Transition of chromatin from the "10 nm" lower order structure, to the "30 nm" higher order structure as followed by small angle X-ray scattering

The Dynamic Influence of Linker Histone Saturation within the Poly-Nucleosome Array

Linker histones bind to nucleosomes and modify chromatin structure and dynamics as a means of epigenetic regulation. Biophysical studies have shown that chromatin fibers can adopt a plethora of conformations with varying levels of compaction. Linker histone condensation, and its specific binding disposition, has been associated with directly tuning this ensemble of states. However, the atomistic dynamics and quantification of this mechanism remains poorly understood. Here, we present molecular dynamics simulations of octa-nucleosome arrays, based on a cryo-EM structure of the 30-nm chromatin fiber, with and without the globular domains of the H1 linker histone to determine how they influence fiber structures and dynamics. Results show that when bound, linker histones inhibit DNA flexibility and stabilize repeating tetra-nucleosomal units, giving rise to increased chromatin compaction. Furthermore, upon the removal of H1, there is a significant destabilization of this compact structure as the fiber adopts less strained and untwisted states. Interestingly, linker DNA sampling in the octa-nucleosome is exaggerated compared to its mono-nucleosome counterparts, suggesting that chromatin architecture plays a significant role in DNA strain even in the absence of linker histones. Moreover, H1-bound states are shown to have increased stiffness within tetra-nucleosomes, but not between them. This increased stiffness leads to stronger long-range correlations within the fiber, which may result in the propagation of epigenetic signals over longer spatial ranges. These simulations highlight the effects of linker histone binding on the internal dynamics and global structure of poly-nucleosome arrays, while providing physical insight into a mechanism of chromatin compaction.

Structure of an H1-Bound 6-Nucleosome Array Reveals an Untwisted Two-Start Chromatin Fiber Conformation

Chromatin adopts a diversity of regular and irregular fiber structures in vitro and in vivo. However, how an array of nucleosomes folds into and switches between different fiber conformations is poorly understood. We report the 9.7 Å resolution crystal structure of a 6-nucleosome array bound to linker histone H1 determined under ionic conditions that favor incomplete chromatin condensation. The structure reveals a flat two-start helix with uniform nucleosomal stacking interfaces and a nucleosome packing density that is only half that of a twisted 30-nm fiber. Hydroxyl radical footprinting indicates that H1 binds the array in an on-dyad configuration resembling that observed for mononucleosomes. Biophysical, cryo-EM, and crosslinking data validate the crystal structure and reveal that a minor change in ionic environment shifts the conformational landscape to a more compact, twisted form. These findings provide insights into the structural plasticity of chromatin and suggest a possible assembly pathway for a 30-nm fiber.

Chromatin structure outside and inside the nucleus

The structure of the 30-nm chromatin fiber has provided, over the years, an important reference in chromatin studies. Originally derived from electron microscopic studies of soluble chromatin fibers released by restriction digestion, the gross structural features of such fragments have been supported by biophysical methods such as low angle X-ray and neutron scattering, sedimentation, light scattering, and electric dichroism. Electron microscopy and sedimentation velocity measurements demonstrated that reconstituted chromatin fibers, prepared from repeating arrays of high affinity nucleosome positioning sequences, retain the same overall features as observed for native chromatin fibers. It had been suggested that the 30 nm fiber might be the form assumed in vivo by transcriptionally silent chromatin, but individual gene or genome-wide studies of chromatin released from nuclei do not reveal any such simple correlation. Furthermore, even though the 30 nm fiber has been thought to represent an intermediate in the hierarchical folding of DNA into chromosomes, most analyses of chromatin folding within the nucleus do not detect any regular extended compact structures. However, there are important exceptions in chicken erythroid cell nuclei as well as in transcribed regions that form extended loops. Localized domains within the nucleus, either at the surface of chromosome domains or constrained as a specialized kind of constitutive heterochromatin by specific DNA binding proteins, may adopt 30 nm fiber-like structures.

The "lnc" between 3D chromatin structure and X chromosome inactivation

The long non-coding RNA Xist directs a remarkable instance of developmentally regulated, epigenetic change known as X Chromosome Inactivation (XCI). By spreading in cis across the X chromosome from which it is expressed, Xist RNA facilitates the creation of a heritably silent, heterochromatic nuclear territory that displays a three-dimensional structure distinct from that of the active X chromosome. How Xist RNA attaches to and propagates across a chromosome and its influence over the three-dimensional (3D) structure of the inactive X are aspects of XCI that have remained largely unclear. Here, we discuss studies that have made significant contributions towards answering these open questions.

Centromeric heterochromatin: the primordial segregation machine

Centromeres are specialized domains of heterochromatin that provide the foundation for the kinetochore. Centromeric heterochromatin is characterized by specific histone modifications, a centromere-specific histone H3 variant (CENP-A), and the enrichment of cohesin, condensin, and topoisomerase II. Centromere DNA varies orders of magnitude in size from 125 bp (budding yeast) to several megabases (human). In metaphase, sister kinetochores on the surface of replicated chromosomes face away from each other, where they establish microtubule attachment and bi-orientation. Despite the disparity in centromere size, the distance between separated sister kinetochores is remarkably conserved (approximately 1 μm) throughout phylogeny. The centromere functions as a molecular spring that resists microtubule-based extensional forces in mitosis. This review explores the physical properties of DNA in order to understand how the molecular spring is built and how it contributes to the fidelity of chromosome segregation.

Pericentric chromatin loops function as a nonlinear spring in mitotic force balance

During mitosis, cohesin- and condensin-based pericentric chromatin loops function as a spring network to balance spindle microtubule force.

The mechanisms by which sister chromatids maintain biorientation on the metaphase spindle are critical to the fidelity of chromosome segregation. Active force interplay exists between predominantly extensional microtubule-based spindle forces and restoring forces from chromatin. These forces regulate tension at the kinetochore that silences the spindle assembly checkpoint to ensure faithful chromosome segregation. Depletion of pericentric cohesin or condensin has been shown to increase the mean and variance of spindle length, which have been attributed to a softening of the linear chromatin spring. Models of the spindle apparatus with linear chromatin springs that match spindle dynamics fail to predict the behavior of pericentromeric chromatin in wild-type and mutant spindles. We demonstrate that a nonlinear spring with a threshold extension to switch between spring states predicts asymmetric chromatin stretching observed in vivo. The addition of cross-links between adjacent springs recapitulates coordination between pericentromeres of neighboring chromosomes.

Orienting rigid and flexible biological assemblies in ferrofluids for small-angle neutron scattering studies

Small-angle scattering from macromolecules in solution is widely used to study their structures, but the information content is limited because the molecules are generally randomly oriented and hence the data are spherically averaged. The use of oriented rodlike structures for scattering, as in fiber diffraction, greatly increases the amount of structural detail that can be obtained. A new technique using a ferromagnetic fluid has been developed to align elongated structures independent of their intrinsic magnetic properties. This technique is ideal for small-angle neutron scattering because the scattering from the ferrofluid particles can be reduced significantly by matching the neutron scattering length density of the particles to a D(2)O solvent ("contrast matching"). The net result is scattering primarily from the ordered biological assembly in a solution environment that can be adjusted to physiological pH and ionic strength. Scattering results from ordered tobacco mosaic virus, tobacco rattle virus, and chromain fibers are presented.

The sequentiallity of nucleosomes in the 30 nm chromatin fibre

The folding of eukaryotic DNA into the 30 nm fibre comprises the first level of transcriptionally dormant chromatin. Understanding its structure and the processes of its folding and unfolding is a prerequisite for understanding the epigenetic regulation in cell differentiation. Although the shape of the fibre and its dimensions and mass per unit length have been described, the path of the internucleosomal linker DNA and the sequentiallity of the nucleosomes in the fibre are poorly understood. In the present study, we have chemically crosslinked adjacent nucleosomes along the helix of chicken erythrocyte oligonucleosome fibres, digested the internucleosomal linker DNA and then examined the digestion products by sucrose gradient sedimentation. We found that the digestion products contain considerable amounts of mononucleosomes but less dinucleosomes, which suggests that there are end-discontinuities in the fibres. This can be explained by a nonsequential arrangement of the nucleosomes along the fibre helix.

Chromatin architecture of the human genome: gene-rich domains are enriched in open chromatin fibers

We present an analysis of chromatin fiber structure across the human genome. Compact and open chromatin fiber structures were separated by sucrose sedimentation and their distributions analyzed by hybridization to metaphase chromosomes and genomic microarrays. We show that compact chromatin fibers originate from some sites of heterochromatin (C-bands), and G-bands (euchromatin). Open chromatin fibers correlate with regions of highest gene density, but not with gene expression since inactive genes can be in domains of open chromatin, and active genes in regions of low gene density can be embedded in compact chromatin fibers. Moreover, we show that chromatin fiber structure impacts on further levels of chromatin condensation. Regions of open chromatin fibers are cytologically decondensed and have a distinctive nuclear organization. We suggest that domains of open chromatin may create an environment that facilitates transcriptional activation and could provide an evolutionary constraint to maintain clusters of genes together along chromosomes.

Computational modeling predicts the structure and dynamics of chromatin fiber

BACKGROUND

The compact form of the chromatin fiber is a critical regulator of fundamental processes such as transcription and replication. These reactions can occur only when the fiber is unraveled and the DNA strands contained within are exposed to interact with nuclear proteins. While progress on identifying the biochemical mechanisms that control localized folding and hence govern access to genetic information continues, the internal structure of the chromatin fiber, let alone the structural pathways for folding and unfolding, remain unknown.

RESULTS

To offer structural insights into how this nucleoprotein complex might be organized, we present a macroscopic computer model describing the mechanics of the chromatin fiber on the polymer level. We treat the core particles as electrostatically charged disks linked via charged elastic DNA segments and surrounded by a microionic hydrodynamic solution. Each nucleosome unit is represented by several hundred charges optimized so that the effective Debye-Hückel electrostatic field matches the field predicted by the nonlinear Poisson-Boltzmann equation. On the basis of Brownian dynamics simulations, we show that oligonucleosomes condense and unfold in a salt-dependent manner analogous to the chromatin fiber.

CONCLUSIONS

Our predicted chromatin model shows good agreement with experimental diffusion coefficients and small-angle X-ray scattering data. A fiber of width 30 nm, organized in a compact helical zigzag pattern with about 4 nucleosomes per 10 nm, naturally emerges from a repeating nucleosome folding motif. This fiber has a cross-sectional radius of gyration of R(c) = 8.66 nm, in close agreement with corresponding values for rat thymus and chicken erythrocyte chromatin (8.82 and 8.5 nm, respectively).

Analytical ultracentrifugation and the characterization of chromatin structure

This mini review consists of two parts. The first part will provide a brief overview of the theoretical aspects involved in the two kinds of experiments that can be conducted with the analytical ultracentrifuge (sedimentation velocity and sedimentation equilibrium) as they pertain to the study of chromatin. In the following sections, I describe the analytical ultracentrifuge experiments which, in my opinion, have contributed the most to our understanding of chromatin. Few other biophysical techniques, with the exception of X-ray scattering and diffraction, have contributed as extensively as the analytical ultracentrifuge to the characterization of so many different aspects of chromatin structure. In the course of his scientific career, Professor Henryk Eisenberg has made many important contributions to the theoretical aspects underlying ultracentrifuge analysis, especially in the analysis of solutions of polyelectrolytes and biological macromolecules [H. Eisenberg, Biological macromolecules and polyelectrolytes in solution, Clarendon Press, Oxford, 1976]. As an example he has devoted some of his research effort to the characterization of chromatin in solution. This review includes these important contributions.

Effect of in vivo histone hyperacetylation on the state of chromatin fibers

We evaluated the contribution of in vivo histone acetylation to the folding of chromatin into its higher-order structures. We have compared high-order folding patterns of hyperacetylated vs. unmodified chromatin in living green monkey kidney cells (CV1 line) using intercalator chloroquine diphospate to induce alterations in the twist of internucleosomal linker DNA. We have shown that histone hyperacetylation induced by antibiotic Trichostatin A significantly alters intercalator-mediated chromatin folding pattern.

X-ray small angle scattering study of chromatin as a function of fiber length

This work investigates the structure of native calf thymus chromatin as a function of fiber length and isolation procedures by using X-ray small angle scattering technique. Two methods of chromatin isolation have been compared in order to better understand the differences reported by various authors in terms of chromatin high order structure. In addition to these experimental results the effects of shearing have also been studied. In order to explain the differences among these chromatin preparations we built several models of chromatin fibers (represented as a chain of spherical subunits) assuming increasing level of condensation at increasing salt concentrations. For all these fiber models the corresponding theoretical X-ray scattering curves have been calculated and these results have been used to explain the influence of fiber length on the scattering profiles of chromatin. The comparison between experimental and theoretical curves confirms that the high molecular weight chromatin-DNA prepared by hypotonic swelling of nuclei (without enzymatic digestion) displays a partially folded structure even at low ionic strength, whereas the low molecular weight chromatin-DNA prepared by a brief nuclease digestion appears very weakly folded at the same ionic conditions.

Electrophoresis of chromatin on nondenaturing agarose gels containing Mg2+. Self-assembly of small chromatin fragments and folding of the 30-nm fiber

We show that nondenaturing agarose gels can be used for the study of the structure and dynamic properties of native (uncross-linked) chromatin. In gels containing 1.7 mM Mg2+, chicken erythrocyte chromatin fragments having from about 6 to 50 nucleosomes produce well defined bands. These bands have an electrophoretic mobility that decreases only slightly with molecular weight. This surprising behavior is not observed in low ionic strength gels. Fragments with less than 6 nucleosomes and low content of histones H1-H5 give rise to broad bands in gels with Mg2+. In contrast, fragments containing only 3-4 nucleosomes but with the normal H1-H5 content are able to form associated structures with a mobility similar to that observed for high molecular weight chromatin. Electron microscopy results indicate that the associated fragments and the fragments of higher molecular weight show similar electrophoretic properties because they become very compact in the presence of Mg2+ and form cylindrical structures with a diameter of approximately 33 nm. Our results suggest that the interactions involved in the self-assembly of small fragments are the same that direct the folding of larger fragments; in both cases, the resulting compact chromatin structure is formed from a basic element containing 5-7 nucleosomes.

A chromatin folding model that incorporates linker variability generates fibers resembling the native structures

The "30-nm" chromatin fibers, as observed in eukaryotic nuclei, are considered a discrete level in a hierarchy of DNA folding. At present, there is considerable debate as to how the nucleosomes and linker DNA are organized within chromatin fibers, and a number of models have been proposed, many of which are based on helical symmetry and imply specific contacts between nucleosomes. However, when observed in nuclei or after isolation, chromatin fibers show considerable structural irregularity. In the present study, chromatin folding is considered solely in terms of the known properties of the nucleosome-linker unit, taking into account the relative rotation between consecutive nucleosomes that results from the helical twist of DNA. Model building based on this premise, and with a constant length of linker DNA between consecutive nucleosomes, results in a family of fiber- and ribbon-like structures. When the linker length between nucleosomes is allowed to vary, as occurs in nature, fibers showing the types of irregularity observed in nuclei and in isolated chromatin are created. The potential application of the model in determining the three-dimensional organization of chromatin in which nucleosome positions are known is discussed.

Interpretation of the X-ray scattering profiles of chromatin at various NaCl concentrations by a simple chain model

In order to interpret the change in the X-ray scattering profiles from rat thymus chromatin, extensive model calculation was carried out. Chromatin is modelled as a string of subunits (nucleosomes) in which disorder is introduced into the positions of adjacent subunits. Disposition parameters characterizing the arrangement of subunits were estimated for various states of chromatin, so that the main feature of the scattering profiles is described. The result indicated that the structure of chromatin changes, as the NaCl concentration increases, from the extended "beads-on-a string" structure to the condensed helical structure. The latter has an outer diameter of about 26 nm with 3-4 nucleosomes per turn. In the intermediate state, it has a loose helical structure. The estimation of disorder suggested that the arrangement of subunits is appreciably disordered even in the condensed helical filament at 50 mM NaCl. Our model for chromatin condensation seems to support models of the "crossed linker" type.

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.

The diameters of frozen-hydrated chromatin fibers increase with DNA linker length: evidence in support of variable diameter models for chromatin

The diameters of chromatin fibers from Thyone briareus (sea cucumber) sperm (DNA linker length, n = 87 bp) and Necturus maculosus (mudpuppy) erythrocytes (n = 48 bp) were investigated. Soluble fibers were frozen into vitrified aqueous solutions of physiological ionic strength (124 mM), imaged by cryo-EM, and measured interactively using quantitative computer image-processing techniques. Frozen-hydrated Thyone and Necturus fibers had significantly different mean diameters of 43.5 nm (SD = 4.2 nm; SEM = 0.61 nm) and 32.0 nm (SD = 3.0 nm; SEM = 0.36 nm), respectively. Evaluation of previously published EM data shows that the diameters of chromatin from a large number of sources are proportional to linker length. In addition, the inherent variability in fiber diameter suggests a relationship between fiber structure and the heterogeneity of linker length. The cryo-EM data were in quantitative agreement with space-filling double-helical crossed-linker models of Thyone and Necturus chromatin. The data, however, do not support solenoid or twisted-ribbon models for chromatin that specify a constant 30 nm diameter. To reconcile the concept of solenoidal packing with the data, we propose a variable-diameter solid-solenoid model with a fiber diameter that increases with linker length. In principle, each of the variable diameter models for chromatin can be reconciled with local variations in linker length.

Interaction of HMG14 with chromatin

Neutron scattering has been used to study the interaction of HMG14 with chromatin. Chromatin depleted of H1/H5 was reconstituted separately with histones H1 and H5, and complexed with HMG14. We have also studied the conformation of complexes formed by the binding of HMG14 to nucleosome dimers without linker DNA. Our data on the binding of HMG14 to linkerless nucleosome dimers argue against a significant change in the exit and entry angles of nucleosomal core DNA. Data on the condensation of chromatin into a higher-order structure suggest that there is no dramatic difference between the roles of H1 and H5 in their influence on HMG14 complex formation. However, there is a decrease of about 25% in the mass per unit length of chromatin fibers on HMG14 binding, which is not accompanied by a change in the fiber repeat distance. This is evidence that there are fewer nucleosomes per repeat in HMG14 containing chromatin fibers than in normal chromatin. Alteration of chromatin structure in this manner may be part of the role of HMG14 in actively transcribed chromatin.

Thermodynamics and the structure of biological macromolecules. Rozhinkes mit mandeln

In this review, I will discuss the role of thermodynamics in both the determination and evaluation of the structure of biological macromolecules. The presentation relates to the historical context, state-of-the-art and projection into the future. Fundamental features relate to the effect of charge, exemplified in the study of synthetic and natural polyelectrolytes. Hydrogen bonding and water structure constitute basic aspects of the medium in which biological reactions occur. Viscosity is a classical tool to determine the shape and size of biological macromolecules. The thermodynamic analysis of multicomponent systems is essential fo the correct understanding of the behavior of biological macromolecules in solution and for the evaluation of results from powerful experimental techniques such as ultracentrifugation, light, X-ray and neutron scattering. The hydration, shape and flexibility of DNA have been studied, as well as structural transitions in nucleosomes and chromatin. A particularly rewarding field of activity is the study of unusual structural features of enzymes isolated from the extreme halophilic bacteria of the Dead Sea, which have adapted to saturated concentrations of salt. Future studies in various laboratories will concentrate on nucleic-acid--protein interactions and on the so-called 'crowding effect', distinguishing the behavior in bacteria, or other cells, from simple test-tube experiments.

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.

Structural studies of proteins by high-flux X-ray and neutron solution scattering

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The superstructure of chromatin and its condensation mechanism. V. Effect of linker length, condensation by multivalent cations, solubility and electric dichroism properties

Comparison between the internucleosomal distance found by X-ray solution scattering for chicken erythrocyte (23 nm) and sea urchin (30 nm) chromatin indicates that this distance is proportional to the linker length. The diameter of the condensed sea urchin chromatin fibers is about 45 nm which is significantly larger than in chicken erythrocyte chromatin (35 nm). Trivalent cations (Gd, Tb, Cr) and polyamines spermine and spermidine were found to induce compaction at much lower concentrations than the divalent cations but Gd, Tb, Cr induce aggregation before full compaction of the fibers. The influence of hydrogen bonding is illustrated by comparison of the effects of NaCl, ammonium chlorides on condensation. Solubility experiments indicate that there is a nearly linear dependence of the Mg++ concentration at which precipitation occurs on chromatin concentration and confirm the differences between cations observed by X-ray scattering. The chicken erythrocyte chromatin samples were further characterized by their reduced electric dichroism. The values found are consistent with the model derived from X-ray scattering and are compared with those reported in the literature.

Comparative study of the condensation of chicken erythrocyte and calf thymus chromatins by di- and multivalent cations

The condensation of chicken erythrocyte (CE) and calf thymus (CT) chromatins upon addition of di- and multivalent cations has been studied using turbidity, precipitation and electric dichroism measurements. For all the cations investigated (Mg2+, Tb3+, Co(NH3)6(3+), spermidine Spd2+ and spermine Sp4+) condensation of CE chromatin occurred before the onset of aggregation, while aggregation of CT chromatin started before condensation with all cations except Mg2+ and Tb3+. Precipitation of CE chromatin required lower di- and multivalent cations concentrations than CT chromatin. The electric dichroism data for both chromatins, at low ionic strength in the absence of di- or multivalent cations, indicated that the nucleoprotein molecules were not totally decondensed but that a "precondensed" state was already present. A positive electric dichroism was observed for the most condensed chromatin fibers, in agreement with the "cross-linker" models. Tb3+ led to less compact condensed particles as judged from the electric dichroism observations, but electron microscopy revealed that "30 nm fibers" were formed. Very little aggregation was produced by Tb3+. On the contrary, spermine produced very large networks of condensed molecules, but large spheroidal particles were also observed. The condensation of CE chromatin happened without changes of solution conductivity upon cation salt addition, regardless of the condensing cation, indicating a cooperative uptake of the ions during this process.

The superstructure of chromatin and its condensation mechanism. IV. Enzymatic digestion, thermal denaturation, effect of netropsin and distamycin

Changes in the structure of chicken erythrocyte chromatin fibres at low ionic strength resulting from enzymatic digestion, thermal denaturation and binding of Netropsin and Distamycin were monitored by synchrotron X-ray solution scattering. Digestion with micrococcal nuclease confirms the previous assignment of the 0.05 nm-1 band to an interference between nucleosomes with an average distance of 23 nm. The results of thermal denaturation indicate that above 40 degrees C there is a progressive increase of the internucleosomal distance and that above 60 degrees C the characteristic structure of the chromatin fibre is destroyed. Binding of Netropsin and Distamycin also results in an increase of the internucleosomal distance which can be estimated to correspond to about 0.2 nm/mol.

Chromatin structures: dissecting their mixed patterns in nuclease digests

Four separate features could be distinguished in Fe-DNAase-1 digestions of human lymphoblast nuclei: a di-nucleosomal (2N) repeat, a mono-nucleosomal (1N) repeat, a component of "random" DNA, and triple splitting of major peaks. The random component is major, is unlikely to be completely artifactual, and is what would be expected from the face to face layering model of Subirana et. al., (1). The 2N pattern appeared to be associated with compact, metaphase-type chromatin, whereas the 1N pattern was associated with more exposed chromatin. These two modes are explained in terms of orderly back-to-back folding of zig-zag nucleofilaments, and face-to-face folding respectively. Hybridization studies indicated that the centromeric classes of repetitive DNA had the same digestion spectra as the major interspersed classes of repetitive DNA, and DNA enriched in transcriptionally active sequences. It is suggested that current coil models are all inadequate explanations of higher order chromatin packing.