A proposed simulation method for directed self-assembly of nanographene.

A methodology for predictive kinetic self-assembly modeling of bottom-up chemical synthesis of nanographene is proposed. The method maintains physical transparency in using a novel array format to efficiently store molecule information and by using array operations to determine reaction possibilities. Within a minimal model approach, the parameter space for the bond activation energies (i.e. molecule functionalization) at fixed reaction temperature and initial molecule concentrations is explored. Directed self-assembly of nanographene from functionalized tetrabenzanthracene and benzene is studied with regions in the activation energy phase-space showing length-to-width ratio tunability. The degree of defects and reaction reproducibility in the simulations is also determined, with the rate of functionalized benzene addition providing additional control of the dimension and quality of the nanographene. Comparison of the reaction energetics to available density functional theory data suggests the synthesis may be experimentally tenable using aryl-halide cross-coupling and noble metal surface-assisted catalysis. With full access to the intermediate reaction network and with dynamic coupling to density functional theory-informed tight-binding simulation, the method is proposed as a computationally efficient means towards detailed simulation-driven design of new nanographene systems.

Polyamines permit the preparation of stable Physarum core particles which have a structure similar to those from higher eukaryotes.

The inherent instability of Physarum nucleosome core particles prepared by micrococcal nuclease digestion in Na+/Ca2+ buffers can be overcome by the addition of 0.15 mM spermine and 0.5 mM spermidine. Neutron scattering, circular dichroism, nuclease digestion and thermal denaturation studies carried out on these stable monosomes show them to be very similar to those obtained from higher eukaryotes.

Low-resolution structure of the complex of human blood platelet factor 4 with heparin determined by small-angle neutron scattering.

Small-angle neutron scattering was used to confirm that human platelet factor 4 was a compact tetrameric globular protein of radius of gyration 1.74 nm and indistinguishable from a sphere. The same technique, when applied to the 1:1 mol/mol complex of platelet factor and heparin of Mr 14000, revealed that the radius of gyration of the particle varied, depending on the relative proportion of 2H2O to H2O in the solvent. Analysis of this variation by the method of Ibel and Stuhrmann (Ibel, K. and Stuhrmann, H.B. (1975) J. Mol. Biol. 93, 255-266) revealed that in the complex the material of greatest neutron-scattering length (the highly sulphated polysaccharide heparin) was furthest from the centre of the particle. This confirms the postulate of Luscombe and Holbrook (Luscombe, M. and Holbrook, J.J. (1983) in Glycoconjugates (Chester, A.M., Heinegård, D., Lundblad, A. and Svensson, S., eds.), pp. 818-819, Secretariat, Lund) that the exact 1:1 mole ratio of heparin (Mr greater than 10 000) to platelet factor in this stable complex arises from the heparin winding around the outside of a globular protein core.

Nuclease digestion patterns as a criterion for nucleosome orientation in the higher order structure of chromatin.

Nuclease digestion patterns have been used to discriminate between possible orientations of nucleosomes in the higher order structure of chromatin. Computer simulations were done assuming 3 basically different orientations of nucleosomes which include all proposed models for the '30 nm fibre'. It is found that only alternating exposure of consecutive nucleosomes can explain the DNase I and DNase II digestion patterns.

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)

Structure of subnucleosomal particles. Tetrameric (H3/H4)2 146 base pair DNA and hexameric (H3/H4)2(H2A/H2B)1 146 base pair DNA complexes.

The tetrameric (H3/H4)2 146 base pair (bp) DNA and hexameric (H3/H4)2(H2A/H2B)1 146 bp DNA subnucleosomal particles have been prepared by depletion of chicken erythrocyte core particles using 3 or 4 M urea, 250 mM sodium chloride, and a cation-exchange resin. The particles have been characterized by cross-linking and sedimentation equilibrium. The structures of the particles, particularly the tetrameric, have been studied by sedimentation velocity, low-angle neutron scattering, circular dichroism, optical melting, and nuclease digestion with DNase I, micrococcal nuclease, and exonuclease III. It is concluded that since the radius of gyration of the DNA in the tetramer particle and its maximum dimension are very close to those of the core particle, no expansion occurs on removal of all the H2A and H2B. Nuclease digestion results indicate that histones H3/H4 in the tetramer particle protect a total of 70 bp of DNA that are centrally located within the 146 bp. Within the 70 bp DNA length, the two terminal regions of 10 bp are, however, not strongly protected from digestion. The optical melting profile of both particles can be resolved into three components and is consistent with the model of histone protection of DNA proposed from nuclease digestion. The structure proposed for the tetrameric histone complex bound to DNA is that of a compact particle containing 1.75 superhelical turns of DNA, in which the H3 and H4 histone location is the same as found for the core particle in chromatin by histone/DNA cross-linking [Shick, V. V., Belyavsky, A. V., Bavykin, S. G., & Mirzabekov, A. D. (1980) J. Mol. Biol. 139, 491-517]. Optical melting of the hexamer particle shows that each (H2A/H2B)1 dimer of the core particle protects about 22 base pairs of DNA.

A further assessment of the sub-nucleosomal product, "peak A", from Physarum polycephalum.

Nuclease digestion studies of Physarum polycephalum nuclei (1-3) and nucleoli (4) over the past few years have been centred on a number of modified nucleosomal products which have been related to active-gene regions of the genome. We have re-investigated one such particle, peak A, using the techniques of differential melting and polyacrylamide gel electrophoresis and show that this material is unlikely to be a specific histone:DNA complex as suggested by earlier authors.

Higher-order structures of chromatin in solution.

Neutron scatter studies have been made on gently prepared chicken erythrocyte chromatin over a range of ionic strength. At low ionic strength the mass per unit length of the '10 nm nucleofilament corresponds to one nucleosome per 8--12 nm and a DNA packing ratio of between 6 and 9. From the contrast dependence of the cross-section radius of gyration of the nucleofilament the following parameters have been obtained; RgDNA' the cross-section radius of gyration (Rg) when DNA dominates the scatter; RgP, the cross-section Rg when protein dominates the scatter; Rc, the cross-section Rg at infinite contrast and alpha, the constant which describes the dependence of the cross-section Rg on contrast variation. From our understanding of the structure of the core particle, various arrangement of core particles in the nucleofilament have been tested. In models consistent with the above parameters the core particles are arranged edge-to-edge or with the faces of the core particles inclined to within 20 degrees to the axis of the nucleofilament. With increase of ionic strength the transition to the second-order chromatin structure has been followed. This gave the interesting result that above 20 microM NaCL or 0.4 mM MgCL2 the cross-section Rg increases abruptly to about 9 nm with a packing ratio of 0.2 nucleosome/mn and with further increase of ionic strength the Rg increases to 9.5 nm while the packing ratio increases threefold to 0.6 nucleosome/nm. This suggests a family of supercoils of nucleosomes which contract with increasing ionic strength. In its most contracted form the diameter of the hydrated supercoil has been found from the radial distribution function to be 34 nm. Models for the arrangements of core particles in the 34-nm supercoil are discussed.

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.

The subunit structure of the eukaryotic chromosome.

New strucutral data have been obtained from neutron scattering studies of chromatin. The concentration-dependent meridional peak at 10-11 nm comes from the interparticle spacing of a subunit structure. Peaks at 5.5 and 3.7 nm have a different contrast behaviour to those at 11.0 and 3.7 nm showing that histones and DNA have a different spatial arrangement in the subunit. A globular model in which apolar segments of histones from the core surrounded by DNA complexed with the basic segments of histones agrees with the data.

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.

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

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. & Schröter, 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.

New crystals of the histone core octamer diffract to higher resolution, 2.65 A.

A new crystal form of the histone octamer, crystallized in 1.6 M KCl, 1.6 M phosphate, diffracts to appreciably better than 2.6 A resolution. The crystals have space group P6(1) or P6(5) and lattice parameters a = b = 158.29, c = 103.27 A, alpha = beta = 90, gamma = 120 degrees, with one molecule per asymmetric unit. The new crystals promise to yield more detail of the histone basic domains and a higher resolution structure for the histone octamer.

Small angle neutron scattering studies of chromatin subunits in solution.

Neutron scattering studies have been performed on dilute solutions of the fundamental subunit of chromatin, the nucleosome. The subunits contain approximately 195 base paris (bp) of DNA and histones H2A, H2B, H3, and H4. Measurements of the small angle scattering curves in various H2O/D2O solvents allow the contrast dependence of the radius of gyration of the subunits to be examined and give the mean scattering density of the particle. Further application of contrast variation to the higher angle scatter curves allows the contributions from the shape and internal structure of the subunits to be analyzed separately. From these results, we are able to propose a spherically averaged structure with most of the histones closely packed into a core of radius 3.2 nm surrounded by a loosely packed DNA-rich shell of 2.0 nm thickness resulting in a particle of 5.2 nm average radius. Model calculations for ellipsoids show that the outer shape of the subunit must have an axial ratio between 0.5 and 1.4 but is probably best described by more spherical particle. These results are correlated with the diffraction from chromatin films to provide an explanation for some of the diffraction rings.

Purification of histone core octamers and 2.15 A X-ray analysis of crystals in KCl/phosphate.

Intact histone octamers, produced by a new method quickly and in bulk, were crystallized in KCl/phosphate, and the X-ray data were analysed to 2.15 A, confirming a P65 space group. This environment preserves the high-resolution structure of the octamers and will be useful for studying them with other functionally important molecules. The octamers form into left-handed superhelices hexagonally spaced by 158.65 A, having a pitch of 102.57 A with six octamers per turn. A dipotassium tetraiodo mercurate derivative had good phasing power and should prove valuable in refining the structure after molecular-replacement analysis with lower resolution coordinates; the heavy atom was isomorphously placed at a unique site between the two H3-cysteine residues in the octamer.

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.

Structure of the histone-core octamer in KCl/phosphate crystals at 2.15 A resolution.

The structure of the native chicken histone octamer, crystallized in 2 M KCl, 1.35 M potassium phosphate pH 6.9, has been refined at 2.15 A resolution to a final R factor of 21.4% and an R(free) of 25.2%. Unique crystal-packing interactions between histone-core octamers are strong and one of them (area 4000 A(2)) involves two chloride ions and direct interactions between six acidic amino-acid residues on one octamer and the equivalent number of basic residues on the next. These interactions are on the structured part of the octamer (not involving tails). Five phosphate ions, 23 chloride ions and 437 water molecules have been identified in the structure. The phosphate and some chloride ions bind to basic amino-acid residues that interact with DNA in the nucleosome. The binding of most of the anions and the packing interactions are unique to these crystals. In other respects, and including the positions of four chloride ions, the octamer structure is very close to that of octamers in nucleosome-core particle crystals, particularly with respect to 'docking' sequences of the histone H2As and H4s. These sequences together with the H2B-H4 four-helix bundles stabilize the histone structure in the nucleosome and prevent the dissociation of the (H2A-H2B) dimers from the (H3-H4)(2) tetramer. Possible reasons why this happens at high salt in the absence of DNA are given.

Neutron and x-ray scatter studies of the histone octamer and amino and carboxyl domain trimmed octamers.

The structure of the nucleosome has been under intense investigation using neutron crystallography, x-ray crystallography, and neutron solution scattering. However the dimension of the histone octamer inside the nucleosome is still a subject of controversy. The radius of gyration (Rg) of the octamer obtained from solution neutron scattering of core particles at 63% 2H2O, 37% 1H2O is 33 A, and x-ray crystallography study of isolated histone octamer gives a Rg of 32.5 A, while the reported values using x-ray crystallography of core particles from two individual studies are 29.7 and 30.4 A, respectively. We report here studies of isolated histone octamer and trypsin-limited digested octamer using both neutron solution scattering and small angle x-ray scattering. The Rg of the octamer obtained is 33 A, whereas that of the trimmed octamer is 29.8 A, similar to the structure obtained from the crystals of the core particles. The N-terminal domains of the core histones in the octamer have been shown by high resolution nuclear magnetic resonance (Schroth, G.P., Yau, P., Imai, B.S., Gatewood, J.M., and Bradbury, E.M. (1990) FEBS Lett. 268, 117-120) to be mobile and flexible; it is likely that these regions are disordered and "not seen" by x-ray crystallography.