Evidence for a novel conformational transition in superhelical DNA

On the assumption that the dependence of the electrophoretic mobility of superhelical DNA upon the number of tertiary turns (Wr) is a monotonously increasing function devoid of points of inflection, it is concluded that the inflection (change of sign of the first derivative) observed on the curve gives evidence for a conformational transition in DNA secondary structure that begins long before the BZ or B cruciform transitions. The transition consumes 60% of the topological turns at native levels of supercoiling. It is proposed that the conformation produced belongs to the A-family. Provided that this transition indeed yields the A form (11 base pairs per turn), the energy of the BA conformational transition is estimatd to be 5.8–10.3 cal per base pair for different nucleotide sequences at physiological ionic strength. The energies of BZ and B cruciform transitions in superhelical DNA estimated from electrophoretic mobilities by the present method coincide perfectly with the values obtained by other authors using other methods. In addition, on the basis of the data of Brady et al. (1983) on the number of tertiary turns in superhelical DNA determined by X-ray scattering, it is concluded that the initial assumption is justified and the ratio of bending to twisting stiffnesses of superhelical DNA is estimated as 71 (in the fully supercoiled molecule containing 50% of the supposed A-conformation).     

Energetics of superhelicity and of B-Z transitions in superhelical DNA

The linking difference, α, imposed upon a superhelically constrained DNA molecule must be partitioned between twisting and bending deformations. Transitions to alternative secondary structures can occur at susceptible sites, altering the local molecular twist by an amount ΔTw _trans. That part of the linking difference not accommodated in this way, the residual linking difference α_res, must be manifested as smooth torsional and flexural deformations of secondary structure. The competition among the alternative ways of accommodating the imposed linking difference α determines a stressed equilibrium state. The superhelical free energy,G(α), is the excess free energy of the equilibrium state at linking difference α above that of the relaxed state under identical conditions. In this paper a method is described by which the free energies associated both to linking,G(α), and to residual linking differences can be determined from data on superhelical conformational transitions. The application of this approach to previously published experimental data on the B-Z transition suggests that the free energy associated with α_res is about 30% larger at substantial superhelicities than it is near the relaxed state. At the onset of transition the functional form ofG(α) is shown to change in a manner dependent upon the length of the Z-susceptible site.     

Energetics of superhelicity and of B-Z transitions in superhelical DNA

The linking difference, alpha, imposed upon a superhelically constrained DNA molecule must be partitioned between twisting and bending deformations. Transitions to alternative secondary structures can occur at susceptible sites, altering the local molecular twist by an amount delta Twtrans. That part of the linking difference not accommodated in this way, the residual linking difference alpha res, must be manifested as smooth torsional and flexural deformations of secondary structure. The competition among the alternative ways of accommodating the imposed linking difference alpha determines a stressed equilibrium state. The superhelical free energy, G(alpha), is the excess free energy of the equilibrium state at linking difference alpha above that of the relaxed state under identical conditions. In this paper a method is described by which the free energies associated both to linking, G(alpha), and to residual linking differences can be determined from data on superhelical conformational transitions. The application of this approach to previously published experimental data on the B-Z transition suggests that the free energy associated with alpha res is about 30% larger at substantial superhelicities than it is near the relaxed state. At the onset of transition the functional form of G(alpha) is shown to change in a manner dependent upon the length of the Z-susceptible site.     

The B-A transition in superhelical DNA.

Relaxation of a DNA superhelical stress due to the B to A transition induced by trifluoroethanol has been studied by assessing the change of DNA orientation in a flow gradient. Using DNAs of different superhelical densities, a decrease in the winding angle during the B----A shift of DNA was found to be 1.5 degrees per base pair in solution. Accepting the winding angle for B-DNA in solution to be 34.1 degrees, that for A-DNA must have a value of 32.6 degrees which agrees with the X-ray data for A-DNA in the condensed state. The date obtained within the B-A transition interval make it possible to conclude that there is an increase in winding at each B/A junction, which is about 5 degrees per one junction.     

Nature of conformational restrictions in nuclear superhelical DNA from thymus lymphocytes

The lymphocyte nucleoids of mouse thymus contain about 40% of rapidly labelled nuclear RNA, about 9% of total intracellular protein and all nuclear DNA. Relaxation of superhelical DNA after thymocyte nucleoids treatment with pronase or RNAase suggests that non-histone proteins and/or RNAs are involved in conformational restrictions in the superhelical domains of cell DNAs. Thymocyte nucleoids proteins are represented by two groups of nonhistone proteins with molecular weights of 50 000-60 000 and 75 000-85 000. An essential role in the appearance of conformational restrictions in thymocyte superhelical DNA belongs to disulfide bonds.     

Fluctuations in superhelical DNA.

The effect of superhelicity on the base-pair opening probability and on the probability of occurrence of cruciform states in palindromic regions is theoretically treated. The calculations show that below the superhelix density value of -sigma=0.05 superhelicity does not appreciably affect the characteristics of DNA secondary structure fluctuations. In the range of physiological superhelix densities sigma (-sigma=0.05-0.09) the base-pair opening probability markedly increases. However, within this range of sigma the base-pairs are opened only transiently and permanently open regions are not formed. Permanently opened regions appear at higher negative superhelix densities (-sigma greater than 0.10). At the values of -sigma higher than 0.06 a cruciform structure in the palindromic region centred in position 3965 proves to be the most probable fluctuational disturbance in the 0x174 duplex DNA. Different experimental approaches used for probing the fluctuations in superhelical DNA have been analysed. The results suggest that most direct quantitative information can be derived from data on the nicking of closed DNA by single strand-specific endonucleases. Such data (Wang, 1974) accord with the results of theoretical calculations. Calculations show that, due to base-pair opening, the total free energy of superhelical DNA should depend parabolically on sigma only up to some critical value of sigma=sigmac. If negative superhelicity exceeds this critical value, which under physiological conditions proves to be -sigma=0.085, the free energy should increase linearly with -sigma. The biological role of supercoiling is discussed in the light of obtained results.     

The thermodynamic parameters of the conformational transitions in Mycoplasma DNA

DNA preparations have been isolated from 10 strains of phytopathogenic mycoplasms and collection culture Achole plasma laidlawii PG-8. Thermodynamic parameters of denaturation changes in the secondary structure (transconformation) of DNA of these mycoplasms have been determined. It is shown that denaturation temperature is 82.3-83.1 degree C and enthalpy of conformational DNA transitions calculated per 1 g of dry substance is 56.2-61.9 J/g. Changes in the enthalpy (delta H) and entropy (delta S) calculated per 1 mol of nucleotide pairs varied in the range of 35.6-39.0 J/m.p. and 995-109.6 J degree m.p. respectively. No linear dependence of transconformational thermal adsorption on the temperature of DNA denaturation of the studied strains of mycoplasms are revealed, which is probably connected with structural peculiarities of DNA of these microorganisms.     

Chromatin structural transitions in Drosophila embryo cell-free extract result in a high conformational flexibility of nucleosomal DNA.

DNA within chromatin has considerably more restricted flexibility in comparison with naked DNA. This raises the main question of how the functioning multi-enzyme complexes overcome the nucleosomal level of DNA packaging. We studied the DNA conformational flexibility of reconstituted chromatin in a cell-free system derived from Drosophila embryo extracts. Using this system, we have found evidence for a energy-independent chromatin remodelling process that efficiently destabilizes the nucleosome structure resulting in a high conformational flexibility of nucleosomal DNA. The described chromatin remodelling process may lay on the basis of defined molecular principles governing the molecular heterogeneity of chromatin structures in vivo.     

The influence of protein-lipid interactions on the order-disorder conformational transitions of the hydrocarbon chain.

The phases of simple systems involving one type of protein (lysozyme or cytochrome c) and one type of lipid (phosphatidic acid) have been characterized by X-ray crystallography, chemical analysis and spin-labeling technique as a function of temperature. They are of the lamellar type with alternative protein monolayers and lipid bilayers. According to the pH, two types of lamellar phases are obtained, one where the lipid-protein interactions are mainly hydrophobic, the other where they are electrostatic. In both cases, a phase transition occurs as temperature is lowered, between a high temperature phase, where all the lipids are in the liquid-like state, and another phase where some lipid chains are rigid. In the case of the phases with electrostatic interaction, it is shown that the onset of the order-disorder transition is shifted towards low temperature as compared with the homologous lipid-water phase and that the protein content of the phase decreases as the ratio of the liquid to rigid hydrocarbon chains decreases. This leads us to suggest that in the systems studied in this work the proteins interact only with lipid in the liquid-like state. In the case of the phases with hydrophobic interaction, it is shown that the extent of hydrophobic interaction between protein and lipid increases as the unsaturation of the hydrocarbon chains increases. The onset of the order-disorder transition shows a greater shift towards low temperature than the one observed in the case of the phase with electrostatic interaction.     

Ethanol-induced structural transitions of DNA on mica

The effect of ethanol on the structure of DNA confined to mica in the presence of Mg2+was examined by varying the ethanol concentration and imaging the DNA by atomic force microscopy. Contour length measurements of the DNA show a transition from all-B-form at 0% ethanol to all-A-form at >25% ethanol. At intermediate ethanol concentrations, contour lengths suggest that individual molecules of air-dried DNA are trapped with mixed compositions of A-form and B-form. The relative composition depends on the ethanol concentration. Fitting the length distributions at intermediate ethanol concentrations to a simple binomial model results in an upper bound estimate for the A-form and B-form domains of approximately 54 bp in the individual molecules. In addition to length changes, the apparent persistence length of DNA decreases with increasing ethanol concentration. At high concentrations of ethanol (>20%), DNA formed several higher order structures, including flower shaped condensates and toroids.     

A pH-dependent structural transition in the homopurine-homopyrimidine tract in superhelical DNA

We have inserted the 509-bp-long fragment of sea urchin P. miliaris histone gene spacer region into plasmid pUC19. The fragment contains the 60-bp-long homopurine-homopyrimidine tract that is known to be hypersensitive to the S1 endonuclease. Using two-dimensional gel electrophoresis we have observed a sharp structural transition in the insert with increasing DNA superhelicity. As in the cases of cruciform and Z form formation, the observed transition partly relaxes the superhelical stress. In contrast with the other two well documented transitions, the observed transition strongly depends on pH. At pH7 and above the transition occurs at negative superhelicities exceeding the physiological range (- sigma greater than 0.08). For pH6 the transition occurs at -sigma = 0.055, whereas for pH4.3 it takes place at -sigma = 0.001. A comprehensive analysis of the obtained data has made it possible to define the nature of the observed transition. We conclude that under superhelical stress or/and at low pH homopurinehomopyrimidine tracts adopt a novel spatial structure called the H form.     

Experimental method for studying conformational transitions in DNA

An experimental method combining fiber X-ray and direct fiber dimension measurements is proposed for the study of DNA conformational transitions. Curves corresponding to the A-B and B-C transitions are obtained by using the proportionality which exists between the fiber length and the axial rise per nucleotide in the DNA helix. The A-B transition is shown to be cooperative while the B-C one is a progressive change of helical conformation.     

Changes of hydration during conformational transitions of DNA

Fiber X-ray diffraction and measurement of fiber dimensions yields information about the hydration of DNA in fibers. The results obtained give us the fraction of nucleotides in the B form for the A-B transition or the rate of progression for the B-C transition as functions of the number of water molecules per nucleotide. The present experimental results confirm the importance of cooperativity in the A-B transition and the progressive change of the DNA double helix conformation during the C-B transition. At least twenty additional water molecules per nucleotide are necessary to stabilize the B form for DNA molecules in fibers following the A to B transition whereas only ten are sufficient when the B conformation is obtained starting from the C form. Offprint requests to: S. Premilat     

The influence of protein-lipid interactions on the order-disorder conformational transitions of the hydrocarbon chain

The phases of simple systems involving one type of protein (lysozyme or cytochrome $\text{c}$) and one type of lipid (phosphatidic acid) have been characterized by X-ray crystallography, chemical analysis and spin-labeling technique as a function of temperature. They are of the lamellar type with alternative protein monolayers and lipid bilayers. According to the pH, two types of lamellar phases are obtained, one where the lipid-protein interactions are mainly hydrophobic, the other where they are electrostatic. In both cases, a phase transition occurs as temperature is lowered, between a high temperature phase, where all the lipids are in the liquid-like state, and another phase where some lipid chains are rigid. In the case of the phases with electrostatic interaction, it is shown that the onset of the order-disorder transition is shifted towards low temperature as compared with the homologous lipid-water phase and that the protein content of the phase decreases as the ratio of the liquid to rigid hydrocarbon chains decreases. This leads us to suggest that in the systems studied in this work the proteins interact only with lipid in the liquid-like state. In the case of the phases with hydrophobic interaction, it is shown that the extent of hydrophobic interaction between protein and lipid increases as the unsaturation of the hydrocarbon chains increases. The onset of the order-disorder transition shows a greater shift towards low temperture than the one observed in the case of the phase with electrostatic interaction.     

An evaluation of the conformational changes in the superhelical DNA of eukaryotic cells by direct nucleoid fluorometry. II. The characteristics of the change in acridine orange fluorescence in studying the superhelical DNA of rat thymocytes

Comparative studies of acridine orange (AO) and ethidium bromide interactions with supercoiled DNA (scDNA) of thymocytes were performed in which various conformational changes were induced. AO may be efficiently used for evaluation of conformational alterations of scDNA. Moreover, employing the maximum values of AO fluorescence allows to determine the maximum levels of scDNA relaxation.     

Force-induced structural transitions in cross-linked DNA films

We report on the preparation and characterization of wet-spun films of sodium DNA in which intermolecular cross-links were introduced following formaldehyde treatment. Raman scattering shows that the DNA in moderately cross-linked films is mainly in the B conformation. Stretching experiments show a transition from plastic to elastomeric behavior with increasing exposure to the cross-linking agent. Elastomeric DNA films are strongly disordered. X-ray diffraction shows that stretching of moderately cross-linked films under controlled high humidity conditions results in increased molecular orientation as well as the appearance of meridional reflections at 7.4-7.8 and 8.2 A. These reflections are not observed for any of the classical conformations associated with mixed sequence DNA, and may arise from extended base-pair stacking in a stretched DNA structure.