Effects of pH on low-salt transition of chromatin core particles

Effect of chromatin structure on quantitative ultrasound parameters

High-frequency ultrasound (~20 MHz) techniques were investigated using in vitro and ex vivo models to determine whether alterations in chromatin structure are responsible for ultrasound backscatter changes in biological samples. Acute myeloid leukemia (AML) cells and their isolated nuclei were exposed to various chromatin altering treatments. These included 10 different ionic environments, DNA cleaving and unfolding agents, as well as DNA condensing agents. Raw radiofrequency (RF) data was used to generate quantitative ultrasound parameters from spectral and form factor analyses. Chromatin structure was evaluated using electron microscopy. Results indicated that trends in quantitative ultrasound parameters mirrored trends in biophysical chromatin structure parameters. In general, higher ordered states of chromatin compaction resulted in increases to ultrasound paramaters of midband fit, spectral intercept, and estimated scatterer concentration, while samples with decondensed forms of chromatin followed an opposite trend. Experiments with isolated nuclei demonstrated that chromatin changes alone were sufficient to account for these observations. Experiments with ex vivo samples indicated similar effects of chromatin structure changes. The results obtained in this research provide a mechanistic explanation for ultrasound investigations studying scattering from cells and tissues undergoing biological processes affecting chromatin.

Global analysis of the ground-state wrapping conformation of a charged polymer on an oppositely charged nano-sphere

We investigate the wrapping conformations of a single, strongly adsorbed polymer chain on an oppositely charged nano-sphere by employing a reduced (dimensionless) representation of a primitive chain-sphere model. This enables us to determine the global behavior of the chain conformation in a wide range of values for the system parameters including the chain contour length, its linear charge density and persistence length as well as the nano-sphere charge and radius, and also the salt concentration in the bathing solution. The structural behavior of a charged chain-sphere complex can be described in terms of a few distinct conformational symmetry classes separated by continuous or discontinuous transition lines which are determined by means of appropriately defined (order) parameters. Our results can be applied to a wide class of strongly coupled polymer-sphere complexes including, for instance, complexes that comprise a mechanically flexible or semiflexible polymer chain or an extremely short or long chain and, as a special case, include the biologically relevant example of DNA-histone complexes.

Charge state of the globular histone core controls stability of the nucleosome

Presented here is a quantitative model of the wrapping and unwrapping of the DNA around the histone core of the nucleosome that suggests a mechanism by which this transition can be controlled: alteration of the charge state of the globular histone core. The mechanism is relevant to several classes of posttranslational modifications such as histone acetylation and phosphorylation; several specific scenarios consistent with recent in vivo experiments are considered. The model integrates a description based on an idealized geometry with one based on the atomistic structure of the nucleosome, and the model consistently accounts for both the electrostatic and nonelectrostatic contributions to the nucleosome free energy. Under physiological conditions, isolated nucleosomes are predicted to be very stable (38 +/- 7 kcal/mol). However, a decrease in the charge of the globular histone core by one unit charge, for example due to acetylation of a single lysine residue, can lead to a significant decrease in the strength of association with its DNA. In contrast to the globular histone core, comparable changes in the charge state of the histone tail regions have relatively little effect on the nucleosome's stability. The combination of high stability and sensitivity explains how the nucleosome is able to satisfy the seemingly contradictory requirements for thermodynamic stability while allowing quick access to its DNA informational content when needed by specific cellular processes such as transcription.

Chromatin stability at low concentration depends on histone octamer saturation levels

Studies on the stability of nucleosome core particles as a function of concentration have indicated a lower limit of approximately 5 ng/microL, below which the complexes start to spontaneously destabilize. Until recently little information was available on the effect of low concentration on chromatin. Using the well-characterized array of tandemly repeated 5S rDNA reconstituted into chromatin, we have investigated the effect of dilution. In this study, we demonstrate that the stability of saturated nucleosomal arrays and that of nucleosome core particles are within the same order of magnitude, and no significant loss of histones is monitored down to a concentration of 2.5 ng/microL. We observed that levels of subsaturation of the nucleosomal arrays were directly correlated with an increased sensitivity to histone loss, suggesting a shielding effect. The loss of histones from our linear nucleosomal arrays was shown not to be random, with a significant likelihood to occur at the end of the template than toward the center. This observation indicates that centrally located nucleosomes are more stable than those close to the end of the DNA templates. Itis important to take this information into account for the proper design of experiments pertaining to histone composition and the folding ability of chromatin samples.

Complexes of semiflexible polyelectrolytes and charged spheres as models for salt-modulated nucleosomal structures

We investigate the complexation behavior between a semiflexible charged polymer and an oppositely charged sphere with parameters appropriate for the DNA-histone system. We determine the ground state of a simple free energy expression (which includes electrostatic interactions on a linear level) numerically and use symmetry arguments to divide the obtained DNA configuration into broad classes, thereby obtaining global phase diagrams. We pay specific attention to the effects of salt concentration, DNA length variation, DNA charge renormalization, and externally applied force on the obtained complex structures.

Influence of nucleosome structure on the three-dimensional folding of idealized minichromosomes

BACKGROUND

The closed circular, multinucleosome-bound DNA comprising a minichromosome provides one of the best known examples of chromatin organization beyond the wrapping of the double helix around the core of histone proteins. This higher level of chain folding is governed by the topology of the constituent nucleosomes and the spatial disposition of the intervening protein-free DNA linkers.

RESULTS

By simplifying the protein-DNA assembly to an alternating sequence of virtual bonds, the organization of a string of nucleosomes on the minichromosome can be treated by analogy to conventional chemical depictions of macromolecular folding in terms of the bond lengths, valence angles, and torsions of the chain. If the nucleosomes are evenly spaced and the linkers are sufficiently short, regular minichromosome structures can be identified from analytical expressions that relate the lengths and angles formed by the virtual bonds spanning the nucleosome-linker repeating units to the pitch and radius of the organized quaternary structures that they produce.

CONCLUSIONS

The resulting models with 4-24 bound nucleosomes illustrate how a minichromosome can adopt the low-writhe folding motifs deduced from biochemical studies, and account for published images of the 30 nm chromatin fiber and the simian virus 40 (SV40) nucleohistone core. The marked sensitivity of global folding to the degree of protein-DNA interactions and the assumed nucleosomal shape suggest potential mechanisms for chromosome rearrangements upon histone modification.

Nucleosome structural transition during chromatin unfolding is caused by conformational changes in nucleosomal DNA

We have recently reported that certain core histone-DNA contacts are altered in nucleosomes during chromatin unfolding (Usachenko, S. I., Gavin I. M., and Bavykin, S. G. (1996) J. Biol. Chem. 271, 3831-3836). In this work, we demonstrate that these alterations are caused by a conformational change in the nucleosomal DNA. Using zero-length protein-DNA cross-linking, we have mapped histone-DNA contacts in isolated core particles at ionic conditions affecting DNA stiffness, which may change the nucleosomal DNA conformation. We found that the alterations in histone-DNA contacts induced by an increase in DNA stiffness in isolated core particles are identical to those observed in nucleosomes during chromatin unfolding. The change in the pattern of micrococcal nuclease digestion of linker histone-depleted chromatin at ionic conditions affecting chromatin compaction also suggests that the stretching of the linker DNA may alter the nucleosomal DNA conformation, resulting in a structural transition in the nucleosome which may play a role in rendering the nucleosome competent for transcription and/or replication.

Mechanisms of stabilizing nucleosome structure. Study of dissociation of histone octamer from DNA

The influence of ionic strength on DNA-histone and histone-histone interactions in reconstituted nucleosomes was studied by measuring the parameters of histone tyrosine fluorescence: fluorescence intensity and lambda(max) position. The first parameter is sensitive to histone-DNA interactions. The changes of the second one accrue due to hydrogen bond formation/disruption between tyrosines in the histone H2A-H2B dimer and the (H3-H4)2 tetramer. The simultaneous measurement of these parameters permits the recording of both the dissociation of histone complexes from DNA, as well as changes in histone-histone interactions. As ionic strength is increased, the H2A-H2B histone dimer dissociated first, followed by dissociation of the (H3-H4)2 tetramer [Yager, T.G., McMurray, C.T. and Van Holde, K.E. (1989) Biochemistry 28, 2271-2276]. The H2A-H2B dimer is dissociated in two stages: first, the ionic bonds with DNA were disrupted, followed by the dissociation of the histone dimer from the tetramer. And secondly, the disruption of dimer-tetramer specific H-bonds. It was established that the energy of electrostatic interactions of the histone dimer with DNA within the nucleosome is much less than the energy of interaction of the histone dimer with the tetramer.

Scanning force microscopy reveals ellipsoid shape of chicken erythrocyte nucleosomes

Scanning force microscopy was used to investigate the conformation of hypotonic spread chicken erythrocyte nucleosomes. Nucleosomal chains were prepared in low-salt conditions and fixed before centrifugation onto glass coverslips and air drying. The images of single nucleosomes were isolated by image processing, and the height and geometry of the resulting three-dimensional structures were investigated. An average nucleosome height of 4.2 +/- 1.1 nm was determined. A virtual cross section at half-maximum height of the nucleosome structure was used for a characterization of the nucleosome geometry. The shape of this cross section was best described by an ellipse with an aspect ratio (major/minor axis) of approximately 1.30.

Structural states of the nucleosome

The nucleosome is the fundamental component of the eukaryotic chromosome, participating in the packaging of DNA and in the regulation of gene expression. Its numerous interactions imply a structural dynamism. Previous biophysical studies under limited sets of conditions have not been able to reconcile structural differences and transitions observed. We have determined a series of nucleosome conformations over a >10,000-fold range in salt concentration using a combination of biochemical methods, spectroscopic electron microscopy, and three-dimensional reconstruction techniques for randomly oriented single particles. This study indicates several ionic strength-dependent nucleosome conformations and also reconciles the differences between currently existing divergent models for the nucleosome. At low ionic environments, the particle appears highly elongated, becoming more compact and prolate ellipsoidal as ionic strength is increased to 10 mm NaCl. At 30 mM NaCl, the particle exhibits a spheroidal conformation. As ionic strength is increased to 150 mM NaCl, the nucleosome conformation changes and becomes oblate. Above 450 mM NaCl, the structure becomes highly elongated again. The result of this study is a unifying concept in which the three-dimensional structure of the nucleosome is inferred to be dynamic in response to ionic interactions and in accord with biochemical and genetic studies.

Dynamics of interaction of RNA polymerase II with nucleosomes. I. Effect of salts

Mononucleosomes were labeled with the sulfhydryl-specific fluorescence probe 1,5-IAEDANS (5-(2-((iodoacetyl)amino)ethyl)amino-naphthalene-1-sulfonic acid) by attaching the dye to the single cysteine of H3 through a covalent linkage. The enzyme RNA polymerase II (pol II) utilized the native and the reconstituted fluorescent nucleosomes as templates with greatest efficiency when 0.2 M potassium acetate (AcOK) was used as the supporting salt; 0.2 M NaCl was found to be very much inhibitory. Measurement of polarity of the microenvironment of the dye at its binding site in the nucleosome showed the conformation to be more open in the presence of AcOK, compared to that in 0.1 or 0.2 M NaCl. The binding of pol II to the nucleosome resulted in a relatively more compact structure when measured in terms of the polarity of the microenvironment of the dye in various salt-dependent conformations of the nucleosomes. Time-resolved fluorescence spectroscopy showed that the probe molecule at its binding site undergoes certain excited-state processes, and the presence/absence or rate of these excited-state processes depends on the conformation of nucleosomes, which in turn depends on the type and concentration of the ion present in the medium. Time-resolved emission spectra showed that binding of nucleosomes by pol II established some new contacts that resulted in inaccessibility of the dye to the bulk solvent, reflecting a more hydrophobic environment for the dye in the steady-state spectra. Thus, binding or transcription of nucleosomes by pol II did not break open their structure. Rather, some transient internal adjustments within the histone octamer may take place to accommodate the bulky pol II molecule.

Conformational characterization of nucleosomes by principal component analysis of their electron micrographs

Optimized fixation conditions were determined for protein-protein and protein-DNA crosslinking within calf-thymus nucleosomes in low monovalent salt concentrations. Nucleosomes were examined without heavy-atom staining by darkfield electron microscopy. The dimensions of these macromolecular complexes and those of HeLa core particles optimally fixed in divalent salt were analysed using principal component analysis. According to this analysis the structure of the calf-thymus nucleosomes was best presented by a prolate ellipsoid. Particle images had average major and minor axis lengths of 14.1 and 10.5 nm, respectively. In contrast, the HeLa nucleosomes were best modelled by an oblate ellipsoid from the analysis of their images, which had average major and minor axes of 13.3 and 11.5 nm. The applicability of this multivariate statistical analysis to the interpretation of macromolecular images is illustrated and discussed.

The structure and dynamics of H1-depleted chromatin

The size of DNA involved in the interaction with a histone octamer in H1-depleted chromatin was re-examined. We compared the thermal untwisting of chromatin DNA and naked DNA using CD and electrophoretic topoisomer analysis, and found that DNA of 175 +/- 10 base pairs (bp) in length interacted with the histone core under physiological conditions. The decrease of ionic strength below 20 mM NaCl reduced this length down to 145 bp: apparently, an extra 30 bp DNA dissociated from the histone core to yield well-known 145-bp core particle. Histone cores partly dissociate within the temperature range of 25 to 40 degrees C. Quantitative analysis of histone thermal dissociation from DNA shows that the size of DNA protected against thermal untwisting would be significantly overestimated if this effect is neglected. The results presented in this paper also suggest that the dimers (H2A, H2B) act as a lock, which prevents transmission of conformational alterations from a linker to nucleosome core DNA. The histone core dissociation as well as (H2A, H2B) dimer displacement are discussed in the light of their possible participation in the eukaryotic genome activation.

An analysis of transcription factor TFIIIA-mediated DNA supercoiling

We have analyzed transcription factor-mediated DNA supercoiling catalyzed by the Xenopus oocyte extract (S-150). Under conditions that inhibit endogenous supercoiling activity (2 mM EDTA), the 5S RNA specific transcription factor, TFIIIA, promotes a negative change in DNA linking number. The SV40 binding protein, T antigen, appears not to promote DNA supercoiling under these conditions. A nucleosomal ladder can be seen after DNase I digestions only if the DNA template is pre-bound by TFIIIA prior to the addition of the S-150 extract. These studies suggest that TFIIIA may stimulate DNA supercoiling by enhancing the development of protein-DNA interactions via a mechanism that may include nucleosome assembly.

Nucleosome assembly of simian virus 40 DNA in a mammalian cell extract

We report here a mammalian cell-free system that can support chromatin assembly. Effective nucleosome assembly in HeLa cell extracts occurred at 125 to 200 mM KCl or potassium glutamate. At this physiological K+ ion concentration, two types of chromatin assembly were observed. The first was interfered with by Mg2+. Other cations such as Mn2+, Ca2+, Fe3+, and spermidine also inhibited this type of nucleosome assembly. The second type of assembly occurred in the presence of Mg2+ and at least equimolar ATP. However, even in the presence of ATP, excess Mg2+ inhibited assembly and promoted catenation of DNA; these effects could be circumvented by excess ATP, GTP, EDTA, or polyglutamic acid. The critical DNA concentration for optimum assembly in both pathways suggested a stoichiometric association of histones with DNA. The spacing of nucleosomes formed by both types of assembly on linear and circular DNA was reasonably regular, but chromatin assembled in the presence of ATP and Mg2+ was more stable.

Nucleosome assembly of simian virus 40 DNA in a mammalian cell extract

We report here a mammalian cell-free system that can support chromatin assembly. Effective nucleosome assembly in HeLa cell extracts occurred at 125 to 200 mM KCl or potassium glutamate. At this physiological K+ ion concentration, two types of chromatin assembly were observed. The first was interfered with by Mg2+. Other cations such as Mn2+, Ca2+, Fe3+, and spermidine also inhibited this type of nucleosome assembly. The second type of assembly occurred in the presence of Mg2+ and at least equimolar ATP. However, even in the presence of ATP, excess Mg2+ inhibited assembly and promoted catenation of DNA; these effects could be circumvented by excess ATP, GTP, EDTA, or polyglutamic acid. The critical DNA concentration for optimum assembly in both pathways suggested a stoichiometric association of histones with DNA. The spacing of nucleosomes formed by both types of assembly on linear and circular DNA was reasonably regular, but chromatin assembled in the presence of ATP and Mg2+ was more stable.

Effect of nucleosome distortion on the linking deficiency in relaxed minichromosomes

The wrapping of closed circular DNA on a protein surface, followed by relaxation with a topoisomerase and removal of proteins, produces a characteristic DNA linking deficiency, delta Lk. We show that the magnitude of delta Lk depends upon the surface shape, and we calculate changes in delta Lk caused by particular distortions of the protein wrapping surface. If the DNA remains attached to the surface during distortion, the DNA winding number, phi, is not altered. The change in delta Lk is then equal to the change in the surface linking number, SLk, which is a straightforward measure of the wrapping of the DNA around the surface. For left-handed wrapping, as in a nucleosome, SLk = -n, the number of times that the DNA axis winds around the axis of the protein complex. We calculate values of SLk for the helical wrapping of a constant length of DNA on protein surfaces having the shapes of cylinders and of ellipsoids and hyperboloids of revolution. If the equatorial radius of the protein is fixed, change in shape from a cylinder to a hyperboloid increases SLk, while the corresponding change to an ellipsoid reduces SLk. We apply the general results to the interpretation of experiments in which minichromosomes are relaxed with topoisomerase at various temperatures and delta Lk is determined. The result is that a distortion of the nucleosome core by at most 5% (the change in the radius at the axial extremity relative to the equator) is sufficient to explain the observed delta Lk changes.

Histone hyperacetylation. Its effects on nucleosome core particle transitions

Effects of histone hyperacetylation on transitions of HeLa cell nucleosome core particles were studied. The transitions examined were induced by low salt concentrations, pH, temperature, and nondissociating high salt. Effects of salt dissociation were also examined. The low-salt transition was found to shift to higher ionic strength by approximately three fold for hyperacetylated particles, a change which may be due simply to the increased overall negative charge on the particles caused by acetylation of lysine residues. Some differences were also seen in the way in which core particles refold after exposure to very low salt (which induces a nonreversible change in the particles). Otherwise no significant effects of hyperacetylation were observed.

Reversibility of the low-salt transition of chromatin core particles

The low-salt transition of chromatin core particles is reversible if the monovalent cation concentration is kept above 0.2 mM. Exposure of the particles to salt concentrations below this value results in a nonreversible secondary transition. The nonreversible changes are relatively slow with a half-time of about 15 minutes. Once exposed to such low ionic strength, the particles then begin to refold with increasing salt in at least two steps over a much higher ionic strength range than is required for the usual low-salt transition. The refolding is very fast, with a half-time less than a minute. Small differences between particles which had or had not been exposed to very low salt persist even when the particles are returned to near physiological ionic strengths.

Spectroscopic studies on histone-DNA interactions. II. Three transitions in nucleosomes resolved by salt-titration

The multiple-step transitions in DNA-histone interactions in chicken erythrocyte nucleosomes with increasing ionic strength are resolved by salt-titration spectroscopy. Both the circular dichroism of the DNA and the fluorescence of the histones in nucleosomes change during the titration process with concentrations of NaCl from 0.1 M to 2.5 M. By differentiating the titration curves, three distinct peaks corresponding to three structural transitions are observed. The two peaks near 0.95 M and 1.45 M-NaCl are common to the circular dichroism and fluorescence curves. The circular dichroism curve has another peak near 0.55 M-NaCl. Because the derivative of the fluorescence titration curve for the DNA-(H3, H4) complex has only one peak near 1.45 M-NaCl, that peak is attributed to the dissociation of the histone dimer (H3, H4). The peak near 0.95 M-NaCl corresponds to the dissociation of the dimer (H2A, H2B) from the DNA-(H3, H4) complex, as shown by binding experiments of (H2A, H2B) to the DNA-(H3, H4) complex at the salt concentration near this peak. The peak near 0.55 M-NaCl reflects some inner-core structural change. As the change of the circular dichroism signal is reversible, salt-titration spectroscopy is applicable to equilibrium studies of the physical chemical properties of DNA-histone interactions. By the assumption of a non-co-operative model, the binding constant for the chicken erythrocyte (H2A, H2B) dimer to the DNA-(H3, H4) complex is calculated as 2.8 X 10(6) M-1 at 1.0 M-NaCl (20 degrees C, pH 7.6). The DNA sequence dependence of the stability of the DNA-(H3, H4) interaction is observed in the salt-titration profiles of reconstituted material. Decreasing stability of the interaction of (H3, H4) is observed following the order: poly[(dG)-(dC)] much greater than chicken erythrocyte DNA greater than poly[(dA)-(dT)]. It is concluded that histones (H3, H4) have a different DNA sequence dependence from histones (H2A, H2B).

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

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

The intrinsic tyrosine fluorescence of histone H1. Steady state and fluorescence decay studies reveal heterogeneous emission

In wavelength-resolved steady state spectra we observe three different kinds of emission from histone H1, a class A protein with only a single tyrosine residue. Unfolded H1 emissions that peak at approximately 300 and 340 nm can both be excited maximally at approximately 280 nm. Another, peaking much further to the red at approximately 400 nm, can be excited maximally at approximately 320 nm. The 300-nm fluorescence can be resolved by lifetime measurements into three components with decay times of approximately 1, 2, and 4 ns. On sodium-chloride-induced refolding of H1, simplification of the emission properties occurs. The 340 and 400-nm components disappear while the two shorter lifetime components of the 300-nm band diminish in amplitude and are replaced by the 4-ns decay. We believe that the 340-nm emission is tyrosinate fluorescence resulting from excited-state proton transfer. The origin of the 400-nm emission remains uncertain. We assign the 1 and 2-ns components of the 300-nm emission to two states of tyrosine in denatured H1 and the 4-ns decay to fluorescence of the single tyrosine residue in the globular region of refolded H1. Our results support the contention that salt induced folding of H1 is a cooperative two state process, and permit us to better understand the previously reported increases in fluorescence intensity and anisotropy on salt-induced folding.

Effects of pH on the stability of chromatin core particles

Chromatin core particles near physiological ionic strength undergo a reversible transition induced by changes in pH near neutrality. While sedimentation studies indicate no significant effect on size or shape, changes in tyrosine fluorescence anisotropy and in circular dichroism suggest a somewhat looser structure at high pH. Further support of this suggestion is given by high salt dissociation experiments; at pH 8 core particles begin to show changes at lower salt concentration than at pH 6. The pH transition appears unaffected by the presence of Mg2+ but can be blocked by crosslinking of the histones. A possible relationship is suggested between this transition and increases in intracellular pH which correlate with enhancement in several aspects of cellular activity including DNA replication.

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.