Analysis of the dynamic equilibrium of histone oligomers in a solution. The nature of forces stabilizing the (H2A-H2B-H3-H4)2 octamer structure

Dynamic equilibrium analysis of the (H2A-H2B-H3-H4)2 histone octamer with lower oligomers was performed in 2 M NaCl. Calculated data on the relative content of histone oligomers upon changing protein concentration in solution are given. The red shift of lambda max for histone tyrosine fluorescence spectra is shown to be due to hydrogen bond formation by tyrosyl OH-groups. Analysis of free energy changes of histone oligomers upon association (delta G = -17,37 +/- 0,14 kcal/mole) as well as the effect of urea on histone octamer dissociation made it possible to conclude that virtually all tyrosyls in octamer form hydrogen bonds. Intermolecular hydrogen bonds formed by tyrosyls contribute substantially to octamer stabilization. The (H2A-H2B) dimer positive cooperativity in association with the (H3-H4)2 tetramer was found. This cooperativity is caused by interaction between association sites with a two order increase in an apparent constant of dimers with tetramer association. The histone octamer was determined to be of asymmetric structure due to unequivolency of the two binding sites for the (H2A-H2B) dimers.     

Salt effects on histone subunit interactions as studied by fluorescence spectroscopy

The salt concentration dependence of the aggregation properties of calf thymus and chicken erythrocyte histones has been investigated by using fluorescence spectroscopy. The isolated H2A/H2B and H3/H4 subunit preparations were labeled with 5-(dimethylamino)naphthalene-1- sulfonyl (dansyl). This long-lived fluorescence probe allows for the observation of rotations due to tumbling of the particle and thus is a probe for changes in the size of macromolecular assemblies. The fluorescence polarization and lifetime were measured as a function of salt concentration for these isolated preparations. Next, each labeled preparation was reconstituted with its unlabeled complement, and the salt concentration dependence of histone core octamer interactions was investigated in the same manner. Salt-induced core particle formation was observed by monitoring the dansyl-labeled dimers for both the calf thymus and chicken erythrocyte preparations. Evidence for subunit dissociation of the isolated H2A-H2B preparations was also found, as well as aggregation of the isolated H3/H4 subunits to at least dimers of tetramers. The calf thymus H3/H4 preparation was in aggregated form under all conditions studied, whereas the chicken erythrocyte H3/H4 only formed aggregates at high protein or salt concentrations. We have found evidence that the dimer can displace the tetramer from the higher order aggregate in order to form core particles. Such competition between the subunit interfaces in the histone system suggests that they may play a regulatory role in histone-DNA interactions.     

The nature of forces stabilizing nucleosome structure. Dissociation of histone octamers from DNA

We have used the measurements of the histone fluorescence parameters to study the influence of the ionic strength on histone-DNA and histone-histone interactions in reconstructed nucleosomes. The ionic strength increase lead to the two-stage nucleosome dissociation. The dimer H2A-H2B dissociates at the first stage and the tetramer (H3-H4)2 at the second one. The dimer H2A-H2B dissociation from nucleosome is a two-stage process also. The ionic bonds between (H2A-H2B) histone dimer and DNA break at first and then the dissociation of dimer from histone tetramer (H3-H4)2 occurs. According to the proposed model the dissociation accompanying a nucleosome "swelling" and an increase of DNA curvature radius. It was shown that the energy of electrostatic interactions between histone dimer and DNA is sufficiently less than the energy of dimer-tetramer interaction. We propose that the nucleosome DNA ends interact with the dimer and tetramer simultaneously. The calculated number (approximately 30 divided by 40) of ionic bonds between DNA and histone octamer globular part practically coincides with the number of exposed cationic groups on the surface of octamer globular head. On this basis we have assumed that the spatial distribution of these groups is precisely determined, which explains the high evolutionary conservatism of the histone primary structure.     

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.     

Enhanced stability of histone octamers from plant nucleosomes: role of H2A and H2B histones.

Gel filtration and sedimentation studies have previously established that the vertebrate animal core histone octamer is in equilibrium with an (H3-H4)2 tetramer and an H2A-H2B dimer [Eickbush, T. H., & Moudrianakis, E. N. (1978) Biochemistry 17, 4955-4964; Godfrey, J. E., Eickbush, T. H., & Moudrianakis, E. N. (1980) Biochemistry 19, 1339-1346]. We have investigated the core histone octamer of wheat (Triticum aestivum L.) and have found it to be much more stable than its vertebrate animal counterpart. When vertebrate animal histone octamers are subjected to gel filtration in 2 M NaCl, a trailing peak of H2A-H2B dimer can be clearly resolved from the main octamer peak. When the plant octamer is subjected to the identical procedure, there is no trailing peak of H2A-H2B dimer, but rather a single peak containing the octamer. A sampling across the octamer peak from leading to trailing edge shows no change in the ratio of H2A-H2B to (H3-H4)2. Surprisingly, the plant octamer shows the same stability at 0.6 M NaCl, a salt concentration in which the vertebrate animal octamer dissociates into dimers and tetramers. Equilibrium sedimentation data indicate that the assembly potential of the wheat histones in 2 M NaCl is very high at all protein concentrations above 0.1 mg mL-1. In order to disrupt the forces stabilizing the plant histone octamer at high histone concentrations, the concentration of NaCl must be lowered to approximately 0.3 M.(ABSTRACT TRUNCATED AT 250 WORDS)     

Accessibility of histone oligomers to the action of trypsin in a solution or in chromatin with different degrees of compactness

The accessibility to trypsin of "core" histones within the dimer (H2A-H2B), tetramer (H3-H4)2, octamer (H2A-H2B-H3-H4)2 and in chromatin was studied. It was shown that the hydrolysis of histones H2A and H2B within the dimer and octamer occurs in essentially the same way. The tetramer (H2-H4)2 becomes more compact with an increase in the ionic strength. Some of the tetramer (H3-H4)2 sites within the octamer are protected against trypsin. It was demonstrated that in terms of the histone accessibility to trypsin chromatin can exist in three states, i.e., tightly packed (in the presence of histone H1 and bivalent cations), intermediate (in the absence of histone H1 or bivalent cations) and folded (in the absence of histone H1 and bivalent cations). The folding of histones in neither of these chromatin states coincides with that within the octamer in 2M NaCl.     

Equilibrium folding of the core histones: the H3-H4 tetramer is less stable than the H2A-H2B dimer

To compare the stability of structurally related dimers and to aid in understanding the thermodynamics of nucleosome assembly, the equilibrium stabilities of the recombinant wild-type H3-H4 tetramer and H2A-H2B dimer have been determined by guanidinium-induced denaturation, using fluorescence and circular dichroism spectroscopies. The unfolding of the tetramer and dimer are highly reversible. The unfolding of the H2A-H2B dimer is a two-state process, with no detected equilibrium intermediates. The H3-H4 tetramer is unstable at moderate ionic strengths (mu approximately 0.2 M). TMAO (trimethylamine-N-oxide) was used to stabilize the tetramer; the stability of the H2A-H2B dimer was determined under the same solvent conditions. The equilibrium unfolding of H3-H4 was best described by a three-state mechanism, with well-folded H3-H4 dimers as a populated intermediate. When compared to H2A-H2B, the H3-H3 tetramer interface and the H3-H4 histone fold are strikingly less stable. The free energy of unfolding, in the absence of denaturant, for the H3-H4 and H2A-H2B dimers are 12.4 and 21.0 kcal mol(-)(1), respectively, in 1 M TMAO. It is postulated that the difference in stability between the histone dimers, which contain the same fold, is the result of unfavorable tertiary interactions, most likely the partial to complete burial of three salt bridges and burial of a charged hydrogen bond. Given the conservation of these buried interactions in histones from yeast to mammals, it is speculated that the H3-H4 tetramer has evolved to be unstable, and this instability may relate to its role in nucleosome dynamics.     

Spectropolarimetric analysis of the core histone octamer and its subunits

The secondary structure of the calf thymus core histone octamer, (H2A-H2B-H3-H4)2, and its two physiological subunits, the H2A-H2B dimer and (H3-H4)2 tetramer, was analyzed by ORD spectropolarimetry as a function of temperature and solvent ionic strength within the ranges of these experimental parameters where assembly of the core histone octamer exhibits pronounced sensitivity. While the secondary structure of the dimer is relatively stable from 0.1 to 2.0 M NaCl, the secondary structure of the tetramer exhibits complex changes over this range of NaCl concentrations. Both complexes exhibit only modest responses to temperature changes. ORD spectra of very high and very low concentrations of stoichiometric mixtures of the core histones revealed no evidence of changes in the ordered structure of the histones as a result of the octamer assembly process at NaCl concentrations above 0.67 M, nor were time-dependent changes detected in the secondary structure of tetramer dissolved in low ionic strength solvent. The secondary structure of the chicken erythrocyte octamer dissolved in high concentrations of ammonium sulfate, including those of our crystallization conditions, was found to be essentially unchanged from that in 2 M NaCl when examined by both ORD and CD spectropolarimetry. The two well-defined cleaved products of the H2A-H2B dimer, cH2A-H2B and cH2A-cH2B, exhibited reduced amounts of ordered structure; in the case of the doubly cleaved moiety cH2A-cH2B, the reductions were so pronounced as to suggest marked structural rearrangements.     

Isolation and physico-chemical properties of native histone complexes: dimer (H2-H2B), tetramer (H3-H4)2 and octamer (H3-H4-H2A-H2B)2

The paper is concerned with the isolation of the native histone complexes: dimer (H2A-H2B), tetramer (H3-H4)2 and octamer (H3-H4-H2A-H2B)2 from the calf thymus chromatin under soft conditions (hydroxyl apatite) fractionation with the subsequent gel filtration). Parameters of hydroxyl apatite saturation with chromatin are determined. The complexes obtained are free of DNA and nonhistone proteins. Absorption spectra parameters, quantum efficiencies and fluorescence spectra typical of the corresponding histone oligomers are established. Comparison of free tyrosine fluorescence spectra with histone tyrosyl ones revealed a long-wave shift in the latter.     

The oxidised histone octamer does not form a H3 disulphide bond

A H3 dimer band is produced when purified native histone octamers are run on an SDS-PAGE gel in a beta-mercaptoethanol-free environment. To investigate this, native histone octamer crystals, derived from chicken erythrocytes, and of structure (H2A-H2B)-(H4-H3)-(H3'-H4')-(H2B'-H2A'), were grown in 2 M KCl, 1.35 M potassium phosphates and 250-350 microM of the oxidising agent S-nitrosoglutathione, pH 6.9. X-ray diffraction data were acquired to 2.10 A resolution, yielding a structure with an Rwork value of 18.6% and an Rfree of 22.5%. The space group is P6(5), the asymmetric unit of which contains one complete octamer. Compared to the 1.90 A resolution, unoxidised native histone octamer structure, the crystals show a reduction of 2.5% in the c-axis of the unit cell, and free-energy calculations reveal that the H3-H3' dimer interface in the latter has become thermodynamically stable, in contrast to the former. Although the inter-sulphur distance of the two H3 cysteines in the oxidised native histone octamer has reduced to 6 A from the 7 A of the unoxidised form, analysis of the hydrogen bonds that constitute the (H4-H3)-(H3'-H4') tetramer indicates that the formation of a disulphide bond in the H3-H3' dimer interface is incompatible with stable tetramer formation. The biochemical and biophysical evidence, taken as a whole, is indicative of crystals that have a stable H3-H3' dimer interface, possibly extending to the interface within an isolated H3-H3' dimer, observed in SDS-PAGE gels.     

Spatial organization of the (H3-H4-H2A-H2B)2 histone octamer

Structure of the (H2A-H2B-H3-H4)2 histone octamer isolated from calf thymus chromatin at ionic strength 0.1 to 4.0 M NaCl, pH 7.6, was studied spectrofluorometrically. Sensitivity of lambda max tyrosine fluorescence position to structural changes of histone oligomers and to the processes of their association was shown. It were detect two ranges of cooperative changes in histone optical parameters at 0.6-1.4 M NaCl (transition I) and at 2.4-3.4 M NaCl (transition II): Transition I corresponds to the formation of equilibrium system (hexamer) + (dimer) in equilibrium octamer. Transition II corresponds to the structural changes of the histone octamer. Thus, fluorescence anisotropy increases, lambda max for fluorescence spectrum is shifted to the longer wavelengths, contributions of two components to fluorescence decay change, a fraction of fluorescence accessible to the quenching by I- decreases. Histone octamer formation is characterized by making specific contacts between the (H2A-H2B) dimer and (H3-H4)2 tetramer. These contacts are realized at gradual changing of ionic strengths (by dialysis). In the case of abrupt local changes of the environment the process is irreversibly shifted to formation of unspecific high molecular aggregates. The important function role for energetically degenerated states of histone oligomers, energy barriers between which can be overcome by changing total conditions of histone microenvironment in chromatin is discussed.     

Macromolecular binding equilibria in the lac repressor system: studies using high-pressure fluorescence spectroscopy

High hydrostatic pressure coupled with fluorescence polarization has been used to investigate protein subunit interactions and protein-operator association in lac repressor labeled with a long-lived fluorescent probe. On the basis of observation of a concentration-dependent sigmoidal decrease in the dansyl fluorescence polarization, we conclude that application of high hydrostatic pressure results in dissociation of the lac repressor tetramer. The 2-fold decrease in the rotational relaxation time and the high-pressure plateau are consistent with a tetramer to dimer transition. The volume change for tetramer dissociation to dimer is -82 +/- 5 mL/mol. The dissociation constant calculated from the data taken at 4.5 degrees C is 4.3 +/- 1.3 nM. The tetramer dissociation constant increases by a factor of 3 when the temperature is raised from 4.5 to 21 degrees C. A very small effect of inducer binding on the subunit dissociation is observed at 4.5 degrees C; the Kd increases from 4.5 to 7.1 nM. At 21 degrees C, however, inducer binding stabilizes the tetramer by approximately 0.8 kcal/mol. Pressure-induced monomer formation is indicated by the curves obtained upon raising the pH to 9.2. The addition of IPTG shifts the pressure transition to only slightly higher pressures at this pH, indicating that the stabilization of the tetramer by inducer is not as marked as that observed at pH 7.1. From the decrease in the polarization of the dansyl repressor-operator complexes, we also conclude that the application of pressure results their dissociation and that the volume change is large in absolute value (approximately 200 mL/mol). The lac repressor-operator complex is more readily dissociated upon the application of pressure than the tetramer alone, indicating that operator binding destabilizes the lac repressor tetramer.     

A rapid method of preparing the (H3-H4-H2A-H2b)(2) histone octamer in large quantities]

A simple and fast method for isolation of large amounts of the histone octamer (H2A-H2B-H3-H4)2 is proposed. This method is based on chromatin adsorption by hydroxyapatite with subsequent extraction of the histone octamer with 50 mM sodium-phosphate buffer containing 4 M NaCl pH 8.0. It was shown that the properties of the histone octamer isolated by this extractive procedure are identical with those of the histone octamer obtained by elution on a Sephadex G-100 column. The histone tetramer (H3-H4)2 and dimer (H2A-H2B) were obtained after gel filtration on Sephadex G-100 in 50 mM sodium-acetate (pH 5.6).     

Histone octamer instability under single molecule experiment conditions

We have studied the sample concentration-dependent and external stress-dependent stability of native and reconstituted nucleosomal arrays. Whereas upon stretching a single chromatin fiber in a solution of very low chromatin concentration the statistical distribution of DNA length released upon nucleosome unfolding shows only one population centered around approximately 25 nm, in nucleosome stabilizing conditions a second population with average length of approximately 50 nm was observed. Using radioactively labeled histone H3 and H2B, we demonstrate that upon lowering the chromatin concentration to very low values, first the linker histones are released, followed by the H2A-H2B dimer, whereas the H3-H4 tetramer remains stably attached to DNA even at the lowest concentration studied. The nucleosomal arrays reconstituted on a 5 S rDNA tandem repeat exhibited similar behavior. This suggests that the 25-nm disruption length is a consequence of the histone H2A-H2B dimer dissociation from the histone octamer. In nucleosome stabilizing conditions, a full approximately 145 bp is constrained in the nucleosome. Our data demonstrate that the nucleosome stability and histone octamer integrity can be severely degraded in experiments where the sample concentration is low.     

H2a-specific proteolysis as a unique probe in the analysis of the histone octamer

We have utilized the H2a-specific protease as a unique probe to investigate the nature of the interactions between the protein subunits which form the core histone octamer. Upon incubation in high ionic strength media this protease, normally found tightly associated with isolated calf thymus chromatin, releases the 15 COOH-terminal amino acids of histone H2a by specifically cleaving the H2a polypeptide between Val114 and Leu115, yielding cleaved H2a (cH2a) and a free pentadecapeptide (Eickbush, T. H., Watson, D. K., and Moudrianakis, E. N. (1976) Cell 9, 785-792). We find that removal of this pentadecapeptide results in a marked dissociation of the octamer into its H2a:H2b dimer and H3:H4 tetramer subunits. Reconstitution experiments indicate that cH2a is capable of forming a dimer with H2b, but this cH2a:H2b dimer has a substantially lower affinity for the H3:H4 tetramer than native H2a:H2b dimer. Kinetic studies of H2a cleavage in high ionic strength solutions demonstrate that H2a molecules in the octamer are relatively resistant to proteolytic attack compared to H2a molecules in the dimer. The extent of this resistance, in response to various experimental parameters, is directly correlated to the strength of interaction between the H2a:H2b dimer and H3:H4 tetramer subunits. These reconstitution and kinetic experiments suggest that the histone domains proximal to the H2a cleavage site have an important function in maintaining the association of the histone octamer subunits.     

Dissociation of the lactose repressor protein tetramer using high hydrostatic pressure

Dissociation of lac repressor tetramer by high hydrostatic pressures was monitored with intrinsic tryptophan fluorescence. With the assumption of complete dissociation to monomer, tryptophan polarization data gave delta V a approximately 170 mL/mol and the concentration for 50% tetramer dissociation, C1/2, was 3.8 X 10(-8) M. Upon addition of inducer, the calculated delta V a increased to approximately 220 mL/mol and the C1/2 decreased to approximately 1 X 10(-8) M, a free energy difference of approximately 0.7 kcal. These results indicate a modest stabilization of the tetramer by the presence of inducer. Monitoring the average energy of tryptophan emission demonstrated that tetramer dissociation takes place over the same range of pressures as evidenced by the polarization data and IPTG dissociation can be more or less superimposed upon tetramer dissociation depending upon the ligand concentration used. Although the two transitions cannot be separated entirely, the delta V a for the region of the pressure dependence dominated by ligand dissociation was 69 mL/mol, an unexpectedly large value. For tetramer modified with methyl methanethiosulfonate, subunit dissociation was shifted to much higher pressures and IPTG dissociation did not occur. The delta V a for subunit association was calculated as approximately 160 mL/mol, and the C1/2 was 3.5 X 10(-9) M. Interactions at the subunit interface of the modified protein are apparently stronger than in the unmodified protein. The absence of inducer dissociation from the MMTS-modified tetramer by the application of high hydrostatic pressure suggests that the volume change for inducer binding to the modified protein is much smaller than that observed for the unmodified repressor.     

Pressure dissociation and conformational drift of the beta dimer of tryptophan synthase

Micromolar solutions of tryptophan synthase beta 2 dimer dissociate into monomers in the pressure range of 800-1600 bars as shown by studies of the spectral shift of the intrinsic fluorescence and of the fluorescence polarization of dansyl conjugates. At 25 degrees C the standard change in volume on dissociation (dV0) of the holoprotein was -162 mL mol-1, and the dissociation constant at 1 bar was K0 = 3.7 10(-10) M. Pyridoxal-reduced holoprotein and apoprotein had, within 10%, the same dV0, but K0 was decreased in the reduced protein (6 X 10(-11) M) and increased in the apoprotein (3.6 X 10(-9) M). At 4 degrees C the free energy of association of the holoprotein was reduced by 1.4 kcal mol-1, but dV0 was unchanged. In all the protein forms the decompression curves differed from the respective compression curves, indicating the loss of some free energy of association following separation of the monomers. This hysteretic behavior was largest in the apoprotein and amounted to a loss of 2.6 kcal mol-1 in the free energy of association. When the pressure was rapidly raised to 2.2 kbars, half-dissociation of the reduced pyridoxal beta 2 dimer took approximately 12 min. Upon return to atmospheric pressure reassociation was complete in 2-3 min and half of the enzyme activity was regained in 10 min; pyridoxal fluorescence recovered more slowly with a biphasic course. The independent return of these properties and the hysteretic behavior indicate that subunit separation is followed by a conformational drift like that observed in lactate dehydrogenase dissociated by either pressure or temperature or in enolase dissociated by dilution.     

Association-dissociation of histone oligomers. A spin label study

The spin label method has been used to obtain information about conformational changes of histone oligomers taking advantage of the fact that at a low ionic strength and in the presence of other histones about 45% of cysteine residues of histone H3 react with the 3-maleimido-2,2,5,5-tetramethyl-1-pyrrolidinyloxyl spin label. For the labeled complexes H3-H4 and H nu the degree of immobilization of the spin label is a function of the ionic strength. This variation is identical for both complexes within a long range of ionic strengths, including the interval of 0.8-2 M NaCl, under which conditions interactions are known to exist between the tetramer (H3)2 (H4)2 and the dimer (H2A) (H2B). This finding suggests a negligible influence of the dimer for modifying the cysteine residue environment of histone H3 on octamer formation. GuHCl treatment at high ionic strength of the labeled complexes gives rise to a non-lineal increase in the degree of mobility of the spin label. This increase, at low GuHCl concentration (0-0.5 M GuHCl), is interpreted as showing a lowering in rigidity for the Cys residue environment, without affecting the general stability of the tetramer (H3)2 (H4)2. At higher GuHCl concentration (2-3 M GuHCl) the increase in the spin label mobility is related to a dissociation of the complexes in single histones. Our results are consistent with the view that the overall structure of the tetramer, as well as its conformational changes during complex structuration or denaturation, are not strongly affected by the presence of the dimer (H2A) (H2B).