Higher order structure of chromatin: orientation of nucleosomes within the 30 nm chromatin solenoid is independent of species and spacer length

We have used electric dichroism to study the arrangement of nucleosomes in 30 nm chromatin solenoidal fibers prepared from a variety of sources (CHO cells, HeLa cells, rat liver, chicken erythrocytes, and sea urchin sperm) in which the nucleosome spacer length varies from approximately 10 to approximately 80 bp. Field-free relaxation times are consistent only with structures containing 6 +/- 1 nucleosomes for every 11 nm of solenoidal length. With very few assumptions about the arrangement of the spacer DNA, our dichroism data are consistent with the same orientation of the chromatosomes for every chromatin sample examined. This orientation, which maintains the faces of the radially arranged chromatosomes inclined at an angle between 20 degrees-33 degrees to the solenoid axis, thus appears to be a general structural feature of the higher order chromatin fiber.     

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.     

Organization of internucleosomal DNA in rat liver chromatin

A detailed analysis of the length distribution of DNA in nucleosome dimers trimmed with exonuclease III and S1 nuclease suggests that the previously described variation of internucleosomal distance in rat liver occurs, at least for a subset of the nucleosomes, by integral multiples of the helical repeat of the DNA. Results obtained upon digestion of chromatin with DNase II further suggest that lengths of internucleosomal DNA are integral multiples of the helical repeat of the DNA plus approximately 5 bp. Restraints imposed by these features on the arrangement of nucleosomes along the fiber are discussed.     

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.     

Localization of linker histone in chromatosomes by cryo-atomic force microscopy

Linker histones play a fundamental role in determining higher order chromatin structure as a consequence of their association with nucelosomal DNA. Yet the locations and structural consequences of linker histone binding are still enigmatic. Here, using cryo-atomic force microscopy, we show that the linker histone H5 in native chromatin and in chromatosomes reconstituted on the 5S rDNA template is located at the dyad of the nucleosome core particle, within the "stem" structure. Direct measurement also indicates that the length of free linker DNA between chromatosomes in native chromatin is approximately 30 bp, slightly shorter than that estimated from nuclease digestion assays.     

Differential association of linker histones H1 and H5 with telomeric nucleosomes in chicken erythrocytes.

Rat liver telomeric DNA is organised into nucleosomes characterised by a shorter and more homogeneous average nucleosomal repeat than bulk chromatin as shown by Makarov et al. (1). The latter authors were unable to detect the association of any linker histone with the telomeric DNA. We have confirmed these observations but show that in sharp contrast chicken erythrocyte telomeric DNA is organised into nucleosomes whose spacing length and heterogeneity are indistinguishable from those of bulk chromatin. We further show that chicken erythrocyte telomeric chromatin contains chromatosomes which are preferentially associated with histone H1 relative to histone H5. This contrasts with bulk chromatin where histone H5 is the more abundant species. This observation strongly suggests that telomeric DNA condensed into nucleosome core particles has a higher affinity for H1 than H5. We discuss the origin of the discrimination of the lysine rich histones in terms of DNA sequence preferences, telomere nucleosome preferences and particular constraints of the higher order chromatin structure of telomeres.     

Nucleosome positioning in relation to nucleosome spacing and DNA sequence-specific binding of a protein

Nucleosome positioning is an important mechanism for the regulation of eukaryotic gene expression. Folding of the chromatin fiber can influence nucleosome positioning, whereas similar electrostatic mechanisms govern the nucleosome repeat length and chromatin fiber folding in vitro. The position of the nucleosomes is directed either by the DNA sequence or by the boundaries created due to the binding of certain trans-acting factors to their target sites in the DNA. Increasing ionic strength results in an increase in nucleosome spacing on the chromatin assembled by the S-190 extract of Drosophila embryos. In this study, a mutant lac repressor protein R3 was used to find the mechanisms of nucleosome positioning on a plasmid with three R3-binding sites. With increasing ionic strength in the presence of R3, the number of positioned nucleosomes in the chromatin decreased, whereas the internucleosomal spacings of the positioned nucleosomes in a single register did not change. The number of the positioned nucleosomes in the chromatin assembled in vitro over different plasmid DNAs with 1-3 lac operators changed with the relative position and number of the R3-binding sites. We found that in the presence of R3, nucleosomes were positioned in the salt gradient method of the chromatin assembly, even in the absence of a nucleosome-positioning sequence. Our results show that nucleosome-positioning mechanisms are dominant, as the nucleosomes can be positioned even in the absence of regular spacing mechanisms. The protein-generated boundaries are more effective when more than one binding site is present with a minimum distance of approximately 165 bp, greater than the nucleosome core DNA length, between them.     

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.     

RNA sequences specifically associated with mouse intracisternal A particles.

Electron microscopic examination of the histone H1-depleted, folded genomes of Drosophila melanogaster reveals that they are composed of long cylindrical cables of about 100 Å diameter. Limited single-strand nicking with DNAase I relaxes the 100 Å fibers to a “beads-on-a-string” structure, showing the nucleosomes and internucleosome DNA.Based on these results and other available data, we have constructed a detailed space-filling model for the higher order DNA coiling in chromatin, starting with the symmetrical nucleosome core previously described (Weintraub, Worcel and Alberts, 1976). The model defines the path of the DNA helix and the nucleosome arrangement along the DNA coil for both the 100 Å and the 200–300 Å fibers.Following Sobell et al. (1976), we believe that the DNA is coiled in the 100 Å nucleofilament in a uniform left-handed supercoil of about 90 base pairs (bp) per turn and 47 Å pitch; the 140 bp symmetrical nucleosome cores align themselves along this uniform DNA superhelix so that the isologous outer surfaces of adjacent nucleosomes touch and the internucleosome spacer DNA coils between them. A few single-strand discontinuities [about one nick per 85 kilobases (kb); Benyajati and Worcel, 1976] in the H1-depleted 100 Å fiber can thus relax the negatively supercoiled internucleosome DNA generating the “beads-on -a-string” appearance.We propose that histone H1 binds to the 100 Å diameter superhelix and coils it into tightly packed, 110 Å pitch super-superhelices (“solenoids;” Finch and Klug, 1976) of variable diameter (between 200–300 Å). In our model, the “thick” 200–300 Å fiber is stabilized at metaphase by histone H1-H1 heterologous interactions between adjacent helical turns of the nucleofilament, and the internucleosome spacer DNA is located on the outside. Symmetry considerations demand that changes in the length of the repeat should lead to variations in the number of nucleosomes per helical turn and in the handedness of these turns in the 200–300 Å metaphase fiber.     

A critical role for linker DNA in higher-order folding of chromatin fibers

Nucleosome-nucleosome interactions drive the folding of nucleosomal arrays into dense chromatin fibers. A better physical account of the folding of chromatin fibers is necessary to understand the role of chromatin in regulating DNA transactions. Here, we studied the unfolding pathway of regular chromatin fibers as a function of single base pair increments in linker length, using both rigid base-pair Monte Carlo simulations and single-molecule force spectroscopy. Both computational and experimental results reveal a periodic variation of the folding energies due to the limited flexibility of the linker DNA. We show that twist is more restrictive for nucleosome stacking than bend, and find the most stable stacking interactions for linker lengths of multiples of 10 bp. We analyzed nucleosomes stacking in both 1- and 2-start topologies and show that stacking preferences are determined by the length of the linker DNA. Moreover, we present evidence that the sequence of the linker DNA also modulates nucleosome stacking and that the effect of the deletion of the H4 tail depends on the linker length. Importantly, these results imply that nucleosome positioning in vivo not only affects the phasing of nucleosomes relative to DNA but also directs the higher-order structure of chromatin.     

Chromatin fibers are left-handed double helices with diameter and mass per unit length that depend on linker length

Four classes of models have been proposed for the internal structure of eukaryotic chromosome fibers--the solenoid, twisted-ribbon, crossed-linker, and superbead models. We have collected electron image and x-ray scattering data from nuclei, and isolated chromatin fibers of seven different tissues to distinguish between these models. The fiber diameters are related to the linker lengths by the equation: D(N) = 19.3 + 0.23 N, where D(N) is the external diameter (nm) and N is the linker length (base pairs). The number of nucleosomes per unit length of the fibers is also related to linker length. Detailed studies were done on the highly regular chromatin from erythrocytes of Necturus (mud puppy) and sperm of Thyone (sea cucumber). Necturus chromatin fibers (N = 48 bp) have diameters of 31 nm and have 7.5 +/- 1 nucleosomes per 10 nm along the axis. Thyone chromatin fibers (N = 87 bp) have diameters of 39 nm and have 12 +/- 2 nucleosomes per 10 nm along the axis. Fourier transforms of electron micrographs of Necturus fibers showed left-handed helical symmetry with a pitch of 25.8 +/- 0.8 nm and pitch angle of 32 +/- 3 degrees, consistent with a double helix. Comparable conclusions were drawn from the Thyone data. The data do not support the solenoid, twisted-ribbon, or supranucleosomal particle models. The data do support two crossed-linker models having left-handed double-helical symmetry and conserved nucleosome interactions.     

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.     

A phase relationship associates tRNA structural gene sequences with nucleosome cores

DNA (760 bp) isolated from nucleosome tetramers of staphylococcal nuclease-digested chicken embryo chromatin was highly enriched for tRNA genes and subsequently cloned in E. coli chi 1776. The location of genes coding for chicken embryo tRNALys, tRNAPhe and tRNAiMet within the cloned nucleosome tetramer DNA was determined using restriction endonucleases for which single cleavage sites could be predicted from the respective tRNA base sequence. All our tRNA genes reside nonrandomly at four locations on nucleosome tetramer DNA. The spacing between the tRNA gene locations is approximately 190 bp, similar to the DNA repeat length of chicken embryo chromatin. The four tRNA gene locations were also defined in noncloned nucleosome tetramer DNA highly enriched for tRNA genes. The majority of genes coding for tRNALys, tRNAPhe and tRNAiMet, respectively, are located in equal proportion 40-45, 230, 420 and 610 bp distant from the 5' end of the tRNA-identical strand. Thus the tRNA structural gene sequences all appear to begin about 20 bp "inside" the nucleosome core. As observed with nucleosomal DNA not enriched for tRNA genes, the phase relationship between tRNA genes and nucleosome location is maintained over a distance of 4-6 subsequent nucleosomes. A cloned molecule of nucleosomal DNA containing both a tRNALys gene and a tRNAiMet gene in the same polarity reveals that a phase adjustment might be necessary for the nucleosomes between these two tRNA genes in chicken embryo chromatin.     

ATP dependent histone phosphorylation and nucleosome assembly in a human cell free extract.

Physiologically spaced nucleosome formation in HeLa cell extracts is ATP dependent. ATP hydrolysis is required for chromatin assembly on both linear and covalently closed circular DNA. The link between the phosphorylation state of histones and nucleosome formation has been examined and we demonstrate that in the absence of histone phosphorylation no stable and regularly spaced nucleosomes are formed. Phosphorylated H3 stabilizes the nucleosome core; while phosphorylation of histone H2a is necessary to increase the linker length between nucleosomes from 0 to approximately 45 bp. Histone H1 alone, whether phosphorylated or unphosphorylated, does not increase the nucleosome repeat length in the absence of core histone phosphorylation. Phosphorylations of H1 and H3 correlate with condensation of chromatin. Maximum ATP hydrolysis which is necessary to increase the periodicity of nucleosomes from approximately 150 to approximately 185 bp, not only inhibits H1 and H3 phosphorylation but facilitates their dephosphorylation.     

Preferentially quantized linker DNA lengths in Saccharomyces cerevisiae

The exact lengths of linker DNAs connecting adjacent nucleosomes specify the intrinsic three-dimensional structures of eukaryotic chromatin fibers. Some studies suggest that linker DNA lengths preferentially occur at certain quantized values, differing one from another by integral multiples of the DNA helical repeat, approximately 10 bp; however, studies in the literature are inconsistent. Here, we investigate linker DNA length distributions in the yeast Saccharomyces cerevisiae genome, using two novel methods: a Fourier analysis of genomic dinucleotide periodicities adjacent to experimentally mapped nucleosomes and a duration hidden Markov model applied to experimentally defined dinucleosomes. Both methods reveal that linker DNA lengths in yeast are preferentially periodic at the DNA helical repeat ( approximately 10 bp), obeying the forms 10n+5 bp (integer n). This 10 bp periodicity implies an ordered superhelical intrinsic structure for the average chromatin fiber in yeast.     

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.     

Modeling Studies of Chromatin Fiber Structure as a Function of DNA Linker Length

Chromatin fibers encountered in various species and tissues are characterized by different nucleosome repeat lengths (NRLs) of the linker DNA connecting the nucleosomes. While single cellular organisms and rapidly growing cells with high protein production have short NRL ranging from 160 to 189 bp, mature cells usually have longer NRLs ranging between 190 and 220 bp. Recently, various experimental studies have examined the effect of NRL on the internal organization of chromatin fiber. Here, we investigate by mesoscale modeling of oligonucleosomes the folding patterns for different NRL, with and without linker histone (LH), under typical monovalent salt conditions using both one-start solenoid and two-start zigzag starting configurations. We find that short to medium NRL chromatin fibers (173 to 209 bp) with LH condense into zigzag structures and that solenoid-like features are viable only for longer NRLs (226 bp). We suggest that medium NRLs are more advantageous for packing and various levels of chromatin compaction throughout the cell cycle than their shortest and longest brethren; the former (short NRLs) fold into narrow fibers, while the latter (long NRLs) arrays do not easily lead to high packing ratios due to possible linker DNA bending. Moreover, we show that the LH has a small effect on the condensation of short-NRL arrays but has an important condensation effect on medium-NRL arrays, which have linker lengths similar to the LH lengths. Finally, we suggest that the medium-NRL species, with densely packed fiber arrangements, may be advantageous for epigenetic control because their histone tail modifications can have a greater effect compared to other fibers due to their more extensive nucleosome interaction network.     

Topological analysis of plasmid chromatin from yeast and mammalian cells

Yeast has proven to be a powerful system for investigation of chromatin structure. However, the extent to which yeast chromatin can serve as a model for mammalian chromatin is limited by the significant number of differences that have been reported. To further investigate the structural relationship between the two chromatins, we have performed a DNA topological analysis of pRSSVO, a 5889 base-pair plasmid that can replicate in either yeast or mammalian cells. When grown in mammalian cells, pRSSVO contains an average of 33 negative supercoils, consistent with one nucleosome per 181 bp. This is close to the measured nucleosome repeat length of 190 bp. However, when grown in yeast cells, pRSSVO contains an average of only 23 negative supercoils, which is indicative of only one nucleosome per 256 bp. This is dramatically different from the measured nucleosome repeat length of 165 bp. To account for these observations, we suggest that yeast chromatin is composed of relatively short ordered arrays of nucleosomes with a repeat of 165 bp, separated by substantial gaps, possibly corresponding to regulatory regions.