Light scattering measurements supporting helical structures for chromatin in solution

Radiation-induced conformational changes in chromatin structure in resting human peripheral blood mononuclear cells

Abstract Background: Ionizing radiation induces a plethora of DNA damage including double-strand breaks (DSB) that may trigger a series of events such as transcription, DNA repair and alteration in the conformation of chromatin structure in human cells. We have made an attempt to study the conformational changes in chromatin fibers in irradiated human peripheral blood mononuclear cells (PBMC) using Dynamic Light Scattering (DLS) as a new tool.

MATERIALS AND METHODS

Venous blood samples were collected from 10 random, healthy individuals with written informed consent, approved by institutional ethics committee. PBMC were separated from blood, irradiated with different doses of gamma radiation from 0.25-1.0 Gy. Native chromatin was isolated from irradiated PBMC and changes in the hydrodynamic diameter of the chromatin fiber were measured using DLS. Both dose response and time kinetics was studied in order to see the chromatin changes. Radiation-induced DNA double-strand breaks were measured using gamma-H2AX (histone 2A member X) as a biomarker using flow cytometry and foci were visualized in confocal microscopy.

RESULTS

A significant alteration in hydrodynamic diameter of the chromatin fiber was observed at lower doses (0.25 and 0.50 Gy), whereas at higher dose (1.0 Gy), the size of the chromatin fiber was comparable to unirradiated control. Among the 10 individuals studied, five individuals showed significant increase (p ≤ 0.002) in hydrodynamic size at 0.25 Gy whereas four individuals showed significant decrease (p ≤ 0.009) at 0.25 Gy. One individual did not show any significant difference as compared to control. However, dose-dependent increase in gamma-H2AX fluorescence signals as well as foci number was observed. Increased fragmentation of chromatin fiber was also observed using Atomic Force Microscopy at higher doses.

CONCLUSION

Radiation-induced DNA damage response can lead to individual specific conformational changes in chromatin structure at lower doses (0.25 Gy and 0.50 Gy) which can be detected using dynamic light scattering method in resting human PBMC.

Nanoscale squeezing in elastomeric nanochannels for single chromatin linearization

This paper describes a novel nanofluidic phenomenon where untethered DNA and chromatin are linearized by rapidly narrowing an elastomeric nanochannel filled with solutions of the biopolymers. This nanoscale squeezing procedure generates hydrodynamic flows while also confining the biopolymers into smaller and smaller volumes. The unique features of this technique enable full linearization then trapping of biopolymers such as DNA. The versatility of the method is also demonstrated by analysis of chromatin stretchability and mapping of histone states using single strands of chromatin.

Computer simulation of the 30-nanometer chromatin fiber

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

Three-dimensional structure of extended chromatin fibers as revealed by tapping-mode scanning force microscopy

Unfixed chicken erythrocyte chromatin fibers in very low salt have been imaged with a scanning force microscope operating in the tapping mode in air at ambient humidity. These images reveal a three-dimensional organization of the fibers. The planar "zig-zag" conformation is rare, and extended "beads-on-a-string" fibers are seen only in chromatin depleted of histones H1 and H5. Glutaraldehyde fixation reveals very similar structures. Fibers fixed in 10 mM salt appear somewhat more compacted. These results, when compared with modeling studies, suggest that chromatin fibers may exist as irregular three-dimensional arrays of nucleosomes even at low ionic strength.

Electrostatic mechanism of chromatin folding

We describe a theoretical analysis of cation binding in the nucleosome, and in chromatin as it folds, using Manning's polyelectrolyte theory. The theory accounts remarkably well, even quantitatively, both for the interaction of histone charges with DNA in chromatin, and for the essential features of the folding process. The degree of chromatin folding under different ion conditions is reliably predicted by the electrostatic free energy of DNA in the H1 binding site, which determines repulsions between linker DNA segments thus limiting how closely they may approach. The electrostatic free energy is a function of the ionic strength and the residual (unneutralized) DNA charge. Monovalent cations effect chromatin folding primarily by screening the residual charge whilst divalent or trivalent cations bind to DNA reducing its residual charge. The binding of H1 to the linker DNA considerably reduces its electrostatic free energy by displacing bound cations and reducing the residual charge. Thus, native chromatin folds at lower salt concentrations than does H1-depleted chromatin. We conclude that the mechanism of chromatin folding is primarily electrostatic in nature. In vivo ion conditions are such that chromatin is compact but H1 molecules are able to exchange freely, probably due to a low degree of salt-induced dissociation. When H1 molecules exchange, transient local disruptions may occur in the chromatin filament due to repulsion of temporarily H1-free linker DNA from within the filament, such that chromatin "breathes". Thus, the cell can maintain its chromatin in a compact form and access to DNA for sequence-specific DNA-binding proteins and the transcription machinery is still possible.

NaCl-induced chromatin condensation. Application of static light scattering at 90 degrees and stopped flow technique

We have studied the NaCl-induced condensation of calf thymus chromatin by static light scattering of 90 degrees and shown that the increase in NaCl concentration up to 120-170 mM results in a large increase in scattering intensity of the total chromatin. Histones H1-depleted and trypsinized chromatin preparations do not reveal such a large increase in scattering intensity. The increase in the scattering intensity reflects the folding of the chromatin filaments, but not their aggregation. We have used this effect to monitor the kinetics of the chromatin condensation in response to a jump to higher NaCl concentrations by means of a stopped-flow technique. The results show that the condensation is a fast complex process consisting of at least two steps. The first step is only partially resolved by the stopped-flow apparatus. The second step has a time constant in the range of 20-50 ms, which does not depend on chromatin concentration.

Chromatin higher-order structure studied by neutron scattering and scanning transmission electron microscopy

Neutron scattering in solution and scanning transmission electron microscopy were simultaneously done on chicken erythrocyte chromatin at various salt and magnesium concentrations. We show that chromatin is organized into a higher-order structure even at low ionic strength and that the mass per unit length increases continuously as a function of salt concentration, reaching a limiting value of between six and seven nucleosomes per 11 nm. There is no evidence of a transition from a 10-nm to a 30-nm fiber. Fiber diameter is correlated with mass per unit length, showing that both increase during condensation. We also find that there is no essential difference between the mass per unit length measured by scanning transmission electron microscopy and neutron scattering in solution, showing that the ordered regions seen in micrographs are representative of chromatin in solution.

Influence of DNA-binding drugs on chromatin condensation

We have used transient electric dichroism to study the ability of DNA-binding drugs to affect the folding of chromatin from the 10- to the 30-nm fiber, either by themselves or in conjunction with multivalent cations. Variables considered include the cationic charge of the drug, the comparative influence of intercalation and groove binding as modes of interaction, and the effect of bis-intercalation compared to mono-intercalation. In parallel with our findings with other cations, we observe that a drug must have a charge of 3+ or greater in order to condense chromatin at concentrations substantially lower than the concentration of chromatin, measured in base pairs. Drugs of low charge, whether groove binders or mono-or bis-intercalators, are unable to condense chromatin on their own. Bis-intercalators of high charge, however, are extremely efficient condensers, being able to cross-link chromatin with greater efficiency than polyamines of corresponding charge. When Mg2+ is used in combination with bis-intercalators of high charge, the order of addition of the two determines whether compaction or cross-linking is favored. Finally, the antibiotics actinomycin D, daunomycin, and distamycin, despite varied modes of binding to DNA, all inhibit the compaction of chromatin beyond a critical point in a remarkably similar manner.

Condensation of chromatin: role of multivalent cations

We have used electric dichroism to investigate the influence of multivalent cations upon the compaction of chicken erythrocyte chromatin from the unfolded, 10-nm fiber to the 30-nm solenoid and subsequent aggregation. The pattern of condensation, which consists of compaction plus aggregation, is found to be strikingly similar for a variety of cations of differing charge, including the physiologically important polyamines spermine and spermidine. With a few exceptions such as Cu2+ and Gd3+, an optimally compacted fiber with reproducible hydrodynamic properties is produced prior to the onset of aggregation. We report the concentrations of di-, tri-, and tetravalent cations required for optimal condensation; in addition, for tri- and tetravalent cations, we were able to estimate the extent of charge neutralization produced by their binding to the optimally compacted fiber. The results show that the multivalent ion concentration required for optimal compaction decreases as cationic charge increases. In addition, the effect of a mixture of dilute mono- and multivalent cations on chromatin condensation is synergistic, rather than competitive as has been found for the multivalent cation induced condensation of DNA or the B----Z conformational transition. A simple calculation indicates that the entropy of ion uptake in chromatin condensation is surprisingly constant for a range of ionic conditions; this factor may be a dominant one in determining the folding equilibrium.

Salt-dependent co-operative interaction of histone H1 with linear DNA

The nature of the complexes formed between histone H1 and linear double-stranded DNA is dependent on ionic strength and on the H1 : DNA ratio. At an input ratio of less than about 60% (w/w) H1 : DNA, there is a sharp transition from non-co-operative to co-operative binding at a critical salt concentration that depends on the DNA size and is in the range 20 to 50 mM-NaCl. Above this critical ionic strength the H1 binds to only some of the DNA molecules leaving the rest free, as shown by sedimentation analysis. The ionic strength range over which this change in behaviour occurs is also that over which chromatin folding is induced. Above the salt concentration required for co-operative binding of H1 to DNA, but not below it, H1 molecules are in close proximity as shown by the formation of H1 polymers upon chemical cross-linking. The change in binding mode is not driven by the folding of the globular domain of H1, since this is already folded at low salt in the presence of DNA, as indicated by its resistance to tryptic digestion. The H1-DNA complexes at low salt, where H1 is bound distributively to all DNA molecules, contain thickened regions about 6 nm across interspersed with free DNA, as shown by electron microscopy. The complexes formed at higher salt through co-operative interactions are rods of relatively uniform width (11 to 15 nm) whose length is about 1.6 times shorter than that of the input DNA, or are circular if the DNA is long enough. They contain approximately 70% (w/w) H1 : DNA and several DNA molecules. These thick complexes can also be formed at low salt (15 mM-NaCl) when the H1 : DNA input ratio is sufficiently high (approximately 70%).

Chromatin fibers are left-handed double helices with diameter and mass per unit length that depend on linker length

Four classes of models have been proposed for the internal structure of eukaryotic chromosome fibers--the solenoid, twisted-ribbon, crossed-linker, and superbead models. We have collected electron image and x-ray scattering data from nuclei, and isolated chromatin fibers of seven different tissues to distinguish between these models. The fiber diameters are related to the linker lengths by the equation: D(N) = 19.3 + 0.23 N, where D(N) is the external diameter (nm) and N is the linker length (base pairs). The number of nucleosomes per unit length of the fibers is also related to linker length. Detailed studies were done on the highly regular chromatin from erythrocytes of Necturus (mud puppy) and sperm of Thyone (sea cucumber). Necturus chromatin fibers (N = 48 bp) have diameters of 31 nm and have 7.5 +/- 1 nucleosomes per 10 nm along the axis. Thyone chromatin fibers (N = 87 bp) have diameters of 39 nm and have 12 +/- 2 nucleosomes per 10 nm along the axis. Fourier transforms of electron micrographs of Necturus fibers showed left-handed helical symmetry with a pitch of 25.8 +/- 0.8 nm and pitch angle of 32 +/- 3 degrees, consistent with a double helix. Comparable conclusions were drawn from the Thyone data. The data do not support the solenoid, twisted-ribbon, or supranucleosomal particle models. The data do support two crossed-linker models having left-handed double-helical symmetry and conserved nucleosome interactions.

The superstructure of chromatin and its condensation mechanism. I. Synchrotron radiation X-ray scattering results

Synchroton radiation X-ray scattering experiments have been performed on chicken erythrocyte chromatin fibres over a wide range of ionic conditions and on various states of the fibres (i.e. "native" in solution, in gels and in whole nuclei; chromatin depleted of the H1 (H5) histones and chromatin with bound ethidium bromide). A correlation between the results obtained with the various chromatin preparations provides evidence for a model according to which at low ionic strength the chromatin fibre already possesses a helical superstructure, with a diameter comparable to that of condensed chromatin, held together by the H1(H5) histone. The most significant structural modification undergone upon an increase of the ionic strength is a reduction of the helix pitch, this leads to condensation in a manner similar to the folding of an accordion. The details of this process depend on whether monovalent or divalent cations are used to raise the ionic strength, the latter producing a much higher degree of condensation. Measurements of the relative increase of the mass per unit length indicate that the most condensed state is a helical structure with a pitch around 3.0-4.0 nm. In this paper we give a detailed presentation of the experimental evidence obtained from static and time-resolved scattering experiments, which led to this model.

Histone phosphorylation in native chromatin induces local structural changes as probed by electric birefringence

In order to understand how the phosphorylation of histones affects the chromatin structure, we used electron microscopy, sedimentation velocity, circular dichroism and electric birefringence to monitor the salt-induced filament reversible solenoid transition of phosphorylated and native chromatin. Phosphorylation in vitro of chicken erythrocyte chromatin by cyclic-AMP-dependent protein kinase from porcine heart led to the modification of the histones H3 and H5 only, which were modified at a level of one phosphate and about three phosphate groups per molecule, respectively. In contrast to circular dichroism and sedimentation studies, which tend to suggest that phosphorylation of H3 and H5 does not affect chromatin structure, electron microscopy reveals that phosphorylation causes a relaxation of structure at low ionic strength. Electric birefringence and relaxation time measurements clearly prove that local structural changes are induced in chromatin: we observe a decrease of the steady-state birefringence with the appearance of a negative contribution in the signal and a marked increase of the flexibility of fibres. The component with the negative birefringence presents very short relaxation times, like those exhibited by small DNA fragments or individual nucleosomes. Two possibilities are then suggested. First, the conformational change is consistent with what would be expected from the presence of DNA segments loosely associated with the core histone H3. That the length of such segments could correspond to about one to two base-pairs per nucleosome strongly suggests that phosphorylation induces changes affecting some specific H3-DNA interactions only. This result could corroborate previous observations indicating that the N-terminal region of H3, where the site of phosphorylation is located, plays a decisive role in maintaining the superstructure of chromatin. Second, phosphorylation could introduce hinge points between each nucleosome. In this case, the negative birefringence results from partial orientation of the swinging nucleosomes. A possible mode of action of phosphorylation might be to weaken structural restraints imposed by histone H3, thus facilitating further condensation of chromatin.

Scatter analysis of discrete-sized chromatin fragments favours a cylindrical organization

Fragments of chromatin containing 23 +/- 2.5 nucleosomes have been fractionated after light nuclease treatment of chicken erythrocyte nuclei. Low-angle scattering measures the total z-average radius of gyration of the already well-defined particles and the shape of scatter curves can be compared with three-dimensional analysis as opposed to cross-section analysis of long chromatin fragments. The data show that the particles are not spherical, have no detectable hole in the center of the structure and are best represented by a solid rod-like shape such as that generated by a coil of nucleosomes with the centre perhaps filled with linker DNA and histone H1/H5. 23 nucleosome fragments, where the DNA is partially fragmented, have near-identical scatter curves to the above-defined intact particles, indicating the primary importance of histone proteins in maintaining the integrity of the chromatin higher-order structure. Neutron scattering shows the radii of gyration to be contrast-independent, which fits in with the model calculations for solenoids. Particles with fragmented DNA and the intact particles, therefore, behave as sections of a solenoidal higher-order structure and possibly are observed as "superbeads' only during the folding and unfolding pathways of nucleosome multimers.

Condensation of the chromatin gel by cations

Calf thymus chromatin gel, containing strongly bound nonhistone proteins, was used to study the effect of easily removable and tightly bound cations on the condensation of chromatin. The chromatin volume was found to be linearly dependent on the reciprocal square root of the concentration of easily removable cations (Tris X H+ + Na+ and Mg2+) except for the initial stages of condensation (up to 7-10 mM monovalent and 0.15-0.2 mM divalent cations). The effect of Mg2+ at the initial stage of condensation was not reproduced by Na+ and vice versa. At higher concentrations the effects of Na+ and Mg2+ were additive. The removal of tightly bound divalent cations by a treatment of the chromatin gel with 1,10-phenanthroline led to an approx. 50% increase in the volume of the chromatin gel, which was maintained at each concentration of easily removable cations. The 1,10-phenanthroline-caused decondensation of the chromatin gel was reversed by Ca2+ but not by Mg2+, Zn2+ and Cu2+. The chromatin gel pretreated with Ca2+ was not further decondensed by 1,10-phenanthroline.

The effect of histone H1 on the compaction of oligonucleosomes. A quasielastic light scattering study

The structural properties of H1-depleted oligonucleosomes are investigated by the use of quasielastic laser light scattering, thermal denaturation and circular dichroism and compared to those of H1-containing oligomers. To obtain information on the role of histone H1 in compaction of nucleosomes, translational diffusion coefficients (D) are determined for mono-to octanucleosomes over a range of ionic strength. The linear dependences of D on the number of nucleosomes show that the conformation of stripped oligomers is very extended and does not change drastically with increasing the ionic strength while the rigidness of the chain decreases due to the folding of linker DNA. The results prove that the salt-induced condensation is much smaller for H1-depleted than for H1-containing oligomers and that histone H1 is necessary for the formation of a supercoiled structure of oligonucleosomes, already present at low ionic strength.

Higher order structure of chromatin: influence of ionic strength and proteolytic digestion on the birefringence properties of polynucleosomal fibers

Effects of ionic strength and proteolytic digestion on the conformation of chromatin fibers were studied by electric birefringence and relaxation measurements. The results confirm that at low ionic strength chromatin presents structural features reflecting those observed in the presence of cations. Soluble chromatin prepared from rat liver nuclei by brief nuclease digestion exhibits a positive birefringence. As the salt concentration is increased, the transition to a compact solenoidal structure is deduced from changes in electro-optical properties: the positive birefringence gradually decreases and the observed reduction in 40 mM NaCl is nearly 95%; the relaxation time decreases dramatically and the character of the kinetic changes since the decay of birefringence described initially by a spectrum of relaxation times becomes monoexponential. On digestion with proteases at low ionic strength we observe at first a rapid increase of the positive birefringence concomitant with an increase of the relaxation time. Then the birefringence decreases and becomes negative. Chromatin undergoes two successive transitions: the first transition is explained by a lengthening of nucleosomal chains without modification of the orientation of nucleosomes within the superstructure and the second one by the unwinding of the DNA tails and internucleosomal segments. When chromatin is digested at 30 mM NaCl we find a single unfolding transition characterized by the decrease of birefringence and a slight increase in the relaxation time. The results imply that the positive birefringence of chromatin does not depend on the presence of whole histone H1 and that a salt concentration of 30 mM NaCl is sufficient to modify the initial site or/and the effects of proteolytic attack.

The structural organization of oligonucleosomes

We have used electric birefringence to study the structure of oligonucleosomes and to show the influence of histone H1 depletion on their conformation in solution. Measurements are made at low ionic strength on monodisperse samples containing up to 8 nucleosomes. For each oligomer, having H1 or not, the analysis of both relaxation and orientation times gives information about the particle's orientation mechanism through the ratio r of permanent over induced dipole terms. For native oligomers, the data confirm the previous finding of a discontinuity in hydrodynamic behavior between pentamer and heptamer: the rotational times are multiplied by 10 and r increases from 0.2 to 0.7 showing the appearance of a non-negligible contribution of a permanent dipole to the orientation mechanism. We suggest a model for the hexanucleosome at low ionic strength and discuss its implications for the higher-order structure of chromatin. The treatment for H1 depletion abolishes the transitions in electro-optical properties: the value of r remains constant, r = 0.15, and both rotational times increase progressively with the number of nucleosomes in the chain. That reflects an important unfolding of oligonucleosomal structure which we attributed to the unwinding of DNA tails and internucleosomal segments. The disc planes of nucleosomes become closely parallel to the nucleosomal chain axis.

Transcriptionally active chromatin

Eukaryotic chromatin has a dynamic, complex hierarchical structure. Active gene transcription takes place on only a small proportion of it at a time. While many workers have tried to characterize active chromatin, we are still far from understanding all the biochemical, morphological and compositional features that distinguish it from inactive nuclear material. Active genes are apparently packaged in an altered nucleosome structure and are associated with domains of chromatin that are less condensed or more open than inactive domains. Active genes are more sensitive to nuclease digestions and probably contain specific nonhistone proteins which may establish and/or maintain the active state. Variant or modified histones as well as altered configurations or modifications of the DNA itself may likewise be involved. Practically nothing is known about the mechanisms that control these nuclear characteristics. However, controlled accessibility to regions of chromatin and specific sequences of DNA may be one of the primary regulatory mechanisms by which higher cells establish potentially active chromatin domains. Another control mechanism may be compartmentalization of active chromatin to certain regions within the nucleus, perhaps to the nuclear matrix. Topological constraints and DNA supercoiling may influence the active regions of chromatin and be involved in eukaryotic genomic functions. Further, the chromatin structure of various DNA regulatory sequences, such as promoters, terminators and enhancers, appears to partially regulate transcriptional activity.

Interaction of chromatin with NaCl and MgCl2. Solubility and binding studies, transition to and characterization of the higher-order structure

Chicken erythrocyte chromatin containing histones H1 and H5 was carefully separated into a number of well-characterized fractions. A distinction could be made between chromatin insoluble in NaCl above about 80 mM, and chromatin soluble at all NaCl concentrations. Both chromatin forms were indistinguishable electrophoretically and both underwent the transition from the low salt "10 nm" coil to the "30 nm" higher-order structure solenoid by either raising the MgCl2 concentration to about 0.3 mM or the NaCl concentration to about 75 mM. The transitions were examined in detail by elastic light-scattering procedures. It could be shown that the 10 nm form is a flexible coil. For the 30 nm solenoid, the assumption of a rigid cylindrical structure was in good agreement with 5.7 nucleosomes per helical turn. However, disagreement of calculated frictional parameters with values derived from quasielastic light-scattering and sedimentation introduced the possibility that the higher-order structure, under these conditions, is more extended, flexible, or perhaps a mixture of structures. Values for density and refractive index increments of chromatin are also given. To understand the interaction of chromatin with NaCl and with MgCl2, a number of experiments were undertaken to study solubility, precipitation, conformational transitions and binding of ions over a wide range of experimental conditions, including chromatin concentration.

The higher-order structure of chromatin: evidence for a helical ribbon arrangement

Both intact and nuclease-isolated chromatin fibers have been examined at different degrees of salt-induced compaction, using a variety of preparation techniques. The results suggest that the initial folding step in nucleosome packing involves the formation of a zig-zag ribbon as has been proposed by others (Thoma F., T. Koller, and A. Klug, 1979, J. Cell Biol., 83:403-427; Worcel A., S. Strogartz, and D. Riley, 1981, Proc. Natl. Acad. Sci. USA, 78:1461-1465), and that subsequent compaction occurs by coiling of the ribbon to form a double helical structure. This type of folding generates a fiber in which the nucleosome-nucleosome contacts established in the zig-zag ribbon are maintained and in which the histone H1 molecules occupy equivalent sites. The diameter of the fiber is not dependent upon the nucleosome repeat length. Direct mass values for individual isolated fibers obtained from electron scattering measurements showed that the mass per length was dependent on ionic strength, and ranged from 6.0 X 10(4) daltons/nm at 10 mM NaCl to 27 X 10(4) daltons/nm at 150 mM salt. These values are equivalent to 2.5 nucleosomes/11 nm at 10 mM NaCl and to 11.6 nucleosomes/11 nm at 150 mM salt and are consistent with the range of packing ratios for the proposed helical ribbon.

Differences of supranucleosomal organization in different kinds of chromatin: cell type-specific globular subunits containing different numbers of nucleosomes

Fractions of homogeneously-sized supranucleosomal particles can be obtained in high yield and purity from various types of cells by brief micrococcal nuclease digestion (10 or 20 s) of condensed chromatin in 100 mM NaCl followed by sucrose gradient centrifugation and agarose gel electrophoresis. These chromatin particles, which contain only DNA and histones, differed according to cell type. Sea urchin spermatozoa (Paracentrotus lividus) gave rise to heavy particles (ca. 260 S) with a mean diameter (48 nm). These resembled the unit chromatin fibrils fixed in situ, which contain an average of 48 nucleosomes, as determined both by electron microscopy after unraveling in low salt buffer and gel electrophoresis. In contrast, higher order particles from chicken erythrocyte chromatin were smaller (105 S; 36-nm diam) and contained approximately 20 nucleosomes. The smallest type of supranucleosomal particle was obtained from chicken and rat liver (39 S; 32-nm diam; eight nucleosomes). Oligomeric chains of such granular particles could be recognized in regions of higher sucrose density, indicating that distinct supranucleosomal particles of globular shape are not an artifact of exposure to low salt concentrations but can be obtained at near-physiological ionic strength. The demonstration of different particle sizes in chromatin from different types of nuclei is contrary to the view that such granular particles are produced by artificial breakdown into "detached turns" from a uniform and general solenoid structure of approximately six nucleosomes per turn. Our observations indicate that the higher order packing of the nucleosomal chain can differ greatly in different types of nuclei and the supranucleosomal organization of chromatin differs between cell types and is related to the specific state of cell differentiation.

Involvement of the globular domain of histone H1 in the higher order structures of chromatin

We have attacked H1-containing soluble chromatin by alpha-chymotrypsin under conditions where chromatin adopts different structures. Soluble rat liver chromatin fragments depleted of non-histone components were digested with alpha-chymotrypsin in NaCl concentrations between 0 mM and 500 mM, at pH 7, or at pH 10, or at pH 7 in the presence of 4 M-urea. alpha-Chymotrypsin cleaves purified rat liver histone H1 at a specific initial site (CT) located in the globular domain and produces an N-terminal half (CT-N) which contains most of the globular domain and the N-terminal tail, and a C-terminal half (CT-C) which contains the C-terminal tail and a small part of the globular domain. Since in sodium dodecyl sulfate/polyacrylamide-gel electrophoresis CT-C migrates between the core histones and H1, cleavage of chromatin-bound H1 by alpha-chymotrypsin can be easily monitored. The CT-C fragment was detected under conditions where chromatin fibers were unfolded or distorted: under conditions of H1 dissociation at 400 mM and 500 mM-NaCl (pH 7 and 10); at very low ionic strength where chromatin is unfolded into a filament with well-separated nucleosomes; at pH 10 independent of the ionic strength where chromatin never assumes higher order structures; in the presence of 4 M-urea (pH 7), again independent of the ionic strength. However, hardly any CT-C fragment was detected under conditions where fibers are observed in the electron microscope at pH 7 between 20 mM and 300 mM-NaCl. Under these conditions H1 is degraded by alpha-chymotrypsin into unstable fragments with a molecular weight higher than that of CT-C. Thus, the data show that there are at least two different modes of interaction of H1 in chromatin which correlate with the physical state of the chromatin. Since the condensation of chromatin into structurally organized fibers upon raising the ionic strength starts by internucleosomal contacts in the fiber axis (zig-zag-shaped fiber), where H1 appears to be localized, it is likely that in chromatin fibers the preferential cleavage site for alpha-chymotrypsin is protected because of H1-H1 contacts. The data suggest that the globular part of H1 is involved in these contacts close to the fiber axis. They appear to be hydrophobic and to be essential for the structural organization of the chromatin fibers.(ABSTRACT TRUNCATED AT 400 WORDS)

Eukaryotic genome: model considerations

The paper presents a new model of chromosome structure based on the assumption that multiple circular subunits of DNA exist. The essential difference with previously described models is the circular DNA unit forms a central chromosome axis. Chromosome configurations during various phases of the cell cycle depend on the various conformations of this central integrating unit. The described model can be generalized for all haploid set of eukaryotic nucleus. Some aspects of the chromosome structure and their functions have been discussed.

Salt-induced conformational transitions in chromatin. A flow linear dichroism study

The chromatin structure in solution has been studied by the flow linear dichroism method (LD) in a wide range of ionic strengths. It is found that increasing the ionic strength from 0.25 mM Na2EDTA, pH 7.0 to 100 mM NaCl leads to a strong reduction of the LD amplitude of chromatin and inversion of the LD sign from negative to positive at 2 mM NaCl. Chromatin exhibits a positive LD maximum value at 10-20 mM NaCl. These data enable us to conclude that in very low ionic strength (0.25 mM Na2EDTA) the nucleosome discs are oriented with their flat faces more or less parallel to the chromatin filament axis. Increasing ionic strength up to 20 mM NaCl leads to reorientation of the nucleosome discs and to formation of chromatin structures with nucleosome flat faces inclined to the fibril axis. A conformational transition of that kind is not revealed in H1-depleted chromatin. The condensation of the chromatin filaments with increasing concentration of NaCl from 20 mM to 100 mM slightly influences the orientation of the nucleosomes.

Low angle x-ray diffraction studies of chromatin structure in vivo and in isolated nuclei and metaphase chromosomes

Diffraction of x-rays from living cells, isolated nuclei, and metaphase chromosomes gives rise to several major low angle reflections characteristic of a highly conserved pattern of nucleosome packing within the chromatin fibers. We answer three questions about the x-ray data: Which reflections are characteristic of chromosomes in vivo? How can these reflections be preserved in vitro? What chromosome structures give rise to the reflections? Our consistent observation of diffraction peaks at 11.0, 6.0, 3.8, 2.7 and 2.1 nm from a variety of living cells, isolated nuclei, and metaphase chromosomes establishes these periodicities as characteristic of eukaryotic chromosomes in vivo. In addition, a 30-40- nm peak is observed from all somatic cells that have substantial amounts of condensed chromatin, and a weak 18-nm reflection is observed from nucleated erythrocytes. These observations provide a standard for judging the structural integrity of isolated nuclei, chromosomes, and chromatin, and thus resolve long standing controversy about the "tru" nature of chromosome diffraction. All of the reflection seen in vivo can be preserved in vitro provided that the proper ionic conditions are maintained. Our results show clearly that the 30-40-nm maximum is a packing reflection. The packing we observe in vivo is directly correlated to the side-by-side arrangement of 20- 30-nm fibers observed in thin sections of fixed and dehydrated cells and isolated chromosomes. This confirms that such packing is present in living cells and is not merely an artifact of electron microscopy. As expected, the packing reflection is shifted to longer spacings when the fibers are spread apart by reducing the concentration of divalent cations in vitro. Because the 18-, 11.0-, 6.0-, 3.8-, 2.7-, and 2.1-nm reflections are not affected by the decondensation caused by removal of divalent cations, these periodicities must reflect the internal structure of the chromaticn fibers.

Nucleomeric organization of chromatin

In the nuclei fixed in situ, as well as in nuclei in low-ionic-strength solutions containing magnesium ions, chromatin is represented by globular nucleomeric fibrils 20-25 nm in diameter. Staphylococcal or endogenous nucleases cleave chromatin fibrils to nucleomers and multinucleomers. On removal of firmly bound magnesium, the nucleomers unfold into chains of four, six or eight nucleosomes. Mild staphylococcal nuclease digestion of nuclear chromatin releases mononucleomers, dinucleomers and trinucleomers that sediment in the sucrose density gradient in the presence of EDTA as 37-S, 47-S and 55-S particles, respectively. The mononucleomers in the sucrose density gradient with MgCl2 sediment as 45-S particles. The determination of the length of staphylococcal-nuclease-digested DNAs contained in the chromatin fragments showed that a nucleomer is composed of 8, and a dimer and trimer of 14-16 and 21-24 nucleosomes, respectively. When deprived of Mg2+ ions, the monomers lose their compactness (45 S) and become loose particles (37 S). This transition is completely reversible if nucleomers contain histone H1. Removal of this histone or dialysis of the nucleomer against EDTA at low ionic strength results in the complete unfolding of the nucleomer into a chain of nucleosomes. A structural model of a nucleomer fibril is suggested where the helicity of the nucleosome chain in a nucleomer (two turns of four nucleosomes each) is periodically discontinued. Such an organization of chromatin apparently provides additional hindrances for site-specific recognition of DNA in chromatin but permits local changes (within a single nucleomer) in chromatin when a hindrance is abolished.

Higher order folding of two different classes of chromatin isolated from chicken erythrocyte nuclei. A light scattering study

Bulk chromatin fragments were excised from chicken erythrocyte nuclei by digestion with micrococcal nuclease. Fractionation into S chromatin (soluble at physiological ionic strengths) and I chromatin (insoluble at physiological ionic strengths) was achieved by dialysis against buffers containing 0.15 M NaCl. The effects of NaCl concentration on the molecular dimensions of S and I chromatins were determined by dynamic and static light scattering. Series of fragment lengths were obtained by gel filtration of S and I chromatins under ionic conditions which lead to maximal intramolecular compaction. Hydrodynamic radii and radii of gyration were determined for fragment lengths ranging from 8 to 53 nucleosomes. These data are in excellent agreement with calculations for extended helical structures. Close-packed solenoidal or superbead structures are not compatible with these data. Comparisons of molecular dimensions derived from light scattering and electron microscopy indicate that considerable shrinkage of chromatin fragments can occur when common methods of sample preparation are used for microscopy.

Conformation of chromatin oligomers. A new argument for a change with the hexanucleosome

Quasielastic laser light scattering measurements have been made on chromatin oligomers to obtain information on the transition in their electrooptical properties, previously observed for the hexameric structures [Marion, C. and Roux, B. (1978) Nucleic Acids Res. 5, 4431-4449]. Translational diffusion coefficients were determined for mononucleosomes to octanucleosomes containing histone H1 over a range of ionic strength. At high ionic strength, oligomers show a linear dependence of the logarithm of diffusion coefficient upon the logarithm of number of nucleosomes. At low ionic strength a change occurs between hexamer and heptamer. Our results agree well with the recent sedimentation data of Osipova et al. [Eur. J. Biochem. (1980) 113, 183-188] and of Butler and Thomas [J. Mol. Biol. (1980) 140, 505-529] showing a change in stability with hexamer. Various models for the arrangements of nucleosomes in the superstructure of chromatin are discussed. All calculations clearly indicate a conformational change with the hexanucleosome and the results suggest that, at low ionic strength, the chromatin adopts a loosely helical structure of 28-nm diameter and 22-nm pitch. These results are also consistent with a discontinuity every sixth nucleosome, corresponding to a turn of the helix. This discontinuity may explain the recent electric dichroism data of Lee et al. [Biochemistry (1981) 20, 1438-1445]. The hexanucleosome structure which we have previously suggested, with the faces of nucleosomes arranged radially to the helical axis has been recently confirmed by Mc Ghee et al. [Cell (1980) 22, 87-96]. With an increase of ionic strength, the helix becomes more regular and compact with a slightly reduced outer diameter and a decreased pitch, the dimensions resembling those proposed for solenoid models.

Chicken erythrocyte nucleus contains two classes of chromatin that differ in micrococcal nuclease susceptibility and solubility at physiological ionic strength

Inactive chromatin of the chicken erythrocyte nucleus is shown to consist of two distinct classes (I and S). I chromatin (approximately 60% of the total genome) is insoluble at greater than 0.1 M ionic strength whereas S chromatin (approximately 40% of the total genome) is soluble at all ionic strengths studied (0.01--0.3 M). These chromatins are released from nuclei upon digestion with micrococcal nuclease by two separate parallel processes that do not have a precursor--product relationship to each other. Isolated I-chromatin fragments show a progressive reduction in size from 250 to approximately 50 nucleosome equivalents with increasing digestion times at 0-2 degrees C. Prolonged digestion of nuclei at 37 degrees C results in conversion of I chromatin to mononucleosomes that are insoluble at greater than 30 mM NaCl. Isolated S-chromatin fragments show a constant size distribution, independent of digestion time, that peaks at approximately 35 nucleosome equivalents. Prolonged digestion of nuclei at 37 degrees C results in the conversion of S chromatin to mononucleosomes that are soluble at physiological ionic strength. Both I and S chromatins contain a full complement of histones with no nonhistone proteins.

Structural investigations on isolated chromatin of higher-order organisation

Chromatin of a high structural order was prepared by a method avoiding drastic mechanical stress, as well as strong changes of the ionic strength, and was investigated by small-angle X-ray scattering. The results obtained support the idea that the quaternary structure of completely hydrated chromatin in solution is a solenoid with a diameter of about 32-34 nm. Gel chromatography of this chromatin yields solutions containing mainly quaternary structures with differing portions of tertiary structure. Decrease of the ionic strength results in an increase of loosening and unfolding of quaternary structures. Reconstitution by readjustment of the physiological ionic strength indicates slight differences between reconstituted and original higher-order structures.

Solution structural studies of chromatin fibers

We report solution structural studies on 9--16-kilobase (kb) fragments of the 30-nm chromatin fiber isolated from calf thymus nuclei. Samples were stabilized by dimethylsuberimidate cross-linking in 100 mM salt concentration to ensure retention of a compact conformation. Electron microscopy, sedimentation diffusion, light scattering, and gel electrophoresis were used to characterize materials which were fractionated by size by utilizing sucrose gradient sedimentation. Measurements reported include the translational frictional coefficient as determined by quasielastic light scattering and the rotational frictional coefficient as deduced from transient electric dichroism. These frictional properties were combined to yield 33 +/- 3 nm for the diameter of the fiber and a length of 1.5 +/- 0.1 nm per nucleosome. Assuming a superhelix pitch of 11 nm, we calculate 7.5 +/- 0.5 nucleosomes per superhelical turn. The 30-nm fiber was found to reach saturation of electric field orientation at about 10--13 kV/cm and to lack a detectable permanent dipole moment, implying no polarity of the fiber. The limiting reduced dichroism rho was found to be +0.06, intermediate between the values expected if the nucleosomal disk diameters were parallel (rho expected = -3/8) or perpendicular (rho expected +3/4) to the fiber axis. This result implies an average angle of 51 degrees between the fiber axis and the local DNA (nucleosomal) superhelix axis and rules out many of the simple models which have been proposed for the detailed structure of the 30-nm fiber.

The higher order structure of chicken erythrocyte chromosomes in vivo

Recently eukaryotic chromosomes have been shown to consist of a repeating subunit, called the nucleosome. Although electron microscopy, neutron scattering and X-ray diffraction have been used to determine the low resolution structure of the nucleosome, these techniques have yielded little information about the disposition of nucleosomes within chromosomes. Electron microscopy has produced many models for chromosome structure based on uniform fibres of 150-500A diameter or on globular 'superbeads. Unfortunately the models are based on microscope images that fail to reveal the strong structural periodicities shown by X-ray scattering to be characteristic of isolated chromatin in solution. Moreover it has not been demonstrated that the chromosomes of living cells are composed of such fibres. We have used low-angle X-ray scattering to investigate the organization of chromosomes in vivo and to account for the previously observed inconsistencies in many X-ray and electron microscope observations. We report here that chicken erythrocytes have a 400 A periodicity due to a nuclear structure that is directly related to the 300 A side-by-side packing of chromosome fibres revealed by electron microscopy of embedded cells, and that this periodicity can be preserved in isolated nuclei provided that the proper buffers are used.

Aggregation of small oligonucleosomal chains into 300-A globular particles

Chicken erythrocyte oligonucleosomes (trimers to about 20-mers) are able to interact with each other through the very lysine-rich histones (H1 and H5) and form heterogeneous globular particles with a mean diameter of about 300 A. These particles assemble spontaneously during micrococcal nuclease digestion of chromatin in the presence of 30 mM NaCl and contain approximately 25 nucleosomes. They are sensitive to ionic strength and unfold at lower salt concentrations but can be reconstituted by restoring the initial salt concentration. Even at 30 mM NaCl, the particles remain dynamic structures, being in equilibrium with their oligonucleosomal components as revealed by the fact that particle stability depends on the concentration of oligonucleosomes.

X-ray small-angle scattering study of mononucleosomes and of the close packing of nucleosomes in polynucleosomes

The radius of gyration of mononucleosomes determined by X-ray small-angle scattering is 4.35 nm. The maximum dimension determined from the distance distribution function and the volume amount to 12.9 nm and 370 nm3, respectively. For a particular fraction of polynucleosomes a mean radius of gyration 16 nm, a maximum dimension 65 nm, and a mean volume 25,240 nm3 is obtained. The shape is approximated by an elongated cylinder having a diameter of 28 nm. A polynucleosome is built up from 69 nucleosomes, on the average. The distance of neighbouring nucleosomes in the polynucleosome amounts to 5.2 nm. Moreover, this distance shows that the nucleosomes in the polynucleosome are very closely packed.

Structure of the chromosomal material in inactive nuclei of chicken red blood cells

Electron microscope sections have been cut of chicken red blood cell nuclei by a novel procedure that produces zones of material below 100 A in thickness. After fixing and staining, electron dense structures are observed that have dimensions closely correlating with those determined for nucleosomes. These structures appear as wedge-shaped or as circular objects with a diameter of approximately 90-100 A. Five to eight of these objects are arranged in a spiral around a central core giving rise to a 250-300 A structure which may represent a superbead or a cross section of a solenoidal fibre.

Interparticle effects in low-angle x-ray and neutron diffraction from chromatin

Published diffraction data are critically reviewed, and replotted in a new way to show the variation with concentration of the 8- to 25- nm diffraction maximum. Most of the early data are found to be consistent with a single model for a liquid-type array of mutually repulsive particles, whose molecular weight is calculated to be that of a nucleosome or possibly a dimer. The data for all but the highest concentrations, where distortion due to dehydration is possible, support no particular model for the higher-order coiling of chains of nucleosomes, and cannot be used to support models for "native" chromatin. Only in the presence of excess salts or after isolation with polyamines is there aggregation in solution of nucleosomes, which then give peaks at 11 and 5.5 nm that do not change much with concentration. Recent work by the authors confirms that under some conditions nucleosome undergo a transition to a state whose diffraction is consistent with hexagonal packing of extended DNA to which histones are still attached. This state is probably responsible for much of the strong 2.7-nm peak previously obtained from certain samples, which was in some cases assigned to nucleosome structure. Only the peak at 3.7 nm is clearly attributable to the form factor of the isolated native nucleosome.

A repeating unit of higher order chromatin structure in chick red blood cell nuclei

The organization of nucleosomes in higher order chromatin structures has been studied by electron microscopy of chick red blood cell nuclei. Chromatin appears as a thick fiber with an average diameter of approximately 300 A when prepared for electron microscopy in buffers which approximate physiological ionic strength. Progressive steps of disassembly of the thick fiber into individual nucleosomes could be induced either by ionic strength reduction or by tRNA treatment (which removes histone H1 and some non-histone chromosomal proteins). When disassembly was induced by ionic strength reduction in the presence of Mg++ (or Ca++), the lengths of the intermediate disassembly products were found to be multiples of 330 A. The diameter of these structures was estimated to be 275 A. This intermediate in the disassembly process is not observed if thick fiber disassembly is induced by ionic strength reduction in the absence of divalent cations. To investigate whether the higher order structural unit is present in the thick fiber at physiological ionic strengths, tRNA treatment was used to induce thick fiber disassembly under physiological monovalent ionic conditions. In this case, either with or without divalent cations, a supranucleosomal unit was found with dimensions similar to those given above. This data provides evidence for a slightly oblong supranucleosomal structure (330 x 275 A) whick forms a repeating unit in the chromatin thick fiber.