Comparative study of the condensation of chicken erythrocyte and calf thymus chromatins by di- and multivalent cations

The condensation of chicken erythrocyte (CE) and calf thymus (CT) chromatins upon addition of di- and multivalent cations has been studied using turbidity, precipitation and electric dichroism measurements. For all the cations investigated (Mg2+, Tb3+, Co(NH3)6(3+), spermidine Spd2+ and spermine Sp4+) condensation of CE chromatin occurred before the onset of aggregation, while aggregation of CT chromatin started before condensation with all cations except Mg2+ and Tb3+. Precipitation of CE chromatin required lower di- and multivalent cations concentrations than CT chromatin. The electric dichroism data for both chromatins, at low ionic strength in the absence of di- or multivalent cations, indicated that the nucleoprotein molecules were not totally decondensed but that a "precondensed" state was already present. A positive electric dichroism was observed for the most condensed chromatin fibers, in agreement with the "cross-linker" models. Tb3+ led to less compact condensed particles as judged from the electric dichroism observations, but electron microscopy revealed that "30 nm fibers" were formed. Very little aggregation was produced by Tb3+. On the contrary, spermine produced very large networks of condensed molecules, but large spheroidal particles were also observed. The condensation of CE chromatin happened without changes of solution conductivity upon cation salt addition, regardless of the condensing cation, indicating a cooperative uptake of the ions during this process.     

Condensation of chromatin: role of multivalent cations

We have used electric dichroism to investigate the influence of multivalent cations upon the compaction of chicken erythrocyte chromatin from the unfolded, 10-nm fiber to the 30-nm solenoid and subsequent aggregation. The pattern of condensation, which consists of compaction plus aggregation, is found to be strikingly similar for a variety of cations of differing charge, including the physiologically important polyamines spermine and spermidine. With a few exceptions such as Cu2+ and Gd3+, an optimally compacted fiber with reproducible hydrodynamic properties is produced prior to the onset of aggregation. We report the concentrations of di-, tri-, and tetravalent cations required for optimal condensation; in addition, for tri- and tetravalent cations, we were able to estimate the extent of charge neutralization produced by their binding to the optimally compacted fiber. The results show that the multivalent ion concentration required for optimal compaction decreases as cationic charge increases. In addition, the effect of a mixture of dilute mono- and multivalent cations on chromatin condensation is synergistic, rather than competitive as has been found for the multivalent cation induced condensation of DNA or the B----Z conformational transition. A simple calculation indicates that the entropy of ion uptake in chromatin condensation is surprisingly constant for a range of ionic conditions; this factor may be a dominant one in determining the folding equilibrium.     

Electric and Flow Linear Dichroism of Unfolded and Condensed Chromatin: A Comparative Study at Low and Intermediate Ionic Strength

Abstract

Identical samples containing polynucleosomal chains of chicken erythrocyte (CE) and Ehrlich ascites tumour (EA) chromatin were studied under various ionic conditions with regard to electric linear dichroism (ELD) and flow linear dichroism (FLD). Both orientation techniques consistently confirmed that, in the limit of very low ionic strength and in the absence of multivalent cations, the reduced linear dichroism of chromatin is negative in the DNA-base absorption band, as expected for an extended zig-zag polynucleosomal conformation. With increasing electrolyte content, both ELD and FLD decreased drastically in amplitude, but in contrast to the ELD which remains negative in an intermediate range of low ionic strength (0.1–0.5 mM Mg²⁺) the FLD changes sign and becomes positive. The ELD and FLD amplitudes decrease with higher Mg²⁺ concentrations and FLD even vanishes in the region of 0.2–0.4 mM; both signals are positive above 0.4–0.5 mM Mg²⁺.

The origin of the dissimilarities between ELD and FLD observations is still not fully understood. Several possibilities are considered: ELD signals are more influenced than FLD by the presence of short chromatin chains, nucleosomes and small pieces of naked DNA, while FLD is more susceptible to the presence of large, easily orientable, scattering aggregates. Different preferred orientation directions of the chromatin fibre with respect to electric and hydrodynamic fields may also be involved. Finally, FLD and ELD probably “see” different features of the chromatin structure.     

Interplay of ion binding and attraction in DNA condensed by multivalent cations

We have measured forces generated by multivalent cation-induced DNA condensation using single-molecule magnetic tweezers. In the presence of cobalt hexammine, spermidine, or spermine, stretched DNA exhibits an abrupt configurational change from extended to condensed. This occurs at a well-defined condensation force that is nearly equal to the condensation free energy per unit length. The multivalent cation concentration dependence for this condensation force gives the apparent number of multivalent cations that bind DNA upon condensation. The measurements show that the lower critical concentration for cobalt hexammine as compared to spermidine is due to a difference in ion binding, not a difference in the electrostatic energy of the condensed state as previously thought. We also show that the resolubilization of condensed DNA can be described using a traditional Manning–Oosawa cation adsorption model, provided that cation–anion pairing at high electrolyte concentrations is taken into account. Neither overcharging nor significant alterations in the condensed state are required to describe the resolubilization of condensed DNA. The same model also describes the spermidine³⁺/Na⁺ phase diagram measured previously.     

The superstructure of chromatin and its condensation mechanism

Comparison between the internucleosomal distance found by X-ray solution scattering for chicken erythrocyte (23 nm) and sea urchin (30 nm) chromatin indicates that this distance is proportional to the linker length. The diameter of the condensed sea urchin chromatin fibers is about 45 nm which is significantly larger than in chicken erythrocyte chromatin (35 nm). Trivalent cations (Gd, Tb, Cr) and the polyamines spermine and spermidine were found to induce compaction at much lower concentrations than the divalent cations but Gd, Tb and Cr induce aggregation before full compaction of the fibers. The influence of hydrogen bonding is illustrated by comparison of the effects of NaCl, ammonium chloride and alkylammonium chlorides on condensation. Solubility experiments indicate that there is a nearly linear dependence of the Mg^-- concentration at which precipitation occures on chromatin concentration and confirm the differences between cations observed by X-ray scattering.The chicken erythrocyte chromatin samples were further characterized by their reduced electric dichroism. The values found are consistent with the model derived from X-ray scattering and are compared with those reported in the literature.     

Inhibition of cation-induced DNA condensation by intercalating dyes

Several intercalating dyes are shown to inhibit the cation-induced condensation of λ-DNA when Co³⁺(NH₃)₆ is the condensing agent. The dyes that have been studied are ethidium, propidium, proflavin, quinacrine, and actinomycin D. Earlier work has shown that intercalating dyes inhibit ψ-DNA condensation. [Lerman, L. S. (1971) Prog. Mol. Subcell. Biol. 2 , 382–391; Cheng, S. & Mohr, S. C. (1975) Biopolymers 14 , 663–674.] Dye-induced decondensation of intramolecularly condensed DNA has been studied by making use of conditions in which Co³⁺(NH₃)₆ produces intramolecular condensation without significant aggregation. Some aggregation is caused, however, during dye-induced decondensation. Dye titration curves of DNA decondensation have been measured by excess light scattering to monitor decondensation and by fluorescence to monitor intercalation. All of the dyes studied act as competing cations in displacing the condensing cation Co³⁺(NH₃)₆ from the DNA. Competition occurs both in and below the transition zone for condensation. The effectiveness of a dye as a competing cation increases with its net positive charge. Before decondensation begins, no intercalated dye can be detected, suggesting that intercalation might be incompatible with the proper helix packing needed for cation-induced DNA condensation. To test this last point, methidium–spermine was synthesized: it contains an intercalating methidium head group combined with a polyamine tail. Methidium–spermine is found to cause λ-DNA condensation, but aggregation accompanies condensation, as has been found earlier for spermine and spermidine. Fluorescence and absorption spectra indicate that the methidium group is intercalated when the DNA is condensed, indicating that intercalation need not be incompatible with DNA condensation. The presence of aggregates among the condensed DNA molecules makes this last conclusion tentative.     

Optical Anisotropy of Chromatin. Flow Linear Dichroism and Electric Dichroism Studies

Abstract

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentraitons by the use of flow linear dichroism (LD) and electric dichroism.

We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA—2 mM NaCl and close positive values in the range of 2–100 mM NaCl. Mg²⁺ cations, in contrast to Na⁺ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5–10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers.

The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA—for chromatins with the linker DNA of 10–30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible.

Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin.

Presented resutls explain the contradictory data obtained by electrooptical and hydrooptical methods.     

Erratum

Abstract

The condensation and the precipitation of rat liver chromatin upon addition of spermine⁴⁺, spermidine³⁺, hexamminecobalt(III)³⁺ and Mg²⁺ cations have been studied using solubility, fluorescence, circular dichroism, melting curves, electric dichroism and spermidine binding measurements, made on both soluble and precipitated complexes. The soluble complexes obtained with tetra- and trivalent cations were depleted from all histones and enriched in other proteins, particularly high mobility group proteins 1 and 2, which brings about an important enhancement of tryptophan fluorescence without modification of its two lifetimes 5.1 and 1.2 ns. In the precipitates the non-histone proteins are eliminated. Under precipitation by Mg²⁺ ions, the distribution of proteins remains practically unchanged. The electric dichroism and the melting curves indicate that the soluble complexes between polyamines and chromatin undergo important condensation and, at high ratios of cation over phosphate, are constituted by heterogeneous assemblies of non-histone proteins and DNA. On the contrary, the insoluble complexes seem to retain the main features of original chromatin. Precipitation by Mg²⁺ ions reveal much less drastic changes than those produced by polyamines. Precipitation by spermidine occurs when one cation is bound per eight nucleotides, which in addition to the histone positive charges brings about a complete neutralization of chromatin phosphates.     

The condensation of chromatin and histone H1-depleted chromatin by spermine

At low ionic strength, spermine induces aggregation of native and H1-depleted chromatin at spermine/phosphate (Sp/P) ratios of 0.15 and 0.3, respectively. Physico-chemical methods (electric dichroism, circular dichroism and thermal denaturation) show that spermine, at Sp/P less than 0.15, does not appreciably alter the conformation of native chromatin and interacts unspecifically with all parts of chromatin DNA (linker as well as regions slightly or tightly bound to histones). In chromatin, the role of spermine could be more important in the stabilization of higher-order structure than in the condensation of the 30 nm solenoid. The addition of spermine to H1-depleted chromatin revealed two important features: (i) spermine can partially mimic the role of histone H1 in the condensation of chromatin; (ii) the core histone octamer does not appear to play any role in the aggregation process by spermine as DNA and H1-depleted chromatin aggregate at the same Sp/P ratio.     

Condensation and precipitation of chromatin by multivalent cations

The condensation and the precipitation of rat liver chromatin upon addition of spermine4+, spermidine3+, hexamminecobalt(III)3+ and Mg2+ cations have been studied using solubility, fluorescence, circular dichroism, melting curves, electric dichroism and spermidine binding measurements, made on both soluble and precipitated complexes. The soluble complexes obtained with tetra- and trivalent cations were depleted from all histones and enriched in other proteins, particularly high mobility group proteins 1 and 2, which brings about an important enhancement of tryptophan fluorescence without modification of its two lifetimes 5.1 and 1.2 ns. In the precipitates the non-histone proteins are eliminated. Under precipitation by Mg2+ ions, the distribution of proteins remains practically unchanged. The electric dichroism and the melting curves indicate that the soluble complexes between polyamines and chromatin undergo important condensation and, at high ratios of cation over phosphate, are constituted by heterogeneous assemblies of non-histone proteins and DNA. On the contrary, the insoluble complexes seem to retain the main features of original chromatin. Precipitation by Mg2+ ions reveal much less drastic changes than those produced by polyamines. Precipitation by spermidine occurs when one cation is bound per eight nucleotides, which in addition to the histone positive charges brings about a complete neutralization of chromatin phosphates.     

Redistribution of Terbium Ions Across Acetylcholine Receptor-Enriched Membranes Induced by Agonist Desensitization

Using small-angle x-ray diffraction from centrifugally oriented acetylcholine receptor (AChR) enriched membranes coupled with anomalous scattering from terbium ions (Tb³⁺) titrated into presumed Ca²⁺ binding sites, we have mapped the distribution of Tb³⁺ perpendicular to the membrane plane using a heavy atom refinement algorithm. We have compared the distribution of Tb³⁺ in the closed resting state with that in the carbamylcholine-desensitized state. In the closed resting state we find 45 Tb³⁺ ions distributed in 10 narrow peaks perpendicular to the membrane plane. Applying the same refinement procedure to the data from carbamylcholine desensitized AChR we find 18 fewer Tb³⁺ ions in eight peaks, and slight rearrangements of Tb³⁺ density in the peaks near the ends of the AChR ion channel pore. These agonist dependent changes in the Tb³⁺ stoichiometry and distribution suggest a likely role for multivalent cations in stabilizing the different functional states of the AChR, and the changes in the Tb³⁺ distribution at the two ends of the pore suggest a potential role for multivalent cations in the gating of the ion channel.     

Effect of Glycine on DNA Structural Transitions Induced by Multivalent Cationic Compounds

Abstract

We have investigated the effect of glycine (an organic osmolyte) on several DNA transitions induced by Tb³⁺, spermidine³⁺ and spermine⁴⁺ addition, using light scattering, circular dichroism, UV spectroscopy and electric linear dichroism techniques.

DNA condensation and B-Z transition by the three compounds is perturbed by glycine: more Tb-¹⁺, spermidine³⁺ and spermine⁴⁺ must be added to obtain the same extent of condensation or Z-form as compared to the behaviour in the absence of this organic osmolyte. However, according to the light scattering experiments, glycine has also a structural effect on the DNA condensation that could be explained by an influence of the medium dielectric constant on the morphology of particles formed or on the rate of the condensation process.

Contrary to these transitions, the particular B-B'-ψ transition resulting from the addition of Tb³⁺ to a DNA solution is not observed in the presence of glycine. Since the chelation of Tb³⁺ by the phosphate group and the N-7 of guanine is presumably responsible for this transition, the glycine effect could probably be explained by a perturbation of this chelation by the change in solvent polarity and the chelating ability of the organic osmolyte.     

Monomolecular condensation of lambda-DNA induced by cobalt hexamine

Measurements of static and dynamic light scattering have been used to distinguish between monomolecular DNA condensation and aggregation of condensed molecules. In low salt, using Co³⁺(NH₃)₆ as the condensing agent, and at λ-DNA concentrations below 0.2 μg/mL, the transition curves for monomolecular condensation and aggregation are well separated for times of 16 h. In these conditions, the intensity of scattered light (90°) and also the diffusion coefficient of the condensed DNA show reasonable values for monomolecular condensation that are independent of DNA concentration and also of Na⁺ Co³⁺(NH₃)₆ concentrations for which monomolecular condensation is complete. At higher Co³⁺(NH₃)₆ concentrations, which produce aggregation (as judged by the intensity of scattered light), the diffusion coefficient decreases sharply. The transition curve for monomolecular condensation is independent of DNA concentration but shows a hysteresis loop. The kinetics of condensation are slow in the forward direction and fast in the reverse direction, indicating that the actual transition curve is measured closely by reversal experiments. Aggregation is blocked kinetically in both the forward and reverse directions when Co³⁺(NH₃)₆ is the condensing agent at low Na⁺ concentrations. When spermine or spermidine is the condensing agent and observations are made at 16 h, it is not possible to separate the transition curves for monomolecular condensation and for aggregation in conditions that are successful with Co³⁺(NH₃)₆. Some interesting properties of monomolecular condensation are noted. (1) The transition is not a two-state reaction, as judged by measurements of the diffusion coefficient through the transition zone. (2) The transition for monomolecular condensation is diffuse. (3) The dimensions of the monomolecular condensates have been calculated from the translational diffusion coefficient for an assumed toroidal shape by the formula derived by Allison and coworkers [(1981) Biopolymers 20 , 469–488]. These dimensions are in reasonable agreement with ones deduced from electron microscopy by Chattoraj and coworkers [(1978) J. Mol. Biol. 121 , 327–337]. (4) The phase diagram relating the Na⁺ to the Co³⁺(NH₃)₆ concentrations needed for condensation has a slope of 0.6 in a log–log plot. According to numerical solutions of Manning's theory for the atmospheric binding of competing cations to DNA, this means that condensation occurs at a late stage in the replacement of Na⁺ by Co³⁺(NH₃)₆ around the DNA. The fraction of DNA phosphate charge neutralized at condensation is computed to be in the neighborhood of 0.9, as found by Wilson and Bloomfield [(1979) Biochemistry 18 , 2192–2196], but to vary with the Na⁺ concentration.     

Onset of DNA aggregation in presence of monovalent and multivalent counterions

We address theoretically aggregation of DNA segments by multivalent polyamines such as spermine and spermidine. In experiments, the aggregation occurs above a certain threshold concentration of multivalent ions. We demonstrate that the dependence of this threshold on the concentration of DNA has a simple form. When the DNA concentration c(DNA) is smaller than the monovalent salt concentration, the threshold multivalent ion concentration depends linearly on c(DNA), having the form alphac(DNA) + beta. The coefficients alpha and beta are related to the density profile of multivalent counterions around isolated DNA chains, at the onset of their aggregation. This analysis agrees extremely well with recent detailed measurements on DNA aggregation in the presence of spermine. From the fit to the experimental data, the number of condensed multivalent counterions per DNA chain can be deduced. A few other conclusions can then be reached: 1), the number of condensed spermine ions at the onset of aggregation decreases with the addition of monovalent salt; 2), the Poisson-Boltzmann theory overestimates the number of condensed multivalent ions at high monovalent salt concentrations; and 3), our analysis of the data indicates that the DNA charge is not overcompensated by spermine at the onset of aggregation.     

Polyamine-DNA interactions. Condensation of chromatin and naked DNA

We have used flow linear dichroism (LD) and light scattering at 90 degrees to study the condensation of both DNA and calf thymus chromatin by polyamines, such as spermine, spermidine and its analogs designated by formula NH3+(CH2)iNH2+(CH2)jNH3+, where i = 2,3 and j = 2,3, putrescine, cadaverine and MgCl2. It has been found that the different polyamines affect DNA and chromatin in a similar way. The level of compaction of the chromatin fibers induced by spermine, spermidine and the triamines NH3+(CH2)3NH2+(CH2)3NH3+ and NH3+(CH2)3NH2+(CH2)2NH3+ and MgCl2 is found to be identical. The triamine NH3+(CH2)3NH2+(CH2)2NH3+ and the diamines studied condense neither chromatin nor DNA. This drastic difference in the action of the triamines indicates that not only the charge, but also the structure of the polycations might play essential roles in their interactions with DNA and chromatin. It is shown that a mixture of mono- and multivalent cations affect DNA and chromatin condensation competitively, but not synergistically, as claimed in a recent report by Sen and Crothers (Biochemistry 25, 1495-1503, 1986). We have also estimated the extent of negative charge neutralization produced by some of the polyamines on their binding to chromatin fibers. The stoichiometry of polyamine binding at which condensation of chromatin is completed is found to be two polyamine molecules per DNA turn. The extent of neutralization of the DNA phosphates by the histones in these compact fibers is estimated to be about 55%. The model of polyamine interaction with chromatin is discussed.     

Linear dichroism of chromatin fibers

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Friend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations by the use of flow linear dichroism and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA--2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA--for chromatins with linker DNA 10-30 b.p. it is partially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric fields do not have an effect on chromatin structure, while higher electric fields (more than 7 kV/cm) distort the structure of chromatin.     

Polyamine addition to preparation media induces chromatin condensation, irreversibly at low ionic strength

Polyamines (spermine, spermidine) are commonly used as stabilizing cations in the chromatin preparation media. Their residual binding to chromatin is not easily reversed at low ionic strength, even after extensive dialysis, as evidenced by the use of labelled spermidine. Electric dichroism measurements show that their presence interferes with the physico-chemical characterization of chromatin by maintaining a condensed structure. These results give a definite answer to the controversy about the sign of optical anisotropy of chromatin determined by electric and flow dichroism techniques.     

Optical anisotropy of chromatin. Flow linear dichroism and electric dichroism studies

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentrations by the use of flow linear dichroism (LD) and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA - 2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA - for chromatins with the linker DNA of 10-30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin. Presented results explain the contradictory data obtained by electrooptical and hydrooptical methods.     

Interaction of polyamines with chromatin and DNA: formation of compact structures

We have used flow linear dichroism (LD) and light scattering at 90 degrees to study the condensation of both DNA and calf thymus chromatin induced by spermine, triamines NH3+(CH2)iNH+(CH2)jNH3+, designated as much less than i, j much greater than: much less than 3, 4 much greater than (spermidine), much less than 3, 3 much greater than, much less than 2, 3 much greater than, much less than 2, 2 much greater than; the diamines putrescine and cadaverine and MgCl2. It is found that the different polyamines affected DNA and chromatin in a similar way. The degree of compaction of the chromatin fibers induced by spermine, triamines except much less than 2, 2 much greater than and Mg2+ has been found to be identical. The triamine much less than 2, 2 much greater than and the diamines studied do not condense either chromatin of DNA. Such a big difference in the action of the triamines indicates that not only the charge, but also the structure of the polycations are important for their interactions with DNA and chromatin. The stoichiometry of polyamine binding to chromatin at which condensation occurred is found to be 2 polyamine molecules per DNA helical turn. Polyamines are supposed to bind to the exposed sites of core DNA every 10 b.p. The extent of DNA phosphate neutralization by the histones is estimated to be about 55%. It has been shown that a mixture of mono- and multivalent cations affected DNA and chromatin condensation competitively and not synergistically, as claimed in a recent report by Sen and Crothers.     

Denaturation level of DNA-Pt complexes evidenced by Tb3+ fluorescence enhancement and electric dichroism

The Tb³⁺ fluorescence is greatly enhanced, as a result of binding of various platinum coordination complexes to DNA, as compared to native DNA. The largest enhancement is observed for cis-Pt(NH₃)₂Cl₂ but the fluorescence intensity does not however reach the level attained for thermally denatured DNA. Diethylenetriamine-Pt(II) produces very little increase of Tb³⁺ fluorescence. The electric dichroism in the DNA absorption band drastically decreases upon binding of the various Pt compounds investigated except diethylenetriamine-Pt. The results are discussed in terms of the various modes of binding of Pt derivatives to DNA, particularly in relation to the level of denaturation of the double helix.