Structure of the chromatin with long linker DNA

The method of velocity sedimentation have been used to investigate ionic-strength-induced compaction of sea urchin sperm chromatin characterized by extremely long linker DNA (100 b.p.). The dependence of sedimentation coefficients of oligonucleosomes on the number of nucleosomes in the chain have been studied in the range of ionic strength from 0.005 to 0.085. Analysis of these data indicates that such structural parameters of sea urchin sperm chromatin fibre as the diameter of the chain and the length of the chain per nucleosome are quite similar to those of chromatin with shorter linker DNA, but the DNA packing ratio is higher. The structure of sea urchin sperm oligonucleosomes agrees well with the model of three-dimensional zig-zag-shaped chain with linker DNA forming a loop. The possible role of alpha-helical regions of the C-terminal domain of sea urchin sperm histone H1 in the long linker DNA folding is discussed.     

A defined structure of the 30 nm chromatin fibre which accommodates different nucleosomal repeat lengths

Earlier work on the condensation of chromatins of different repeat lengths into the 30 nm fibre has been surveyed and it is shown that the external geometry of the fibre must be the same for all the chromatins. This can only be fitted by a helical coiling of nucleosomes into a solenoid with the linker DNA disposed internally. On this basis, various models were calculated and compared with published electric dichroism data. The only good fit is found with a 'reverse-loop' model, where the linker DNA forms a complete turn into the hole of the solenoid, of opposite hand to the nucleosomal DNA superhelix. This gives a topological linking number of one per nucleosome and would resolve the 'linking number paradox' if the DNA screw is the same in chromatin as in solution. The feasibility of a reverse-loop for short linkers (down to 15 base pairs) was investigated by model building and kinks of approximately 120 degrees into both DNA grooves are described, which will allow such packing. There will, however, be a 'forbidden' range for the linker DNA length, between approximately 1 and 14 bp, corresponding to nucleosomal repeats of 163 and 176 bp.     

Nucleosomal structure of sea urchin and starfish sperm chromatin. Histone H2B is possibly involved in determining the length of linker DNA.

Comparison has been made between sea urchin and starfish sperm chromatin. The only protein by which chromatins from these sources differ significantly is histone H2B. Sea urchin sperm H2B is known to contain an elongated N-terminal region enriched in Arg. Analysis of the micrococcal nuclease digests of sea urchin and starfish nuclei in one- and two-dimensional electrophoresis has shown that sperm chromatin of both animals consists of repeated units similar in general features to those of rat thymus or liver. However, DNA repeat length in chromatin of sea urchin sperm (237 bp) is higher than that of starfish sperm (224 bp), while the core DNA length does not differ and is the same as in the chromatin of rat liver or thymus. A suggestion has been made that the N-terminal region of histone H2B is associated with the linker DNA and is responsible for the increased length of sea urchin linker DNA.     

Higher-order structure of long repeat chromatin.

The higher-order structure of chromatin isolated from sea urchin sperm, which has a long nucleosomal DNA repeat length (approximately 240 bp), has been studied by electron microscopy and X-ray diffraction. Electron micrographs show that this chromatin forms 300 A filaments which are indistinguishable from those of chicken erythrocytes (approximately 212 bp repeat); X-ray diffraction patterns from partially oriented samples show that the edge-to-edge packing of nucleosomes in the direction of the 300 A filament axis, and the radial disposition of nucleosomes around it, are both similar to those of the chicken erythrocyte 300 A filament, which is described by the solenoid model. The invariance of the structure with increased linker DNA length is inconsistent with many other models proposed for the 300 A filament and, furthermore, means that the linker DNA must be bent. The low-angle X-ray scattering in the 300-400 A region both in vitro and in vivo differs from that of chicken erythrocyte chromatin. The nature of the difference suggests that 300 A filaments in sea urchin sperm in vivo are packed so tightly together that electron-density contrast between individual filaments is lost; this is consistent with electron micrographs of the chromatin in vitro.     

The structure of chromatin from the pigeon brain. II. Sedimentation analysis of oligonucleosome density

Compaction of pigeon brain and rat thymus chromatin differing in the length of the linker DNA has been studied by the method of velocity sedimentation. The dependence of sedimentation coefficients of oligonucleosomes on the number of nucleosomes in the chain in solution of different ionic strength (0.005-0.085) has been analyzed. The analyses of these dependences showed that the structure of oligonucleosomes of both cell types at low ionic conditions may be described by the model of a zig-zag-shaped nucleosomal chain. The process of compaction of the oligonucleosomes at higher ionic strength (0.045-0.085) proceeds similarly for brain and thymus chromatin. The formation of a superhelical structure is determined by the interaction of no less than 6 nucleosomes; the compactness of the structure is significantly increased when the number of nucleosomes in the chain exceeds 10. The ability of the brain oligonucleosomes to form a compact structure despite the short linker allow the suggestion that in brain short chromatin the DNA chain does not form two complete turns in the nucleosome. This provides necessary flexibility of brain chromatin.     

Computer simulation of the 30-nanometer chromatin fiber

A new Monte Carlo model for the structure of chromatin is presented here. Based on our previous work on superhelical DNA and polynucleosomes, it reintegrates aspects of the "solenoid" and the "zig-zag" models. The DNA is modeled as a flexible elastic polymer chain, consisting of segments connected by elastic bending, torsional, and stretching springs. The electrostatic interaction between the DNA segments is described by the Debye-Hückel approximation. Nucleosome core particles are represented by oblate ellipsoids; their interaction potential has been parameterized by a comparison with data from liquid crystals of nucleosome solutions. DNA and chromatosomes are linked either at the surface of the chromatosome or through a rigid nucleosome stem. Equilibrium ensembles of 100-nucleosome chains at physiological ionic strength were generated by a Metropolis-Monte Carlo algorithm. For a DNA linked at the nucleosome stem and a nucleosome repeat of 200 bp, the simulated fiber diameter of 32 nm and the mass density of 6.1 nucleosomes per 11 nm fiber length are in excellent agreement with experimental values from the literature. The experimental value of the inclination of DNA and nucleosomes to the fiber axis could also be reproduced. Whereas the linker DNA connects chromatosomes on opposite sides of the fiber, the overall packing of the nucleosomes leads to a helical aspect of the structure. The persistence length of the simulated fibers is 265 nm. For more random fibers where the tilt angles between two nucleosomes are chosen according to a Gaussian distribution along the fiber, the persistence length decreases to 30 nm with increasing width of the distribution, whereas the other observable parameters such as the mass density remain unchanged. Polynucleosomes with repeat lengths of 212 bp also form fibers with the expected experimental properties. Systems with larger repeat length form fibers, but the mass density is significantly lower than the measured value. The theoretical characteristics of a fiber with a repeat length of 192 bp where DNA and nucleosomes are connected at the core particle are in agreement with the experimental values. Systems without a stem and a repeat length of 217 bp do not form fibers.     

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.     

Linker DNA destabilizes condensed chromatin.

The contribution of the linker region to maintenance of condensed chromatin was examined in two model systems, namely sea urchin sperm nuclei and chicken red blood cell nuclei. Linkerless nuclei, prepared by extensive digestion with micrococcal nuclease, were compared with Native nuclei using several assays, including microscopic appearance, nuclear turbidity, salt stability, and trypsin resistance. Chromatin in the Linkerless nuclei was highly condensed, resembling pyknotic chromatin in apoptotic cells. Linkerless nuclei were more stable in low ionic strength buffers and more resistant to trypsin than Native nuclei. Analysis of histones from the trypsinized nuclei by polyacrylamide gel electrophoresis showed that specific histone H1, H2B, and H3 tail regions stabilized linker DNA in condensed nuclei. Thermal denaturation of soluble chromatin preparations from differentially trypsinized sperm nuclei demonstrated that the N-terminal regions of histones Sp H1, Sp H2B, and H3 bind tightly to linker DNA, causing it to denature at a high temperature. We conclude that linker DNA exerts a disruptive force on condensed chromatin structure which is counteracted by binding of specific histone tail regions to the linker DNA. The inherent instability of the linker region may be significant in all eukaryotic chromatins and may promote gene activation in living cells.     

Generation of different nucleosome spacing periodicities in vitro. Possible origin of cell type specificity

We have been able to generate ordered nucleosome arrays that span the physiological range of spacing periodicities, using an in vitro system. Our system (a refinement of the procedure previously developed) uses the synthetic polynucleotide poly[d(A-T)], poly[d(A-T)], core histones, purified H1, and polyglutamic acid, a factor that increases nucleohistone solubility and greatly promotes the formation of ordered nucleosome arrays. This system has three useful features, not found in other chromatin assembly systems. First, it allowed us to examine histones from three different cell types/species (sea urchin sperm, chicken erythrocyte, and HeLa) as homologous or heterologous combinations of core and H1 histones. Second, it allowed us to control the average packing density (core histone to polynucleotide weight ratio) of nucleosomes on the polynucleotide; histone H1 is added in a second distinct step in the procedure to induce nucleosome alignment. Third, it permitted us to study nucleosome array formation in the absence of DNA base sequence effects. We show that the value of the spacing periodicity is controlled by the value of the initial average nucleosome packing density. The full range of physiological periodicities appears to be accessible to arrays generated using chicken erythrocyte (or HeLa) core histones in combination with chicken H5. However, chromatin-like structures cannot be assembled for some nucleosome packing densities in reactions involving some histone types, thus limiting the range of periodicities that can be achieved. For example, H1 histone types differ significantly in their ability to recruit disordered nucleosomes into ordered arrays at low packing densities. Sea urchin sperm H1 is more efficient than chicken H5, which is more efficient than H1 from HeLa or chicken erythrocyte. Sea urchin sperm core histones are more efficient in this respect than the other core histone types used. These findings suggest how different repeat lengths arise in different cell types and species, and provide new insights into the problems of nucleosome linker heterogeneity and how different types of chromatin structures could be generated in the same cell.     

Chromatosome positioning on assembled long chromatin. Linker histones affect nucleosome placement on 5 S rDNA

Long chromatin containing linker histones H1 or H5 was assembled on tandemly repeated 172 or 207 base-pair nucleosome positioning sequences from a sea urchin 5 S RNA gene. The effects of H1 and H5 on spacing and positioning of nucleosomes were assessed. In the absence of linker histones, precise determinations of core particle boundaries showed that, although a large proportion of the histone octamers occupy a unique position, there is a small group of other, less populated sites located around this major site. The dominant position was found 10 to 15 base-pairs upstream from the unique position previously reported for the histone octamer on the monomer 260 base-pair sequence. Linker histones do not override the underlying DNA signals that induce the very regular spacing of nucleosomes in chromatins assembled on these strongly positioning multimer DNA sequences. They were nevertheless found to be decisive in determining the chromatosome positions and their distributions, and as such define the chromatosome as a positioning entity.     

Higher order structure of chromatin: evidence from photochemically detected linear dichroism

We have used photochemically detected linear dichroism to measure the separate average angular orientations of nucleosomes and linker DNA in 30-nm chromatin fibers of varying linker size (20-80 base pairs). Our results indicate that the average tilt angles vary with linker size, but not in a monotonic manner, suggesting that the constancy of geometry of the 30-nm fiber is maintained by compensatory changes of nucleosomal tilt which accommodate packing of variable lengths of linker DNA. We discuss the compatibility of our results with the various classes of models that have been proposed for the 30-nm fiber, including the continuous solenoid model and models built from the basic unit of the zig-zag ribbon. Many models can be eliminated, and all have to be modified to fit our results for chromatins with very long linkers.     

Interaction of sperm histone variants and linker DNA during spermiogenesis in the sea urchin

Several physical properties of sea urchin spermatid chromatin, which contains phosphorylated Sp H1 and Sp H2B histone variants, and mature sperm chromatin, in which these histones are dephosphorylated, were compared. Density, thermal stability, average nucleosomal repeat length, and resistance to micrococcal nuclease digestion are all increased in mature sperm relative to spermatid chromatin. Since the chromatins are identical in histone variant subtypes, the altered physical properties are not a consequence of changes in histone primary structure during spermiogenesis. The data are interpreted to mean that dephosphorylation of the N-terminal regions of Sp H1 and Sp H2B in late spermatid nuclei permits strong ionic binding of these highly basic regions to the extended linker, stabilizing the highly condensed structure of sperm chromatin.     

Linear dichroism of chromatin fibers

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Friend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations by the use of flow linear dichroism and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA--2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA--for chromatins with linker DNA 10-30 b.p. it is partially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric fields do not have an effect on chromatin structure, while higher electric fields (more than 7 kV/cm) distort the structure of chromatin.     

Involvement of histone H1 in the organization of the nucleosome and of the salt-dependent superstructures of chromatin

We describe the results of a systematic study, using electron microscopy, of the effects of ionic strength on the morphology of chromatin and of H1-depleted chromatin. With increasing ionic strength, chromatin folds up progressively from a filament of nucleosomes at approximately 1 mM monovalent salt through some intermediate higher- order helical structures (Thoma, F., and T. Koller, 1977, Cell 12:101- 107) with a fairly constant pitch but increasing numbers of nucleosomes per turn, until finally at 60 mM (or else in approximately 0.3 mM Mg++) a thick fiber of 250 A diameter is formed, corresponding to a structurally well-organized but not perfectly regular superhelix or solenoid of pitch approximately 110 A as described by Finch and Klug (1976, Proc. Natl. Acad. Sci. U.S.A. 73:1897-1901). The numbers of nucleosomes per turn of the helical structures agree well with those which can be calculated from the light-scattering data of Campbell et al. (1978, Nucleic Acids Res. 5:1571-1580). H1-depleted chromatin also condenses with increasing ionic strength but not so densely as chromatin and not into a definite structure with a well-defined fiber direction. At very low ionic strengths, nucleosomes are present in chromatin but not in H1-depleted chromatin which has the form of an unravelled filament. At somewhat higher ionic strengths (greater than 5 mM triethanolamine chloride), nucleosomes are visible in both types of specimen but the fine details are different. In chromatin containing H1, the DNA enters and leaves the nucleosome on the same side but in chromatin depleted of H1 the entrance and exit points are much more random and more or less on opposite sides of the nucleosome. We conclude that H1 stabilizes the nucleosome and is located in the region of the exit and entry points of the DNA. This result is correlated with biochemical and x-ray crystallographic results on the internal structure of the nucleosome core to give a picture of a nucleosome in which H1 is bound to the unique region on a complete two-turn, 166 base pair particle (Fig. 15). In the formation of higher-order structures, these regions on neighboring nucleosomes come closer together so that an H1 polymer may be formed in the center of the superhelical structures.     

Optical anisotropy of chromatin. Flow linear dichroism and electric dichroism studies

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentrations by the use of flow linear dichroism (LD) and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA - 2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA - for chromatins with the linker DNA of 10-30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin. Presented results explain the contradictory data obtained by electrooptical and hydrooptical methods.     

Theoretical models of possible compact nucleosome structures

Chromatin structure seems related to the DNA linker length. This paper presents a systematic search of the possible chromatin structure as a function of the linker lengths, starting from three different low-resolution molecular models of the nucleosome. Gay-Berne potential was used to evaluate the relative nucleosome packing energy. Results suggest that linker DNAs, which bridges and orientate nucleosomes, affect both the geometry and the rigidity of the global chromatin 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.     

Role of the histone "tails" in the folding of oligonucleosomes depleted of histone H1.

An oligonucleosome 12-mer was reconstituted in the absence of linker histones, onto a DNA template consisting of 12 tandemly arranged 208-base pair fragments of the 5 S rRNA gene from the sea urchin Ly-techinus variegatus (Simpson, R. T., Thoma, F. S., and Burbaker, J. M. (1985) Cell 42, 799-808). The ionic strength-dependent folding of this nucleohistone complex was compared with that of a native oligonucleosome fraction obtained from chicken erythrocyte chromatin, which had been carefully stripped of linker histones and fractionated in sucrose gradients. The DNA of this native fraction exhibited a narrow size distribution centered around the length of the 208-12 DNA template used in the reconstituted complex. These two complexes displayed very similar hydrodynamic behavior as judged by sedimentation velocity analysis. By combining these data with electron microscopy analysis, it was shown that the salt-dependent folding of oligonucleosomes in the absence of linker histones involves the bending of the linker DNA region connecting adjacent nucleosomes. It was also found that selective removal by trypsin of the N-terminal regions ("tails") of the core histones prevents the oligonucleosome chains from folding. Thus, in the absence of these histone domains, the bending of the linker DNA necessary to bring the nucleosomes in contact is completely abolished. In addition to the complete lack of folding, removal of the histone tails results in an unwinding at low salt of a 20-base pair region at each flanking side of the nucleosome core particle. The possible functional relevance of these results is discussed.     

Nucleotide sequence-directed mapping of the nucleosomes

The concept of sequence-dependent deformational anisotropy of DNA proposed earlier is further elaborated and a computational procedure is developed for the sequence-directed mapping of the nucleosomes along chromatin DNA nucleotide sequences. The deformational anisotropy is found to be nonuniform along the molecule of the nucleosomal DNA, suggesting that the DNA superhelix in the nucleosome is slightly oval rather than circular in projection. The number of superhelical turns in the nucleosome core particle is estimated to be 2.0 +/- 0.2. Preliminary mapping of the nucleosomes in various chromatin DNA sequences yields the distribution of linker lengths which shows several minima separated by about 10 base-pairs. This is explained by sterical exclusion effects due to overlapping of the nucleosomes in space when some specific linker lengths are chosen. The mapping procedure described is tested by comparing its results with all the most accurate experimental mapping data reported so far. The comparison demonstrates that the exact positions of all the nucleosomes appear to be determined exclusively by the nucleotide sequences.