Small angle scattering of cell nuclei

Neutron and X-ray small angle scattering techniques have been applied to study chromatin structure inside different types of cell nuclei. Scattering from genetically inactive chicken erythrocyte nuclei exhibits a maximum at Q = 0.1-0.15 nm-1 which cannot be observed by studying isolated chromatin derived from the same kind of cells. In highly active transcribing rat liver nuclei such a nuclear pattern is absent. The radius of gyration of isolated "superbeads" was determined. It is discussed whether the characteristic maximum of the nuclei originates from this superstructural organisation of chromatin. Rat liver nuclei were fractionated on sucrose gradients in order to determine whether the absence of the extra maximum in scattering profiles of these nuclei is due to overlapping effects of different chromatin organisation in the various cell types of the liver. As compared to unfractionated nuclei no strong deviations in the scattering profiles of the fractions could be observed. Erythrocyte nuclei were dialysed in buffers differing in the ionic strength of monovalent cations. The typical maximum from the nuclei is shifted from 60 nm (very low salt concentration) to about 35 nm (physiological ionic strength) and is linearly proportional to the decreasing radius of the nuclei. In conclusion, chromatin structure inside the nucleus has a scattering maximum due to an ordered packing of the fibres which is absent in nuclei with high genetic activity.     

The superstructure of chromatin and its condensation mechanism

Synchroton radiation X-ray scattering experiments have been performed on chicken erythrocyte chromatin fibres over a wide range of ionic conditions and on various states of the fibres (i.e. "native" in solution, in gels and in whole nuclei; chromatin depleted of the H1 (H5) histones and chromatin with bound ethidium bromide). A correlation between the results obtained with the various chromatin preparations provides evidence for a model according to which at low ionic strength the chromatin fibre already possesses a helical superstructure, with a diameter comparable to that of condensed chromatin, held together by the H1(H5) histone. The most significant structural modification undergone upon an increase of the ionic strength is a reduction of the helix pitch, this leads to condensation in a manner similar to the folding of an accordion. The details of this process depend on whether monovalent or divalent cations are used to raise the ionic strength, the latter producing a much higher degree of condensation. Measurements of the relative increase of the mass per unit length indicate that the most condensed state is a helical structure with a pitch around 3.0-4.0 nm. In this paper we give a detailed presentation of the experimental evidence obtained from static and time-resolved scattering experiments, which led to this model.     

X-ray small angle scattering study of chromatin as a function of fiber length

This work investigates the structure of native calf thymus chromatin as a function of fiber length and isolation procedures by using X-ray small angle scattering technique. Two methods of chromatin isolation have been compared in order to better understand the differences reported by various authors in terms of chromatin high order structure. In addition to these experimental results the effects of shearing have also been studied. In order to explain the differences among these chromatin preparations we built several models of chromatin fibers (represented as a chain of spherical subunits) assuming increasing level of condensation at increasing salt concentrations. For all these fiber models the corresponding theoretical X-ray scattering curves have been calculated and these results have been used to explain the influence of fiber length on the scattering profiles of chromatin. The comparison between experimental and theoretical curves confirms that the high molecular weight chromatin-DNA prepared by hypotonic swelling of nuclei (without enzymatic digestion) displays a partially folded structure even at low ionic strength, whereas the low molecular weight chromatin-DNA prepared by a brief nuclease digestion appears very weakly folded at the same ionic conditions.     

The superstructure of chromatin and its condensation mechanism

Comparison between the internucleosomal distance found by X-ray solution scattering for chicken erythrocyte (23 nm) and sea urchin (30 nm) chromatin indicates that this distance is proportional to the linker length. The diameter of the condensed sea urchin chromatin fibers is about 45 nm which is significantly larger than in chicken erythrocyte chromatin (35 nm). Trivalent cations (Gd, Tb, Cr) and the polyamines spermine and spermidine were found to induce compaction at much lower concentrations than the divalent cations but Gd, Tb and Cr induce aggregation before full compaction of the fibers. The influence of hydrogen bonding is illustrated by comparison of the effects of NaCl, ammonium chloride and alkylammonium chlorides on condensation. Solubility experiments indicate that there is a nearly linear dependence of the Mg^-- concentration at which precipitation occures on chromatin concentration and confirm the differences between cations observed by X-ray scattering.The chicken erythrocyte chromatin samples were further characterized by their reduced electric dichroism. The values found are consistent with the model derived from X-ray scattering and are compared with those reported in the literature.     

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.     

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.     

The content of various active and inactive genes in chromatin fractions with different accessibilities of DNA to polycyclic aromatic hydrocarbons

Nuclear chromatin was separated into four fractions according to solubility in low (0.2 mM MgCl2, 10 mM Tris-HCl, pH 7.6) and high (2 M NaCl) ionic strengths after digestion of nuclear DNA with nucleases. In nuclear matrix DNA the ratio of active to inactive genes was always higher than that in the original total DNA, i.e., 25 times greater in rat liver nuclei. In DNA released from the nuclei into a low ionic strength buffer the active to inactive gene ratio was lower than in total DNA (3.7 times as low in case of rat liver nuclei). The amount of carcinogens in matrix DNA exceeded that of DNA soluble in a low ionic strength buffer (3-4 times in case of rat liver nuclei and 16 times in case of hamster embryo cells). The two other fractions occupied an intermediate position between the above said fractions of DNA. The experimental results suggest that the level of carcinogen-induced modifications may be increased in active genes, including transcribed protooncogenes.     

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.     

Detection of endonuclease activity and several features of chromatin autolysis in brain cell nuclei]

The presence of Ca2+, Mg2+-dependent endonuclease activity in isolated brain cell nuclei was demonstrated and a comparison of some peculiarities of chromatin autolysis in rat brain and liver cell nuclei was carried out. Endogenous brain nuclease hydrolyzes chromatin into its structural subunits; its specific activity is 10,5 times as low as compared to the endogenous nuclease activity in rat liver nuclei. The dependency of the chromatin autolysis rate on pH and ionic composition of the incubation medium in isolated rate brain and liver nuclei appeared to be the same. The presence of Mn2+ changed the autolysis nature both in brain and in liver cell nuclei, the relative (as compared to Mg2+-dependent) Mn2+-dependent activity being higher in the brain cell nuclei. Possible differences of brain and liver chromatin structure (e. g. the presence of regions free of nucleosomic organization in brain chromatin) are assumed.     

Effect of chromatin decondensation on the intranuclear matrix

We have studied the effect of chromatin condensation on the morphology of the residual structures isolated from rat liver nuclei. DNAse I digestion followed by high salt extraction of nuclei in the presence of Mg++ yields residual structures consisting of a dense peripheral layer surrounding an internal network, similar to those described by Berezney and Coffey [6]. These structures are stable at low ionic strength in the presence of EDTA. When nuclei swollen in EDTA are digested with DNAse II in the presence of EDTA, structures devoid of internal network are obtained even without subsequent treatment with high salt. When swollen nuclei are exposed to Mg++ a specific recondensation of chromatin takes place. The residual structures from recondensed nuclei are similar to those isolated from control nuclei in the presence of Mg++. The results suggest that the integrity and stability of the intranuclear matrix are acquired in the course of the isolation procedure and this is favoured by chromatin condensation.     

Cations and the accessibility of chromatin to nucleases.

When rat liver nuclei prepared with polyamines as stabilising cations are digested with DNAase II, release of both inactive chromatin and Mg-soluble, active chromatin is greatly reduced, in comparison to digestion of liver nuclei prepared with Mg2+ as stabilising cation. Chromatin release from polyamine stabilised nuclei is also inhibited relative to Mg-stabilised nuclei following digestion with micrococcal nuclease under two very different cation conditions. Nuclei prepared with polyamines and monovalent ions as stabilising cations exhibit properties intermediate between these two extremes with both nucleases. These effects are due to residual binding of polyamines to chromatin, which is thus maintained in a condensed state, inaccessible to nucleases. Since polyamine binding is not easily reversed, concentrations of polyamines and other cations must be rigidly controlled in experiments on chromatin structure if artefacts are to be avoided. The significance of these findings to the nature and properties of active chromatin within the intact nucleus is considered.     

Organization in the cell nucleus: divalent cations modulate the distribution of condensed and diffuse chromatin

The organization of rat liver nuclei in vitro depends on the ionic milieu. Turbidity measurements of nuclear suspensions in the presence of varying concentrations of divalent cations have been correlated with nuclear ultrastructure. The concentration of MgCl2 (2 mM) at which turbidity of nuclear suspensions is maximal and chromatin condensation appears most extensive is the same concentration that reportedly (Gottesfeld et al., 1974, Proc. Natl. Acad. Sci. U. S. A. 71:2193-2197) precipitates "inactive" chromatin. Thus, a mechanism is suggested by which chromatin activity and ultrastructural organization within the nucleus may be mediated. The nuclear organizational changes attendant upon the decrease in divalent cation concentration were not entirely reversible.     

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.     

Histone crosslinking patterns indicate dynamic binding of histone H1 in chromatin

Crosslinking of histone H1 molecules to each other and to the core histones with bifunctional reagents in mouse liver nuclei and chromatin was compared with that under the conditions of random 'contacts' between these molecules. The patterns of crosslinking of the H1 subfractions (H1A, H1B, and H10) to each other in nuclei, chromatin and in solution at different ionic strengths due to random collisions were essentially the same. Moreover, the contacts between the H1 molecules were qualitatively the same in nuclei, chromatin and in solution also at the level of the chymotryptic halves of the H1 molecules. The contacts between the H1 molecules and the core histones in nuclei were similar to those obtained in chromatin at 70 mM NaCl, when H1 molecules readily migrate, and at 0.6 M NaCl, when H1 molecules are dissociated from chromatin. We conclude that spatial arrangement of H1 subfractions and mutual orientation of H1 molecules in isolated nuclei are random-like at least in terms of cross-linking. The static and dynamic models of histone H1 binding to chromatin compatible with the known data are considered. Although unequivocal verification of the models is not possible at present, the dynamic models do correspond better to recent data on the location of the histone H1 in nuclei and chromatin.     

Visualization of chromatin substructure: upsilon bodies

Spread chromatin fibers, from isolated eucaryotic nuclei, reveal linear arrays of spherical particles (upsilon bodies), about 70 A in diameter, connected by thin filaments about 15 A wide. These particles have been observed in freshly isolated nuclei from rat thymus, rat liver, and chicken erythrocytes. In addition, upsilon bodies can be visualized in preparations of isolated sheared chromatin, and in chromatin reconstructed from dissociating solvent conditions (i.e., high urea-NaCl concentration). As a criterion for perturbation of native chromatin structure low-angle X-ray diffraction patterns were obtained from nuclear pellets at different stages in the preparation of nuclei fro electron microscopy. These results suggest that the particulate (upsilon body) structures observed by electron microscopy may be closely related to the native configuration of chromatin.     

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.     

The superstructure of chromatin and its condensation mechanism

Changes in the structure of chicken erythrocyte chromatin fibres at low ionic strength resulting from enzymatic digestion, thermal denaturation and binding of Netropsin and Distamycin were monitored by synchrotron X-ray solution scattering. Digestion with micrococcal nuclease confirms the previous assignment of the 0.05 nm^-1 band to an interference between nucleosomes with an average distance of 23 nm. The results of thermal denaturation indicate that above 40°C there is a progressive increase of the internucleosomal distance and that above 60°C the characteristic structure of the chromatin fibre is destroyed. Binding of Netropsin and Distamycin also results in an increase of the internucleosomal distance which can be estimated to correspond to about 0.2 nm/mol.     

γ-线辐射对大鼠肝脾染色质及转录活性染色质模板活性的影响

 本文从染色质及转录活性染色质的模板效率探讨辐射对核转录活性影响的机制。实验结果表明:(1)肝脾染色质模板功能的变化分别平行与肝脾细胞核转录活性的变化提示,辐射至少部份是通过改变染色质的模板功能而影响细胞核的转录活性;(2)体外照射下,活性染色质模板活性较非活性染色质改变明显,提示射线可能主要是通过影响活性染色质区域的模板功能而改变核合成RNA的能力。     

The effects of sodium and magnesium-ion interactions on chromatin structure and solubility

The effects of sodium and magnesium-ion interactions on chromatin structure and solubility were examined in isolated mouse liver nuclei. To facilitate this study, a simple assay of chromatin structure was developed, based on the absorbances at 260 nm (A260) and 320 nm (A320) of nuclei in test solutions. By subtracting the A320 from the A260, a single "spectral index" was obtained which served as a useful, but not absolute, indicator of chromatin structure. Electron microscopy verified the validity of this approach. The results indicate that either 200 mM NaCl or 0.5 mM MgCl2 were capable of preserving the native 20 to 30 nm chromatin fiber structure. Below 200 mM NaCl, the native fiber progressively uncoiled to the 10 nm unit fiber. The presence of 0.5 mM MgCl2 inhibited this uncoiling. Only divalent cations stabilized condensed chromatin (heterochromatin) within the nucleus. Monovalent and divalent cations interacted with one another at critical concentrations and modified their individual effects on chromatin structure; e.g., 10 to 25 mM NaCl interfered with the action of 0.5 to 1.5 mM MgCl2, causing a complete loss of condensed chromatin. Maximum solubility of micrococcal nuclease-digested chromatin occurred at 10 mM NaCl, which treatment allowed the chromatin to unfold to the 10 nm fiber. However, ionic conditions that disrupted condensed chromatin but maintained the native chromatin fiber morphology still resulted in relatively high yields of soluble chromatin. Minimum solubility occurred under conditions which preserved the structure of condensed chromatin.     

Phase transitions in nuclei and chromatin. Is nuclear volume controlled by the chromatin or by the nuclear matrix?

Changes in the volume of rat liver nuclei have been monitored as a function of modifications in ionic environment (from 0 to 20 mM), temperature (from 4 to 37 degrees C), and pH (from 1 to 8). An abrupt reduction of nuclear volume occurred with increasing ion concentration, this contraction being more pronounced with bivalent (either Ca2+ or Mg2+) than with monovalent (either Na+ or K+) cations. The lowering of pH produced a similar effect. Parallel changes in chromatin structure took place at the same time as phase-like transitions. Atomic absorption spectroscopy allowed determination of free and nuclei-bound ions, pointing to the presence of a sizeable number of free binding sites for chromatin-DNA even within intact nuclei. DNA-phosphate sites appear to be neutralized by ions strictly according to the size of the electric charge and polyelectrolyte theory. Partial digestion (by micrococcal nuclease) or simple breaks (by chemical carcinogens) of the chromatin-DNA fiber caused respectively elimination or reduction of the abrupt volume changes in the intact nuclei. The apparent role of chromatin structure versus nuclear matrix in determining the shape and volume of intact nuclei is briefly discussed.