Circular dichroism of histone-bound regions in chromatin.

Native, NaCl-treated, trypsin-treated, and polylysine-bound nucleohistones were studied in 2.5 × 10^?4 M EDTA, pH 8.0, using circular dichroism (CD) and thermal denaturation. Removal of histone I by 0.6 M NaCl has a much smaller effect on both Δε₂₂₀ and Δε₂₇₈ than the removal of other histones. This indicates that histone I has less helical content and less conformational effect on the DNA in nucleohistone. By extrapolating to 100% binding by histones other than I, the positive CD band near 275 nm is close to zero. Comparison is also made between the effects of binding by the more basic and the less basic halves of histones by trypsin-digestion and polylysine-binding experiments. Trypsin digestion of nucleohistone reduces melting band IV at 82°C much more than melting band III at 72°C. However, the CD changes of Δε₂₇₈ and Δε₂₂₀ induced by trypsin digestion are small, unless melting band III is also reduced by the use of a higher trypsin level. This implies that the less basic halves of histones, which stabilize DNA to 72°C (melting band III), have more helical structure and are more responsible for conformational change in DNA than are the more basic halves, which stabilize DNA to 82°C (melting band IV). Polylysine binding to nucleohistone diminishes melting band III but has no effect on melting band IV. This binding affects only slightly the Δε₂₂₀ of nucleohistone, indicating that polylysine interferes very little with the structure of the less basic halves of bound histones. The implications of these studies with respect to chromatin structure are discussed.     

Helix-coil transition in nucleoprotein: renaturation of polylysine-DNA and polylysine-nucleohistone complexes

Thermal denaturation and renaturation of directly mixed and reconstituted polylysine–DNA, directly mixed polylysine–nucleohistone complexes, and NaCl-treated nucleohistones in 2.5 × 10^?4 M EDTA, pH 8.0 have been studied. At the same input ratio of polylysine to DNA, the percent of renaturation of free base pairs in a directly mixed polylysine–DNA complex is higher than that in a reconstituted complex. For a directly mixed complex, the renaturation of free base pairs is proportional to the fraction of DNA bound by polylysine or inversely proportional to the sizes of free DNA loops. A of large amount of renaturation of free base pairs has also been observed for 0.6 M and 1.6 M NaCl-treated nucleohistones. The binding of polylysine to nucleohistone enhances the renaturation of histone-bound base pairs. The percent of renaturation of polylysine–bound base pairs is high and is approximately independent of the extent of binding on DNA by polylysine. This is true in polylysine–DNA complexes prepared either by reconstitution or by directly mixing. It also applies for polylysine–nucleohistone complexes. The model where polylysine-bound base pairs collapse at T_m′ with two complementary strands still bound by polylysine is favored over the model where polylysine is dissociated from DNA during melting. The low renaturation of histone-bound base pairs in nucleo-histone indicates that either histones do not hold two complementary strands of DNA tightly or that histones are fully or partially dissociated from DNA when the nucleo-histone is fully denatured.     

Urea perturbation and the reversibility of nucleohistone conformation

Urea effect on conformation and thermal stabilities in nucleohistone and NaCl-treated partially dehistonized nucleohistones has been studied by circular dichroism (CD) and thermal denaturation. Urea imposes a CD change at 278mm of DNA base pairs in native and NaCl-treated nucleohistones which can be decomposed into two parts: a decrease in Δε₂₇₈ for histone-free base pairs and an increase for histone-bound base pairs. The reduction by urea of Δε₂₂₀ of bound histones is approximately proportional to the increase of Δε₂₇₈ of histone-bound base pairs. Urea also lowers the melting temperatures of base pairs both free and bound by histones. The presence of urea indeed destroys the secondary structure of bound histones, causing changes in the conformation and thermal stabilities of histone-bound base pairs in nucleohistone. Such a urea perturbation on nucleohistone conformation is reversible.     

Ultraviolet radiation response to the physical properties of the reconstituted nucleohistone

The effect of UV irradiation on the reconstituted nucleohistone have been studied with reference to its (nucleohistone) changes in physical properties, after irradiation at different UV doses. The rate of fall of specific viscosity ratio of the reconstituted nucleohistone as a function of UV dose decreased gradually with the increasing histone to DNA weight ratio (r). This effect, was not observed when the histones remained dissociated from DNA, in high ionic strength (1.5 M NaCl). Histone-DNA complex (r=0.97) irradiated up to a dose of 3.6×10⁴ J/m² had a stable melting temperature unlike free DNA where UV irradiation lowered the melting temperature and the heterogeneous melting profiles were observed. Rate of formaldehyde reaction, with DNA recovered from the irradiated complex, was slower than that with native DNA treated at the same dose. All this suggested that the effect of UV in the DNA of the nucleohistone was less, compared to that in free DNA.     

Helix-coil transition in nucleoprotein. Effect of ionic strength on thermal denaturation of polylysine-DNA complexes

Thermal denaturation of direct-mixed and reconstituted polylysine–DNA complexes in 2.5 × 10^?4 M EDTA, pH 8.0 and various concentrations of NaCl has been studied. For both complexes, increasing ionic strength of the solution raises T_m, the melting temperature of free base pairs. The linear dependence of T_m on log Na⁺ indicates that the concept of electrostatic shielding on phosphate lattice of an infinitely long pure DNA by Na⁺ can be applied to short free DNA segments in a nucleoprotein. For a direct-mixed polylysine–DNA complex, the melting temperature of bound base pairs T_m′ remains constant at various ionic strengths. On the other hand, the T_m′ in a reconstituted polylysine–DNA complex is shifted to lower temperature at higher ionic strength. This phenomenon occurs for reconstituted complex with long polylysine of one thousand residues or short polylysine of one hundred residues. It is shown that such a decrease of T_m′ is not due to a reduction of coupling melting between free and bound regions in a complex when the ionic strength is raised. It is also not due to intermolecular or intramolecular change from a reconstituted to a direct-mixed complex. It is suggested that this phenomenon is due to structural change on polylysine-bound regions by ionic strength. It is suggested further that Na⁺ may replace water molecules and bind polylysine-bound regions in a reconstituted complex. Such a dehydration effect destabilizes these regions and lowers T_m′. This explanation is supported by circular dichroism (CD) results.     

Studies on the thermal denaturation of nucleohistones

The thermal denaturation profiles of nucleohistone from calf thymus, sea urchin sperm and sea cucumber male gonad, are studied and compared under a variety of conditions. These include melting in the presence of either one of the following agents: urea, methanol, divalent cations or excess histones. The influence of ionic strength, pH, formaldehyde treatment and partial denaturation is also studied. Particular attention is given to the factors which influence the bimodal appearance of the profiles. The melting curves of the three materials used are qualitatively similar under all conditions, although they show quantitative differences. The histone:DNA ratio appears to be the most important parameter to define the denaturation properties of a given nucleohistone preparation. It is shown that redistribution of histones may determine the melting profile, since during denaturation histones can migrate from locally denatured regions towards those regions which contain native DNA. It is also shown that there are regions of phosphate negative charges of DNA not protected by histone. These regions can be protected against denaturation either by additional histones or by certain divalent cations. The results are interpreted in terms of the various models possible for the distribution of histones on DNA in native nucleohistone. Their biological significance is also discussed.     

Chromosomal DNA denaturation and reassociation in situ.

The degree of chromosomal DNA (cDNA) denaturation and renaturation on polytene chromosomes has been measured by UV microspectrophotometry. Also DNA losses occurring upon denaturation have been quantified by Feulgen, gallocyanin-chromalum and UV. It has been observed that denaturation in alkali (0.07 N NaOH at room temperature) and formamide (90% formamide; 0.1 SSC, pH 7.2) at 65 °C removes about 30% of the DNA. Low DNA loss occurs upon denaturation in HCl (0.24 M) at room temperature and 60% formamide: 2 × 10^?4 M EDTA (pH 8) at 55 °C. The presence of 4% formaldehyde in the denaturation buffer prevents DNA loss. After denaturation of chromosomes in 0.1 × SSC containing 4% formaldehyde at 100 °C for 30 sec, an hyperchromicity of 39 °C is observed. The denaturation efficiency varies with the denaturation treatment. The percentage reassociation was measured from the difference in the UV absorption of renatured chromosomes and that of denatured chromosomes from the same set. It seems that in our conditions DNA:DNA reassociation does not occur. The efficiency of hybridization is proportional to the denaturation extent of the DNA. However, the entire fraction of DNA which has been denatured is not available for hybridization.     

Melting and premelting phenomenon in DNA by laser Raman scattering.

Raman spectra of DNA from calf thymus DNA have been taken over a wide range of temperatures (25°–95°) in both D₂O and H₂O. A study of the temperature dependence of the Raman spectra shows that the temperature profiles of the intensities and frequencies of the various bands fall into four different categories: (1) base bands that show a reversible increase in intensity prior to the melting region, i.e., a definite premelting phenomenon; (2) base bands that show little or no temperature dependence; (3) deoxyribose-phosphate backbone vibrations that show no temperature dependence up to the melting region, at which point large decreases in intensity occur; and (4) slow frequency changes in certain in-plane vibrations of guanine and adenine due to deuteration of the C-8 hydrogen of these purines in D₂O. Certain Raman bands arising from each of the four bases, adenine, thymine, guanine, and cytosine have been found to undergo a gradual increase in intensity prior to the melting region at which point large, abrupt increases in intensity occur. The carbonyl stretching band of thymine, involved in the interbase hydrogen bonding actually undergoes both a gradual shift to a lower frequency as well as an increase in intensity. These changes provide evidence that some change in the geometry of the bases relative to each other begins to occur around 50°C, well below the melting region of 70°–85°C. From the spectra taken at various temperatures, the DNA appears to remain in the B conformation until the melting point is reached, at which time the DNA progresses into a disordered random-coil form. No A-form conformation is found either in the premelting or the melting region.     

Helix–coil transition and conformational studies of protamine–DNA complexes

Protamine–DNA complexes prepared by the method of direct and slow mixing in 2.5 × 10^?4M EDTA, pH 8.0, have been studied by thermal denaturation and circular dichroism. The complexes show biphasic melting with T_m at about 50 °C corresponding to the melting of free DNA regions and T_m′ at about 92 °C corresponding to the melting of protamine-bound regions. In protamine-bound regions there are 1.38 amino acid residues per nucleotide, indicating a nearly completely charge neutralization. T_m is increased but T_m′ is not when the ionic strength of the buffer is raised. This also supports a full charge neutralization in protamine-bound regions. The circular dichroism of the complexes can be decomposed into two components, Δ_ε0 of free DNA regions in B-form conformation and Δ_εb of protamine-bound regions in a characteristic conformation neither that of B- nor C-form but somewhere between them.     

Ionic strength-dependent conformational transitions of chromatin. Circular dichroism and thermal denaturation studies

High-molecular-weight chicken erythrocyte chromatin was prepared by mild digestion of nuclei with micrococcal nuclease. Samples of chromatin containing both core (H3, H4, H2A, H2B) and lysine-rich (H1, H5) histone proteins (whole chromatin) or only core histone proteins (core chromatin) were examined by CD and thermal denaturation as a function of ionic strength between 0.75 and 7.0 × 10^?3M Na⁺. CD studies at 21°C revealed a conformational transition over this range of ionic strengths in core chromatin, which indicated a partial unfolding of a segment of the core particle DNA at the lowest ionic strength studied. This transition is prevented by the presence of the lysine-rich histones in whole chromatin. Thermal-denaturation profiles of both whole and core chromatins, recorded by hyperchromicity at 260 nm, reproducibly and systematically varied with the ionic strength of the medium. Both materials displayed three resolvable thermal transitions, which represented the total DNA hyperchromicity on denaturation. The fractions of the total DNA which melted in each of these transitions were extremely sensitive to ionic strength. These effects are considered to result from intra- and/or internucleosomal electrostatic repulsions in chromatin studied at very low ionic strengths. Comparison of the whole and core chromatin melting profiles indicated substantial stabilization of the core-particle DNA by binding sites between the H1/H5 histones and the 140-base-pair core particle.     

Interaction between poly(L-lysine48, L-histidine52) and DNA.

Poly(Lys⁴⁸, His⁵²), a random copolypeptide of L -lysine (48%) and L -histidine (52%), was used as a model protein for investigating the effects of protonation on the imidazole group of histidines on protein binding to DNA. The complexes formed between poly(Lys⁴⁸, His⁵²) and DNA were examined using absorbance, circular dichroism (CD), and thermal denaturation. Although increasing pH reduces the charges on histidine side chains in the model protein, the protein still binds the DNA with approximately one positive charge per negative charge in protein-bound regions. Nevertheless, CD and melting properties of poly(Lys⁴⁸, His⁵²)-DNA complexes still depend upon the solution pH which determines the protonation state of imidazole group of histidine side chains. At pH 7.0, the complexes show two characteristic melting bands with a t_m (46–51°C) for free base pairs and a t′_m (94°C) for protein-bound base pairs. The t′_m of the complexes is reduced to 90°C at pH 9.2, although at this pH there is still one lysine per phosphate in protein-bound regions. Presumably, the presence of deprotonated histidine residues destabilizes the native structure of protein-bound DNA. The binding of this model protein to DNA causes a red shift of the crossover point and both a red shift and a reduction of the positive CD band of DNA near 275 nm. This phenomenon is similar to that caused by polylysine binding. These effects, however, are greatly diminished when histidine side chains in the model protein are deprotonated. The structure of already formed poly(Lys⁴⁸, His⁵²)·DNA complexes can be perturbed by changing the solution pH. However, the results suggest a readjustment of the complex to accommodate charge interactions rather than a full dissociation of the complex followed by reassociation between the model protein and DNA.     

Activity of endonuclease S1 in denaturing solvents: dimethysulfoxide, dimethylformamide, formamide and formaldehyde.

The endonuclease S₁ from $\text{Aspergillus oryzae}$ is shown to be active in aqueous solutions of greater than 60 percent formamide, 50 percent dimethylsulfoxide, 30 percent dimethylformamide and in 2 percent formaldehyde. The melting profile of T7 DNA is determined by S₁ digestion in 50 percent formamide and is found to agree with the optical melting profile. The single-strand specificity of S₁ is retained in 50 percent formamide at 37°C, 3°C below the DNA melting temperature. S₁ is shown to be active at temperatures greater than 5°C above the DNA melting temperature in this solvent.     

The effect of Cr(III) upon the thermal denaturation of DNA

Thermal denaturation studies of Cr-DNA solutions at pH 6.0 were carried out by monitoring the uv absorbance at 260 nm. The melting curves of solutions of calf thymus and Escherichia coli DNA with added Cr(ClO₄)₃ were broadened and shifted to higher temperatures. As the ratio of Cr: DNA increased, the melting temperature increased until it reached a maximum at Cr: DNA ratios of 0.7 (E. coli) and 0.9 (calf thymus). At higher concentrations of Cr³⁺ the melting temperature decreased and then leveled off, but it never fell as low as that of the pure DNA.     

Thermal denaturation of DNA in situ as studied by acridine orange staining and automated cytofluorometry

Thermal denaturation of nuclear DNA is studied in situ in individual cells or isolated cell nuclei by employing the property of the fluorochrome acridine orange (AO) to differentially stain native and denatured DNA and by using an automated flow-through cytofluorimeter for measurement of cell fluorescence. RNAse-treated cells, or cell nuclei, are heated, stained and measured while in suspension and AO-DNA interaction is studied under equilibrium conditions. Measurements are made rapidly (200 cells/sec); subpopulations of cells from a measured sample can be chosen on the basis of differences in their staining or light-scattering properties and analysed separately. DNA denaturation in situ is rapid; it approaches maximum during the first 5 min of cell heating. Divalent cations stabilize DNA against denaturation. At low pH the transition occurs at lower temperature and the width of the transition curves (‘melting profiles’) is increased. Decrease in ionic strength lowers the DNA melting temperature. This effect is much more pronounced in cells pretreated with acids under conditions known to remove histones. Histones thus appear to stabilize DNA in situ by providing counterions. At least four separate phases can be distinguished in melting profiles of DNA in situ; they are believed to indicate different melting points of DNA in complexes with particular histones. A decrease in cell (nuclear) ability to scatter light coincides with DNA melting in situ, possibly representing altered refractive and/or reflective properties of cell nuclei. Formaldehyde, commonly used to prevent DNA renaturation, is not used in the present method. The heat-induced alterations in nuclear chromatin are adequately stabilized after cell cooling in the absence of this agent. Cells heated at 60–85 °C exhibit increased total fluorescence after AO-staining, which is believed to be due to unmasking of new sites on DNA. This increase is neither correlated with DNA melting, nor with the presence of histones. Possibly, it reflects destruction of DNA superstructure maintained at lower temperatures by DNA associations with other than histone macromolecules (nuclear membrane).     

Studies on poly(L-lysine50, L-tyrosine50)-DNA interaction

Interaction between poly(Lys⁵⁰, Tyr⁵⁰) and DNA has been studied by absorption, circular dichroism (CD), and fluorescence spectroscopy and thermal denaturation in 0.001M Tris, pH 6.8. The binding of this copolypeptide to DNA results in an absorbance enhancement and fluorescence quenching on tyrosine. There is also an increase in the tyrosine CD at 230 nm. The CD of DNA above 250 nm is slightly shifted to the longer wavelength which is qualitatively similar to, but quantitatively much smaller than, that induced by polylysine binding. At physiological pH the poly(Lys⁵⁰, Tyr⁵⁰)–DNA complex is soluble until there is one lysine and one tyrosine per nucleotide in the complex. The same ratio of amino acid residues to nucleotide has also been observed in copolypeptide-bound regions of the complex. The addition of more poly(Lys⁵⁰, Tyr⁵⁰) to DNA yields a constant melting temperature, T_m′, for bound base pairs at 90°C which is close to that of polylysine-bound DNA under the same condition. The melting temperature, T_m, of free base pairs at about 60°C on the other hand, is increased by 10°C as more copolypeptide is bound to DNA. As the temperature is raised, both absorption and CD spectra of the complexes with high coverage are changed, suggesting structural alteration, perhaps deprotonation, on bound tyrosine. The results in this report also suggest that intercalation of tyrosine in DNA is unlikely to be the mode of binding.     

Analysis of Human DNA-Arginine Photoadduct Modified with Peroxynitrite

The aim of the study is the biochemical characterization of human DNA modified with arginine and peroxynitrite. In the present study, DNA was isolated from human blood cells and its adduct was formed with one of the amino acid, arginine. The DNA-arginine adduct was then modified with peroxynitrite, a reactive nitrogen species. The modified DNA adduct was characterized by ultraviolet (UV) absorption spectroscopy, thermal melting profile, and electrophoresis studies. UV spectroscopic analysis of the photoadduct showed hyperchromicity, indicating the formation of single-strand breaks and photomodification. Thermal denaturation studies of DNA-arginine adduct and peroxynitrite-modified adduct showed a decrease in the temperature (T _m) value by 4.5°C and an increase in the T _m of 8°C, respectively. Peroxynitrite modification is evident by an increase in the T _m value and a change in the migration pattern of native and modified photoadducts on agarose gel electrophoresis. The DNA-arginine and peroxynitrite-modified photoadducts could have important implications in various pathophysiological and immunopathological conditions.     

Thermal denaturation of Na- and Li-DNA in salt-free solutions

Thermal denaturation of Na- and Li-DNA from chicken erythrocytes was studied by means of scanning microcalorimetry in salt-free solutions at DNA concentrations (C_p) from 4.5 · 10^?2 to 1 · 10^?3 moles of nucleotides/liter (M). Linear dependencies of DNA melting temperature (T_m) vs lgC_p were obtained: ((1)) ((2)) for Na- and Li-DNA, respectively. Microcalorimetry data were compared with the results of spectrophotometric studies at 260 nm of DNA thermal denaturation in Me-DNA + MeCl solutions at C_p ? (6–8) · 10^?5 M and C_s = 0–40 mM (Me is Na or Li, C_s is salt concentration). It was found that Eqs. (1) and (2) are valid in DNA salt-free solutions over the C_p range 6 · 10^?5?4.5 · 10^?2M. Protonation of DNA bases due to the absorption of CO₂ from air in Na-DNA + NaCl solutions affects DNA melting parameters at C_s < 4 mM. Linear dependence of T_m on lga₊ is found in Na-DNA + NaCl at C_s > 0.4 mMin the absence of contact of solutions with CO₂ from air (a₊ is cation activity). A dependence of [dT_m/dlga₊] on Li⁺ activity was observed in Li-DNA + LiCl solutions at C_s < 10 mM: [dT_m/dlga₊] increases from 17°–18° at C_s > 10 mM to 28°–30° at C_s ? 0.2–0.4 mM. Spectrophotometric measurements at 282 nm show that this effect was caused by protonation of bases in fragments of denatured DNA in neutral solutions. The Poisson–Boltzmann (PB) equation was solved for salt-free DNA at the melting point. The linear dependence of T_m vs lgC_p was interpreted in terms of Manning's condensation theory. PB and Manning's theories fit the experimental data if charge density parameter (ξ) of denatured DNA is in the range 1.8–2.1 (assuming for native DNA ξ = 4.2). Specificity of Li ions in interactions with DNA is discussed. © 1994 John Wiley & Sons, Inc.     

Characterization of DNA from the Dinoflagellate Woloszynskia bostoniensis1

Some physical and chemical properties of DNA isolated from the dinoflagellate Woloszynskia bostoniensis were determined. Analytical cesium chloride gradient centrifugation gave a major component and a minor component banding at 1.719 and 1.693 g/cm, respectively. Thermal denaturation in 0.1 SSC showed a broad transition with a T_m of 70.5° C. Derivation of this curve indicated that two components were present having T_m values of 66° C and 70° C. Base composition analysis showed a GC content of 48.1% and a high degree of thymine replacement by 5-hydroxymethyluracil. Two minor bases, identified as 5-methylcytosine and N⁶-methyladenine, were also detected. Reassociation kinetics showed a typical eukaryotic reassociation pattern with 45% repetitive and 55% single copy sequences.     

The effects of aqueous neutral-salt solutions on the melting temperatures of deoxyribonucleic acids

The helical stability of a variety of DNA samples, ranging in base composition from 0 to 72 mole-% GC, has been studied by heat denaturation at neutral pH in increasing concentrations of LiCl, NaCl, KCl, CsCl, Li₂SO₄, and K₂SO₄. The variation of melting temperature with average base composition, dT_m/dX_GC, was found to decrease drastically in the concentrated salt media, e.g., from 41°C in 0.006M LiCl to 29°C in 3.2M LiCl, and from 39°C in 0.003M Li₂SO₄ to 18°C in 1.6M Li₂SO₄. At the same time, the thermal transition is much more cooperative in the concentrated salt solutions than at low ionic strength. Indeed, at limiting salt concentrations, the transition breadth seems to reach a minimum value irrespective of the compositional heterogeneity of the DNA samples. Attempts to correlate the observed decrease of dT_m/dX_GC with predicted changes in the enthalpy of melting, deduced from a simple theoretical treatment, experimental data on the binding of counterions and water to DNA, and experimental data on thermal denaturation, were unsuccessful. However, the strongly reduced composition dependence of the melting temperature can be understood in terms of a destabilizing effect of the concentrated salt media on GC-base pairs. It is suggested, though not proven, that the destabilization involves the displacement of water molecules from the DNA helix.     

A study of DNA denaturation in the ultracentrifuge

The melting transition of DNA in alkaline CsCl can be followed in the analytical ultracentrifuge. Equilibrium partially denatured states can be observed. These partially denatured DNA bands have bandwidths of up to several times those of native DNA. Less stable molecules melt early and are found at heavier densities in the melting region. An idealized ultracentrifuge melting transition is described. The melting transition of singly nicked PM-2 DNA resembles the idealized curve. The DNA profile is a Gaussian band at all points in the melt. DNA's from mouse, D. Melanogaster, M. lysodeikticus, T4, and T7 also show equilibrium bands at partially denatured densities, some of which are highly asymmetric. Simple sequence satellite DNA shows an all-or-none transition with no equilibrium bands at partially denatured densities. The temperature at which a DNA denatures is an increasing function of the (G + C) content of the DNA. The T_m does not show a molecular-weight dependence in the range 1.2 × 10⁶–1.5 × 10⁷ daltons (single strand) for mouse, M. lysodeikticus, or T4 DNA. The mouse DNA partially denatured bands do not change shape as a function of molecular weight. The T4 DNA intermediate band develops a late-melting tail at low molecular weight. M. lysodeikticus DNA bands at partially denatured densities become broader as the molecular weight is decreased. Mouse DNA is resolved into six Gaussian components at each point in the melting transition.