Modeling apoptotic chromatin condensation in normal cell nuclei. Requirement for intranuclear mobility and actin involvement

Hallmarks of the terminal stages of apoptosis are genomic DNA fragmentation and chromatin condensation. Here, we have studied the mechanism of condensation both in vitro and in vivo. We found that DNA fragmentation per se of isolated nuclei from non-apoptotic cells induced chromatin condensation that closely resembles the morphology seen in apoptotic cells, independent of ATP utilization, at physiological ionic strengths. Interestingly, chromatin condensation was accompanied by release of nuclear actin, and both condensation and actin release could be blocked by reversibly pretreating nuclei with Ca2+, Cu2+, diamide, or low pH, procedures shown to stabilize internal nuclear components. Moreover, specific inhibition of nuclear F-actin depolymerization or promotion of its formation also reduced chromatin condensation. Chromatin condensation could also be inhibited by exposing nuclei to reagents that bind to the DNA minor groove, disrupting native nucleosomal DNA wrapping. In addition, in cultured cells undergoing apoptosis, drugs that inhibit depolymerization of actin or bind to the minor groove also reduced chromatin condensation, but not DNA fragmentation. Therefore, the ability of chromatin fragments with intact nucleosomes to form large clumps of condensed chromatin during apoptosis requires the apparent disassembly of internal nuclear structures that may normally constrain chromosome subdomains in non-apoptotic cells.     

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.     

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.     

Chromatin organization in isolated nuclei: flow cytometric characterization employing forward and perpendicular light scatter

Flow cytometric perpendicular and forward light scatters have been employed to evaluate whether the changes in chromatin organization due to ionic strength, Mg++ concentration and pH, visible in electron microscopy, can be monitored by flow cytometry. The average intensity of the perpendicular light scatter signal increased as nuclear chromatin became decondensed by lowering the ionic strength or releasing H1 histone at low pH values. These results indicate that flow cytometry signals and in particular the perpendicular light scatter allow the detection of the conformational transitions in chromatin and may therefore be useful for studying cell cycle associated morphological changes in isolated nuclei.     

Ionic strength-dependent conformational transitions of chromatin. Circular dichroism and thermal denaturation studies

High-molecular-weight chicken erythrocyte chromatin was prepared by mild digestion of nuclei with micrococcal nuclease. Samples of chromatin containing both core (H3, H4, H2A, H2B) and lysine-rich (H1, H5) histone proteins (whole chromatin) or only core histone proteins (core chromatin) were examined by CD and thermal denaturation as a function of ionic strength between 0.75 and 7.0 × 10^?3M Na⁺. CD studies at 21°C revealed a conformational transition over this range of ionic strengths in core chromatin, which indicated a partial unfolding of a segment of the core particle DNA at the lowest ionic strength studied. This transition is prevented by the presence of the lysine-rich histones in whole chromatin. Thermal-denaturation profiles of both whole and core chromatins, recorded by hyperchromicity at 260 nm, reproducibly and systematically varied with the ionic strength of the medium. Both materials displayed three resolvable thermal transitions, which represented the total DNA hyperchromicity on denaturation. The fractions of the total DNA which melted in each of these transitions were extremely sensitive to ionic strength. These effects are considered to result from intra- and/or internucleosomal electrostatic repulsions in chromatin studied at very low ionic strengths. Comparison of the whole and core chromatin melting profiles indicated substantial stabilization of the core-particle DNA by binding sites between the H1/H5 histones and the 140-base-pair core particle.     

PHYSICAL STUDIES OF ISOLATED EUCARYOTIC NUCLEI

The degree of chromatin condensation in isolated rat liver nuclei and chicken erythrocyte nuclei was studied by phase-contrast microscopy as a function of solvent pH, K⁺ and Mg⁺⁺ concentrations Data were represented as "phase" maps, and standard solvent conditions selected that reproducibly yield granular, slightly granular, and homogeneous nuclei Nuclei in these various states were examined by ultraviolet absorption and circular dichroism (CD) spectroscopy, low-angle X-ray diffraction, electron microscopy, and binding capacity for ethidium bromide Homogeneous nuclei exhibited absorption and CD spectra resembling those of isolated nucleohistone. Suspensions of granular nuclei showed marked turbidity and absorption flattening, and a characteristic blue-shift of a crossover wavelength in the CD spectra. In all solvent conditions studied, except pH < 2 3, low-angle X-ray reflections characteristic of the native, presumably superhelical, nucleohistone were observed from pellets of intact nuclei. Threads (100–200 A diameter) were present in the condensed and dispersed phases of nuclei fixed under the standard solvent conditions, and examined in the electron microscope after thin sectioning and staining Nuclei at neutral pH, with different degrees of chromatin condensation, exhibited similar binding capacities for ethidium bromide. These data suggest a model that views chromatin condensation as a close packing of superhelical nucleohistone threads but still permits condensed chromatin to respond rapidly to alterations in solvent environment.     

The superstructure of chromatin and its condensation mechanism

Solutions of rat liver and chicken erythrocyte chromatin at different ionic strngths were characterized by synchrotron X-ray solution scattering, ultracentrifugation, density and viscosity measurements. Previous observations on nuclei were extended to rat liver, calf thymus and yeast nuclei.It is shown that with monovalent cations condensation is independent of the nature of the cation whereas with divalent cations there are significant differences related to the preference of base binding over phosphate binding. The consistency of hydrodynamic and scattering results confirm the view that chromatin in solution at low ionic strength has a helix-like superstructure. A survey of X-ray and neutron scattering results in the literature shows that previous interpretations, e.g. in terms of a 10 nm filament, are incompatible with the experimental data at low resolution.     

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.     

Isolation and characterization of the nuclear matrix in Friend erythroleukemia cells: chromatin and hnRNA interactions with the nuclear matrix.

Nuclear matrices from undifferentiated and differentiated Friend erythroleukemia cells have been obtained by a method which removes DNA in a physiological buffer. These matrices preserved the characteristic topographical distribution of condensed and diffuse "chromatin" regions, as do nuclei in situ or isolated nuclei. Histone H1 was released from the nuclear matrix of undifferentiated cells by 0.3 M KCl; inner core histones were released by 1 M KCl. Nuclear matrix from differentiated cells did not maintain H1, and histone cores were fully released in 0.7 M KCl. KCl removed the core histones as an octameric structure with no evidence of preferential release of any single histone. Electron microscopy of KCl-treated matrix revealed no condensed regions but rather a network of fibrils in the whole DNA-depleted nuclei. When nuclear matrices from both types of cell were exposed to conditions of very low ionic strength, inner core histones and condensed regions remained. These observations support the contention that inner core histones are bound to matrix through natural ionic bonds or saline-labile elements, and that these interactions are implicated in chromatin condensation. hnRNA remained undegraded and tenaciously associated to the matrix fibrils, and was released only by chemical means which, by breaking hydrophobic and hydrogen bonds, produced matrix lysis. Very few nonhistone proteins were released upon complete digestion of DNA from either type of nuclei. The remaining nonhistone proteins represent a large number of species of which the majority may be matrix components. The molecular architecture in both condensed and diffuse regions of interphase nuclei appears to be constructed of two distinct kinds of fibers; the thicker chromatin fibers are interwoven with the thinner matrix fibers. The latter are formed by a heteropolymer of many different proteins.     

Chicken erythrocyte chromatin and nuclear envelope antigens

Chromatin and inner layer nuclear envelope were isolated from chicken erythrocyte nuclei. Two antisera against dehistonized chromatin and nuclear envelope of chicken erythrocytes were obtained. Using the antiserum against dehistonized chromatin of erythrocytes we found: the presence of the antigens at approximate mol. wts of 56,000 and 77,000 tightly bound with DNA and characteristic of only erythrocyte chromatin; localized antigens at approximate mol. wts of 63,000, 68,000 and 92,000 tightly bound with DNA and common only for chromatin and nuclear envelope of chicken erythrocytes; heterogeneity of the antigens tightly bound with DNA. Using the antiserum against inner layer nuclear envelope we did not find antigens specific only for nuclear envelope and absent in erythrocyte chromatin. Some of the antigens were present in the control preparations of chicken liver chromatin and may be regarded as being species specific.     

DNA intercalators induce specific release of HMG 14, HMG 17 and other DNA-binding proteins from chicken erythrocyte chromatin.

Chicken erythrocyte nuclei were incubated with DNA intercalating agents in order to isolate from chromatin specific DNA-binding proteins whose binding specificity may be determined by DNA secondary and/or tertiary structure. The intercalating agents ethidium bromide (EtBr) and propidium iodide induce the specific release of high mobility group proteins HMG 14 and HMG 17 under low ionic strength conditions. Chloroquine (CQ) intercalation also results in the selective liberation of HMG 14 and HMG 17, but, in addition, selectively releases other nuclear proteins (including histone H1A) in a pH- and ionic strength-dependent fashion. The use of this new 'elutive intercalation' technique for the isolation and purification of 'sequence-specific' and 'helix-specific' DNA-binding proteins is suggested.     

Dynamics of chromatin decondensation reveals the structural integrity of a mechanically prestressed nucleus

Genome organization within the cell nucleus is a result of chromatin condensation achieved by histone tail-tail interactions and other nuclear proteins that counter the outward entropic pressure of the polymeric DNA. We probed the entropic swelling of chromatin driven by enzymatic disruption of these interactions in isolated mammalian cell nuclei. The large-scale decondensation of chromatin and the eventual rupture of the nuclear membrane and lamin network due to this entropic pressure were observed by fluorescence imaging. This swelling was accompanied by nuclear softening, an effect that we quantified by measuring the fluctuations of an optically trapped bead adhered onto the nucleus. We also measured the pressure at which the nuclear scaffold ruptured using an atomic force microscope cantilever. A simple theory based on a balance of forces in a swelling porous gel quantitatively explains the diffusive dynamics of swelling. Our experiments on decondensation of chromatin in nuclei suggest that its compaction is a critical parameter in controlling nuclear stability.     

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.     

The `compartmentation'' of choline acetyltransferase within the synaptosome

1. Choline acetyltransferase may be isolated in either a bound or soluble form after hypo-osmotic treatment of a crude synaptosome fraction, depending on the conditions. 2. In the bound form, the enzyme appears to be associated with the larger membrane fragments rather than with synaptic vesicles. 3. The bound form is predominant at slightly acid pH values and low ionic strength, the soluble form under more physiological conditions of pH and ionic strength. 4. Sodium chloride, potassium chloride, magnesium chloride and calcium chloride at similar ionic strengths solubilize the enzyme. 5. Choline acetyltransferase was found to be soluble under these conditions after release from synaptosomes from rat and pigeon cerebra, guinea-pig cortex and rabbit cortex, caudate nuclei, diencephalon and midbrain. 6. Certain isoenzymes of lactate dehydrogenase behaved similarly.     

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.     

Cycle specific association of nascent chromatin with nuclear envelope components in Physarum polycephalum.

The action of heparin on isolated nuclei derived from different phases of the mitotic cycle in plasmodia of Physarum polycephalum was studied. Heparin addition at two-fold excess over DNA concentration to nuclei in Mg-free low ionic strength buffer (10 mM TRIS-HC1, 10 mM Na2 HPO4, pH = 8) releases 60-80% of chromatin from S, G2, and mitotic phase nuclei. The RNA/protein ratio of herparin-solubilized cromatin is constant through S and G2 phases, but rises about two-fold at early prophase coincident with nucleolar breakdown. Purified nuclear envelopes were obtained from heparin-treated nuclei by sedimentation according to Bornens procedures (Nature 244, 28, 1973), and examined by transmission electron microscopy. Residual chromatin is seen at all stages with fine network of DNA fibrils in contact with the envelop. Regardless of time in S, 80% of 3H-labeled DNA was released into soluble chromatin with identical 3H/14C ratios. The residual chromatin in nuclear envelopes exhibited a preferential association of early S-DNA in nuclei engaged in early S replication, and late S preferential association in nuclei engaged in late S replication.     

Linker histone subtype composition and affinity for chromatin in situ in nucleated mature erythrocytes

The replacement linker histones H1(0) and H5 are present in frog and chicken erythrocytes, respectively, and their accumulation coincides with cessation of proliferation and compaction of chromatin. These cells have been analyzed for the affinity of linker histones for chromatin with cytochemical and biochemical methods. Our results show a stronger association between linker histones and chromatin in chicken erythrocyte nuclei than in frog erythrocyte nuclei. Analyses of linker histones from chicken erythrocytes using capillary electrophoresis showed H5 to be the subtype strongest associated with chromatin. The corresponding analyses of frog erythrocyte linker histones using reverse-phase high performance liquid chromatography showed that H1(0) dissociated from chromatin at somewhat higher ionic strength than the three additional subtypes present in frog blood but at lower ionic strength than chicken H5. Which of the two H1(0) variants in frog is expressed in erythrocytes has thus far been unknown. Amino acid sequencing showed that H1(0)-2 is the only H1(0) subtype present in frog erythrocytes and that it is 100% acetylated at its N termini. In conclusion, our results show differences between frog and chicken linker histone affinity for chromatin probably caused by the specific subtype composition present in each cell type. Our data also indicate a lack of correlation between linker histone affinity and chromatin condensation.     

Interactions of mercury and copper with constitutive heterochromatin and euchromatin in vivo and in vitro.

Mouse liver nuclei were fractionated into (condensed) heterochromatin and (noncondensed) euchromatin by differential centrifugation of sonicated nuclei. The fractions were subsequently characterized as unique nuclear species by thermal denaturation derivative profile analysis, which revealed the heterochromatin fraction enriched in satellite DNA and by endogenous metal content, which displayed partitioning of mercury in euchromatin over heterochromatin by a 10:1 ratio, with a comparatively uniform distribution of copper in both fractions. Fractionation of nuclei following in vivo challenge with copper showed enrichment of copper in heterochromatin, relative to euchromatin, while in vivo exposure to mercury resulted in a 20-fold accumulation of mercury in euchromatin, relative to heterochromatin. Using gel filtration and equilibrium dialysis to measure in vitro binding under relatively physiologic conditions of pH (6.0-7.0) and ionic strength (standard saline citrate or saline), the condensed and noncondensed chromatin fractions exhibited binding specificities toward mercury and copper similar to that observed in the in vivo metal challenge experiments. The level of mercury which binds to euchromatin in vitro, when measured either in physiologic [standard saline citrate (SSC)] or in dilute (1:100 SSC) salt solutions, was comparable (approximately 3 mug of Hg/mg of DNA) to that of in vivo euchromatin-bound mercury after 1 month of challenge with dietary metal. In contrast, copper showed little or no preference for the nuclear fractions in dilute salt solutions and displayed patterns which mimic in vivo binding only at higher ionic strengths (saline). Removal of proteins from the chromatin fractions resulted in a loss of binding specificity toward both metals. Therefore, the binding selectivity of condensed and noncondensed chromatin toward both mercury and copper appears to arise from protein or from protein-DNA associations. The state of chromatin condensation is especially critical in the case of copper.