Radial density distribution of chromatin: evidence that chromatin fibers have solid centers

Fiber diameter, radial distribution of density, and radius of gyration were determined from scanning transmission electron microscopy (STEM) of unstained, frozen-dried chromatin fibers. Chromatin fibers isolated under physiological conditions (ionic strength, 124 mM) from Thyone briareus sperm (DNA linker length, n = 87 bp) and Necturus maculosus erythrocytes (n = 48 bp) were analyzed by objective image-processing techniques. The mean outer diameters were determined to be 38.0 nm (SD = 3.7 nm; SEM = 0.36 nm) and 31.2 nm (SD = 3.6 nm; SEM = 0.32 nm) for Thyone and Necturus, respectively. These data are inconsistent with the twisted-ribbon and solenoid models, which predict constant diameters of approximately 30 nm, independent of DNA linker length. Calculated radial density distributions of chromatin exhibited relatively uniform density with no central hole, although the 4-nm hole in tobacco mosaic virus (TMV) from the same micrographs was visualized clearly. The existence of density at the center of chromatin fibers is in strong disagreement with the hollow-solenoid and hollow-twisted-ribbon models, which predict central holes of 16 and 9 nm for chromatin of 38 and 31 nm diameter, respectively. The cross-sectional radii of gyration were calculated from the radial density distributions and found to be 13.6 nm for Thyone and 11.1 nm for Necturus, in good agreement with x-ray and neutron scattering. The STEM data do not support the solenoid or twisted-ribbon models for chromatin fiber structure. They do, however, support the double-helical crossed-linker models, which exhibit a strong dependence of fiber diameter upon DNA linker length and have linker DNA at the center.     

Structural organization of the sperm chromatin in a fern (Scolopendrium vulgare) studied by spreading methods

To investigate chromatin organization, we applied the spreading techniques to nuclei isolated from Scolopendrium spermatozoids. Well-dispersed chromatin shows three types of fibers: beaded fibers corresponding to a nucleosomal filament with adjacent nucleosomes in close contact, smooth fibers (14 nm in diameter) associated in a complex network, and knobby fibers constituted by local supercoiling of a very thin (4 nm) smooth filament. Along the knobby fibers, beads of variable size are irregularly spaced. The knobby fibers lie parallel and coalesce in thick bundles. The sperms basic proteins identified by electrophoretic analysis probably promote the supercoiling and the side-to-side attachment of the knobby fibers, which are all the more abundant in spread preparations. These results indicate that knobby fibers are probably located in the outer part of the sperm nucleus in which the chromatin is densely packed. As for the nucleosomal and smooth filaments, they may be situated in the inner part.     

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.     

T-DNA of a crown gall tumor is organized in nucleosomes

Nucleosomes were isolated from chromatin of suspension cultured cells of Nicotiana tabacum var. White Burley, which were either habituated or transformed by Agrobacterium tumefaciens, strain T37. Chromatin repeat length in both types of tissue was identical and can be estimated to be 195 ± 10 bp. Using Southern transfer of nucleosomal DNA and hybridization with cloned nick-translated HindIII fragments of pTi C58 we show that the T-DNA originating from the Ti-plasmid of A. tumefaciens is organized in nucleosomes within the chromatin of crown gall tumor cells.     

Ultrastructural organization of heterochromatin within sea urchin sperm nuclei

Chromatin within swollen or lysed isolated sperm nuclei of the sea urchin, Strongylocentrotus purpuratus, was examined by electron microscopy. Spread preparations of lysed sperm nuclei demonstrated dense aggregates of nondispersed material and beaded filaments radiating from these aggregates. These beaded fibers are similar in size and appearance to the “beads-on-a-string” seen as characteristic of chromatin spreads from numerous interphase nuclei. The beads are nucleosomes that have an average diameter of 130 Å. The interconnecting string is 40 Å indiameter and corresponds to the spacer DNA. In thin sections of swollen nuclei the sperm chromatin appears to be composed of 400 Å superbeads that are closely apposed to form 400 Å fibers. As the chromatin disperses, the superbeads are seen to be attached to one another by chromatin fibers of 110 Å diameter. In thin sections, the 400 Å superbeads appear to disperse directly into the 110 Å fibers with no intervening structures. This work demonstrates that the heterochromatin in Strongylocentrotus purpuratus sperm nuclei is composed of nucleosomes that form 100 Å filaments that are compacted into 400 Å superbeads. The superbeads coalesce to give the morphological appearance of 400 Å fibers.     

An all-atom model of the chromatin fiber containing linker histones reveals a versatile structure tuned by the nucleosomal repeat length

In the nucleus of eukaryotic cells, histone proteins organize the linear genome into a functional and hierarchical architecture. In this paper, we use the crystal structures of the nucleosome core particle, B-DNA and the globular domain of H5 linker histone to build the first all-atom model of compact chromatin fibers. In this 3D jigsaw puzzle, DNA bending is achieved by solving an inverse kinematics problem. Our model is based on recent electron microscopy measurements of reconstituted fiber dimensions. Strikingly, we find that the chromatin fiber containing linker histones is a polymorphic structure. We show that different fiber conformations are obtained by tuning the linker histone orientation at the nucleosomes entry/exit according to the nucleosomal repeat length. We propose that the observed in vivo quantization of nucleosomal repeat length could reflect nature's ability to use the DNA molecule's helical geometry in order to give chromatin versatile topological and mechanical properties.     

The effect of various conditions of chromatin isolation on the nucleosomal structure of the isolated chromatin

Chromatin from calf thymus isolated under hypotonic conditions in the presence of various agents was investigated by methods of electron microscopy prior to and after EDTA treatment. It is shown that the presence of chelating agents and, especially, the application of considerable mechanical forces in the course of isolation may cause damage to the nucleosomal structure of the chromatin. Moreover, sufficiently great mechanical forces are liable to destroy the structure of the chromatin nucleosomal fibres even when they are packed in structures of a higher order of organization of the chromatin.     

Direct measurement of local chromatin fluidity using optical trap modulation force spectroscopy

Chromatin assembly is condensed by histone tail-tail interactions and other nuclear proteins into a highly compact structure. Using an optical trap modulation force spectroscopy, we probe the effect of tail interactions on local chromatin fluidity. Chromatin fibers, purified from mammalian cells, are tethered between a microscope coverslip and a glass micropipette. Mechanical unzipping of tail interactions, using the micropipette, lead to the enhancement of local fluidity. This is measured using an intensity-modulated optically trapped bead positioned as a force sensor on the chromatin fiber. Enzymatic digestion of the histone tail interactions of tethered chromatin fiber also leads to a similar increase in fluidity. Our experiments show that an initial increase in the local fluidity precedes chromatin decompaction, suggesting possible mechanisms by which chromatin-remodeling machines access regulatory sites.     

Chromatin under mechanical stress: from single 30 nm fibers to single nucleosomes

About a decade ago, the elastic properties of a single chromatin fiber and, subsequently, those of a single nucleosome started to be explored using optical and magnetic tweezers. These techniques have allowed direct measurements of several essential physical parameters of individual nucleosomes and nucleosomal arrays, including the forces responsible for the maintenance of the structure of both the chromatin fiber and the individual nucleosomes, as well as the mechanism of their unwinding under mechanical stress. Experiments on the assembly of individual chromatin fibers have illustrated the complexity of the process and the key role of certain specific components. Nevertheless a substantial disparity exists in the data reported from various experiments. Chromatin, unlike naked DNA, is a system which is extremely sensitive to environmental conditions, and studies carried out under even slightly different conditions are difficult to compare directly. In this review we summarize the available data and their impact on our knowledge of both nucleosomal structure and the dynamics of nucleosome and chromatin fiber assembly and organization.     

Sperm histones and chromatin structure of the "primitive" sea urchin Eucidaris tribuloides

The "primitive" sea urchin Eucidaris tribuloides resembles the advanced sea urchins (euechinoids) in many respects, yet some features of its biochemistry and morphogenesis are more similar to other echinoderms such as starfish or sea cucumbers. Two unique characteristics of the sperm chromatin of all known euechinoids are an extremely long average nucleosomal repeat length and the presence of two male germ-line-specific histone variants, Sp H1 and Sp H2B. Histone composition and nucleosomal repeat length of the sperm chromatin of Eucidaris were compared to those of several euechinoids and a starfish. Eucidaris sperm chromatin contained large H1 and H2B histone variants typical of euechinoids. The H1 was about nine amino acids smaller than Sp H1 of the advanced urchin Strongylocentrotus purpuratus. Its Sp H2B molecules were the same size as in the euechinoids. Peptide maps showed that N-terminal regions of Sp H1 and Sp H2B contained repeating basic amino acid motifs characteristic of euechinoids. The smaller size of Eucidaris H1 is accounted for by a smaller C-terminal region. The repeat length of Eucidaris sperm chromatin was slightly shorter than that of two euechinoids, but significantly larger than starfish, which lacks a large H2B. The Sp H2B gene of Eucidaris was expressed during spermatogenesis in the same cell types as for S. purpuratus. Thus Sp histone subtype expression and chromatin structure in this distantly related echinoid closely resemble the euechinoids. The presence of an Sp H2B and a very long repeat length appear to be characteristic of the echinoids only.     

Sperm-chromatin maturation in the mouse. A cytochemical approach

Cytochemical techniques were used to study chromatin during spermiogenesis and sperm maturation in the mouse, starting from the stages at which the substitution of somatic histones by testis-specific proteins occurs. It was possible to distinguish and analyze the different temporal incidence of two processes involved in sperm maturation, i.e. chromatin condensation (a tridimensional highly compacted arrangement) and chromatin stabilization (a tough structure, which protects the genome DNA). The first process, involving a reduction in the nuclear size and a decrease in the amount of sperm DNA accessible to specific cytochemical reactions and stainings, was found to reach its maximum in caput-epididymidis spermatozoa, in which electron microscopy revealed that the sheared chromatin was mainly organized into 120-A-thick knobby fibers. No further changes were found in sperm up to their appearance in the fallopian tubes. On the contrary, chromatin stabilization, the onset of which occurs in the testis (at the late spermatid stage) via the formation of -S-S- cross-links, is completed in the vas deferens, where chromatin has a superstructure consisting of thicker fibers, with diameters of 210 and 350 A. The reductive cleavage of disulfides in vas-deferens spermatozoa does not completely destroy the superstructure of sperm chromatin, which could indicate 'coiling' of the basic knobby fiber. In fact, when the ion concentration was increased, the chromatin of vas-deferens spermatozoa appeared to be organized into fibers with diameters similar to those of the caput epididymidis. This unique organization of mature sperm chromatin should have an essential role in the fast swelling of spermatozoa during fertilization.     

The organization of oligonucleosomes in yeast

We have developed a method of preparing yeast chromatin that facilitates the analysis of nucleoprotein organization. Yeast chromatin, isolated as an insoluble complex, is digested with micrococcal nuclease and fractionated into major insoluble and soluble fractions. No nucleosomal repeat is seen early in digestion for the insoluble fraction. Nucleosomal complexes of the soluble fraction are excised by nuclease in a distinctive non-random pattern; they are markedly depleted in mononucleosomes. When we analyze the soluble material by high resolution native electrophoresis, we find that the nucleoproteins resolve into two bands for each DNA multimer of the nucleosomal repeat. Our results suggest that there are structural similarities between bulk yeast chromatin and chromatin configurations found in transcribing genes of complex eukaryotes.     

Ultrastructural analysis of mouse sperm chromatin

Chromatin organization was studied during the maturation processes in the epididymis and vas deferens; these processes lead to a potentially reversible inactivation of the genome. There are progressive increases in resistance to detergent action and -S-S- bridge reduction in both head membranes and chromatin. In all the sites studied, there was a basic "knobby" chromatin fiber of 110 A diameter. In the caput epididymidis only, in addition to the knobby fibers, there were some smooth fibers, which can be considered as markers of a transient situation in which the stabilization of DNA/protamine interactions has not completely been achieved. In the vas deferens, the knobby fibers, the diameters of which are multiples of that of the basic one, can be converted to single units by increasing the ionic strength.     

Chromatin fibers are left-handed double helices with diameter and mass per unit length that depend on linker length

Four classes of models have been proposed for the internal structure of eukaryotic chromosome fibers--the solenoid, twisted-ribbon, crossed-linker, and superbead models. We have collected electron image and x-ray scattering data from nuclei, and isolated chromatin fibers of seven different tissues to distinguish between these models. The fiber diameters are related to the linker lengths by the equation: D(N) = 19.3 + 0.23 N, where D(N) is the external diameter (nm) and N is the linker length (base pairs). The number of nucleosomes per unit length of the fibers is also related to linker length. Detailed studies were done on the highly regular chromatin from erythrocytes of Necturus (mud puppy) and sperm of Thyone (sea cucumber). Necturus chromatin fibers (N = 48 bp) have diameters of 31 nm and have 7.5 +/- 1 nucleosomes per 10 nm along the axis. Thyone chromatin fibers (N = 87 bp) have diameters of 39 nm and have 12 +/- 2 nucleosomes per 10 nm along the axis. Fourier transforms of electron micrographs of Necturus fibers showed left-handed helical symmetry with a pitch of 25.8 +/- 0.8 nm and pitch angle of 32 +/- 3 degrees, consistent with a double helix. Comparable conclusions were drawn from the Thyone data. The data do not support the solenoid, twisted-ribbon, or supranucleosomal particle models. The data do support two crossed-linker models having left-handed double-helical symmetry and conserved nucleosome interactions.     

Nucleosome packing in interphase chromatin.

Higher-order chromatin fibers (200--300 A in diameter) are reproducibly released from nuclei after lysis in the absence of formalin and/or detergent. Electron microscope analysis of these fibers shows that they are composed of a continuous array of closely apposed nucleosomes which display several distinct packing patterns. Analysis of the organization of nucleosomes within these arrays and their distribution along long stretches of chromatin suggest that the basic 100-A chromatin fiber is not packed into discrete superbeads and is not folded into a uniform solenoid within the native 250-A fiber. Furthermore, because similar higher-order fibers have been visualized in metaphase chromosomes, the existence of this fiber class appears to be independent of the degree of in vivo chromatin condensation.     

Aggregation of mono- and dinucleosomes into chromatin-like fibers

Three classes of chicken erythrocyte chromatin particles differing in their content of lysine-rich histones and/or spacer DNA have been studied in order to determine their ability to aggregate into complexes resembling those observed in native chromatin. The complexes have been obtained in the presence of MgCl₂ and NaCl and studied by electron microscopy. Mononucleosomes, containing spacer DNA and histones H1 and H5, give rise to thick (about 70 nm) ellipsoidal particles in the presence of 0.5 mM MgCl₂. These particles are disrupted by the addition of small amounts of NaCl (5–20 mM). On the other hand in 0.5 mM MgCl₂ dinucleosomes give rise to regular fibrous complexes of about 40 nm in diameter which are very similar to native chromatin fibers. These complexes are much more stable when NaCl is added. We conclude that for the stability of nucleosomal aggregates, similar to native chromatin fibers, a continuity of DNA structure is not required, but the presence of divalent cations, spacer DNA and lysine-rich histones is essential.     

The silent information regulator 3 protein, SIR3p, binds to chromatin fibers and assembles a hypercondensed chromatin architecture in the presence of salt

The telomeres and mating-type loci of budding yeast adopt a condensed, heterochromatin-like state through recruitment of the silent information regulator (SIR) proteins SIR2p, SIR3p, and SIR4p. In this study we characterize the chromatin binding determinants of recombinant SIR3p and identify how SIR3p mediates chromatin fiber condensation in vitro. Purified full-length SIR3p was incubated with naked DNA, nucleosome core particles, or defined nucleosomal arrays, and the resulting complexes were analyzed by electrophoretic shift assays, sedimentation velocity, and electron microscopy. SIR3p bound avidly to all three types of templates. SIR3p loading onto its nucleosomal sites in chromatin produced thickened condensed fibers that retained a beaded morphology. At higher SIR3p concentrations, individual nucleosomal arrays formed oligomeric suprastructures bridged by SIR3p oligomers. When condensed SIR3p-bound chromatin fibers were incubated in Mg(2+), they folded and oligomerized even further to produce hypercondensed higher-order chromatin structures. Collectively, these results define how SIR3p may function as a chromatin architectural protein and provide new insight into the interplay between endogenous and protein-mediated chromatin fiber condensation pathways.