30-nm Chromatin Fiber Research Articles

New Insight into the Mitotic Chromosome Structure: Irregular Folding of Nucleosome Fibers Without 30-nm Chromatin Structure

Mitotic chromosomes are essential structures for the faithful transmission of replicated genomic DNA into two daughter cells during cell division. A long strand of DNA is wrapped around a core histone and forms a nucleosome. The nucleosome has long been assumed to be folded into 30-nm chromatin fibers. However, how the nucleosome or 30-nm chromatin fiber is organized into mitotic chromosomes remains unclear, although condensins and topoisomerase IIα are implicated in the condensation process. In fact, what do mitotic chromosomes look like in living cells? When frozen hydrated human mitotic cells were observed using cryo-electron microscopy (cryo-EM), higher-order structures including 30-nm chromatin fibers were not found. We thus propose that the nucleosome fibers in the bulk of mitotic chromosomes do not form 30-nm chromatin fibers but instead exist in a highly irregular state that is locally similar to a polymer melt. We provide new insight into mitotic chromosome structure.

Changes in Chromatin Fiber Density as a Marker for Pluripotency

Extensive alterations in chromatin structure at the nucleosome level are linked to developmental potential. We hypothesize that such alterations in chromatin structure reflect and, to some extent, depend on the large-scale reorganization of the nuclear landscape. We have used electron spectroscopic imaging (ESI) to visualize chromatin organization at the mesoscale level of resolution in both pluripotent and differentiated cell types. Pluripotent cells are characterized by a highly dispersed mesh of 10-nm chromatin fibers that fill the nuclear volume. In contrast, differentiated cells display a propensity to form compact chromatin domains that lead to large regions of the nucleus devoid of DNA. Surprisingly, ESI combined with tomography methods reveals that the compact chromatin domains consist of 10-nm rather than 30-nm chromatin fibers. We propose that the transition between compact silent chromatin and open transcriptionally poised or active chromatin is based on the modulation of the packing density of 10-nm fibers rather than a transition between 10- and 30-nm fiber types.

Insights into Interphase Large-Scale Chromatin Structure from Analysis of Engineered Chromosome Regions

How chromatin folds into mitotic and interphase chromosomes has remained a difficult question for many years. We have used three generations of engineered chromosome regions as a means of visualizing specific chromosome regions in live cells and cells fixed under conditions that preserve large-scale chromatin structure. Our results confirm the existence of large-scale chromatin domains and fibers formed by the folding of 10-nm and 30-nm chromatin fibers into larger, spatially distinct domains. Transcription at levels within severalfold of the levels measured for endogenous loci occur within these large-scale chromatin structures on a condensed template linearly compacted several hundred fold to 1000-fold relative to B-form DNA. However, transcriptional induction is accompanied by a severalfold decondensation of this large-scale chromatin structure that propagates hundreds of kilobases beyond the induced gene. Examination of engineered chromosome regions in mouse embryonic stem cells (ESCs) and differentiated cells suggests a surprising degree of plasticity in this large-scale chromatin structure, allowing long-range DNA interactions within the context of large-scale chromatin fibers. Recapitulation of gene-specific differences in large-scale chromatin conformation and nuclear positioning using these engineered chromosome regions will facilitate identification of cis and trans determinants of interphase chromosome architecture.

A molecular model of chromatin organisation and transcription: how a multi‐RNA polymerase II machine transcribes and remodels the β‐globin locus during development

We present a molecular model of eukaryotic gene transcription. For the beta-globin locus, we hypothesise that a transcription machine composed of multiple RNA polymerase II (PolII) assembles using the locus control region as a foundation. Transcription and locus remodelling can be achieved by pulling DNA through this multi-PolII 'reading head'. Once a transcription complex is formed, it may engage an active gene in several rounds of transcription. Observed intergenic sense and antisense transcripts may be the result of PolII pulling the DNA through the reading head whilst searching for the promoter of a gene. Support for this hypothesis is provided using various data from the literature. In the model, DNA is packed in a 30-nm chromatin fibre, thus gene regulatory regions separated by kilobases are close in space. This, and the need to store transcription-induced supercoiling, may explain why functionally interacting regions are often separated by many kilobases.

Evidence for heteromorphic chromatin fibers from analysis of nucleosome interactions

The architecture of the chromatin fiber, which determines DNA accessibility for transcription and other template-directed biological processes, remains unknown. Here we investigate the internal organization of the 30-nm chromatin fiber, combining Monte Carlo simulations of nucleosome chain folding with EM-assisted nucleosome interaction capture (EMANIC). We show that at physiological concentrations of monovalent ions, linker histones lead to a tight 2-start zigzag dominated by interactions between alternate nucleosomes (i +/- 2) and sealed by histone N-tails. Divalent ions further compact the fiber by promoting bending in some linker DNAs and hence raising sequential nucleosome interactions (i +/- 1). Remarkably, both straight and bent linker DNA conformations are retained in the fully compact chromatin fiber as inferred from both EMANIC and modeling. This conformational variability is energetically favorable as it helps accommodate DNA crossings within the fiber axis. Our results thus show that the 2-start zigzag topology and the type of linker DNA bending that defines solenoid models may be simultaneously present in a structurally heteromorphic chromatin fiber with uniform 30 nm diameter. Our data also suggest that dynamic linker DNA bending by linker histones and divalent cations in vivo may mediate the transition between tight nucleosome packing within discrete 30-nm fibers and self-associated higher-order chromosomal forms.

Large-scale chromatin structure of inducible genes: transcription on a condensed, linear template

The structure of interphase chromosomes, and in particular the changes in large-scale chromatin structure accompanying transcriptional activation, remain poorly characterized. Here we use light microscopy and in vivo immunogold labeling to directly visualize the interphase chromosome conformation of 1–2 Mbp chromatin domains formed by multi-copy BAC transgenes containing 130–220 kb of genomic DNA surrounding the DHFR, Hsp70, or MT gene loci. We demonstrate near-endogenous transcription levels in the context of large-scale chromatin fibers compacted nonuniformly well above the 30-nm chromatin fiber. An approximately 1.5–3-fold extension of these large-scale chromatin fibers accompanies transcriptional induction and active genes remain mobile. Heat shock–induced Hsp70 transgenes associate with the exterior of nuclear speckles, with Hsp70 transcripts accumulating within the speckle. Live-cell imaging reveals distinct dynamic events, with Hsp70 transgenes associating with adjacent speckles, nucleating new speckles, or moving to preexisting speckles. Our results call for reexamination of classical models of interphase chromosome organization.

Rigid assembly and Monte Carlo models of stable and unstable chromatin structures: the effect of nucleosomal spacing

Coarse-grained models are used to assess the packing of the 30-nm chromatin fiber. First, rigid assembly models for nucleosomal repeats from 155 to 211 bp are built using the crystal structure of the mononucleosome and attached straight stretches of B-DNA. The resulting fiber conformations are analyzed for static clashes and classified into stable and unstable structures. The effect of flexibility and thermal fluctuations is then taken into account by conducting Monte Carlo simulations of chromatin fiber models. Here the DNA is approximated by a flexible polymer chain with Debye–Huckel electrostatics, the geometry of the linker DNA connecting the nucleosomes is based on a two-angle zigzag model, and nucleosomes are represented by flat ellipsoids interacting via an attractive Gay–Berne potential. Unstable fibers occur at a particular repeat length period of 10 bp. Also, the regions of densely compacted fibers repeat at intervals of 10 bp. Besides one- and two-start helical zigzag structures, we show evidence for possible three-start structures, which have not been reported in experiments yet. Finally, we show that a local opening of the linker DNA at the nucleosome core—as probably occurs upon histone acetylation—leads to more open and flexible structures.

Histone Octamer Helical Tubes Suggest that an Internucleosomal Four-Helix Bundle Stabilizes the Chromatin Fiber

A major question in chromatin involves the exact organization of nucleosomes within the 30-nm chromatin fiber and its structural determinants of assembly. Here we investigate the structure of histone octamer helical tubes via the method of iterative helical real-space reconstruction. Accurate placement of the x-ray structure of the histone octamer within the reconstructed density yields a pseudoatomic model for the entire helix, and allows precise identification of molecular interactions between neighboring octamers. One such interaction that would not be obscured by DNA in the nucleosome consists of a twofold symmetric four-helix bundle formed between pairs of H2B-α3 and H2B-αC helices of neighboring octamers. We believe that this interface can act as an internucleosomal four-helix bundle within the context of the chromatin fiber. The potential relevance of this interface in the folding of the 30-nm chromatin fiber is discussed.

Removal of histone tails from nucleosome dissects the physical mechanisms of salt-induced aggregation, linker histone H1-induced compaction, and 30-nm fiber formation of the nucleosome array

In order to reveal the roles of histone tails in the formation of higher-order chromatin structures, we employed atomic force microscopy (AFM), and an in vitro reconstitution system to examine the properties of reconstituted chromatin composed of tail-less histones and a long DNA (106-kb plasmid) template. The tail-less nucleosomes did not aggregate at high salt concentrations or with an excess amount of core histones, in contrast with the behavior of nucleosomal arrays composed of nucleosomes containing normal, N-terminal tails. Analysis of our nucleosome distributions reveals that the attractive interaction between tail-less nucleosomes is weakened. Addition of linker histone H1 into the tail-less nucleosomal array failed to promote the formation of 30 nm chromatin fibers that are usually formed in the normal nucleosomal array. These results demonstrate that the attractive interaction between nucleosomes via histone tails plays a critical role in the formation of the uniform 30-nm chromatin fiber.

Analysis of distant communication on defined chromatin templates in vitro.

Regulation of many biological processes in eukaryotes involves distant communication between the regulatory DNA sequences (e.g., enhancers) and their targets over the DNA regions organized in chromatin. However previously developed methods for analysis of communication in chromatin in vitro are artifact-prone and/or do not allow analysis of communication on physiologically relevant, saturated arrays of nucleosomes. Here we describe a method for quantitative analysis of the rate of distant communication in cis on saturated arrays of nucleosomes capable of forming the 30-nm chromatin fibers in vitro.

Analysis of cryo-electron microscopy images does not support the existence of 30-nm chromatin fibers in mitotic chromosomes in situ

Although the formation of 30-nm chromatin fibers is thought to be the most basic event of chromatin compaction, it remains controversial because high-resolution imaging of chromatin in living eukaryotic cells had not been possible until now. Cryo-electron microscopy of vitreous sections is a relatively new technique, which enables direct high-resolution observation of the cell structures in a close-to-native state. We used cryo-electron microscopy and image processing to further investigate the presence of 30-nm chromatin fibers in human mitotic chromosomes. HeLa S3 cells were vitrified by high-pressure freezing, thin-sectioned, and then imaged under the cryo-electron microscope without any further chemical treatment or staining. For an unambiguous interpretation of the images, the effects of the contrast transfer function were computationally corrected. The mitotic chromosomes of the HeLa S3 cells appeared as compact structures with a homogeneous grainy texture, in which there were no visible 30-nm fibers. Power spectra of the chromosome images also gave no indication of 30-nm chromatin folding. These results, together with our observations of the effects of chromosome swelling, strongly suggest that, within the bulk of compact metaphase chromosomes, the nucleosomal fiber does not undergo 30-nm folding, but exists in a highly disordered and interdigitated state, which is, on the local scale, comparable with a polymer melt.

Changes in distribution of basic nuclear proteins and chromatin organization during spermiogenesis in the greater bandicoot rat, Bandicota indica

Male germ cells of the greater bandicoot rat, Bandicota indica, have recently been categorized into 12 spermiogenic steps based upon the morphological appearance of the acrosome and nucleus and the cell shape. In the present study, we have found that, in the Golgi and cap phases, round spermatid nuclei contain 10-nm to 30-nm chromatin fibers, and that the acrosomal granule forms a huge cap over the anterior pole of nucleus. In the acrosomal phase, many chromatin fibers are approximately 50 nm thick; these then thickened to 70-nm fibers and eventually became 90-nm chromatin cords that are tightly packed together into highly condensed chromatin, except where nuclear vacuoles occur. Immunocytochemistry and immunogold localization with anti-histones, anti-transition protein2, and anti-protamine antibodies suggest that histones remain throughout spermiogenesis, that transition proteins are present from step 7 spermatids and remain until the end of spermiogenesis, and that protamines appear at step 8. Spermatozoa from the cauda epididymidis have been analyzed by acid urea Triton X-100 polyacrylamide gel electrophoresis for basic nuclear proteins. The histones, H2A, H3, H2B, and H4, transitional protein2, and protamine are all present in sperm extracts. These findings suggest that, in these sperm of unusual morphology, both transition proteins and some histones are retained, a finding possibly related to the unusual nuclear form of sperm in this species.

Nucleosome repeat length and linker histone stoichiometry determine chromatin fiber structure

To understand how nuclear processes involving DNA are regulated, knowledge of the determinants of chromatin condensation is required. From recent structural studies it has been concluded that the formation of the 30-nm chromatin fiber does not require the linker histone. Here, by comparing the linker histone-dependent compaction of long, reconstituted nucleosome arrays with different nucleosome repeat lengths (NRLs), 167 and 197 bp, we establish that the compaction behavior is both NRL- and linker histone-dependent. Only the 197-bp NRL array can form 30-nm higher-order chromatin structure. Importantly for understanding the regulation of compaction, this array shows a cooperative linker histone-dependent compaction. The 167-bp NRL array displays a limited linker histone-dependent compaction, resulting in a thinner and topologically different fiber. These observations provide an explanation for the distribution of NRLs found in nature.

Crystal Structures of Fission Yeast Histone Chaperone Asf1 Complexed with the Hip1 B-domain or the Cac2 C Terminus

The assembly of core histones onto eukaryotic DNA is modulated by several histone chaperone complexes, including Asf1, CAF-1, and HIRA. Asf1 is a unique histone chaperone that participates in both the replication-dependent and replication-independent pathways. Here we report the crystal structures of the apo-form of fission yeast Asf1/Cia1 (SpAsf1N; residues 1-161) as well as its complexes with the B-domain of the fission yeast HIRA orthologue Hip1 (Hip1B) and the C-terminal region of the Cac2 subunit of CAF-1 (Cac2C). The mode of the fission yeast Asf1N-Hip1B recognition is similar to that of the human Asf1-HIRA recognition, suggesting that Asf1N recognition of Hip1B/HIRA is conserved from yeast to mammals. Interestingly, Hip1B and Cac2C show remarkably similar interaction modes with Asf1. The binding between Asf1N and Hip1B was almost completely abolished by the D37A and L60A/V62A mutations in Asf1N, indicating the critical role of salt bridge and van der Waals contacts in the complex formation. Consistently, both of the aforementioned Asf1 mutations also drastically reduced the binding to Cac2C. These results provide a structural basis for a mutually exclusive Asf1-binding model of CAF-1 and HIRA/Hip1, in which Asf1 and CAF-1 assemble histones H3/H4 (H3.1/H4 in vertebrates) in a replication-dependent pathway, whereas Asf1 and HIRA/Hip1 assemble histones H3/H4 (H3.3/H4 in vertebrates) in a replication-independent pathway.

A variable topology for the 30‐nm chromatin fibre

The structure of the 30-nm chromatin fibre is an important determinant of the regulation of eukaryotic transcription. A fundamental issue is whether the stacking of nucleosomes in this fibre is organized as a one-start or two-start helix. We argue that all recent experimental data are compatible with a two-start helix and propose that the topology of the fibre, but not the mode of stacking the nucleosomes, is dependent on the length of the linker DNA. This arrangement conserves nucleosome stacking and thus the external morphology of the fibre, and also ensures that the fibre adopts the highest available packing density.

The nucleosome surface regulates chromatin compaction and couples it with transcriptional repression

Although it is believed that the interconversion between permissive and refractory chromatin structures is important in regulating gene transcription, this process is poorly understood. Central to addressing this issue is to elucidate how a nucleosomal array folds into higher-order chromatin structures. Such findings can then provide new insights into how the folding process is regulated to yield different functional states. Using well-defined in vitro chromatin-assembly and transcription systems, we show that a small acidic region on the surface of the nucleosome is crucial both for the folding of a nucleosomal template into the 30-nm chromatin fiber and for the efficient repression of transcription, thereby providing a mechanistic link between these two essential processes. This structure-function relationship has been exploited by complex eukaryotic cells through the replacement of H2A with the specific variant H2A.Bbd, which naturally lacks an acidic patch.

Topoisomerase II, scaffold component, promotes chromatin compaction in vitro in a linker-histone H1-dependent manner

TopoisomeraseII (Topo II) is a major component of chromosomal scaffolds and essential for mitotic chromosome condensation, but the mechanism of this action remains unknown. Here, we used an in vitro chromatin reconstitution system in combination with atomic force and fluorescence microscopic analyses to determine how Topo II affects chromosomal structure. Topo II bound to bare DNA and clamped the two DNA strands together, even in the absence of ATP. In addition, Topo II promoted chromatin compaction in a manner dependent on histone H1 but independent of ATP. Histone H1-induced 30-nm chromatin fibers were converted into a large complex by Topo II. Fluorescence microscopic analysis of the Brownian motion of chromatin stained with 4′,6-diamidino-2-phenylindole showed that the reconstituted chromatin became larger following the addition of Topo II in the presence but not the absence of histone H1. Based on these findings, we propose that chromatin packing is triggered by histone H1-dependent, Topo II-mediated clamping of DNA strands.

Atomic Force Microscopy Dissects the Hierarchy of Genome Architectures in Eukaryote, Prokaryote, and Chloroplast

Because of its applicability to biological specimens (nonconductors), a single-molecule-imaging technique, atomic force microscopy (AFM), has been particularly powerful for visualizing and analyzing complex biological processes. Comparative analyses based on AFM observation revealed that the bacterial nucleoids and human chromatin were constituted by a detergent/salt-resistant 30-40-nm fiber that turned into thicker fibers with beads of 70-80 nm diameter. AFM observations of the 14-kbp plasmid and 110-kbp F plasmid purified from Escherichia coli demonstrated that the 70-80-nm fiber did not contain a eukaryotic nucleosome-like "beads-on-a-string" structure. Chloroplast nucleoid (that lacks bacterial-type nucleoid proteins and eukaryotic histones) also exhibited the 70-80-nm structural units. Interestingly, naked DNA appeared when the nucleoids from E. coli and chloroplast were treated with RNase, whereas only 30-nm chromatin fiber was released from the human nucleus with the same treatment. These observations suggest that the 30-40-nm nucleoid fiber is formed with a help of nucleoid proteins and RNA in E. coli and chroloplast, and that the eukaryotic 30-nm chromatin fiber is formed without RNA. On the other hand, the 70-80-nm beaded structures in both E. coli and human are dependent on RNA.

EM measurements define the dimensions of the “30-nm” chromatin fiber: Evidence for a compact, interdigitated structure

Chromatin structure plays a fundamental role in the regulation of nuclear processes such as DNA transcription, replication, recombination, and repair. Despite considerable efforts during three decades, the structure of the 30-nm chromatin fiber remains controversial. To define fiber dimensions accurately, we have produced very long and regularly folded 30-nm fibers from in vitro reconstituted nucleosome arrays containing the linker histone and with increasing nucleosome repeat lengths (10 to 70 bp of linker DNA). EM measurements show that the dimensions of these fully folded fibers do not increase linearly with increasing linker length, a finding that is inconsistent with two-start helix models. Instead, we find that there are two distinct classes of fiber structure, both with unexpectedly high nucleosome density: arrays with 10 to 40 bp of linker DNA all produce fibers with a diameter of 33 nm and 11 nucleosomes per 11 nm, whereas arrays with 50 to 70 bp of linker DNA all produce 44-nm-wide fibers with 15 nucleosomes per 11 nm. Using the physical constraints imposed by these measurements, we have built a model in which tight nucleosome packing is achieved through the interdigitation of nucleosomes from adjacent helical gyres. Importantly, the model closely matches raw image projections of folded chromatin arrays recorded in the solution state by using electron cryo-microscopy.

Electrostatic interactions with histone tails may bend linker DNA in chromatin

Is linker DNA bent in the 30-nm chromatin fiber at physiological conditions? We show here that electrostatic interactions between linker DNA and histone tails including salt condensation and release may bend linker DNA, thus affecting the higher order organization of chromatin.