A new particle of chromatin obtained by proteolysis of histones with clostripain

The proteolysis of the chromatin core particle by the arginine-specific endopeptidase clostripain yields a new nucleoprotein particle containing an unaltered DNA fragment of about 145 base pairs in length and a protein octameric core made up of twice the four histone fragments H2A, H2B, H3 and H4. This composition is suggested by the molecular weight of about 180 kd determined for the new particle by small angle neutron scattering. The histone fragments differ by about 2-3 kd each from the initial histones H2A, H2B, H3 and H4 and they correspond to the cleavage of the N-terminal part of the sequence (20-30 residues). A preliminary investigation by thermal denaturation, circular dichroism and small angle neutron scattering (measurement of a radius of gyration by the H2O-D2O contrast variation technique) indicates that the spatial organization of the new chromatin particle closely resembles that of the initial core particle.     

A low resolution model for the chromatin core particle by neutron scattering

Neutron scattering studies have been applied to chromatin core particles in solution, using the contrast variation technique. On the basis of the contrast dependance of the radius of gyration and the radial distribution function it is shown that the core particle consists of a core containing most of the histone around which is wound the DNA helix,following a path with a mean radius of 4.5 nm,in association with a small proportion of the histones. Separation of the shape from the internal structure, followed by model calculations shows that the overall shape of the particle is that of a flat cylinder with dimensions ca. 11x11x6 nm. Further details of the precise folding of the DNA cannot be deduced from the data, but detailed model calculations support concurrent results from crystallographic studies(25).Images     

Low-angle neutron scattering from chromatin subunit particles.

Monomer chromatin particles containing 140 base pairs of DNA and eight histone molecules have been studied by neutron scattering. From measurements in various H2O/D2O mixtures, radii of gyration and the average scattering density of the particle were determined. The radius of gyration under conditions when scattering from the DNA dominates is 50A, and when scattering from the protein dominates, 30A. Consequently the core of the particle is largely occupied by the histones while the outer shell consists of DNA together with some of the histone.     

Chromatin fiber dimensions and nucleosome orientation: a neutron scattering investigation.

Chromatin fibers were studied in solutions of mM monovalent salt by small angle neutron scattering. The variation of the cross section radius of gyration with H2O/D2O contrast shows that DNA is at much larger average radial distances from the fiber axis than histone. Consequently, the coils of DNA in a core particle must be approximately parallel to the fiber direction. The radii of gyration suggest that the maximum diameter of chromatin and nucleosomes is approximately 14 nm and that the DNA id distributed in two radial layers. The concentration dependence of the scattering maxima near 14 nm spacings furnishes independent support for a 14 nm external diameter and can be interpreted by a double DNA layer configuration.     

Neutron-scattering studies of accurately reconstituted nucleosome core particles and the effect of ionic strength on core particle structure

Chicken erythrocyte nucleosome core particles can be dissociated quantitatively into histones (H3, H4)2 bound to 146 base pairs of DNA, and 2(H2A, H2B). Reconstitution of core particles from the two components produces an 85% yield of particles which neutron scattering studies show to be accurate stoichiometrically and indistinguishable from native core particles: the radii of gyration of the shape, the protein components and the DNA components of the particles are 4.02 nm, 3.3 nm and 4.95 nm respectively. The largest distance and most probable distance which can be drawn in the particles are 11.5 nm and 4.3 nm respectively. The molecular weight of the particles is identical to that of control 'native' core particles. All of these values, within limits of error, are the same as known values for 'native' core particles. These experiments confirm the essential role of histones H3 and H4 in the initial organisation of core-particle structure, make possible the manufacture of perfectly pure and homogeneous core-particle preparations and allow the 100% incorporation of labelled or modified histones. Neutron scattering studies of core particles at high contrast (in D2O and H2O) have been carried out over a range of ionic strengths and pH. No change in structure is detected down to pH 5.5 in 20 mM NaCl or down to ionic strength 2.0 mM at pH 7.     

Physical studies of chromatin. The recombination of histones with DNA.

Experiments have been carried out to define clearly which histone combinations can induce a higher order structure when combined with DNA. The criterion for a higher order structure being the series of low-angle X-ray diffraction maxima nominally at 5.5 nm, 3.7 nm, 2.7 nm and 2.2 nm. Such a pattern, with resolution similar to that of H1-depleted chromatin, is readily attainable by recombining histones H2A + H2B + H3 + H4 with DNA using a salt-gradient dialysis method. However, the use of urea in the recombination procedure is shown to be detrimental to the production of a higher order structure. Low-angle ring patterns are not obtained by recomgining DNA with single pure histones or any combination of histone pairs exept H3 + H4. The diffraction maxima from the latter are, however, weaker than those from chromatin and there are pronounced semi-equatorial arcs. The presence of a third histone, either H2A or H2B in the H3 + H4 recombination mixture tends to distort the recognised low-angle pattern. It is concluded that the histone pair H3 + H4 is essential for the formation of a regular higher order structure in chromatin, although for a complete structural development the presence of H2A + H2B is also required.     

Low angle X-ray scattering studies of chromatin in different solvents; analysis by comparison with computer-simulated scattering curves

Low-angle X-ray scattering curves of isolated calf thymus chromatin, dissolved in 0.2 mm EDTA, 0.2 mm MgCl₂ or 0.5 m NaCl, have been analysed by comparison with simulated scattering curves of models from chromatin subunits and higher order structure. The results provided additional data based on established models. Assuming the protein core as a cylinder of 5.9–6.0 nm diameter and 5.9-2.0 nm height, the centre to centre distance of the cores in tightly packed chromatin was found to be 6.7 nm. Computer simulation of X-ray scattering of chromatin was fitted to experimentally derived data for estimating the ratios of quaternary and tertiary structure. Slight differences of the quaternary structures of 0.15 m NaCl adn in 0.2 mm MgCl₂ were observed.     

Chromatin very small angle neutron scattering: further evidence for a 30 nm diameter super coil in dilute solutions.

Intact chromatin, chromatin minus histone H1, and nuclease digestion fragments have been studied by very small angle neutron scattering. The results are not consistent with a straight chain of nucleosomes and require the presence of a higher order coiling in monovalent salt solutions. The data are interpretable by a structure having a cross section radius of gryration of 8.5 +/- 1 nm, which suggests an outer diameter for a coil of nucleosomes of 27 +/- 3 nm.     

Low resolution models of self-assembled histone fibers from X-ray diffraction studies.

X-ray diffraction data from self-assembled histone fibers are presented for three systems: H4, H3-H4, and the four core histones H2A, H2B, H3 and H4. These data have been obtained under conditions of high ionic strength and high protein concentration which are thought to promote histone conformation similar to that found in intact chromatin. The low angle equatorial scattering (R less than .05 A-1) is analysed, and, with additional constraints imposed by electron microscopy data, four low resolution fibrillar models are derived. Two features common to all the possible models are a maximum outer diameter of approximately 60 A and a subfibril diameter of approximately 25 A. It is the interference of the protein subfibrils across a central region of low electron density - a 10 A "hole" - which gives rise to the characteristic diffraction peak at 36 A. Possible relationships of the models of the histone fibers to the structure of the histone component of chromatin are suggested.     

Changes in distribution of basic nuclear proteins and chromatin organization during spermiogenesis in the greater bandicoot rat, <Emphasis Type="Italic">Bandicota indica</Emphasis>

Male germ cells of the greater bandicoot rat, Bandicota indica, have recently been categorized into 12 spermiogenic steps based upon the morphological appearance of the acrosome and nucleus and the cell shape. In the present study, we have found that, in the Golgi and cap phases, round spermatid nuclei contain 10-nm to 30-nm chromatin fibers, and that the acrosomal granule forms a huge cap over the anterior pole of nucleus. In the acrosomal phase, many chromatin fibers are approximately 50 nm thick; these then thickened to 70-nm fibers and eventually became 90-nm chromatin cords that are tightly packed together into highly condensed chromatin, except where nuclear vacuoles occur. Immunocytochemistry and immunogold localization with anti-histones, anti-transition protein2, and anti-protamine antibodies suggest that histones remain throughout spermiogenesis, that transition proteins are present from step 7 spermatids and remain until the end of spermiogenesis, and that protamines appear at step 8. Spermatozoa from the cauda epididymidis have been analyzed by acid urea Triton X-100 polyacrylamide gel electrophoresis for basic nuclear proteins. The histones, H2A, H3, H2B, and H4, transitional protein2, and protamine are all present in sperm extracts. These findings suggest that, in these sperm of unusual morphology, both transition proteins and some histones are retained, a finding possibly related to the unusual nuclear form of sperm in this species.     

Shape and subunit organisation of the DNA methyltransferase M.AhdI by small-angle neutron scattering

Type I restriction-modification (R-M) systems encode multisubunit/multidomain enzymes. Two genes (M and S) are required to form the methyltransferase (MTase) that methylates a specific base within the recognition sequence and protects DNA from cleavage by the endonuclease. The DNA methyltransferase M.AhdI is a 170 kDa tetramer with the stoichiometry M(2)S(2) and has properties typical of a type I MTase. The M.AhdI enzyme has been prepared with deuterated S subunits, to allow contrast variation using small-angle neutron scattering (SANS) methods. The SANS data were collected in a number of (1)H:(2)H solvent contrasts to allow matching of one or other of the subunits in the multisubunit enzyme. The radius of gyration (R(g)) and maximum dimensions (D(max)) of the M subunits in situ in the multisubunit enzyme (50 A and 190 A, respectively) are close of those of the entire MTase (51 A and 190 A). In contrast, the S subunits in situ have experimentally determined values of R(g)=35 A and D(max)=110 A, indicating their more central location in the enzyme. Ab initio reconstruction methods yield a low-resolution structural model of the shape and subunit organization of M.AhdI, in which the Z-shaped structure of the S subunit dimer can be discerned. In contrast, the M subunits form a much more elongated and extended structure. The core of the MTase comprises the two S subunits and the globular regions of the two M subunits, with the extended portion of the M subunits most probably forming highly mobile regions at the outer extremities, which collapse around the DNA when the MTase binds.     

Neutron scatter and diffraction techniques applied to nucleosome and chromatin structure

Neutron scatter and diffraction techniques have made substantial contributions to our understanding of the structure of the nucleosome, the structure of the 10-nm filament, the "10-nm----30-nm" filament transition, and the structure of the "34-nm" supercoil or solenoid of nucleosomes. Neutron techniques are unique in their properties, which allows for the separation of the spatial arrangements of histones and DNA in nucleosomes and chromatin. They have equally powerful applications in structural studies of any complex two-component biological system. A major success for the application of neutron techniques was the first clear proof that DNA was located on the outside of the histone octamer in the core particle. A full analysis of the neutron-scatter data gave the parameters of Table 3 and the low-resolution structure of the core particle in solution shown in Fig. 6. Initial low-resolution X-ray diffraction studies of core particle crystals gave a model with a lower DNA pitch of 2.7 nm. Higher-resolution X-ray diffraction studies now give a structure with a DNA pitch of 3.0 nm and a hole of 0.8 nm along the axis of the DNA supercoil. The neutron-scatter solution structure and the X-ray crystal structure of the core particle are thus in full agreement within the resolution of the neutron-scatter techniques. The model for the chromatosome is largely based on the structural parameters of the DNA supercoil in the core particle, nuclease digestion results showing protection of a 168-bp DNA length by histone H1 and H1 peptide, and the conformational properties of H1. The path of the DNA outside the chromatosome is not known, and this information is crucial for our understanding of higher chromatin structure. The interactions of the flexible basic and N- and C-terminal regions of H1 within chromatin and how these interactions are modulated by H1 phosphorylation are not known. The N- and C-terminal regions of H1 represent a new type of protein behavior, i.e., extensive protein domains that are designed not to fold up into secondary and tertiary protein structures. This behavior is increasingly observed in DNA and chromatin binding proteins, and in the case of the high-mobility group proteins HMG 14 and 17, the entire polypeptide chain is a flexible random coil over a wide range of solution, ionic, and pH conditions. It follows that the native conformations are probably imposed on these flexible domains and molecules by their binding sites in chromatin.(ABSTRACT TRUNCATED AT 400 WORDS)     

Subunit structure of casein micelles from small-angle neutron-scattering

Wet pellets of whole casein micelles of cows' milk have been studied by small-angle neutron-scattering. Contrast variation using 2H2O/H2O mixtures showed that the previously observed inflection in scattered intensity at Q[4 pi sin theta)/gamma) = 0.035 A-1 is due primarily to scattering from protein, and not from calcium phosphate. Agreement between measured scattering and that calculated for a simple model of packed protein subunits suggests that the whole micelle contains protein subunits of the approximate size of free casein submicelles, packed in a short-range ordered arrangement.     

Studies on chromatin. II. Isolation and characterization of chromatin subunits.

Earlier findings /1-10/ bearing on a subunit organization of chromatin were confirmed and in some points detailed. Besides this, a large-scale isolation of chromatin subunits; their protein composition, electron microscopic appearance and CsCl banding pattern are described. Although the purified chromatin subunit contains all five histones, the relative content of histone H1 i in it is two times lower than that in the original chromatin. tit is shown that a mild digestion of chromatin with staphylococcal nuclease produced not only separate chromatin subunits and their "oligomers' but also deoxyribonucleoprotein particles which sediment more slowly than subunits. It appears that these particles and subunits are produced from different initial structures in the chromatin. Finally, a crystallization of the purified chromatin subunit as a cetyltrimethyl ammonium salt is described.     

Hyperacetylation of core histones does not cause unfolding of nucleosomes. Neutron scatter data accords with disc shape of the nucleosome

Recent studies report that the frictional resistance of partially acetylated core particles increases when the number of acetyl groups/particle exceeds 10 (Bode, J., Gomez-Lira, M. M. & Schr?ter, H. (1983) Eur. J. Biochem. 130, 437-445). This was attributed to an opening of the core particle though other explanations, e.g. unwinding of the DNA ends were also suggested. Another possible explanation is that release of the core histone N-terminal domains by acetylation increased the frictional resistance of the particle. Neutron scatter studies have been performed on core particles acetylated to different levels up to 2.4 acetates/H4 molecule. Up to this level of acetylation the neutron scatter data show no evidence for unfolding of the core particle. The fundamental scatter functions for the envelope shape and internal structure are identical to those obtained previously for bulk core particles. The structure that gave the best fit to these fundamental scatter functions was a flat disc of diameter 11-11.5 nm and of thickness 5.5-6 nm with 1.7 +/- 0.2 turns of DNA coiled with a pitch of 3.0 nm around a core of the histone octamer. The data analysis emphasizes the changes in pair distance distribution functions at relatively low contrasts, particularly when the protein is contrast matched and DNA dominates the scatter. Under these conditions there is no evidence for the unwinding of long DNA ends in the hyperacetylated core particles. The distance distribution functions go to zero between 11.5 and 12 nm which gives the maximum chord length in a particle of dimension, 11 nm X 5.5 nm. The distance distribution function for the histone octamer contains 85% of the vectors within the 7.0-nm diameter of the histone core. 15% of the histone vectors lie between 7.0 and 12.0 nm, and these are attributed to the N-terminal domains of the core histones which extend out from the central histone core. Histone vectors extending beyond 7.0 nm are necessary to account for the measured radius of gyration of the histone core of 3.3 nm. A similar value of 3.2 nm is calculated for the recent ellipsoidal shape of 11.0 X 6.5 X 6.5 nm from the crystal structure of the octamer. However, the nucleosome model based on this structure is globular, roughly 11 nm in diameter, which does not accord with the flat disc shape core particle obtained from detailed neutron scatter data nor with the cross-section radii of gyration of the histone and DNA found previously for extended chromatin in solution.     

Chromatin superstructure: synchrotron radiation X-ray scattering study on solutions and gels.

X-ray small angle scattering patterns of solutions and gels of native chicken erythrocyte chromatin and chromatin depleted of H5 histones have been measured under several ionic conditions using synchrotron radiation. Features of the patterns are interpreted as resulting from a superstructure with an outer diameter of about 300A which is already present in uncondensed nucleofilaments. This superstructure which is shown to be maintained by the H5 histones also explains the rapid condensation of the nucleofilaments in higher ionic strengths.     

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.     

Structural Insights into the A1 ATPase from the archaeon, Methanosarcina mazei Gö1

The low-resolution structure and overall dimensions of the A(3)B(3)CDF complex of the A(1) ATPase from Methanosarcina mazei G?1 in solution is analyzed by synchrotron X-ray small-angle scattering. The radius of gyration and the maximum size of the complex are 5.03 +/- 0.1 and 18.0 +/- 0.1 nm, respectively. The low-resolution shape of the protein determined by two independent ab initio approaches has a knob-and-stalk-like feature. Its headpiece is approximately 9.4 nm long and 9.2 nm wide. The stalk, which is known to connect the headpiece to its membrane-bound A(O) part, is approximately 8.4 nm long. Limited tryptic digestion of the A(3)B(3)CDF complex was used to probe the topology of the smaller subunits (C-F). Trypsin was found to cleave subunit C most rapidly at three sites, Lys(20), Lys(21), and Arg(209), followed by subunit F. In the A(3)B(3)CDF complex, subunit D remained protected from proteolysis.     

Small-angle X-ray study on the quaternary structure of erythrocruorin from Helisoma trivolvis

The erythrocruorin from the aquatic snail Helisoma trivolvis was studied in sodium phosphate buffer at pH 6.7 by small angle X-ray scattering. The following molecular parameters were determined: radius of gyration 9.4 ± 0.1 nm and maximum dimension 29 ± 1 nm. A model which fits the experimental data well is presented. The overall shape is best described by a slightly ellipsoidal shape with a hole in the centre. A model consisting of 12 subunits forming a slightly ellipsoidal shape fits very well all scattering data.     

Oligomeric domain structure of human complement factor H by X-ray and neutron solution scattering.

Factor H is a regulatory component of the complement system. It has a monomer Mr of 150,000. Primary structure analysis shows that the polypeptide is divided into 20 homologous regions, each 60 amino acid residues long. These are independently folding domains and are termed "short consensus repeats" (SCRs) or "complement control protein" (CCP) repeats. High-flux synchrotron X-ray and neutron scattering studies were performed in order to define its solution structure in conditions close to physiological. The Mr of factor H was determined as 250,000-320,000 to show that factor H is dimeric. This structure is maintained at concentrations between 1 and 11 mg/mL in the pH range 5-9. Zn2+ ions are an inhibitor of C3b cleavage by factor I, a reaction in which factor H acts as a cofactor. Additions of Zn2+ to factor H caused it to form oligomers containing 4-10 monomers. The radius of gyration RG of native factor H by X-rays or by neutrons in 0% or 100% 2H2O buffers is not measurable but is greater than 12.5 nm. Two cross-sectional radii of gyration RXS-1 and RXS-2 were determined as 3.0-3.1 and 1.8 nm, respectively. Analyses of the cross-sectional intensities show that factor H is composed of two distinct subunits. The RXS-1 corresponds to the cross-sectional properties of both subunits and exhibits an unusual radiation dependence on the X-ray flux. Since RXS-2 is close to the corresponding RXS of C4b binding protein (91% of which is formed from SCR/CCP domains), it is inferred that the SCR/CCP domains of factor H and C4b binding protein have similar solution structures. The use of hydrodynamic spheres to reproduce literature sedimentation coefficients of 5.5-5.6 S showed that these were compatible with a V-shaped arrangement of two rods (36 spheres each, length 87 +/- 5 nm) joined at an angle of 5 degrees. The use of a similar arrangement of 244 spheres arranged in two rods (length 77 nm) to fit the experimental X-ray and neutron scattering curves showed that the two rods are joined at an angle of 5 degrees. This model corresponds to an actual RG of 21-23 nm. The separation between each SCR/CCP in factor H is close to 4 nm. In the solution structure of factor H, the SCR/CCP domains are in a highly extended conformation.