Chromatin as dynamic 10-nm fibers - PubMed (original) (raw)

Review

Chromatin as dynamic 10-nm fibers

Kazuhiro Maeshima et al. Chromosoma. 2014 Jun.

Abstract

Since Flemming described a nuclear substance in the nineteenth century and named it "chromatin," this substance has fascinated biologists. What is the structure of chromatin? DNA is wrapped around core histones, forming a nucleosome fiber (10-nm fiber). This fiber has long been assumed to fold into a 30-nm chromatin fiber and subsequently into helically folded larger fibers or radial loops. However, several recent studies, including our cryo-EM and X-ray scattering analyses, demonstrated that chromatin is composed of irregularly folded 10-nm fibers, without 30-nm chromatin fibers, in interphase chromatin and mitotic chromosomes. This irregular folding implies a chromatin state that is physically less constrained, which could be more dynamic compared with classical regular helical folding structures. Consistent with this, recently, we uncovered by single nucleosome imaging large nucleosome fluctuations in living mammalian cells (∼50 nm/30 ms). Subsequent computational modeling suggested that nucleosome fluctuation increases chromatin accessibility, which is advantageous for many "target searching" biological processes such as transcriptional regulation. Therefore, this review provides a novel view on chromatin structure in which chromatin consists of dynamic and disordered 10-nm fibers.

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Figures

Fig. 1

Fig. 1

Old and novel views of chromatin structure. A long DNA molecule with a diameter of ∼2 nm is wrapped around a core histone octamer and forms a nucleosome with a diameter of 11 nm (Alberts et al. 2007). The nucleosome has long been assumed to fold into 30-nm chromatin fibers (left) and subsequently into the higher order organization of interphase nuclei or mitotic chromosomes. The right panel shows the novel hypothesis of irregularly folded nucleosome fibers

Fig. 2

Fig. 2

Two classical models of 30-nm chromatin fibers and higher order chromatin structures. a One-start helix (solenoid), b two-start helix (zigzag). (Top) A scheme of the two different topologies of chromatin fibers is shown (Robinson and Rhodes 2006). Positions from the first (N1) to the eighth (N8) nucleosome are labeled. c Two classical higher order chromatin structure models: the hierarchical helical folding model (Sedat and Manuelidis 1978) and the radial loop model (Laemmli et al. 1978). In the radial loop model, many loop structures of the 30-nm fiber (red) wrap around the scaffold structure (gray) (Laemmli et al. 1978), which consists of condensin and topoisomerase IIα (Maeshima and Laemmli 2003)

Fig. 3

Fig. 3

Small angle X-ray scattering (SAXS) analysis of chromatin structure. a Experimental design. The chromosome pellet in a quartz capillary tube was exposed to synchrotron X-ray beams, and the scattering patterns were recorded using the imaging plate (Nishino et al. 2012). b When non-crystal materials were irradiated with X-rays, scattering at small angles generally reflected periodic structures. Images a and b were reproduced from Joti et al. (2012), with some modifications. c Upper left Typical SAXS patterns of purified mitotic HeLa chromosome fractions. Three peaks at ∼6, ∼11 (weak), and ∼30 nm were detected (arrows). (Upper right) After the removal of ribosome aggregates, the 30-nm peak disappeared, whereas the other peaks remained. (Bottom) A model whereby the 30-nm peak in SAXS results from regularly spaced ribosome aggregates and not from the chromosomes. Image c was reproduced from Nishino et al. (2012), with some modification

Fig. 4

Fig. 4

Polymer melt model. a Under low-salt conditions, nucleosome fibers could form 30-nm chromatin fibers via intra-fiber nucleosome associations. An increase in salt (cation) concentration results in inter-fiber nucleosomal contacts that interfere with intra-fiber nucleosomal associations, leading to a polymer melt scenario. Note that in these illustrations, we show a highly simplified two-dimensional nucleosome model. Arrows and dotted lines show repulsion forces and interactions, respectively. b During the melting process, the 30-nm chromatin fibers become irregularly folded nucleosome fibers

Fig. 5

Fig. 5

Higher order structure of interphase chromatin. a Condensed chromatin domains. Active chromatin regions are transcribed on the surfaces of chromatin domains with transcriptional complexes (purple spheres) and RNA polymerase II (green spheres). NPC nuclear pore complex, NE nuclear envelope. b (Left) Condensed chromatin is more resistant to radiation damage or chemical attack. (Right) Reactive radicals arising from the radiolysis of water molecules by irradiation can damage decondensed chromatin; decondensed chromatin is also more accessible to chemicals (labeled “Ch”)

Fig. 6

Fig. 6

Mitotic chromosome structure. Axial localizations of condensins I and II in mitotic chromosomes in live mammalian cells. For DNA staining, DM (Indian Muntjac cells) cells stably expressing EGFP-Kleisin γ (condensin I) and EGFP-Kleisin β (condensing II) were stained with Hoechst 33342. Live-cell imaging was performed using a Delta Vision microscope (applied precision). a Clear axial signals of EGFP-Kleisin γ in mitotic chromosomes are shown. b End-on-view of mitotic chromosomes. The upper panel shows DM cells expressing EGFP-Kleisin γ, whereas the lower panel shows DM cells expressing EGFP-Kleisin β stably. Restricted dot signals from two types of EGFP-Kleisin in the cross-section of a chromosome body (DNA staining) are shown. c Quantitative data using line-profile analysis (blue line, DNA; red line, Kleisin signals) is shown. There is clear axial localization of condensins I and II in mitotic chromosomes in live mammalian cells. d Chromosomes consist of irregularly folded 10-nm nucleosome fibers. Condensins (blue) hold the nucleosome fibers (red) around the center of the chromosome. Locally, the nucleosome fibers are folded in an irregular or disordered manner, forming loop structures that collapse towards the center of the chromosome center (blue). The collapsed fiber (red) then forms a domain

Fig. 7

Fig. 7

Single nucleosome imaging. a A small portion of PA-GFP-H4 was activated spontaneously without laser activation and was used for single nucleosome imaging. b Single nucleosome image of a DM cell (Indian Muntjac cell) nucleus that expresses PA-GFP-H4. PA-GFP-H4 is observed as a bright dot using oblique illumination microscopy. The dots were fitted to an assumed Gaussian point spread function to determine the precise center of signals with higher resolution. Bar = 5 μm. c Representative three trajectories of fluorescently tagged single nucleosomes. d Chromatin fluctuations as a basis for scanning genome information. In cells, nucleosome fibers (red spheres and lines) are folded irregularly. The nucleosomes fluctuate, and these nucleosome dynamics facilitate chromatin accessibility. The images were reproduced from (Hihara et al. ; Nozaki et al. 2013) with some modification

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