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.     

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.     

Exchange of H1 histone depends on aggregation of chromatin, not simply on ionic strength

Chromatin solubility was observed at several concentrations of various cations. Spermine and spermidine precipitated (50%) chromatin at about 0.2 mM, Ca2+ and Mg2+ at about 1-2 mM, and Na+ at about 100 mM. Further increases in cation concentration induced more aggregation, but eventually excess cation increased chromatin solubility so that 50% solubility was observed again at 60 mM Mg2+ and 180 mM Na+. H1 histone was 50% released by 80 mM MgCl2 or 425 mM NaCl. Combinations of MgCl2 and NaCl showed that Mg2+ and Na+ are synergistic in the induction of aggregation in lower concentrations (less than 2 mM) of Mg2+ but antagonistic at higher concentrations, and a similar effect of NaCl on spermidine-induced precipitation was shown below and above about 0.2 mM spermidine. At 5 mM, MgCl2 proved capable of precipitating chromatin depleted of H1 histone, but no concentration of NaCl was capable of doing so. These phenomena can be rationalized by supposing that neutralization of chromatin by any cation (including H1 histone) favors aggregation and also that cross-linking of chromatin fibers by multivalent cations (including H1 histone) is also critically important. The exchange of H1 histone between chromatin fragments was tested in various concentrations of different salts. H1 exchange was correlated with chromatin aggregation rather than with ionic strength and thus appears to depend on fiber to fiber contact. Under conditions where H1 exchanges between chromatin fibers that are permitted to make contact with each other, no H1 exchange occurred between chromatin inside the nucleus and chromatin outside, even though H1 histone is capable of passage through the nuclear membrane.     

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.     

Porcine follitropin. The amino-acid sequence of the beta subunit

By treatment with tRNA in the presence of 1 mM MgCl2, a chromatin preparation was obtained containing all five major histone fractions but lacking a considerable portion of non-histone proteins. This chromatin preparation as well as chromatin extracted with 0.6 M NaCl (depleted of H1 histone and some non-histone proteins) were characterized in respect of solubility and chromatin DNA accessibility. Both samples possessed practically the same solubility in the presence of 0.15 M NaCl and 1 mM MgCl2. The solubility of tRNA-treated chromatin in 5 and 10 mM MgCl2 was higher than that of salt-extracted chromation. The accessibility of the DNA of these chromatin preparations was tested with DNA-dependent RNA polymerase of Escherichia coli as a probe, using procedure that permits measurement of binding site frequency. Both tRNA-treated and salt-extracted chromatin contained as many as 33% and untreated chromatin as few as 4% of the number of binding sites found on protein-free DNA. These results demonstrate that at least in part the non-histone proteins are responsible for salt-induced insolubility and low DNA accessibility of chromatin, thus revealing the importance of non-histone proteins in the maintenance of an overall chromatin structure.     

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.     

Distribution of estradiol receptor and vitellogenin gene in chick liver chromatin fractions.

The distribution of estradiol receptor and vitellogenin gene was studied in estradiol stimulated chick liver chromatin fractions prepared by limited DNAse II digestion and MgCl2 precipitation. The receptor was found in all fractions, undigested chromatin (P1), Mg2+ insoluble chromatin (P2) and Mg2+ soluble chromatin (S2). This last fraction was rich in acidic proteins, had a high protein:DNA ratio (7.0 w/w), contained 28% of rapidly labelled RNA, 20% of the receptor, 3-5% of chromatin DNA and showed a 2 fold enrichment of vitellogenin DNA sequences over unfractionated chromatin as well as P1 and P2 DNA. On isopycnic metrizamide gradients, all chromatin fractions showed a receptor peak banding at 1.23 g/cm3, the density of nucleoproteins. Hybridization experiments showed that the DNA banding at this density in fraction S2 was enriched 4 fold in vitellogenin DNA sequences over unfractionated chromatin as well as P1 and P2 DNA. These results suggest an association of hormone receptor complex with nucleoprotein structures of an apparently active chromatin fraction.     

The effect of poly(ADP-ribosyl)ation on native and H1-depleted chromatin. A role of poly(ADP-ribosyl)ation on core nucleosome structure

The effect of poly(ADP-ribosyl)ation on native and H1-depleted chromatin was analyzed by gel electrophoresis, electron microscopy, and velocity sedimentation. In parallel, the interaction of automodified poly(ADP-ribose) polymerase with native and H1-depleted chromatin was analyzed. In H1-depleted chromatin histone H2B becomes the major poly(ADP-ribose) histone acceptor protein, whereas in native chromatin histone H1 was the major histone acceptor. Poly(ADP-ribosyl)ation of H1-depleted chromatin prevented the recondensation of polynucleosomes reconstituted with exogenous histone H1. This is probably due to the presence of modified poly(ADP-ribose) polymerase and hyper(ADP-ribosyl)ated histone H2B. Indeed, about 40% of the modified enzyme remained associated with H1-depleted chromatin, while less than 1% of the modified enzyme was bound to native chromatin. The influence of poly(ADP-ribosyl)ation on the chromatin conformation was also studied at the level of nucleosome in using monoclonal and polyclonal antibodies specific for individual histones and synthetic peptides of histones. In native chromatin incubated in the presence of Mg2+ there was a drop in the accessibility of histone epitopes to monoclonal and polyclonal antibodies whereas upon poly(ADP-ribosyl)ation their accessibility was found to remain even in the presence of Mg2+. In poly(ADP-ribosyl)ated H1-depleted chromatin an increased accessibility of some histone tails to antibodies was observed.     

Selective removal of histone H1 from nucleosomes at low ionic strength

The method for removal of histone H 1 from chromatin by treatment with ion-exchange resin AG 50 WX 2 in the presence of 100 mM NaCl and 50 mM phosphate buffer (Thoma and Koller, 1977, Cell, 12, 101–107) results in production not only of H1-depleted chromatin but also free DNA. We have now modified this procedure so that the nucleosome is treated with the cation exchange resin in two steps, first in 50 mM sodium phosphate buffer and then in 50 mM sodium phosphate and 50 mM NaCl whereby histone H 1 is selectively removed without a release of free DNA at low resin concentrations.Abbreviations NaP Sodium phosphate buffer of molarities and pH as stated in the text - SDS Sodium dodecyl sulfate     

Novel nucleosomal particles containing core histones and linker DNA but no histone H1

Eukaryotic chromosomal DNA is assembled into regularly spaced nucleosomes, which play a central role in gene regulation by determining accessibility of control regions. The nucleosome contains ∼147 bp of DNA wrapped ∼1.7 times around a central core histone octamer. The linker histone, H1, binds both to the nucleosome, sealing the DNA coils, and to the linker DNA between nucleosomes, directing chromatin folding. Micrococcal nuclease (MNase) digests the linker to yield the chromatosome, containing H1 and ∼160 bp, and then converts it to a core particle, containing ∼147 bp and no H1. Sequencing of nucleosomal DNA obtained after MNase digestion (MNase-seq) generates genome-wide nucleosome maps that are important for understanding gene regulation. We present an improved MNase-seq method involving simultaneous digestion with exonuclease III, which removes linker DNA. Remarkably, we discovered two novel intermediate particles containing 154 or 161 bp, corresponding to 7 bp protruding from one or both sides of the nucleosome core. These particles are detected in yeast lacking H1 and in H1-depleted mouse chromatin. They can be reconstituted in vitro using purified core histones and DNA. We propose that these ‘proto-chromatosomes’ are fundamental chromatin subunits, which include the H1 binding site and influence nucleosome spacing independently of H1.     

Structural transition in chromatin induced by ions in solution

Structural transition in chromatin was measured as a function of counter ions in solution (NaCl or MgCl(2)) and of histones bound on the DNA. The addition of counter ions to aqueous solutions of chromatin, partially dehistonized chromatin, and DNA caused a drastic reduction in viscosity and a significant increase in sedimentation coefficient. Transitions occurred primarily at about 2 x 10(-3) M NaCl and 1 x 10(-5) M MgCl(2) and are interpreted as a change in structure of chromatin induced by tight binding of cations (Na(+) or Mg(++)) to DNA, either free or bound by histones, and is an intrinsic property of DNA rather than of the type of histone bound. At a given ionic condition, removal of histone H1 from chromatin had only a minor effect on the hydrodynamic properties of chromatin while removal of other histones caused a drastic change in these properties. An increase in the sedimentation coefficient of DNA was observed also for protamine. DNA complexes wherein the bound protein contains only unordered coil rather than the alpha-helices found in histones.     

Different repeat lengths in rat satellite I DNA containing chromatin and bulk chromatin.

The nucleosome repeat structure of a rat liver chromatin component containing the satellite I DNA (repeat length 370 bp) was investigated. Digestion experiments with micrococcal nuclease, DNAase II, and the Ca2+/Mg2+-dependent endogenous nuclease of rat liver nuclei revealed a repeat unit of 185 nucleotide pairs which is shorter by approximately 10 bp than the repeat unit of the bulk chromatin of this cell type. The difference seems not to be related to the histone composition which was found to be similar in the two types of chromatin.     

Increased stability of the higher order structure of chicken erythrocyte chromatin: nanosecond anisotropy studies of intercalated ethidium

Internal motion of the DNA in chicken erythrocyte chromatin fibers was studied by measurement of the fluorescence anisotropy decay of ethidium intercalated in the linker region. A comparison of the decay curves of the dye in chicken erythrocyte chromatin with those of calf thymus chromatin [Ashikawa, I., Kinosita, K., Jr., Ikegami, A., Nishimura, Y., Tsuboi, M., Watanabe, K., Iso, K., & Nakano, T. (1983) Biochemistry 22, 6018-6026] revealed greater suppression of nucleosome movement in chicken erythrocyte chromatin. Furthermore, the transition of this chromatin to the compact (solenoidal) structure occurred at lower solvent concentrations of Na+ or Mg2+ than those for calf thymus chromatin. These results demonstrated increased stability of the higher order structure (the solenoid) of chicken erythrocyte chromatin, which may be related to the reduction of nuclear activity in the chicken erythrocyte cell. In addition to intact chicken erythrocyte chromatin, we studied the structural transitions of H1-depleted and H1,H5-depleted chromatins. The result indicated that histone H5 of this chromatin stabilizes the higher order structure in the presence of magnesium (or divalent) cation and did not induce the transition in the solution containing only sodium cation.     

Nucleosome rearrangement in vitro. 1. Two phases of salt-induced nucleosome migration in nuclei

We have investigated the salt- and temperature-induced rearrangement of nucleosomes in both intact and H1-depleted nuclei from human cells. In agreement with previous reports on the rearrangement of nucleosomes in isolated chromatin or chromatin fragments, we observed a decrease in the average nucleosome repeat length following incubation of nuclei at 37 degrees C in elevated salt concentrations. However, this decrease occurred in two distinct phases. First, incubation of H1-depleted nuclei at 37 degrees C for as little as 10 min in low-salt, isotonic buffer (containing 0.025 M KCl) resulted in a shift in the limiting repeat value from approximately 190 to 168 base pairs (bp). A similar shift was observed for intact nuclei incubated at 37 degrees C for 1 h in buffer containing near-physiological salt concentrations (i.e., 0.175 M KCl). This limiting repeat value was maintained in both intact and H1-depleted nuclei up to a salt concentration of 0.45 M KCl in the incubation buffer. Second, at salt concentrations of 0.625 M KCl, a limiting repeat of approximately 146 bp was obtained, and the nuclei had clearly lysed. During the first shift in repeat length, little additional exchange of nuclear proteins occurred compared to nuclei kept on ice in a low-salt buffer. This was the case even though the conditions used to monitor exchange were optimized by using a high DNA to chromatin ratio. On the other hand, a significant increase in the exchange of nuclear proteins, and formation of nucleosomes on the naked DNA, was observed during the shift in repeat length to 146 bp.(ABSTRACT TRUNCATED AT 250 WORDS)