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.     

Characteristics of the structural state of DNA in chromatin with short linker

Various fragments of pigeon brain neuron chromatin with very short linker DNA have been studied by circular dichroism (CD). The DNA structure in core particles of the brain and thymus chromatins is very similar. Linker DNA and a part of core DNA in the mononucleosomes of brain chromatin is extended. This conclusion follows from increasing CD amplitude of the brain mononucleosomes as compared with the corresponding value for thymus mononucleosomes. The internucleosome interactions stabilized the compactness of core DNA in the brain oligonucleosomes. The whole linker DNA of the brain chromatin unlike thymus chromatin is extended at low ionic strength. This fact can explain the brain chromatin ability to form a compact structure with increasing ionic strength.     

Structural transformations of oligonucleosomes from pigeon erythrocyte chromatin

The methods of velocity sedimentation and circular dichroism have been used to investigate structural rearrangements of pigeon erythrocyte oligonucleosomes isolated after digestion with micrococcal nuclease (oligonucleosomes-M) or pancreatic DNase I (oligonucleosomes-D), in the wide range of ionic strength (mu from 0.005 to 0.5). The electrophoretic analysis of DNA isolated from the oligonucleosomes has revealed internal cuts in the DNA chain of oligonucleosomes-D. In spite of this fact the conformational parameters of DNA in both types of oligonucleosomes are practically indistinguishable, and their optical and hydrodynamic properties vary in a similar way with increasing ionic strength of the solution. The specificity of DNase I action results in the ability of oligonucleosomes-D to form homogeneous associates at mu = 0.065, which seems to be due to the existence of elongated intact ends of linker DNA in oligonucleosomes-D. It has been shown that the integrity of oligonucleosomes-D in a wide range of ionic strength is maintained by histones H1 and H5, because after their dissociation the sedimentation coefficient sharply decreases. The results obtained reveal the multifunctional role of lysine-rich histones and intact linker in the processes of compaction and association of oligonucleosomes.     

The effect of histone H1 on the compaction of oligonucleosomes. A quasielastic light scattering study

The structural properties of H1-depleted oligonucleosomes are investigated by the use of quasielastic laser light scattering, thermal denaturation and circular dichroism and compared to those of H1-containing oligomers. To obtain information on the role of histone H1 in compaction of nucleosomes, translational diffusion coefficients (D) are determined for mono-to octanucleosomes over a range of ionic strength. The linear dependences of D on the number of nucleosomes show that the conformation of stripped oligomers is very extended and does not change drastically with increasing the ionic strength while the rigidness of the chain decreases due to the folding of linker DNA. The results prove that the salt-induced condensation is much smaller for H1-depleted than for H1-containing oligomers and that histone H1 is necessary for the formation of a supercoiled structure of oligonucleosomes, already present at low ionic strength.     

Comparative study of nucleosome particles in chromatin from normal and tumor cells. II. Reconstitution, compaction and association induced by ionic strength of a solution

The method of circular dichroism (CD) has been used to investigate the reconstitution of mononucleosomes from C3HA mice liver and ascitic hepatoma 22A cells chromatin. It has been revealed that the more unfolding state of DNA in ascitic nucleosomes (discovered earlier) is determined by the peculiarities of the interactions between DNA and the dimers H2A-H2B, as well as by the linker histones of the H1 group. The investigation of the DNA folding in the oligonucleosome chains with increasing ionic strength has shown complete invariability of the DNA compactness in the ascitic chromatin up to 100 mM NaCl, while in liver nucleosomes an additional folding of the linker portion of the DNA was observed within the range of 20-40 mM NaCl. Oligonucleosomes from ascitic chromatin are less inclined to association upon increasing ionic strength, as compared with those from liver chromatin.     

Structural properties of barley nucleosomes

The structural properties of barley oligonucleosomes are investigated and compared to those of rat liver oligomers. Extraction of barley chromatin was performed using mild nuclease digestion of isolated nuclei leading to a low ionic strength soluble fraction. Oligonucleosomes were fractionated on sucrose gradients and characterized for DNA and histone content. Physico-chemical studies (sedimentation, circular dichroism and electric birefringence) showed that barley oligonucleosomes exhibit properties very close to those of the H1-depleted rat liver counterparts. Moreover, in situ, barley linker DNA was more sensitive to micrococcal nuclease digestion than that of rat liver. These results suggest that barley oligonucleosomes show a less compact structure than their rat liver counterparts and appear to be in contradiction with the very condensed organization of barley chromatin previously suggested.     

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.     

Higher-order structure of nucleosome oligomers from short-repeat chromatin

Sedimentation measurements and electron microscopy at a series of ionic strengths suggest that chromatin from neurons of the cerebral cortex is able to form condensed structures in vitro that are probably several turns of a solenoid with about six nucleosomes per turn. Since neuronal chromatin has a short nucleosomal repeat (approximately 165 bp) allowing virtually no linker DNA between nucleosomes, and yet forms apparently 'normal' elements of solenoid, the packing of nucleosomes in the solenoid must be highly constrained. This permits only a limited number of possible models, and enables tentative suggestions to be made about the location of the linker DNA in the typical solenoid.     

The structural organization of dinucleosomes and oligonucleosomes. Electric dichroism and birefringence study.

The spatial organization of nucleosomes and linker DNA in dinucleosomes and oligonucleosomes of various chain lengths has been investigated through electric dichroism, birefringence and relaxation times measurements at low ionic strengths (0.5 to 2.2 mM). From the negative dichroism observed for all the samples, it is concluded that the nucleosome subunits in the oligonucleosome chain must lie with their disc planes closely parallel to the fibre axis. The large increase of the negative dichroism of dinucleosomes upon Hl removal is interpreted by the unwinding of the DNA tails and the internucleosomal segment. All the samples displayed, under bipolar pulses, a predominantly induced orientation mechanism.     

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.     

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.     

Chromatin superstructure-dependent crosslinking with DNA of the histone H5 residues Thr1, His25 and His62

The points of histone H5 interactions with DNA within nucleosomes and chromatin at different levels of compaction are delineated by identification of H5 amino acid residues that can be covalently bound to DNA. Three major crosslinkable points of H5 are His25, His62 (both within the globular part of the molecule), and N-terminal Thr1. His25 interacts with the terminal regions of nucleosomal DNA; His62 appears to bind more distal segments of the linker DNA. The His25-DNA crosslink predominates in the isolated mononucleosomes and persists throughout the chromatin condensation states studied, from extended oligonucleosomal chains to nuclei. His62 is the strongest crosslinking site in nuclei; in oligonucleosomes, the predominance of the His62-DNA crosslink requires the number of nucleosomes in the chain to be above some critical value. The Thr1-DNA crosslink is generated only in decondensed poly- or oligonucleosomes, but not in mononucleosomes. Thus, underlying the higher-order folding transitions of the nucleosomal chain is the restructuring of H5-DNA interactions.     

The structural organization of oligonucleosomes

We have used electric birefringence to study the structure of oligonucleosomes and to show the influence of histone H1 depletion on their conformation in solution. Measurements are made at low ionic strength on monodisperse samples containing up to 8 nucleosomes. For each oligomer, having H1 or not, the analysis of both relaxation and orientation times gives information about the particle's orientation mechanism through the ratio r of permanent over induced dipole terms. For native oligomers, the data confirm the previous finding of a discontinuity in hydrodynamic behavior between pentamer and heptamer: the rotational times are multiplied by 10 and r increases from 0.2 to 0.7 showing the appearance of a non-negligible contribution of a permanent dipole to the orientation mechanism. We suggest a model for the hexanucleosome at low ionic strength and discuss its implications for the higher-order structure of chromatin. The treatment for H1 depletion abolishes the transitions in electro-optical properties: the value of r remains constant, r = 0.15, and both rotational times increase progressively with the number of nucleosomes in the chain. That reflects an important unfolding of oligonucleosomal structure which we attributed to the unwinding of DNA tails and internucleosomal segments. The disc planes of nucleosomes become closely parallel to the nucleosomal chain axis.     

Nucleomeric organization of chromatin

Chromatin in the nuclei fixed in tissue and in the nuclei isolated by low ionic strength solutions in the presence of Mg2+ is represented by globular (nucleomeric) fibrils, 20-25 nm in diameter. The staphylococcal or endogenous nuclear nuclease splits the chromatin fibrils resulting in fragments corresponding to nucleomers and their multimers. Upon removal of firmly bound Mg2+ the nucleomers unfold to form chains consisting of 4-6-8 nucleosomes. Mild hydrolysis of nuclear chromatin by staphylococcal nuclease results in a split-off of mono-, di- and trimers of nucleomers sedimenting in a sucrose density gradient in the presence of EDTA as particles with the sedimentation coefficients of 37, 47 and 55S, respectively. The sedimentation coefficient for the mononucleomer in a sucrose density gradient with MgCl2 is 45S. Determination of the length of DNA fragments of chromatin split-off by staphylococcal nuclease showed that the nucleomer consists of 8 nucleosomes, while the dimer and trimer of the nucleomer consists of 14-16 and 21-24 nucleosomes, respectively. The nucleomeric monomer undergoes structural transition from the compact (45S) to the "loose" state (37S) after removal of Mg2+. This transition is completely reversible, when the nucleomer contains histone H1. The removal of the latter or dialysis of the nucleomer against EDTA in low ionic strength solutions results in a complete unfolding of the nucleomer into a nucleosomal chain fragment. A model for the nucleomer fibril structure in which the helical organization of the nucleosomal chain in the nucleomer (2 turns with 4 nucleosomes in each) is alternated with the impaired helical bonds between the nucleomers is discussed. The functional significance of the nucleomeric organization of chromatin may be an additional restriction of the site-specific recognition of DNA in chromatin with the possibility of local (at the level of one nucleomer) changes in chromatin conformation excluding this restriction.     

The Structural Organization of Oligonucleosomes

Abstract

We have used electric birefringence to study the structure of oligonucleosomes and to show the influence of histone H1 depletion on their conformation in solution. Measurements are made at low ionic strength on monodisperse samples containing up to 8 nucleosomes. For each oligomer, having H1 or not, the analysis of both relaxation and orientation times gives information about the particle's orientation mechanism through the ratio r of permanent over induced dipole terms. For native oligomers, the data confirm the previous finding of a discontinuity in hydrodynamic behavior between pentamer and heptamer: the rotational times are multiplied by 10 and r increases from 0.2 to 0.7 showing the appearance of a non-negligible contribution of a permanent dipole to the orientation mechanism. We suggest a model for the hexanucleosome at low ionic strength and discuss its implications for the higher-order structure of chromatin.

The treatment for H1 depletion abolishes the transitions in electro-optical properties: the value of r remains constant, r=0.15, and both rotational times increase progressively with the number of nucleosomes in the chain. That reflects an important unfolding of oligonucleosomal structure which we attributed to the unwinding of DNA tails and internucleosomal segments. The disc planes of nucleosomes become closely parallel to the nucleosomal chain axis.     

Homogeneous reconstituted oligonucleosomes, evidence for salt-dependent folding in the absence of histone H1

Using the method of salt dialysis, we have reconstituted histone octamers onto DNA templates consisting of 12 tandem repeats, each containing a fragment of the sea urchin 5S rRNA gene [Simpson, R.T., Thoma, F., & Brubaker, J.M. (1985) Cell 42, 799-808]. In these templates, each sea urchin repeat contains a sequence for preferred nucleosome positioning. Sedimentation velocity and sedimentation equilibrium studies in the analytical ultracentrifuge indicate that at molar histone/DNA ratios of 1.0-1.1 extremely homogeneous preparations of fully loaded oligonucleosomes (12 nucleosomes/template) can be regularly obtained. Digestion of the oligonucleosomes with micrococcal nuclease, followed by restriction mapping of purified nucleosome-bound DNA sequences, yields a complicated but consistent pattern of nucleosome positioning. Roughly 50% of the nucleosomes appear to be phased at positions 1-146 of each repeat, while the remainder of the nucleosomes occupy a number of other minor discrete positions along the template that differ by multiples of 10 bp. From sedimentation velocity studies of the oligonucleosomes in 0-0.2 M NaCl, we observe a reversible increase in mean sedimentation coefficient by almost 30%, accompanied by development of heterogeneity in sedimentation. These results, in combination with theoretical predictions, indicate that linear stretches of chromatin in the absence of lysine-rich histones exist in solution in a salt-dependent equilibrium between an extended (low salt) conformation and one or more folded (high salt) structures. In addition, by 100 mM NaCl, salt-dependent dissociation of histone octamers from these linear oligonucleosomes is observed.     

Distribution of H1 histone in chromatin digested by micrococcal nuclease.

The relative amount of H1 histone associated with isolated nucleosomes from calf thymus was determined as a function of the extent of DNA digestion by micrococcal nuclease. Generally the amount of H1 histone associated with mononucleosomes decreases with increasing digestion until 60% of the original H1 remains associated with DNA 150 base pirs or less in size. Coincidentally, H1 histone increases relative to the other histones in aggregated material that sediments through sucrose gradients to form a pellet. However, the level of H1 histone remains at control values for oligonucleosomes (dimer to hexamer) over the 30% digestion range studied. An increase in ionic strength to 0.3 M NaCl in the density gradient reveals a different pattern of H1 binding, whereby the amount of H1 reflects the average size of the DNA fragments with which it is associated. Although there is significant binding to nucleosomes per se, it appears that the major ionic involvement of H1 is with internucleosomal spacer DNA.     

Thermodynamics of condensation of nuclear chromatin. A differential scanning calorimetry study of the salt-dependent structural transitions

We present a detailed thermodynamic investigation of the conformational transitions of chromatin in calf thymus nuclei. Differential scanning calorimetry was used as the leading method, in combination with infrared spectroscopy, electron microscopy, and techniques for the molecular characterization of chromatin components. The conformational transitions were induced by changes in the counterion concentration. In this way, it was possible to discriminate between the interactions responsible for the folding of the higher order structure and for the coiling of nucleosomal DNA. Our experiments confirm that the denaturation of nuclear chromatin at physiological ionic strength occurs at the level of discrete structural domains, the linker and the core particle, and we were able to rule out that the actual denaturation pattern might be determined by dissociation of the nucleohistone complex and successive migration of free histones toward native regions, as recently suggested. The sequence of the denaturation events is (1) the conformational change of the histone complement at 66 degrees C, (2) the unstacking of the linker DNA at 74 degrees C, and (3) the unstacking of the core particle DNA, that can be observed either at 90 or at 107 degrees C, depending on the degree of condensation of chromatin. Nuclear chromatin unfolds in low-salt buffers, and can be refolded by increasing the ionic strength, in accordance with the well-known behavior of short fragments. The process is athermal, therefore showing that the stability of the higher order structure depends on electrostatic interactions. The transition between the folded conformation and the unfolded one proceeds through an intermediate condensation state, revealed by an endotherm at 101 degrees C. The analysis of the thermodynamic parameters of denaturation of the polynucleosomal chain demonstrates that the wrapping of the DNA around the histone octamer involves a large energy change. The most striking observation concerns the linker segment, which melts a few degrees below the peak temperature of naked DNA. This finding is in line with previous thermal denaturation investigations on isolated chromatin at low ionic strength, and suggests that a progressive destabilization of the linker occurs in the course of the salt-induced coiling of DNA in the nucleosome.