The layered organization of nucleosomes in 30 nm chromatin fibers

We have used electron microscopy and established methods of three-dimensional reconstruction to obtain structural information on the 30 nm chromatin fibers from sea cucumber sperm and chicken erythrocytes. The fibers show a longitudinal periodicity of 10–11 nm. We have interpreted this periodicity as due to a grouping of nucleosomes into disks, each disk containing about 5–6 nucleosomes. These disks are closely stacked to form the chromatin fiber. We have built a detailed model for four fibers and we have determined the approximate coordinates of all the nucleosomes in them. The average distance found between neighboring nucleosomes has a value close to 11 nm. They may be connected either as a regularly distorted helix or as a layered zigzag. The second model appears more appropriate, since in the constrictions of the fibers the nucleosomes can only be connected as a zigzag.     

Chromatin organization - the 30 nm fiber

Despite over 30 years of work, the fundamental structure of eukaryotic chromatin remains controversial. Here, we review the roots of this controversy in disparities between results derived from studies of chromatin in nuclei, chromatin isolated from nuclei, and chromatin reconstituted from defined components. Thanks to recent advances in imaging, modeling, and other approaches, it is now possible to recognize some unifying principles driving chromatin architecture at the level of the ubiquitous '30 nm' chromatin fiber. These suggest that fiber architecture involves both zigzag and bent linker motifs, and that such heteromorphic structures facilitate the observed high packing ratios. Interactions between neighboring fibers in highly compact chromatin lead to extensive interdigitation of nucleosomes and the inability to resolve individual fibers in compact chromatin in situ.     

An all-atom model of the chromatin fiber containing linker histones reveals a versatile structure tuned by the nucleosomal repeat length

In the nucleus of eukaryotic cells, histone proteins organize the linear genome into a functional and hierarchical architecture. In this paper, we use the crystal structures of the nucleosome core particle, B-DNA and the globular domain of H5 linker histone to build the first all-atom model of compact chromatin fibers. In this 3D jigsaw puzzle, DNA bending is achieved by solving an inverse kinematics problem. Our model is based on recent electron microscopy measurements of reconstituted fiber dimensions. Strikingly, we find that the chromatin fiber containing linker histones is a polymorphic structure. We show that different fiber conformations are obtained by tuning the linker histone orientation at the nucleosomes entry/exit according to the nucleosomal repeat length. We propose that the observed in vivo quantization of nucleosomal repeat length could reflect nature's ability to use the DNA molecule's helical geometry in order to give chromatin versatile topological and mechanical properties.     

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.     

Nucleosome geometry and internucleosomal interactions control the chromatin fiber conformation

Based on model structures with atomic resolution, a coarse-grained model for the nucleosome geometry was implemented. The dependence of the chromatin fiber conformation on the spatial orientation of nucleosomes and the path and length of the linker DNA was systematically explored by Monte Carlo simulations. Two fiber types were analyzed in detail that represent nucleosome chains without and with linker histones, respectively: two-start helices with crossed-linker DNA (CL conformation) and interdigitated one-start helices (ID conformation) with different nucleosome tilt angles. The CL conformation was derived from a tetranucleosome crystal structure that was extended into a fiber. At thermal equilibrium, the fiber shape persisted but relaxed into a structure with a somewhat lower linear mass density of 3.1 ± 0.1 nucleosomes/11 nm fiber. Stable ID fibers required local nucleosome tilt angles between 40° and 60°. For these configurations, much higher mass densities of up to 7.9 ± 0.2 nucleosomes/11 nm fiber were obtained. A model is proposed, in which the transition between a CL and ID fiber is mediated by relatively small changes of the local nucleosome geometry. These were found to be in very good agreement with changes induced by linker histone H1 binding as predicted from the high resolution model structures.     

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.     

Chromatin structure. Evidence that the 30-nm fiber is a helical coil with 12 nucleosomes/turn

Sedimentation analysis has been used to compare the structure of 30-nm chromatin fibers, isolated and digested under conditions that maintain the native structure, with relaxed-refolded chromatin. The native chromatin fibers show sharp, ionic strength-dependent changes in sedimentation coefficient that are not apparent in relaxed-refolded fibers. The first transition at approximately 20 mM ionic strength reflects the organization of the 10-nm polynucleosome chain into a loose helically coiled 30-nm fiber. Between 20 and 60 mM ionic strength there is considerable interaction between nucleosomes within the coils to generate a stable helical array with 12 nucleosomes/turn. Above 60 mM ionic strength the helical coil continues to condense until it precipitates at ionic strengths slightly greater than those considered physiological, indicating that there is no end point in fiber formation. The data is incompatible with a solenoid model with 6 nucleosomes/turn and also rules out the existence of a beaded subunit structure.     

Changing Chromatin Fiber Conformation by Nucleosome Repositioning

Chromatin conformation is dynamic and heterogeneous with respect to nucleosome positions, which can be changed by chromatin remodeling complexes in the cell. These molecular machines hydrolyze ATP to translocate or evict nucleosomes, and establish loci with regularly and more irregularly spaced nucleosomes as well as nucleosome-depleted regions. The impact of nucleosome repositioning on the three-dimensional chromatin structure is only poorly understood. Here, we address this issue by using a coarse-grained computer model of arrays of 101 nucleosomes considering several chromatin fiber models with and without linker histones, respectively. We investigated the folding of the chain in dependence of the position of the central nucleosome by changing the length of the adjacent linker DNA in basepair steps. We found in our simulations that these translocations had a strong effect on the shape and properties of chromatin fibers: i), Fiber curvature and flexibility at the center were largely increased and long-range contacts between distant nucleosomes on the chain were promoted. ii), The highest destabilization of the fiber conformation occurred for a nucleosome shifted by two basepairs from regular spacing, whereas effects of linker DNA changes of ∼10 bp in phase with the helical twist of DNA were minimal. iii), A fiber conformation can stabilize a regular spacing of nucleosomes inasmuch as favorable stacking interactions between nucleosomes are facilitated. This can oppose nucleosome translocations and increase the energetic costs for chromatin remodeling. Our computational modeling framework makes it possible to describe the conformational heterogeneity of chromatin in terms of nucleosome positions, and thus advances theoretical models toward a better understanding of how genome compaction and access are regulated within the cell.     

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.     

Contributions of linker histones and histone H3 to chromatin structure: scanning force microscopy studies on trypsinized fibers.

Little is known about the mechanisms that organize linear arrays of nucleosomes into the three-dimensional structures of extended and condensed chromatin fibers. We have earlier defined, from scanning force microscopy (SFM) and mathematical modeling, a set of simple structural determinants of extended fiber morphology, the critical parameters being the entry-exit angle between consecutive linkers and linker length. Here we study the contributions of the structural domains of the linker histones (LHs) and of the N-terminus of histone H3 to extended fiber morphology by SFM imaging of progressively trypsinized chromatin fibers. We find that cleavage of LH tails is associated with a lengthening of the internucleosomal center-to-center distance, and that the somewhat later cleavage of the N-terminus of histone H3 is associated with a flattening of the fiber. The persistence of the "zigzag" fiber morphology, even at the latest stages of trypsin digestion, can be attributed to the retention of the globular domain of LH in the fiber.     

Changing Chromatin Fiber Conformation by Nucleosome Repositioning

Chromatin conformation is dynamic and heterogeneous with respect to nucleosome positions, which can be changed by chromatin remodeling complexes in the cell. These molecular machines hydrolyze ATP to translocate or evict nucleosomes, and establish loci with regularly and more irregularly spaced nucleosomes as well as nucleosome-depleted regions. The impact of nucleosome repositioning on the three-dimensional chromatin structure is only poorly understood. Here, we address this issue by using a coarse-grained computer model of arrays of 101 nucleosomes considering several chromatin fiber models with and without linker histones, respectively. We investigated the folding of the chain in dependence of the position of the central nucleosome by changing the length of the adjacent linker DNA in basepair steps. We found in our simulations that these translocations had a strong effect on the shape and properties of chromatin fibers: i), Fiber curvature and flexibility at the center were largely increased and long-range contacts between distant nucleosomes on the chain were promoted. ii), The highest destabilization of the fiber conformation occurred for a nucleosome shifted by two basepairs from regular spacing, whereas effects of linker DNA changes of ∼10 bp in phase with the helical twist of DNA were minimal. iii), A fiber conformation can stabilize a regular spacing of nucleosomes inasmuch as favorable stacking interactions between nucleosomes are facilitated. This can oppose nucleosome translocations and increase the energetic costs for chromatin remodeling. Our computational modeling framework makes it possible to describe the conformational heterogeneity of chromatin in terms of nucleosome positions, and thus advances theoretical models toward a better understanding of how genome compaction and access are regulated within the cell.     

Small angle x-ray scattering of chromatin. Radius and mass per unit length depend on linker length.

Analyses of low angle x-ray scattering from chromatin, isolated by identical procedures but from different species, indicate that fiber diameter and number of nucleosomes per unit length increase with the amount of nucleosome linker DNA. Experiments were conducted at physiological ionic strength to obtain parameters reflecting the structure most likely present in living cells. Guinier analyses were performed on scattering from solutions of soluble chromatin from Necturus maculosus erythrocytes (linker length 48 bp), chicken erythrocytes (linker length 64 bp), and Thyone briareus sperm (linker length 87 bp). The results were extrapolated to infinite dilution to eliminate interparticle contributions to the scattering. Cross-sectional radii of gyration were found to be 10.9 +/- 0.5, 12.1 +/- 0.4, and 15.9 +/- 0.5 nm for Necturus, chicken, and Thyone chromatin, respectively, which are consistent with fiber diameters of 30.8, 34.2, and 45.0 nm. Mass per unit lengths were found to be 6.9 +/- 0.5, 8.3 +/- 0.6, and 11.8 +/- 1.4 nucleosomes per 10 nm for Necturus, chicken, and Thyone chromatin, respectively. The geometrical consequences of the experimental mass per unit lengths and radii of gyration are consistent with a conserved interaction among nucleosomes. Cross-linking agents were found to have little effect on fiber external geometry, but significant effect on internal structure. The absolute values of fiber diameter and mass per unit length, and their dependencies upon linker length agree with the predictions of the double-helical crossed-linker model. A compilation of all published x-ray scattering data from the last decade indicates that the relationship between chromatin structure and linker length is consistent with data obtained by other investigators.     

Organization of chromatin during spermiogenesis: beaded fibers,partly beaded fibers,and loss of nucleosomal structure

The aggregation of chromatin during spermiogenesis in the house cricket and many other animals is an orderly process involving the formation of a series of long, thick, well defined structures. The differentiation of chromatin preliminary to the development of such unusual structures is given attention here. Examination of nuclei after lysis and spreading indicated that fibers with closely spaced nucleosomes, like the fibers of somatic chromatin, make up the chromatin in all stages of early spermiogenesis and most of middle spermiogenesis. The thick structures of late spermatids cannot be formed by aggregation of fibers of this somatic type, however; just before thick structures form, chromatin fibers lose the nucleosomal structure. During the process, fibers with nucleosomes spaced at irregular intervals and with long stretches of smooth thin fiber are found, as if nucleosomes at one site on a fiber are broken down independently of those at adjacent sites. Since prior studies of cricket proteins have indicated that somatic histones persist during the stages when nucleosome structure disappears, the observations imply that the histones which are organized in nucleosomes during early stages must become incorporated into different kinds of nucleoprotein complexes during succeeding stages of spermiogenesis.     

Linker DNA Length is a Key to Tri-nucleosome Folding

The folding of a nucleosome array has long been one of the fundamental and unsolved problems in chromatin biology. In this study, we address how nucleosome array folding depends on the length of linker DNA. We performed molecular dynamics simulations of a tri-nucleosome, a minimal model of chromatin folding, with various linker lengths (LLs) ranging from 20 to 40 base pairs (bps). We found that the tri-nucleosome folding strongly depends on LLs, and classified the structure ensemble into five classes, named from trinuc-1 to trinuc-5. As a function of LL, the different classes appear, on average, every 2 bps with a period of 10 bps, and are characterized by distinct inter-nucleosome interactions. The trinuc-1 conformation corresponds to LL ~ 10n, where n is an integer, and is stabilized by the tight packing between the first and the third nucleosomes, consistent with a zigzag fiber form. Structures of the other four classes are more diverse and distributed continuously in the space of possible configurations. Histone-DNA electrostatic interactions in the tri-nucleosome are further analyzed.     

Pyrimidine dimer formation as a probe of nucleosome core and linker structure in situ

The photoinduced dimerization of adjacent pyrimidines in DNA is influenced in predictable ways by DNA conformation. A method is described for determining patterns of pyrimidine dimer formation under conditions in which the chromatin is minimally perturbed. The relation of such patterns to the conformation of nucleosomal core DNA and linker DNA, as well as the interaction of histone H1 with nucleosomal DNA, is presented. Such data indicate that sharp bends in the path of DNA seen in crystals of isolated nucleosome core particles are also present in intact chromatin. They also indicate that most of the linker has very little curvature except for a small bend at its junction with the nucleosome core. The linker path inferred from such experiments supports models in which the chromatin fiber consists of a zigzag chain of nucleosomes.     

Nucleosomes and the chromatin fiber

During the past year and a half, significant progress has been made in understanding the structure and dynamics of nucleosomes and the chromatin fiber, the mechanism of action of the core histone amino termini, the structure and function of histone variants, and the function of linker histones in the chromatin fiber.