Higher-order chromatin structure of human granulocytes

The structural organisation of chromatin in eukaryotes plays an important role in a number of biological processes. Our results provide a comprehensive insight into the nuclear topography of human peripheral blood granulocytes, mainly neutrophils. The nuclei of granulocytes are characterised by a segmented shape consisting of two to five lobes that are in many cases connected by a thin DNA-containing filament. The segregation of chromosomes into the nuclear lobes was studied using fluorescence in situ hybridisation (FISH). We were able to distinguish different topographic types of granulocytes on the basis of the pattern of segregation. Five topographic types were detected using dual-colour FISH in two-lobed nuclei. The segregation of four sets of genetic structures could be studied with the aid of repeated FISH and a large number of topographic types were observed. In all these experiments a non-random distribution of chromosomes into nuclear lobes was found. The painting of a single type of chromosome in two-lobed nuclei showed the prevalence of symmetric topographic types (on average in 65.5% of cases) with significant variations among individual chromosomes. The results of analysis of five topographic types (defined by two chromosomes in two-lobed nuclei) showed that the symmetric topographic types for both chromosomes are significantly more frequent than predicted. Repeated hybridisation experiments confirmed that the occurrence of certain patterns of chromosome segregation is much higher than that predicted from the combination of probabilities. The frequency of symmetric topographic types for chromosome domains was systematically higher than for genes located on these chromosomes. It appears that the prevalence of symmetric segregation patterns is more probable for large objects such as chromosome domains than for genes located on chromatin loops extending outwards from the surface of the domain defined by specific chromosome paints. This means that one chromosome domain may occur in different lobes of granulocytic nuclei. This observation is supported by the fact that both genes and centromeres were observed on filaments joining different lobes. For all chromosomes, the distances between the membrane and fluorescence gravity centre of the chromosome were measured and correlated with the segregation patterns. A higher percentage of symmetric topographic types was found in those chromosomes that were located closer to the nuclear membrane. Nuclear positioning of all genetic elements in granulocytic nuclei was studied in two-dimensional projection; however, the results were verified using three-dimensional analysis.     

Higher-order structure of chromatin and chromosomes

The linear array of nucleosomes that comprises the primary structure of chromatin is folded and condensed to varying degrees in nuclei and chromosomes forming 'higher order structures'. We discuss the recent findings from novel experimental approaches that have yielded significant new information on the different hierarchical levels of chromatin folding and their functional significance.     

Higher-order structure of nucleosome oligomers from short-repeat chromatin

Sedimentation measurements and electron microscopy at a series of ionic strengths suggest that chromatin from neurons of the cerebral cortex is able to form condensed structures in vitro that are probably several turns of a solenoid with about six nucleosomes per turn. Since neuronal chromatin has a short nucleosomal repeat (approximately 165 bp) allowing virtually no linker DNA between nucleosomes, and yet forms apparently 'normal' elements of solenoid, the packing of nucleosomes in the solenoid must be highly constrained. This permits only a limited number of possible models, and enables tentative suggestions to be made about the location of the linker DNA in the typical solenoid.     

Higher-order chromatin structure: bridging physics and biology

Advances in microscopy and genomic techniques have provided new insight into spatial chromatin organization inside of the nucleus. In particular, chromosome conformation capture data has highlighted the relevance of polymer physics for high-order chromatin organization. In this context, we review basic polymer states, discuss how an appropriate polymer model can be determined from experimental data, and examine the success and limitations of various polymer models of higher-order interphase chromatin organization. By taking into account topological constraints acting on the chromatin fiber, recently developed polymer models of interphase chromatin can reproduce the observed scaling of distances between genomic loci, chromosomal territories, and probabilities of contacts between loci measured by chromosome conformation capture methods. Polymer models provide a framework for the interpretation of experimental data as ensembles of conformations rather than collections of loops, and will be crucial for untangling functional implications of chromosomal organization.     

Higher-order structure of mammalian chromatin deduced from viscoelastometry data

The results of viscoelastometry (VE) for mammalian DNA have been puzzling because they have two orders of magnitude smaller measured viscoelastic relaxation times for mammalian chromosomes than that expected for DNA linear coils of chromosomal size. In an attempt to resolve this discrepancy, we have applied a recent model of G1 chromosome structure (J.Y. Ostashevsky, Mol Biol. Cell 9, 3031-3040, 1998) in which the 30 nm chromatin fiber of each chromosome forms a string of loop clusters (micelles). This model has two parameters: the number of loops per micelle (f) and the average loop size (Mf), which can be estimated independently from VE data. Using our VE data for plateau phase V79 Chinese hamster cells (unirradiated and X-irradiated with doses up to 40 Gy) we show that f approximately 13 , which is close to other estimates made using the model (f ranges from 10-20), and Mf approximately 2 Mbp, which is similar to estimates made from our nucleoid data (1.3 Mbp) and to estimates made in the literature using a variety of techniques (1-3 Mbp).     

Higher-order structures of chromatin in solution.

Neutron scatter studies have been made on gently prepared chicken erythrocyte chromatin over a range of ionic strength. At low ionic strength the mass per unit length of the '10 nm nucleofilament corresponds to one nucleosome per 8--12 nm and a DNA packing ratio of between 6 and 9. From the contrast dependence of the cross-section radius of gyration of the nucleofilament the following parameters have been obtained; RgDNA' the cross-section radius of gyration (Rg) when DNA dominates the scatter; RgP, the cross-section Rg when protein dominates the scatter; Rc, the cross-section Rg at infinite contrast and alpha, the constant which describes the dependence of the cross-section Rg on contrast variation. From our understanding of the structure of the core particle, various arrangement of core particles in the nucleofilament have been tested. In models consistent with the above parameters the core particles are arranged edge-to-edge or with the faces of the core particles inclined to within 20 degrees to the axis of the nucleofilament. With increase of ionic strength the transition to the second-order chromatin structure has been followed. This gave the interesting result that above 20 microM NaCL or 0.4 mM MgCL2 the cross-section Rg increases abruptly to about 9 nm with a packing ratio of 0.2 nucleosome/mn and with further increase of ionic strength the Rg increases to 9.5 nm while the packing ratio increases threefold to 0.6 nucleosome/nm. This suggests a family of supercoils of nucleosomes which contract with increasing ionic strength. In its most contracted form the diameter of the hydrated supercoil has been found from the radial distribution function to be 34 nm. Models for the arrangements of core particles in the 34-nm supercoil are discussed.     

Nucleosome repeat lengths and columnar chromatin structure

Thorough quantitative study of nucleosome repeat length (NRL) distributions, conducted in 1992 by J. Widom, resulted in a striking observation that the linker lengths between the nucleosomes are quantized. Comparison of the NRL average values with the MNase cut distances predicted from the hypothetical columnar structure of chromatin (this work) shows a close correspondence between the two. This strongly suggests that the NRL distribution, actually, reflects the dominant role of columnar chromatin structure common for all eukaryotes.     

Higher order structure in a short repeat length chromatin

Polynucleosomes from calf brain cortical neurone nuclei have an average repeat length of less than 168 base pairs. The ability of this material to adopt higher order structure has been assessed by various physical techniques. Although containing on average less DNA per nucleosome than is required to form a chromatosome, this short repeat length chromatin folded in an H1 dependent manner to a structure with properties similar to those observed for longer repeat length chromatins such as that of chicken erythrocyte (McGhee, J.D., D.C. Rau, E. Charney, and G. Felsenfeld, 1980, Cell, 22:87-96). These observations are discussed in the context of H1 location in the higher order chromatin fiber.     

Different repeat lengths in rat satellite I DNA containing chromatin and bulk chromatin.

The nucleosome repeat structure of a rat liver chromatin component containing the satellite I DNA (repeat length 370 bp) was investigated. Digestion experiments with micrococcal nuclease, DNAase II, and the Ca2+/Mg2+-dependent endogenous nuclease of rat liver nuclei revealed a repeat unit of 185 nucleotide pairs which is shorter by approximately 10 bp than the repeat unit of the bulk chromatin of this cell type. The difference seems not to be related to the histone composition which was found to be similar in the two types of chromatin.     

Higher-order structures of chromatin: the elusive 30 nm fiber

Despite progress in understanding chromatin function, the structure of the 30 nm chromatin fiber has remained elusive. However, with the recent crystal structure of a short tetranucleosomal array, the 30 nm fiber is beginning to come into view.     

The chromatin structure of specific genes: II. Disruption of chromatin structure during gene activity.

We have compared the chromatin structure in the active and inactive states at loci encoding the major heat shock protein in Drosophila. DNAase I and micrococcal nuclease were used as probes of higher order organization and nucleosomal integrity. Such integrity is gauged here by the characteristic pattern of discrete DNA fragments produced at specific chromosomal loci by nucleolytic cleavage. The specific fragment patterns are visualized by gel electrophoresis, Southern blotting onto nitrocellulose sheets, hybridization with 32P-labeled cloned DNA containing the heat shock genes and autoradiography. Using this criterion, a disruption in nucleosomal and possibly in higher order organization are observed as indicated by a relative loss or smearing of the characteristic discrete DNA fragment patterns from the heat shock loci in the active state. The fragment patterns are restored when cells are allowed to recover from heat shock and these loci return to the inactive state.     

A defined structure of the 30 nm chromatin fibre which accommodates different nucleosomal repeat lengths

Earlier work on the condensation of chromatins of different repeat lengths into the 30 nm fibre has been surveyed and it is shown that the external geometry of the fibre must be the same for all the chromatins. This can only be fitted by a helical coiling of nucleosomes into a solenoid with the linker DNA disposed internally. On this basis, various models were calculated and compared with published electric dichroism data. The only good fit is found with a 'reverse-loop' model, where the linker DNA forms a complete turn into the hole of the solenoid, of opposite hand to the nucleosomal DNA superhelix. This gives a topological linking number of one per nucleosome and would resolve the 'linking number paradox' if the DNA screw is the same in chromatin as in solution. The feasibility of a reverse-loop for short linkers (down to 15 base pairs) was investigated by model building and kinks of approximately 120 degrees into both DNA grooves are described, which will allow such packing. There will, however, be a 'forbidden' range for the linker DNA length, between approximately 1 and 14 bp, corresponding to nucleosomal repeats of 163 and 176 bp.     

Large-scale chromatin structure and function.

Recent results in living cells have now established the existence of levels of chromatin folding above the 30 nm fiber within interphase chromosomes. We discuss the potential functional impact of this large-scale chromatin organization, including its possible role in regulating gene expression.     

Higher-order chromatin domains link eQTLs with the expression of far-away genes

Distal expression quantitative trait loci (distal eQTLs) are genetic mutations that affect the expression of genes genomically far away. However, the mechanisms that cause a distal eQTL to modulate gene expression are not yet clear. Recent high-resolution chromosome conformation capture experiments along with a growing database of eQTLs provide an opportunity to understand the spatial mechanisms influencing distal eQTL associations on a genome-wide scale. We test the hypothesis that spatial proximity contributes to eQTL-gene regulation in the context of the higher-order domain structure of chromatin as determined from recent Hi-C chromosome conformation experiments. This analysis suggests that the large-scale topology of chromatin is coupled with eQTL associations by providing evidence that eQTLs are in general spatially close to their target genes, occur often around topological domain boundaries and preferentially associate with genes across domains. We also find that within-domain eQTLs that overlap with regulatory elements such as promoters and enhancers are spatially more close than the overall set of within-domain eQTLs, suggesting that spatial proximity derived from the domain structure in chromatin plays an important role in the regulation of gene expression.     

A model for chromatin structure.

A model for chromatin structure is presented. (a) Each of four histone species, H2A (IIbl or f2a2), H2B (IIb2 or f2b), H3 (III or f3) and H4 (IV or f2al) can form a parallel dimer. (b) These dimers can form two tetramers, (H2A)2(H2b)2 and (H3)2(H4)2. (C) These two tetramers bind a segment of DNA and condense it into a "C" segments. (d) The adjacent segments, termed extended or "E" segments, are bound by histone H1 (I or fl) for the major fraction of chromatin; the other "E" regions can be either bound by non-histone proteins or free of protein binding. (e) The binding of histones causes a structural distortion of the DNA which, depending upon the external conditions, may generate the formation of either an open structure with a heterogeneous and non-uniform supercoil or a compact structure with a string of beads. The model is supported by experimental data on histone-histone interaction, histone-DNA interaction and histone subunit-DNA interaction.     

Urea denaturation of chromatin periodic structure.

Isolated chicken erythrocyte nuclei dispersed in urea solutions (0-5.0 M) have been examined in terms of their low-angle X-ray diffraction and electron microscopic properties. At high urea concentrations, the characteristic low-angle X-ray reflections of chromatin are absent, and the spheroid chromatin particles (v bodies) are markedly perturbed. This lability of chromatin periodic structure to high concentrations of urea is consistent with previous hydrodynamic and spectroscopic studies.     

The structure of SV 40 chromatin.

Simian virus 40 (SV40) nucleoprotein complexes were studied with the electron microscope. Depending on the isolation procedure, SV40 chromatin has two different conformations: complexes isolated in the presence of 0.15 M NaCl appeared as very compact globular structures, while those isolated in the presence of 0.6 M NaCl had the typical 'beads-on-a-string' appearance of the primary nucleofilament. Concomitant with this structural change was a variation in the histone pattern and sedimentation behaviour of the complexes: with NaCl at 0.15 mol 1(-1) the isolated complexes contained both the nucleosomal histones and histone H1, and sedimented in sucrose gradients at 70S. Increasing the ionic strength to 0.6 M NaCl resulted in the removal of histone H1 from the complexes and in a decrease of the sedimentation coefficient to 40S. DNA relaxing enzyme is associated with the SV40 nucleoprotein complexes. The numbers of superhelical turns in DNA from compact and open types of complexes were found to be the same. Therefore the transition from the condensed to the open structure of viral chromatin does not require a change in the topological winding number of its DNA.     

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.