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.     

A reexamination of the reported B----Z DNA transition in nucleosomes reconstituted with poly(dG-m5dC).poly(dG-m5dC)

Polynucleosomes with poly(dG-m5dC).poly(dG-m5dC) have been reconstituted, and well-defined nucleosome core particles from these have been prepared. Upon addition of MgCl2 to the levels used to induce the B to Z transition in this highly methylated DNA, significant changes in the circular dichroism spectrum are observed in solutions of these particles. However, such core particles also exhibit a noticeable instability when compared to chicken erythrocyte core particles under the same conditions. The change in circular dichroism can be entirely accounted for on the assumption that only free nucleotide, released by core particle dissociation, undergoes the B----Z transition. Therefore, no evidence has been found for "Z nucleosomes" in these solutions. In fact, the histone-DNA interaction in the nucelosome seems to partially inhibit the B to Z transition of the DNA. The analysis of our results is consistent with a model in which all of the DNA that remains bound to the histone octamer retains the B form.     

A nonuniform distribution of excision repair synthesis in nucleosome core DNA

We have investigated the distribution in nucleosome core DNA of nucleotides incorporated by excision repair synthesis occurring immediately after UV irradiation in human cells. We show that the differences previously observed for whole nuclei between the DNase I digestion profiles of repaired DNA (following its refolding into a nucleosome structure) and bulk DNA are obtained for isolated nucleosome core particles. Analysis of the differences obtained indicates that they could reflect a significant difference in the level of repair-incorporated nucleotides at different sites within the core DNA region. To test this possibility directly, we have used exonuclease III digestion of very homogeneous sized core particle DNA to "map" the distribution of repair synthesis in these regions. Our results indicate that in a significant fraction of the nucleosomes the 5' and 3' ends of the core DNA are markedly enhanced in repair-incorporated nucleotides relative to the central region of the core particle. A best fit analysis indicates that a good approximation of the data is obtained for a distribution where the core DNA is uniformly labeled from the 5' end to position 62 and from position 114 to the 3' end, with the 52-base central region being devoid of repair-incorporated nucleotides. This distribution accounts for all of the quantitative differences observed previously between repaired DNA and bulk DNA following the rapid phase of nucleosome rearrangement when it is assumed that linker DNA and the core DNA ends are repaired with equal efficiency and the nucleosome structure of newly repaired DNA is identical with that of bulk chromatin. Furthermore, the 52-base central region that is devoid of repair synthesis contains the lowest frequency cutting sites for DNase I in vitro, as well as the only "internal" locations where two (rather than one) histones interact with a 10-base segment of each DNA strand.     

DNA folding by histones: the kinetics of chromatin core particle reassembly and the interaction of nucleosomes with histones.

The kinetics of the chromatin core particle reassembly reaction in solution were quantitatively studied under conditions such that nucleohistone aggregation did not occur. Core particles, salt-jumped rapidly by dilution from 2.5 m-NaCl (in which DNA and histones do not interact) to 0.6 m-NaCl (in which core particles are nearly intact), reassemble in two distinct time ranges. Approximately 75% of the DNA refolds into core particle-like structures “instantaneously” as measured by several physical and chemical techniques with dead times in the seconds to minutes time range. The remaining DNA refolds with relaxation times ranging from 250 minutes at 0 °C to 80 minutes at 37 °C; this slow effect cannot be attributed to sample heterogeneity. The fraction of slowly refolding DNA and the slow relaxation time are independent of the core particle concentration. Transient intermediates present during the slow phase of refolding were identified as free DNA and core particle-like structures containing excess histone. Mixing experiments with DNA, histones, and core particles showed that core particle-histone interactions are responsible for the slow kinetics of DNA refolding. Upon treatment of reassembling core particles with the protein crosslinking reagent, dimethylsuberimidate, the slow phase of the reassembly reaction was arrested and a 13 S particle containing DNA and two octamers of histone was isolated. Consistent with the nature of this kinetic intermediate, it is shown that in 0.6 m-NaCl, core particles co-operatively bind at least one additional equivalent of histones with high affinity in the form of excess octamers. Also, core particles continue to adsorb considerably more histones with a weaker association constant of the order 10⁵m^?1 (in units of octamers) to a maximum value of 12 ± 2 equivalents (octamers) per core particle. The sedimentation coefficient increases with the two-thirds power of the molecular weight of the complex, as it would in the case of clustered spheres.A reassembly mechanism consistent with the data is presented, and other simple mechanisms are excluded. In the proposed mechanism, core particles reassemble very rapidly and compete effectively with DNA for histones such that approximately one-third of the particles initially formed are complexed with an excess octamer of histones, and 25% of the total DNA remains uncomplexed. The amount of this unusual reaction intermediate decays slowly to an equilibrium value of about 10%, thereby leaving 9% of the total DNA uncomplexed. Approximate values are calculated for the free energies, rate constants, and two of the activation energies which characterize this migrating octamer mechanism. This mechanism provides a means whereby histone octamers can be temporarily stripped off DNA at a modest free energy cost, approximately 2.6 kcal per nucleosome. Also, the properties of excess histone adsorption by chromatin and octamer migration suggest an efficient mechanism, consistent with observations by others, for nucleosome assembly in vivo during replication.     

Nucleosome core particle self-assembly kinetics and stability at physiological ionic strength

Micrococcal nuclease, DNase I, and trypsin have been employed to study the kinetics of core particle self-assembly by salt jump from 2.0 to 0.2 M NaCl. A few seconds after the initiation of the reassociation reaction, the bulk of core particle DNA becomes protected from digestion by micrococcal nuclease, whereas free DNA, under the same conditions, is completely hydrolyzed. The central and C-terminal regions of core histones are also protected from trypsin digestion immediately after the 2.0-0.2 M NaCl salt jump. Moreover, the extent of degradation produced by trypsin is the same for samples digested a few seconds after the salt jump and for samples digested 20 min after the salt jump. With DNase I, minor structural differences have been detected between samples obtained at different times during the reaction. However, even in this case our results indicate that many of the characteristic histone-DNA contacts within the core particle are made a few seconds after the initiation of the self-assembly reaction. Furthermore, core particles have been labeled with the fluorescent reagent N-(1-pyrenyl)maleimide (NPM), which was previously used as a sensitive probe for nucleosome conformation. Extensive DNase I or trypsin digestion of NPM-labeled core particles in 0.2 M NaCl does not produce significant changes in excimer fluorescence. This allows us to conclude that the covalent continuity of DNA is not required for the maintenance of the folded conformation of the core particle and that the trypsin-resistant domains of core histones play a fundamental role in the stabilization of this structure.     

H2A and H2B tails are essential to properly reconstitute nucleosome core particles

The conformation of recombinant Nucleosome Core Particles (NCPs) lacking H2A and H2B histone tails (gH2AgH2B) are studied. The migration of these particles in acrylamide native gels is slowed down compared to intact reconstituted NCPs. gH2AgH2B NCPs are also much more sensitive to nuclease digestion than intact NCPs. Small angle X-ray scattering (SAXS) experiments point out that the absence of H2A and H2B tails produces small but significant conformational changes of the octamers conformation (without wrapped DNA), whereas gH2AgH2B NCP conformations are significantly altered. A separation of about 25–30 bp from the core could account for the experimental curves, but other types of DNA superhelix deformation cannot be excluded. The distorted gH2AgH2B octamer may not allow the correct winding of DNA around the core. The absence of the H2A and H2B tails would further prevent the secondary sliding of the DNA around the core and therefore impedes the stabilisation of the particle. Cryo-electron microscopy on the same particles also shows a detachment of DNA portions from the particle core. The effect is even stronger because the vitrification of the samples worsens the instability of gH2AgH2B NCPs.     

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.     

Neutron scattering studies of nucleosome structure at low ionic strength

Ionic strength studies using homogeneous preparations of chicken erythrocyte nucleosomes containing either 146 or 175 base pairs of DNA show a single unfolding transition at about 1.5 mM ionic strength as determined by small-angle neutron scattering. The transition seen by some investigators at between 2.9 and 7.5 mM ionic strength is not observed by small-angle neutron scattering in either type of nucleosome particle. The two contrasts measured (H2O and D2O) indicate that only small conformational changes occur in the protein core, but the DNA is partially unfolded below the transition point. Patterson inversion of the data and analysis of models indicate that the DNA in both types of particle is unwinding from the ends, leaving about one turn of supercoiled DNA bound to the histone core in approximately its normal (compact) conformation. The mechanism of unfolding appears to be similar for both types of particles and in both cases occurs at the same ionic strength. The unfolding observed for nucleosomes in this study is in definite disagreement with extended superhelical models for the DNA and also disagrees with models incorporating an unfolded histone core.     

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.     

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.     

The structure of the nucleosome core particle of chromatin in chicken erythrocytes visualized by using atomic force microscopy

The structure of the nuclosome core particle of chromatin in chicken erythrocytes has been examined by using AFM.The 146 bp of DNA wrapped twice around the core histone octamer are clearly visualized.Both the ends of entry/exit of linker DNA are also demonstrated.The dimension of the nucleosome core particles is - 1-4 nm in height and - 13-22 nm in width.In addition,superbeads (width of - 48-57 nm,height of - 2-3 nm )are occasionally revealed,two turns of DNA around the core particles are also detected.     

Binding of ethidium to the nucleosome core particle. 1. Binding and dissociation reactions

We have examined binding properties of and dissociation induced by the intercalating dye ethidium bromide when it interacts with the nucleosome core particle under low ionic strength conditions. Ethidium binding to the core particle results in a reversible dissociation which requires the critical binding of 14 ethidium molecules. Under low ionic strength conditions, dissociation is about 90% completed in 5 h. The observed ethidium binding isotherm was corrected for the presence of free DNA due to particle dissociation. The corrected curve reveals that the binding of ethidium to the core particle itself is a highly cooperative process characterized by a low intrinsic binding constant of KA = 2.4 X 10(4) M-1 and a cooperativity parameter of omega = approximately 140. The number of base pairs excluded to another dye molecule by each bound dye molecule (n) is 4.5. Through the use of a chemical probe, methidiumpropyl-EDTA (MPE), we have localized the initial binding sites of ethidium in the core particle to consist of an average of 27 +/- 4 bp of DNA that are distributed near both ends of the DNA termini. MPE footprint analysis has also revealed that, prior to dissociation, the fractional population of core particles which bind the dye (f) may be as low as 50%. Comparison of the binding and dissociation data showed that the cooperative maximum of the binding curve occurred at or near the critical value, i.e., at the point where dissociation began. The data were used to generate a detailed model for the association of ethidium with chromatin at the level of the nucleosome.     

Structure of nucleosomes and organization of internucleosomal DNA in chromatin

We have compared the mononucleosomal pattern produced by micrococcal nuclease digestion of condensed and unfolded chromatin and chromatin in nuclei from various sources with the repeat length varying from 165 to 240 base-pairs (bp). Upon digestion of isolated H1-containing chromatin of every tested type in a low ionic strength solution (unfolded chromatin), a standard series of mononucleosomes (MN) was formed: the core particle, MN145, and H1-containing, MN165, MN175, MN185, MN195, MN205 and MN215 (the indexes give an approximate length of the nucleosomal DNA that differs in these particles by an integral number of 10 bp). In addition to the pattern of unfolded chromatin, digestion of whole nuclei or condensed chromatin (high ionic strength of Ca2+) gave rise to nuclei-specific, H1-lacking MN155. Digestion of H1-lacking chromatin produced only MN145, MN155 and MN165 particles, indicating that the histone octamer can organize up to 165 bp of nucleosomal DNA. Although digestion of isolated sea urchin sperm chromatin (repeat length of about 240 bp) at a low ionic strength gave a typical "unfolded chromatin pattern", digests of spermal nuclei contained primarily MN145, MN155, MN235 and MN245 particles. A linear arrangement of histones along DNA (primary organization) of the core particle was found to be preserved in the mononucleosomes, with the spacer DNA length from 10 to 90 bp on one (in MN155) or both sides of core DNA being a multiple of about 10 bp. In MN235, the core particle occupies preferentially a central position with the length of the spacer DNA on both sides of the core DNA being usually about 30 + 60 or 40 + 50 bp. Histone H1 is localized at the ends of these particles, i.e. close to the centre of the spacer DNA. The finding that globular part of histones H3 and sea urchin sperm H2B can covalently bind to spacer DNA suggests their involvement in the organization of chromatin superstructure. Our data indicate that decondensation of chromatin is accompanied by rearrangement of histone H1 on the spacer DNA sites adjacent to the core particle and thus support a solenoid model for the chromatin superstructure in nuclei in which the core DNA together with the spacer DNA form a continuous superhelix.     

Protein kinase in HeLA nucleosomes: a reevaluation of the interactions of histomes with the ends of core particle DNA.

HeLa chromatin core particles contain a protein kinase which transfers phosphate from ATP to both nonhistone proteins and histones. The enzyme preferentially modifies H3 among the histones; about 7% of the H3 molecules in the nucleoprotein are modified at saturation. Activity of this kinase likely contributed to earlier results using crosslinking methodology to study which histones interact with the ends of core particle DNA. When the kinase is largely removed by sedimentation of core particles through sucrose gradients containing 0.45 M NaCl, crosslinking of the 5'-terminal label on DNA is observed only to histone H3. The overall efficiency of the crosslinking reaction is about 15%. The origin of the 5'-terminal 32P previously assigned as crosslinked to H4 is not explained by the current experiments.     

H3 and H4 histone tails play a central role in the interactions of recombinant NCPs

Using small-angle x-ray scattering, we probe the effect of histone tails on both internucleosomal interactions and nucleosome conformation. To get insight into the specific role of H3 and H4 histone tails, perfectly monodisperse recombinant nucleosome core particles were reconstituted, either intact or deprived of both H3 and H4 histone tails (gH3gH4). The main result is that H3 and H4 histone tails are necessary to induce attractive interactions between NCPs. A pair potential model was used to describe interactions between NCPs. At all salt concentrations, interactions between gH3gH4 NCPs are best described by repulsive interactions exclusively. For intact NCPs, an additional attractive term, with a 5–10 kT magnitude and 20 Å range, is required to account for interparticle interactions above 50 mM monovalent salt. Regarding conformation, intact NCPs in solution are similar to NCPs in 3D crystals. gH3gH4 NCPs instead give rise to slightly different small-angle x-ray scattering curves that can be understood as a more opened conformation of the particle, where DNA ends are slightly detached from the core.     

Molecular flexibility in protein-DNA interactions

In living cells protein-DNA interactions are fundamental processes. Here, we compare the 3D structures of several DNA-binding proteins frequently determined with and without attached DNA. We studied the global structure (backbone-traces) as well as the local structure (binding sites) by comparing pair-wise the related atoms. The DNA-interaction sites of uncomplexed proteins show conspicuously high local structural flexibility. Binding to DNA results in specific local conformations, which are clearly distinct from the unbound states. The adaptation of the protein's binding site to DNA can never be described by the lock and key model but in all cases by the induced fit model. Conformational changes in the seven protein backbone traces take place in different ways. Two of them dock onto DNA without a significant change, while the other five proteins are characterized by a backbone conformation change caused by DNA docking. In the case of three proteins of the latter group the DNA-complexed conformation also occurs in a few uncomplexed structures. This behavior can be described by a conformational ensemble, which is narrowed down by DNA docking until only one single DNA-complexed conformation occurs. Different docking models are discussed and each of the seven proteins is assigned to one of them.     

lac Operator nucleosomes. 2. lac Nucleosomes can change conformation to strengthen binding by lac repressor

We have shown previously that lac repressor binds specifically and quantitatively to lac operator restriction fragments which have been complexed with histones to form artificial nucleosomes (203 base pair restriction fragment) or core particles (144 base pair restriction fragment. We describe here a quantitative method for determining the equilibrium binding affinities of repressor for these lac reconstitutes. Quantitative analysis shows that the operator-histone reconstitutes may be grouped into two affinity classes: those with an affinity for repressor close to that of naked DNA and those with an affinity 2 or more orders of magnitude less than that of naked DNA. All particles in the lac nucleosome preparations bind repressor with high affinity, but the lac core particle preparations contain particles of both high and low affinities for repressor. Formaldehyde cross-linking causes all high-affinity species to suffer a 100-fold decrease in binding affinity. In contrast, there is no effect of cross-linking on species of low affinity. Therefore, the ability of a particle to be bound tightly by repressor depends on a property of the particle which is eliminated by cross-linking. Control experiments have shown that chemical damage to the operator does not accompany cross-linking. Therefore, the property sensitive to cross-linking must be the ability of the particle to change conformation. We infer that the particles of low native affinity, like cross-linked particles, are of low affinity because of an inability to facilitate repressor binding by means of this conformational change. Dimethyl suberimidate cross-linking experiments show that histone-histone cross-linking is sufficient to preclude high-affinity binding. Thus, the necessary conformational change involves a nucleosome histone core event. We find that the ability of a particle to undergo a repressor-induced facilitating conformational change appears to depend on the position of the operator along the DNA binding path of the nucleosome core. We present a general model which proposes that nucleosomes are divided into domains which function differentially to initiate conformational changes in response to physiological stimuli.     

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.