The superstructure of chromatin and its condensation mechanism

Model calculations on the superstructure of uncondensed and condensed chromatin are presented. It is found that agreement between the calculated X-ray solution scattering patterns and the experimental observations can be reached with the assumptions that: a) The uncondensed chromatin fibre in solution has a helix-like structure, with a pitch of ca. 33.0 nm, a helical diameter of ca. 20.0 nm and 2.75–3.25 nucleosomes per turn. b) The most condensed state of the chromatin fibre in solution is best represented by a helix-like structure with ca. 2.56 nucleosomes per turn, a pitch of ca. 3.0 nm and a helical diameter of ca. 27.0 nm.     

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.     

Nucleosomes stacked with aligned dyad axes are found in native compact chromatin in vitro

In this study, electron tomograms of plunge-frozen isolated chromatin in both open and compacted form were recorded. We have resolved individual nucleosomes in these tomograms in order to provide a 3D view of the arrangement of nucleosomes within chromatin fibers at different compaction states. With an optimized template matching procedure we obtained accurate positions and orientations of nucleosomes in open chromatin in "low-salt" conditions (5 mM NaCl). The mean value of the planar angle between three consecutive nucleosomes is 70°, and the mean center-to-center distance between consecutive nucleosomes is 22.3 nm. Since the template matching approach was not effective in crowded conditions, for nucleosome detection in compact fibers (40 mM NaCl and 1 mM MgCl(2)) we developed the nucleosome detection procedure based on the watershed algorithm, followed by sub-tomogram alignment, averaging, and classification by Principal Components Analysis. We find that in compact chromatin the nucleosomes are arranged with a predominant face-to-face stacking organization, which has not been previously shown for native isolated chromatin. Although the path of the DNA cannot be directly seen in compact conditions, it is evident that the nucleosomes stack with their dyad axis aligned in forming a "double track" conformation which is a consequence of DNA joining adjacent nucleosome stacks. Our data suggests that nucleosome stacking is an important mechanism for generating chromatin compaction in vivo.     

The superstructure of chromatin and its condensation mechanism

Synchroton radiation X-ray scattering experiments have been performed on chicken erythrocyte chromatin fibres over a wide range of ionic conditions and on various states of the fibres (i.e. "native" in solution, in gels and in whole nuclei; chromatin depleted of the H1 (H5) histones and chromatin with bound ethidium bromide). A correlation between the results obtained with the various chromatin preparations provides evidence for a model according to which at low ionic strength the chromatin fibre already possesses a helical superstructure, with a diameter comparable to that of condensed chromatin, held together by the H1(H5) histone. The most significant structural modification undergone upon an increase of the ionic strength is a reduction of the helix pitch, this leads to condensation in a manner similar to the folding of an accordion. The details of this process depend on whether monovalent or divalent cations are used to raise the ionic strength, the latter producing a much higher degree of condensation. Measurements of the relative increase of the mass per unit length indicate that the most condensed state is a helical structure with a pitch around 3.0-4.0 nm. In this paper we give a detailed presentation of the experimental evidence obtained from static and time-resolved scattering experiments, which led to this model.     

Cryo-electron microscopy of vitrified SV40 minichromosomes: the liquid drop model.

The structure of SV40 minichromosomes has been studied by cryo-electron microscopy of vitrified thin layers of solution. In high-salt buffer (130 mM NaCl), freshly prepared minichromosomes are condensed into globules 30 nm or more in diameter. On the micrograph, they appear to be formed by the close packing of 10 nm granules which give rise to a 10 nm reflection in the optical diffractogram. The globules can adopt many different conformations. At high concentration, they fuse into a homogeneous 'sea' of closely packed 10 nm granules. In low-salt buffer (less than 10 mM NaCl), the globules open, first into 10 nm filaments, and then into nucleosome-strings. The 'liquid drop' model is proposed to explain the condensed structure of the minichromosome in high-salt buffer: nucleosomes stack specifically on top of one another, thus forming the 10 nm filaments. 10 nm filaments in turn, tend to aggregate laterally. Optimizing both these interactions results in the condensation of 10 nm filaments or portions thereof into a structure similar to that of a liquid. Some implications of this model for the structure of cellular chromatin are discussed.     

Nucleosomes arrangement in chromatin

The spatial arrangement of nucleosomes in rat liver chromatin has been examined using the electric birefringence technique. All chromatin subunits studied (up to 9 consecutive nucleosomes) contain their full complement of the five histone types associated with about 200 base pairs repeat length DNA.     

Higher levels of organization in chromosomes.

On the basis of recent results a unified view of different aspects of the higher levels in the organization of chromatin in chromosomes is presented. Basic to these forms of organization is the arrangement of DNA in the complex with nucleosomes and recent studies suggest that at least some species of satellite DNA may maintain a fixed DNA sequence relationship to the phasing of nucleosomes. Special proteins such as the high-mobility group (HMG) proteins or other non-histone proteins could serve specific functions in the recognition of satellite DNA sequences.In the presence of histone H1 the 110 Å nucleosome fiber formed from the basic string of nucleosomes can be further condensed into a thicker 250–300 Å fiber formed by a solenoidal coiling of the 110 Å fiber with about 6–8 nucleosomes per turn and the available evidence suggests that these structures are found in mitotic chromosomes as well as other forms of inactive chromatin. A further level of coiling of the 250–300 Å solenoid has been suggested by our recent studies of disintegrated mitotic chromosomes consisting of a thin-walled tube with an outer diameter of 4000 Å referred to as the unit fiber. This structure would account for a factor of 1400 × contraction of DNA in mitotic chromosomes which in their intact state are only 5-fold more contracted. The recently described “scaffold” proteins could be responsible for this final coiling of the unit fibers in intact chromosomes.Meiotic chromosomes are generally less contracted than mitotic chromosomes. An extreme example of this are lampbrush chromosomes that apart from the axial segments which might contain some structural proteins appear to consist of naked DNA arranged in lateral loops. In the later stages of meiosis more condensed structures arise as exemplified by the synaptonemal complex during the pachytene stage in many organisms. The characteristic features of this structure are interpreted to suggest that the structure consists of lateral components containing two parallel 110 Å nucleosome fibers each representing the axial segments of two sister chromatids. From these paired regions loops protrude laterally in a manner which closely resembles the less condensed lampbrush chromosomes. The implication of this structure in the process of crossingover is discussed.Less is known about the organization of chromatin in interphase nuclei, but structures analogous to the loop-like structures in meiotic chromosomes are suggested on the basis of the isolation of supercoiled DNA loops constrained by RNA-DNA and protein-DNA interactions. The position of these loops is suggested to be fixed by specific repeated DNA sequences that could be associated with specific tenacious non-histone or HMG proteins.     

Differential scattering of circularly polarized light by chromatin modeled as a helical array of dielectric ellipsoids within the born approximation

Theoretical predictions within the Born approximation of the expected differential light scattering of circularly polarized light (CIDS) were made for the 300-Å chromatin fiber, modeled as a helical array of dielectric ellipsoids. Computed CIDS values were strongly dependent on the exact geometry of the solenoid model, depending particularly on parameters relaed to the chiral nature of the fiber and the orientation of the nucleosomes within the helix, in contrast to the values of the total light scattering, which mainly probed size and shape. In particular, both a superbead model and a strict linear 110-Å nucleosome filament would be predicted as giving rise to zero CIDS (in disagreement with the finite values observed). At the same time, helical models in which the normal vectors to the nucleosome faces were exactly parallel to the helical axis also yielded zero CIDS. Confirming earlier expectations, CIDS values were significantly less dependent on helical length than total light scattering. Finally, comparison of these calculated results from those extrapolated from available experimental data indicates that predicted CIDS values, based on currently accepted models of solenoid structure, are within an order of magnitude of those experimentally observed. Together, these results indicate the potential of differential light scattering measurements as a probe of chromatin higher-order structure, complementary to existing scattering measurements.     

Electron microscopic and biochemical evidence that chromatin structure is a repeating unit

Electron microscopic and biochemical studies demonstrate that the fundamental structure of chromatin depleted of lysine-rich histones is composed of a flexible chain of spherical particles (nucleosomes), about 125 Å in diameter, connected by DNA filaments. Such a chromatin preparation can be separated by centrifugation into two fractions which differ in the spacing of the nucleosomes. In one fraction almost all of the DNA is condensed in nucleosomes, while the other fraction contains long stretches of free DNA connecting regions where the nucleosomes are closely packed. The isolated nucleosomes contain about 200 base pairs of DNA and the four histones F2a₁, F2a₂, and F2b, and F3 in an overall histone/DNA ratio of 0.97. In such a structure the DNA is compacted slightly more than five times from its extended length. The same basic structure can be visualized in chromatin spilling out of lysed nuclei. However, in this latter case the nucleosomes are very closely packed, suggesting that histone F1 is involved in the superpacking of DNA in chromosomes and nuclei. The chromatin fiber appears to be a self-assembling structure, since the nucleosomal arrangement can be reconstituted in vitro from DNA and the four histones F2a₁, F2a₂, F2b and F3 only, irrespective of their cellular origin.     

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.     

Some properties of tobacco protoplast chromatin.

Chromatin was prepared from tobacco-leaf protoplasts. Its solubility in increasing molarities of NaCl was studied and the structure of the soluble fraction observed by electron microscopy. We demonstrate that in plants, the DNA and histones are associated in beaded structures similar to those called omicron-bodies or nucleosomes in animal chromatin. The nucleosomes were associated with DNA in either compact or extended forms. The compact arrangement was predominant in the fraction solubilized between 0.1 and 0.4 M NaCl. The extended form, present at 0.5 and 0.6 M NaCl. showed DNA filaments of various lengths interspacing the nucleosomes. At these ionic strengths ring structures were present, associated with the DNA. At 0.7 M NaCl and above, only DNA filaments were present, occasionally associated with big rings, and nucleosomes were compoetely dissociated. Free DNA molecules were present at all ionic strengths used. The possible origin and significance of the rings are discussed.     

The higher order repeat structure of chromatin is built up of globular particles containing eight nucleosomes

Mild nuclease digestion of rat liver chromatin generates particles with sedimentation coefficients of about 33S, 60S, and 90S (in 50 mM NaCl). The kinetics of appearance and disappearance of these particles with progressive digestion suggest that they are produced by cleavage from a higher order repeat structure, the 33S particle representing the monomer. At an intermediate stage of digestion, about 75 % of the nuclear chromatin can be recovered as monomers to trimers of this higher order structure. Sedimentation profiles indicate that monomer particles containing 7–8 nucleosomes occur at the highest frequency. The DNA fragments in monomers have a size corresponding to hepta- and octanucleosomes, and those in dimers have a size corresponding to chains of sixteen nucleosomes. The higher order repeat structure is only stable between 30 and 200 mM NaCl; the particles unfold below 30 and above 200 mM NaCl. When examined by electron microscopy, monomers and dimers appear as compact globular structures. Relaxation by lowering the salt concentration results in the appearance of polynucleosomes with a chain length of eight beads in the monomer and sixteen in the dimer particle. These results indicate that the unit particle of the higher order repeat structure of rat liver chromatin contains eight nucleosomes.     

Preferential nucleosome occupancy at high values of DNA helical rise

Nucleosomes are the basic structural units of eukaryotic chromatin and play a key role in the regulation of gene expression. Nucleosome formation depends on several factors, including properties of the sequence itself, but also physical constraints and epigenetic factors such as chromatin-remodelling enzymes. In this view, a sequence-dependent approach is able to capture a general tendency of a region to bind a histone octamer. A reference data set of positioned nucleosomes of Saccharomyces cerevisiae was used to study the role of DNA helical rise in histone-DNA interaction. Genomic sequences were transformed into arrays of helical rise values by a tetranucleotide code and then turned into profiles of mean helical rise values. These profiles resemble maps of nucleosome occupancy, suggesting that intrinsic histone-DNA interactions are linked to helical rise. The obtained results show that preferential nucleosome occupancy occurs where the mean helical rise reaches its largest values. Mean helical rise profiles obtained by using maps of positioned nucleosomes of the Drosophila melanogaster and Plasmodium falciparum genomes, as well as Homo sapiens chromosome 20 confirm that nucleosomes are mainly located where the mean helical rise reaches its largest values.     

Light scattering measurements supporting helical structures for chromatin in solution.

Laser light scattering measurements have been made on a series of polynucleosomes containing from 50 to 150 nucleosomes. Radii of gyration have been determined as a function of polynucleosome length for different ionic strength solutions. The results suggest that at low ionic strength the chromatin adopts a loosely helical structure rather than a random coil. The helix becomes more regular on increasing the ionic strength, the dimension resembling those proposed by Finch and Klug for their solenoid model.     

The fine structure of chromatin in Paranosema grylli (Microsporida)

Nucleosomes were found for the first time in the nuclear chromatin of Microsporida--organisms known among the smallest eukaryotes on Earth. Chromatin of Paranosema grylli sporoplasm was studied by Miller's technique. On low ionic-strength cell spreads, this chromatin was represented by 10 nm nucleosome filaments, 20 nm filaments, and "smooth" (nucleosome-free) filaments of 3-4 nm in diameter. Nucleosome filaments display structural heterogeneity seen as irregular arrangement of nucleosome particles along the filament length. Different nucleosome filaments show 13-30 nucleosomes per 1 microm with the length of linker DNA ranging from 10 to 45 nm. The present results suggest that microsporidian chromatin is weakly condensed. Only lower-order chromatin packaging levels displayed some structural peculiarities.     

The effects of sodium and magnesium-ion interactions on chromatin structure and solubility

The effects of sodium and magnesium-ion interactions on chromatin structure and solubility were examined in isolated mouse liver nuclei. To facilitate this study, a simple assay of chromatin structure was developed, based on the absorbances at 260 nm (A260) and 320 nm (A320) of nuclei in test solutions. By subtracting the A320 from the A260, a single "spectral index" was obtained which served as a useful, but not absolute, indicator of chromatin structure. Electron microscopy verified the validity of this approach. The results indicate that either 200 mM NaCl or 0.5 mM MgCl2 were capable of preserving the native 20 to 30 nm chromatin fiber structure. Below 200 mM NaCl, the native fiber progressively uncoiled to the 10 nm unit fiber. The presence of 0.5 mM MgCl2 inhibited this uncoiling. Only divalent cations stabilized condensed chromatin (heterochromatin) within the nucleus. Monovalent and divalent cations interacted with one another at critical concentrations and modified their individual effects on chromatin structure; e.g., 10 to 25 mM NaCl interfered with the action of 0.5 to 1.5 mM MgCl2, causing a complete loss of condensed chromatin. Maximum solubility of micrococcal nuclease-digested chromatin occurred at 10 mM NaCl, which treatment allowed the chromatin to unfold to the 10 nm fiber. However, ionic conditions that disrupted condensed chromatin but maintained the native chromatin fiber morphology still resulted in relatively high yields of soluble chromatin. Minimum solubility occurred under conditions which preserved the structure of condensed chromatin.     

Influence of histone H1 on chromatin structure

Removal of histone H1 produces a transition in the structure of chromatin fibers as observed by electron microscopy. Chromatin containing all histone proteins appears as fibers with a diameter of about 250 A. The nucleosomes within these fibers are closely packed. If histone H1 is selectively removed with 50-100 mM NaCl in 50 mM sodium phosphate buffer (pH 7.0) in the presence of the ion-exchange resin AG 50 W - X2, chromatin appears as "beads-on-a-string" with the nucleosomes separated from each other by distances of about 150-200 A. If chromatin is treated in the presence of the resin with NaCl at concentrations of 650 mM or more, the structural organization of the chromatin is decreased, yielding fibers of irregular appearance.