Three-dimensional reconstruction of chromatin fibers

We have obtained tilt series of thin sections of chromatin fibers embedded in araldite-epon and stained with uranyl acetate. The tilt series contain between 12 and 18 micrographs, spanning tilt ranges between 84 and 117 degrees. Reconstructions in three dimensions have been obtained by filtered back-projection from each tilt series. The reconstructions have been low-pass filtered in order to reduce the amount of noise. In the reconstructions it is possible to approximately localize the nucleosomes. In several regions they show a clear zigzag arrangement, but in other regions it is difficult to determine the sequence of the nucleosomes. In any case there is no clear indication of a solenoidal arrangement. We discuss the rules which may give rise to a 3-D arrangement of the nucleosomal zigzag.     

Optical model studies of the salt-induced 10-30-nm fiber transition in chromatin

Fractionated chicken erythrocyte chromatin fibers consisting of 10-mer and 75-mer polynucleosomes have been studied by flow birefringence and viscosity over a range of Na+ and Mg2+ ion concentrations sufficient to span the 10-30-nm fiber transition. Negative intrinsic flow bifringence was observed under all solvent conditions investigated. The intrinsic birefringence, obtained from the reduced birefringence to intrinsic viscosity ratio, was used to evaluate various optical models for the DNA conformation in the fiber. Results are consistent with an extended chromatosome-linker "necklace" model for the unfolded, low-salt fiber and with a solenoidal model of edge-stacked chromatosomes for the condensed fiber at high salts. These results are consistent with and independently corroborative of similar models based upon electric dichroism and neutron scattering reported by others.     

Computer simulation of the 30-nanometer chromatin fiber

A new Monte Carlo model for the structure of chromatin is presented here. Based on our previous work on superhelical DNA and polynucleosomes, it reintegrates aspects of the "solenoid" and the "zig-zag" models. The DNA is modeled as a flexible elastic polymer chain, consisting of segments connected by elastic bending, torsional, and stretching springs. The electrostatic interaction between the DNA segments is described by the Debye-Hückel approximation. Nucleosome core particles are represented by oblate ellipsoids; their interaction potential has been parameterized by a comparison with data from liquid crystals of nucleosome solutions. DNA and chromatosomes are linked either at the surface of the chromatosome or through a rigid nucleosome stem. Equilibrium ensembles of 100-nucleosome chains at physiological ionic strength were generated by a Metropolis-Monte Carlo algorithm. For a DNA linked at the nucleosome stem and a nucleosome repeat of 200 bp, the simulated fiber diameter of 32 nm and the mass density of 6.1 nucleosomes per 11 nm fiber length are in excellent agreement with experimental values from the literature. The experimental value of the inclination of DNA and nucleosomes to the fiber axis could also be reproduced. Whereas the linker DNA connects chromatosomes on opposite sides of the fiber, the overall packing of the nucleosomes leads to a helical aspect of the structure. The persistence length of the simulated fibers is 265 nm. For more random fibers where the tilt angles between two nucleosomes are chosen according to a Gaussian distribution along the fiber, the persistence length decreases to 30 nm with increasing width of the distribution, whereas the other observable parameters such as the mass density remain unchanged. Polynucleosomes with repeat lengths of 212 bp also form fibers with the expected experimental properties. Systems with larger repeat length form fibers, but the mass density is significantly lower than the measured value. The theoretical characteristics of a fiber with a repeat length of 192 bp where DNA and nucleosomes are connected at the core particle are in agreement with the experimental values. Systems without a stem and a repeat length of 217 bp do not form fibers.     

Structure of hyperacetylated chromatin: light scattering and flow linear dichroism study

Cation-induced folding of 10 nm chromatin filament to 30 nm fiber was studied with hyperacetylated chromatin using light scattering at 90 degrees and flow linear dichroism. Acetylated chromatin folded in a way indistinguishable from that of the control chromatin: both the compactness of chromatin and the orientation of nucleosomes relative to the fiber axis were identical at a given salt concentration.     

Organisation of subunits in chromatin.

There is considerable current interest in the organisation of nucleosomes in chromatin. A strong X-ray and neutron semi-meridional diffraction peak at approximately 10 nm had previously been attributed to the interparticle specing of a linear array of nucleosomes. This diffraction peak could also result from a close packed helical array of nucleosomes. A direct test of these proposals is whether the 10 nm peak is truly meridional as would be expected for a linear array of nucleosomes or is slightly off the meridian as expected for a helical array. Neutron diffraction studies of H1-depleted chromatin support the latter alternative. The 10 nm peak has maxima which form a cross-pattern with semi-meridional angle of 8 to 9 degrees. This is consistent with a coil of nucleosomes of pitch 10 nm and outer diameter of approximately 30 nm. These dimensions correspond to about six nucleosomes per turn of the coli.     

The superstructure of chromatin and its condensation mechanism

Electric dichroism and X-ray scattering measurements on solutions of uncondensed and condensed chicken erythrocyte chromatin were interpreted on the basis of model calculations. Information about the state of uncondensed fibers in the conditions of electric dichroism measurements was obtained from scattering patterns recorded as a function of pH, in the presence of spermine and at very low monovalent cation concentrations. Electric dichroism measurements on a complex of uncondensed chromatin with methylene blue were made to determine the contribution of the linker and of the nucleosomes to the total dichroism.A new approach to calculate the dichroism from realistic structural models, which also yields other structural parameters (radius of gyration, radius of gyration of the cross-section, mass per unit length) was used. Only a restricted range of structures is simultaneously compatible with all experimental results. Further, it is shown that previous interpretations of dichroism measurements on chromatin were in contradiction with X-ray scattering data and failed to take into account the distribution of orientation of the nucleosomes in the fibers. When this is done, it is found that the linker DNA in chicken erythrocyte and sea urchin chromatin must run nearly perpendicularly to the fibre axis. Taken together with the dependence of the fibre diameter on the linker length, these results provede the strongest evidence hitherto available for a model in which the linker crosses the central part of the fibre.     

Small angle x-ray scattering of chromatin. Radius and mass per unit length depend on linker length.

Analyses of low angle x-ray scattering from chromatin, isolated by identical procedures but from different species, indicate that fiber diameter and number of nucleosomes per unit length increase with the amount of nucleosome linker DNA. Experiments were conducted at physiological ionic strength to obtain parameters reflecting the structure most likely present in living cells. Guinier analyses were performed on scattering from solutions of soluble chromatin from Necturus maculosus erythrocytes (linker length 48 bp), chicken erythrocytes (linker length 64 bp), and Thyone briareus sperm (linker length 87 bp). The results were extrapolated to infinite dilution to eliminate interparticle contributions to the scattering. Cross-sectional radii of gyration were found to be 10.9 +/- 0.5, 12.1 +/- 0.4, and 15.9 +/- 0.5 nm for Necturus, chicken, and Thyone chromatin, respectively, which are consistent with fiber diameters of 30.8, 34.2, and 45.0 nm. Mass per unit lengths were found to be 6.9 +/- 0.5, 8.3 +/- 0.6, and 11.8 +/- 1.4 nucleosomes per 10 nm for Necturus, chicken, and Thyone chromatin, respectively. The geometrical consequences of the experimental mass per unit lengths and radii of gyration are consistent with a conserved interaction among nucleosomes. Cross-linking agents were found to have little effect on fiber external geometry, but significant effect on internal structure. The absolute values of fiber diameter and mass per unit length, and their dependencies upon linker length agree with the predictions of the double-helical crossed-linker model. A compilation of all published x-ray scattering data from the last decade indicates that the relationship between chromatin structure and linker length is consistent with data obtained by other investigators.     

ACF catalyses chromatosome movements in chromatin fibres

Nucleosome-remodelling factors containing the ATPase ISWI, such as ACF, render DNA in chromatin accessible by promoting the sliding of histone octamers. Although the ATP-dependent repositioning of mononucleosomes is readily observable in vitro, it is unclear to which extent nucleosomes can be moved in physiological chromatin, where neighbouring nucleosomes, linker histones and the folding of the nucleosomal array restrict mobility. We assembled arrays consisting of 12 nucleosomes or 12 chromatosomes (nucleosomes plus linker histone) from defined components and subjected them to remodelling by ACF or the ATPase CHD1. Both factors increased the access to DNA in nucleosome arrays. ACF, but not CHD1, catalysed profound movements of nucleosomes throughout the array, suggesting different remodelling mechanisms. Linker histones inhibited remodelling by CHD1. Surprisingly, ACF catalysed significant repositioning of entire chromatosomes in chromatin containing saturating levels of linker histone H1. H1 inhibited the ATP-dependent generation of DNA accessibility by only about 50%. This first demonstration of catalysed chromatosome movements suggests that the bulk of interphase euchromatin may be rendered dynamic by dedicated nucleosome-remodelling factors.     

Higher-order structure of long repeat chromatin.

The higher-order structure of chromatin isolated from sea urchin sperm, which has a long nucleosomal DNA repeat length (approximately 240 bp), has been studied by electron microscopy and X-ray diffraction. Electron micrographs show that this chromatin forms 300 A filaments which are indistinguishable from those of chicken erythrocytes (approximately 212 bp repeat); X-ray diffraction patterns from partially oriented samples show that the edge-to-edge packing of nucleosomes in the direction of the 300 A filament axis, and the radial disposition of nucleosomes around it, are both similar to those of the chicken erythrocyte 300 A filament, which is described by the solenoid model. The invariance of the structure with increased linker DNA length is inconsistent with many other models proposed for the 300 A filament and, furthermore, means that the linker DNA must be bent. The low-angle X-ray scattering in the 300-400 A region both in vitro and in vivo differs from that of chicken erythrocyte chromatin. The nature of the difference suggests that 300 A filaments in sea urchin sperm in vivo are packed so tightly together that electron-density contrast between individual filaments is lost; this is consistent with electron micrographs of the chromatin in vitro.     

A triple helix model for the structure of chromatin fiber

A model of chromatin fiber structure is presented in which a repeating unit of a trinucleosome forms a 3-dimensional zigzag. Twisting and compression of the zigzag result in a triple helix structure. The model is built mainly on the flow linear dichroism data showing that nucleosomal disc faces are tilted relative to the fiber axis, the orientation of nucleosomes does not change upon folding and unfolding of chromatin, and the orientation of nucleosomes is maintained by the globular domain of histone H1.     

Higher order folding of chromatin is induced in different ways by monovalent and by bivalent cations

The condensation of the 10 nm chromatin filament in the 30 nm fiber by monovalent cations, polyamines and bivalent cations was studied with light scattering at 90 degrees and flow linear dichroism methods. It was found that monovalent cation- and polyamine-induced folding was a two-step process: a precondensation, when a rotation of nucleosomes takes place only, and a condensation step without changes in nucleosome orientation. Divalent cations affected the structure of chromatin in one step only -- condensation of the chromatin filament being accompanied by nucleosome reorientation.     

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.     

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.     

Organization of internucleosomal DNA in rat liver chromatin

A detailed analysis of the length distribution of DNA in nucleosome dimers trimmed with exonuclease III and S1 nuclease suggests that the previously described variation of internucleosomal distance in rat liver occurs, at least for a subset of the nucleosomes, by integral multiples of the helical repeat of the DNA. Results obtained upon digestion of chromatin with DNase II further suggest that lengths of internucleosomal DNA are integral multiples of the helical repeat of the DNA plus approximately 5 bp. Restraints imposed by these features on the arrangement of nucleosomes along the fiber are discussed.     

Structure of nucleosomes and organization of inter-nucleosomal DNA in chromatin

We have compared mononucleosomes that were obtained by hydrolysis of chromatin micrococcal nuclease from a number of sources with the length of a nucleosomal repeat 185--245 b. p. long. For hydrolysis of chromatin isolated from nuclei, a series of nucleosomes was formed: MN145 (core particle), MN165, MN175...MN205, MN215, the lengths of their DNAs differing (by approximately 10.n b.p. where n = 1, 2, 3...) by a factor of 10. A feature of hydrolysis of chromatin in nuclei was the appearance of an additional H1-depleted MN155 particle. It is suggested that upon isolation of chromatin from nuclei, its partial decompactization takes place. This decompactization changes the character of nuclease splitting and seems to be connected with rearrangement of histone H1. These observations demonstrate that besides core particles MN145 and chromatosomes MN165, the major particles of digest of nuclei appear to be MN155, and for isolated chromatin--MN175. Unlike this standard picture, mainly MN145, MN155, MN235 and MN245 are formed upon hydrolysis of sea urchin sperm nuclei.     

Histone phosphorylation in native chromatin induces local structural changes as probed by electric birefringence

In order to understand how the phosphorylation of histones affects the chromatin structure, we used electron microscopy, sedimentation velocity, circular dichroism and electric birefringence to monitor the salt-induced filament reversible solenoid transition of phosphorylated and native chromatin. Phosphorylation in vitro of chicken erythrocyte chromatin by cyclic-AMP-dependent protein kinase from porcine heart led to the modification of the histones H3 and H5 only, which were modified at a level of one phosphate and about three phosphate groups per molecule, respectively. In contrast to circular dichroism and sedimentation studies, which tend to suggest that phosphorylation of H3 and H5 does not affect chromatin structure, electron microscopy reveals that phosphorylation causes a relaxation of structure at low ionic strength. Electric birefringence and relaxation time measurements clearly prove that local structural changes are induced in chromatin: we observe a decrease of the steady-state birefringence with the appearance of a negative contribution in the signal and a marked increase of the flexibility of fibres. The component with the negative birefringence presents very short relaxation times, like those exhibited by small DNA fragments or individual nucleosomes. Two possibilities are then suggested. First, the conformational change is consistent with what would be expected from the presence of DNA segments loosely associated with the core histone H3. That the length of such segments could correspond to about one to two base-pairs per nucleosome strongly suggests that phosphorylation induces changes affecting some specific H3-DNA interactions only. This result could corroborate previous observations indicating that the N-terminal region of H3, where the site of phosphorylation is located, plays a decisive role in maintaining the superstructure of chromatin. Second, phosphorylation could introduce hinge points between each nucleosome. In this case, the negative birefringence results from partial orientation of the swinging nucleosomes. A possible mode of action of phosphorylation might be to weaken structural restraints imposed by histone H3, thus facilitating further condensation of chromatin.     

Superstructures of wet inactive chromatin and the chromosome surface

Superpacking of chromatin and the surface features of metaphase chromosomes have been studied by SiO replication of wet, unstained, and unfixed specimens in an exceedingly thin (≤ 1 nm) aqueous layer, keeping them wet. Hydrophilic Formvar substrates allow controlled thinning of the aqueous layer covering the wet specimens. Whole mounts of chromatin and chromosomes were prepared by applying a microsurface spreading method to swollen nuclei and mitotic cells at metaphase. The highest level of nucleosome folding of the inactive chromatin in chicken erythrocytes and rat liver nuclei is basically a second-order superhelical organization (width 150–200 nm, pitch distance 50–150 nm) of the elementary nucleosome filament. In unfavorable environments (as determined by ionic agents, fixative, and dehydrating agents) this superstructure collapses into chains of superbeads and beads. Formalin (10%) apparently attacks at discrete sites of chromatin, which are then separated into superbeads. The latter consist of 4–6 nucleosomes and seemingly correspond to successive turns of an original solenoidal coil (width 30–35 nm), which forms the superhelical organization. When this organization is unfolded, eg, in 1–2 mM EDTA, DNAse-sensitive filaments (diameter 1.7 nm) are seen to be wrapped around the nucleosomes. The wet chromosomes in each metaphase spread are held to each other by smooth microtubular fibers, 20–30 nm in diameter. Before they enter into a chromsome, these fibers branch into 9–13 protofilaments, each 5 nm wide. The chromosome surface contains a dense distribution of subunits about 10–25 nm in diameter. This size distribution corresponds to that of nucleosomes and their superbeads. Distinct from this beaded chromosome surface are several smooth, 23–30-nm-diameter fibers, which are longitudinal at the centromere and seem to continue into the chromatid structure. The surface replicas of dried chromosomes do not show these features, which are revealed only in wet chromosomes.     

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.