Labelling of histone H5 and its interaction with DNA. 2. Cooperative binding of histone H5 to DNA as probed by steady-state fluorescence and diffusion-enhanced energy transfer

The interaction of histone H5 labelled with fluorescein isothiocyanate (FITC) with DNA has been studied by fluorescence titration, and diffusion-enhanced fluorescence energy transfer (DEFET) measurements with Tb(III) lanthanide chelates as donors. Analysis of the binding data by the model of Schwarz and Watanabe (J.Mol.Biol. 163, 467-484 (1983)) yielded a mean stoichiometry of 60 nucleotides per H5 molecule, independently of ionic strength, in the range of 3 to 300 mM NaCl, at very low DNA concentration (6 microM in mononucleotide). It ensues an approximate electroneutrality of the saturated complexes. Histone H5 molecules appeared to be clustered along the DNA lattice in clusters containing on average 3 to 4 H5 molecules separated by about 79 base pairs, at mid-saturation of the binding sites. The interaction process was found highly cooperative but the cooperativity parameter was also insensitive to ionic strength in the above range. DEFET experiments indicated an important decrease of accessibility of the FITC label to the TbHED3A and TbEDTA- chelates with ionic strength in the 0 to 100 mM NaCl range. In the presence of DNA, H5 appears already folded at low ionic strength so that the FITC probe is also not accessible to the donor chelate. The present study constitutes an indispensable preliminary step to further studies on the localization of histone H5 in condensed chromatin structures.     

Conformations of the core nucleosome: effects of ionic strength and high mobility group protein 14 and 17 binding on the fluorescence emission and polarization of dansylated methionine-84 of histone H4

Chicken histone H4 labeled at Met-84 with the fluor N-[(acetylamino)ethyl]-8-naphthyl-amine-1-sulfonic acid has been incorporated into a nucleosome which has physical characteristics virtually identical with those of native core nucleosomes. The fluorescence emission and polarization properties of the labeled nucleosome were measured as a function of ionic strength and the binding of high mobility group (HMG) proteins 14 and 17. Also, the accessibility of the fluor to the quenching agent acrylamide was determined. It was found that the fluorescence emission changes in the range 0.1-1000 mM NaCl are rather small and indicate that no major unfolding of the octamer structure occurs around Met-84 on H4 at least. Five or perhaps six discrete states were found in that ionic strength range. Each has a different accessibility to the quenching agent. The range of accessibilities varied from 9 X 10(-7) to 32 X 10(-7) mol-1 s-1 for 0.1-1000 mM NaCl, respectively. Polarization measurements showed that there was little change in the rotational relaxation lifetime of the fluor at ionic strengths less than 50 mM NaCl. Above this value, the rotational relaxation lifetimes decreased from 107 to 25 ns at 600 mM NaCl, indicating a moderately increased rotational freedom for the fluor. It is suggested that the histone octamer changes its degree of compaction in the range 0.1-600 mM NaCl but that no major protein unfolding occurs.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Thermal denaturation and fluorescence study of nucleosomes containing non-histone chromosomal protein HMG2

Interaction of calf thymus non-histone chromosomal protein HMG2 with H1,H5-depleted nucleosomes from chicken erythrocytes was studied by means of thermal denaturation and an N-(3-pyrene)maleimide fluorescence probe. Under low ionic conditions (2 mM Tris buffer plus EDTA) addition of 1-2 molecules of HMG2 per nucleosome markedly stabilized the segment of the linker DNA against thermal denaturation. Under approximately physiological ionic conditions (0.1 M NaCl) addition of two HMG2 molecules per nucleosome, labeled by N-(3-pyrene)maleimide at the sulfhydryl groups of Cys-110 of histones H3, resulted in a decrease of the pyrene excimer fluorescence corresponding to the slight movement of the sulfhydryl groups of the two histone H3 molecules apart.     

Energetics and affinity of the histone octamer for defined DNA sequences

Previous studies have compared the relative free energies for histone octamer binding to various DNA sequences; however, no reports of the equilibrium binding affinity of the octamer for unique sequences have been presented. It has been shown that nucleosome core particles (NCPs) dissociate into free DNA and histone octamers (or free histones) on dilution without generation of stable intermediates. Dissociation is reversible, and an equilibrium distribution of NCPs and DNA is rapidly attained. Under low ionic strength conditions (<400 mM NaCl), NCP dissociation obeys the law of mass action, making it possible to calculate apparent equilibrium dissociation constants (K(d)s) for NCPs reconstituted on defined DNA sequences. We have used two DNA sequences that have previously served as model systems for nucleosome reconstitution studies, human alpha-satellite DNA and Lytechinus variegatus 5S DNA, and find that the octamer exhibits K(d)s of 0.03 and 0.06 nM, respectively, for these sequences at 50 mM NaCl. These DNAs form NCPs that are approximately 2 kcal/mol more stable than total NCPs isolated from cellular chromatin. As for mixed-sequence NCPs, increasing ionic strength or temperature promotes dissociation. van't Hoff plots of K(a)s versus temperature reveal that the difference in binding free energy for alpha-satellite and 5S NCPs compared to bulk NCPs is due almost entirely to a more favorable entropic component for NCPs formed on the unique sequences compared to mixed-sequence NCPs. Additionally, we address the contribution of the amino-terminal tail domains of histones H3 and H4 to octamer affinity through the use of recombinant tailless histones.     

Internal architecture of the core nucleosome: fluorescence energy transfer studies at methionine-84 of histone H4

Chicken histone H4, labeled separately at Met-84 with N-[[(iodoacetyl)amino]ethyl]-5-naphthylamine-1-sulfonic acid and 5-(iodoacetamido)fluorescein, was reassociated with unlabeled histones H2A, H2B, and H3 and 146 base pairs of DNA to produce fluorescently labeled nucleosomes having physical characteristics virtually the same as those of native core particles. Four types of particles were prepared containing respectively unlabeled H4, dansylated H4, fluoresceinated H4, and a mixture of the two labeled H4 molecules. Quantitative singlet-singlet energy-transfer measurements were carried out to determine changes in the distance between the two Met-84 H4 sites within the same nucleosome following conformational transitions which we have reported earlier. In the ionic strength range 0.1-100 mM NaCl, the distance between these sites is less than 2 nm except at 1 mM. Between 100 and 600 mM monovalent salt the distance separating the donor and acceptor fluors at Met-84 H4 increases to 3.8 nm. The conformational change centered around 200 mM NaCl is cooperative. Our results and those of others indicate that there is little unfolding of the histone octamer, at least around Met-84 H4, in the entire ionic strength range studied. A mechanism involving the rotation of the globular portion of H4 is proposed to account for this transition which occurs at physiological ionic strengths.     

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.     

Interactions of H1 and H5 histones with polynucleotides of B- and Z-DNA conformations

Interactions of chicken H1 and H5 histones with poly(dA-dT), poly(dG-dC), and the Z-DNA structure brominated poly(dG-dC) were measured by a nitrocellulose filter binding assay and circular dichroism. At low protein:DNA ratios, both H1 and H5 bound more Z-DNA than B-DNA, and binding of Z-DNA was less sensitive to interference by an increase in ionic strength (to 600 mM NaCl). H5 histone bound a higher percentage of all three polynucleotides than did H1 and caused more profound CD spectral changes as well. For spectral studies, histones and DNA were mixed in 2.0 M NaCl and dialyzed stepwise to low ionic strength. Prepared in this way or by direct mixing in 150 mM NaCl, complexes made with right-handed poly(dG-dC) showed a deeply negative psi spectrum (deeper with H5 than with H1). Complexes of histone and Br-poly(dG-dC) showed a reduction in the characteristic Z-DNA spectral features, with H5 again having a greater effect. Complexes of poly(dA-dT) and H5, prepared by mixing them at a protein:DNA ratio of 0.5, displayed a distinctive spectrum that was not achieved with H1 even at higher protein:DNA ratios. It included a new negative band at 287 nm and a large positive band at 255 nm, giving the appearance of an inverted spectrum relative to spectra of various forms of B-DNA. These findings may reflect an ability of the different lysine-rich histones to cause varying conformational changes in the condensation of chromatin in DNA regions of highly biased base sequence.     

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.     

Differences in the binding of H1 variants to DNA. Cooperativity and linker-length related distribution

A study of the complexes formed between short linear DNA and three H1 variants, a typical somatic H1, and the extreme variants H5, from chicken erythrocytes, and spH1 from sea urchin sperm, has revealed differences between H1, H5 and spH1 that have implications for chromatin structure and folding. 1. All three histones bind cooperatively to DNA in 35 mM NaCl forming similar, but not identical, rod-like complexes. With sufficiently long DNA the complexes may be circular, circles forming more easily with H5 and spH1 than with H1. 2. The binding of H5 and spH1 to DNA is cooperative even in 5 mM NaCl, resulting in well-defined thin filaments that appear to contain two DNA molecules bridged by histone molecules. In contrast, H1 binds distributively over all the DNA molecules in 5 mM NaCl, but forms short stretches similar in appearance to the thin filaments formed with H5 and spH1. Rods appear to arise from the intertwining of regular thin filaments containing cooperatively bound histone molecules on raising the NaCl concentration to 35 mM. 3. The compositions of the rods correspond to one histone molecule for about every 47 bp (H1), 81 bp (H5) and 112 bp (spH1), suggesting average spacings of 24 bp (H1), 41 bp (H5) and 56 bp (spH1) in the component thin (double) filaments. Strikingly, these values are proportional to the linker lengths of the chromatins in which the particular H1 variant is the main or sole H1.     

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.     

Effect of ionic strength of the medium on the structure and aggregation of histone H1 from the calf thymus

In the region of 50 mM NaCl histone HI has the structure with a great number of binding sites with fluorescent probe 1.8-ANS as compared to the structure formed in solution of 0.6-1.0 M NaCl. These sites, however, have a lower constant of binding with the probe and are characterized by a higher surrounding polarity. At local significant increase of the ionic strength histone HI molecules form stable oligomers having hydrophobic cavities. A conclusion is made about the importance of cationic envelope formed by N- and C-ends around the globular "head", for manifesting effective interactions between several molecules of histone HI.     

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.     

Self-assembled pearling structure of long duplex DNA with histone H1.

We report that complexes of giant DNA molecules with histone H1 proteins form a pearl necklace-like structure when the complexes are prepared by natural dilution from a high-salt solution (2 M NaCl) to a low-salt solution (0.2 M and 50 mM NaCl). We performed real-time observations on the conformational changes of individual T4 phage DNA (166 kb) molecules in bulk solution by fluorescence microscopy. To identify H1-binding regions on individual DNA molecules, we also performed immunofluorescence microscopic observations on the DNA-H1 complex spread on a glass surface. It was found that histone H1 binds DNA in a highly co-operative manner and is accompanied by local folding of the DNA. On the basis of the experimental observations and a theoretical simulation, we propose a self-assembling mechanism for the pearling structure.     

Physiologically relevant concentrations of NaCl and KCl increase DNA photocleavage by an N-substituted 9-aminomethylanthracene dye

This paper describes the synthesis of a new 9-aminomethylanthracene dye N-substituted with a pyridinylpolyamine side chain (4). The effects of NaCl and KCl on anthracene/DNA interactions were then studied, with the goal of simulating the conditions of high ionic strength that a DNA photosensitizer might encounter in the cell nucleus (~150 mM of NaCl and 260 mM of KCl). As exemplified by methylene blue (5), the expected effect of increasing ionic strength is to decrease DNA binding and photocleavage yields. In contrast, the addition of 150 mM of NaCl in combination with 260 mM of KCl to photocleavage reactions containing micromolar concentrations of 4 triggers the conversion of supercoiled, nicked, and linear forms of pUC19 plasmid into a highly degraded band of DNA fragments (350 nm hν, pH 7.0). Circular dichroism spectra point to a correlation between salt-induced unwinding of the DNA helix and the increase in DNA photocleavage yields. The results of circular dichroism, UV-vis absorption, fluorescence emission, thermal denaturation, and photocleavage inhibition experiments suggest that the combination of salts causes a change in the DNA binding mode of 4 from intercalation to an external interaction. This in turn leads to an increase in the anthracene-sensitized production of DNA-damaging reactive oxygen species.     

Differing accessibility in chromatin of the antigenic sites of regions 1-58 and 63-125 of histone H2B

Experiments with antibodies induced by separated fragments 1-58 and 63- 125 of H2B histone indicated that the 1-58 portion of the molecule is much more accessible in chromatin than is the 63-125 region. In immunoabsorption and immunoelectron microscopic assays with bovine and chicken chromatins, anti-1-58 antibodies reacted with sheared or unsheared chromatin both at low ionic strength (1 mM Tris-HCl) and in 0.14 M NaCl. Anti-63-125 antibodies were bound only weakly by chromatin at low ionic strength and not at all in 0.14 M NaCl. Antibodies to whole H2B showed intermediate reactivity with chromatin in both assays. In tests of immunofluorescence with unfixed calf liver nuclei in suspension, anti-1-58 caused nucleolar as well as nucleoplasmic fluorescence, whereas anti-63-125 did not lead to detectable fluorescence; anti-H2B showed intermediate staining intensity. In control experiments, anti-H1 antibody was bound by chromatin at low ionic strength but not in 0.14 M NaCl; anti-H3 antibody was bound poorly under either condition.     

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.     

Specific interaction of histone H1 with eukaryotic DNA.

The interaction of calf thymus histone H1 with homologous and heterologous DNA has been studied at different ionic strengths. It has been found that about 0.5 M NaCl histone H1, and its fragments N-H1 (residues 1-72) and C-H1 (residues 73-C terminal), precipitate selectively a small fraction of calf thymus DNA. This selective precipitation is preserved up to very high values (less than 2.0) of the input histone H1/DNA ratio. The percentage of DNA insolubilized by histone H1 under these ionic conditions is dependent upon the molecular weight of the nucleic acid, diminishing from 18% fro a Mw equals 1.0 x 10(7) daltons to 5% for a Mw equals 8.0 x 10(4) daltons. The base composition of the precipitated DNA is similar to that of the bulk DNA. Calf thymus histone H1 also selectively precipitates a fraction of DNA from other eukaryotes (herring, trout), but not from some prokaryotes (E. coli, phage gamma. On the other hand, at 0.5 M NaCl, the whole calf thymus DNA (but not E. coli DNA) presents a limited number of binding sites for histone H1, the saturation ratio histone H1 bound/total DNA being similar to that found in chromatin. A similar behavior is observed from the histone H1 fragments, N-H1 and C-H1, which bind to DNA in complementary saturation ratios. It is suggested that in eukaryotic organisms histone H1 molecules maintain specific interactions with certain DNA sequences. A fraction of such specific complexes could act as nucleation points for the high-order levels of chromatin organization.     

Thermodynamic analysis of monoclonal antibody binding to duplex DNA.

A technique based on fluorescence polarization (anisotropy) was used to measure the binding of antibodies to DNA under a variety of conditions. Fluorescein-labeled duplexes of 20 bp in length were employed as the standard because they are stable even at low ionic strength yet sufficiently short so that both arms of an IgG cannot bind to the same duplex. IgG Jel 274 binds duplexes in preference to single-stranded DNA; in 80 mM NaCl Kobs for (dG)20.(dC)20 is 4.1x10(7) M-1 compared with 6.4x10(5) M-1 for d(A5C10A5). There is little sequence specificity, but the interaction is very dependent on ionic strength. From plots of log Kobs against log[Na+] it was deduced that five or six ion pairs are involved in complex formation. At low ionic strength,Kobs is independent of temperature and complex formation is entropy driven with DeltaH degrees obs and DeltaC degrees p,obs both zero. In contrast, in 80 mM NaCl DeltaC degrees p,obs is -630 and -580 cal mol-1K-1 for [d(TG)]10.[d(CA)]10 and (dG)20.(dC)20 respectively. IgG Jel 241 also binds more tightly to duplexes than single-stranded DNA, but sequence preferences were apparent. The values for Kobs to [d(AT)]20 and [d(GC)]20 are 2.7x10(8) and 1.3x10(8) M-1 respectively compared with 5.7x10(6) M-1 for both (dA)20. (dT)20 and (dG)20.(dC)20. As with Jel 274, the binding of Jel 241 is very dependent on ionic strength and four or five ionic bonds are involved in complex formation with all the duplex DNAs which were tested. DeltaC degrees p,obs for Jel 241 binding to [d(AT)]20 was negative (-87 cal mol-1K-1) in 80 mM NaCl but was zero at high ionic strength (130 mM NaCl). Therefore, for duplex-specific DNA binding antibodies DeltaC degrees p,obs is dependent on [Na+] and a large negative value does not correlate with sequence-specific interactions.