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.     

Influence of histones H1/H5 on the DNA coiling in the nucleosome — electric dichroism and birefringence study

Removal of histones H1 and H5 from chicken erythrocyte mononucleosomes results in a large increase of the negative electric birefringence and dichroism, and of the relaxation times, towards the values observed for mononucleosomal DNA. Cross-linking with dimethylsuberimidate does not yield important changes in the electro-optical properties of mononucleosomes, provided that the reaction is performed at low ionic strength. We suggest that in the absence of H1/H5 the linker DNA is flexible, and that this DNA tail is unwound at low ionic strength and responsible for most of the negative anisotropy of these particles. Bipolar pulse experiments revealed that the orientation mechanism of chromatosomes and H1/H5-depleted nucleosomes is predominantly of the induced dipole type.     

Electrostatics and electrodynamics of bacteriorhodopsin.

The stationary electric dichroism of bacteriorhodopsin is in qualitative, but not quantitative, agreement with the orientation function for disks having a permanent dipole directed perpendicular to the plane and an induced dipole in the plane. Fits of the orientation function to data measured at low field strengths demonstrate: an increase of the permanent dipole moment mu with the square of the disk radius r2, whereas the polarizability alpha increases with r4; the ionic strength dependence is small for mu and clearly stronger for alpha; the permanent dipole moment is 4x10(6) D at r = 0.5 micron. According to the risetime constants, the induced dipole does not saturate and increases to 4x10(8) D at 40 kV/cm and r = 0.5 micron. The data indicate that the permanent dipole is not of some interfacial character but is due to a real assymetry of the charge distribution. The experimental dipole moment per protein monomer is approximately 55 D, whereas calculations based on the structure of Grigorieff et al. (Grigorieff, N., T.A. Ceska, K.H. Downing, J.M. Baldwin, and R. Henderson. 1996. Electron-crystallographic refinement of the structure of bacteriorhodopsin. J. Mol. Biol. 259:393-421) provide a dipole moment of approximately 570 D. The difference is probably due to a nonsymmetric distribution of charged lipid residues. It is concluded that experimental dipole moments reflect the mu-potential at the plane of shear for rotational diffusion, in analogy to the sigma-potential used for translational diffusion. It is suggested that the permanent dipole of bacteriorhodopsin supports proton transport by attraction of protons inside and repulsion of protons outside of the cell. Dichroism rise curves at field strengths between E = 150 and 800 V/cm reveal an exponential component with time constants tau 3r in the range between 1 and 40 ms, which is not found in Brownian dynamics simulations on a disk structure using hydrodynamic and electric parameters characteristic of bacteriorhodopsin disks. The experimental data suggest that this process reflects a cooperative change of the bacteriorhodopsin structure, which is induced already at a remarkably low field strength of approximately 150 V/cm.     

An electro-optical study of the mechanisms of DNA condensation induced by spermine

Condensation of DNA by spermine has been studied by electric dichroism, electric birefringence and rotational relaxation times at 1 mM ionic strength. Using Manning's theory, we found that condensation occurs for a fraction of neutralized phosphate charges (r) equal to 0.90, in good agreement with previous studies using spermidine, synthetic polyamines and trivalent cations (e.g. Co(NH3)36 +, Tb3 +). Our results are compatible with the presence in solution of torus-shaped condensed structures in a narrow range of spermine concentration; further addition of the polyamine produced precipitation due to the self-aggregation of several toroids. For spermine concentrations lower than that required for collapse, important changes of the orientation mechanism in the electric field and of DNA stiffness were observed. Whereas free DNA was mainly oriented by a fast-induced polarizability mechanism, DNA-spermine complexes displayed an important permanent dipole component, in the spermine concentration range where extension of the DNA molecules was present. The birefringence relaxation times suggested that, in the first step, the stiffness of the DNA molecules increased, and then, at higher spermine concentration, bending of the DNA molecules occurred so that condensation into toroidal particles became possible.     

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.     

Unravelled nucleosomes,nucleosome beads and higher order structures of chromatin: Influence of non-histone components and histone H1

Effects of non-histone components and histone H1 on the morphology of nucleosomes and chromatin were studied by electron microscopy. Soluble rat liver ehromatin was depleted of non-histone components [NH]or non-histone components and H1 [NH and H1] by dissociation and subsequent fractionation in sucrose gradients in the presence of 300 to 350 mm or 500 mm-NaCl, respectively. In reconstitution experiments the depleted samples were mixed either with [NH] or with [NH and H1] or with purified H1. The morphology of the ionic strength-dependent condensation of the samples was monitored by electron microscopy using 0 mm to 100 mm-NaCl. Based on the appearance of the different types of fibres in very low salt (0 mm up to 10 mm-NaCl), namely the zigzag-shaped, the beads-on-a-string or the DNA-like filaments, it is possible to distinguish between nucleosomes, partially unravelled nucleosomes and unravelled nucleosomes, respectively. Only those fibres which were zigzag-shaped at low ionic strength condense at increasing ionic strength into higher order structures of compact fibres. We demonstrate the dependence of the appearance of nucleosomes and chromatin upon its composition and upon the ionic strength of the solvent.[NH] have no detectable influence upon the formation of higher order chromatin structures, but they can prevent the unravelling of nucleosomes at very low ionic strength, presumably by charge shielding.For the appearance of zigzag-shaped fibres and for the condensation into compact fibres with increasing ionic strength, H1 must be present in about native amounts. Partial removal of H1 (about 10%) promotes a change from fibres into tangles. This supports the model that an H1 polymer is stabilizing the higher order chromatin structures.Reconstitution experiments with purified H1 regenerated fibres containing all the features of [NH]-depleted chromatin. Reconstitution experiments with [NH and H1] promoted fibres compatible with control chromatin. Overloading of chromatin with H1 led to additional condensation. The detailed morphology of the reconstituted fibres showed local distortions. One possibility explaining these local distortions would be competition between “main” and “additional” binding sites for histone H1.     

Histone H1 can be removed selectively from chicken erythrocyte chromatin at near physiological conditions.

Histone H1 was depleted selectively from chicken erythrocyte polynucleosomes, without any detectable concomitant loss of H5 or core particle histones. The depletion is performed with ion exchange resin at low ionic strength (80 mM NaCl). The nucleosomes did not slide during the procedure. In contrast to the native chromatin, H1 depleted polynucleosomes are completely soluble in the 5--600 mM NaCl range.     

Reconstitution of chromatin higher-order structure from histone H5 and depleted chromatin

Reconstitution of the 30 nm filament of chromatin from pure histone H5 and chromatin depleted of H1 and H5 has been studied using small-angle neutron-scattering. We find that depleted, or stripped, chromatin is saturated by H5 at the same stoichiometry as that of linker histone in native chromatin. The structure and condensation behavior of fully reconstituted chromatin is indistinguishable from that of native chromatin. Both native and reconstituted chromatin condense continuously as a function of salt concentration, to reach a limiting structure that has a mass per unit length of 6.4 nucleosomes per 11 nm. Stripped chromatin at all ionic strengths appears to be a 10 nm filament, or a random coil of nucleosomes. In contrast, both native and reconstituted chromatin have a quite different structure, showing that H5 imposes a spatial correlation between neighboring nucleosomes even at low ionic strength. Our data also suggest that five to seven contiguous nucleosomes must have H5 bound in order to be able to form a higher-order structure.     

Iodination of nucleosomes at low ionic strength: conformational changes in H4 and stabilization by H1.

Radioactive iodine has been used to probe the relative reactivities of nucleosomal H4 tyrosine residues under various conditions of subphysiological ionic strength. We observe that tyrosine 72 of H4, which is not reactive over the range 20-150 mM NaCl, becomes the predominant site of iodination within H4 when nucleosomes are subjected to conditions of very low ionic strength. Conversely, the other H4 tyrosine residues, which are reactive within nucleosomes in solutions of moderate ionic strength (20-150 mM NaCl), become nonreactive when the ionic strength is reduced. This "flip-flop" in the H4 iodination pattern is the manifestation of a reversible nucleosomal conformational change. A method is presented which enables the conformational status of H4 in nucleosomes to be determined by simply electrophoresing the histones on a Triton gel after probing nucleosomes with labeled iodine. Using this technique, we demonstrate that the presence of H1 on one side of the nucleosome stabilizes a histone core domain on the other side so that all four tyrosines of H4 are maintained in their physiological ionic strength conformation even under conditions of no added salt.     

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.     

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.     

Chromatin on a membrane: accessibility of histone H5 for antibodies in the supernucleosomal structure

Histone H5 accessibility for the antibodies in chromatin was studied. Chromatin was immobilised on the nitrocellulose membrane in conditions which provide different levels of its compactization. Antiserum specific to the globular domain of histone H5 was used. It was shown, that for establishing real protection of histone H5 in the supernucleosomal structure it is necessary to use long fibers of chromatin. Their linking to the membrane must occur by a minimum quantity of points. It was established, that histone H5 is 5 times more accessive in the preparations of dispersed chromatin (low ionic strength) then in chromatin with the supernucleosomal organization (physiological ionic strength). We suppose that the small level of accessibility of histone H5 for the antibodies in the compact chromatin can be explained by some disruptions in the supernucleosomal organization. On the contrary, the long equable solenoid of nucleosomes provides complete protection of histone H5. In accordance with the results obtained, the model of ordered packaging of nucleosomes in the solenoid is discussed. In this model the point of entrance and exit of DNA on the nucleosomes, fixed by globular region of histone H5, is localized inside the solenoid.     

Electric properties and structure of DNA-restriction fragments from measurements of the electric dichroism

The electric dichroism of 17 homogeneous DNA fragments, ranging in size from 43 to 4362 base-pairs, has been analyzed in high electric fields. The orientation of the small fragments can be described in terms of an induced dipole moment, whereas the large fragments are oriented according to a constant dipole mechanism. In the intermediate size range, DNA orients according to an induced dipole mechanism at low field strengths and according to a constant dipole mechanism at high field strengths. From these observations we propose an orientation mechanism with a saturating induced dipole. The induced dipole observed at low field strengths is saturated at a field strength Eo within a transition range Em to give a constant dipole moment at high field strengths. These parameters together with the polarizability and the limit reduced dichroism are evaluated by a least-squares analysis of the experimental data. Eo and Em are found to decrease with increasing chain length from Eo approximately 40 kV/cm (Em approximately 14 kV/cm) at 65 base-pairs to 10 kV/cm (6 kV/cm) at 194 base-pairs. The polarizability is found to increase with the square of the chain length, whereas the saturated dipole increases with chain length N at low N and goes to a limit value at high N. The temperature dependence of the orientation parameters is found to be very small. The values obtained for the limit dichroism are between -1.0 and -1.3 for chain lengths between 60 and 1000 base-pairs, whereas values around -1.4 are observed at chain lengths greater than 1000 base-pairs. These data indicate that electric fields extend the contour of DNA strands at high chain lengths from a weakly bent to a more linear form. The variations of the limit dichroism observed for short fragments suggest sequence-dependent differences in the secondary structure of the helix. The experimental results are compared with numerical calculations based on simple polyelectrolyte models. For short fragments the magnitude of several electrochemical parameters can be adequately explained by a polarization of the ion cloud around the DNA molecules. However, these polyelectrolyte models do not adequately describe the observed chain length dependence of the orientation phenomena.     

Histone Hl-DNA interaction. Influence of phosphorylation on the interaction of histone Hl with linear fragmented DNA.

By measuring the fluorescence polarization of fluorescent histone H1 derivatives complexed with DNA, binding of the histone to DNA was studied as a function of ionic strength in the solution prior to and after the H1 phosphorylation on Ser-37 residue. Fluorescent labels were covalently linked either specifically to Tyr-72 residues or unspecifically to lysine residues in the H1 polypeptide chain. The values of the corresponding rotational relaxation times showed that at low ionic strength all the segments of the H1 molecule were immobilized on binding to DNA. The gradual increasing NaC1 concentration in the solution of H1-DNA complex was accompanied at first by additional retardation of the histone mobility in the complex, and then by progressive release of histone H1 from from the complex which was completed at 0.5-0.6 M NaC1 irrespective of phosphorylation. tat the same time the phosphorylation of histone H1 led to removal of the central and, presumably, N-terminal regions of H1 from DNA.     

Histone H5 promotes the association of condensed chromatin fragments to give pseudo-higher-order structures

We describe two distinct situations in which chicken erythrocyte chromatin fragments associate in solution. The erythrocyte-specific histone H5 is implicated since chromatins that do not contain H5 do not show this behaviour. Well-defined oligomers of between approximately 6 and approximately 18 nucleosomes prepared at low ionic strength condense and associate when the ionic strength is raised to 75 mM, forming pseudo-higher-order structures. The associated forms, probably predominantly dimers, are stabilized by migration of about 10% of the H5, and of the minor lysine-rich histone H1, from the non-associated forms, probably reflecting the preference of H5 for higher-order structures observed previously [Thomas, J. O. and Rees, C. (1983) Eur. J. Biochem. 134, 109-115]. Since the final (H1 + H5) content of the aggregate at 75 mM is never higher than that of the fragment prepared at low ionic strength, migration is probably to a small proportion of sites that have inevitably become vacant due to handling losses at the higher (but not at low) ionic strength. H5 thus maximizes its interactions in the condensed state of chromatin and even maintains the association of two or more fragments without continuity of the DNA. Aggregates of oligomers larger than about 18 nucleosomes may be too long to withstand hydrodynamic shear forces in the absence of such continuity. During nuclease digestion of nuclear chromatin, H5 and, to a lesser extent, H1, are released from the ends of very short fragments and bind to larger oligomers of various sizes leading to heterogeneous aggregates that survive exposure to low ionic strength. These aggregates, in contrast to those described above, have up to 60% more H5 and 20% more H1 than chromatin prepared at low ionic strength. Whether the excess H5 and H1 bind non-specifically or to a second low-affinity binding site on each nucleosome is not known. The associated forms described above (1) are well defined and potentially useful for structural studies, whereas the other aggregates (2) seem less likely to be directly relevant to the native structure of chromatin.     

Salt-induced conformational transitions in chromatin. A flow linear dichroism study

The chromatin structure in solution has been studied by the flow linear dichroism method (LD) in a wide range of ionic strengths. It is found that increasing the ionic strength from 0.25 mM Na2EDTA, pH 7.0 to 100 mM NaCl leads to a strong reduction of the LD amplitude of chromatin and inversion of the LD sign from negative to positive at 2 mM NaCl. Chromatin exhibits a positive LD maximum value at 10-20 mM NaCl. These data enable us to conclude that in very low ionic strength (0.25 mM Na2EDTA) the nucleosome discs are oriented with their flat faces more or less parallel to the chromatin filament axis. Increasing ionic strength up to 20 mM NaCl leads to reorientation of the nucleosome discs and to formation of chromatin structures with nucleosome flat faces inclined to the fibril axis. A conformational transition of that kind is not revealed in H1-depleted chromatin. The condensation of the chromatin filaments with increasing concentration of NaCl from 20 mM to 100 mM slightly influences the orientation of the nucleosomes.     

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.     

Distinct effects of histone H1 and non-histone chromosomal proteins on the structure of nucleosomes and the chromatin fibre in solution

In this study we attempt to differentiate between the effects of the non-histone chromosomal proteins and histone H1 on the structure of the nucleosomes and the chromatin fibre in solution. The properties of chromatin preparations with different histone H1 and non-histone protein compositions were compared using circular dichroism and flow linear dichroism and the following conclusions were drawn. When histone H1 is absent the non-histone proteins partially prevent the unfolding of the nucleosomes at low ionic strength. The complete blocking of this unfolding, however, is accomplished only in the presence of histone H1. The non-histone proteins do not affect the orientation of the nucleosomes along the fibre axis. Only histone H1 can maintain the positive anisotropy of the chromatin fibre.     

Structural aspects and orientation mechanism of mitochondrial F1 adenosinetriphosphatase. Evidence for a negative electric birefringence due to a permanent moment perpendicular to the long axes of the particle

The electric birefringence technique was used to investigate the steady-state birefringence, the orientational relaxation time, and the orientation mechanism of pig heart mitochondrial F1 adenosine-5'-triphosphatase (F1-ATPase). The electrooptical properties of this enzyme in solution were studied as functions of pH, protein concentration, and applied electric field. The F1-ATPase exhibits a surprising negative electric birefringence with a specific Kerr constant of -1.5 X 10(-3) esu cgs. The field-independent relaxation time was found to be 0.65 +/- 0.05 microseconds, corresponding to a rotational diffusion constant of 2.55 X 10(5) s-1. The overall size and shape of F1-ATPase have been calculated from both translational and rotational diffusion constants. The enzyme may be assumed to be an oblate ellipsoid of revolution with dimensions of about 170 X 170 X 70 A. The orientation mechanism of F1-ATPase was analyzed by fitting experimental birefringence rising curves with theoretical rising functions. The ratio of the permanent to induced dipole moment is found to be very high; therefore, the birefringence of F1-ATPase is due to a strong permanent dipole moment in a direction perpendicular to the long axes of the particle. These particular electric properties can be explained by the oligomeric structure of the protein and seem likely to play a role in its mechanism of functioning.