Small angle x-ray scattering of chromatin. Radius and mass per unit length depend on linker length.

Analyses of low angle x-ray scattering from chromatin, isolated by identical procedures but from different species, indicate that fiber diameter and number of nucleosomes per unit length increase with the amount of nucleosome linker DNA. Experiments were conducted at physiological ionic strength to obtain parameters reflecting the structure most likely present in living cells. Guinier analyses were performed on scattering from solutions of soluble chromatin from Necturus maculosus erythrocytes (linker length 48 bp), chicken erythrocytes (linker length 64 bp), and Thyone briareus sperm (linker length 87 bp). The results were extrapolated to infinite dilution to eliminate interparticle contributions to the scattering. Cross-sectional radii of gyration were found to be 10.9 +/- 0.5, 12.1 +/- 0.4, and 15.9 +/- 0.5 nm for Necturus, chicken, and Thyone chromatin, respectively, which are consistent with fiber diameters of 30.8, 34.2, and 45.0 nm. Mass per unit lengths were found to be 6.9 +/- 0.5, 8.3 +/- 0.6, and 11.8 +/- 1.4 nucleosomes per 10 nm for Necturus, chicken, and Thyone chromatin, respectively. The geometrical consequences of the experimental mass per unit lengths and radii of gyration are consistent with a conserved interaction among nucleosomes. Cross-linking agents were found to have little effect on fiber external geometry, but significant effect on internal structure. The absolute values of fiber diameter and mass per unit length, and their dependencies upon linker length agree with the predictions of the double-helical crossed-linker model. A compilation of all published x-ray scattering data from the last decade indicates that the relationship between chromatin structure and linker length is consistent with data obtained by other investigators.     

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.     

Higher order structure of chromatin: orientation of nucleosomes within the 30 nm chromatin solenoid is independent of species and spacer length

We have used electric dichroism to study the arrangement of nucleosomes in 30 nm chromatin solenoidal fibers prepared from a variety of sources (CHO cells, HeLa cells, rat liver, chicken erythrocytes, and sea urchin sperm) in which the nucleosome spacer length varies from approximately 10 to approximately 80 bp. Field-free relaxation times are consistent only with structures containing 6 +/- 1 nucleosomes for every 11 nm of solenoidal length. With very few assumptions about the arrangement of the spacer DNA, our dichroism data are consistent with the same orientation of the chromatosomes for every chromatin sample examined. This orientation, which maintains the faces of the radially arranged chromatosomes inclined at an angle between 20 degrees-33 degrees to the solenoid axis, thus appears to be a general structural feature of the higher order chromatin fiber.     

Spectral analysis of chromatin and its components in the vacuum ultraviolet region of the spectrum

Electronic absorption spectra of thin films of chromatin and chromatin components in ultraviolet (140-280 nm) were investigated. The absorption coefficients mu (lambda) of chromatin, nucleosomes with and without histone H1, total histones (TH), DNA were compared. The spectra of nucleosomes and chromatin differ from summary spectra of DNA + TH. The lack of additivity of absorption coefficients at different wavelengths may be explained by different conformational changes of free DNA, TH and DNA, TH in nucleosomes and chromatin during the process of drying aqueous solutions for the preparations of thin films. The obtained mu (lambda) values are necessary for the estimation of the DNA and TH parts of absorption in chromatin and nucleosomes in the investigations of UV and VUV irradiation damages.     

Reconstitution of chromatin higher-order structure from histone H5 and depleted chromatin

Reconstitution of the 30 nm filament of chromatin from pure histone H5 and chromatin depleted of H1 and H5 has been studied using small-angle neutron-scattering. We find that depleted, or stripped, chromatin is saturated by H5 at the same stoichiometry as that of linker histone in native chromatin. The structure and condensation behavior of fully reconstituted chromatin is indistinguishable from that of native chromatin. Both native and reconstituted chromatin condense continuously as a function of salt concentration, to reach a limiting structure that has a mass per unit length of 6.4 nucleosomes per 11 nm. Stripped chromatin at all ionic strengths appears to be a 10 nm filament, or a random coil of nucleosomes. In contrast, both native and reconstituted chromatin have a quite different structure, showing that H5 imposes a spatial correlation between neighboring nucleosomes even at low ionic strength. Our data also suggest that five to seven contiguous nucleosomes must have H5 bound in order to be able to form a higher-order structure.     

DNA-protein interactions in nucleosomes and in chromatin. Structural studies of chromatin stabilized by ultraviolet-light induced crosslinking.

Crosslinking induced by ultraviolet light irradiation at 254 nm has been utilized to investigate the structure of chromatin and isolated nucleosomes. The results presented here imply that the four core histones, as well as histone H1, have reactive groups within a bond length of the DNA bases. In nucleosomes depleted of H1, all of the core histones react similarly with the DNA and form crosslinks. In chromatin, the rate of crosslinking of all histones to DNA is essentially similar. Comparison of mononucleosomes, dinucleosomes and whole chromatin shows that the rate of crosslinking increases significantly with increasing number of connected nucleosomes. These differences in the rate of crosslinking are interpreted in terms of interactions between neighbouring nucleosomes on the chromatin fiber, which are absent in an isolated mononucleosome.     

Organisation of subunits in chromatin.

There is considerable current interest in the organisation of nucleosomes in chromatin. A strong X-ray and neutron semi-meridional diffraction peak at approximately 10 nm had previously been attributed to the interparticle specing of a linear array of nucleosomes. This diffraction peak could also result from a close packed helical array of nucleosomes. A direct test of these proposals is whether the 10 nm peak is truly meridional as would be expected for a linear array of nucleosomes or is slightly off the meridian as expected for a helical array. Neutron diffraction studies of H1-depleted chromatin support the latter alternative. The 10 nm peak has maxima which form a cross-pattern with semi-meridional angle of 8 to 9 degrees. This is consistent with a coil of nucleosomes of pitch 10 nm and outer diameter of approximately 30 nm. These dimensions correspond to about six nucleosomes per turn of the coli.     

Preparation and physical characterization of a homogeneous population of monomeric nucleosomes from HeLa cells.

We describe a method of isolating a homogeneous population of "trimmed" monomeric nucleosomes from Hela cells. These nucleoprotein particles contain a 140 +/- 5 base pair length of DNA and have a histone/DNA ratio of 1.2. They lack H1 and contain equal amounts of the four smaller histones. The DNA contains no single strand nicks. The particles sediment with an S20,w of 11S in D2O density gradients. After formaldehyde fixation, they band at a density of 1.4370 in neutral CsCl. Digestion of nucleosomes with either micrococcal nuclease or DNase I generates the same pattern of DNA fragments observed when intact nuclei are digested. Circular dichroism spectra indicate that the 280 nm positive ellipticity maximum of nucleosomes is about one-half that of chromatin. In the presence of 6 M urea, nucleosomes sediment with an S20,w of 6S, have a multiphasic thermal denaturation profile, and exhibit a circular dichroic spectrum nearly identical to that of B-form DNA. Our yield of purified nucleosomes (10-15% of the input DNA) is similar to the yields of other methods; our nucleosome population is substantially more homogeneous than those previously reported.     

The fine structure of chromatin in Paranosema grylli (Microsporida)

Nucleosomes were found for the first time in the nuclear chromatin of Microsporida--organisms known among the smallest eukaryotes on Earth. Chromatin of Paranosema grylli sporoplasm was studied by Miller's technique. On low ionic-strength cell spreads, this chromatin was represented by 10 nm nucleosome filaments, 20 nm filaments, and "smooth" (nucleosome-free) filaments of 3-4 nm in diameter. Nucleosome filaments display structural heterogeneity seen as irregular arrangement of nucleosome particles along the filament length. Different nucleosome filaments show 13-30 nucleosomes per 1 microm with the length of linker DNA ranging from 10 to 45 nm. The present results suggest that microsporidian chromatin is weakly condensed. Only lower-order chromatin packaging levels displayed some structural peculiarities.     

The superstructure of chromatin and its condensation mechanism

Model calculations on the superstructure of uncondensed and condensed chromatin are presented. It is found that agreement between the calculated X-ray solution scattering patterns and the experimental observations can be reached with the assumptions that: a) The uncondensed chromatin fibre in solution has a helix-like structure, with a pitch of ca. 33.0 nm, a helical diameter of ca. 20.0 nm and 2.75–3.25 nucleosomes per turn. b) The most condensed state of the chromatin fibre in solution is best represented by a helix-like structure with ca. 2.56 nucleosomes per turn, a pitch of ca. 3.0 nm and a helical diameter of ca. 27.0 nm.     

Nucleosomes stacked with aligned dyad axes are found in native compact chromatin in vitro

In this study, electron tomograms of plunge-frozen isolated chromatin in both open and compacted form were recorded. We have resolved individual nucleosomes in these tomograms in order to provide a 3D view of the arrangement of nucleosomes within chromatin fibers at different compaction states. With an optimized template matching procedure we obtained accurate positions and orientations of nucleosomes in open chromatin in "low-salt" conditions (5 mM NaCl). The mean value of the planar angle between three consecutive nucleosomes is 70°, and the mean center-to-center distance between consecutive nucleosomes is 22.3 nm. Since the template matching approach was not effective in crowded conditions, for nucleosome detection in compact fibers (40 mM NaCl and 1 mM MgCl(2)) we developed the nucleosome detection procedure based on the watershed algorithm, followed by sub-tomogram alignment, averaging, and classification by Principal Components Analysis. We find that in compact chromatin the nucleosomes are arranged with a predominant face-to-face stacking organization, which has not been previously shown for native isolated chromatin. Although the path of the DNA cannot be directly seen in compact conditions, it is evident that the nucleosomes stack with their dyad axis aligned in forming a "double track" conformation which is a consequence of DNA joining adjacent nucleosome stacks. Our data suggests that nucleosome stacking is an important mechanism for generating chromatin compaction in vivo.     

The layered organization of nucleosomes in 30 nm chromatin fibers

We have used electron microscopy and established methods of three-dimensional reconstruction to obtain structural information on the 30 nm chromatin fibers from sea cucumber sperm and chicken erythrocytes. The fibers show a longitudinal periodicity of 10–11 nm. We have interpreted this periodicity as due to a grouping of nucleosomes into disks, each disk containing about 5–6 nucleosomes. These disks are closely stacked to form the chromatin fiber. We have built a detailed model for four fibers and we have determined the approximate coordinates of all the nucleosomes in them. The average distance found between neighboring nucleosomes has a value close to 11 nm. They may be connected either as a regularly distorted helix or as a layered zigzag. The second model appears more appropriate, since in the constrictions of the fibers the nucleosomes can only be connected as a zigzag.     

Chromatin fiber structure and plectonemic model of chromosome condensation in Drosophila cells

Reversible permeable cells have been used to isolate chromatin structures during the process of chromosome condensation. Analysis of individual structures slipping out from nuclei after reversal of permeabilization revealed that chromosomes of Drosophila cells consist of small units called rodlets. The fluorescent images of chromatin fibers were subjected to computer analysis allowing the computer-aided visualization of chromatin fibers. The zig-zag array of fibers consisting of 12-15 nucleosomes with a length of 270-330 nm (average 300 nm) showed decondensed extended strings, condensed loops, and coiled condensed loops. Theoretical considerations leading to the plectonemic model of chromatin condensation are based on experimental data, and give an explanation how the 30 chromatin fibers are formed and further condensed to the 300 nm chromatin loops in Drosophila cells.     

Nucleotide sequence-directed mapping of the nucleosomes

The concept of sequence-dependent deformational anisotropy of DNA proposed earlier is further elaborated and a computational procedure is developed for the sequence-directed mapping of the nucleosomes along chromatin DNA nucleotide sequences. The deformational anisotropy is found to be nonuniform along the molecule of the nucleosomal DNA, suggesting that the DNA superhelix in the nucleosome is slightly oval rather than circular in projection. The number of superhelical turns in the nucleosome core particle is estimated to be 2.0 +/- 0.2. Preliminary mapping of the nucleosomes in various chromatin DNA sequences yields the distribution of linker lengths which shows several minima separated by about 10 base-pairs. This is explained by sterical exclusion effects due to overlapping of the nucleosomes in space when some specific linker lengths are chosen. The mapping procedure described is tested by comparing its results with all the most accurate experimental mapping data reported so far. The comparison demonstrates that the exact positions of all the nucleosomes appear to be determined exclusively by the nucleotide sequences.     

Histone acetylation reduces nucleosome core particle linking number change

Nucleosome core particles differing in their levels of histone acetylation have been formed on a closed circular DNA that contains a tandemly repeated 207 bp nucleosome positioning sequence. The effect of acetylation on the linking number per nucleosome particle has been determined. With increasing levels of acetylation, the negative linking number change per nucleosome decreases from -1.04 +/- 0.08 for control to -0.82 +/- 0.05 for highly acetylated nucleosomes. These results indicate that histone acetylation has the ability to release negative supercoils previously constrained by nucleosomes into a closed chromatin loop and in effect function as a eukaryotic gyrase.     

Binding of androgen receptor to prostatic chromatin requires intact linker DNA.

Receptor-chromatin complexes were recovered from prostatic chromatin digested with micrococcal nuclease. The fragments of chromatin were separated on linear 7.6 to 76% (v/v) glycerol density gradients. With extensive digestion of DNA, receptor labeled with [1,2-3H]dihydrotestosterone was released from the chromatin. After 5% digestion of DNA to acid-soluble products, only a trace amount of labeled receptor was detected in the unbound form. In the latter instance, most of the labeled receptor was recovered from the gradients in association with five A260 peaks representing oligomeric and monomeric nucleosomes with a repeat length of 182 +/- 14 (mean +/- S.D.) base pairs. The concentration of receptors was highest in the A260 peaks, which contained large oligomers of nucleosomes, and lowest in fractions containing primarily monomer structures. Hence, the extent to which receptors remained bound to chromatin was dependent on the relative amount of intact, linker DNA present.     

Changes in chromatin structure induced by EDTA treatment and partial removal of histone H1.

Electron microscopy shows that EDTA treatment or partial removal of histone HI converts 200-250 A chromatin fibres characteristic for native chromatin, isolated in low ionic strength conditions into fibres consisting of nucleosomes connected by segments of DNA. This structural transition is accompanied by an increase in the amplitude of positive band of CD spectra at 280 nm. Comparison of electron microscopic, thermal denaturation and electrophoretic data suggests that multiphasic character of melting curves, observed for chromatin, lacking histone HI is due to the removal of histone HI and destabilisation of the DNA segments, connecting nucleosomes. It is also shown that bivalent cations play an important part both in the stabilisation of 200 A globules and of nucleosomes.     

Changes in the compactness of nucleosome chromatin from the bovine liver during aging

Electrophoresis methods used to study the fragments of chromatin revealed under the effect of Ca,Mg-dependent endonuclease on it have permitted establishing that stability of chromatin to the nucleosome level increases with aging. Changes in the compactness of the chromatin structure with aging make the accessibility of the linker DNA to nuclease lower the size of DNA fragments corresponding to mononucleosomes increasing from 192 +/- 5 pairs of bases to 209 +/- 5 pairs. Stabilization of the chromatin structure begins from certain nucleosomes which become more compact with the age. When analyzing basic proteins of chromatin by electrophoresis in different systems no qualitative changes were found in the subfraction composition of histones with aging, that permits supposing nonhistone proteins of chromatin and histone H1 to participate in the change of the chromatin structure compactness with the age.