Viscosity of chromatin solutions increases with increasing ionic strength

Increasing the ionic strength of rat liver chromatin solutions above 0.4 M causes increasing viscosity. This indicates transformation of the compact chromatin molecules to more elongated forms. In the range of 0.4–0.5 M ionic strength histone H1 is dissociating continuously from the chromatin and the quaternary structure chromatin unravels. At ionic strength higher than 0.5 M the viscosities of chromatin solutions are furthermore increasing due to structural deformation. Near 0.7 M ionic strength the core histones H2A and H2B begin to dissociate from the chromatin, and the opening of the nucleosome cores leads to increasing elongation of the chromatin molecules.     

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.     

Structure of the interphase chromatin in the ciliata Bursaria truncatella macronucleus. II. Loop organization of inactive chromatin clumps

Electron microscopic study of chromatin organization in isolated macronuclei of a ciliate Bursaria truncatella showed macronuclear chromatin to be organized in compact clumps 120--180 nm in diameter linked with each other by one or several chromatin fibres. Macronucleus being dispersed in a solution of low ionic strength, radial loops basically of nucleosomal structure start appearing around chromatin clumps. Long-time dispersing of macronuclear chromatin brings complete decompactization of chromatin clumps into a set of nucleosome fibres. The way the fibres of interphase chromatin are packed in a chromatin clump is discussed.     

Highly compact folding of chromatin induced by cellular cation concentrations. Evidence from atomic force microscopy studies in aqueous solution

We have performed a very extensive investigation of chromatin folding in different buffers over a wide range of ionic conditions similar to those found in eukaryotic cells. Our results show that in the presence of physiological concentrations of monovalent cations and/or low concentrations of divalent cations, small chicken erythrocyte chromatin fragments and chromatin from HeLa cells observed by transmission electron microscopy (TEM) show a compact folding, forming circular bodies of approximately 35 nm in diameter that were found previously in our laboratory in studies performed under very limited conditions. Since TEM images are obtained with dehydrated samples, we have performed atomic force microscopy (AFM) experiments to analyze chromatin structure in the presence of solutions containing different cation concentrations. The highly compact circular structures (in which individual nucleosomes are not visible as separated units) produced by small chromatin fragments in interphase ionic conditions observed by AFM are equivalent to the structures observed by TEM with chromatin samples prepared under the same ionic conditions. We have also carried out experiments of sedimentation and trypsin digestion of chromatin fragments; the results obtained confirm our AFM observations. Our results suggest that the compaction of bulk interphase chromatin in solution at room temperature is considerably higher than that generally considered in current literature. The dense chromatin folding observed in this study is consistent with the requirement of compact chromatin structures as starting elements for the building of metaphase chromosomes, but poses a difficult physical problem for gene expression during interphase.     

Higher-order structures of chromatin in solution.

Neutron scatter studies have been made on gently prepared chicken erythrocyte chromatin over a range of ionic strength. At low ionic strength the mass per unit length of the '10 nm nucleofilament corresponds to one nucleosome per 8--12 nm and a DNA packing ratio of between 6 and 9. From the contrast dependence of the cross-section radius of gyration of the nucleofilament the following parameters have been obtained; RgDNA' the cross-section radius of gyration (Rg) when DNA dominates the scatter; RgP, the cross-section Rg when protein dominates the scatter; Rc, the cross-section Rg at infinite contrast and alpha, the constant which describes the dependence of the cross-section Rg on contrast variation. From our understanding of the structure of the core particle, various arrangement of core particles in the nucleofilament have been tested. In models consistent with the above parameters the core particles are arranged edge-to-edge or with the faces of the core particles inclined to within 20 degrees to the axis of the nucleofilament. With increase of ionic strength the transition to the second-order chromatin structure has been followed. This gave the interesting result that above 20 microM NaCL or 0.4 mM MgCL2 the cross-section Rg increases abruptly to about 9 nm with a packing ratio of 0.2 nucleosome/mn and with further increase of ionic strength the Rg increases to 9.5 nm while the packing ratio increases threefold to 0.6 nucleosome/nm. This suggests a family of supercoils of nucleosomes which contract with increasing ionic strength. In its most contracted form the diameter of the hydrated supercoil has been found from the radial distribution function to be 34 nm. Models for the arrangements of core particles in the 34-nm supercoil 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.     

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.     

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.     

A magnetic viscometer for shear-sensitive macromolecules

This paper is a report about a rotation-viscometer with a submerged rotor which has been developed for measuring the viscosity of biological macromolecules. The device avids the effects of surface disturbance. The rotor is centered and height-balanced electromagnetically and is controlled by a light barrier. The driving force is rotating electromagnetic field and rotor revolution periods are measured by an electronic timer controlled by a second light barrier. Shearing effects are negligible if very slow revolution are pre-selected; thus, intrinsic viscosity for DNA can be obtained by merely extrapolating the concentration dependence. In contrast to DNA, chromatin has a very low viscosity with almost no dependence on concentration. If the ionic strength of a chromatin solution is decreased, the viscosity increases due to structural unfolding.     

Electric birefringence of DNA and chromatin. Influence of divalent cations.

The effects of divalent cations on the DNA and chromatin conformation have been investigated by electric birefringence and birefringence relaxation measurements at low and constant ionic strength (0.001). An important decrease of the intrinsic optical anisotropy of DNA has been found in the presence of Mn2+ and Cu2+, but not with Mg2+. A complex variation of the mean relaxation time with the ratio I/P of ion to DNA-phosphate molar concentration has been evidenced in the presence of Mn2+ and Cu2+, while the mean relaxation time monotonously decreased in the presence of Mg2+. These observations are interpreted in terms of a specific organization of DNA in a compact, rigid structure, in the presence of Mn2+ and Cu2+, and a non-specific coiling in the presence of Mg2+. Drastic conformational changes encountered by chromatin in the presence of Mg2+ and Mn2+ cations have also been evidenced through electric birefringence measurements. They are interpreted by the formation of a superhelical compact arrangement of nucleosome strings which yielded a reversal of the birefringence sign with respect to the negative anisotropy observed in the presence of Na+ ions. The removal of the histone H1 prevented the appearance of this quaternary structure. More extended fragments of the chromatin chain obtained by ECTHAM chromatography of sonicated chromatin could not afford such compact arrangements.     

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.     

Chromatin structure. Further evidence against the existence of a beaded subunit for the 30-nm fiber

The size distribution of chromatin fragments released by micrococcal nuclease digestion of liver chromatin at various ionic strengths was examined. Below 20 mM ionic strength, gradient profiles with a peak centered at 6 nucleosomes are generated, whereas between 20 and 50 mM the peak is always centered on 12 nucleosomes, and above 50 mM ionic strength the 30-nm fiber becomes less accessible to the nuclease and there is a corresponding increase in the size distribution of fragments in the gradients. However, extensive digestions always give profiles with a peak of 12 nucleosomes as nuclease-resistant dodecamers accumulate. All of these observations are consistent with the winding of the 10-nm polynucleosome chain into a helical coil commencing at about 20 mM ionic strength. The helical turns are stabilized by histone H1 interactions between 20 and 50 mM ionic strength producing stable dodecamers. Above 50 mM ionic strength the coil condenses longitudinally and the profiles are consistent with a random attack of this fiber by the nuclease. Consequently it is not necessary to invoke the existence of a subunit bead to explain the profiles. We further define the conditions at which specific structural transitions take place and provide methodology for the preparation of chromatin at various levels of condensation.     

Histone H1: Ultracentrifugation studies of the effects of ionic strength and denaturants on the solution conformation

The conformation of histone H1 has been examined under native and denaturing conditions in the absence of DNA or chromatin. Sedimentation coefficients were determined for Histone H1 in 0.1 m KCl and in 6 m guanidine hydrochloride solutions at pH 7.4. The influence of ionic strength on the conformation of histone H1 has been determined by measurement of the sedimentation coefficient in tetramethylammonium chloride solutions of up to 2.5 m and extrapolated to infinite ionic strength. Results from these experiments suggest that the native conformation of histone H1 is very asymmetric in shape. The molecule is best described as a prolate ellipsoid with axes of 312 Å (2a) and 16 Å (2b) in low ionic strength media and also as a prolate ellipsoid with axes of 202 Å (2a) and 20 Å (2b) at high ionic strength or when associated with polyanions, e.g., DNA. Denaturation of histone H1 by guanidine hydrochloride was found to be completely reversible. In 6 m guanidine hydrochloride, the H1 molecule collapses to a sphere but the original extended conformation of the protein is readily restored on dialysis. This suggests rigid conformational requirements for the H1 molecule as incorporated into chromatin. The shape and dimensions for the H1 molecule at high ionic strength are not sufficiently conclusive to locate H1 in the chromatin structure. It is proposed, however, that viable models for chromatin architecture must be consistent with the histone H1 solution dimensions obtained here.     

The involvement of histone H1[0] in chromatin structure.

Micrococcal nuclease digestion and light scattering are used to compare native chromatins with various histone H1[0] contents. The experimental data show that the higher the H1[0] content, the greater the ability to form compact structures with increasing ionic strength, and the lower the DNA accessibility to micrococcal nuclease. On the contrary, reconstituted samples from H1-depleted chromatin and pure individual H1 fractions behave in such a way that samples reconstituted with pure H1 degree give rise to a looser structure, more accessible to nuclease than samples reconstituted with H1-1. This contradiction suggests that the effect of H1o on chromatin structure must originate from the interaction of this histone with other components in native chromatin among which other histone H1 subfractions are good candidates.     

Higher Order Structure of Chromatin: Influence of Ionic Strength and Proteolytic Digestion on the Birefringence Properties of Polynucleosomal Fibers

Abstract

Effects of ionic strength and proteolytic digestion on the conformation of chromatin fibers were studied by electric birefringence and relaxation measurements. The results confirm that at low ionic strength chromatin presents structural features reflecting those observed in the presence of cations. Soluble chromatin prepared from rat liver nuclei by brief nuclease digestion exhibits a positive birefringence. As the salt concentration is increased, the transition to a compact solenoidal structure is deduced from changes in electro-optical properties: the positive birefringence gradually decreases and the observed reduction in 40 mM NaCl is nearly 95%; the relaxation time decreases dramatically and the character of the kinetic changes since the decay of birefringence described initially by a spectrum of relaxation times becomes monoexponential.

On digestion with proteases at low ionic strength we observe at first a rapid increase of the positive birefringence concomitant with an increase of the relaxation time. Then the birefringence decreases and becomes negative. Chromatin undergoes two successive transitions: the first transition is explained by a lengthening of nucleosomal chains without modification of the orientation of nucleosomes within the superstructure and the second one by the unwinding of the DNA tails and internucleosomal segments.

When chromatin is digested at 30 mM NaCl we find a single unfolding transition characterized by the decrease of birefringence and a slight increase in the relaxation time. The results imply that the positive birefringence of chromatin does not depend on the presence of whole histone HI and that a salt concentration of 30 mM NaCl is sufficient to modify the initial site or/and the effects of proteolytic attack.     

Higher order structure of chromatin: influence of ionic strength and proteolytic digestion on the birefringence properties of polynucleosomal fibers

Effects of ionic strength and proteolytic digestion on the conformation of chromatin fibers were studied by electric birefringence and relaxation measurements. The results confirm that at low ionic strength chromatin presents structural features reflecting those observed in the presence of cations. Soluble chromatin prepared from rat liver nuclei by brief nuclease digestion exhibits a positive birefringence. As the salt concentration is increased, the transition to a compact solenoidal structure is deduced from changes in electro-optical properties: the positive birefringence gradually decreases and the observed reduction in 40 mM NaCl is nearly 95%; the relaxation time decreases dramatically and the character of the kinetic changes since the decay of birefringence described initially by a spectrum of relaxation times becomes monoexponential. On digestion with proteases at low ionic strength we observe at first a rapid increase of the positive birefringence concomitant with an increase of the relaxation time. Then the birefringence decreases and becomes negative. Chromatin undergoes two successive transitions: the first transition is explained by a lengthening of nucleosomal chains without modification of the orientation of nucleosomes within the superstructure and the second one by the unwinding of the DNA tails and internucleosomal segments. When chromatin is digested at 30 mM NaCl we find a single unfolding transition characterized by the decrease of birefringence and a slight increase in the relaxation time. The results imply that the positive birefringence of chromatin does not depend on the presence of whole histone H1 and that a salt concentration of 30 mM NaCl is sufficient to modify the initial site or/and the effects of proteolytic attack.     

Studies on the stability of the higher-order structure of rat liver chromatin containing high-mobility-group proteins

The stability of the higher-order structure of chromatin containing high-mobility-group (HMG) proteins has been studied in rat liver nuclei by mild micrococcal nuclease digestion at low temperature and fractionation by sucrose gradient centrifugation. Nuclei preparation and digestion, chromatin solubilization and analysis have been carried out in two ionic conditions, 140 mM and 40 mM monovalent cation concentration, avoiding drastic changes in ionic conditions and temperature during preparation and analysis. During the time course of digestion at 140 mM ionic strength a material stable at 80 S appears, whose DNA is cleaved at values around 12 nucleosomes. The distribution of HMG proteins in different chromatin fractions was analyzed by immunodot using antibodies elicited against proteins HMG-1, HMG-2, and HMG-14 and 17. It appears that these proteins have a distribution distinctly different from the bulk of chromatin. They are never found in the chromatin fragments that keep their internucleosomal interactions, indicating that these proteins tend to accumulate in points where the chromatin has a less stable structure.