Studies on chromatin. V. A model for the structure of chromatin subunit

Nucleosome structure(s) and stability: variations on a theme

Chromatin is a highly regulated, modular nucleoprotein complex that is central to many processes in eukaryotes. The organization of DNA into nucleosomes and higher-order structures has profound implications for DNA accessibility. Alternative structural states of the nucleosome, and the thermodynamic parameters governing its assembly and disassembly, need to be considered in order to understand how access to nucleosomal DNA is regulated. In this review, we provide a brief historical account of how the overriding perception regarding aspects of nucleosome structure has changed over the past thirty years. We discuss recent technical advances regarding nucleosome structure and its physical characterization and review the evidence for alternative nucleosome conformations and their implications for nucleosome and chromatin dynamics.

Nucleosomes arrangement in chromatin

The spatial arrangement of nucleosomes in rat liver chromatin has been examined using the electric birefringence technique. All chromatin subunits studied (up to 9 consecutive nucleosomes) contain their full complement of the five histone types associated with about 200 base pairs repeat length DNA. From the relaxation times and the orientation mechanisms, the nucleosome may be assimilated to an oblate ellipsoid of dimensions about 140 x 140 x 70 A, and the DNA superhelical axis is parallel to its shorter axis. The most important result is a sharp transition in the electro-optical properties of subunits when the number of nucleosomes in the chain is greater than 6 : the initial negative birefringence, as for DNA, becomes positive and the relaxation time is multiplied by ten. The hexanucleosome, which presents no birefringence, has an helical symmetrical structure without preferential orientation axis. This structure is approximatively spherical of about 250 A diameter and the chromatin appears as a periodic array of such a structure.

Laser Raman spectra of calf thymus histones H1, H2A, and H2B

Laser Raman spectra of the calf thymus histones H1, H2A, and H2B in aqueous solutions are presented. The amide III band in the spectrum of the very lysine-rich histone H1 in aqueous solution appears at 1245 cm-1, which is almost at the same frequency as the corresponding vibration of the ionized form of poly(L-lysine). Upon increasing the NaCl concentration to 1 M, the frequency of the amide III vibration shifts to 1250 cm-1 as a result of the formation of a more compact disordered structure of at least the N-terminal region of the protein. Changing the pH from 3 to 5 induces the same frequency shift. The amide III regions of the Raman spectra of the slightly lysine-rich histones H2A and H2B shows two bands at 1247 and 1265 cm-1 for H2A, and at 1254 and 1265 cm-1 for H2B. These doublets are attributed to vibrations involving the backbone of at least two structurally distinct parts of the histone molecules. The low frequency component is assigned to the random-coil regions of the proteins which appear to have similar conformations for H1 and H2A. The frequency of this component also suggest that the structure of the disordered regions of H2B are more compact and less extended. These conclusions confirm the conformation predictions based on the primary structures of these proteins. The high frequency component at 1265 cm-1 is assigned to the alpha-helical and rigid disordered structures of H2A and H2B, since this band increases in intensity upon addition of NaCl. The amide I' region of the histone spectra is also presented but appears to be much less sensitive to the conformation than the amide III region. The intensity of the bands due to the single bond C-C stretching modes, as well as the intensity ratio of the tyrosine Fermi doublet at 855 and 830 cm-1, are also discussed.

The effect of H1 histone on the action of DNA-relaxing enzyme

The action of DNA-relaxing enzyme on H1-DNA complexes was investigated. Complexes of superhelical and relaxed closed circular duplex DNA with H1 were treated with mammalian relaxing enzyme, deproteinized, and electrophoresed on agarose gels. At relatively low ratios of H1 to superhelical DNA, molecules of superhelical density intermediate between those of the starting material and relaxed DNA, the normal product, were generated. At relatively high H1 histone concentrations (H1:DNA greater than 0.4 w/w), the superhelical DNA was not relaxed. Further, no superhelical turns were introduced into relaxed closed duplex DNA at any concentration of H1 tested. Thus, the binding of H1 histone to DNA prevents the action of the relaxing enzyme. Moreover, H1 histone does not appear to unwind the DNA duplex upon binding. The implications of these observations and the previously demonstrated specificity of H1 histone for superhelical DNA are discussed in relation to the structure of chromatin.

Nuclease cleavage of chromatin at 100-nucleotide pair intervals

Digestion of mouse liver nuclei with DNase II leads to a novel cleavage pattern with a 100-nucleotide pair periodicity. From chromatin, this pattern or the standard 200-nucleotide pair repeat can be produced depending on the ionic conditions. The results are interpreted by assuming different conformational states of the nuclear material, including condensed and extended forms.

Model studies of chromatin structure based on X-ray diffraction data

Model calculations are presented in order to interpret the X-ray diffraction diagrams given by chromatin gels. It is shown that by taking into account the hydration of chromatin subunits, the problem of calculating the interference function in concentrated gels is greatly simplified. In this way it is spossible to fully interpret the influence of concentration on the position and intensity of the various rings present in the X-ray diffraction patterns. The possibilities and limitations of models based on spherical symmetry are also discussed. It is concluded that each chromatin subunit most likely contains three turns of DNA in each 200 base pairs segment surrounding a central protein core. With the method presented here it is possible to test if other models of chromatin based on different kinds of evidence are compatible with the X-ray diffraction data.

A model for chromatin based upon two symmetrically paired half-nucleosomes

We propose that the basic unit of chromatin is constructed of two isologously paired heterotypic protein tetramers each containing one molecule of H2A, H2B, H3, and H4 histone. These proteins form a core that holds 140 base pairs (bp) of DNA in a single left-handed, non-interwound DNA super-coil approximately 95 bp in circumference, creating a nucleosome particle (DNA and protein) organized about a dyad axis of symmetry. Such a nucleosome can open up into its separate half-nucleosomes to allow genetic readout without requiring histone displacement.

Mapping DNAase l-susceptible sites in nucleosomes labeled at the 5' ends

We have used lambda-32P-ATP and polynucleotide kinase to label stoichiometrically the 5' ends of DNA in intact isolated HeLa cell nucleosomes. DNA is not nicked or degraded during the modification reaction. We have used these modified nucleosomes to study both the distribution and the relative availability of sites within the nucleosome which are susceptible to digestion by DNAase l. The results show that the nucleosome contains a potential cleavage site every 10 nucleotides, with the exception of the site 80 nucleotides from the 5' end. Favored cleavage sites are located 20, 40, 50, 100, 120, and 130 nucleotides from the 5' end; sites 30 and 110 nucleotides from the 5' end are strongly disfavored, while the potential site 80 nucleotides from the 5' end is virtually never cleaved. These findings provide constraints for models of histone-DNA interactions within the chromatin subunit.

Studies on chromatin. Free DNA in sheared chromatin

Chromatin which has been hydrodynamically sheared in a low-ionic-strength buffer lacking divalent cations (I = 0.0005 M) contains a heterogeneous set of deoxyribonucleoprotein particles but no molecules of free DNA. The main finding is that a transference of sheared chromatin to 1--2 mM MgCl2 or to 0.1--0.2 M NaCl results in appearance of completely free DNA molecules. A salt-induced rearrangement of DNA-bound histones but not a partial loss of them is responsible for the observed phenomenon. Formation of free DNA molecules is accompanied by aggregation of the majority of remaining deoxyribonucleoprotein particles. The percentage of free DNA molecules in the chromatin which was sheared to an average DNA length of about 400 base pairs is increased from zero in the initial sample to 8-9% in 1 mM MgCl2 and further to approximately 25% of the total DNA in 0.15 M NaCl, 2 mM MgCl2. Free DNA molecules in the sheared chromatin are observed not only upon isopycnic banding of formaldehyde-fixed deoxyribonucleoproteins in CsCl gradients but also in non-ionic metrizamide gradients with either fixed or unfixed deoxyribonucleoprotein samples. The process of free DNA formation is a reversible one; its direction and the equilibrium state depend in particular on the ionic conditions of the medium.