Binding of ethidium to the nucleosome core particle. 2. Internal and external binding modes

We have previously reported that the binding of ethidium bromide to the nucleosome core particle results in a stepwise dissociation of the structure which involves the initial release of one copy each of H2A and H2B (McMurray & van Holde, 1986). In this report, we have examined the absorbance and fluorescence properties of intercalated and outside bound forms of ethidium bromide. From these properties, we have measured the extent of external, electrostatic binding of the dye versus internal, intercalation binding to the core particle, free from contribution by linker DNA. We have established that dissociation is induced by the intercalation mode of binding to DNA within the core particle DNA, and not by binding to the histones or by nonintercalative binding to DNA. The covalent binding of [3H]-8-azidoethidium to the core particle clearly shows that less than 1.0 adduct is formed per histone octamer over a wide range of input ratios. Simultaneously, analyses of steady-state fluorescence enhancement and fluorescence lifetime data from bound ethidium complexes demonstrate extensive intercalation binding. Combined analyses from steady-state fluorescence intensity with equilibrium dialysis or fluorescence lifetime data revealed that dissociation began when approximately 14 ethidium molecules are bound by intercalation to each core particle and less than 1.0 nonintercalated ion pair was formed per core particle.     

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.     

Fluorescence anisotropy decay of ethidium bound to nucleosome core particles. 1. Rotational diffusion indicates an extended structure at low ionic strength

The fluorescence decay of ethidium intercalated into the DNA of nucleosome core particles increases in average lifetime from about 22 ns in H2O to about 39 ns in D2O. This increase, combined with the acquisition of large amounts of data (on the order of 10(8) counts per decay), allows measurement of anisotropy decays out to more than 350 ns. The overall slow rotational motions of the core particle may thereby be more clearly distinguished from the faster torsional motions of the DNA. In 10 mM NaCl at 20 degrees C, we recover a long correlation time of 198 ns in D2O (159 ns when corrected to a viscosity of 1.002 cP), in agreement with the value of 164 ns obtained in H2O. These values are consistent with hydrodynamic calculations based on the expected size and shape of the hydrated particle. To support our conclusion that this long correlation time derives from Brownian rotational diffusion, we show that the value is directly proportional to the viscosity and inversely proportional to the temperature. No significant changes in the rotational correlation time are observed between 1 and 500 mM ionic strength. Below 1 mM, the particle undergoes the "low-salt transition" as measured by steady-state tyrosine fluorescence anisotropy. However, we observe little change in shape until the ionic strength is decreased below approximately 0.2 mM, where the correlation time increases nearly 2-fold, indicating that the particle has opened up into an extended form. We have previously shown that the transition becomes nonreversible below 0.2 mM salt.     

Fluorescence anisotropy decay of ethidium bound to chromatin

The fluorescence anisotropy decays of the chromatin ethidium complexes have been measured in solutions in which the dye was bound to the high affinity sites of the nucleosome DNA. Energy transfers between chromatin-bound ethidium molecules cause an increase of the anisotropy decay rate for much smaller values of the concentration ratio of dye to nucleotide than in the case of nacked DNA-ethidium complexes. This result implies that the high affinity sites are clustered on a short nucleosomal DNA segment. Quantitative analysis of the experimental data by computer simulations of the energy transfer process, shows that these sites are gathered on a single nucleosomal DNA segment, 28 base pairs long. Such a segment probably belongs to the nucleosome “linker”, contributing about half of it.     

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.     

Arginine residues involved in strong histone--DNA interactions to fold DNA into the nucleosome core particle.

The numbers of the arginine residues involved in strong histone-DNA interactions to fold DNA into a nucleosome core particle were determined for each of the four core histones, by kinetic studies of chemical modification of the residues in the nucleosome core particle. It was suggested that the arginines in the globular region of H3 histone make major contributions to the strong binding of the octameric histones to the core DNA.     

Dynamics of Z-form DNA

The torsional and bending rigidities of Z-form DNA have been studied by nanosecond fluorescence anisotropy measurements of intercalated ethidium. The results suggested that Z-form DNA was considerably more flexible than B-form DNA. We have investigated the temperature dependence of the rigidity of B- and Z-form DNA and found that the temperature dependence of the torsional rigidity of Z-form DNA was remarkably lower than that of B-form DNA.     

Asymmetry and polarity of nucleosomes in chicken erythrocyte chromatin.

Nucleosome dimers containing, on average, a single molecule of histone H5 have been isolated from chicken erythrocyte nuclei and the associated DNA fragments cloned and sequenced. The average sequence organization of at least one of the two nucleosomes in the dimers is highly asymmetric and suggests that the torsional, as well as the axial, flexibility of DNA is a determinant of nucleosome positioning. On average the nucleosome dimer is a polar structure containing linker DNA of variable lengths. The sequences associated with H5 containing nucleosomes and core particles are sufficiently different to indicate that removal of histone H5 (or H1) from chromatin may result in the migration of the histone octamer and a consequent exposure of sites for regulatory proteins.     

Change of conformation and internal dynamics of supercoiled DNA upon binding of Escherichia coli single-strand binding protein

The influence of Escherichia coli single-strand binding (SSB) protein on the conformation and internal dynamics of pBR322 and pUC8 supercoiled DNAs has been investigated by using dynamic light scattering at 632.8 and 351.1 nm and time-resolved fluorescence polarization anisotropy of intercalated ethidium. SSB protein binds to both DNAs up to a stoichiometry that is sufficient to almost completely relax the superhelical turns. Upon saturation binding, the translational diffusion coefficients (D0) of both DNAs decrease by approximately 20%. Apparent diffusion coefficients (Dapp) obtained from dynamic light scattering display the well-known increase with K2 (K = scattering vector), leveling off toward a plateau value (Dplat) at high K2. For both DNAs, the difference Dplat - D0 increases upon relaxation of supercoils by SSB protein, which indicates a corresponding enhancement of the subunit mobilities in internal motions. Fluorescence polarization anisotropy measurements on free and complexed pBR322 DNA indicate a (predominantly) uniform torsional rigidity for the saturated DNA/SSB protein complex that is significantly reduced compared to the free DNA. These observations are all consistent with the notion that binding of SSB protein is accompanied by a gradual loss of supercoils and saturates when the superhelical twist is largely removed.     

Role of the histone amino termini in facilitated binding of a transcription factor, GAL4-AH, to nucleosome cores.

Facilitated, "cooperative" binding of GAL4-AH to nucleosomal DNA occurred in response to inhibition from the core histone amino termini. The binding of GAL4-AH (which contains the DNA-binding and dimerization domains of GAL4) to nucleosome cores containing multiple binding sites initiated at the end of a nucleosome core and proceeded in a cooperative manner until all sites were occupied. However, following tryptic removal of the core histone amino termini, GAL4-AH binding appeared to be noncooperative, similar to binding naked DNA. Binding of GAL4-AH to nucleosomes bearing a single GAL4 site at different positions indicated that inhibition of GAL4 binding was largely mediated by the histone amino termini and primarily occurred at sites well within the core and not near the end. When the histone amino termini were intact, binding of GAL4-AH to sites near the center of a nucleosome core was greatly enhanced by the presence of additional GAL4 dimers bound to more-accessible positions. These data illustrate that the binding of a factor to more-accessible sites, near the end of a nucleosome, allows facilitated binding of additional factors to the center of the nucleosome, thereby overcoming repression from the core histone amino termini. This mechanism may contribute to the binding of multiple factors to complex promoter and enhancer elements in cellular chromatin.     

Torsional motion of eosin-labeled F-actin as detected in the time-resolved anisotropy decay of the probe in the sub-millisecond time range

The internal motion of F-actin in the time range from 10(-6) to 10(-3) second has been explored by measuring the transient absorption anisotropy of eosin-labeled F-actin using laser flash photolysis. The transient absorption anisotropy of eosin-F-actin at 20 degrees C has a component that decays in the submicrosecond time scale to an anisotropy of about 0.3. This anisotropy then decays with a relaxation time of about 450 microseconds to a residual anisotropy of about 0.1 after 2 ms. When the concentration of eosin-F-actin was varied in the range from 7 to 28 microM, the transient absorption anisotropy curves obtained were almost indistinguishable from each other. These results show that the anisotropy decay arises from internal motion of eosin-F-actin. Analysis of the transient absorption anisotropy curves indicates that the internal motion detected by the decay in anisotropy is primarily a twisting of actin protomers in the F-actin helix; bending of the actin filament makes a minor contribution only to the measured decay. The torsional rigidity calculated from the transient absorption anisotropy is 0.2 X 10(-17) dyn cm2 at 20 degrees C, which is about an order of magnitude smaller than the flexural rigidity determined from previous studies. Thus, we conclude that F-actin is more flexible in twisting than in bending. The calculated root-mean-square fluctuation of the torsional angle between adjacent actin protomers in the actin helix is about 4 degrees at 20 degrees C. We also found that the torsional rigidity is approximately constant in the temperature range from 5 to approximately 35 degrees C, and that the binding of phalloidin does not appreciably affect the torsional motion of F-actin.     

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.     

Solvent mediated interactions in the structure of the nucleosome core particle at 1.9 a resolution

Solvent binding in the nucleosome core particle containing a 147 base pair, defined-sequence DNA is characterized from the X-ray crystal structure at 1.9 Å resolution. A single-base-pair increase in DNA length over that used previously results in substantially improved clarity of the electron density and accuracy for the histone protein and DNA atomic coordinates. The reduced disorder has allowed for the first time extensive modeling of water molecules and ions.Over 3000 water molecules and 18 ions have been identified. Water molecules acting as hydrogen-bond bridges between protein and DNA are approximately equal in number to the direct hydrogen bonds between these components. Bridging water molecules have a dual role in promoting histone-DNA association not only by providing further stability to direct protein-DNA interactions, but also by enabling formation of many additional interactions between more distantly related elements. Water molecules residing in the minor groove play an important role in facilitating insertion of arginine side-chains. Water structure at the interface of the histones and DNA provides a means of accommodating intrinsic DNA conformational variation, thus limiting the sequence dependency of nucleosome positioning while enhancing mobility.Monovalent anions are bound near the N termini of histone α-helices that are not occluded by DNA phosphate groups. Their location in proximity to the DNA phosphodiester backbone suggests that they damp the electrostatic interaction between the histone proteins and the DNA. Divalent cations are bound at specific sites in the nucleosome core particle and contribute to histone-histone and histone-DNA interparticle interactions. These interactions may be relevant to nucleosome association in arrays.     

DNA recognition and nucleosome organization

The affinity of a DNA sequence for the histone octamer in a core nucleosome depends on the intrinsic flexibility of the DNA. This parameter can be affected both by the sequence-dependent conformational preferences of individual base steps and by the nature and location of the exocyclic groups of the DNA bases. By adopting highly preferred conformations particular types of base step can influence the rotational positioning of the DNA on the surface of the histone octamer. The asymmetry of the next higher order of chromatin structure is determined in part by the asymmetric binding of the globular domain of histone H5 to the core nucleosome. © 1998 John Wiley & Sons, Inc. Biopoly 44: 423–433 1997     

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.     

Characterization of monoclonal antibodies to histone 2B. Localization of epitopes and analysis of binding to chromatin

Two mouse monoclonal IgM antibodies have been isolated which bind to histone 2B (H2B), as shown by protein blotting and immunostaining and by solid-phase radioimmunoassay (RIA). One of these (HBC-7) was specific for H2B by both techniques whereas the other (2F8) cross-reacted with histone H1 by RIA. Both antibodies failed to recognize H2B limit peptides from trypsin-digested chromatin and did not bind to Drosophila H2B, which differs extensively from vertebrate H2B only in the N-terminal region. These findings indicate that both antibodies recognize epitopes within the trypsin-sensitive, N-terminal region comprising residues 1-20. Binding of antibody HBC-7 was inhibited by in vitro ADP-ribosylation of H2B at glutamic acid residue 2. This strongly suggests that the epitope recognized by HBC-7 is located at the N-terminus of H2B, probably between residues 1 and 8. We have used solid-phase radioimmunoassay to investigate factors which influence the accessibility of this epitope in chromatin. Removal of H1 ('stripping') from high-molecular-mass chromatin had no effect on HBC-7 binding, nor was any difference observed between binding to stripped chromatin and to 146-base-pair (bp) core particles derived from it by nuclease digestion. These results suggest that accessibility of the N-terminal region of H2B is not influenced by H1 itself or by the size or conformation of linker DNA. In contrast, binding of antibody HBC-7 to 146-bp core particles derived from unstripped chromatin was reduced by up to 70%. Binding was restored by exposure of these core particles to the conditions used for stripping. Analysis of the protein content of core particle preparations from stripped and unstripped chromatin suggests that these findings may be attributable to redistribution of non-histone proteins during nuclease digestion. Pre-treatment of high-molecular-mass chromatin or 146-bp core particles with the intercalating dye ethidium bromide resulted in a severalfold increase in binding of HBC-7. The major changes in nucleosome morphology induced by ethidium are therefore accompanied by an increase in accessibility of the N-terminal region of H2B, possibly as a direct result of changes in the spatial relationship between H2B and core DNA.     

Construction of nucleosome cores from defined DNA sequences of prokaryotic origin.

A procedure for the de novo construction of nucleosome core particles from defined DNA sequences of prokaryotic origin is described. Efficient de novo reconstitution without added carrier DNA is demonstrated. DNase I and exonuclease III analysis of a nucleosome core prepared from a 154 base pair fragment extending from base 853 to base 1006 of pBR322 indicates a non-random positioning of the histone core along the DNA. As bacteria have no histones, their DNA cannot be expected to have a histone core positioning signal encoded in it, the efficient formation of a uniquely positioned core particle is not self evident. The possibility that a phosphate end group positions DNA fragments on the histone is considered. The de novo reconstitution of carrier-less defined nucleosome core particles should facilitate the physicochemical study of nucleosomes on the fine structural level.