Salt-induced conformational transitions in chromatin. A flow linear dichroism study

The chromatin structure in solution has been studied by the flow linear dichroism method (LD) in a wide range of ionic strengths. It is found that increasing the ionic strength from 0.25 mM Na2EDTA, pH 7.0 to 100 mM NaCl leads to a strong reduction of the LD amplitude of chromatin and inversion of the LD sign from negative to positive at 2 mM NaCl. Chromatin exhibits a positive LD maximum value at 10-20 mM NaCl. These data enable us to conclude that in very low ionic strength (0.25 mM Na2EDTA) the nucleosome discs are oriented with their flat faces more or less parallel to the chromatin filament axis. Increasing ionic strength up to 20 mM NaCl leads to reorientation of the nucleosome discs and to formation of chromatin structures with nucleosome flat faces inclined to the fibril axis. A conformational transition of that kind is not revealed in H1-depleted chromatin. The condensation of the chromatin filaments with increasing concentration of NaCl from 20 mM to 100 mM slightly influences the orientation of the nucleosomes.     

Chromatin structure. Further evidence against the existence of a beaded subunit for the 30-nm fiber

The size distribution of chromatin fragments released by micrococcal nuclease digestion of liver chromatin at various ionic strengths was examined. Below 20 mM ionic strength, gradient profiles with a peak centered at 6 nucleosomes are generated, whereas between 20 and 50 mM the peak is always centered on 12 nucleosomes, and above 50 mM ionic strength the 30-nm fiber becomes less accessible to the nuclease and there is a corresponding increase in the size distribution of fragments in the gradients. However, extensive digestions always give profiles with a peak of 12 nucleosomes as nuclease-resistant dodecamers accumulate. All of these observations are consistent with the winding of the 10-nm polynucleosome chain into a helical coil commencing at about 20 mM ionic strength. The helical turns are stabilized by histone H1 interactions between 20 and 50 mM ionic strength producing stable dodecamers. Above 50 mM ionic strength the coil condenses longitudinally and the profiles are consistent with a random attack of this fiber by the nuclease. Consequently it is not necessary to invoke the existence of a subunit bead to explain the profiles. We further define the conditions at which specific structural transitions take place and provide methodology for the preparation of chromatin at various levels of condensation.     

Chromatin structure. Evidence that the 30-nm fiber is a helical coil with 12 nucleosomes/turn

Sedimentation analysis has been used to compare the structure of 30-nm chromatin fibers, isolated and digested under conditions that maintain the native structure, with relaxed-refolded chromatin. The native chromatin fibers show sharp, ionic strength-dependent changes in sedimentation coefficient that are not apparent in relaxed-refolded fibers. The first transition at approximately 20 mM ionic strength reflects the organization of the 10-nm polynucleosome chain into a loose helically coiled 30-nm fiber. Between 20 and 60 mM ionic strength there is considerable interaction between nucleosomes within the coils to generate a stable helical array with 12 nucleosomes/turn. Above 60 mM ionic strength the helical coil continues to condense until it precipitates at ionic strengths slightly greater than those considered physiological, indicating that there is no end point in fiber formation. The data is incompatible with a solenoid model with 6 nucleosomes/turn and also rules out the existence of a beaded subunit structure.     

Synchrotron X-ray scattering study of chromatin condensation induced by monovalent salt: analysis of the small-angle scattering data

Small-angle X-ray scattering experiments were carried out on rat thymus chromatin in "native" and "H1-depleted" states at various NaCl concentrations using synchrotron radiation. From the analysis of cross-sectional Guinier plots, the radius of gyration of the cross section (Rc) and the mass per unit length (Mc) of native chromatin were evaluated. In the absence of NaCl, the cross section of chromatin filament has a radius of gyration of 3.44 nm, suggesting the structure corresponding to the "10 nm" filament. With increasing NaCl concentration, the Rc value increases steeply to 6.74 nm at 5 mM NaCl and then gradually to 8.82 nm at 50 mM NaCl, whereas the Mc value, which is determined relative to that of tobacco mosaic virus (TMV), increases steadily from 1.58 nucleosomes per 10 nm in the absence of NaCl to 7.66 nucleosomes per 10 nm at 50 mM NaCl. However, since calibration with TMV tends to overestimate the Mc value, the actual Mc values may be less than those values. Above about 40 mM NaCl, aggregation of chromatin is suggested. Similar analysis of H1-depleted chromatin confirmed that H1-depleted chromatin takes a more disordered structure than native chromatin at low ionic strength and does not undergo a definite structure change upon further addition of NaCl.     

Histone H5 promotes the association of condensed chromatin fragments to give pseudo-higher-order structures

We describe two distinct situations in which chicken erythrocyte chromatin fragments associate in solution. The erythrocyte-specific histone H5 is implicated since chromatins that do not contain H5 do not show this behaviour. Well-defined oligomers of between approximately 6 and approximately 18 nucleosomes prepared at low ionic strength condense and associate when the ionic strength is raised to 75 mM, forming pseudo-higher-order structures. The associated forms, probably predominantly dimers, are stabilized by migration of about 10% of the H5, and of the minor lysine-rich histone H1, from the non-associated forms, probably reflecting the preference of H5 for higher-order structures observed previously [Thomas, J. O. and Rees, C. (1983) Eur. J. Biochem. 134, 109-115]. Since the final (H1 + H5) content of the aggregate at 75 mM is never higher than that of the fragment prepared at low ionic strength, migration is probably to a small proportion of sites that have inevitably become vacant due to handling losses at the higher (but not at low) ionic strength. H5 thus maximizes its interactions in the condensed state of chromatin and even maintains the association of two or more fragments without continuity of the DNA. Aggregates of oligomers larger than about 18 nucleosomes may be too long to withstand hydrodynamic shear forces in the absence of such continuity. During nuclease digestion of nuclear chromatin, H5 and, to a lesser extent, H1, are released from the ends of very short fragments and bind to larger oligomers of various sizes leading to heterogeneous aggregates that survive exposure to low ionic strength. These aggregates, in contrast to those described above, have up to 60% more H5 and 20% more H1 than chromatin prepared at low ionic strength. Whether the excess H5 and H1 bind non-specifically or to a second low-affinity binding site on each nucleosome is not known. The associated forms described above (1) are well defined and potentially useful for structural studies, whereas the other aggregates (2) seem less likely to be directly relevant to the native structure of chromatin.     

Size-dependence of a stable higher-order structure of chromatin

We have recently reported a study of the formation of higher-order structures of chromatin with increasing ionic strength, in which we measured sedimentation coefficients of long nucleosome oligomers. We found that somewhere in the range of 30 to 60mer the sedimentation coefficient developed a jump of about 10% between ionic strengths of 45 mm and 55 mm, which persisted for larger oligomers (Butler & Thomas, 1980).This posed the question of whether the jump observed represented a greater relative compaction at high ionic strength on the part of long polymers, or a relatively lesser resistance to hydrodynamic shear forces at low ionic strength.We now define the dependence of the jump upon oligomer size in detail, the critical size being 50 nucleosomes. We also show that it occurs because the sedimentation of a large oligomer appears “slow” for its size at lower ionic strength, but “normal” at higher ionic strengths. We interpret this as the consequence of insufficient axial interaction to stabilize the helical coiling of long nucleosome filaments at low ionic strength, leading to a more open and slowly sedimenting structure.     

Organisation of subunits in chromatin.

There is considerable current interest in the organisation of nucleosomes in chromatin. A strong X-ray and neutron semi-meridional diffraction peak at approximately 10 nm had previously been attributed to the interparticle specing of a linear array of nucleosomes. This diffraction peak could also result from a close packed helical array of nucleosomes. A direct test of these proposals is whether the 10 nm peak is truly meridional as would be expected for a linear array of nucleosomes or is slightly off the meridian as expected for a helical array. Neutron diffraction studies of H1-depleted chromatin support the latter alternative. The 10 nm peak has maxima which form a cross-pattern with semi-meridional angle of 8 to 9 degrees. This is consistent with a coil of nucleosomes of pitch 10 nm and outer diameter of approximately 30 nm. These dimensions correspond to about six nucleosomes per turn of the coli.     

Reconstitution of chromatin higher-order structure from histone H5 and depleted chromatin

Reconstitution of the 30 nm filament of chromatin from pure histone H5 and chromatin depleted of H1 and H5 has been studied using small-angle neutron-scattering. We find that depleted, or stripped, chromatin is saturated by H5 at the same stoichiometry as that of linker histone in native chromatin. The structure and condensation behavior of fully reconstituted chromatin is indistinguishable from that of native chromatin. Both native and reconstituted chromatin condense continuously as a function of salt concentration, to reach a limiting structure that has a mass per unit length of 6.4 nucleosomes per 11 nm. Stripped chromatin at all ionic strengths appears to be a 10 nm filament, or a random coil of nucleosomes. In contrast, both native and reconstituted chromatin have a quite different structure, showing that H5 imposes a spatial correlation between neighboring nucleosomes even at low ionic strength. Our data also suggest that five to seven contiguous nucleosomes must have H5 bound in order to be able to form a higher-order structure.     

Unravelled nucleosomes,nucleosome beads and higher order structures of chromatin: Influence of non-histone components and histone H1

Effects of non-histone components and histone H1 on the morphology of nucleosomes and chromatin were studied by electron microscopy. Soluble rat liver ehromatin was depleted of non-histone components [NH]or non-histone components and H1 [NH and H1] by dissociation and subsequent fractionation in sucrose gradients in the presence of 300 to 350 mm or 500 mm-NaCl, respectively. In reconstitution experiments the depleted samples were mixed either with [NH] or with [NH and H1] or with purified H1. The morphology of the ionic strength-dependent condensation of the samples was monitored by electron microscopy using 0 mm to 100 mm-NaCl. Based on the appearance of the different types of fibres in very low salt (0 mm up to 10 mm-NaCl), namely the zigzag-shaped, the beads-on-a-string or the DNA-like filaments, it is possible to distinguish between nucleosomes, partially unravelled nucleosomes and unravelled nucleosomes, respectively. Only those fibres which were zigzag-shaped at low ionic strength condense at increasing ionic strength into higher order structures of compact fibres. We demonstrate the dependence of the appearance of nucleosomes and chromatin upon its composition and upon the ionic strength of the solvent.[NH] have no detectable influence upon the formation of higher order chromatin structures, but they can prevent the unravelling of nucleosomes at very low ionic strength, presumably by charge shielding.For the appearance of zigzag-shaped fibres and for the condensation into compact fibres with increasing ionic strength, H1 must be present in about native amounts. Partial removal of H1 (about 10%) promotes a change from fibres into tangles. This supports the model that an H1 polymer is stabilizing the higher order chromatin structures.Reconstitution experiments with purified H1 regenerated fibres containing all the features of [NH]-depleted chromatin. Reconstitution experiments with [NH and H1] promoted fibres compatible with control chromatin. Overloading of chromatin with H1 led to additional condensation. The detailed morphology of the reconstituted fibres showed local distortions. One possibility explaining these local distortions would be competition between “main” and “additional” binding sites for histone H1.     

Fractionation of nucleosomes by salt elution from micrococcal nuclease- digested nuclei

The solubilization of nucleosomes and histone H1 with increasing concentrations of NaCl has been investigated in rat liver nuclei that had been digested with micrococcal nuclease under conditions that did not substantially alter morphological properties with respect to differences in the extent of chromatin condensation. The pattern of nucleosome and H1 solubilization was gradual and noncoordinate and at least three different types of nucleosome packing interactions could be distinguished from the pattern. A class of nucleosomes containing 13-- 17% of the DNA and comprising the chromatin structures most available for micrococcal nuclease attack was eluted by 0.2 M NaCl. This fraction was solubilized with an acid-soluble protein of apparent molecular weight of 20,000 daltons and no histone H1. It differed from the nucleosomes released at higher NaCl concentrations in content of nonhistone chromosomal proteins. 40--60% of the nucleosomes were released by 0.3 M NaCl with 30% of the total nuclear histone H1 bound. The remaining nucleosomes and H1 were solublized by 0.4 M or 0.6 M NaCl. H1 was not nucleosome bound at these ionic strengths, and these fractions contained, respectively, 1.5 and 1.8 times more H1 per nucleosome than the population released by 0.3 M NaCl. These fractions contained the DNA least available for micrococcal nuclease attach. The strikingly different macromolecular composition, availability for nuclease digestion, and strength of the packing interactions of the nucleosomes released by 0.2 M NaCl suggest that this population is involved in a special function.     

Specific histone-histone contacts are ruptured when nucleosomes unfold at low ionic strength.

The ordered unfolding of the nucleosome core within chromatin at low ionic strengths has been studied. The results show that, when nuclei are lysed gently in solutions of very low ionic strength, their constituent nucleosomes rupture at a major H2B-H4 binding site but remain unperturbed at the site of the H2A-H2B interaction. These conclusions are based on data which show that at least four separate but closely spaced H2B-H4 contacts, identifiable by contact-site cross-linking in intact nuclei, are broken when nuclei are suspended in very dilute buffers. Appropriate controls on purified nucleosomes monomers demonstrate that the H2B-H4 contacts being broken are indeed intranucleosomal. Sedimentation of nucleosomes in the ultracentrifuge at various salt concentrations reveals that a significant conformational transition occurs in the range of ionic strength over which the H2B-H4 binding site ruptures.     

Effect of salt on the binding of the linker histone H1 to DNA and nucleosomes

The linker histones are involved in the salt-dependent folding of the nucleosomes into higher-order chromatin structures. To better understand the mechanism of action of these histones in chromatin, we studied the interactions of the linker histone H1 with DNA at various histone/DNA ratios and at different ionic strengths. In direct competition experiments, we have confirmed the binding of H1 to superhelical DNA in preference to linear or nicked circular DNA forms. We show that the electrophoretic mobility of the H1/supercoiled DNA complex decreases with increasing H1 concentrations and increases with ionic strengths. These results indicate that the interaction of the linker histone H1 with supercoiled DNA results in a soluble binding of H1 with DNA at low H1 or salt concentrations and aggregation at higher H1 concentrations. Moreover, we show that H1 dissociates from the DNA or nucleosomes at high salt concentrations. By the immobilized template pull-down assay, we confirm these data using the physiologically relevant nucleosome array template.     

Quantitative analysis of chromatin structure by circular dichroism

Quantitative analysis of the circular dichroism of nucleohistones and protein-free DNA was carried out in order to determine the structure and the role of the linker region DNA in chromatin, in terms of the conformational change of chromatin as a function of the ionic strength. It is shown clearly that the circular dichroism of Hl-depleted chromatin isolated from calf thymus is determined only by the ratio of the core region to the linker region and demonstrated by the linear combination of the spectrum of protein-free DNA and that of the nucleosome core in 5 mm-Tris · HCl, 1 mm-EDTA (pH 7.8). The calculated spectrum for the linker region in the H1-depleted chromatin was in good agreement with that of protein-free DNA. From the difference spectra between nucleohistones and protein-free DNA, it is suggested that the chromatin has an additional winding of DNA other than 146 base-pairs of DNA around the histone core. By decreasing the ionic strength to values lower than 5 mm-Tris · HCl, 1 mm-EDTA, the ellipticity of H1-depleted chromatin increased greatly between 250 nm and 300 nm while the increase was small in the case of chromatin and the nucleosome core. Nucleosomes with linker region DNA but without histone H1 also show great increase in ellipticity in this range of wavelengths as the ionic strength is decreased. Therefore, the linker region in H1-depleted chromatin plays an important role in the conformational changes brought about by changes in the ionic strength, and the conformational changes caused in the DNA of chromatin by decreasing the ionic strength are suppressed by the presence of histone H1.     

Thermal denaturation and fluorescence study of nucleosomes containing non-histone chromosomal protein HMG2

Interaction of calf thymus non-histone chromosomal protein HMG2 with H1,H5-depleted nucleosomes from chicken erythrocytes was studied by means of thermal denaturation and an N-(3-pyrene)maleimide fluorescence probe. Under low ionic conditions (2 mM Tris buffer plus EDTA) addition of 1-2 molecules of HMG2 per nucleosome markedly stabilized the segment of the linker DNA against thermal denaturation. Under approximately physiological ionic conditions (0.1 M NaCl) addition of two HMG2 molecules per nucleosome, labeled by N-(3-pyrene)maleimide at the sulfhydryl groups of Cys-110 of histones H3, resulted in a decrease of the pyrene excimer fluorescence corresponding to the slight movement of the sulfhydryl groups of the two histone H3 molecules apart.     

Stability of nucleosomes in native and reconstituted chromatins.

The stability of nucleosomes of SV40 minichromosomes extracted from infected cells or reconstituted by association of SV40 DNA and the four histones H2A, H2B, H3 and H4 was studied as a function of the ionic strength. As a measure of the stability of the nucleosome, we followed the disappearance of the nucleosomes from the original chromatin and their appearance on a "competing" DNA. We show here that the DNA and the histone components of the nucleosomes do not apprecially dissociate below 800 mM NaCl. At 800 mM and above, the histone moiety of the nucleosomes can dissociate from the DNA and efficiently participate to the formation of nucleosomes on a "competing" DNA.     

Nucleosomes are assembled into discrete size structures by histone H1 in vitro

The involvement of histone H1 in the formation and maintenance of higher order chromatin structures in vitro was investigated biochemically. Addition of exogenous histone H1 to isolated calf thymus mononucleosomes in low ionic strength buffer resulted in the formation of electrophoretically distinct mononucleosome assemblies (supernucleosomes). The smaller supernucleosomes were composed of about 12, 18, 24, or 30 nucleosomes and one to two molecules of histone H1 per nucleosome. It was difficult to determine accurately the size of the larger supernucleosomes, but their bands from native gels contained probably between 60 and 300 nucleosomes or more. Similar supernucleosome size classes were also obtained when oligonucleosomes instead of mononucleosomes were employed. When the assembly of mono- and oligo-nucleosomes with histone H1 took place in 0.15 M NaCl, discrete supernucleosomes containing only mono- or di-nucleosomes, but not a mixture of both, were formed. It is proposed that the small supernucleosomes containing oligomers of 6 nucleosomes may represent integral multiples of the second-order chromatin structural subunit, whereas the larger supernucleosomes containing about 60 to 300 or more nucleosomes may correspond to chromatin domains or third-order chromatin structures observed by other techniques.     

Nucleosome positioning in relation to nucleosome spacing and DNA sequence-specific binding of a protein

Nucleosome positioning is an important mechanism for the regulation of eukaryotic gene expression. Folding of the chromatin fiber can influence nucleosome positioning, whereas similar electrostatic mechanisms govern the nucleosome repeat length and chromatin fiber folding in vitro. The position of the nucleosomes is directed either by the DNA sequence or by the boundaries created due to the binding of certain trans-acting factors to their target sites in the DNA. Increasing ionic strength results in an increase in nucleosome spacing on the chromatin assembled by the S-190 extract of Drosophila embryos. In this study, a mutant lac repressor protein R3 was used to find the mechanisms of nucleosome positioning on a plasmid with three R3-binding sites. With increasing ionic strength in the presence of R3, the number of positioned nucleosomes in the chromatin decreased, whereas the internucleosomal spacings of the positioned nucleosomes in a single register did not change. The number of the positioned nucleosomes in the chromatin assembled in vitro over different plasmid DNAs with 1-3 lac operators changed with the relative position and number of the R3-binding sites. We found that in the presence of R3, nucleosomes were positioned in the salt gradient method of the chromatin assembly, even in the absence of a nucleosome-positioning sequence. Our results show that nucleosome-positioning mechanisms are dominant, as the nucleosomes can be positioned even in the absence of regular spacing mechanisms. The protein-generated boundaries are more effective when more than one binding site is present with a minimum distance of approximately 165 bp, greater than the nucleosome core DNA length, between them.     

DNase I digestion reveals alternating asymmetrical protection of the nucleosome by the higher order chromatin structure

DNase I was used to probe the higher order chromatin structure in whole nuclei. The digestion profiles obtained were the result of single-stranded cuts and were independent of pH, type of divalent ion and chromatin repeat length. Furthermore, the protection from digestion of the DNA at the entry/exit points on the nucleosome was found to be caused not by the H1/H5 histone tails, but by the compact structure that these proteins support. In order to resolve symmetry ambiguities, DNase I digestion fragments over several nucleosome repeat lengths were analysed quantitatively and compared with computer simulations using combinations of the experimentally obtained rate constants (some of which were converted to 0 to simulate steric protection from DNase I digestion). A clear picture of precisely defined, alternating, asymmetrically protected nucleosomes emerged. The linker DNA is inside the fibre, while the nucleosomes are positioned above and below a helical path and/or with alternating orientation towards the dyad axis. The dinucleosomal modulation of the digestion patterns comes from alternate protection of cutting sites inside the nucleosome and not from alternating exposure to the enzyme of the linker DNA.