Optical anisotropy of chromatin. Flow linear dichroism and electric dichroism studies

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentrations by the use of flow linear dichroism (LD) and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA - 2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA - for chromatins with the linker DNA of 10-30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin. Presented results explain the contradictory data obtained by electrooptical and hydrooptical methods.     

Linear dichroism of chromatin fibers

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Friend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations by the use of flow linear dichroism and electric dichroism. We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA--2 mM NaCl and close positive values in the range of 2-100 mM NaCl. Mg2+ cations, in contrast to Na+ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5-10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers. The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA--for chromatins with linker DNA 10-30 b.p. it is partially reversible, while for preparations with longer linker DNA it is irreversible. Relatively low electric fields do not have an effect on chromatin structure, while higher electric fields (more than 7 kV/cm) distort the structure of chromatin.     

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.     

Optical Anisotropy of Chromatin. Flow Linear Dichroism and Electric Dichroism Studies

Abstract

The optical anisotropy of chromatin with different length of the linker DNA isolated from a variety of sources (Frend erythroleukemia cells, calf thymus, hen erythrocytes and sea urchin sperm) has been studied in a large range of mono- and bivalent cations concentraitons by the use of flow linear dichroism (LD) and electric dichroism.

We have found that all chromatins studied displayed negative LD values in the range of 0.25 mM EDTA—2 mM NaCl and close positive values in the range of 2–100 mM NaCl. Mg²⁺ cations, in contrast to Na⁺ cations, induce optically isotropic chromatin fibers. All chromatin samples exhibit positive form effect amounting to 5–10% of LD amplitude observed at 260 nm. This form effect is determined by the anisotropic scattering of polarized light by single chromatin fibers.

The conformational transition at 2 mM NaCl leads to the distortion of chromatin filament structure. The reversibility of this distortion depends on the length of the linker DNA—for chromatins with the linker DNA of 10–30 b.p. it is parially reversible, while for preparations with longer linker DNA it is irreversible.

Relatively low electric field does not affect chromatin structure, while higher electric field (more than 7 kV/cm) distorts the structure of chromatin.

Presented resutls explain the contradictory data obtained by electrooptical and hydrooptical methods.     

The mechanism of nucleosome assembly onto oligomers of the sea urchin 5 S DNA positioning sequence

We have used a model system composed of tandem repeats of Lytechinus variegatus 5 S rDNA (Simpson, R. T., Thoma, F., and Brubaker, J. M. (1985) Cell 42, 799-808) reconstituted into chromatin with chicken erythrocyte core histones to investigate the mechanism of chromatin assembly. Nucleosomes are assembled onto the DNA template by mixing histone octamers and DNA in 2 M NaCl followed by stepwise dialysis into very low ionic strength buffer over a 24-h period. By 1.0 M NaCl, a defined intermediate composed of arrays of H3.H4 tetramers has formed, as shown by analytical and preparative ultracentrifugation. Digestion with methidium propyl EDTA.Fe(II) indicates that these tetramers are spaced at 207 base pair intervals, i.e. one/repeat length of the DNA positioning sequence. In 0.8 M NaCl, some H2A.H2B has become associated with the H3.H4 tetramers and DNA. Surprisingly, under these conditions DNA is protected from methidium propyl EDTA.Fe(II) digestion almost as well as in the complete nucleosome, even though these structures are quite deficient in H2A.H2B. By 0.6 M NaCl, nucleosome assembly is complete, and the MPE digestion pattern is indistinguishable from that observed for oligonucleosomes at very low ionic strength. Below 0.6 M NaCl, the oligonucleosomes are involved in various salt-dependent conformational equilibria: at approximately 0.6 M, a 15% reduction in S20,w that mimics a conformational change observed previously with nucleosome core particles; at and above 0.1 M, folding into a more compact structure(s); at and above 0.1 M NaCl, a reaction involving varying amounts of dissociation of histone octamers from a small fraction of the DNA templates. In low ionic strength buffer (less than 1 mM NaCl), oligonucleosomes are present as fully loaded templates in the extended beads-on-a-string structure.     

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.     

Comparative study of nucleosome particles in chromatin from normal and tumor cells. II. Reconstitution, compaction and association induced by ionic strength of a solution

The method of circular dichroism (CD) has been used to investigate the reconstitution of mononucleosomes from C3HA mice liver and ascitic hepatoma 22A cells chromatin. It has been revealed that the more unfolding state of DNA in ascitic nucleosomes (discovered earlier) is determined by the peculiarities of the interactions between DNA and the dimers H2A-H2B, as well as by the linker histones of the H1 group. The investigation of the DNA folding in the oligonucleosome chains with increasing ionic strength has shown complete invariability of the DNA compactness in the ascitic chromatin up to 100 mM NaCl, while in liver nucleosomes an additional folding of the linker portion of the DNA was observed within the range of 20-40 mM NaCl. Oligonucleosomes from ascitic chromatin are less inclined to association upon increasing ionic strength, as compared with those from liver chromatin.     

Conformation of the HMG17-nucleosome complex

The nucleosome core binds more than two molecules of HMG17 at low ionic strength (8.9 mM Tris-HCl/8.9 mM boric acid/0.25 mM Na2EDTA, pH 8.3). Circular dichroism of the complexes showed only minor conformational changes of the nucleosome core DNA on binding of HMG17, with no detectable change in the histone secondary structure. The fluorescence of N-(3-pyrene) maleimide bound to -SH groups at Cys-110 of H3 histones in the core particle suggested that the structure of the histone octamer assembly changed little upon binding of HMG17 to the nucleosome. These observations support the idea that even a high level of HMG17 binding, e.g., four HMGs per nucleosome, alone, does not open up the core particle.     

Chromatin structure studied by linear dichroism at different salt concentrations

We have studied the linear dichroism (LD) of rat liver chromatin oriented by flow. Soluble chromatin, prepared by brief nuclease digestion, is found to exhibit a positive LD at low ionic strength (1 mM NaCl), with a constant LD/A over the absorption band centered at 260 nm (A, isotropic absorbance). Several previous dichroism studies on soluble chromatin have been performed on sonicated materials and have given negative LD, probably due to the presence of uncoiled DNA. The positive dichroism can be interpreted in terms of a supercoil of DNA in chromatin with a pitch angle larger than 55°, and is, for example, consistent with a model where the cylindrical nucleosome core particles are stacked face to face in the chromatin filament. In contrast to the nuclease-digested chromatin, sonicated chromatin was confirmed to exhibit negative LD. This difference can be attributed to a partial uncoiling of the linker regions between the nucleosomes due to the shearing. The structural transition of chromatin to a compact form can be observed as a reduction of the positive LD of the nuclease-digested chromatin to almost zero in 0.1 M NaCl or in 0.1 mM MgCl₂. This transition is due to a decreased electrostatic repulsion between negative phosphate groups on the DNA chain. In the case of Na⁺, this can be explained as a screening effect due to the bulk concentration of Na⁺. With Mg²⁺ a considerably stronger effect may indicate a more localized binding to the phosphates. At ionic strengths higher than 0.5M NaCl, the dissociation of the histones from DNA leads to uncoiling of chromatin. The change in LD during this process shows that histone H1 contributes only to a small degree to the coiling of the DNA chain, whereas histones H3 and H4 play the major role in the coiling.     

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.     

Exchange of H1 histone depends on aggregation of chromatin, not simply on ionic strength

Chromatin solubility was observed at several concentrations of various cations. Spermine and spermidine precipitated (50%) chromatin at about 0.2 mM, Ca2+ and Mg2+ at about 1-2 mM, and Na+ at about 100 mM. Further increases in cation concentration induced more aggregation, but eventually excess cation increased chromatin solubility so that 50% solubility was observed again at 60 mM Mg2+ and 180 mM Na+. H1 histone was 50% released by 80 mM MgCl2 or 425 mM NaCl. Combinations of MgCl2 and NaCl showed that Mg2+ and Na+ are synergistic in the induction of aggregation in lower concentrations (less than 2 mM) of Mg2+ but antagonistic at higher concentrations, and a similar effect of NaCl on spermidine-induced precipitation was shown below and above about 0.2 mM spermidine. At 5 mM, MgCl2 proved capable of precipitating chromatin depleted of H1 histone, but no concentration of NaCl was capable of doing so. These phenomena can be rationalized by supposing that neutralization of chromatin by any cation (including H1 histone) favors aggregation and also that cross-linking of chromatin fibers by multivalent cations (including H1 histone) is also critically important. The exchange of H1 histone between chromatin fragments was tested in various concentrations of different salts. H1 exchange was correlated with chromatin aggregation rather than with ionic strength and thus appears to depend on fiber to fiber contact. Under conditions where H1 exchanges between chromatin fibers that are permitted to make contact with each other, no H1 exchange occurred between chromatin inside the nucleus and chromatin outside, even though H1 histone is capable of passage through the nuclear membrane.     

Structure of histone octamers in reconstituted polynucleosomes

The salt-dependent structural changes of the histone octamer in complex with high-molecular-weight DNA have been studied by fluorescent spectroscopy. Changes in both the spectra maximum position and anisotropy of the histone tyrosine fluorescence reveal structural transitions in nucleosome within the ranges of 0.5-3 mM and 20-30 mM NaCl. Comparison of the octamer fluorescent parameters in complex with DNA as well as in a free state permits to interpret the revealed structural transitions as a change in degree of contacts stability between (H2A-H2B) dimer and (H3-H4)2 tetramer. More pronounced conformational changes in histone octamer are observed under the conditions of polynucleosome fibers interaction within the range of physiological ionic strength (100-600 mM NaCl). As far as fluorescent parameters are concerned, the aforementioned changes are connected with entire destruction of (H2A-H2B) dimer specific contacts with (H3-H4)2 tetramer. The obtained results suggest the possibility of existence of different structural states of histone octamer in the chromatin composition including those which are quite dissimilar from the octamer structure in the 2M NaCl solution.     

Salt-dependent compaction of di- and trinucleosomes studied by small-angle neutron scattering

Using small-angle neutron scattering (SANS), we have measured the salt-dependent static structure factor of di- and trinucleosomes from chicken erythrocytes and from COS-7 cells. We also determined the sedimentation coefficients of these dinucleosomes and dinucleosomes reconstituted on a 416-bp DNA containing two nucleosome positioning sequences of the 5S rDNA of Lytechinus variegatus at low and high salt concentrations. The internucleosomal distance d was calculated by simulation as well as Fourier back-transformation of the SANS curves and by hydrodynamic simulation of sedimentation coefficients. Nucleosome dimers from chicken erythrocyte chromatin show a decrease in d from approximately 220 A at 5 mM NaCl to 150 A at 100 mM NaCl. For dinucleosomes from COS-7 chromatin, d decreases from 180 A at 5 mM to 140 A at 100 mM NaCl concentration. Our measurements on trinucleosomes are compatible with a compaction through two different mechanisms, depending on the salt concentration. Between 0 and 20 mM NaCl, the internucleosomal distance between adjacent nucleosomes remains constant, whereas the angle of the DNA strands entering and leaving the central nucleosome decreases. Above 20 mM NaCl, the adjacent nucleosomes approach each other, similar to the compaction of dinucleosomes. The internucleosomal distance of 140-150 A at 100 mM NaCl is in agreement with distances measured by scanning force microscopy and electron microscopy on long chromatin filaments.     

Involvement of histone H1 in the organization of the nucleosome and of the salt-dependent superstructures of chromatin

We describe the results of a systematic study, using electron microscopy, of the effects of ionic strength on the morphology of chromatin and of H1-depleted chromatin. With increasing ionic strength, chromatin folds up progressively from a filament of nucleosomes at approximately 1 mM monovalent salt through some intermediate higher- order helical structures (Thoma, F., and T. Koller, 1977, Cell 12:101- 107) with a fairly constant pitch but increasing numbers of nucleosomes per turn, until finally at 60 mM (or else in approximately 0.3 mM Mg++) a thick fiber of 250 A diameter is formed, corresponding to a structurally well-organized but not perfectly regular superhelix or solenoid of pitch approximately 110 A as described by Finch and Klug (1976, Proc. Natl. Acad. Sci. U.S.A. 73:1897-1901). The numbers of nucleosomes per turn of the helical structures agree well with those which can be calculated from the light-scattering data of Campbell et al. (1978, Nucleic Acids Res. 5:1571-1580). H1-depleted chromatin also condenses with increasing ionic strength but not so densely as chromatin and not into a definite structure with a well-defined fiber direction. At very low ionic strengths, nucleosomes are present in chromatin but not in H1-depleted chromatin which has the form of an unravelled filament. At somewhat higher ionic strengths (greater than 5 mM triethanolamine chloride), nucleosomes are visible in both types of specimen but the fine details are different. In chromatin containing H1, the DNA enters and leaves the nucleosome on the same side but in chromatin depleted of H1 the entrance and exit points are much more random and more or less on opposite sides of the nucleosome. We conclude that H1 stabilizes the nucleosome and is located in the region of the exit and entry points of the DNA. This result is correlated with biochemical and x-ray crystallographic results on the internal structure of the nucleosome core to give a picture of a nucleosome in which H1 is bound to the unique region on a complete two-turn, 166 base pair particle (Fig. 15). In the formation of higher-order structures, these regions on neighboring nucleosomes come closer together so that an H1 polymer may be formed in the center of the superhelical structures.     

Histone-histone interaction mediates chromatin unfolding at physiological ionic strength

High-resolution thermal denaturation data on chicken erythrocyte chromatin are reported over 4 orders of magnitude in NaCl concentration which includes the physiological region. A novel technique using critical-point polyacrylamide sols instead of ordinary solvents effectively stabilizes chromatin against precipitation at high salt concentrations. These sols are optically transparent from 260 to 320 nm and are thermally stable over the temperature ranges studied. At Na+ ion concentrations below 10 mM, the polyacrylamide slightly destabilizes chromatin at the nucleosome level, possibly through interactions of histones H1 and H5 with the carboxylic acid residues. At the same low salts, polyacrylamide stabilizes pure DNA against denaturation, presumably by mechanically stabilizing it against helix-distorting thermal fluctuations. In both cases, however, the polyacrylamide sols are entirely noninvasive at higher salts. Prominent low-temperature thermal transitions are observed in chromatin at and above 100 mM NaCl which evidently are associated with conformational changes in DNA. Our results are in accord with the idea that histone-histone interactions at physiological ionic strengths (approximately 100 mM Na+) may be comparable to histone-DNA interactions and hence may be sufficient to promote the destabilization of the DNA helix in chromatin under these conditions. The biological implications of this are discussed, and a possible model for the local decondensation of chromatin under physiological conditions is proposed.     

The effect of a high mobility group protein (HMG 17) on the structure of acetylated and control core HeLa cell chromatin

The effect of binding a high mobility group protein (HMG 17) on the stability and conformation of acetylated and control HeLa high molecular weight core chromatin (stripped of H1 and non-histone chromosomal proteins) was studied by circular dichroism and thermal-denaturation measurements. Previously it had been shown that conformational differences exist between native whole chromatin derived from butyrate-treated (acetylated) and control HeLa cells and that these conformational differences disappear by removing H1 and non-histone chromosomal proteins (Reczek, P.R., Weissman, D., Huvos, P.E. and Fasman, G.D. (1982) Biochemistry 21, 993–1002). The circular dichroism spectra and the thermal denaturation profiles of control and acetylated core chromatin were found to be similar. The circular dichroism properties of HMG 17 reconstituted highly acetylated and control core chromatin indicated the same alteration of chromatin structure at low ionic strength (1 mM sodium phosphate/0.25 mM EDTA, pH 7.0). The magnitudes of the decrease in ellipticity were proportional to the amount of HMG 17 bound and were found to be the same for both the acetylated and control core chromatin. Thermal denaturation profiles confirmed this change in structure induced by HMG 17 on control and highly acetylated core chromatin. The thermal denaturation profiles, which were resolved into three component transitions, exhibited a shifting of hyperchromicity from the lower melting transitions to the higher melting transitions, with a concomitant rise in T_m, on HMG 17 binding to both control and acetylated chromatin. The natures of the interactions of HMG 17 at higher ionic strength (50 mM NaCl/0.25 mM EDTA/1 mM sodium phosphate, pH 7.0) with acetylated and control core chromatin were slightly different, as measured by circular dichroism; however, a decrease in ellipticity was observed for both samples upon binding of HMG 17. These observations suggest that acetylation coupled with HMG 17 binding to core chromatin does not loosen chromatin structure. HMG 17 binding to control and acetylated core chromatin produces an overall stabilization and compaction of chromatin structure.