Unexpected binding motifs for subnucleosomal particles revealed by atomic force microscopy

The structure of individual nucleosomes organized within reconstituted 208-12 arrays at different levels of compaction was examined by tapping mode atomic force microscopy in air and liquid. Reconstitution at lower histone octamer to DNA weight ratios showed an extended beads-on-a-string morphology with less than the expected maximum of 12 nucleosome core particles per array, each particle located in the most favored positioning site. A correlation of the contour lengths of these arrays with the number of observed particles revealed two distinct populations of particles, one with approximately 50 nm of bound DNA and a second population with approximately 25 nm. The measured nucleosome center-to-center distances indicate that this approximately 25 nm is not necessarily symmetrically bound about the dyad axis, but can also correspond to DNA bound from either the entry or exit point of the particle to a location at or close to the dyad axis. An assessment of particle heights suggests that particles wrapping approximately 25 nm of DNA are most likely to be subnucleosomal particles, which lack either one or both H2A-H2B dimers. At a higher reconstitution ratio, folded compact arrays fully populated with 12 nucleosome core particles, were observed. Liquid measurements demonstrated dynamic movements of DNA loops protruding from these folded arrays.     

Conformation of reconstituted mononucleosomes and effect of linker histone H1 binding studied by scanning force microscopy

The conformation of mononucleosome complexes reconstituted with recombinant core histones on a 614-basepair-long DNA fragment containing the Xenopus borealis 5S rRNA nucleosome positioning sequence was studied by scanning/atomic force microscopy in the absence or presence of linker histone H1. Imaging without prior fixation was conducted with air-dried samples and with mononucleosomes that were injected directly into the scanning force microscopy fluid cell and visualized in buffer. From a quantitative analysis of approximately 1,700 complexes, the following results were obtained: i), In the absence of H1, a preferred location of the nucleosome at the X. borealis 5S rRNA sequence in the center of the DNA was detected. From the distribution of nucleosome positions, an energy difference of binding to the 5S rRNA sequence of DeltaDeltaG approximately 3 kcal mol(-1) as compared to a random sequence was estimated. Upon addition of H1, a significantly reduced preference of nucleosome binding to this sequence was observed. ii), The measured entry-exit angles of the DNA at the nucleosome in the absence of H1 showed two maxima at 81 +/- 29 degrees and 136 +/- 18 degrees (air-dried samples), and 78 +/- 25 degrees and 137 +/- 25 degrees (samples imaged in buffer solution). In the presence of H1, the species with the smaller entry-exit angle was stabilized, yielding average values of 88 +/- 34 degrees for complexes in air and 85 +/- 10 degrees in buffer solution. iii), The apparent contour length of the nucleosome complexes was shortened by 34 +/- 13 nm as compared to the free DNA due to wrapping of the DNA around the histone octamer complex. Considering an 11 nm diameter of the nucleosome core complex, this corresponds to a total of 145 +/- 34 basepairs that are wound around the nucleosome.     

1H NMR investigation of the conformational states of DNA in nucleosome core particles.

In this study 1H NMR has been used to investigate the conformational state of DNA in nucleosome core particles. The nucleosome core particles exhibit partially resolved low field (10-15 ppm) spectra due to imino protons in Watson-Crick base pairs (one resonance per GC or AT base pair). To a first approximation, the spectrum is virtually identical with that of protein-free 140 base pair DNA, and from this observation we draw two important conclusions: (i) Since the low field spectra of DNA are known to be sensitive to conformation, the conformation of DNA in the core particles is essentially the same as that of free DNA (presumably B-form), (ii) since kinks occurring at a frequency at 1 in 10 or 1 in 20 base pairs would result in a core particle spectrum different from that of free DNA we find no NMR evidence supporting either the Crick-Klug or the Sobell models for kinking DNA around the core histones. Linewidth considerations indicate that the rotational correlation time for the core particles is approximately 1.5 X 10(-7) sec, whereas the end-over-end tumbling time of the free 140 base pair DNA is 3 X 10(-7) sec.     

Hyperacetylation of core histones does not cause unfolding of nucleosomes. Neutron scatter data accords with disc shape of the nucleosome

Recent studies report that the frictional resistance of partially acetylated core particles increases when the number of acetyl groups/particle exceeds 10 (Bode, J., Gomez-Lira, M. M. & Schr?ter, H. (1983) Eur. J. Biochem. 130, 437-445). This was attributed to an opening of the core particle though other explanations, e.g. unwinding of the DNA ends were also suggested. Another possible explanation is that release of the core histone N-terminal domains by acetylation increased the frictional resistance of the particle. Neutron scatter studies have been performed on core particles acetylated to different levels up to 2.4 acetates/H4 molecule. Up to this level of acetylation the neutron scatter data show no evidence for unfolding of the core particle. The fundamental scatter functions for the envelope shape and internal structure are identical to those obtained previously for bulk core particles. The structure that gave the best fit to these fundamental scatter functions was a flat disc of diameter 11-11.5 nm and of thickness 5.5-6 nm with 1.7 +/- 0.2 turns of DNA coiled with a pitch of 3.0 nm around a core of the histone octamer. The data analysis emphasizes the changes in pair distance distribution functions at relatively low contrasts, particularly when the protein is contrast matched and DNA dominates the scatter. Under these conditions there is no evidence for the unwinding of long DNA ends in the hyperacetylated core particles. The distance distribution functions go to zero between 11.5 and 12 nm which gives the maximum chord length in a particle of dimension, 11 nm X 5.5 nm. The distance distribution function for the histone octamer contains 85% of the vectors within the 7.0-nm diameter of the histone core. 15% of the histone vectors lie between 7.0 and 12.0 nm, and these are attributed to the N-terminal domains of the core histones which extend out from the central histone core. Histone vectors extending beyond 7.0 nm are necessary to account for the measured radius of gyration of the histone core of 3.3 nm. A similar value of 3.2 nm is calculated for the recent ellipsoidal shape of 11.0 X 6.5 X 6.5 nm from the crystal structure of the octamer. However, the nucleosome model based on this structure is globular, roughly 11 nm in diameter, which does not accord with the flat disc shape core particle obtained from detailed neutron scatter data nor with the cross-section radii of gyration of the histone and DNA found previously for extended chromatin in solution.     

Computer simulation of the 30-nanometer chromatin fiber

A new Monte Carlo model for the structure of chromatin is presented here. Based on our previous work on superhelical DNA and polynucleosomes, it reintegrates aspects of the "solenoid" and the "zig-zag" models. The DNA is modeled as a flexible elastic polymer chain, consisting of segments connected by elastic bending, torsional, and stretching springs. The electrostatic interaction between the DNA segments is described by the Debye-Hückel approximation. Nucleosome core particles are represented by oblate ellipsoids; their interaction potential has been parameterized by a comparison with data from liquid crystals of nucleosome solutions. DNA and chromatosomes are linked either at the surface of the chromatosome or through a rigid nucleosome stem. Equilibrium ensembles of 100-nucleosome chains at physiological ionic strength were generated by a Metropolis-Monte Carlo algorithm. For a DNA linked at the nucleosome stem and a nucleosome repeat of 200 bp, the simulated fiber diameter of 32 nm and the mass density of 6.1 nucleosomes per 11 nm fiber length are in excellent agreement with experimental values from the literature. The experimental value of the inclination of DNA and nucleosomes to the fiber axis could also be reproduced. Whereas the linker DNA connects chromatosomes on opposite sides of the fiber, the overall packing of the nucleosomes leads to a helical aspect of the structure. The persistence length of the simulated fibers is 265 nm. For more random fibers where the tilt angles between two nucleosomes are chosen according to a Gaussian distribution along the fiber, the persistence length decreases to 30 nm with increasing width of the distribution, whereas the other observable parameters such as the mass density remain unchanged. Polynucleosomes with repeat lengths of 212 bp also form fibers with the expected experimental properties. Systems with larger repeat length form fibers, but the mass density is significantly lower than the measured value. The theoretical characteristics of a fiber with a repeat length of 192 bp where DNA and nucleosomes are connected at the core particle are in agreement with the experimental values. Systems without a stem and a repeat length of 217 bp do not form fibers.     

Analysis of the effects of antibiotics on the structure of nucleosome core particles determined by DNAase I cleavage

Patterns of sensitivity to DNAase I cleavage have been analysed in order to investigate the effects of anti-tumour antibiotics and related drugs on nucleosome core particles containing different DNA restriction fragments. In this article, we review the experimental results which show that after controlled digestion of defined-sequence core particles, new cleavage products appear in the enzyme digestion patterns which lie approximately mid-way between the strong bands characteristic of native nucleosome core particles. The effects of the antibiotics, which include bis-intercalators as well as minor groove-binding ligands (but not monofunctional intercalators), are explained in terms of an induced change in rotational setting (phasing) of the core DNA. The new rotational positioning of DNA induced by antibiotic binding appears to be almost independent of DNA sequence, although some differences can be observed with the various pieces of DNA, most likely reflecting the exact number and disposition of antibiotic binding sites.     

Self-assembly of single and closely spaced nucleosome core particles.

Self-assembly of DNA with the four core histones but in the absence of H1 generates nucleosome core particles which are spaced randomly over large distances. Closely spaced core particles, however, exhibit a preferred short linkage which is not a multiple of 10 base pairs. They bind about 140 base pairs whereas apparently shorter DNA lengths per nucleosome observed after digestion with micrococcal nuclease are the result of degradation from the ends. The DNA length of one superhelical turn in the core particle is 83 +/- 4 base pairs. Single core particles may bind more DNA than closely spaced core particles but probably less than two full turns of 168 base pairs. The internal structures of single and of native core particles are very similar as judged by their amount of DNA, sedimentation coefficient, appearance in the electron microscope, and digestion with DNase I. In addition to core particles, a particle is described which sediments at 9 S and consists of 108 base pairs of DNA bound to the histone octamer. It appears to be the smallest stable "core particle" but it is not a degradation product of the 146-base-pair core particle. Digestion of end-labeled 9 S and nucleosome core particles with DNase I shows distinct differences.     

Effect of HMG protein 17 on the thermal stability of control and acetylated HeLa oligonucleosomes.

Many studies have implicated histone acetylation and HMG proteins 14 and 17 in the structure of active chromatin. Studies of the binding of HMG 14 and 17 to chromatin core particles have shown that there are two binding sites for HMG 14 or 17 located within 20-25 bp of the DNA ends of the core particles [13-15]. Such binding sites may result from the free DNA ends in the core particle being available for the binding of HMG 14 and 17. We have studied the effects of the binding of HMG 17 on the thermal denaturation of DNA in mono, di and trinucleosomes. In each case the binding of 1 HMG 17 molecule per nucleosome reduces the DNA premelt region by 50%, while the binding of 2 HMG 17 molecules per nucleosome abolishes the premelt region. From this it is concluded that there are two HMG 17 binding sites per nucleosome which are located between the entry and exit points to the nucleosome and the strongly complexed central DNA region. Highly acetylated mono, di and trinucleosomes have been isolated from butyrate treated HeLa S3 cells. For this series of acetylated oligonucleosomes, it has been found that there are also two HMG 17 binding sites per acetylated nucleosome.     

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.     

The structure of nucleosome core particles as revealed by difference Raman spectroscopy.

Raman spectra have been observed of nucleosome core particles (I) prepared from chicken erythrocyte chromatin, its isolated 146 bp DNA (II), and its isolated histone octamer (H2A+H2B+H3+H4)2 (III). By examining the difference Raman spectra, (I)-(II), (I)-(III), and (I)-(II)-(III), several pieces of information have been obtained on the conformation of the DNA moiety, the conformation of the histone moiety, and the DNA-histone interaction in the nucleosome core particles. In the nucleosome core particles, about 15 bp (A.T rich) portions of the whole 146 bp DNA are considered to take an A-form conformation. These are considered to correspond to its bent portions which appear at intervals of 10 bp.     

DNA base excision repair of uracil residues in reconstituted nucleosome core particles

The human base excision repair machinery must locate and repair DNA base damage present in chromatin, of which the nucleosome core particle is the basic repeating unit. Here, we have utilized fragments of the Lytechinus variegatus 5S rRNA gene containing site-specific U:A base pairs to investigate the base excision repair pathway in reconstituted nucleosome core particles in vitro. The human uracil-DNA glycosylases, UNG2 and SMUG1, were able to remove uracil from nucleosomes. Efficiency of uracil excision from nucleosomes was reduced 3- to 9-fold when compared with naked DNA, and was essentially uniform along the length of the DNA substrate irrespective of rotational position on the core particle. Furthermore, we demonstrate that the excision repair pathway of an abasic site can be reconstituted on core particles using the known repair enzymes, AP-endonuclease 1, DNA polymerase beta and DNA ligase III. Thus, base excision repair can proceed in nucleosome core particles in vitro, but the repair efficiency is limited by the reduced activity of the uracil-DNA glycosylases and DNA polymerase beta on nucleosome cores.     

DNA repair within nucleosome cores of UV-irradiated human cells

We have compared the distributions of repair synthesis and pyrimidine dimers (PD) in nucleosome core DNA during the early (fast) repair phase and the late (slow) repair phase of UV-irradiated human fibroblasts. As shown previously [Lan, S. Y., & Smerdon, M. J. (1985) Biochemistry 24, 7771-7783], repair synthesis is nonuniform in nucleosome core particles during the fast repair phase, and the distribution curve can be approximated by a model where repair synthesis occurs preferentially in the 5' and 3' end regions. In this report, we show that, during the slow repair phase, [3H]dThd-labeled repair patches are much more uniformly distributed in core DNA, although they appear to be preferentially located in sequences degraded slowly by exonuclease III. This change in distribution cannot be explained by an increase in patch size during slow repair, since the size of these patches actually decreases to about half the size measured during the fast repair phase. Furthermore, PD mapping within core DNA at the single-nucleotide level demonstrated that, at least within the 30-130-base region from the 5' end, there is little (or no) selective removal of PD during the fast repair phase. However, the nonuniform distribution of repair synthesis obtained during fast repair throughout most of the core DNA region (approximately 40-146 bases) is accounted for by the nonuniform distribution of PD in core DNA. The near-uniform distribution of repair synthesis observed during slow repair may result from more extensive nucleosome rearrangement and/or nucleosome modification during this phase.     

Novel nucleosomal particles containing core histones and linker DNA but no histone H1

Eukaryotic chromosomal DNA is assembled into regularly spaced nucleosomes, which play a central role in gene regulation by determining accessibility of control regions. The nucleosome contains ∼147 bp of DNA wrapped ∼1.7 times around a central core histone octamer. The linker histone, H1, binds both to the nucleosome, sealing the DNA coils, and to the linker DNA between nucleosomes, directing chromatin folding. Micrococcal nuclease (MNase) digests the linker to yield the chromatosome, containing H1 and ∼160 bp, and then converts it to a core particle, containing ∼147 bp and no H1. Sequencing of nucleosomal DNA obtained after MNase digestion (MNase-seq) generates genome-wide nucleosome maps that are important for understanding gene regulation. We present an improved MNase-seq method involving simultaneous digestion with exonuclease III, which removes linker DNA. Remarkably, we discovered two novel intermediate particles containing 154 or 161 bp, corresponding to 7 bp protruding from one or both sides of the nucleosome core. These particles are detected in yeast lacking H1 and in H1-depleted mouse chromatin. They can be reconstituted in vitro using purified core histones and DNA. We propose that these ‘proto-chromatosomes’ are fundamental chromatin subunits, which include the H1 binding site and influence nucleosome spacing independently of H1.     

Effect of DNA length and H4 acetylation on the thermal stability of reconstituted nucleosome particles

To examine the factors involved with nucleosome stability, we reconstituted nonacetylated particles containing various lengths (192, 162, and 152 base pairs) of DNA onto the Lytechinus variegatus nucleosome positioning sequence in the absence of linker histone. We characterized the particles and examined their thermal stability. DNA of less than chromatosome length (168 base pairs) produces particles with altered denaturation profiles, possibly caused by histone rearrangement in those core-like particles. We also examined the effects of tetra-acetylation of histone H4 on the thermal stability of reconstituted nucleosome particles. Tetra-acetylation of H4 reduces the nucleosome thermal stability by 0.8 degrees C as compared with nonacetylated particles. This difference is close to values published comparing bulk nonacetylated nucleosomes and core particles to ones enriched for core histone acetylation, suggesting that H4 acetylation has a dominant effect on nucleosome particle energetics.     

Neutron-scattering studies of accurately reconstituted nucleosome core particles and the effect of ionic strength on core particle structure

Chicken erythrocyte nucleosome core particles can be dissociated quantitatively into histones (H3, H4)2 bound to 146 base pairs of DNA, and 2(H2A, H2B). Reconstitution of core particles from the two components produces an 85% yield of particles which neutron scattering studies show to be accurate stoichiometrically and indistinguishable from native core particles: the radii of gyration of the shape, the protein components and the DNA components of the particles are 4.02 nm, 3.3 nm and 4.95 nm respectively. The largest distance and most probable distance which can be drawn in the particles are 11.5 nm and 4.3 nm respectively. The molecular weight of the particles is identical to that of control 'native' core particles. All of these values, within limits of error, are the same as known values for 'native' core particles. These experiments confirm the essential role of histones H3 and H4 in the initial organisation of core-particle structure, make possible the manufacture of perfectly pure and homogeneous core-particle preparations and allow the 100% incorporation of labelled or modified histones. Neutron scattering studies of core particles at high contrast (in D2O and H2O) have been carried out over a range of ionic strengths and pH. No change in structure is detected down to pH 5.5 in 20 mM NaCl or down to ionic strength 2.0 mM at pH 7.     

X-ray scattering study of the shape of the DNA region in nucleosome core particle with synchrotron radiation.

The structure of the DNA region in rat thymus nucleosome core particle has been studied by synchrotron X-ray scattering analysis and the contrast-variation technique has been applied to determine the contribution of the DNA to the total scatterings. Small-angle contrast-matching measurements show that the entire core particle and isolated histone octamers are contrast-matched by solvents containing 64 and 54% (w/w) sucrose, respectively. At a contrast of 54% sucrose, where the scattering of the DNA dominates, the scattering data extending to higher angle of about 0.05 A-1 have been collected from relatively concentrated solutions (10 mg/ml) of core particles and interpreted on the basis of the regular helical model for the DNA region. The model calculations show that the shape of the DNA around the histone core is approximately by 1.8 turns of regular helix of 42 A radius and 28 A pitch. These values for helical parameters of our model are in good agreement with those of the structure of DNA in crystallized nucleosome cores shown by earlier diffraction studies.     

Factors affecting nucleosome disassembly by protamines in vitro. Histone hyperacetylation and chromatin structure, time dependence, and the size of the sperm nuclear proteins

Histone displaced in vitro from nuclei by protamine competition display a higher degree of hyperacetylation than the residual histones. In addition, hyperacetylated core particle pools are disassembled in vitro with a higher efficiency than control or nonacetylated core particles and when analyzed by electron microscopy display an elongated shape (length/width ratio = 1.52 +/- 0.19) instead of the round compact shape of control nucleosomes (length/width ratio = 1.06 +/- 0.06). In the absence of histone hyperacetylation, the fish protamines, salmine and iridine (32-33 residues), are relatively inefficient in disassembling nucleosomal core particles in vitro as compared to the large (65-70 residues), tyrosine-containing protamines from rooster (galline), squid, and cuttlefish which disassemble nucleosomes in a range of protamine concentrations close to physiological. The fact that an artificially cross-linked salmine dimer acquires the ability of the large protamines from rooster, squid, and cuttlefish to disassemble core particles in vitro and also binds more tightly to the DNA, suggests that the size of the sperm nuclear protamines is a critical factor in this process. Even when the core histones of spermatid chromatin are hyperacetylated in the trout testis, the replacement process by iridine or salmine is slow and time-dependent in vitro. However, since spermiogenesis in trout occurs over several weeks, the slow in vitro nucleosome disassembly process by salmine is sufficient to allow complete displacement, thus supporting the hypothesis that a protamine-mediated displacement of the histones from DNA in vivo may take place in the salmonid fishes by a mechanism similar to that in the rooster, squid, and cuttlefish.     

The interaction of high mobility proteins HMG14 and 17 with nucleosomes.

The interaction of the high mobility group proteins, HMG14 and HMG17, with nucleosome core particles has been studied. The results show that two molecules of HMG14/17 can be bound tightly but reversibly to each core particle and that their affinity for core particles is greater than their affinity for histone-free DNA of core size. Thermal denaturation and nuclease digestion studies suggest that major sites of interaction are located near the ends of the nucleosome core DNA. When nucleosome preparations from chicken erythrocyte nuclei stripped of HMG proteins are partially titrated with HMG14/17, the nucleosome-HMG complex fraction is enriched in beta-globin gene sequences.