X-Ray Structure of the Nucleosome Core Particle

Abstract

Two monoclinic crystal forms (P2₁,C2) of chicken erythrocyte nucleosomes have been under study in this laboratory. The x-ray structure of the P2₁ crystal form has been solved to 15 Å resolution. The B-DNA superhelix has a relatively uniform curvature, with only several local distortions observed in the superhelix. The individual histone domains have been localized and specific contacts between each histone and the DNA can be observed. Histone contacts to the inner surface of the DNA superhelix occur predominantly at the minor groove sites. Most of the histone core is contained within the inner surface of the superhelical DNA, except for part of H2A which extends between the DNA gyres near the terminus of the DNA. No part of H2A blocks the DNA terminus or would prevent a smooth exit of the DNA into the linker region. A similar extension of a portion of histone H4 between the DNA gyres occurs close to the dyad axis. Both unique nucleosomes in the P2₁ asymmetric unit demonstrate good dyad symmetry and are similar to each other throughout the histone core and DNA regions.     

H2A and H2B tails are essential to properly reconstitute nucleosome core particles

The conformation of recombinant Nucleosome Core Particles (NCPs) lacking H2A and H2B histone tails (gH2AgH2B) are studied. The migration of these particles in acrylamide native gels is slowed down compared to intact reconstituted NCPs. gH2AgH2B NCPs are also much more sensitive to nuclease digestion than intact NCPs. Small angle X-ray scattering (SAXS) experiments point out that the absence of H2A and H2B tails produces small but significant conformational changes of the octamers conformation (without wrapped DNA), whereas gH2AgH2B NCP conformations are significantly altered. A separation of about 25–30 bp from the core could account for the experimental curves, but other types of DNA superhelix deformation cannot be excluded. The distorted gH2AgH2B octamer may not allow the correct winding of DNA around the core. The absence of the H2A and H2B tails would further prevent the secondary sliding of the DNA around the core and therefore impedes the stabilisation of the particle. Cryo-electron microscopy on the same particles also shows a detachment of DNA portions from the particle core. The effect is even stronger because the vitrification of the samples worsens the instability of gH2AgH2B NCPs.     

Structure of the nucleosome core particle at 8 A resolution

The x-ray crystallographic structure of the nucleosome core particle has been determined using 8 A resolution diffraction data. The particle has a mean diameter of 106 A and a maximum thickness of 65 A in the superhelical axis direction. The longest chord through the histone core measures 85 A and is in a non-axial direction. The 1.87 turn superhelix consists of B-DNA with about 78 base pairs or 7.6 helical repeats per superhelical turn. The mean DNA helical repeat contains 10.2 +/- 0.05 base pairs and spans 35 A, slightly more than standard B-DNA. The superhelix varies several Angstroms in radius and pitch, and has three distinct domains of curvature (with radii of curvature of 60, 45 and 51 A). These regions are separated by localized sharper bends +/- 10 and +/- 40 base pairs from the center of the particle, resulting in an overall radius of curvature about 43 A. Compression of superhelical DNA grooves on the inner surface and expansion on the outer surface can be seen throughout the DNA electron density. This density has been fit with a double helical ribbon model providing groove width estimates of 12 +/- 1 A inside vs. 19 +/- 1 A outside for the major groove, and 8 +/- 1 A inside vs. 13 +/- 1 A outside for the minor groove. The histone core is primarily contained within the bounds defined by the superhelical DNA, contacting the DNA where the phosphate backbone faces in toward the core. Possible extensions of density between the gyres have been located, but these are below the significance level of the electron density map. In cross-section, a tripartite organization of the histone octamer is apparent, with the tetramer occupying the central region and the dimers at the extremes. Several extensions of histone density are present which form contacts between nucleosomes in the crystal, perhaps representing flexible or "tail" histone regions. The radius of gyration of the histone portion of the electron density is calculated to be 30.4 A (in reasonable agreement with solution scattering values), and the histone core volume in the map is 93% of its theoretical volume.     

Crystallization of belladonna mottle virus

Belladonna mottle virus belongs to the turnip yellows mosaic virus group of the small spherical plant viruses. It contains 180 protein subunits, which are arranged in a T = 3 icosahedral surface lattice. The top and bottom viral components crystallize isomorphously in hexagonal space group R3 ($\text{a = b = 296}\text{A}\text{?}\text{, c = 729}\text{A}\text{?}$). The unit cell contains three virus particles, while the crystallographic asymmetric unit consists of only one-third of a particle. X-ray diffraction data from the crystals extend to at least 3.8 Å resolution.     

Neutron diffraction studies on crystals of nucleosome cores using contrast variation

Neutron diffraction data have been collected from crystals of intact nucleosome core particles to a resolution of 25 Å. By varying the proportion of D₂O, the scattering of the mother liquor relative to the protein and DNA can be altered. At 39% D₂O, the solvent scattering matches that of the protein and so only the DNA is scattering, and similarly at 65% D₂0 only the protein scatters. Using this approach the neutron scattering of the two components and of the complete particle (0% D₂O) have been measured. The data corresponding to the principal projections are consistent with a model in which 1.8 turns of a DNA superhelix of pitch 27·5 Å and radius 42 Å are wound around a protein core.     

Letter: Electron microscopy of pyruvate kinase crystals from Saccharomyces carlsbergensis

Crystals of pyruvate kinase have been analysed by electron microscopy, optical diffraction and filtering, and the following parameters were obtained: $\text{2a = 93}\text{A}\text{?}$, $\text{2b = 126}\text{A}\text{?}$, $\text{l = 35·2}\text{A}\text{?}$. A comparison of these data with the parameters obtained from small-angle X-ray scattering measurements indicates that two molecules of the tetrameric enzyme are arranged in one packing unit.     

X-ray structure of the nucleosome core particle

Two monoclinic crystal forms (P2(1),C2) of chicken erythrocyte nucleosomes have been under study in this laboratory. The x-ray structure of the P2(1) crystal form has been solved to 15 A resolution. The B-DNA superhelix has a relatively uniform curvature, with only several local distortions observed in the superhelix. The individual histone domains have been localized and specific contacts between each histone and the DNA can be observed. Histone contacts to the inner surface of the DNA superhelix occur predominantly at the minor groove sites. Most of the histone core is contained within the inner surface of the superhelical DNA, except for part of H2A which extends between the DNA gyres near the terminus of the DNA. No part of H2A blocks the DNA terminus or would prevent a smooth exit of the DNA into the linker region. A similar extension of a portion of histone H4 between the DNA gyres occurs close to the dyad axis. Both unique nucleosomes in the P2(1) asymmetric unit demonstrate good dyad symmetry and are similar to each other throughout the histone core and DNA regions.     

Kinetics of histone hyperacetylation and deacetylation in human diploid fibroblasts

We have utilized sodium butyrate-treated normal human diploid fibroblasts to study core histone hyperacetylation kinetics. We report a small, distinct population of core histone characterized by a very rapid rate of hyperacetylation ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈10–15}\text{min}$ for monoacetylated histone H4) compared to the slower rate ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈140–200}\text{min}$ for monoacetylated H4) observed for bulk histone. Two rates of core histone deacetylation were also detected and we demonstrated that the rapidly hypermodified histone H4 population was also rapidly deacetylated. The kinetics of histone H4 hyperacetylation and deacetylation in these cells were not significantly altered, regardless of whether cultures were exponentially growing, confluent or arrested in an essentially non-mitotic state.     

Crystallization of a DNA-unwinding protein: Preliminary X-ray analysis of fd bacteriophage gene 5 product

The gene 5 protein from bacteriophage fd, which binds to single-stranded progeny fd DNA, was obtained as large single crystals and subjected to X-ray diffraction analysis. The crystals are of monoclinic space group C2 with $\text{a = 75.8}\text{A}\text{?}\text{, b = 28.0}\text{A}\text{?}\text{, c = 42.5}\text{A}\text{?}\text{and}\text{β = 103 °12′}$. The unit cell has one molecule of 9800 daltons as the asymmetric unit.     

X-ray scattering study of the shape of the DNA region in nucleosome core particle with synchrotron radiation.

The structure of the DNA region in rat thymus nucleosome core particle has been studied by synchrotron X-ray scattering analysis and the contrast-variation technique has been applied to determine the contribution of the DNA to the total scatterings. Small-angle contrast-matching measurements show that the entire core particle and isolated histone octamers are contrast-matched by solvents containing 64 and 54% (w/w) sucrose, respectively. At a contrast of 54% sucrose, where the scattering of the DNA dominates, the scattering data extending to higher angle of about 0.05 A-1 have been collected from relatively concentrated solutions (10 mg/ml) of core particles and interpreted on the basis of the regular helical model for the DNA region. The model calculations show that the shape of the DNA around the histone core is approximately by 1.8 turns of regular helix of 42 A radius and 28 A pitch. These values for helical parameters of our model are in good agreement with those of the structure of DNA in crystallized nucleosome cores shown by earlier diffraction studies.     

DNA reassociation kinetic analysis of the brine shrimp, Artemia salina

DNA reassociation kinetics have been partly elucidated for the brine shrimp $\text{Artemia salina}$, using calf thymus DNA as a standard. The $\text{Artemia}$ single-copy DNA sequences comprise 45% of the genome; sequences having a repetition frequency of about 2–90 are not detectable. The average repetition frequency of the intermediately redundant DNA component is about 5,000 copies. Reassociation kinetic data are consistent with a unit genome size of 1.5 pg.     

Shape and thermodynamic parameters of a Ca2+-dependent ATPase. A solution x-ray scattering and sedimentation equilibrium study

Solution X-ray scattering and sedimentation equilibrium experiments in solvents of variable density were used to determine some thermodynamic parameters of deoxycholate-solubilized ATPase monomers. Molecular weight and partial specific volume of the unsolvated deoxycholate-ATPase complexes were determined from X-ray scattering and/or sedimentation equilibrium data in $\text{H}{}_2\text{O}\text{H}{}_2$¹⁸O mixtures. Volume, mean density (electron density) and hydration were determined by analysis of both solution X-ray scattering and sedimentation equilibrium data recorded in solvents containing various concentrations of sucrose. Protein shape was investigated further with the help of the autocorrelation function corresponding to the scattering curve recorded in the absence of sucrose. This curve was shown to represent mainly the particle shape. The autocorrelation function is fitted adequately by a model formed by two adjacent and coaxial cylinders of different heights and diameters. One cylinder is assumed to bind deoxycholate, while the other one, which is larger, is considered to represent the portion of the ATPase molecule that, in sarcoplasmic reticulum membranes, is exposed to the outer medium.     

Postnatal increase in histone H1a in the rat pancreas

Adult rat pancreas contains an unusually high amount of histone H1a; $\text{H1a}\text{H1}$ ratio = 0.27. Histone H1a is not detectable in embryonic or newborn rat pancreas. This histone begins to appear at about 1 week postnatally and reaches the adult level about 5 weeks after birth. There is an inverse relationship between the appearance of histone H1a and DNA synthesis, as indicated by the nuclear labeling index after [³H]thymidine autoradiography.     

Crystallization of a tryptic core of the single-stranded DNA binding protein of bacteriophage T4

A tryptic core (residues 22 to 253) of the single-stranded DNA binding protein, or gene 32 protein, of bacteriophage T4 has been crystallized in four different crystal forms. One of these forms appears suitable for high-resolution X-ray crystallographic studies. It is triclinic, space group PI, with $\text{a = 67.7}\text{A}\text{?}\text{, b = 67.8}\text{A}\text{?}\text{, c = 66.0}\text{A}\text{?}\text{, α = 101.6 °, β = 107.0 °, γ = 105.2 °}$. There appear to be three protein protomers in a near-rhombohedral packing in the unit cell.     

A rapid procedure to detect in situ DNA/RNA hybrids

We developed a new method for detecting DNA/RNA hybrids formed $\text{in}\text{situ}$ using $\text{anti-}\text{DNA}\text{RNA}$ antibodies and the Peroxidase-antiperoxidase immunohistochemical procedure. Using RNA synthesised $\text{in}\text{vitro}$ from cloned $\text{Drosophila}$ histone genes (pDm 500H), we localized by this procedure, the histone genes to the 39 D-E region of the left arm of the second chromosome. This method has several advantages compared to conventional procedures.     

An investigation of the structure of Alfalfa mosaic virus by small-angle neutron scattering

Small-angle neutron scattering experiments have been performed on the tubular bottom component of Alfalfa mosaic virus (AMV) and the “30 S” particle (a quasispherical reassembled AMV coat protein particle) with the aim of determining the internal structure of the virus. Scattering curves were obtained out to a resolution of $\text{1}\text{50}\text{A}\text{?}{}^{\mathrm{?1}}$ at a number of H₂O/²H₂O ratios and were analysed using a model fitting technique. This involves calculating the scattering intensity due to a parameterised distribution of scattering density representing the particle and comparing this to the experimental data after taking into account the effect of instrumental smearing. The use of the contrast variation method enables the internal consistency of the model to be well tested.Three models are used in an attempt to explain the scattering curve of the 30 S particle. A single homogeneous shell is shown to be inadequate and two other models introducing the presumed T = 1 icosahedral symmetry of the particle are presented and discussed. The most satisfactory of these consists of 60 spherical monomers of radius 19 Å symmetrically placed in pairs about the 2-fold icosahedral positions.The analysis of the bottom component data has yielded a low resolution model for the virus, which is shown to be consistent with its composition as given by earlier physico-chemical measurements. In the model the RNA is uniformly packed throughout the interior of the capsid (which is cylindrical with hemispherical ends) out to a radius of about 65 Å and with a packing fraction of 20%. Within the limitations of an homogeneous shell model, the protein capsid has an outer radius of 94 Å and thickness of 23 Å, but arguments are presented based on the marked lattice structure of the cylindrical capsid and the analysis of the scattering data of the 30 S particle, that this model underestimates the thickness of the protein shell and that it in fact makes contact with the RNA at about 65 Å.     

Small-angle x-ray scattering study of lysine transfer RNA ligase from yeast

The scattered X-ray intensities from dilute solutions of lysine transfer RNA ligase, in 0.1 m-phosphate buffer at pH 7.0, have been measured at 21 °. The radius of gyration R (37.5 Å), the molecular weight M (114,000), and the volume V (295,000 ų) were determined.A comparison between the scattering curves obtained from the enzyme and the theoretical scattering curves of different triaxial bodies shows that the shape of the molecule can be represented by an oblate ellipsoid with the semiaxes A = 62.7, B = 50.1 and $\text{C = 23.5}\text{A}\text{?}$.     

The repetitive sequence structure of component alpha DNA and its relationship to the nucleosomes of the African green monkey.

An analysis of the repeat structure of the highly repetitive sequence, component α DNA of the African green monkey, shows that the DNA contains restriction sites for EcoRI, $\text{Eco}\text{RI}{}^1$, HindIII and HaeIII. All four restriction enzyme activities indicate a basic repeat length of 176 ± 4 base-pairs. In addition to primary $\text{Eco}\text{RI}{}^1$ and HindIII sites, about 59% of the repeat sequences contain secondary $\text{Eco}\text{RI}{}^1$ sites and about 36% of the repeat sequences contain secondary HindIII sites. The secondary sites are located less than 176 base-pairs from the primary sites and their cleavage yields several complex series of minor, intermediate segments in gels of the partial $\text{Eco}\text{RI}{}^1$ or HindIII digests. Cleavage at the secondary sites yields segments shorter than the unit monomer in the limit digests. The sites for EcoRI, $\text{Eco}\text{RI}{}^1$, HindIII and HaeIII have been mapped within the repeat unit.Treatment of the monkey nuclei with micrococcal nuclease at 2 °C and in the presence of 80 mm-NaCl reveals two distinct populations of nucleosomes. One population contains bulk DNA sequences, and after cleavage with micrococcal nuclease this population yields heterogeneous segments of DNA spanning 180 to 200 base-pairs in length. The other population contains component α sequences and after cleavage with micrococcal nuclease yields homogeneous segments of component α DNA that are exact multiples of the basic sequence repeat unit of 176 base-pairs. Thus, the cleavage by micrococcal nuclease of nucleosomal arrays containing component α sequences is as regular and precise as the cleavage of the purified DNA by the restriction enzymes. The resolution of the two distinct subsets of nucleosomes in the monkey nuclei is dependent upon the conditions of ionic strength and temperature employed during the nuclear isolation and the micrococcal nuclease digestion.These observations are consistent with a phase relation between the component α repeat sequences and the associated nucleosomal proteins (Musich et al., 1977b). They are also in accord with the hypothesis that the subunit structure of constitutive heterochromatin modulates or determines the repeat sequence structure and hence, the evolution of many highly repetitive mammalian DNAs (Maio et al., 1977).