综述: 30 nm染色质纤维的结构及调控

真核细胞中,基因组DNA缠绕组蛋白八聚体形成核小体,核小体再经过多层次折叠压缩形成具有高级结构的染色质．过去30多年,科学家对30 nm染色质纤维的结构进行了大量的研究,然而关于30 nm染色质纤维的精细结构仍然存在很大的争议．本文综述了近年来对30 nm染色质纤维结构的最新研究进展,并重点阐述了最近解析的30 nm染色质纤维左 手双螺旋结构．同时,我们还进一步讨论了一些对30 nm染色质纤维结构起调控作用的因子及其作用机制．最后,我们对30 nm染色质纤维结构与功能领域所面临的挑战和问题进行了展望．     

Scanning electron microscopy of the centromeric region of L-cell chromosomes after treatment with Hoechst 33258 combined with 5-bromodeoxyuridine

When mouse L-cells were treated with a combination of 5-bromodeoxyuridine (BrdUrd) and Hoechst 33258, the metaphase chromosomes revealed undercondensation of the chromatin fibers in the sister centromeres. The application of the osmium-thiocarbohydrazide technique to the air-dried chromosome preparations made it possible to elucidate the ultrastructure of the undercondensed centromeric region at the level of the 30 nm chromatin fiber. Scanning electron microscopy revealed that the undercondensed region consisted of a coiled fiber with a diameter of about 400 nm, and a gyre diameter of approximately 600 nm. The coiled fiber was composed of the 30 nm chromatin fiber loops. These findings indicate that a continuous coiled structure, which is the final higher order structure of the condensed chromatin fiber, exists throughout the entire length of the mouse L-cell metaphase chromosome.     

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.     

Nucleosome gaping supports a functional structure for the 30nm chromatin fiber

The biological functions played by the nucleus of eukaryotic cells and especially those involved in cellular differentiation not only depend on the genomic sequence but also on all the proteins which form the nucleo-protein complex named chromatin. The tridimensional organization of this huge polymer involves many structural levels, the most basic one being the nucleosome. Nucleosomes further organize into the so-called 30nm fiber, which, according to recent works, is likely to be the main functional level of chromatin. We wish here to propose a plausible structure for the 30nm chromatin fiber that could explain its functional role. In our model, silenced chromatin is locked by nucleosome stacking interactions. This is achieved by a conformational transition within the nucleosome core particle (NCP) which allows nucleosomes to stack along two helices without bending the DNA linkers. We used molecular modeling to check that this conformational transition was plausible. Then we proposed to modify the well-known two-angle model according to these atomic level results. The emerging picture is an allosteric behavior of the nucleosomes induced by their collective organization within the 30nm chromatin fiber.     

Structure of hyperacetylated chromatin: light scattering and flow linear dichroism study

Cation-induced folding of 10 nm chromatin filament to 30 nm fiber was studied with hyperacetylated chromatin using light scattering at 90 degrees and flow linear dichroism. Acetylated chromatin folded in a way indistinguishable from that of the control chromatin: both the compactness of chromatin and the orientation of nucleosomes relative to the fiber axis were identical at a given salt concentration.     

Higher order folding of chromatin is induced in different ways by monovalent and by bivalent cations

The condensation of the 10 nm chromatin filament in the 30 nm fiber by monovalent cations, polyamines and bivalent cations was studied with light scattering at 90 degrees and flow linear dichroism methods. It was found that monovalent cation- and polyamine-induced folding was a two-step process: a precondensation, when a rotation of nucleosomes takes place only, and a condensation step without changes in nucleosome orientation. Divalent cations affected the structure of chromatin in one step only -- condensation of the chromatin filament being accompanied by nucleosome reorientation.     

The globular domain of histone H5 is internally located in the 30 nm chromatin fiber: an immunochemical study.

The location of the globular domain of histone H5 relative to the axis of the 30 nm chromatin fiber was investigated by following the accessibility of this region of the molecule in chicken erythrocyte chromatin to specific antibodies as a function of chromatin structure. Antibodies to the globular domain of H5 as well as their Fab fragments were found to react with chromatin at ionic strengths ranging from 1-80 mM NaCl, the reaction gradually decreasing upon increase of salt concentration. If, however, Fab fragments were conjugated to ferritin, no reaction of the complex with chromatin was observed at salt concentrations higher than 20 mM. The accessibility of the globular part of H5 in unfolded chromatin to the Fab-ferritin complex was also demonstrated with trypsin-digested chromatin. The experiments were carried out by both solid-phase immunoassay and inhibition experiments. The data obtained are consistent with a structure in which the globular domain of H5 is internally located in the 30 nm chromatin fiber.     

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.     

30nm染色质纤维结构与表观遗传调控

真核生物的DNA以染色质形式通过逐级折叠压缩形成高级结构存在于细胞核中。染色质高级结构直接参与了真核基因的转录调控和其它与DNA相关的生物学事件,因此研究染色质高级结构对了解表观遗传学分子机制有着至关重要的作用。近些年,研究者们针对30 nm染色质高级结构提出了两个模型:螺线管模型和Zig-Zag模型。2014年,我们利用体外染色质组装体系重建了30 nm染色质纤维,运用高精度冷冻电镜技术得到了分辨率为11?的30 nm染色质纤维的精细结构,提出了30 nm染色质高级结构的左手双螺旋Zig-Zag模型。本文综述了30 nm染色质纤维结构研究方面的相关进展,并对30 nm染色质高级结构的表观遗传调控机理以及单分子成像和操纵技术在研究30 nm染色质高级结构中潜在的应用作出讨论和展望。     

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.     

Studies on the structure of isolated chromatin in three different solvents.

Properties of calf thymus chromatin, prepared by mild procedures, have been studied in various solvents. In 0.2 mM EDTA s-values ranged from 20 to 30 S and intrinsic viscosities from 5 to 24 dl/g. Dialysis against 0.15 M NaCl or 0.2 mM MgCl2 changed these values to 80 to 100 S and 0.2 to 5 dl/g, respectively, indicating an essentially more compact structure. In 0.2 mM EDTA X-ray scattering yielded a cross section diameter of 9 nm, which is associated with the tertiary structure of chromatin fiber (M/L = 21200 Dalton/nm). By dialysis against 0.15 M NaCl or 0.2 mM MgCl2 part of the material spontaneously formed quarterny structures (cross section diameters 25-29 nm). The rest of the material with cross section diameters less than 9 nm is supposed to be more strongly sheared tertiary structure which seems to be unable to form quarterny structure due to artificial conformational changes.     

Chromatin superstructure A study with an immobilized trypsin

Hen erythrocyte chromatin was treated with trypsin immobilized on collagen membranes and the unfolding of chromatin fiber was followed by light scattering at 90° and flow linear dichroism. Chromatin was found almost completely decondensed when the bulk of H1 and H5 was digested while H3 was still intact. Further digestion leading to degradation of both H3 and the rest of H1 and H5 accounted for no more than 10–15% of the total effect. When chromatin with trypsin-cleaved H1 and H5 was titrated with increasing amounts of spermidine it folded similarly to the control sample. This finding suggests that charge neutralization appears a likely mechanism for maintaining the structure of the 30 nm chromatin fiber by the C-terminal domain of H1 and H5.     

Linker histone H1 per se can induce three-dimensional folding of chromatin fiber

Higher-order architectures of chromosomes play important roles in the regulation of genome functions. To understand the molecular mechanism of genome packing, an in vitro chromatin reconstitution method and a single-molecule imaging technique (atomic force microscopy) were combined. In 50 mM NaCl, well-stretched beads-on-a-string chromatin fiber was observed. However, in 100 mM NaCl, salt-induced interaction between nucleosomes caused partial aggregation. Addition of histone H1 promoted a further folding of the fiber into thicker fibers 20-30 nm in width. Micrococcal nuclease digestion of these thicker fibers produced an approximately 170 bp fragment of nucleosomal DNA, which was approximately 20 bp longer than in the absence of histone H1 ( approximately 150 bp), indicating that H1 is correctly placed at the linker region. The width of the fiber depended on the ionic strength. Widths of 20 nm in 50 mM NaCl became 30 nm as the ionic strength was changed to 100 mM. On the basis of these results, a flexible model of chromatin fiber formation was proposed, where the mode of the fiber compaction changes depending both on salt environment and linker histone H1. The biological significance of this property of the chromatin architecture will be apparent in the closed segments ( approximately 100 kb) between SAR/MAR regions.     

Supranucleosomal organization of chromatin

A systematic study of the effect of different ionic conditions on the morphology of the 25–30 nm chromatin fiber from chicken erythrocytes has revealed that, as the ionic strength is increased, knobby fibers with a clear superbead structure are formed in the presence of either Mg⁺⁺ or Na⁺, or both. A further increase in ionic strength results in smooth chromatin fibers due to a tight packing of superbeads. Cross-linking such fibers with formaldehyde and reversal of the ionic conditions, demonstrates the superbead structures underlying the smooth fibers observed at high ionic concentrations. The average size of the superbeads is 34 nm along the length of the fibers, in agreement with the value found in embedded sea cucumber chromatin. A second class of superbeads has an average length of 25 nm and probably corresponds to partially disrupted structures.