Organization of nucleosomes and spacer DNA in chromatin fibres

In this paper we analyse in detail the orientation of X-ray diffraction diagrams obtained from the following materials: nucleosome cores, whole nuclei and the sodium and thallium salts of H1-depleted nucleohistone and of briefly digested chromatin. Our analysis indicates that spacer DNA is organized in bundles of parallel segments which contribute to the equatorial maxima in the diagrams. Several models are compatible with this organization, in particular a modified solenoid model in which the central part is filled with such a bundle of spacer DNA segments parallel to the axis of the fibre. It is also shown that spacer DNA is covered by histones, probably the N-terminal regions. This observation indicates that the differential activity of nucleases on chromatin is strongly influenced by conformational features of DNA. An analysis of the orientation of the low angle rings found in the X-ray diffraction patterns of H1-depleted nucleohistone shows that the 11 nm peak has maxima which are ～ 0.007 nm^?1 off the meridian. The 5.5 and 8 nm peaks have a meridional maximum plus two side maxima which occur at spacings between 0.02 and 0.055 nm^?1 from the meridian, depending on the conditions. A comparison of these results with those reported by Finch et al.¹ for crystals indicates that in fibres the nucleosome cores are arranged with their short axis perpendicular to the axis of the fibre. Some evidence on the path of DNA in the nucleosome cores is also obtained.     

Neutron scattering studies of subcomponent C1q of first component C1 of human complement and its association with subunit C1r2C1s2 within C1

Neutron scattering studies are reported on subcomponent C1q of component C1 of human complement, and on C1, the complex of C1q with subunit C1r₂C1s₂. For C1q, the molecular weight was determined as 460,000. The radius of gyration at infinite contrast R_c is 12.8 nm. The R_c values for the proteolytically cleaved forms of C1q, namely the heads and the stalks, are 1.5 to 2 nm and 11 nm, respectively, and thus the axis-to-arm angle of C1q is estimated at 45 °. Neutron data for subunit C1r₂C1s₂ are published elsewhere. The neutron data on C1 lead to an R_c value of 12.6 nm for proenzymic C1 and a molecular weight of 820,000. The wideangle scattering curve of C1q exhibits a minimum at Q = 0.28 nm^?1 and a maximum at 0.39 nm^?1; on the addition of C1r₂C1s₂, this minimum disappears. The neutron data on C1 indicate that C1q and C1r₂C1s₂ have complexed with a large conformational change in one or both parts. No conformational changes can be detected on the activation of C1 by this method.     

Molar extinction coefficients and other properties of an improved reaction center preparation from Rhodopseudomonas viridis

Reaction centers have been purified from chromatophores of Rhodopseudomonas viridis by treatment with lauryl dimethyl amine oxide followed by hydroxyapatite chromatography and precipitation with ammonium sulfate. The absorption spectrum at low temperature shows bands at 531 and 543 nm, assigned to two molecules of bacteriopheophytin b. The 600 nm band of bacteriochlorophyll b is resolved at low temperature into components at 601 and 606.5 nm. At room temperature the light-induced difference spectrum shows a negative band centered at 615 nm, where the absorption spectrum shows only a weak shoulder adjacent to the 600 nm band. The fluorescence spectrum shows a band at 1000 nm and no fluorescence corresponding to the 830 nm absorption band. Two molecules of cytochrome 558 and three of cytochrome 552 accompany each reaction center. The differential extinction coefficient (reduced minus oxidized) of cytochrome 558 at 558 nm was estimated as 20 ± 2 mM^?1 · cm^?1 through a coupled reaction with equine cytochrome c. The extinction coefficient of reaction centers at 960 nm was determined to be 123 ± 25 mM^?1 · cm^?1 by measuring the light-induced bleaching of P-960 and the coupled oxidation of cytochrome 558. The corresponding extinction coefficient at 830 nm is 300 ± 65 mM^?1 · cm^?1. The absorbance ratio $\text{a}{}_{\mathrm{<mtext>280</mtext><mtext>nm</mtext>}}\text{a}{}_{\mathrm{<mtext>830</mtext><mtext>nm</mtext>}}$ in our preparations was 2.1, and there was 190 kg protein per mol of reaction centers. Sodium dodecyl sulfate-polyacrylamide gel electrophoresis showed three major components of apparent molecular weights 31 000, 37 000 and 41 000.     

X-ray small-angle scattering study of mononucleosomes and of the close packing of nucleosomes in polynucleosomes

The radius of gyration of mononucleosomes determined by X-ray small-angle scattering is 4.35 nm. The maximum dimension determined from the distance distribution function and the volume amount to 12.9 nm and 370 nm³, respectively. For a particular fraction of polynucleosomes a mean radius of gyration 16 nm, a maximum dimension 65 nm, and a mean volume 25,240 nm³ is obtained.The shape is approximated by an elongated cylinder having a diameter of 28 nm. A polynucleosome is built up from 69 nucleosomes, on the average. The distance of neighbouring nucleosomes in the polynucleosome amounts to 5.2 nm. Moreover, this distance shows that the nucleosomes in the polynucleosome are very closely packed.     

The superstructure of chromatin and its condensation mechanism

Changes in the structure of chicken erythrocyte chromatin fibres at low ionic strength resulting from enzymatic digestion, thermal denaturation and binding of Netropsin and Distamycin were monitored by synchrotron X-ray solution scattering. Digestion with micrococcal nuclease confirms the previous assignment of the 0.05 nm^-1 band to an interference between nucleosomes with an average distance of 23 nm. The results of thermal denaturation indicate that above 40°C there is a progressive increase of the internucleosomal distance and that above 60°C the characteristic structure of the chromatin fibre is destroyed. Binding of Netropsin and Distamycin also results in an increase of the internucleosomal distance which can be estimated to correspond to about 0.2 nm/mol.     

Collagen fibril morphology in developing chick metatarsal tendoms: 1. X-ray diffraction studies

The low angle equatorial X-ray diffraction ($\text{R ? 30 μ}\text{m}{}^{\mathrm{?1}}$) from hydrated embryonic chick metatarsal tendon contains minima and maxima that are not seen in mature tendons. This diffraction derives from the disordered array of parallel, cylindrical fibrils of collagen of small, uniform diameter that comprise the major part of this tissue. Comparison of the positions of the minima and maxima with those expected from an array of cylinders allows estimation of the mean diameter of the cylinders and the average centre-to-centre nearest neighbour separation. It was found that in the age range from 13 to 19 days fetal, the mean diameter increased from ～ 46 to ～ 58 nm, whereas the mean nearest neighbour separation remained constant at ～ 90 nm. Detailed analysis of the X-ray intensity profile of a 17 day fetal tendon indicated the presence of a paucidisperse distribution of fibril diameters with two or more discrete populations of preferred diameters separated by 10 to 12 nm.     

Neutron scattering on nuclei.

Very small angle neutron scattering studies have been made on intact nuclei under a variety of solution conditions. Scattering maxima are observed at 30 to 40 nm and at 18 nm in most environments. Although the spacing, intensity and presence of the maximum near 40 nm varies considerably with environment the 18 nm is rather constant. The 30 to 40 nm maximum appears to be best interpreted by the presence of 35 to 50 nm diameter fibers in nuclei. An important result is that no scattering maximum was observed near 11 nm, suggesting that a tightly super coiled nucleofilament with such a pitch is not present.     

Bovine sperm chromatin is not protected from the effects of ultrasmall gold nanoparticles

The response of ejaculated bovine spermatozoa to gold nanoparticles was studied by the standard method of nuclear chromatin decondensation in vitro. After the treatment of semen samples with a hydrosol containing gold nanoparticles with an average diameter of ～3.0 nm and a concentration of 1 × 10¹⁵ particles/mL, the ability of sperm nuclei to decondense in the presence of sodium dodecyl sulfate (SDS) and dithiothreitol (DTT) dramatically changed compared to the control. The frequencies of gametes with nondecondensed (“intact”), partially decondensed, and completely decondensed nuclei correlated as 40: 32: 28% and 0: 36: 64% in the experiment and the control, respectively. Moreover, the appearance of a sufficiently large number of gametes with destructed and almost completely destroyed nuclei was noticed in the spermatozoa treated with gold nanoparticles. This article suggests the putative mechanisms of action of ultrasmall gold nanoparticles on the structural and functional integrity of the deoxyribonucleoprotein (DNP) complex of mature male gametes.     

Electron microscopy of human interphase nuclei

Quantitative electron microscopy was used to analyze surface-spread, critical-point-dried human interphase nuclei and chromatin. The following information is presented: (1) Unstimulated interphase nuclei of lymphocytes from peripheral blood have a mean dry mass of 50.30×10^?12 g. The mean dry mass of stimulated nuclei of lymphocytes was determined to be 59.34×10^?12 g, a significant statistical difference from the unstimulated ones. (2) Mean diameter of chromatin fibers and mean fiber mass per micron were 199ű15% coefficient of variation (C.V.) and 5.95×10^?16g×29% C.V., respectively. (3) A line of regression of fiber mass on fiber diameter for 83 fibers indicated that a 200-Å fiber has a mass of 5.86×10^?16g/μ, or almost the same as the mean fiber mass of 5.95× 10^?16g/μ. (4) With the value 7×10^?12g for the DNA content of an unstimulated lymphocyte nucleus, a total length of 215 cm is calculated for the DNA double helix. When this length is compared to the mean length of chromatin fiber per nucleus (7.59 cm), a ratio of 28.3 to 1 results, which is called the DNA-packing ratio. (5) This DNA-packing ratio of 28.3 is reasonably close to the packing ratio of 26.9 suggested from model calculations for the second DNA supercoil in a 200-Å chromatin fiber.     

Molecular size and shape of the native and reassociated forms of the extracellular haemoglobin of Tubifex tubifex

The extracellular haemoglobin of Tubifex tubifex and the product of its reassociation at neutral pH subsequent to dissociation at alkaline pH, were examined by small-angle X-ray scattering. The following molecular parameters were determined for the native and reassociated molecules, respectively: maximum diameter 30.0±1.0 and 32.0±1.0nm; radius of gyration 10.66±0.15 and 11.07±0.15 nm; molecular weight (3.09±0.15) × 10⁶ and (2.99±0.15) × 10⁶ dalton. Although the scattering curves of the native and reassociated haemoglobin possess similar shapes the distance distribution functions exhibit slight differences in their shape as well as in the position of their maximum. The best fit with the experimental distribution functions was obtained with models consisting of 12 spheres arranged in two hexagonal layers. In the case of the native haemoglobin each of the 12 spheres has a diameter of 9.3 nm while for the reassociated haemoglobin each of the 12 spheres has a diameter of 11.5 nm. The results suggest that although their molecular weights are the same, the reassociated molecule is slightly larger than the native molecule     

Quaternary structure of immunoglobulin m: A model based on small-angle X-ray scattering data

This paper presents some data on a human Waldenström immunoglobulin M.IgM_GAL based on small-angle X-ray scattering data. the IgM_GAL had molecular weight 970 000, volume 1760 nm³, radius of gyration 12 nm and maximum diameter 37 nm. The conclusions from various model calculations are discussed. A flat, star-shaped model is compatible both with X-ray scattering data and electron micrographs.     

Small-angle X-ray studies of Lumbricus terrestris haemoglobin

Small-angle X-ray scattering of Lumbricus terrestris haemoglobin was measured in dilute solutions in 0.1 M Tris HCl buffer, pH 7.0. The following molecular parameters were determined: radius of gyration 11.2 nm, volume 7700 nm³, maximum diameter 29 nm, molecular weight 3.95 × 10⁶. The experimental scattering curve was compared with the scattering curves and distance distribution functions calculated for various models. The overall shape of the haemoglobin could be approximated by a hollow cylinder with the following dimensions: outer radius 13.5 nm, inner radius 5.4 nm, height 16.0 nm. The best fit was obtained with a model which consists of 12 large subunits arranged in two superimposed hexagonal rings with a number of smaller subunits between the large subunits and in the centre of the molecule.     

Influence of chromatin structure, antibiotics, and endogenous histone methylation on phosphorylation of histones H1 and H3 in the presence of protein kinase A in rat liver nuclei in vitro

In vitro phosphorylation of histones H1 and H3 by cAMP-dependent protein kinase A and endogenous phosphokinases in the presence of [γ-³²P]ATP was studied in isolated rat liver nuclei with different variants of chromatin structural organization: condensed (diameter of fibrils 100–200 nm; N-1) and partly decondensed (diameter of fibrils ～30 nm; N-2). In the N-1 state histone, H1 is phosphorylated approximately twice as much than histone H3. Upon the decondensation of the chromatin in the N-2 state, 1.5-fold decrease of total phosphorylation of H1 is observed, while that of H3 does not change, although the endogenous phosphorylation of both histones is reduced by half. Changes in histone phosphorylation in the presence of low or high concentrations of distamycin and chromomycin differ for H1 and H3 in N-1 and N-2. It was found that distamycin (DM) stimulates the phosphorylation of tightly bound H1 fraction, which is not extractable by polyglutamic acid (PG), especially in N-1. Chromomycin (CM) increases the phosphorylation of both histones in PG extracts and in the nuclear pellets, particularly in N-2. At the same time, in N-1 one can detect phosphorylation of a tightly bound fraction of histones H1 whose N-termini are located on AT-rich sites that become inaccessible for protein kinase in the process of chromatin decondensation in N-2. At the same time, in N-2 the accessibility for protein kinase A of tightly bound H1 fractions, whose N-termini are located on GC-rich sites, increases dramatically. High concentrations of both CM and DM in N-1 and N-2 stimulated phosphorylation of the non-extractable by PG fraction of H1 whose N-termini are located on sites where AT ≈ GC. CM at high concentration stimulated 4–7 times the phosphorylation of a small fraction of H3, which is extracted by PG from both types of nuclei. We detected an effect of endogenous methylation of histones H1 and H3 in the nuclei on their subsequent phosphorylation depending on the chromatin structure, histone-chromatin binding strength, and concentration of DM.     

Small angle scattering of cell nuclei

Neutron and X-ray small angle scattering techniques have been applied to study chromatin structure inside different types of cell nuclei. Scattering from genetically inactive chicken erythrocyte nuclei exhibits a maximum at Q = 0.1-0.15 nm-1 which cannot be observed by studying isolated chromatin derived from the same kind of cells. In highly active transcribing rat liver nuclei such a nuclear pattern is absent. The radius of gyration of isolated "superbeads" was determined. It is discussed whether the characteristic maximum of the nuclei originates from this superstructural organisation of chromatin. Rat liver nuclei were fractionated on sucrose gradients in order to determine whether the absence of the extra maximum in scattering profiles of these nuclei is due to overlapping effects of different chromatin organisation in the various cell types of the liver. As compared to unfractionated nuclei no strong deviations in the scattering profiles of the fractions could be observed. Erythrocyte nuclei were dialysed in buffers differing in the ionic strength of monovalent cations. The typical maximum from the nuclei is shifted from 60 nm (very low salt concentration) to about 35 nm (physiological ionic strength) and is linearly proportional to the decreasing radius of the nuclei. In conclusion, chromatin structure inside the nucleus has a scattering maximum due to an ordered packing of the fibres which is absent in nuclei with high genetic activity.     

Ionic strength-dependent conformational transitions of chromatin. Circular dichroism and thermal denaturation studies

High-molecular-weight chicken erythrocyte chromatin was prepared by mild digestion of nuclei with micrococcal nuclease. Samples of chromatin containing both core (H3, H4, H2A, H2B) and lysine-rich (H1, H5) histone proteins (whole chromatin) or only core histone proteins (core chromatin) were examined by CD and thermal denaturation as a function of ionic strength between 0.75 and 7.0 × 10^?3M Na⁺. CD studies at 21°C revealed a conformational transition over this range of ionic strengths in core chromatin, which indicated a partial unfolding of a segment of the core particle DNA at the lowest ionic strength studied. This transition is prevented by the presence of the lysine-rich histones in whole chromatin. Thermal-denaturation profiles of both whole and core chromatins, recorded by hyperchromicity at 260 nm, reproducibly and systematically varied with the ionic strength of the medium. Both materials displayed three resolvable thermal transitions, which represented the total DNA hyperchromicity on denaturation. The fractions of the total DNA which melted in each of these transitions were extremely sensitive to ionic strength. These effects are considered to result from intra- and/or internucleosomal electrostatic repulsions in chromatin studied at very low ionic strengths. Comparison of the whole and core chromatin melting profiles indicated substantial stabilization of the core-particle DNA by binding sites between the H1/H5 histones and the 140-base-pair core particle.     

Structure of bacterial extracellular polymeric substances at different pH values as determined by SAXS

Extracellular polymeric substances (EPS) play an important role in cell aggregation, cell adhesion, and biofilm formation, and protect cells from a hostile environment. The EPS was isolated by trichloroacetic acid/ethanol extraction from broth culture of a marine bacterium isolate. The EPS was composed of glucose and galactose as determined by HPLC and TLC; the protein content was on average 15 ± 5% of EPS dry mass. The solution structure of EPS at different values of pH was revealed by small-angle x-ray scattering. Scattering curves of EPS solutions (0.4%, w/v) consistently showed two nearly linear log-log regions with slopes a and b in the q-ranges from 0.06 nm⁻¹ to 0.26 nm⁻¹, and from 0.27 nm⁻¹ to 0.88 nm⁻¹, respectively. Slope a was sensitive to pH changes whereas slope b was not. The observed sensitivity to pH was not a consequence of ionic strength variation with pH, as checked by salt addition. The pH variation causes major rearrangements of EPS structure mainly at length scales above 24 nm. To get a better understanding of the pH effect on EPS structure, the original model proposed by Geissler was refined into a mathematical model that enabled fitting of the experimental scattering curves in the pH range from 0.7 to 11.0. The model describes EPS structure as a network of randomly coiled polymeric chains with denser domains of polymeric chains. The results obtained from the model indicate that dense domains increase in average size from 19 nm at pH 11.0 to 52 nm at pH 0.7. The average distance between the polysaccharide chains at pH 0.7 was 2.3 nm, which indicates a compact EPS structure. Swelling was found to be at a maximum around pH = 8.8, where the average distance between the chains was 4.8 nm.     

Small-angle x-ray studies on malate synthase from baker's yeast.

Malate synthase was investigated in solution by the small-angle X-ray scattering technique. The substrate-free enzyme was shown to have a molecular weight of 186000, a radius of gyration of 3.96 nm, a maximum particle diameter of 11.2 nm, a volume of 343 nm³, a radius of gyration of the thickness of 1.04 nm, and an axial ratio of 1:0.33. The enzyme molecule undergoes small changes in overall structure upon binding substrates. Investigation of the enzyme under prolonged exposure to X-rays led to an aggregation of the enzyme and allowed statements concerning the way of aggregation and factors influencing aggregation.     

A circular dichroic absorption study of the reaction of oxidized pyridine nucleotides with cyanide ions.

A Circular Dichroic absorption study of the reaction of oxidized pyridine nucleotides with cyanide ions fully confirms the occurence of a very weak Cotton effect around 435 nm in the Circular Dichroic spectrum of the reduced coenzymes and therefore the very faint transition (λ_max = 435 nm; ?_max ～ 1 M^?1 cm^?1) from which the Cotton effect originates.     

PRIMARY PRODUCTION OF CRUSTOSE CORALLINE RED ALGAE IN A HIGH ARCTIC FJORD1

Crustose coralline algae occupied ～1%–2% (occasionally up to 7%) of the sea floor within their depth range of 15–50 m, and they were the dominant encrusting organisms and macroalgae beyond 20 m depth in Young Sound, NE Greenland. In the laboratory, oxygen microelectrodes were used to measure net photosynthesis (P) versus downwelling irradiance (E_d) and season for the two dominant corallines [Phymatolithon foecundum (Kjellman) Düwel et Wegeberg 1996 and Phymatolithon tenue (Rosenvinge) Düwel et Wegeberg 1996] representing> 90% of coralline cover. Differences in P‐E_d curves between the two species, the ice‐covered and open‐water seasons, or between specimens from 17 and 36 m depth were insignificant. The corallines were low light adapted, with compensation irradiances (E_c) averaging 0.7–1.8 μmol photons·m ^{? 2}·s ^{? 1} and light adaptation (E_k) indices averaging 7–17 μmol photons·m ^{? 2}·s ^{? 1}. Slight photoinhibition was evident in most plants at irradiances up to 160 μmol photons·m ^{? 2}·s ^{? 1}. Photosynthetic capacity (P_m) was low, averaging 43–67 mmol O₂·m ^{? 2} thallus·d ^{? 1} (～250–400 g C·m ^{? 2} thallus·yr ^{? 1}). Dark respiration rates averaged ～5 mmol O₂·m ^{? 2} thallus·d ^{? 1}. In ice covered periods, E_d at 20 m depth averaged ～1 μmol photons·m ^{? 2}·s ^{? 1}, with daily maxima of 2–3 μmol photons·m ^{? 2}·s ^{? 1}. During the open water season, E_d at 20 m depth averaged ～7 μmol photons·m ^{? 2}·s ^{? 1} with daily maxima of ～30 μmol photons·m ^{? 2}·s ^{? 1}. Significant net primary production of corallines was apparently limited to the 2–3 months with open water, and the small contribution of corallines to primary production seems due to low P_m values, low in situ irradiance, and their relatively low abundance in Young Sound.     

The regulation of liver glycogen synthetase D phosphatase by ATP and glucose

Cortisol at a concentration of 5×10^?6M induces profound changes in U.V. absorption spectra of isolated nuclei from rat liver and thymus. The changes occur within the first 10 min of cortisol action. In both types of nuclei, a blue shift of 5–10 nm from the normal absorption maximum at 260–270 nm is evident. In addition, liver nuclei exhibit an elevation of the spectrum at 230–270 nm (increased U.V. absorption), while the spectrum of thymus nuclei becomes flattened. No such changes occur in nuclei exposed to a physiologically inactive hormone (pregnenolone). The results are interpreted as evidence for cortisol-induced perturbations in deoxyribonucleoprotein structure with consequent changes in the degree of condensation of nuclear chromatin.