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.     

Linker histone H1 per se can induce three-dimensional folding of chromatin fiber

Higher-order architectures of chromosomes play important roles in the regulation of genome functions. To understand the molecular mechanism of genome packing, an in vitro chromatin reconstitution method and a single-molecule imaging technique (atomic force microscopy) were combined. In 50 mM NaCl, well-stretched beads-on-a-string chromatin fiber was observed. However, in 100 mM NaCl, salt-induced interaction between nucleosomes caused partial aggregation. Addition of histone H1 promoted a further folding of the fiber into thicker fibers 20-30 nm in width. Micrococcal nuclease digestion of these thicker fibers produced an approximately 170 bp fragment of nucleosomal DNA, which was approximately 20 bp longer than in the absence of histone H1 ( approximately 150 bp), indicating that H1 is correctly placed at the linker region. The width of the fiber depended on the ionic strength. Widths of 20 nm in 50 mM NaCl became 30 nm as the ionic strength was changed to 100 mM. On the basis of these results, a flexible model of chromatin fiber formation was proposed, where the mode of the fiber compaction changes depending both on salt environment and linker histone H1. The biological significance of this property of the chromatin architecture will be apparent in the closed segments ( approximately 100 kb) between SAR/MAR regions.     

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.     

Structural transitions of chromatin at low salt concentrations: a flow linear dichroism study

We have studied the structure of nuclease-solubilized chromatin from Ehrlich ascites cells by flow linear dichroism (LD) using the anisotropic absorption of the DNA bases and of two intercalated dyes, ethidium bromide and methylene blue. It is confirmed that intercalation occurs preferentially in the linker part of the chromatin fiber, at binding ratios (dye/base) below 0.020. Using this information, we determined the orientation of the linker in relation to the average DNA organization in chromatin. The LD measurements indicate that the conformation of chromatin is considerably changed in the ionic strength interval 0.1-10 mM NaCl: with increasing salt concentration, the LD of the intrinsic DNA base absorption changes signs, from negative to positive, at approximately 2.5 mM NaCl. The LD of the intercalated dyes also changes signs, however, at a somewhat higher salt concentration. The results are analyzed in terms of possible allowed combinations of tilt angles of nucleosomes and pitch or tilt angles of linker DNA sections relative to the fiber axis, at different salt concentrations in the interval 0.1-10 mM NaCl. Two models for the salt-induced structural change of chromatin are discussed.     

Exchange of proteins during immunofractionation of chromatin

The migration and rearrangement of chromosomal proteins during immunofractionation of chromatin has been investigated. Oligonucleosomes from two different chromatins, chicken erythrocyte or rat liver, were mixed with oligonucleosomes from the other species which had been depleted of histones H1/H5 and high mobility group proteins (HMGs). The mixture was treated with buffers of various ionic strengths and immunofractionated on an anti-H1 degrees/H5 or anti-HMG-17 IgG-Sepharose column. The type of DNA, which was retained as the bound fraction on the column, was determined by slot blot analysis using nick-translated repetitive DNA probes from either chicken or rat. The results indicate that in low ionic strength buffers (i.e., below 40 mM NaCl), there is very little exchange of either histone H5 or HMG-17 among nucleosomes and therefore we suggest that it is possible to fractionate nucleosomes according to their antigenic content.     

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.     

Structure of the chromatin with long linker DNA

The method of velocity sedimentation have been used to investigate ionic-strength-induced compaction of sea urchin sperm chromatin characterized by extremely long linker DNA (100 b.p.). The dependence of sedimentation coefficients of oligonucleosomes on the number of nucleosomes in the chain have been studied in the range of ionic strength from 0.005 to 0.085. Analysis of these data indicates that such structural parameters of sea urchin sperm chromatin fibre as the diameter of the chain and the length of the chain per nucleosome are quite similar to those of chromatin with shorter linker DNA, but the DNA packing ratio is higher. The structure of sea urchin sperm oligonucleosomes agrees well with the model of three-dimensional zig-zag-shaped chain with linker DNA forming a loop. The possible role of alpha-helical regions of the C-terminal domain of sea urchin sperm histone H1 in the long linker DNA folding is discussed.     

Involvement of histone H1 in the organization of the nucleosome and of the salt-dependent superstructures of chromatin

We describe the results of a systematic study, using electron microscopy, of the effects of ionic strength on the morphology of chromatin and of H1-depleted chromatin. With increasing ionic strength, chromatin folds up progressively from a filament of nucleosomes at approximately 1 mM monovalent salt through some intermediate higher- order helical structures (Thoma, F., and T. Koller, 1977, Cell 12:101- 107) with a fairly constant pitch but increasing numbers of nucleosomes per turn, until finally at 60 mM (or else in approximately 0.3 mM Mg++) a thick fiber of 250 A diameter is formed, corresponding to a structurally well-organized but not perfectly regular superhelix or solenoid of pitch approximately 110 A as described by Finch and Klug (1976, Proc. Natl. Acad. Sci. U.S.A. 73:1897-1901). The numbers of nucleosomes per turn of the helical structures agree well with those which can be calculated from the light-scattering data of Campbell et al. (1978, Nucleic Acids Res. 5:1571-1580). H1-depleted chromatin also condenses with increasing ionic strength but not so densely as chromatin and not into a definite structure with a well-defined fiber direction. At very low ionic strengths, nucleosomes are present in chromatin but not in H1-depleted chromatin which has the form of an unravelled filament. At somewhat higher ionic strengths (greater than 5 mM triethanolamine chloride), nucleosomes are visible in both types of specimen but the fine details are different. In chromatin containing H1, the DNA enters and leaves the nucleosome on the same side but in chromatin depleted of H1 the entrance and exit points are much more random and more or less on opposite sides of the nucleosome. We conclude that H1 stabilizes the nucleosome and is located in the region of the exit and entry points of the DNA. This result is correlated with biochemical and x-ray crystallographic results on the internal structure of the nucleosome core to give a picture of a nucleosome in which H1 is bound to the unique region on a complete two-turn, 166 base pair particle (Fig. 15). In the formation of higher-order structures, these regions on neighboring nucleosomes come closer together so that an H1 polymer may be formed in the center of the superhelical structures.     

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.     

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.     

The structure of chromatin from the pigeon brain. II. Sedimentation analysis of oligonucleosome density

Compaction of pigeon brain and rat thymus chromatin differing in the length of the linker DNA has been studied by the method of velocity sedimentation. The dependence of sedimentation coefficients of oligonucleosomes on the number of nucleosomes in the chain in solution of different ionic strength (0.005-0.085) has been analyzed. The analyses of these dependences showed that the structure of oligonucleosomes of both cell types at low ionic conditions may be described by the model of a zig-zag-shaped nucleosomal chain. The process of compaction of the oligonucleosomes at higher ionic strength (0.045-0.085) proceeds similarly for brain and thymus chromatin. The formation of a superhelical structure is determined by the interaction of no less than 6 nucleosomes; the compactness of the structure is significantly increased when the number of nucleosomes in the chain exceeds 10. The ability of the brain oligonucleosomes to form a compact structure despite the short linker allow the suggestion that in brain short chromatin the DNA chain does not form two complete turns in the nucleosome. This provides necessary flexibility of brain chromatin.     

Daunomycin-induced unfolding and aggregation of chromatin.

Using equilibrium dialysis and sedimentation velocity analysis, we have characterized the binding of the anti-tumor drug daunomycin to chicken erythrocyte chromatin before and after depletion of linker histones and to its constitutive DNA under several ionic strengths (5, 25, and 75 mM NaCl). The equilibrium dialysis experiments reveal that the drug binds cooperatively to both the chromatin fractions and to the DNA counterpart within the range of ionic strength used in this study. A significant decrease in the binding affinity was observed at 75 mM NaCl. At any given salt concentration, daunomycin exhibits higher binding affinity for DNA than for linker histone-depleted chromatin or chromatin (in decreasing order). Binding of daunomycin to DNA does not significantly affect the sedimentation coefficient of the molecule. This is in contrast to binding to chromatin and to its linker histone-depleted counterpart. In these instances, preferential binding of the drug to the linker DNA regions induces an unfolding of the chromatin fiber that is followed by aggregation, presumably because of histone-DNA interfiber interactions.     

The effect of histone H1 on the compaction of oligonucleosomes. A quasielastic light scattering study

The structural properties of H1-depleted oligonucleosomes are investigated by the use of quasielastic laser light scattering, thermal denaturation and circular dichroism and compared to those of H1-containing oligomers. To obtain information on the role of histone H1 in compaction of nucleosomes, translational diffusion coefficients (D) are determined for mono-to octanucleosomes over a range of ionic strength. The linear dependences of D on the number of nucleosomes show that the conformation of stripped oligomers is very extended and does not change drastically with increasing the ionic strength while the rigidness of the chain decreases due to the folding of linker DNA. The results prove that the salt-induced condensation is much smaller for H1-depleted than for H1-containing oligomers and that histone H1 is necessary for the formation of a supercoiled structure of oligonucleosomes, already present at low ionic strength.     

Histone H1 can be removed selectively from chicken erythrocyte chromatin at near physiological conditions.

Histone H1 was depleted selectively from chicken erythrocyte polynucleosomes, without any detectable concomitant loss of H5 or core particle histones. The depletion is performed with ion exchange resin at low ionic strength (80 mM NaCl). The nucleosomes did not slide during the procedure. In contrast to the native chromatin, H1 depleted polynucleosomes are completely soluble in the 5--600 mM NaCl range.     

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.     

The effect of low ionic strength on the circular dichroic spectrum of chromatin and nucleosomal subunits

Circular dichroism has been used to measure the conformation changes in the DNA of chromatin and chromatin subunits as a function of ionic strength. Transfer of chromatin from 0.15 M to 0.25 mM salt led to an enhancement of the circular dichroic bands at 275 and 285 nm. Removal of histone H1 did not appreciably affect the circular dichroic spectrum when measured in 0.15 M salt, but in 0.25 mM salt H1 depletion led to a marked increase in the ellipticity. Conformation changes due to low ionic strength were also observed with a 145- and a 172-bp chromatin subunit. A linear combination of the ellipticities of the DNA of the two domains in chromatin, namely core and linker, was successful for measurements at 0.15 M salt, but large unexplained discrepancies appeared with the data from measurements in 0.25 mM salt.     

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.