Interaction of chloroquine with linear and supercoiled DNAs. Effect on the torsional dynamics, rigidity, and twist energy parameter

The magnitude and uniformity of the torsion elastic constant (alpha) of linear pBR322 DNA and supercoiled pBR322 DNAs with high-twist (sigma = -0.083) and normal-twist (sigma = -0.48) are measured in 0.1 M NaCl as a function of added chloroquine/base-pair ratio (chl/bp) by studying the fluorescence polarization anisotrophy (FPA) of intercalated ethidium dye. The time-resolved FPA is measured by using a picosecond dye laser for excitation and time-correlated single-photon counting detection. A general theory is developed for the binding of ligands that unwind superhelical DNAs, and the simultaneous binding of two different intercalators is treated in detail. The equilibrium constant (K) for binding chloroquine to linear pBR322 DNA and the number (r) of bound chloroquines per base pair are determined from the relative amplitude ratio of the slow (normally intercalated) and fast (free) components in the decay of the (probe) ethidium fluorescence intensity as a function of chl/bp. For chloroquine binding to supercoiled pBR322 DNAs, the intrinsic binding constant is assumed to be the same as for the linear DNA, but the twist energy parameter ET (N times the free energy to change the linking number from 0 to 1 in units of kBT) is regarded as adjustable. Using the best-fit ET, the binding ratios r are calculated for each chl/bp ratio. Twist energy parameters are also determined for ethidium binding to these supercoiled DNAs by competitive dialysis. For chloroquine binding, we obtain ET = 360 and 460 respectively for the normal-twist and high-twist supercoiled DNAs. For ethidium binding the corresponding values are ET = 280 +/- 70 and 347 +/- 50. Like other dye-binding values, these are substantially lower than those obtained by ligation methods. In the absence of chloroquine, the torsion constants of all three DNAs are virtually identical, alpha = (5.0 +/- 0.4) x 10(-12) dyn.cm. For linear pBR322 DNA, the magnitude and uniformity of alpha remain unaltered by intercalated chloroquine up to r = 0.19. This finding argues that the FPA is not significantly relaxed by diffusion of any kinks or solitons. If alpha d denotes the torsion constant between a dye and a base pair and alpha 0 that between two base pairs, then our data imply that alpha d/alpha 0 lies in the range 0.65-1.64, with a most probable value of 1.0.(ABSTRACT TRUNCATED AT 400 WORDS)     

Effect of ethidium on the torsion constants of linear and supercoiled DNAs.

The torsion elastic constants (alpha) of linear pBR322 (4363 bp) and pUC8 (2717 bp) DNAs and supercoiled pBR322 and pJMSII (4375 bp) DNAs are measured in 0.1 M NaCl as a function of added ethidium/base-pair (EB/BP) ratio by studying the fluorescence polarization anisotropy (FPA) of the intercalated ethidium. The time-resolved FPA is measured by using a picosecond dye laser for excitation and time-correlated single photon counting detection. Previously developed theory for the emission anisotropy is generalized to incorporate rotations of the transition dipole due to excitation transfer. The excitation transfers are simulated by a Monte Carlo procedure (Genest et al., Biophys. Chem. 1 (1974) 266-278) and the consequent rotations of the transition dipole are superposed on the Brownian rotations. After accounting for excitation transfer, the torsion constants of the linear DNAs are found to be essentially independent of intercalated ethidium up to a binding ratio r = 0.10 dye/bp. Dynamic light scattering measurements on linear pUC8 DNA confirm that the torsion constant is independent of binding ratio up to r = 0.20 dye/bp. If alpha d denotes the torsion constant between ethidium and a base-pair, and alpha 0 that between two base-pairs, then our data imply that alpha d/alpha 0 lies in the range 0.65 to 1.64 with a most probable value of 1.0. The torsion constants of supercoiled DNAs decrease substantially with increasing binding ratio even after accounting for excitation transfer. At the binding ratio r* = 0.064, where the superhelix density vanishes and superhelical strain is completely relaxed, the torsion constant of the supercoiled pBR322 DNA/dye complex lies below that of the corresponding linear DNA/dye complex by about 30%. This contradicts the conventional view according to which linear, nicked circular, and supercoiled DNA/dye complexes with r = r* should coexist with the same concentration of free dye, display the same distribution of bound dye, and exhibit identical secondary structures, twisting and bending rigidities, and FPA dynamics. These and other observations imply the existence of metastable secondary structure in freshly relaxed supercoiled DNAs. A tentative explanation is presented for these and other unexpected observations on supercoiled DNAs.     

Can reliable torsion elastic constants be determined from FPA data on 24 and 27 base-pair DNAs?

Torsion elastic constants obtained from fluorescence polarization anisotropy (FPA) measurements on fifty-three 24 and 27 base-pair (bp) DNAs were recently reported [F. Pedone, F. Mazzei, D. Santoni, Sequence-dependent DNA torsional rigidity: a tetranucleotide code, Biophys. Chem. 112 (2004) 77-88; F. Pedone, F. Mazzei, M. Matzeu, F. Barone, Torsional constant of 27-mer DNA oligomers of different sequences, Biophys. Chem. 94 (2001) 175-184]. The problem of extracting reliable torsion elastic constants (alpha) from FPA measurements on such short DNAs is examined in detail. The difficulty is illustrated by two (fictitious) 24 bp DNAs with approximately 5-fold different torsion elastic constants and 10% different initial anisotropies (r(0)), which exhibit practically indistinguishable anisotropy decays for all t>1 ns. FPA data were simulated for 24 bp DNAs with different input values of alpha and r(0) in the presence and absence of Poisson noise, and were fitted using different choices of the adjustable and fixed parameters. Experimental data for a 24 bp DNA were fitted in a similar manner. For either the simulated or experimental FPA data, it was not possible to determine both the initial anisotropy, r(0), and the torsion elastic constant, alpha, in a reliable (i.e. statistically significant) manner in the presence of Poisson noise. When r(0) is assumed to be fixed at any particular value in the fitting protocol, a unique best-fit value of alpha is obtained, but that best-fit alpha is extremely sensitive to small deviations of the assumed fixed value of r(0) away from the input r(0)-value of the simulated data. Pedone et al. fitted their FPA data by assuming that r(0)=0.360, and adjusting alpha, the hydrodynamic radius (R(H)), and effective length (L). In fact, the reported best-fit values of R(H) and L lay significantly outside their expected ranges. When this same fitting protocol is applied to simulated data for 27 bp DNAs, better overall agreement with the reported experimental values (alpha, R(H), and L) is obtained for a model, wherein all DNAs have the same typical input alpha=5.9 x 10(-12) dyn cm, R(H)=10.0 A, and L=27 (3.4)+2.7=94.5 A, but a 1.00- to 1.13-fold range of r(0)-values, than for the model of Pedone et al., wherein all DNAs have the same input r(0)=0.360, R(H)=10.0 A, and L=94.5 A, but a approximately 3-fold range of alpha-values. It is concluded that, in the absence of reliable independent estimates of r(0) for every DNA, the alpha-values reported for 24 and 27 bp DNAs cannot be regarded as experimentally justified. The reliability of the torsion elastic constants reported for the 136 distinct tetranucleotide steps, which are inferred from the values reported for the fifty-three 24 and 27 bp DNAs, is also briefly discussed.     

High-resolution separation and accurate size determination in pulsed-field gel electrophoresis of DNA. 4. Influence of DNA topology

Pulsed-field gel electrophoresis is a powerful technique for the fractionation of linear DNA molecules with sizes above 50 kilobase pairs (kb). Here it is demonstrated that this technique is also effective for separating smaller DNAs including linear, circular, and supercoiled species. The mobilities of linear DNAs larger than 8 kb can be modulated by pulse times between 0.1 and 100 s. The mobility of supercoiled DNA molecules up to 16 kb is generally unaffected by these pulse times except that 10-s pulse times cause a small but distinct increase in the mobility. The general insensitivity of small supercoiled DNAs to pulse time presumably occurs because these species reorient so rapidly that they spend most of their time undergoing conventional electrophoresis. However, the mobilities of larger supercoiled DNAs are affected by pulse times of less than 1 s, and at 0.1 s the molecules are better resolved by pulsed electrophoresis than by ordinary electrophoresis. The mobility of 3-19 kb nicked and relaxed circular DNA molecules is also affected by pulse time but in a complex way.     

Preferential binding of E.coli histone-like protein HU alpha to negatively supercoiled DNA.

Binding specificity of histone-like HU alpha protein to supercoiled DNA was examined by gel retardation assay and chemical probing with OsO4. The latter method was proved to be a unique means for detecting torsional tension restrained in supercoiled plasmid in the presence of HU alpha. It was shown that HU alpha protein has preferential affinity to negatively supercoiled DNA relative to relaxed, nicked and linearized DNAs. There were two modes for binding of HU alpha to the supercoiled DNA: one was the binding associated with topological changes in DNA and the other was relatively strong binding, probably specific to certain particular structures of DNA. It was suggested that HU in vivo interacts preferentially with the regions deformed under torsional stress or with the metabolically active regions along DNA.     

Isolation of Z-DNA binding proteins from SV40 minichromosomes: evidence for binding to the viral control region

Proteins dissociated from SV40 minichromosomes by increasing NaCl concentration were tested for their binding to Z-DNA [Br-poly(dG-dC)] and B-DNA [poly (dG-dC)]. Z-DNA binding proteins are largely released in 0.2 M NaCl whereas most B-DNA binding proteins are not released until 0.6 M NaCl. Incubation of SV40 minichromosomes with Z-DNA-Sephadex in low salt solution results in proteins with Z-DNA binding activity (PZ proteins). These proteins bind to negatively supercoiled DNAs containing left-handed Z-DNA but not to relaxed DNAs. They compete with anti-Z-DNA antibodies in binding to negatively supercoiled DNAs. The binding is tighter to negatively supercoiled SV40 DNA than to other plasmids, suggesting sequence-specific Z-DNA binding. PZ proteins binding to negatively supercoiled SV40 DNA interfere with cleavage at the Sph I sites, within the 72 bp repeat sequences of the viral control region, but not with cleavage at the Bgl I site, at the origin of replication. Removal of PZ proteins also exposes the Sph I sites in the SV40 minichromosomes while addition of PZ proteins makes the sites inaccessible.     

Histone stoichiometry and DNA circularization in archaeal nucleosomes.

Recombinant (r)HMfB (archaealhistone B fromMethanothermusfervidus) formed complexes with increasing stability with DNA molecules increasing in length from 52 to 100 bp, but not with a 39 bp molecule. By using125I-labeled rHMfB-YY (an rHMfB variant with I31Y and M35Y replacements) and32P-labeled 100 bp DNA, these complexes, designated archaeal nucleosomes, have been shown to contain an archaeal histone tetramer. Consistent with DNA bending and wrapping, addition of DNA ligase to archaeal nucleosomes assembled with 88 and 128 bp DNAs resulted in covalently-closed monomeric circular DNAs which, following histone removal, were positively supercoiled based on their electrophoretic mobilities in the presence of ethidium bromide before and after relaxation by calf thymus topoisomerase I. Ligase addition to mixtures of rHMfB with 53 or 30 bp DNA molecules also resulted in circular DNAs but these were circular dimers and trimers. These short DNA molecules apparently had to be ligated into longer linear multimers for assembly into archaeal nucleosomes and ligation into circles. rHMfB assembled into archaeal nucleosomes at lower histone to DNA ratios with the supercoiled, circular ligation product than with the original 88 bp linear version of this molecule. Archaeal histones are most similar to the globular histone fold region of eukaryal histone H4, and the results reported are consistent with archaeal nucleosomes resembling the structure formed by eukaryal histone (H3+H4)2tetramers.     

Improved electrophoretic separation of supercoiled and relaxed DNA in the presence of ethidium bromide.

Supercoiled and relaxed DNA were resolved electrophoretically in the presence of 0.5 micrograms/ml ethidium bromide. Under these conditions the Gaussian distributions of topological isomers of both supercoiled and relaxed DNA migrated as discrete bands. The separation of these DNAs was optimized by varying the concentration of electrode buffer. Electrophoresis in the presence of 160 mM Tris-acetate, pH 8.3, 4 mM EDTA resulted in a 20-fold increase in the separation of relaxed and supercoiled DNA relative to electrophoresis in 40 mM Tris-acetate, pH 8.3, 1 mM EDTA.     

Rapid microscale procedure for visualizing intracellular plasmid DNA by electron microscopy

A rapid microscale procedure is described that releases plasmid DNA in situ from the bacterial cell and that allows selective observation of the plasmid bound to cellular components. The released plasmid DNA was adsorbed preferentially on mica in a divalent cation-free medium then processed for electron microscopy. The plasmid DNAs studied were pAO3 (1683 base pairs (bp²)), λdv021 (3505 bp), pTSO118 (4000 bp), pAO65 (4786 bp), ColE1 (6500 bp), and RSF2124 (11,400 bp). These DNAs were seen as supercoiled circles or as relaxed circles of corresponding length. Occasionally an internal loop of replicating DNA was present. One micrometer of measured length corresponded to 3100 bp.     

Plasmid migration using orthogonal-field-alternation gel electrophoresis.

The migration properties of a series of supercoiled plasmids ranging in size from 4 to 16 kilobases (kb) have been analyzed by orthogonal-field-alternation gel electrophoresis (OFAGE). These circular DNAs enter the gel and are well resolved. Unlike linear DNA molecules, the relative mobilities of these plasmids are constant over a wide range of pulse times, from 10 to 120 seconds, as well as over a broad range of total running times, from 6 to 24 hours. Electrophoresis of supercoiled, relaxed, and nicked open circular forms as well as topoisomers of pBR322 shows that the extent of supercoiling has a dramatic effect on plasmid migration on OFAGE. Several practical applications for exploiting the different migration properties of circular and linear DNA molecules on OFAGE are presented.     

Torsional rigidities of weakly strained DNAs

Measurements on unstrained linear and weakly strained large (> or =340 bp) circular DNAs yield torsional rigidities in the range C = 170-230 fJ fm. However, larger values, in the range C = 270-420 fJ fm, are typically obtained from measurements on sufficiently small (< or =247 bp) circular DNAs, and values in the range C = 300-450 fJ fm are obtained from experiments on linear DNAs under tension. A new method is proposed to estimate torsional rigidities of weakly supercoiled circular DNAs. Monte Carlo simulations of the supercoiling free energies of solution DNAs, and also of the structures of surface-confined supercoiled plasmids, were performed using different trial values of C. The results are compared with experimental measurements of the twist energy parameter, E(T), that governs the supercoiling free energy, and also with atomic force microscopy images of surface-confined plasmids. The results clearly demonstrate that C-values in the range 170-230 fJ fm are compatible with experimental observations, whereas values in the range C > or = 269 fJ fm, are incompatible with those same measurements. These results strongly suggest that the secondary structure of DNA is altered by either sufficient coherent bending strain or sufficient tension so as to enhance its torsional rigidity.     

Isolation,characterization, and structure of the folded interphase genome of Drosophila melanogaster

The intact interphase genome of Drosophila melanogaster has been isolated by sucrose gradient centrifugation after gentle lysis of tissue culture cells in 0.9 M NaCl-0.4% Nonidet P40. The nonviscous folded DNA sediments as a single broad 5000S peak in a complex with RNA (a fraction of the nuclear nascent RNA) and protein (all of the four intranucleosome histones: H2A, H2B, H3, and H4).The folded DNA is supercoiled and can be relaxed to slower sedimenting forms either by intercalating ethidium or by nicking with DNAase I. Incomplete DNAase treatment gives partially relaxed complexes, indicating that each nick relaxes only a stretch of DNA (defined as a supercoiled DNA loop) without affecting the superhelical content of the rest of the genome. The concentration of superhelices in the Drosophila folded DNA is the same as in the E. coli and SV40 closed circular DNAs—that is, about one negative turn every 200 base pairs (bp) in 0.15 M NaCl at 26°C. The estimated average size of the supercoiled DNA loops, about 85,000 bp, equals the size of the larger Drosophila chromomeres.Ethidium intercalation in 0.9 M NaCl both removes the negative superhelical turns and dissociates the four histones from the DNA. The four histones are dissociated in equimolar concentrations, and the relative proportion of histones displaced from the DNA is a function of ethidium concentration. The histones are completely dissociated from the folded DNA at the ethidium concentration which removes all of the negative superhelices. Thus the data strongly suggest that the rotation of the Watson Crick helix which accompanies ethidium intercalation causes the loss of nucleosomes from the DNA.The results are interpreted in terms of a model for the folded Drosophila genome which has the DNA constrained (by both protein-DNA and RNA-DNA interactions) into independent supercoiled loops containing on the average 400 nucleosomes per loop. Each nucleosome is composed of a histone core with the DNA wound around it in a 360° left-handed toroidal supercoil; each nucleosome toroidal supercoil plus its relaxed internucleosome DNA contains, on the average, 200 bp.     

Effects of ethylene glycol on the torsion elastic constant and hydrodynamic radius of p30delta DNA

Upon increasing the concentration of ethylene glycol (EG) at 37 degrees C, the twist energy parameter, E(T), which governs the supercoiling free energy, was recently found to undergo a decreasing (or reverse) sigmoidal transition with a midpoint near 20 w/v % EG. In this study, the effects of adding 20 w/v % EG on the torsion elastic constant (alpha) of linear p30delta DNA and on the hydrodynamic radius (R(H)) of a synthetic 24 bp duplex DNA were examined at both 40 and 20 degrees C. The time-resolved fluorescence intensity and fluorescence polarization anisotropy (FPA) of intercalated ethidium were measured in order to assess the effects of 20 w/v % EG on: (1) alpha; (2) R(H); (3) the lifetimes of intercalated and non-intercalated dye; (4) the amplitude of dye wobble in its binding site; and (5) the binding constant for intercalation. The effects of 20 w/v % EG on the circular dichroism (CD) spectrum of the DNA and on the emission spectrum of the free dye were also measured. At 40 degrees C, addition of 20 w/v % EG caused a substantial (1.27- to 1.35-fold) increase in alpha, a significant change in the CD spectrum, and a very small, marginally significant increase in R(H), but little or no change in the amplitude of dye wobble in its binding site or the lifetime of intercalated dye. Together with previously reported measurements of E(T), these results imply that the bending elastic constant of DNA is significantly decreased by 20 w/v % EG at 40 degrees C. At 20 degrees C, addition of 20 w/v % EG caused a marginally significant decrease in alpha and very little change in any other measured properties. Also at 20 degrees C, addition of 30 w/v % betaine caused a marginally significant increase in alpha and significant but modest change in the CD spectrum, but very little change in any other properties.     

Effects of supercoiling in electrophoretic trapping of circular DNA in polyacrylamide gels.

Electrophoretic velocity and orientation have been used to study the electric-field-induced trapping of supercoiled and relaxed circular DNA (2926 and 5386 bp) in polyacrylamide gels (5% T, 3.3% C) at 7.5-22.5 V/cm, using as controls linear molecules of either the same contour length or the same radius of gyration. The circle-specific trapping is reversible. From the duration of the reverse pulse needed to detrap the molecules, the average trap depth is estimated to be 90 A, which is consistent with the molecular charge and the field strengths needed to keep molecules trapped. Trapped circles exhibit a strong field alignment compared to the linear form, and there is a good correlation between the enhanced field alignment for the circles and the onset of trapping in both constant and pulsed fields. The circles do not exhibit the orientation overshoot response to a field pulse seen with linear DNA, and the rate of orientation growth scales as E(-2+/-0.1) with the field, as opposed to E(-1.1+/-0.1) for the linear form. These results show that the linear form migrates by cyclic reptation, whereas the circles most likely are trapped by impalement on gel fibers. This proposal is supported by very similar velocity and orientation behavior of circular DNA in agarose gels, where impalement has been deemed more likely because of stiffer gel fibers. The trapping efficiency is sensitive to DNA topology, as expected for impalement. In polyacrylamide the supercoiled form (superhelical density sigma = -0.05) has a two- to fourfold lower probability of trapping than the corresponding relaxed species, whereas in agarose gels the supercoiled form is not trapped at all. These results are consistent with existing data on the average holes in the plectonemic supercoiled structures and the fiber thicknesses in the two gel types. On the basis of the topology effect, it is argued that impalement during pulsed-field electrophoresis in polyacrylamide gels may be useful for the separation of more intricate DNA structures such as knots. The results also indicate that linear dichroism on field-aligned molecules can be used to measure the supercoiling angle, if relaxed DNA circles are used as controls for the global degree of orientation.     

Evidence for allosteric transitions in secondary structure induced by superhelical stress

Previous studies suggest that the global secondary structures of native supercoiled and equilibrium linear DNAs may differ somewhat. Recent evidence also indicates that metastable secondary structure commonly persists following complete relaxation of the superhelical stress by intercalating dyes or by the action of topoisomerase I. In this work, the torsion constants (alpha) of pBR322, pUC8 and M13mp7 (replicative form) DNAs are determined by time-resolved fluorescence polarization anisotropy at various times subsequent to linearization. In all three cases, the torsion constants are relatively low immediately after linearization, and evolve for eight to ten weeks before reaching their apparent equilibrium values. It is shown in detail how the persistence of metastable secondary structure, subsequent to relaxation of superhelical stress, necessarily implies that one or more transitions in equilibrium secondary structure are induced as the superhelix density is varied from zero to native, or vice versa. Samples of pUC8 dimer (5434 base-pairs) with different superhelix densities are prepared by the action of topoisomerase I in the presence of various amounts of ethidium. Their median linking number differences are determined by standard band counting methods. The translational diffusion coefficient (Do) and the plateau diffusion coefficient (Dplat) characterizing internal motions over short distances (225 A) are determined by dynamic light-scattering. The torsion constant (alpha) between base-pairs and the circular dichroism spectrum are also measured for each sample. Curves of Dplat, Do, alpha and molar ellipticity ([theta]) (at the minimum near 250 nm) versus superhelix density (sigma) are constructed. The curve of Do versus sigma is very similar to that for sedimentation coefficient versus sigma for simian virus 40 (SV40) and polyoma DNAs. The curves of Dplat, Do, alpha and [theta] versus sigma show that, with increasing negative superhelix density, a structural transition occurs near sigma = -0.020 to an intermediate state with low torsion constant, and a second structural transition occurs near sigma = -0.035 to a state that exhibits more normal properties by sigma = -0.048. These data are consistent with the hypothesis that supercoiling induces two successive allosteric transitions to alternative global secondary structures. The data are much less consistent with the hypothesis that supercoiling induces some radical secondary structure at one or a few sites of small extent at sigma = -0.020, and at other sites at sigma = -0.035, or with hypotheses based on changes in tertiary structure alone.(ABSTRACT TRUNCATED AT 400 WORDS)     

Superhelical torsion controls DNA interstrand cross-linking by antitumor cis- diamminedichloroplatinum(II).

Negatively supercoiled, relaxed and linearized forms of pSP73 DNA were modified in cell-free medium by cis-diamminedichloroplatinum(II) (cisplatin). The frequency of interstrand cross-links (ICLs) formed in these DNAs has been determined by: (i) immunochemical analysis; (ii) an assay employing NaCN as a probe of DNA ICLs of cisplatin; (iii) gel electrophoresis under denaturing conditions. At low levels of the modification of DNA (<1 Pt atom fixed per 500 bp) the number of ICLs formed by cisplatin was radically enhanced in supercoiled in comparison with linearized or relaxed DNA. At these low levels of modification, the frequency of ICLs in supercoiled DNA was enhanced with increasing level of negative supercoiling or with decreasing level of modification. In addition, the replication mapping of DNA ICLs of cisplatin was consistent with these lesions being preferentially formed in negatively supercoiled DNA between guanine residues in both the 5'-d(GC)-3' and the 5'-d(CG)-3' sites. Among the DNA adducts of cisplatin the ICL has the markedly greatest capability to unwind the double helix. We suggest that the formation of ICLs of cisplatin is thermodynamically more favored in negatively supercoiled DNA owing mainly to the relaxation of supercoils.     

The problems of eukaryotic and prokaryotic DNA packaging and in vivo conformation posed by superhelix density heterogeneity

Systems for gel electrophoresis in the presence of one of the intercalative unwinding ligands, ethidium or chloroquine, have been developed which permit the resolution of highly supercoiled closed circular DNA molecules differing by unit values of the topological winding number, alpha. All native closed circular DNAs examined, including the viral and intracellular forms of SV40 and polyoma DNA, bacterial plasmid DNAs, and the double stranded closed circular DNA genome of the marine bacteriophage, PM2, are more heterogeneous with respect to the number of superhelical turns present than are the thermal distributions observed in the limit products of the action of nicking-closing (N-C) enzyme on the respective DNAs. In the cases of SV40 and polyoma, where it has been shown that the supercoiling is a combined consequence of the binding of the four nucleosomal histones, H2a, H2b, H3 and H4, and the action of N-C enzyme, the breadth of the distributions within the form I DNAs poses specific problems since the work of other laboratories indicates that the number of nucleosomes on the respective minichromosomes falls within a narrow distribution of 21. If it is assumed that all nucleosomes have identical structures, and that the DNA within a nucleosome is not free to rotate, the native DNA would be anticipated to be less heterogeneous than the thermal equilibrium mixtures present in N-C enzyme relaxed SV40 and polyoma DNAs.The absolute number of superhelical turns (at 37 degrees C in 0.2 M NaCl) in virion polyoma DNA has been determined to be 26 +/- 1, which is the same value obtained for virion SV40 DNA. This is consistent with the observations that polyoma DNA has a higher molecular weight, a lower superhelix density, but the same number of nucleosomes as SV40 DNA. In addition, the distributions within the virion and intracellular form I DNAs of both SV40 and polyoma were found to be indistinguishable.Images     

Polyamine-induced hydrolysis of apurinic sites in DNA and nucleosomes.

The ability of different polyamines to catalyze hydrolysis of phosphodiester linkages in apurinic and apyrimidinic (AP) sites has been investigated in supercoiled, relaxed and denatured DNA, and also in core and chromatosome particles. The rate constants for the hydrolysis in the DNAs have been determined. In general the order of effectiveness of the polyamines were: spermine greater than spermidine greater than putrescine greater than cadaverine. A 9 fold difference in rate constants was found between spermine and cadaverine. No difference in the rate of hydrolysis was seen between AP-sites in supercoiled and relaxed DNAs, whereas the rate for the single-stranded DNA and DNA in core and chromatosome particles was only half of that in the double-stranded DNA. All AP-sites in both free DNA and DNA-histone particles were hydrolyzed in the presence of polyamines. For all polyamines, with the exception of spermine, increasing concentration of both Mg++ and salts such as KCl both led to a large decrease in the rate of polyamine-induced hydrolysis of AP-sites. The rate of hydrolysis increased markedly with increasing pH in the pH range pH 6 - pH 11.     

Histone H1 preferentially binds to superhelical DNA molecules of higher compaction.

In chromatin, the physiological amount of H1 is one molecule per nucleosome or, roughly, one molecule per 200 bp of DNA. We observed that at such a stoichiometry, H1 selectively binds to supercoiled DNA with magnitude of sigma > or = 0.012 (both negative and positive), leaving relaxed, linear, or nicked DNA molecules unbound. When negative and positive DNA topoisomers of varying superhelicity are simultaneously present in the binding mixture, H1 selectively binds to the molecules with highest superhelicity; less supercoiled forms are gradually involved in binding upon increasing the amount of input protein. We explain this topological preference of H1 as the consequence of an increased probability for more than one H1-DNA contact provided by the supercoiling. The existence of simultaneous contacts of H1 with both intertwined DNA strands in the supercoiled DNA molecules is also inferred by topoisomerase relaxation of H1-DNA complexes that had been prefixed with glutaraldehyde.