Study of the internal structure of Escherichia coli ribosomes by neutron and x-ray scattering.

Neutron scattering curves of the small and large subparticles of Escherichia coli ribosomes are presented over a wide range of scattering angles and for several contrasts. It was verified that the native ribosome structure was not affected by ²H₂O in the buffer. The reliability of the neutron scattering curves, obtained in H₂O buffer, was established by X-ray scattering experiments on the same material.The non-homogeneous distribution of RNA and protein in the subparticles of E. coli ribosomes is confirmed, with RNA predominantly within the particle and protein predominantly on its periphery. The distances between the centres of gravity of the RNA and protein components do not exceed 25 Å and 30 Å, in the large and small subparticles, respectively.The volume occupied by the RNA within the large and small subparticles is determined. The ratio of the “dry” volume of the RNA to the occupied volume is found to be 0.56; it is the same in both subparticles. Such packing of RNA is characteristic of single helices of ribosomal RNA at their crystallization and of the helices in transfer RNA crystals. A conclusion is drawn that RNA in ribosomes is in a similar state.Experimental scattering curves for the small subparticle depend significantly on the contrast in the angular region in which the scattering is mainly determined by the particle shape. The scattering curve, as infinite contrast is approached, is similar to that calculated for the particle as observed by electron microscopy. Thus, the long-existing contradiction between electron microscopy data (an elonggated particle with an axial ratio 2:1) and X-ray data (an oblate particle with an axial ratio 1:3.5), concerning the overall shape of the 30 S subparticle, is settled in favour of electron microscopy. The experimental neutron scattering curve of RNA within the small subparticle is well-described by the V-like RNA model proposed recently by Vasiliev et al. (1978).Experimental data are given to support the hypothesis that the maxima in the X-ray scattering curves, in the region of scattering angles corresponding to Bragg distances of 90 to 20 Å, arise from the ribosomal RNA component alone. It is shown that the prominence of the peaks in this region of the scattering curve depends only on the scattering fraction of the RNA component. The scattering fraction can be changed both by using the “native contrast” (ribosomal particles containing different amounts of protein) and by varying the solvent composition. The maxima are most pronounced where the RNA scattering fraction is highest or in solvents where the protein density is matched by the solvent. The scattering vectors of the maxima in the X-ray and neutron scattering curves, however, remain unchanged. This allows us to propose the tight packing of RNA as a common principle for the structural arrangement of RNA in ribosomes.     

Molecular dynamics simulations of palmitoyloleoylphosphatidylglycerol bilayers

Phosphatidylglycerol (PG) is one of the important components of biological membranes, but there is a paucity of experimental data to test the accuracy of molecular dynamics (MD) simulations. This work consists of testing the accuracy of the CHARMM36 (C36) lipid force field on 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphoglycerol (POPG) lipid bilayers. MD simulations of POPG lipid bilayers are compared to recently available X-ray and neutron scattering and deuterium NMR measurements. Overall, the C36 lipid force field accurately represents the X-ray and neutron form factors, bilayer and hydrocarbon thicknesses and chain deuterium order parameters. The surface area per lipid from MD simulations with C36 (67.7 ± 0.2 Å²) is in excellent agreement with the experimentally determined value of 66.0 ± 1.3 Å². C36 outperforms the lipid force field developed by Berger et al. [15] and suggests that past studies with this force field may result in lateral areas that are too small. Moreover, our studies give some insight into the structural model used in experiments and suggest that the functional form for the head group may not be Gaussian-like. Based on our simulations, the POPG lipid in the C36 lipid force field is well parameterised and can be used for other PG lipids and membrane models with mixed lipids.     

Amylose conformation in aqueous solution: a small-angle X-ray scattering study

An investigation of the small-angle X-ray scattering properties of aqueous solutions of an amylose derivative has been carried out. Experiments have been conducted in stable and fairly concentrated polymer solutions (up to 3.2%) by using a slightly substituted carboxymethylamylose having a degree of substitution of 0.08. Scattering intensities display a maximum in the low angle range which prevents extrapolation of the angular dependence to zero angle. Data obtained in the range of scattering vector 0.01<η<0.1Å^?1 yield 8 Å as the radius of gyration of the chain cross-section and 140 dalton Å^?1 as the mass per unit length. These results are analysed in terms of the current model of amylose solution conformation and compared with the theoretical calculations of the Debye scattering function of the isolated chain.     

Structural investigations of influenza B virus

Purified preparations of influenza B/Hong Kong/5/72 have been characterized by hydrodynamical measurements, electron microscopy and small-angle neutron scattering. As judged by these techniques the preparations are highly monodisperse, the virus particles being spherical and of molecular weight about 200 × 10⁶. The lipid bilayer is located at a radius of 425 Å and its molecular weight is estimated to be 60 × 10⁶, constituting about 30% of the total virus mass. The external radius is about 580 Å.     

Changes in the x-ray solution scattering of aspartate transcarbamylase following the allosteric transition.

Aspartate transcarbamylase (Escherichia coli) has been studied by X-ray solution scattering in the s range 0.002 to 0.06 Å^?1. The spectra display sharp maxima and minima whose positions and amplitudes show considerable changes upon ligation with the transition state analogue N-(phosphonacetyl)-l-aspartate. The magnitude of the change in diffraction pattern is so large that X-ray solution scattering should be a useful technique for studying the proportions of different quaternary forms in solutions of this enzyme. In particular, the kinetics of the allosteric transition appear to be within the reach of X-ray diffraction experiments.Some structural parameters of the allosteric transition were obtained from the diffraction patterns. The radius of gyration of the native enzyme is 45.9 ± 0.5 Å, and after ligation it increases to 48.4 ± 1.0 Å. At the same time, the peak of the pair distribution function is shifted from 58 Å to 63 Å. These changes indicate that the molecule swells after the allosteric transition to the R form. However, the maximum distance (from the pair distribution function) does not increase after ligation, and may even decrease slightly. Some probable subunit movements during allosteric activation are discussed.     

The structure of lipid bilayers and the effects of general anaesthetics: An X-ray and neutron diffraction study

We have looked for the effects of three clinically used inhalational anaesthetics (nitrous oxide, halothane and cyclopropane) on the structure of lecithin/ cholesterol bilayers. The anaesthetics were delivered to the membranes in the gaseous phase, so that effects at clinical concentrations could be determined.High-resolution X-ray diffraction patterns were recorded out to 4 Å and analyzed using swelling experiments. Parallel neutron diffraction experiments were performed and analyzed using H₂O-²H₂O exchange. Methods were developed which enabled us to obtain confidence limits for the X-ray and neutron structure factors.The resultant X-ray and neutron scattering density profiles clearly define the positions of the principal molecular groups in the unperturbed bilayer. In particular, the high-resolution electron density profiles reveal features directly attributable to the cholesterol molecule. A comparison with the neutron scattering density profiles shows that cholesterol is anchored with its hydroxyl group at the water/hydrocarbon interface, aligned with the fatty acid ester groups of the lecithin molecule. We suggest that this positioning of the cholesterol molecule allows it to act as a thickness buffer for plasma membranes.In the presence of very high concentrations of general anaesthetics, the bilayers show increased disorder while maintaining constant membrane thickness. At surgical concentrations, however, there are no significant changes in bilayer structure at 95% confidence levels. We briefly review the literature previously used to support lipid bilayer hypotheses of general anaesthesia. We conclude that the lipid bilayer per se is not the primary site of action of general anaesthetics.     

X-Ray Characterization of Melanins—I

The intrinsic local structure characterization of natural sepia melanin and L-dopa and tyrosine synthetic melanin powder has been carried out by X-ray diffraction using synchrotron radiation. The derived structure factor, S(q), shows six significant diffuse peaks within the q-range from 0.3 Å^-1 to 16 Å^-1 in the reciprocal space (q= (4π sin θ)/λ, 2θ is the scattering angle). The Fourier transform of S(q), which yields the radial distribution function (RDF), gives us information in real space of a 1.42 Å distance averaged over the C-C, C-O and C-N bond lengths as well as peaks at 2.40-2.41 Å, 3.67-3.71 Å and 4.67-4.70 Å discrete neighbor distances. There is a great similarity in the scattering intensity profiles of the natural and synthetic melanins indicating that the synthetically prepared material may be essentially similar to “real” melanin in its local atomic arrangements. An evidence of a prepeak at q = 0.45 Å^-1 has been confirmed which indicates a preferred length scale of ～ 13-20 Å that corresponds to the initial particle size in colloidal melanin solutions.     

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 $\text{C = 23.5}\text{A}\text{?}$.     

Yeast tRNAAsp-Aspartyl-tRNA Synthetase Complex: Low Resolution Crystal Structure

Abstract

Yeast aspartyl-tRNA synthetase, a dimer of molecular weight 125000, and two molecules of its cognate tRNA (M_r = 24160) cocrystallize in the cubic space group 1432 (a = 354 Å). The crystal structure was solved to low resolution using neutron and X-ray diffraction data. Neutron single crystal diffraction data were collected in five solvents differing by their D₂O content in order to use the contrast variation method to distinguish between the protein and tRNA The synthetase was first located at 40 Å resolution using the 65% D₂O neutron data (tRNA matched). tRNA molecules were found at 20 Å resolution using both neutron and X-ray data. The resulting model was refined against 10 Å resolution X-ray data, using density modification and least-squares refinement of the tRNA positions. The crystal structure, solved without a priori phase knowledge, was confirmed later by isomorphous replacement. The molecular model of the complex is in good agreement with results obtained in solution by probing the protected part of the tRNA by chemical reagents.     

Conformation of <Emphasis Type="Italic">Thermus thermophilus</Emphasis> ribosomal protein S1 in solution at different ionic strengths

Small-angle x-ray and neutron scattering were used to study the structure of the ribosomal protein S1 (61 kDa) from Thermus thermophilus in solution at low and moderate ionic strength (0 and 100 mM NaCl). The protein was found to be globular in both cases. Modeling of the S1 structure comprising six homologous domains on the basis of the NMR data for one domain showed that the best fit to scattering data was provided by compact domain packing. The calculated gyration radius was 28–29 Å, as typical of globular proteins about 60 kDa. The protein was prone to self-association, forming mainly dimers and trimers at moderate ionic strength and higher compact associates at low ionic strength. Neutron scattering assays in heavy water at 100 mM NaCl revealed markedly elongated associates. The translational diffusion coefficient calculated for S1 at 100 mM NaCl from dynamic light scattering was markedly lower than the one expected for its globular monomer (D _20,w = (2.7 ± 0.1)·10^?7 versus (5.8–6.0)·10^?7 cm² s^?1), confirming protein association under equilibrium conditions.     

Structure of Fully Hydrated Fluid Phase Lipid Bilayers with Monounsaturated Chains

Quantitative structures are obtained at 30°C for the fully hydrated fluid phases of palmitoyloleoylphosphatidylcholine (POPC), with a double bond on the sn-2 hydrocarbon chain, and for dierucoylphosphatidylcholine (di22:1PC), with a double bond on each hydrocarbon chain. The form factors F(q _z ) for both lipids are obtained using a combination of three methods. (1) Volumetric measurements provide F(0). (2) X-ray scattering from extruded unilamellar vesicles provides ΙF(q _z )Ι for low q _z . (3) Diffuse X-ray scattering from oriented stacks of bilayers provides ΙF(q _z )Ι for high q _z . Also, data using method (2) are added to our recent data for dioleoylphosphatidylcholine (DOPC) using methods (1) and (3); the new DOPC data agree very well with the recent data and with (4) our older data obtained using a liquid crystallographic X-ray method. We used hybrid electron density models to obtain structural results from these form factors. The result for area per lipid (A) for DOPC 72.4 ± 0.5 Ų agrees well with our earlier publications, and we find A = 69.3 ± 0.5 Ų for di22:1PC and A = 68.3 ± 1.5 Ų for POPC. We obtain the values for five different average thicknesses: hydrophobic, steric, head-head, phosphate-phosphate and Luzzati. Comparison of the results for these three lipids and for our recent dimyristoylphosphatidylcholine (DMPC) determination provides quantitative measures of the effect of unsaturation on bilayer structure. Our results suggest that lipids with one monounsaturated chain have quantitative bilayer structures closer to lipids with two monounsaturated chains than to lipids with two completely saturated chains.     

Neutron scattering studies of escherichia coli tyrosyl-trna synthetase and of its interaction with trna tyr

Small-angle neutron scattering studies of Escherichia coli tyrosyl-tRNA synthetase indicate that in solution this enzyme is a dimer of M_r, 91 (±6) × 10³ with a radius of gyration R_G of 37.8 ± 1.1 Å.The increase in the scattering mass of the enzyme upon binding tRNA^Tyr has been followed in 20 mm-imidazole · HCl (pH 7.6), 10 mm-MgCl₂, 0.1 mm-EDTA, 10 mm-2-mercaptoethanol, 150 mm-KCl. A stoichiometry of one bound tRNA per dimeric enzyme molecule was found. The R_G of the complex is equal to 41 ± 1 Å. Titration experiments in 74% ²H₂O, close to the matching point of tRNA, show an R_G of 38.5 ± 1 Å for the enzyme moiety in the complex. From these values, a minimum distance of 49 Å between the centre of mass of the bound tRNA and that of the enzyme was calculated.In low ionic strength conditions (20 mm-imidazole-HCl (pH 7.6), 10 mm-MgCl₂, 0.1 mm-EDTA, 10 mm-2-mercaptoethanol) and at limiting tRNA concentrations with respect to the enzyme, titrations of the enzyme by tRNA^Tyr are characterized by the appearance of aggregates, with a maximum scattered intensity at a stoichiometry of one tRNA per two enzyme molecules. At this point, the measured M_r and R_G values are compatible with a compact 1:2, tRNA: enzyme complex. This complex forms with a remarkably high stability constant: (enzyme:tRNA:enzyme)/(enzyme:tRNA)(enzyme) of 0.1 to 0.3(× 10⁶) m^?1 (at 20 °C). Upon addition of more tRNA, the complex dissociates in favour of the 1:1, enzyme:tRNA complex, which has a higher stability constant (1 to 3 (× 10⁶) m^?1).     

Chromatin subunit small angle neutron scattering: A DNA rich coil surrounds a protein-DNA core

The small angle neutron scattering radii of gyration of 185 base pair subunits have been determined in H₂O and D₂O These values suggest that the outer diameter is 120 to 150Å. The results are not consistent with models in which all of the DNA is in an external shell. The neutron scattering profiles are in good agreement with a model based upon freeze etching electron microscopy (4) having two concentric coils of DNA with 80Åand 150Åexternal diameters.     

Neutron scattering study of the 13 S fragment of 16 S RNA and its complex with ribosomal protein S4

A fragment with a molecular weight of 170,000 and a sedimentation coefficient of 13 S which is capable of specifically binding ribosomal protein S4 has been obtained by digestion of Escherichia coli 16 S RNA with ribonuclease A. The 13 S fragment of 16 S RNA and its complex with protein S4 have been studied by different physical methods; in the first place, by neutron scattering. It has been shown that this fragment is very compact in solution. The radii of gyration of this fragment (50 ± 3 Å) and of protein S4 within the complex (17 ± 3 Å) coincide, within the limits of experimental error, with the radii of gyration for the free RNA fragment (47 ± 2 Å) and the free ribosomal protein S4 in solution (18 ± 2 Å). Hence the conclusion is drawn that the compactness of the RNA fragment and the ribosomal protein does not change on complex formation. The compact 13 S fragment of 16 S RNA is shown to be contrast-matched in solvent containing 70% ²H₂O which corresponds to a value for the partial specific volume of RNA of 0.537 cm³/g.     

Light scattering studies of supercoiled and nicked DNA

Static and dynamic light scattering measurements were made of solutions of pGem1a plasmids (3730 base pairs) in the relaxed circular (nicked) and supercoiled forms. The static structure factor and the spectrum of decay modes in the autocorrelation function were examined in order to determine the salient differences between the behaviors of nicked DNA and supercoiled DNA. The concentrations studied are within the dilute regime, which is to say that the structure and dynamics of an isolated DNA molecule were probed. Static light scattering measurements yielded estimates for the molecular weight M, second virial coefficient A₂, and radius of gyration R_G. For the nicked DNA, M = (2.8 ± 0.4) × 10⁶g/mol, A₂ = (0.9 ± 0.2) × 10⁻³ mol cm³/g², and R_G = 90 ± 3 nm were obtained. For the supercoiled DNA, M = (2.5 ± 0.4) × 10⁶ g/mol, A₂ = (1.2 ± 0.2) × 10⁻³ mol cm³/g², and R_G = 82 ± 2.5 nm were obtained. The static structure factors for the nicked and supercoiled DNA were found to superpose when they were scaled by the radius of gyration. The intrinsic stiffness of DNA was evident in the static light scattering data. Homodyne intensity autocorrelation functions were collected for both DNAs at several angles, or scattering vectors. At the smallest scattering vectors the probe size was comparable to the longest intramolecular distance, while at the largest scattering vectors the probe size was smaller than the persistence length of the DNA. Values of the self-diffusion coefficients D were obtained from the low-angle data. For the nicked DNA, D = (2.9 ± 0.3) × 10⁻⁸ cm²/s, and for the supercoiled DNA, D = (4.11 ± 0.21) × 10⁻⁸ cm²/s. The contribution to the correlation function from the internal dynamics of the DNA was seen to result in a strictly bimodal decay function. The rates of the faster mode Γ_int, reached plateau values at low angles. For the nicked DNA, Γ_int = 2500 ± 500 s⁻¹, and for the supercoiled DNA, Γ_int = 5000 ± 500 s⁻¹. These rates correspond to the slowest internal relaxation modes of the DNAs. The dependence of the relaxation rates on scattering vector was monitored with the aid of cumulants analysis and compared with theoretical predictions for the semiflexible ring molecule. The internal mode rates and the dependence of the cumulants moments reflected the difference between the nicked DNA and the supercoiled DNA dynamical behavior. The supercoiled DNA behavior seen here indicates that conformational dynamics might play a larger role in DNA behavior than is suggested by the notion of a branched interwound structure. © 1996 John Wiley & Sons, Inc.     

Structure Determination of Functional Membrane Proteins using Small-Angle Neutron Scattering (SANS) with Small, Mixed-Lipid Liposomes: Native Beef Heart Mitochondrial Cytochrome c Oxidase Forms Dimers

The low-resolution three-dimensional structure of purified native beef heart mitochondrial cytochrome c oxidase (COX) in asolectin unilamellar liposomes has been measured by small-angle neutron scattering under the conditions where the protein remains fully functional. From a neutron scattering perspective, the use of mixed-lipid liposomes provided for a more homogeneous matrix than can be achieved using a single lipid. As a result, the measurements were able to be performed under conditions where the liposome scattering was essentially eliminated (contrast-matched conditions). The protein structure in the membrane was modeled as a simple parallelepiped with side lengths of (59 × 70 × 120) Å with uncertainties, respectively, (11, 12, 20 Å). The molecular mass calculated for a typical protein with this volume is estimated to be (410 ± 124) kDa, which indicates the mass of a COX dimer. The longest dimension has some uncertainty due to intermolecular scattering contributing to the data. Nevertheless, that length was estimated using an average protein density and the known dimer molecular mass. Using the same cross sectional dimensions for the structure, the length is estimated to be 120 Å. However, the measured scattering curve of the dimer in the liposome differs significantly from that calculated from the X-ray structure of the dimer in a crystal of mixed micelles (PDB 3AG1). The calculated SANS scattering from the crystal structure was fit with a parallelepiped, measuring (59 × 101 × 129) Å with fitting uncertainties, respectively, (2, 3, 3 Å). Our results suggest that COX is a functional dimer when reconstituted into mixed-lipid liposomes.     

Hydrodynamic properties of nitrogenase — the MoFe protein from Azotobacter vinelandii studied by dynamic light scattering and hydrodynamic modelling

Experimental results for the nitrogenase MoFe protein from Azotobacter vinelandii obtained by dynamic light scattering (DLS) are presented. The translational diffusion coefficient was determined to D=(4.0±0.2)×10⁻⁷ cm²/s. Complementary, we have performed hydrodynamic model calculations based on the X-ray crystallographic data of the MoFe protein. The calculated transport coefficient suggests that the size and shape of the protein in solution is consistent with that in the crystal structure.     

On the structure of agglutinated sheep red blood cell membranes

Specimens of isolated sheep red blood cell membranes are prepared by an agglutination technique in which membranes are stacked in regular arrays. X-ray diffraction patterns are recorded from such specimens which show meridional and equatorial diffraction phenomena. The meridional reflections correspond to single lamellar repeat periods of 160–186 Å. It is concluded that two asymmetric membranes are contained inthe elementary period. Lipid phases with preferentialyl oriented hydrocarbon chains are part of the membrane structure. The stacking of membranes is also demonstrated in the electron microscope. The X-ray scattering curve of intracellular hemoglobin of intact sheep red blood cells is recorded to a spacing of about 8 Å^?1. The broad diffraction rings of this scattering curve are replaced by a series of rather sharp rings, when the red blood cells are agglutinated and placed in a hypertonic medium. Both the presence of a functioning membrane and the agglutination appear to be essential for the full expression of this phenomenon.