Structural properties of barley nucleosomes

The structural properties of barley oligonucleosomes are investigated and compared to those of rat liver oligomers. Extraction of barley chromatin was performed using mild nuclease digestion of isolated nuclei leading to a low ionic strength soluble fraction. Oligonucleosomes were fractionated on sucrose gradients and characterized for DNA and histone content. Physico-chemical studies (sedimentation, circular dichroism and electric birefringence) showed that barley oligonucleosomes exhibit properties very close to those of the H1-depleted rat liver counterparts. Moreover, in situ, barley linker DNA was more sensitive to micrococcal nuclease digestion than that of rat liver. These results suggest that barley oligonucleosomes show a less compact structure than their rat liver counterparts and appear to be in contradiction with the very condensed organization of barley chromatin previously suggested.     

Organizational changes in chromatin at different malignant stages of Friend erythroleukemia.

The chromatin structure of morphologically-similar, but increasingly-malignant erythroleukemia cells was investigated using milk micrococcal nuclease digestion of isolated nuclei. The maximum solubilization of chromatin was unique for each of the three cell types: the least malignant (our Stage II) released 61% of its chromatin DNA, the most malignant (Stage IV), 46%, and the intermediate (Stage III) released 36%. An analysis of the nucleosome oligomers liberated by digestion also demonstrated differences. After 15 minutes of digestion when release was reaching its maximum, a greater proportion of large nucleosomal oligomers (sizes > trinucleosome) was released from Stage II nuclei than from Stage III or IV nuclei. The cell types also differed in the relative amount of H1-depleted mononucleosomes released. Analysis of the size of the double-stranded DNA associated with mononucleosomal particles showed that Stage III mononucleosomes were smaller (148 bp) than Stage IV (167 bp) or Stage II (190 bp). In addition, while the DNA of mononucleosomes depleted in H1 was smaller than that in the H1-containing species, relative size differences among the different cell types were retained. These data suggested that the difference in the mononuocleosome particle size resistant to nuclease digestion was independent of histone H1. Differences in nucleosome repeat length were also noted among the cell types. These studies have demonstrated dramatic differences in chromatin structure associated with malignant potential of an otherwise morphologically identical cell type. These findings may reflect changes in the relative amounts of H2a variants which we have previously described among the different malignant cell types.     

Structure of rat liver nuclei after depletion and reassociation of histone H1

Chromatin in isolated rat liver nuclei was compared with chromatin in (i) nuclei depleted of H1 by acid extraction; (ii) nuclei treated at pH 3.2 (without removal of H1), and (iii) depleted nuclei following reassociation of H1. Electron microscopy and digestion by DNase I, micrococcal nuclease and endogenous Ca/Mg endonuclease were used for this comparative examination. Electron micrographs of H1-depleted nuclei showed a dispersed and finely granular appearance. The rate of DNA cleavage by micrococcal nuclease or DNase I was increased several-fold after H1 removal. Discretely sized intermediate particles produced by Ca/Mg endonuclease in native nuclei were not observed in digests of depleted nuclei. Digestion by micrococcal nuclease to chromatin particles soluble in 60 mM NaCl buffer appeared not to be affected in depleted nuclei. When nuclei were treated at pH 3.2, neither the appearance of chromatin in electron micrographs nor the mode or rate of nuclease digestion changed appreciably. Following reassociation of H1 to depleted nuclei, electron micrographs demonstrated the reformation of compacted chromatin, but the lower rate of DNA cleavage in native nuclei was not restored. Further, H1 reassociation produced a significant decrease in the solubility of nuclear chromatin cleaved by micrococcal nuclease or Ca/Mg endonuclease. In order to evaluate critically the reconstitution of native chromatin from H1-depleted chromatin we propose the use of digestion by a variety of nucleases in addition to an electron microscopic examination.     

Laser-induced crosslinking of histones to DNA in chromatin and core particles: implications in studying histone-DNA interactions.

UV laser irradiation has been used to covalently crosslink histones to DNA in nuclei, chromatin and core particles and the presence of the different histone species in the covalently linked material was detected immunochemically. When nuclei were irradiated and then trypsinized to cleave the N- and C- terminal histone tails, no histones have been found covalently linked to DNA. This finding shows that UV laser-induced crosslinking of histones to DNA is accomplished via the non-structured domains only. This unexpected way of crosslinking operated in chromatin, H1-depleted chromatin and core particles, i.e. independently of the chromatin structure. The efficiency of crosslinking, however, showed such a dependence: whilst the yield of crosslinks was similar in total and H1-depleted chromatin, in core particles the efficiency was 3-4 times lower for H2A, H2B and H4 and 10-12 times lower for H3. The decreased crosslinking efficiency, especially dramatic in the case of H3, is attributed to a reduced number of binding sites, and, respectively, is considered as a direct evidence for interaction of nonstructured tails of core histones with linker DNA.     

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.     

Ionic strength-dependent conformational transitions of chromatin. Circular dichroism and thermal denaturation studies

High-molecular-weight chicken erythrocyte chromatin was prepared by mild digestion of nuclei with micrococcal nuclease. Samples of chromatin containing both core (H3, H4, H2A, H2B) and lysine-rich (H1, H5) histone proteins (whole chromatin) or only core histone proteins (core chromatin) were examined by CD and thermal denaturation as a function of ionic strength between 0.75 and 7.0 × 10^?3M Na⁺. CD studies at 21°C revealed a conformational transition over this range of ionic strengths in core chromatin, which indicated a partial unfolding of a segment of the core particle DNA at the lowest ionic strength studied. This transition is prevented by the presence of the lysine-rich histones in whole chromatin. Thermal-denaturation profiles of both whole and core chromatins, recorded by hyperchromicity at 260 nm, reproducibly and systematically varied with the ionic strength of the medium. Both materials displayed three resolvable thermal transitions, which represented the total DNA hyperchromicity on denaturation. The fractions of the total DNA which melted in each of these transitions were extremely sensitive to ionic strength. These effects are considered to result from intra- and/or internucleosomal electrostatic repulsions in chromatin studied at very low ionic strengths. Comparison of the whole and core chromatin melting profiles indicated substantial stabilization of the core-particle DNA by binding sites between the H1/H5 histones and the 140-base-pair core particle.     

The effects of salt concentration and H-1 depletion on the digestion of calf thymus chromatin by micrococcal nuclease.

We have removed histone H1 specifically from calf thymus nuclei by low pH treatment, and studied the digestion of such nuclei in comparison with undepleted nuclei. By a number of criteria the nuclei do not appear damaged. The DNA repeat-length in nuclear chromatin is found to be the same (192 +/- 4 bp) in the presence or absence of H1. These experiments demonstrate that the core histone complex of H2A, H2B, H3, and H4 can itself protect DNA sequences as long as 168 bp from nuclease. Our interpretation is that this represents an important structural element in chromatin, carrying two full turns of superhelical DNA. Depending on conditions of digestion this 168 bp fragment may be metastable and is normally rapidly converted by exonucleolytic trimming to the well-known "core-particle" containing 145 bp. Larger stable DNA fragments observed indigestion of H-1 depleted nuclei appear to arise from oligomers assembled from 168 bp cores in close contact exhibiting trimming of 0-20 bp at the ends. Electrophorograms of undepleted nuclear digests reveal oligomer bands in several size classes, each corresponding to one or more combinations of 168 bp particles, H1-protected spacers of about 20 bp length, and particles with ends trimmed to varying degrees.     

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.     

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.     

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.     

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)     

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.     

Studies on chromatin

Chromatin lacking histone H1 was found by electron microscopy to contain 'beaded' deoxyribonucleoprotein fibers. Adjacent beads are connected with each other by threads having a DNA-like appearance. At least some of threads are shown to be free DNA stretches. Average length and the content of free DNA stretches in histone H1-depleted chromatin depends on the ionic conditions of the medium. The appearance of individual beads is similar to that of chromatin subunits or v-bodies [1] in the original chromatin. Thus, in agreement with the X-ray data [2], histone H1 apparently is not required for maintenance of a compact state of DNA in chromatin subunits.     

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.     

Structural organization of the meiotic prophase chromatin in the rat testis

Pachytene nuclei were isolated from rat testes by the unit gravity sedimentation technique and contained histone variants H1a, H1t, TH2A, TH2B, and X2 in addition to the somatic histones H1bde, H1c, H2A, H2B, H3, and H4. The basic organization of the pachytene chromatin namely the nucleosome repeat length and the accessibility to micrococcal nuclease, was similar to that of rat liver interphase chromatin. However, when digested by DNase I, the susceptibility of pachytene chromatin was 25% more than liver chromatin under identical conditions. Nucleosome core particles were isolated from both liver and pachytene nuclei and were characterized for their DNA length and integrity of the nucleoprotein on low ionic strength nucleoprotein gels. While liver core particles contained all the somatic histones H2A, H2B, H3, and H4, in the pachytene core particles, histone variants TH2A, X2, and TH2B had replaced nearly 60% of the respective somatic histones. A comparison of the circular dichroism spectra obtained for pachytene and liver core particles indicated that the pachytene core particles were less compact than the liver core particles. Studies on the thermal denaturation properties of the two types of core particles revealed that the fraction of the pachytene core DNA melting at the premelting temperature region of 55-60 degrees C was significantly higher than that of the liver core DNA.     

Histone crosslinking patterns indicate dynamic binding of histone H1 in chromatin

Crosslinking of histone H1 molecules to each other and to the core histones with bifunctional reagents in mouse liver nuclei and chromatin was compared with that under the conditions of random 'contacts' between these molecules. The patterns of crosslinking of the H1 subfractions (H1A, H1B, and H10) to each other in nuclei, chromatin and in solution at different ionic strengths due to random collisions were essentially the same. Moreover, the contacts between the H1 molecules were qualitatively the same in nuclei, chromatin and in solution also at the level of the chymotryptic halves of the H1 molecules. The contacts between the H1 molecules and the core histones in nuclei were similar to those obtained in chromatin at 70 mM NaCl, when H1 molecules readily migrate, and at 0.6 M NaCl, when H1 molecules are dissociated from chromatin. We conclude that spatial arrangement of H1 subfractions and mutual orientation of H1 molecules in isolated nuclei are random-like at least in terms of cross-linking. The static and dynamic models of histone H1 binding to chromatin compatible with the known data are considered. Although unequivocal verification of the models is not possible at present, the dynamic models do correspond better to recent data on the location of the histone H1 in nuclei and chromatin.     

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.     

Structure of nucleosomes and organization of internucleosomal DNA in chromatin

We have compared the mononucleosomal pattern produced by micrococcal nuclease digestion of condensed and unfolded chromatin and chromatin in nuclei from various sources with the repeat length varying from 165 to 240 base-pairs (bp). Upon digestion of isolated H1-containing chromatin of every tested type in a low ionic strength solution (unfolded chromatin), a standard series of mononucleosomes (MN) was formed: the core particle, MN145, and H1-containing, MN165, MN175, MN185, MN195, MN205 and MN215 (the indexes give an approximate length of the nucleosomal DNA that differs in these particles by an integral number of 10 bp). In addition to the pattern of unfolded chromatin, digestion of whole nuclei or condensed chromatin (high ionic strength of Ca2+) gave rise to nuclei-specific, H1-lacking MN155. Digestion of H1-lacking chromatin produced only MN145, MN155 and MN165 particles, indicating that the histone octamer can organize up to 165 bp of nucleosomal DNA. Although digestion of isolated sea urchin sperm chromatin (repeat length of about 240 bp) at a low ionic strength gave a typical "unfolded chromatin pattern", digests of spermal nuclei contained primarily MN145, MN155, MN235 and MN245 particles. A linear arrangement of histones along DNA (primary organization) of the core particle was found to be preserved in the mononucleosomes, with the spacer DNA length from 10 to 90 bp on one (in MN155) or both sides of core DNA being a multiple of about 10 bp. In MN235, the core particle occupies preferentially a central position with the length of the spacer DNA on both sides of the core DNA being usually about 30 + 60 or 40 + 50 bp. Histone H1 is localized at the ends of these particles, i.e. close to the centre of the spacer DNA. The finding that globular part of histones H3 and sea urchin sperm H2B can covalently bind to spacer DNA suggests their involvement in the organization of chromatin superstructure. Our data indicate that decondensation of chromatin is accompanied by rearrangement of histone H1 on the spacer DNA sites adjacent to the core particle and thus support a solenoid model for the chromatin superstructure in nuclei in which the core DNA together with the spacer DNA form a continuous superhelix.