DNA methylation affects nuclear organization, histone modifications, and linker histone binding but not chromatin compaction

DNA methylation has been implicated in chromatin condensation and nuclear organization, especially at sites of constitutive heterochromatin. How this is mediated has not been clear. In this study, using mutant mouse embryonic stem cells completely lacking in DNA methylation, we show that DNA methylation affects nuclear organization and nucleosome structure but not chromatin compaction. In the absence of DNA methylation, there is increased nuclear clustering of pericentric heterochromatin and extensive changes in primary chromatin structure. Global levels of histone H3 methylation and acetylation are altered, and there is a decrease in the mobility of linker histones. However, the compaction of both bulk chromatin and heterochromatin, as assayed by nuclease digestion and sucrose gradient sedimentation, is unaltered by the loss of DNA methylation. This study shows how the complete loss of a major epigenetic mark can have an impact on unexpected levels of chromatin structure and nuclear organization and provides evidence for a novel link between DNA methylation and linker histones in the regulation of chromatin structure.     

The XIST noncoding RNA functions independently of BRCA1 in X inactivation

Females with germline mutations in BRCA1 are predisposed to develop breast and ovarian cancers. A previous report indicated that BRCA1 colocalizes with and is necessary for the correct localization of XIST, a noncoding RNA that coats the inactive X chromosome (Xi) to mediate formation of facultative heterochromatin. A model emerged from this study suggesting that loss of BRCA1 in female cells could reactivate genes on the Xi through loss of the XIST RNA. However, our independent studies of BRCA1 and XIST RNA revealed little evidence to support this model. We report that BRCA1 is not enriched on XIST RNA-coated chromatin of the Xi. Neither mutation nor depletion of BRCA1 causes significant changes in XIST RNA localization or X-linked gene expression. Together, these results do not support a role for BRCA1 in promoting XIST RNA localization to the Xi or regulating XIST-dependent functions in maintaining the stability of facultative heterochromatin.     

M33 condenses chromatin through nuclear body formation and methylation of both histone H3 lysine 9 and lysine 27

Heterochromatin, a type of condensed DNA in eukaryotic cells, has two main categories: Constitutive heterochromatin, which contains H3K9 methylation, and facultative heterochromatin, which contains H3K27 methylation. Methylated H3K9 and H3K27 serve as docking sites for chromodomain-containing proteins that compact chromatin. M33 (also known as CBX2) is a chromodomain-containing protein that binds H3K27me3 and compacts chromatin in vitro. However, whether M33 mediates chromatin compaction in cellulo remains unknown. Here we show that M33 compacts chromatin into DAPI-intense heterochromatin domains in cells. The formation of these heterochromatin domains requires H3K27me3, which recruits M33 to form nuclear bodies. G9a and SUV39H1 are sequentially recruited into M33 nuclear bodies to create H3K9 methylated chromatin in a process that is independent of HP1α. Finally, M33 decreases progerin-induced nuclear envelope disruption caused by loss of heterochromatin. Our findings demonstrate that M33 mediates the formation of condensed chromatin by forming nuclear bodies containing both H3K27me3 and H3K9me3. Our model of M33-dependent chromatin condensation suggests H3K27 methylation corroborates with H3K9 methylation during the formation of facultative heterochromatin and provides the theoretical basis for developing novel therapies to treat heterochromatin-related diseases.     

30 nm chromatin fibre decompaction requires both H4-K16 acetylation and linker histone eviction

The mechanism by which chromatin is decondensed to permit access to DNA is largely unknown. Here, using a model nucleosome array reconstituted from recombinant histone octamers, we have defined the relative contribution of the individual histone octamer N-terminal tails as well as the effect of a targeted histone tail acetylation on the compaction state of the 30 nm chromatin fiber. This study goes beyond previous studies as it is based on a nucleosome array that is very long (61 nucleosomes) and contains a stoichiometric concentration of bound linker histone, which is essential for the formation of the 30 nm chromatin fiber. We find that compaction is regulated in two steps: Introduction of H4 acetylated to 30% on K16 inhibits compaction to a greater degree than deletion of the H4 N-terminal tail. Further decompaction is achieved by removal of the linker histone.     

Differential underacetylation of histones H2A,H3 and H4 on the inactive X chromosome in human female cells

It has previously been shown that the acetylated forms of histone H4 are depleted or absent in both constitutive, centric heterochromatin and in the facultative heterochromatin of the inactive X chromosome (Xi) in female cells. By immunostaining of metaphase chromosomes from human lymphocytes with antibodies to the acetylated isoforms of histones H2A and H3, we now show that these histones too are underacetylated in both Xi and centric heterochromatin. Xi shows two prominent regions of residual H3 acetylation, one encompassing the pseudoautosomal region at the end of the short arm and one at about Xg22. Both these regions have been shown previously to be sites of residual H4 acetylation. H2A acetylation on Xi is higher overall than that of H3 or H4 and is particularly high around the pseudoautosomal region, but not at Xg22. The results suggest that the acetylated isoforms of H3 and H4 have at least some effects on chromosomal structure and function that are not shared by acetylated H2A.     

Depletion Effects Massively Change Chromatin Properties and Influence Genome Folding

We present a Monte Carlo model for genome folding at the 30-nm scale with focus on linker-histone and nucleosome depletion effects. We find that parameter distributions from experimental data do not lead to one specific chromatin fiber structure, but instead to a distribution of structures in the chromatin phase diagram. Depletion of linker histones and nucleosomes affects, massively, the flexibility and the extension of chromatin fibers. Increasing the amount of nucleosome skips (i.e., nucleosome depletion) can lead either to a collapse or to a swelling of chromatin fibers. These opposing effects are discussed and we show that depletion effects may even contribute to chromatin compaction. Furthermore, we find that predictions from experimental data for the average nucleosome skip rate lie exactly in the regime of maximum chromatin compaction. Finally, we determine the pair distribution function of chromatin. This function reflects the structure of the fiber, and its Fourier-transform can be measured experimentally. Our calculations show that even in the case of fibers with depletion effects, the main dominant peaks (characterizing the structure and the length scales) can still be identified.     

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

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

Monoubiquitylation of H2A.Z distinguishes its association with euchromatin or facultative heterochromatin

H2A.Z is a histone H2A variant that is essential for viability in organisms such as Tetrahymena thermophila, Drosophila melanogaster, and mice. In Saccharomyces cerevisiae, loss of H2A.Z is tolerated, but proper regulation of gene expression is affected. Genetics and genome-wide localization studies show that yeast H2A.Z physically localizes to the promoters of genes and functions in part to protect active genes in euchromatin from being silenced by heterochromatin spreading. To date, the function of H2A.Z in mammalian cells is less clear, and evidence so far suggests that it has a role in chromatin compaction and heterochromatin silencing. In this study, we found that the bulk of H2A.Z is excluded from constitutive heterochromatin in differentiated human and mouse cells. Consistent with this observation, analyses of H2A.Z- or H2A-containing mononucleosomes show that the H3 associated with H2A.Z has lower levels of K9 methylation but higher levels of K4 methylation than those associated with H2A. We also found that a fraction of mammalian H2A.Z is monoubiquitylated and that, on the inactive X chromosomes of female cells, the majority of this histone variant is modified by ubiquitin. Finally, ubiquitylation of H2A.Z is mediated by the RING1b E3 ligase of the human polycomb complex, further supporting a silencing role of ubiquitylated H2A.Z. These new findings suggest that mammalian H2A.Z is associated with both euchromatin and facultative heterochromatin and that monoubiquitylation is a specific mark that distinguishes the H2A.Z associated with these different chromatin states.     

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.     

Photofootprint of nucleosome core DNA in intact chromatin having different structural states

Recently, we reported that the distribution of ultraviolet light (u.v.) induced pyrimidine dimers in nucleosome core DNA has a striking 10.3(+/- 0.1) base periodicity and the regions of enhanced quantum yield map to positions where DNA strands are farthest from the core histone surface. Improvement of the mapping procedure has allowed us to analyze this distribution in more detail, and compare the distribution pattern for nucleosome cores from intact chromatin having different higher-order structures (from the 10 nm filament to the 30 nm fiber). At all levels of chromatin compaction, we observed the following. (1) The average periodicity in pyrimidine dimer yield is 10.3 bases. (2) The peak-to-peak spacing in this distribution is significantly different from 10.3 bases in the region covering three helix turns immediately 5' of the dyad axis. (3) There is a suppression of photoproduct formation in the region of the dyad axis, especially at position 84 from the 5' end. (4) The approximately 10 base ensembles have alternating peak intensities throughout core DNA. Furthermore, peak deconvolution analysis of the pyrimidine dimer pattern yielded a striking similarity in photoproduct yield for the different levels of chromatin compaction. Irradiation of isolated core DNA yields a much more random distribution of photoproducts, although a weak modulation pattern is observed (indicating that there is a non-random alignment of adjacent pyrimidines in our core DNA preparations). This pattern includes a depression in photoproduct yield near position 95, suggesting that the sequence in this region plays a role in nucleosome positioning. These results show that the u.v. photofootprint is a sensitive, diagnostic probe of core histone-DNA interactions in intact chromatin, and these interactions are not significantly altered by changes in the structural state of the chromatin fiber.