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.     

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.     

Irreversible changes occur in chromatin structure upon dissociation of histone H1

The role of histone H1 in the actual interactions bringing about chromatin folding is investigated by studying the reversibility of its dissociation. H1 was dissociated by increase of the NaCl concentration and reassociated by dialysis, without removal from the dialysis bag. To scrutinize the fidelity of this stoichiometric form of chromatin reconstitution, we use circular dichroism, nuclease digestion, thermal denaturation and the sensitive electric birefringence method. No alteration of the repeat length and no nucleosomal sliding are observed upon the reassociation procedure. However, under all the different conditions investigated, the original value of the positive electric birefringence is never recovered, indicating an irreversible change of structure. CD and melting profiles confirm that DNA-protein interactions are modified, and orientational relaxation time measurements indicate that these structural perturbations affect the salt-induced transition of polynucleosomal fibers. The striking conclusion of these studies is that variations of ionic concentration are sufficient to induce irreversible structural alterations affecting the higher-order folding of chromatin. It is of interest that the only sample which exhibits behavior upon reassociation comparable to that of native chromatin is the one which experienced the fastest salt transitions. We suggest that these conformational changes arise from the unbinding to DNA of certain basic tails of histone(s), and that a competition for DNA binding locations exists upon the reassociation. These results are then additional arguments (Mazen, A., Hacques, M.F. and Marion, C.,J. Mol. Biol. 194, 741-745 (1987)), to suggest that dissociation of H1 might modify a direct interaction between basic tails of core histones and H1.     

Rearrangement of chromatin structure induced by increasing ionic strength and temperature.

Native rat liver chromatin fragments exposed to 600 mM NaCl at 37 degrees C for 45 min exhibit substantial modification of their original (approximately 200 base pairs) repeating subunit structure: a new repeat of 140 base pairs, superimposed on a high background, is observed after micrococcal nuclease digestion. The same material appears, in the electron microscope, as clusters of tightly packed beads connected by stretches of 'free' DNA. These modifications are not observed when the native chromatin is incubated at 37 degrees C at NaCl concentrations up to 400 mM. When native rat liver chromatin depleted of histone H1 by tRNA extraction is exposed to ionic strengths up to 600 mM NaCl at 4 degrees C, almost no modifications of the original native repeating structure are observed. However, when the incubation is carried out at 37 degrees C in 150, 300 or 400 mM NaCl, rearrangements of the native structure occur as indicated by micrococcal nuclease digestion and electron microscopic studies. Incubation of H1-depleted chromatin at 600 mM NaCl for 45 min at 37 degrees C induces, as for the native chromatin, a complete rearrangement characterized by the appearance of a 140-base-pair repeat superimposed on a high background upon digestion by micrococcal nuclease. It is suggested that these rearrangements are mediated by hydrophobic interactions between the histone cores and are prevented at ionic strengths lower than 500 mM by the presence of histone H1.     

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.     

Structural transitions of chromatin at low salt concentrations: a flow linear dichroism study

We have studied the structure of nuclease-solubilized chromatin from Ehrlich ascites cells by flow linear dichroism (LD) using the anisotropic absorption of the DNA bases and of two intercalated dyes, ethidium bromide and methylene blue. It is confirmed that intercalation occurs preferentially in the linker part of the chromatin fiber, at binding ratios (dye/base) below 0.020. Using this information, we determined the orientation of the linker in relation to the average DNA organization in chromatin. The LD measurements indicate that the conformation of chromatin is considerably changed in the ionic strength interval 0.1-10 mM NaCl: with increasing salt concentration, the LD of the intrinsic DNA base absorption changes signs, from negative to positive, at approximately 2.5 mM NaCl. The LD of the intercalated dyes also changes signs, however, at a somewhat higher salt concentration. The results are analyzed in terms of possible allowed combinations of tilt angles of nucleosomes and pitch or tilt angles of linker DNA sections relative to the fiber axis, at different salt concentrations in the interval 0.1-10 mM NaCl. Two models for the salt-induced structural change of chromatin are discussed.     

Irreversible Changes Occur in Chromatin Structure Upon Dissociation Of Histone H1

Abstract

The role of histone H1 in the actual interactions bringing about chromatin folding is investigated by studying the reversibility of its dissociation. HI was dissociated by increase of the NaCl concentration and reassociated by dialysis, without removal from the dialysis bag. To scrutinize the fidelity of this stoichiometric form of chromatin reconstitution, we use circular dichroism, nuclease digestion, thermal denaturation and the sensitive electric birefringence method. No alteration of the repeat length and no nucleosomal sliding are observed upon the reassociation procedure. However, under all the different conditions investigated, the original value of the positive electric birefringence is never recovered, indicating an irreversible change of structure. CD and melting profiles confirm that DNA-protein interactions are modified, and orientational relaxation time measurements indicate that these structural perturbations affect the salt- induced transition of poly nucleosomal fibers. The striking conclusion of these studies is that variations of ionic concentration are sufficient to induce irreversible structural alterations affecting the higher-order folding of chromatin. It is of interest that the only sample which exhibits behavior upon reassociation comparable to that of native chromatin is the one which experienced the fastest salt transitions. We suggest that these conformational changes arise from the unbinding to DNA of certain basic tails of histone(s), and that a competition for DNA binding locations exists upon the reassociation. These results are then additional arguments (Mazen, A., Hacques, M.F. and Marion, C., J. Mol. Biol. 194, 741–745 (1987)), to suggest that dissociation of H1 might modify a direct interaction between basic tails of core histones and H1.     

Linker histone H1 per se can induce three-dimensional folding of chromatin fiber

Higher-order architectures of chromosomes play important roles in the regulation of genome functions. To understand the molecular mechanism of genome packing, an in vitro chromatin reconstitution method and a single-molecule imaging technique (atomic force microscopy) were combined. In 50 mM NaCl, well-stretched beads-on-a-string chromatin fiber was observed. However, in 100 mM NaCl, salt-induced interaction between nucleosomes caused partial aggregation. Addition of histone H1 promoted a further folding of the fiber into thicker fibers 20-30 nm in width. Micrococcal nuclease digestion of these thicker fibers produced an approximately 170 bp fragment of nucleosomal DNA, which was approximately 20 bp longer than in the absence of histone H1 ( approximately 150 bp), indicating that H1 is correctly placed at the linker region. The width of the fiber depended on the ionic strength. Widths of 20 nm in 50 mM NaCl became 30 nm as the ionic strength was changed to 100 mM. On the basis of these results, a flexible model of chromatin fiber formation was proposed, where the mode of the fiber compaction changes depending both on salt environment and linker histone H1. The biological significance of this property of the chromatin architecture will be apparent in the closed segments ( approximately 100 kb) between SAR/MAR regions.     

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.     

Histone phosphorylation in native chromatin induces local structural changes as probed by electric birefringence

In order to understand how the phosphorylation of histones affects the chromatin structure, we used electron microscopy, sedimentation velocity, circular dichroism and electric birefringence to monitor the salt-induced filament reversible solenoid transition of phosphorylated and native chromatin. Phosphorylation in vitro of chicken erythrocyte chromatin by cyclic-AMP-dependent protein kinase from porcine heart led to the modification of the histones H3 and H5 only, which were modified at a level of one phosphate and about three phosphate groups per molecule, respectively. In contrast to circular dichroism and sedimentation studies, which tend to suggest that phosphorylation of H3 and H5 does not affect chromatin structure, electron microscopy reveals that phosphorylation causes a relaxation of structure at low ionic strength. Electric birefringence and relaxation time measurements clearly prove that local structural changes are induced in chromatin: we observe a decrease of the steady-state birefringence with the appearance of a negative contribution in the signal and a marked increase of the flexibility of fibres. The component with the negative birefringence presents very short relaxation times, like those exhibited by small DNA fragments or individual nucleosomes. Two possibilities are then suggested. First, the conformational change is consistent with what would be expected from the presence of DNA segments loosely associated with the core histone H3. That the length of such segments could correspond to about one to two base-pairs per nucleosome strongly suggests that phosphorylation induces changes affecting some specific H3-DNA interactions only. This result could corroborate previous observations indicating that the N-terminal region of H3, where the site of phosphorylation is located, plays a decisive role in maintaining the superstructure of chromatin. Second, phosphorylation could introduce hinge points between each nucleosome. In this case, the negative birefringence results from partial orientation of the swinging nucleosomes. A possible mode of action of phosphorylation might be to weaken structural restraints imposed by histone H3, thus facilitating further condensation of chromatin.     

Parameters influencing the flow cytometric analysis of DNA sensitivity to nuclease S1

Some parameters that influence the analysis in situ of DNA sensitivity to digestion with nuclease S1 have been studied in isolated HeLa nuclei with flow cytometry. DNA staining with the intercalating fluorochrome propidium iodide allowed the nucleolytic activity on double-stranded (ds) DNA to be determined by monitoring the relative reduction in nuclear fluorescence intensity. Nuclei isolated in buffer at low ionic strength in order to decondense chromatin fibres, showed a lower fluorescence intensity than nuclei with native chromatin, after digestion with nuclease S1 under identical conditions. Nuclei prepared with dispersed chromatin and digested with increasing amounts of enzyme showed a decrease in fluorescence intensity that reached a limit value at about 50% of the value of undigested control samples. On the other hand, in nuclei with native chromatin, fluorescence intensity decreased only about 18%. The NaCl concentration in the reaction buffer strongly influenced the DNA sensitivity to S1 nuclease. By increasing salt molarity from 5 mM to 200 mM, the digestion of dsDNA was significantly reduced as also shown by the amount of released nucleotides from purified calf thymus DNA. The detection of DNA sensitivity to nuclease S1, as assessed by the cytometric method, was shown to be more sensitive than a biochemical technique involving hydrolysis of purines. These results indicate that both the procedure for nuclei isolation and the digestion conditions have to be carefully controlled when evaluating in situ the presence of S1-sensitive sites.     

Study of chromatin organization with trypsin immobilized on collagen membranes

Trypsin immobilized on collagen membranes has been used to digest chromatin polynucleosomes. With this method, the use of protease inhibitor is avoided and the digestion time easily controlled simply by taking the membrane out of the chromatin solution. Its most fundamental advantage is however to allow the mild removing of the most accessible histone fragments without addition of salt then without perturbation of their ionic environment. Degradation of histone fractions were correlated with conformational changes using circular dichroism and electric birefringence measurements. On digestion, the sign of birefringence reversed, becoming negative, and an increase of molar ellipticity was observed. These changes reflecting the unfolding of DNA correspond to the digestion of H1 and also of fragments of H3. This would indicate that H3 and particularly its basic terminal regions, play a fundamental role in the maintenance of chromatin in a compact structure.     

Salt effects on internal motions of superhelical and linear pUC8 DNA. Dynamic light scattering studies

The plasmid pUC8 (2717 bp) has been studied in its native superhelical and Eco RI-linearized forms by dynamic light scattering at NaCl concentrations from 1.1 mM to 1 M. The data were analyzed using the biexponential model for the dynamic structure factor described by us in a previous paper (J. Langowski, U. Giesen and C. Lehmann, Biophys. Chem. 25 (1986) 191). As before, we could identify two decay components corresponding to the center-of-mass diffusion and to internal motions of the DNA, where the fast component could be identified as a rotational diffusion contribution in the case for superhelical, but not for linear DNA. We found that the conformation of superhelical pUC8 is not affected by changing the ionic strength, while the amplitude of the internal relaxation increases approx. 2-fold when [NaCl] is raised from 1.1 mM to 1 M. The linearized DNA shows an increase of the diffusion coefficient with ionic strength which is, however, not quite as pronounced as that found by others (Z. Kam, N. Borochov and H. Eisenberg, Biopolymers 20 (1981) 2671), and, together with the unchanged conformation of the superhelical DNA, suggests a persistence length which is not strongly dependent on ionic strength. In contrast to the increasing amplitude of internal relaxation for the superhelical DNA, this amplitude remains constant or decreases slightly for linear DNA on going from 1.1 mM to 1 M salt. Our findings are further discussed with respect to possible models of the interwound form of superhelical DNA.     

The effect of low ionic strength on the circular dichroic spectrum of chromatin and nucleosomal subunits

Circular dichroism has been used to measure the conformation changes in the DNA of chromatin and chromatin subunits as a function of ionic strength. Transfer of chromatin from 0.15 M to 0.25 mM salt led to an enhancement of the circular dichroic bands at 275 and 285 nm. Removal of histone H1 did not appreciably affect the circular dichroic spectrum when measured in 0.15 M salt, but in 0.25 mM salt H1 depletion led to a marked increase in the ellipticity. Conformation changes due to low ionic strength were also observed with a 145- and a 172-bp chromatin subunit. A linear combination of the ellipticities of the DNA of the two domains in chromatin, namely core and linker, was successful for measurements at 0.15 M salt, but large unexplained discrepancies appeared with the data from measurements in 0.25 mM salt.     

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.     

Superstructural differences between chromatin in nuclei and in solution are revealed by kinetics of micrococcal nuclease digestion.

Digestion of chromatin in nuclei by micrococcal nuclease, measured as the change in the concentration of monomer-length DNA with time, displays Michaelis-Menten kinetics. Redigestion of soluble chromatin prepared from nuclei by micrococcal nuclease treatment, however, is apparently first order in enzyme and independent of chromatin concentration. This qualitative difference results from an increase in the apparent second order rate constant, kcat/Km, for liberation of monomer DNA: the apparent Km for soluble chromatin is lower by close to 3 orders of magnitude than that for chromatin in nuclei, whereas kcat decreases by less than 1 order of magnitude. Neither the integrity of the nuclear membrane nor the presence of histone H1 contributes to the high Michaelis constant characteristic of chromatin in nuclei. Moreover, differences due to the buffers used for digestion and redigestion are minimal. Low catalytic efficiency is, however, correlated with the presence of higher order chromatin superstructure. Micrococcal nuclease added to soluble chromatin under nondigesting conditions at low ionic strength (I = 0.002) co-sediments with chromatin in sucrose gradients. In 0.15 M NaCl, added nuclease no longer sediments with chromatin and redigestion kinetics become first order in both enzyme and substrate. Kinetic analysis of this type may afford an assay for native, higher order structures in chromatin. Our results suggest that micrococcal nuclease binds to soluble chromatin through additional interactions not present in nuclei, which may be partly ionic in nature.     

The salt dependence of chicken and yeast chromatin structure. Effects on internucleosomal organization and relation to active chromatin

The ionic strength dependences of yeast and chicken erythrocyte chromatin structure have been examined by analysis of nuclear DNase I and Staphylococcal nuclease digestions done under various salt and divalent cation concentrations. The basic features of yeast DNase I profiles (intracore/intercore patterns and their 5-base pair offset) remain present under all conditions tested. However, there are changes in specific parts of the patterns. In very low salt, the intercore DNase I pattern is enhanced; even very small intercore bands can be detected. Staphylococcal nuclease intracore cleavage becomes prominent. Increasing salt enhances the large DNase I intracore bands and the frequency of spacer cleavage for both nucleases. Thus, yeast has a salt-dependent higher order structure: a chromatin fiber with a prominent spacer/core distinction in (physiological) salt; a fiber with a decreased distinction between spacer and core, i.e. a more uniform fiber, in very low salt. The salt-dependent bulk changes resemble single gene chromatin changes during gene expression and may provide a model for that process. Above bands 16.5-17.5, chicken and yeast intercore patterns are coincident. Thus, at least a fraction of chicken chromatin has discrete length spacers like yeast does. This fraction may be significant, for the prominence of the intercore pattern, and hence the apparent abundance of discrete spacers, can be significantly enhanced by digestion in very low salt. The major differences between the two chromatins are in the intracore/intercore transition region: the region is larger and more complex in chicken; ionic strength changes affect the chicken transition region more strongly. Since this region of the profile corresponds to digestion near the ends of the core, that part of the nucleosome must differ in structure and in conformational flexibility in the two chromatins.     

Discrimination of assembled and disassembled forms of gizzard myosin by papain

Chicken gizzard myosin in 0.15 M or 0.5 M NaCl was cleaved at two sites of heavy chain with 2-10 micrograms/ml papain. MgATP inhibited these cleavages of myosin in 0.15 M NaCl but not in 0.5 M NaCl. The protective effect of ATP was observed at concentrations as low as 10 microM and increased in proportion to ATP concentration to a maximum at 1 mM. ADP was as effective as ATP, while adenosine 5'-[beta, gamma-imido]triphosphate, an unhydrolyzable ATP analogue, was less effective than ATP or ADP. AMP had no protective effect on the digestion of myosin and GTP inhibited slightly the digestion. When the papain-insensitive myosin in 0.15 M NaCl and 2.5 mM MgATP was phosphorylated by Ca2+/calmodulin-dependent myosin light-chain kinase, the myosin restored the vulnerability to papain. However, the two papain-susceptible forms, nonphosphorylated form in the absence of MgATP and phosphorylated form in the presence of MgATP, yielded very similar but distinct proteolytic fragments upon the digestion. When the extent of myosin assembly was estimated by the turbidimetry of myosin suspension in 0.15 M NaCl, nonphosphorylated myosin in the absence and presence of MgATP was assembled and disassembled, respectively, and phosphorylated myosin in the presence of MgATP was assembled. These results suggest that, at physiological ionic strength, papain as a probe distinguishes disassembled myosin and assembled myosin as papain-insensitive and papain-sensitive forms, respectively.     

Reversibility of the low-salt transition of chromatin core particles.

The low-salt transition of chromatin core particles is reversible if the monovalent cation concentration is kept above 0.2 mM. Exposure of the particles to salt concentrations below this value results in a nonreversible secondary transition. The nonreversible changes are relatively slow with a half-time of about 15 minutes. Once exposed to such low ionic strength, the particles then begin to refold with increasing salt in at least two steps over a much higher ionic strength range than is required for the usual low-salt transition. The refolding is very fast, with a half-time less than a minute. Small differences between particles which had or had not been exposed to very low salt persist even when the particles are returned to near physiological ionic strengths.