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Multivalent ions are necessary for poly[d(AC).d(GT)] to assume the Z form: a CD study.

In previous work, it was shown that poly[d(AC).d(GT)] could be forced into the Z form by strong dehydrating conditions, provided EDTA was not present. Presumably multivalent impurities were also necessary for the transition. In order to gain control over the B to Z transition for this DNA, we carefully removed all divalent contaminants from the sample and asked the obvious question: What ions are necessary for the transition under dehydrating conditions? We systemically investigated the effect of various multivalent ions. The common contaminants Ca2+, Mg2+, and Fe3+ will not cause the transition, but Co2+ and Ni2+ facilitate the transition, undoubtedly because of their well-known propensity to bind to purine N7. Since the transition also depends on the synergistic dehydrating action of sodium perchlorate and ethanol, we include CD spectra for the independent variations of these two factors. In addition, vacuum-uv CD spectra for the A form and various B forms of poly[d(AC).d(GT)] are presented for the first time.

Circular Dichroism↗

A molecular dynamics study of conformational changes and hydration of left-handed d(CGCGCGCGCGCG)2 in a nonsalt solution.

Twelve dinucleotides (one complete turn) of left-handed, flexible, double-helix poly(dG-dC) Z-DNA have been simulated in aqueous solution with K+ counterions for 70 ps. Most of the d(GpC) phosphates have rotated in accordance with a ZI----ZII transition. The ZII conformation was probably partly stabilized by counterions, which coordinate one of the anionic oxygens and the guanine-N7 of the next (5'----3' direction) base. The presence of base-coordinating ions close to the helical axis rotated and pulled about half of the d(CpG) phosphates further into the groove. These ions also gave rise to rather large deviations from the crystal structure (ZI) with their tendency of pulling the bases closer toward the helical axis. A flipping of the orientation about the glycosyl bond from the +sc to the -sc region was observed for one guanosine, also leading to deviations from the crystal structure. Many bridges containing one or two water molecules were found, with a dominance for the latter. They essentially formed a network of intra- and interstrand bridges between anionic and esterified phosphate oxygens. A "spine" of water molecules could be distinguished as a dark zig-zag pattern in the water density map. The lifetime of a bridge containing one water was about twice as long as that of a two-water bridge and it lasted 5-15 times longer than a hydrogen bond in water. The lifetimes were also calculated for a selection of bridge types, in order of decreasing stability: O1P/O2P ... W ... O'4 much greater than O1P/O2P ... W ... guanine-N2 greater than O1P/O2P ... W ... O1P/O2P. The reorientational motion of water molecules in the first hydration shell around selected groups was slowed down considerably compared to bulk water and the decreasing order of correlation times was guanine-N2 greater than O'4 greater than O'3/O'5 greater than O1P/O2P.

Base Sequence↗

How many numbers are required to specify sequence-dependent properties of polynucleotides?

There are 10 unique dinucleotides of double-stranded DNA, but only 8 independent nearest-neighbor energies that occur in circular DNA, as shown by D. M. Gray and I. Tinoco [(1970) Biopolymers 9, 223-244]. We extend that analysis to include end effects, and show that the number of unique dinucleotide pairs (including ends) is 14, but there are only 12 independent energies. We discuss how these 12 energies (or spectra or any other pairwise additive property) can be measured and displayed, and how they should and should not be compared between experimenters. As an example, we analyzed the recently reported melting curves [M.J. Doktycz et al. (1992) Biopolymers, 32, 849-864.] of 16 DNA dumbbells in two different Na+ environments. This analysis reveals a new means for evaluating end effects and the emergence of longer than nearest-neighbor interactions at low salt concentration.

Base Composition↗

Linear dichroism demonstrates that the bases in poly[d(AC)].poly[d (GT)] and poly[d(AG)].poly[d(CT)] are inclined from perpendicular to the helix axis.

Flow linear dichroism is used to measure specific inclinations for each of the four bases in poly[d(AC)].poly[d(GT)] and poly[d(AG)].poly[d(CT)] in both the B and A forms. For the B form in solution the bases are found to have a sizable inclination. Inclination is increased in the A form, as expected. In all cases the pyrimidines are more inclined than the purines.

Adenine↗

Persistence analysis of the static and dynamical helix deformations of DNA oligonucleotides: application to the crystal structure and molecular dynamics simulation of d(CGCGAATTCGCG)2.

A theory and graphical presentation for the analysis of helix structure and deformations in oligonucleotides is presented. The parameters "persistence" and "flexibility" as defined in the configurational statistics of polymers of infinite length are reformulated at the oligonucleotide level in an extension of J. A. Schellman's method [(1974) Biopolymers, Vol. 17, pp. 217-226], and used as a basis for a systematic "Persistence Analysis" of the helix deformation properties for all possible subsequences in the structure. The basis for the analysis is a set of link vectors referenced to individual base pairs, and is limited to sequences exhibiting only perturbed rod-like behavior, i.e., below the threshold for supercoiling. The present application of the method is concerned with a physical model for the angular component of bending, so the link vectors are defined as the unit components of a global helix axis obtained by the procedure "Curves" of R. Lavery and H. Sklenar [(1988) J. Biomol. Struct. Dynam., Vol. 6, pp. 63-91; (1989) ibid., Vol. 6, pp. 655-667]. A discussion of the relationship between global bending and relative orientation of base pairs is provided. Our approach is illustrated by analysis of some model oligonucleotide structures with intrinsic kinks, the crystal structure of the dodecamer d(CGCGAATTCGCG)2, and the results of two molecular dynamics simulations on this dodecamer using two variations of the GROMOS force field. The results indicate that essentially all aspects of curvature in short oligonucleotides can be determined, such as the position and orientation of each bend, the sharpness or smoothness, and the location and linearity of subsequences. In the case of molecular dynamics simulations, where a Boltzmann ensemble of structures is analyzed, the spatial extent of the deformations (flexibility) is also considered.

Base Sequence↗

Molecular dynamics simulations of B-DNA: an analysis of the role of initial molecular configuration, randomly assigned velocity distribution, long integration times, and nonconstrained termini.

Molecular dynamics simulations of three DNA sequences using the AMBER 3.0 force field were performed with implicit inclusion of water through a distance-dependent dielectric constant and solvated counterions. Simulations of the self-complementary DNA dodecamer d(CGCGAATTCGCG) were started from a regular B-DNA structure and the x-ray single crystal B-DNA structure. Although mean convergence during the 89-ps calculation was confirmed, localized differences in backbone torsionals and base-pair helicoidals were observed. A nanosecond simulation of the nonself-complementary 14 base-pair DNA d(GGCGGAATTGGCGG) indicates that most structural parameters stabilize within the first 100-200 ps, while isolated features show low-frequency oscillations throughout the calculation. The lack of harmonic constraints on the ends of the molecules was shown not to perturb the structural dynamics of the internal oligonucleotide beyond the external 2 base pairs. Comparison of three simulations of the nonself-complementary 14 base-pair DNA d(GGCGAAATTCGCGG), identical in all respects other than the assignment of initial Maxwellian atomic velocity distributions, revealed the inherent systematic variability. The three calculations result in nearly superimposable global structures, with localized variations in torsionals and helicoidals. Our results provide a basis for performing a comparative analysis of the effect of DNA sequence on localized structure.

Base Sequence↗

Z-->B transition in poly[d(G-m5C)2] induced by interaction with 4',6-diamidino-2-phenylindole.

The Z form of poly[d(G-m5C)2], in presence of Mg2+ ion, is found to be transformed into B form upon interaction with 4',6-diamidino-2-phenylindole (DAPI). The Z-->B transformation is complete at a mixing ratio of about 0.07 DAPI per DNA base pairs, i.e., each DAPI molecule may be related to the conversion of 6-7 base pairs. An interaction between DAPI and poly[d(G-m5C)2] in its Z form at low drug: DNA ratios is suggested from optical dichroism and time-resolved luminescence anisotropy results. The spectroscopic behaviour of DAPI indicates that the Z conformation of DNA does not provide normal binding sites for DAPI, such as groove or intercalation sites, but that the initial association may be of external nature.

Chemical Phenomena↗

Spatial translational motions of base pairs in DNA molecules: application of the extended matrix generator method.

We have used the elementary generator matrices outlined in the preceding paper to examine the conformational plasticity of the nucleic acid double helix. Here we investigate kinked DNA structures made up of alternating B- and A-type helices and intrinsically curved duplexes perturbed by the intercalation of ligands. We model the B-to-A transition by the lateral translation of adjacent base pairs, and the intercalation of ligands by the vertical displacement of neighboring residues. We report a complete set of average configuration-dependent parameters, ranging from scalars (i.e., persistence lengths) to first- and second-order tensor parameters (i.e., average second moments of inertia), as well as approximations of the associated spatial distributions of the DNA and their angular correlations. The average structures of short chains (of lengths less than 100 base pairs) with local kinks or intrinsically curved sequences are essentially rigid rods. At the smallest chain lengths (10 base pairs), the kinked and curved chains exhibit similar average properties, although they are structurally perturbed compared to the standard B-DNA duplex. In contrast, at lengths of 200 base pairs, the curved and kinked chains are more compact on average and are located in a different space from the standard B- or A-DNA helix. While A-DNA is shorter and thicker than B-DNA in x-ray models, the long flexible A-DNA helix is thinner and more extended on average than its B-DNA counterpart because of more limited fluctuations in local structure. Curved polymers of 50 base pairs or longer also show significantly greater asymmetry than other DNAs (in terms of the distribution of base pairs with respect to the center of gravity of the chain). The intercalation of drugs in the curved DNA straightens and extends the smoothly deformed template. The dimensions of the average ellipsoidal boundaries defining the configurations of the intercalated polymers are roughly double those of the intrinsically curved chain. The altered proportions and orientations of these density functions reflect the changing shape and flexibility of the double helix. The calculations shed new light on the possible structural role of short A-DNA fragments in long B-type duplexes and also offer a model for understanding how GC-specific intercalative ligands can straighten naturally curved DNA. The mechanism is not immediately obvious from current models of DNA curvature, which attribute the bending of the chain to a perturbed structure in repeating tracts of A.T base pairs.

Base Sequence↗

DNA binding of a spermine derivative: spectroscopic study of anthracene-9-carbonyl-N1-spermine with poly[d(G-C).(d(G-C)] and poly[d(A-T).d(A-T)].

The binding of polyamines, including spermidine (1) and spermine (2), to poly[d(G-C).d(G-C)] was probed using spectroscopic studies of anthracene-9-carbonyl-N1-spermine (3); data from normal absorption, linear dichroism (LD), and circular dichroism (CD) are reported. Ligand LD and CD for transitions located in the DNA region of the spectrum were used. The data show that 3 binds to DNA in a manner characteristic of both its amine and polycyclic aromatic parts. With poly[(dG-dC).(dG-dC)], binding modes are occupied sequentially and different modes correspond to different structural perturbations of the DNA. The most stable binding mode for 3 with poly[d(G-C).d(G-C)] has a site size of 6 +/- 1 bases, and an equilibrium binding constant of (2.2 +/- 1.1) x 10(7) M-1 with the anthracene moiety intercalated. It dominates the spectra from mixing ratios of approximately 133:1 until 6:1 DNA phosphate: 3 is reached. The analogous data for poly[d(A-T).d(A-T)] between mixing ratios 36:1 and 7:1 indicates a site size of 8.3 +/- 1.1 bases and an equilibrium binding constant of (6.6 +/- 3.3) x 10(5) M-1. Thus, 3 binds preferentially to poly[d(G-C).d(G-C)] at these concentrations.

Circular Dichroism↗

Structural modification of DNA by a DNA-binding motif SPKK: detection of changes in base-pair hydrogen bonding and base stacking by UV resonance Raman spectroscopy.

Interactions of a DNA-binding motif SPKK with polynucleotides have been investigated by uv resonance Raman spectroscopy. Analysis of the Raman spectra has shown that the tetrapeptide SPKK weakens the adenine-thymine base-pair hydrogen bonding in poly(dA-dT).poly(dA-dT) and reduces the adenine-adenine base stacking interactions in poly(dA).poly(dT), both effects being indicative of destabilization of the DNA double helical structure. On the other hand, poly(dG-dC).poly(dG-dC) and poly(dG).poly(dC) do not show any structural change in the presence of SPKK. The present observations confirm that the SPKK motif, which is frequently found in histone H1 proteins, specifically binds to A/T-rich regions of DNA and loosens the DNA double-helical structure. One of the roles of the SPKK motifs in histones may be to increase DNA flexibility so that DNA can wrap around core histones and be assembled into chromosomes more easily.

Amino Acid Sequence↗

Pressure dependence of the helix-coil transition temperature of poly[d(G-C)].

The pressure dependence of the helix-coil transition temperature (Tm) of poly[d(G-C)] was studied as a function of sodium ion concentration in phosphate buffer. The molar volume change of the transition (delta V) was calculated using the Clapeyron equation and calorimetrically determined enthalpies. The delta V of the transition increased from +4.80 (+/- 0.56) to +6.03 (+/- 0.76) mL mol-1 as the sodium ion concentration changed from 0.052 to 1.0M. The van't Hoff enthalpy of the transition calculated from the half-width of the differentiated transition displayed negligible pressure dependence; however, the value of this parameter decreased with increasing sodium ion concentration, indicating a decrease in the size of the cooperative unit. The volume change of the transition exhibits the largest magnitude of any double-stranded DNA polymer measured using this technique. For poly[d(G-C)] the magnitude of the change in delta V with sodium ion concentration (0.94 +/- 0.05 mL mol-1) is approximately one-half that observed for either poly[d(A-T)] or poly(dA).poly(dT). The delta V values are interpreted as arising from changes in the hydration of the polymer due to the release of counterions and changes in the stacking of the bases of the coil form. As a consequence of solvent electrostriction, the release of counterions makes a net negative contribution to the total delta V, implying that disruption of the stacking interactions contributes a positive volume change to the total delta V.(ABSTRACT TRUNCATED AT 250 WORDS)

Hydrostatic Pressure↗

Sequence and temperature dependence of the interbase hydrogen-bond breathing modes in B-DNA polymers: comparison with low-frequency Raman peaks and their role in helix melting.

We carry out temperature-dependent lattice dynamics calculations to determine the vibrational normal modes associated with the interbase H-bond breathing motion in several B-DNA copolymers at temperatures from room temperature to the melting temperatures. We take into consideration Raman selection rules and incorporate a simple empirical model of Raman susceptibility in the interbase H bonds in our calculation and compare them to Raman measurements. Our calculations are carried out using empirical force constants that are not further refined to low-frequency spectra. Our calculations show the existence of strong interbase H-bond breathing modes at frequencies and with relative oscillator strengths close to the observed Raman peaks in the range of 60-140 cm-1 for the DNA sequences considered except for one helix. The correlation between the calculated and observed frequencies and oscillator strengths indicates that the observed Raman peaks in the frequency range are likely interbase H-bond breathing modes. We find that these modes exhibit sizable temperature as well as sequence dependence. We show the softening of these modes on approaching thermal denaturation that is also in agreement with the observed behavior in Raman and melting measurements. The sensitivity of the calculation on the empirical model of Raman susceptibility and the possible reasons for the discrepancy between a few calculated values and observations are discussed.

Animals↗

Normal mode calculation of a netropsin-DNA complex: effect of structural deformation on vibrational spectrum.

Calculations of the normal mode spectrum of a netropsin-DNA complex, an isolated DNA helix of the same sequence, and a free netropsin molecule were carried out and compared with observations. We find that the frequency of modes of the complex that are primarily vibrations localized to the helix are relatively unchanged from the frequencies found for similar modes of the isolated helix. On the other hand, the frequencies of thosemodes of the complex that are found to be primarily in the netropsin are found to change significantly in the complex from that of the free netropsin. Further analysis indicates that the changes in the "netropsin modes" are primarily due to the conformational deformation induced in the netropsin by formation of the complex. All the frequencies and shifts in frequency are in good agreement with recent Raman measurements.

Base Composition↗

Characterization of the binding of YO to [poly(dA-dT)]2 and [poly(dG-dC)]2, and of the fluorescent properties of YO and YOYO complexed with the polynucleotides and double-stranded DNA.

The interaction between the fluorescent dye YO (oxazole yellow) and the alternating polynucleotides [poly(dA-dT)]2 [the duplex of alternating poly(dA-dT)] and [poly(dG-dC)]2 [the duplex of alternating poly(dG-dC)] has been studied with optical spectroscopic techniques including absorbance, flow linear dichroism, CD, and fluorescence measurements. The principal features of the spectra are very similar for the two polynucleotide solutions, showing that YO binds quite similarly to AT and GC base pairs. From a strongly negative reduced linear dichroism (LDr) in the dye absorption band, an induced negative CD, and transfer of energy from the bases to bound YO, we conclude that at low mixing ratios YO is intercalated in both [poly(dA-dT)]2 and [poly(dG-dC)]2. At higher mixing ratios an external binding mode starts to contribute, evidenced from the appearance of an exciton CD. The conclusion that YO binds in a similar way to AT and GC base pairs should be valid also for the dimer YOYO since its YO units have been found to bind to double-stranded (dsDNA) in the same way as the YO monomer. The fluorescence properties of YO and YOYO complexed with DNA or the polynucleotides have been characterized by studying the dependence of fluorescence intensity on temperature, mixing ratio, and ionic strength. The fluorescence intensity and fluorescence lifetime of YO-DNA decrease strongly with increasing mixing ratio, whereas the fluorescence intensity of YOYO-DNA shows a weaker dependence, indicating that the quantum yield depends on the distance between the YO chromophores on the DNA chain. Further, the fluorescence intensity of YO depends on the base sequence; the quantum yield and fluorescence lifetime for YO complexed with [poly(dG-dC)]2 are about twice as large as for YO complexed with [poly(dA-dT)]2. Measurements of excitation spectra at different mixing ratios and different emission wavelengths indicate that the fluorescence of the externally bound chromophores is negligible compared to the intercalated ones.

Benzoxazoles↗

Comparison of base inclination of ribo-GC and deoxyribo-GC polymers, and synthesis of poly(rGrC)-poly(rGrC).

The inclination angle between the base normal and the helix axis, and the axes around which the bases incline, are measured for ribo-GC polymers in buffer by using flow linear dichroism (LD), and compared to measurements for deoxyribo-GC polymers in buffer and under dehydrating conditions. A new method is designed to synthesize poly(rGrC)-poly(rGrC), which is not available commercially, in large quantities. The LD of this RNA reveals inclination angles that are similar to the B-form DNA in buffer, although the axes are different. The CD of poly(dGdC)-poly(dGdC) under the dehydrating conditions is similar to poly(rGrC)-poly(rGrC), indicating it is in the A form, and the LD gives larger inclination angles than either the B form or the corresponding RNA. Poly(dG)-poly(dC) is in the A form in buffer. Comparison among poly(rG)-poly(rC) in buffer, and poly(dG)-poly(dC) in buffer under dehydrating conditions, reveals similar inclination angles and axes, although the LD shows that the DNA has the largest inclination angles. Except for poly(rGrC)-poly(rGrC), which has a unique reduced dichroism, all the axes for G are similar, as are the axes for C.

Circular Dichroism↗

The protective mechanisms of defibrotide on liver ischaemia-reperfusion injury.

During some surgical interventions, temporary occlusion of the hepatic blood supply may cause ischaemia-reperfusion (I/R) injury and hepatic dysfunction. In this study the protective effect of defibrotide (DEF) was evaluated in a rat model of liver I/R injury. Four groups of rats were subjected to the following protocols: saline infusion without ischaemia, DEF infusion without ischaemia, DEF infusion with hepatic I/R, and saline infusion with hepatic I/R. After a midline laporatomy, liver ischaemia was induced by 45 min of portal occlusion. DEF 175 mg/kg(-1) was infused before ischaemia in 10 ml of saline. The same volume of saline was infused into the control animals. At the end of the 45-min reperfusion interval, the animals were sacrified. Superoxide dismutase (SOD) and glutathione peroxidase (GSH-Px) enzyme activities were determined in haemolysates, and malondialdehyde (MDA) level in the liver tissue was measured. Tissue MDA levels were significantly higher in the I/R plus saline group compared to the sham operation control groups (p < 0.01 and p < 0.05, respectively). Tissue MDA levels decreased in the DEF plus I/R group compared to the I/R plus saline group (p < 0.05), but DEF could not reduce tissue lipid peroxidation to the levels of the control sham operation groups. SOD and GSH-Px enzyme activities were significantly higher in DEF-treated animals than in the other groups (p < 0.05). These results suggest that DEF protects liver against I/R injury by increasing the antioxidant enzyme levels.

Animals↗

Catalytic properties of DNA polymerase alpha activity associated with the heart-stabilized nuclear matrix prepared from HeLa S3 cells.

We have investigated whether or not ATP or other nucleoside di- and trisphosphates (including some nonhydrolysable ATP analogues) can stimulate the activity and/or the processivity of DNA polymerase alpha associated with the nuclear matrix obtained from HeLa S3 cell nuclei that had been stabilized at 37 degrees C prior to subfractionation, as has been reported previously for DNA polymerase alpha bound to the nuclear matrix prepared from 22-h regenerating rat liver. We have found that HeLa cell matrix-associated DNA polymerase alpha activity could not be stimulated at all by ATP or other nucleotides, a behaviour which was shared also by DNA polymerase alpha activity that solubilizes from cells during the isolation of nuclei and that is thought to be a form of the enzyme not actively engaged in DNA replication. Moreover, the processivity of matrix-bound DNA polymerase alpha activity was low (< 10 nucleotides). These results were obtained with the matrix prepared with either 2 M NaCl or 0.25 M (NH4)2SO4 and led us to consider that a 37 degree incubation of isolated nuclei renders resistant to high-salt extraction a form of DNA polymerase alpha which is unlikely to be involved in DNA replication in vivo.

Adenosine Triphosphate↗