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.     

The involvement of histone H1[0] in chromatin structure.

Micrococcal nuclease digestion and light scattering are used to compare native chromatins with various histone H1[0] contents. The experimental data show that the higher the H1[0] content, the greater the ability to form compact structures with increasing ionic strength, and the lower the DNA accessibility to micrococcal nuclease. On the contrary, reconstituted samples from H1-depleted chromatin and pure individual H1 fractions behave in such a way that samples reconstituted with pure H1 degree give rise to a looser structure, more accessible to nuclease than samples reconstituted with H1-1. This contradiction suggests that the effect of H1o on chromatin structure must originate from the interaction of this histone with other components in native chromatin among which other histone H1 subfractions are good candidates.     

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.     

The structural role of histone H1: properties of reconstituted chromatin with various H1 subfractions (H1-1, H1-2, and H1o).

A previous study on the distribution of histone H1 subfractions in chromatin suggested that these proteins differ in the protection they confer to DNA. To elucidate further this suggestion, reconstitution experiments were carried out with purified H1 subfractions (H1-1, H1-2, H1o) and H1-depleted chromatin. We have studied the structural properties of H1o as compared to those of other H1 fractions by electrophoretic analysis of DNA and mononucleosomes obtained after micrococcal nuclease digestion, thermal denaturation, and electron microscopy. The three fractions studied reassociate to H1-depleted chromatin. However, differences in the extent of DNA protection are observed between H1o and the other fractions: H1o induces a more rapid degradation of long oligomers into mononucleosomes; these mononucleosomes bearing H1o only, have a greater electrophoretic mobility; furthermore, thermal denaturation shows that a small fraction of DNA is less efficiently protected by H1o than by the other fractions. Electron microscopy, on the other hand, shows that these differences are not due to areas of chromatin devoid of H1o in the reconstitute and that the reconstituted samples are able, under proper ionic conditions, to refold in a higher-order structure.     

Influence of linker histone H1 on chromatin remodeling.

Chromatin-remodeling complexes have been a central area of focus for research dealing with accessing cellular DNA sequestered in chromatin. Although the linker histone H1 plays a major role in promoting and maintaining higher-order chromatin structure, it has been noticeably absent from assays utilizing chromatin-remodeling enzymes. This review focuses on two ATP-dependent chromatin-remodeling complexes, Drosophila ISWI and mammalian SWI/SNF, that have been assayed using chromatin templates containing histone H1.     

Asymmetry of chromatin subunits probed with histone H1 in an H1-DNA complex

Treatment of nucleosomes with a low concentration of sodium dodecyl sulfate removed all proteins except histone H1 from DNA, thus confirming our previous observation on sheared chromatin. No redistribution of H1 occurred during this procedure for isolation of the H1-DNA complex. The H1-DNA complex was isolated from a nucleosome monomer, doubly labeled in its protein and DNA and fractionated according to the length of DNA, and then the distribution of H1 was analyzed quantitatively. The results indicated that the monomer consisted of two subspecies, one containing 160 base pairs of DNA and one molecule of H1, and the other containing 140 base pairs of DNA and no H1. Since no monomer with two molecules of H1 was found, it is concluded that the nucleosome core has a binding site for H1 on only one side, and thus that the nucleosome is not a dyad.     

Psoralen-crosslinking of soluble and of H1-depleted soluble rat liver chromatin

We purified soluble rat liver chromatin and H1-depleted chromatin and photocrosslinked its DNA with psoralen at pH 7. Digestion of this chromatin with micrococcal nuclease produced a normal nucleosomal repeat. Chromatin was photoreacted in the presence of 0 to 700 mM-NaCl and was fractionated in sucrose gradients containing the same NaCl concentrations. The dissociation of H1 occurred as in the non-crosslinked controls and no preferential dissociation of core histones was observed. The samples between 100 and 500 mM-NaCl showed precipitation. In the electron microscope, the fibers appeared indistinguishable from the controls at low ionic strength. In the presence of 40 mM-NaCl, the fibers of the photoreacted chromatin were slightly more compact than the controls, and at 500 mM-NaCl, despite the complete dissociation of H1, there were still apparently intact fibers at this ionic strength. The disruption of the psoralen-treated chromatin fibers occurred only in 600 mM-NaCl, as opposed to 500 mM-NaCl in controls. The DNA of all the photoreacted samples was spread for electron microscopy under denaturing conditions. They revealed, for all the samples, single-stranded bubbles corresponding to 200 to 400 base-pairs in size. H1-depleted chromatin containing stoichiometric amounts of core histones was photoreacted at pH 10 and very low ionic strength. Under these conditions many of the nucleosomes appeared to be unraveled, although to a variable extent. In the electron microscope, the purified DNA from these samples showed extensive crosslinking when spread under denaturing conditions. These observations show that histone-DNA interactions different from those in intact nucleosomes may be created, which allow extensive access of psoralen to the DNA.     

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 structure and dynamics of H1-depleted chromatin

The size of DNA involved in the interaction with a histone octamer in H1-depleted chromatin was re-examined. We compared the thermal untwisting of chromatin DNA and naked DNA using CD and electrophoretic topoisomer analysis, and found that DNA of 175 +/- 10 base pairs (bp) in length interacted with the histone core under physiological conditions. The decrease of ionic strength below 20 mM NaCl reduced this length down to 145 bp: apparently, an extra 30 bp DNA dissociated from the histone core to yield well-known 145-bp core particle. Histone cores partly dissociate within the temperature range of 25 to 40 degrees C. Quantitative analysis of histone thermal dissociation from DNA shows that the size of DNA protected against thermal untwisting would be significantly overestimated if this effect is neglected. The results presented in this paper also suggest that the dimers (H2A, H2B) act as a lock, which prevents transmission of conformational alterations from a linker to nucleosome core DNA. The histone core dissociation as well as (H2A, H2B) dimer displacement are discussed in the light of their possible participation in the eukaryotic genome activation.     

Histone H1: Ultracentrifugation studies of the effects of ionic strength and denaturants on the solution conformation

The conformation of histone H1 has been examined under native and denaturing conditions in the absence of DNA or chromatin. Sedimentation coefficients were determined for Histone H1 in 0.1 m KCl and in 6 m guanidine hydrochloride solutions at pH 7.4. The influence of ionic strength on the conformation of histone H1 has been determined by measurement of the sedimentation coefficient in tetramethylammonium chloride solutions of up to 2.5 m and extrapolated to infinite ionic strength. Results from these experiments suggest that the native conformation of histone H1 is very asymmetric in shape. The molecule is best described as a prolate ellipsoid with axes of 312 Å (2a) and 16 Å (2b) in low ionic strength media and also as a prolate ellipsoid with axes of 202 Å (2a) and 20 Å (2b) at high ionic strength or when associated with polyanions, e.g., DNA. Denaturation of histone H1 by guanidine hydrochloride was found to be completely reversible. In 6 m guanidine hydrochloride, the H1 molecule collapses to a sphere but the original extended conformation of the protein is readily restored on dialysis. This suggests rigid conformational requirements for the H1 molecule as incorporated into chromatin. The shape and dimensions for the H1 molecule at high ionic strength are not sufficiently conclusive to locate H1 in the chromatin structure. It is proposed, however, that viable models for chromatin architecture must be consistent with the histone H1 solution dimensions obtained here.     

Specific interaction of histone H1 with eukaryotic DNA.

The interaction of calf thymus histone H1 with homologous and heterologous DNA has been studied at different ionic strengths. It has been found that about 0.5 M NaCl histone H1, and its fragments N-H1 (residues 1-72) and C-H1 (residues 73-C terminal), precipitate selectively a small fraction of calf thymus DNA. This selective precipitation is preserved up to very high values (less than 2.0) of the input histone H1/DNA ratio. The percentage of DNA insolubilized by histone H1 under these ionic conditions is dependent upon the molecular weight of the nucleic acid, diminishing from 18% fro a Mw equals 1.0 x 10(7) daltons to 5% for a Mw equals 8.0 x 10(4) daltons. The base composition of the precipitated DNA is similar to that of the bulk DNA. Calf thymus histone H1 also selectively precipitates a fraction of DNA from other eukaryotes (herring, trout), but not from some prokaryotes (E. coli, phage gamma. On the other hand, at 0.5 M NaCl, the whole calf thymus DNA (but not E. coli DNA) presents a limited number of binding sites for histone H1, the saturation ratio histone H1 bound/total DNA being similar to that found in chromatin. A similar behavior is observed from the histone H1 fragments, N-H1 and C-H1, which bind to DNA in complementary saturation ratios. It is suggested that in eukaryotic organisms histone H1 molecules maintain specific interactions with certain DNA sequences. A fraction of such specific complexes could act as nucleation points for the high-order levels of chromatin organization.     

Accessibility of the globular domain of histones H1 and H5 to antibodies upon folding of chromatin

Antibodies to the globular domain of histones H1 and H5 were purified by affinity chromatography and used to study the accessibility of this region of H1 and H5 in folded and unfolded rat liver and hen erythrocyte chromatin respectively. The different conformations of the chromatin filament were induced by varying the ionic strength from 1 mM to 80 mM NaCl and maintained by fixation with glutaraldehyde. Treatment with glutaraldehyde at a given salt concentration affected neither the orientation of nucleosomes relative to the fiber axis nor the compactness of chromatin. Solid-phase immunoassay and inhibition experiments showed no binding of the antibody against the globular domain of H1 to chromatin at the entire range of salt concentrations, while the antibody to the whole H1 molecule reacted with chromatin at low salt. On the other hand, the antibody to the globular region of H5 reacted with hen erythrocyte chromatin independently of the extent of chromatin condensation. These results indicate that the antigenic determinants of the globular domain of H5 are accessible to the antibody both in folded and unfolded chromatin, while those of the same region of H1 are masked, probably by interaction with DNA or proteins.     

The application of ESR to chromatin. Spin-labelling of the histone H3 cysteine residues in situ.

The possibility has been investigated of selectively spin-labelling the cysteine residues of histone H3 in chromatin and probing by ESR conformational changes affecting the labelled area as the molecular environment is altered. About 90% of bound labels are attached to the thiol groups and are strongly immobilized in deep crevices. The remaining labels are bound to amino groups mainly on histone H1, giving rise to a more mobile component in the chromatin spectrum. No conformational changes involving the labelled cysteins could be detected as the histones were dissociated stepwise from the complex by NaCl, but treatment with urea led to a cooperative increase in mobility, indicating that the hydrophobic region around the cysteine residues is folded in a compact tertiary structure to which histone H4 may be bound in the native complex, but which is not affected by dissociation of the H3-H4 unit from the DNA. In addition, chymotryptic disruption of the chromatin has been followed and an estimate made from the rotational correlation times of the size and origin of the digestion fragment carrying spin-labelled cysteine 110.     

Histone H1--DNA interaction. On the mechanism of DNA strands crosslinking by histone H1.

Crosslinking of DNA fibers by histone H1 or phosphorylated on Ser-37 histone H1, and by the individual fragments of the H1 polypeptide chain was studied by the method of turbidimetry. The dependence of the turbidity of DNA-protein complexes on the ionic strength in solution suggests that the condensation of H1.DNA complexes in vitro is apparently due to both specific histone-DNA interactions with the contribution of hydrogen and/or hydrophobic bonds and the formation of polycationic "bridges" fastening the DNA fibers. The effectiveness of the condensation is postulated to be a function of a proportion between the two mechanisms which in turn can be controlled by slight changes in ionic surroundings. The sharp dependence of shrinkage of H1.DNA complexes on ionic strength at "physiological" salt concentrations could provide a mechanism to regulate density and consequently the total activity of chromatin in the cell nuclei. The phosphorylation of histone H1 on Ser-37 by a specific histone kinase does not noticeably affect the pattern of DNA crosslinking by the H1.     

The distribution of histone H1 subfractions in chromatin subunits.

Rat liver chromatin was digested with micrococcal nuclease to various extents and fractionated into nucleosomes, di and trimers of nucleosomes on an isokinetic sucrose gradient. In conditions under which degradation of linker DNA within the particles was limited, the electrophoretic analysis of the histone content showed that the overall content of H1 histone increased from nucleosomes to higher order oligomers. Moreover, the histone H1 subfractions were found unevenly distributed among the chromatin subunits, one of them, H1--3 showing most variation. A more regular distribution of these subfractions was found in subunits obtained from a more extended digestion level of chromatin. It is suggested that the H1 subfractions differ in the protection they confer upon DNA.     

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.     

Comparative study of nucleosome particles in chromatin from normal and tumor cells. II. Reconstitution, compaction and association induced by ionic strength of a solution

The method of circular dichroism (CD) has been used to investigate the reconstitution of mononucleosomes from C3HA mice liver and ascitic hepatoma 22A cells chromatin. It has been revealed that the more unfolding state of DNA in ascitic nucleosomes (discovered earlier) is determined by the peculiarities of the interactions between DNA and the dimers H2A-H2B, as well as by the linker histones of the H1 group. The investigation of the DNA folding in the oligonucleosome chains with increasing ionic strength has shown complete invariability of the DNA compactness in the ascitic chromatin up to 100 mM NaCl, while in liver nucleosomes an additional folding of the linker portion of the DNA was observed within the range of 20-40 mM NaCl. Oligonucleosomes from ascitic chromatin are less inclined to association upon increasing ionic strength, as compared with those from liver chromatin.