation and momentum space. Calculations of electrostatic interactions, which depend on many physical factors, such as the details of solvent, solvent accessibility in macromolecules, and molecular polarizability, are always developed in a compromise between more rigorous, detailed models and the need for immediate application to complicated biological systems. In this paper, a middle ground is taken between the more exact theoretical models and the simplest constant values for the dielectric constant. The effects of solvent, counterions, and molecular polarizability are incorporated through a set of adjustable parameters that should be determined from experimental conditions. Several previous forms for the dielectric function are compared with the new ones. The present methods use Langevin functions to span the region of dielectric constant between bulk solvent and cavity values. Application of such dielectric models to double-helical DNA is important because base-stacking preferences were previously demonstrated [A. Sarai, J. Mazur, R. Nussinov, and R. L. Jernigan (1988) Biochemistry, vol. 27, pp. 8498-8502] to be sensitive to the electrostatic formulation. Here we find that poly(dG).poly(dC) can be A form for high screening and B form for low screening. By contrast, poly(dA).poly(dT) can only take the B form. Base stacking is more sensitive to the form of the dielectric function than are the sugar-phosphate backbone conformations. Also in B form, the backbone conformations are not so affected by the base types as in A form.

Base Sequence↗
PubMed1991

The CD of ligand-DNA systems. I. Poly(dG-dC) B-DNA.

A systematic theoretical study of the CD of double-stranded poly(dG-dC) and its complexes with small molecules is presented. The intrinsic CD of the polymer and the induced CD of a transition belonging to a molecule bound to DNA are calculated using the matrix method. The calculations show considerable differences between pyrimidine-purine and purine-pyrimidine binding sites, and we find that the induced CD of a groove bound molecule is one order of magnitude stronger than that of an intercalated molecule. The results form a sound basis for interpreting the CD of ligand-DNA systems in terms of molecular geometry, interactions, and spectroscopy.

Circular Dichroism↗