The evaluation of standard sedimentation coefficient in band sedimentation of macromolecules

Standardization in the calculation of the sedimentation coefficient of macromolecules by means of band techniques is discussed. When a sample of macromolecules suspended in a solvent is layered on to a denser bulk solution, the macromolecules do not sediment in this solution alone, but sediment in a mixture of bulk solution and sample solvent. This is caused by the diffusion between sample solvent and bulk solution. Experimental evidence of this process is shown during band sedimentation of ribosomes when the variation of the density and the viscosity along the cell is measured. The calculation shows that in the experimental conditions frequently used, standardization made in the usual way leads to a sedimentation coefficient which is largely overestimated; while standardization yields the correct coefficient if the diffusion effect of the sample solvent in to the bulk solution is taken into account, together with possible deuteration effects. A method to calculate the standard coefficient with the aid of a computer is proposed.     

Simultation of gradient and band propagation in the centrifuge.

A technique is developed for simulating the behavior of both the gradient-forming solute and macromolecular bands in a centrifuge. The change with time of the density gradient due to diffusion and sedimentation of the gradient-forming solute is calculated by a finite difference method, making use of the results of earlier work on the theory of the equilibrium density gradient. Using a perturbation technique, the concentration profiles of dilute bands of macromolecules are then calculated as they sediment and diffuse through the varying supporting gradient. Results of the stimulaion techniques are compared with experiment.     

Zone Centrifugation in a Cesium Chloride Density Gradient Caused by Temperature Change

In this communication is described a new technique for the determination of sedimentation coefficients of macromolecules banded in equilibrium density gradients. Initially, the macromolecules are banded in the analytical ultracentrifuge at a low temperature of about 5°C. After equilibrium has been obtained, the temperature is increased to 25°C. The equilibrium band will now sediment to a new equilibrium position in the ultracentrifuge cell: (a) By following the position of the migrating band as a function of time, sedimentation coefficients may be determined. (b) If several species having different sedimentation coefficients are present in the original band, then during the course of the migration the band may split into several new bands which eventually reunite at the final equilibrium position. (c) If different chemical species of macromolecules such as nucleic acids and carbohydrates are present, in general they will exhibit different temperature density relationships, and can move different distances and directions in response to temperature change.     

Band centrifugation of macromolecules in self-generating density gradients. II. Sedimentation and diffusion of macromolecules in bands

Three approaches to the simultaneous sedimentation and diffusion of hands or zones of noninteracting homogeneous macromolecules are examined: (1) The authors' method of moments: (2) the transport me of Sehumaker and Rosenbloom; and (3) the stochastic solution of the Lamm equation due to Gehatia and Katehalski. All three methods indicate that the motion of the maximum of the hand may be used to evaluate the sedimentation coefficient. The moment, method provides relations which appear to be useful for measuring diffusion coefficients. Relations are given for the analysis of resolved components. The problem of measuring sedimentation coefficients of macromolecules with concentration-dependent sedimentation coefficients is examined. Methods are described for evaluating the sedimentation coefficient in these systems and for obtaining the sedimentation coefficient at infinite dilution. Methods are described for determining the weight-average sedimentation coefficient in Multi-component systems, and the differential and integral distribution of sedimentation coefficients of macromolecules with low-diffusion coefficients.     

A model for sedimentation in inhomogeneous media. II. Compressibility of aqueous and organic solvents

The effects of solvent compressibility on the sedimentation behavior of macromolecules as observed in analytical ultracentrifugation are examined. Expressions for the density and pressure distributions in the solution column are derived and combined with the finite element solution of the Lamm equation in inhomogeneous media to predict the macromolecular concentration distributions under different conditions. Independently, analytical expressions are derived for the sedimentation of non-diffusing particles in the limit of low compressibility. Both models are quantitatively consistent and predict solvent compressibility to result in a reduction of the sedimentation rate along the solution column and a continuous accumulation of solutes in the plateau region. For both organic and aqueous solvents, the calculated deviations from the sedimentation in incompressible media can be very large and substantially above the measurement error. Assuming conventional configurations used for sedimentation velocity experiments in analytical ultracentrifugation, neglect of the compressibility of water leads to systematic errors underestimating sedimentation coefficients by approximately 1% at a rotor speeds of 45000 rpm, but increasing to 2-5% with increasing rotor speeds and decreasing macromolecular size. The proposed finite element solution of the Lamm equation can be used to take solvent compressibility quantitatively into account in direct boundary models for discrete species, sedimentation coefficient distributions or molar mass distributions. Using the analytical expressions for the sedimentation of non-diffusing particles, the ls-g*(s) distribution of apparent sedimentation coefficients is extended to the analysis of sedimentation in compressible solvents. The consideration of solvent compressibility is highly relevant not only when using organic solvents, but also in aqueous solvents when precise sedimentation coefficients are needed, for example, for hydrodynamic modeling.     

Evidence for the attachment of RNA to pulse-labeled DNA in the slime mold, Physarum polycephalum

When $\text{Physarum}\text{polycephalum}$ is pulse-labeled for up to 20 minutes with ³H-thymidine and the shortest labeled DNA strands are partially purified by sedimentation through a neutral aqueous sucrose gradient and then through a formamide-sucrose gradient, these short strands band in Cs₂SO₄ isopycnic density gradients at a density greater than that of bulk single-stranded DNA. Their density is brought partially or nearly completely back to that of single-stranded DNA by hydrolysis with pancreatic RNase A or alkali, respectively. Therefore the dense material attached to the short pulse-labeled DNA strands consists at least partially of RNA.     

Quasi-elastic light scattering of Artemia ribosomes sedimented in a CsCl density gradient

It is impossible to measure the diffusion coefficient of macromolecules directly and accurately by quasi—elastic light scattering, when aggregates cannot be eliminated from the solutions to be investigated. Nevertheless, a simple method can be applied to overcome this problem in many cases. Aggregates are separated from the monomeric macromolecules by rate-zonal sedimentation in a CsCl density gradient in a transparent centrifugation tube; the monomers are then located by laser light scattering intensity measurements; photon correlation spectroscopy of the scattered light finally yields their diffusion coefficient. The viscosity of aqueous CsCl solutions at different temperatures and concentrations allows a good separation by centrifugation and a low uncertainty in the reduction of the measured diffusion coefficient to standard conditions.The application of the method to eukaryotic large ribosomal subunits is described as an example.     

Fluorescence correlation spectroscopy and nonideal solutions

The information that may be obtained from a fluorescence correlation spectroscopic study of a nonideal solution is considered. If all of the macromolecules in a two-component solution are fluorescently labeled, the mutual diffusion coefficient will be measured. If only a few of the macromolecules in a solution are fluorescently labeled, the tracer diffusion coefficient will be obtained. Two nonideal systems that probably may usefully be studied with fluorescence correlation spectroscopy are proposed. The application of fluorescence correlation spectroscopy to studies of lateral diffusion in biological membranes is discussed; the form of the contribution to the fluorescence correlation spectrum of bulk motion within a membrane is noted.     

Anomalies in sedimentation. 3. A model for the inherent instability of solutions of very large particles in high centrifugal fields

Sedimentation, diffusion, and hydrodynamic interaction are included in a simplified model for the behavior of a solution macromolecules in a centrifugal field. The model is simulated by a program on a digital computer. As the diffusion coefficient is allowed to decrease, the simulation shows that the molecules tend to cluster in high centrifugal fields. The clusters move through the solution in the direction of sedimentation in a wave-like fashion, acquiring new molecules at the front and shedding old ones to the rear. It is suggested that this tendency to cluster could account for the loss of DNA and other very large molecules from solution which is observed to occur at high centrifugal fields.     

Nucleic Acid of Rubella Virus and Its Replication in Hamster Kidney Cells

Ribonucleic acid (RNA) has been isolated from partially purified rubella virus preparations and fractionated by rate zonal centrifugation in sucrose density gradients. The bulk of the RNA sedimented as a sharp band with a sedimentation coefficient of 38S. Rubella virus RNA appears to be single-stranded on the basis of its sensitivity to the degrading action of ribonuclease. Fractionation by precipitation with 1 m NaCl, followed by chromatography on cellulose columns, and by rate zonal centrifugation in sucrose density gradients of labeled RNA isolated from actinomycin D-treated and infected baby hamster kidney cells revealed the presence of the following virus-specific types of RNA: (i) single-stranded RNA with a heterogeneous sedimentation pattern, the 38S viral RNA becoming the predominant species only after long periods of labeling late after infection; (ii) double-stranded RNA with a sedimentation coefficient of 20S; (iii) RNA apparently composed of 20S double-stranded RNA and single-stranded branches. On the basis of their properties, the last two species were tentatively identified as the replicative form and the replicative intermediate of rubella virus RNA. Rubella virus RNA was infectious.     

Pig liver fatty acid synthetase: purification and physicochemical properties.

This paper reports the first detailed study of the physicochemical properties of a fatty acid synthetase multienzyme complex from a mammalian liver. Fatty acid synthetase from pig liver was purified by a procedure including the following main steps: (i) preparation of a clarified supernatant solution (50,000 g), (ii) ammonium sulfate fractionation, (iii) DEAE-cellulose chromatography to separate 11 S catalase from the 13 S fatty acid synthetase, (iv) a preparative sucrose density gradient step to remove a 7 S impurity, and (v) a calcium phosphate gel step to remove an unusual yellow 16 S heme protein to yield a colorless preparation. The purified fatty acid synthetase was colorless and showed a single symmetrical peak in sucrose density gradient and conventional sedimentation velocity experiments. Fatty acid synthetase was very stable at 4 °C in the presence of 1 mm dithiothreitol and 25% sucrose. Extrapolation to zero protein concentration yielded values of S^o_20,w = 13.3 S and D^o_20,w = 2.60 × 10^?7cm²/s for the sedimentation and diffusion coefficients of the enzyme. Frictional coefficient values of 1.55 and 1.56 × 10^?7 cm, respectively, were calculated from the values for the sedimentation and diffusion coefficients. Based on these frictional coefficient values, the Stokes radius of the enzyme was calculated to be 82.4 Å. Sedimentation and diffusion coefficient data yielded a molecular weight value of $\text{M}{}_{\mathrm{<mtext>w</mtext>}}\text{(}\text{s}\text{D}\text{) = 478,000}$ and sedimentation equilibrium data yielded a value of M_w = 476,000. Preliminary intrinsic viscosity measurements at 20 °C gave a value of 7.3 ml/g, indicating that the enzyme is somewhat asymmetric. This is supported by the value of 1.58 calculated for the frictional ratio and by the fact that the values for the sedimentation and diffusion coefficients are both slightly lower than expected for a globular protein of molecular weight 478,000. The enzyme possesses about 90 SH groups per molecule, assuming a molecular weight of 478,000. The ultraviolet absorption spectrum of the enzyme shows a maximum at 280 nm and an unusual shoulder at 290 nm. The fluorescence spectrum of the enzyme is dominated by tryptophan fluorescence and, over the excitation range of 260–300 nm, there is a single emission maximum at 344 nm.     

Studies on Transformations of Hemophilus influenzae : II. The molecular weight of transforming DNA by sedimentation and diffusion measurements

The sedimentation and diffusion coefficients have been determined for Hemophilus influenzae transforming activity and DNA using P³²-labeled DNA. The methods employed the Spinco fixed boundary separation cell for measurements of the sedimentation coefficient and the Northrop-Anson diffusion cell to determine the diffusion coefficient. There was a very close correlation between the amount of DNA and transforming activity sedimented or diffused. The sedimentation coefficient (s_20°), for both biological activity and DNA was 27 and the diffusion coefficient (D_20°) 1 x 10^-8 cm²/sec. The molecular weight calculated from these coefficients gave a value of 16 million. There was no difference in the sedimentation coefficients for the two unlinked markers, streptomycin and erythromycin resistance, and the diffusion coefficients for single markers or the linked markers, streptomycin and cathomycin, were the same.     

Sedimentation studies of giant DNA molecules present in unsheared whole-cell lysates of D. melanogaster cells.

We have used band sedimentation in shallow density gradients of CsCl in the preparative centrifuge to analyze the distribution of sedimentation coefficients present in tritium labelled DNA from D. melanogaster cells. The cells were lysed according to the method of Kavenoff and Zimm to preserve very high molecular weight DNA. Sedimentation measurements have been carried out as a function of speed of centrifugation. The resulting distribution functions have been interpreted with the aid of the Zimm-Schumaker equation for the speed dependence of the sedimentation coefficient of very high molecular weight DNA. Low-speed centrifugation (3000 rpm) indicates that DNA molecules from the lysate are evenly distributed over values of S_20,w from 0 to 514S. This distribution is very sensitive to changes in speed of centrifugation and is transformed into a bimodal distribution at 12,080 rpm. Analysis of this transformation allows us to postulate that perhaps 55% of the DNA in the lysate may have molecular weights in excess of 40 × 10⁹ g/mol. Some of these molecules may also possess a variety of configurations including partially replicated branched structures.     

Computational and experimental studies of the electronic excitation spectra of EDTA and DTPA substituted tetraphenylporphyrins and their Lu complexes

Ethylendiaminetetraacetic acid (EDTA) substituted and diethylenetriaminopentaacetic acid (DTPA) substituted aminated free-base tetraphenylporphyrins (H₂ATPP) and the corresponding lutetium(III) complexes have been studied computationally at the density functional theory (DFT) and second-order algebraic diagrammatic construction (ADC(2)) levels using triple-ξ basis sets augmented with polarization functions. The molecular structures were optimized using Becke's three-parameter hybrid functional (B3LYP). The electronic excitation spectra in the range of 400–700 nm were calculated using the ADC(2) and the linear-response time-dependent DFT methods. The calculated spectra are compared to those measured in ethanol solution. The calculated excitation energies agree well with those deduced from the experimental spectra. The excitation energies for the Q_x band calculated at the B3LYP and ADC(2) level are 0.20-0.25 eV larger than the experimental values. The excitation energies for the Q_y band calculated at the B3LYP level are 0.10-0.20 eV smaller than the ADC(2) ones and are thus in good agreement with experiment. The calculated excitation energies corresponding to the B_x and B_y bands are 0.10-0.30 eV larger than the experimental values. The excitation energies of the B_x and B_y bands calculated at the B3LYP level are in somewhat better agreement with experiment than the ADC(2) ones. The calculated and measured band strengths largely agree.

Hydrodynamic Molecular Weight of Solubilized Cholinergic Synaptic Vesicle Glycoprotein ATPase

The Torpedo californica electric organ synaptic vesicle glycoprotein ATPase was solubilized with octaethyleneglycoldodecyl ether and stabilized with phosphatidylserine. The complex was analyzed by size exclusion chromatography and band sedimentation velocity ultracentrifugation in water/glycerol and deuterium oxide/glycerol density gradients. The complex was found to have a Stokes' radius of 79 +/- 0.7 A, a sedimentation velocity coefficient at 20 degrees C in water of 6.8 +/- 0.2S, a partial specific volume of 0.81 +/- 0.01 cm3/g, and a frictional coefficient of 1.6. The molecular weight of the solubilized complex was calculated to be 320,000 +/- 7,000 and that of the protein 210,000 +/- 9,000. The relationship of this latter value to the major transport ATPase types is discussed.     

Mechanical Transmission, Purification and Properties of an Isolate of Maize Stripe Virus from Venezuela

A Venezuelan isolate of maize stripe virus (MStpV) was successfully transmitted mechanically and by the leafhopper Peregrinus maidis from field infected plants to sweet cv. Iochief. After purification of maize infected with MStpV, fine spiral filamentous particles about 4 nm in diameter and with variable lengths were consistently associated with a nucleoprotein band present in CsCl or Cs₂SO₄ isopycnic gradients. Purified preparations exhibited a typical nucleoprotein absorption spectrum with a maximum at 260–263 nm and a minimum at 240–243 nm and a 260–280 ratio of 1.38. The density of the nucleoprotein in CsCl gradients was estimated at 1.29 g/ml. The sedimentation coefficient was calculated at 62 S. The nucleoprotein consisted of 5 % single stranded RNA and a capsid protein of molecular weight 33.500 daltons. Large quantities of non-capsid proteins were isolated from infected tissue with a molecular weight of 17.500 and 16.500 daltons. Peregrinus maidis, injected with purified MStpV preparation failed to transmit the disease to healthy plants. However, they were infectious when injected with clarified infected plant sap. Antisera against capsid and non-capsid proteins from MStpV-Florida strain reacted positively with the Venezuelan antigens.     

Hydrodynamic properties of human cervical-mucus glycoproteins in 6M-guanidinium chloride.

Cervical mucins and fragments thereof were studied by sedimentation-velocity, rotatory viscometry and laser light-scattering performed as photon-correlation spectroscopy as well as low-angle total-intensity measurements. The Mr of the whole mucins is 10 X 10(6)-15 X 10(6), whereas fragments obtained after reduction of disulphide bonds ('subunits') have Mr 2.1 X 10(6)-2.9 X 10(6), depending on the method used. Subsequent trypsin digestion of subunits afforded glycopeptides with Mr approx. 0.4 X 10(6). The high frictional ratio for the whole mucins is interpreted as a large degree of expansion. The Stokes radius calculated from the diffusion coefficient is approx. 110nm for the whole mucins, which is in agreement with that estimated from the radius of gyration (130nm) by using the concept of the equivalent hydrodynamic sphere. The ratio of the concentration-dependence parameter for the reciprocal sedimentation coefficient (Ks) to the intrinsic viscosity ( [eta] ) for the whole mucins is 1.42, suggesting that the individual macromolecule occupies a spheroidal domain in solution. The relationship between [eta] and Mr for whole mucins, subunits and T-domains suggests that they are linear flexible macromolecules behaving as somewhat 'stiff' random coils. This conclusion is supported by the relationships between the sedimentation coefficients, the diffusion coefficients and the Mr. The hydrodynamic behaviour of the mucins is thus close to that expected for coiling macromolecules entrapping a lot of solvent, which is consistent with the postulated polymeric structure.     

Mass isolation of pole cells from Drosophila melanogaster.

Crude cell suspensions were obtained from 3 × 10⁶ pregastrula staged embryos. These cells fractionated into three bands on Renografin density gradients. Using ultrastructural characteristics for identification, pole cells were localized in the two denser bands. EM analyses also revealed a striking difference in the frequency of lipid vacuoles found in the pole-cell cytoplasm versus the cytoplasm of other embryonic cells. This difference has enabled us to identify pole cells by light microscopy using a neutral lipid stain. Through detailed analyses of the Renografin fractions with this stain, we have shown that pole cells resolve into two to three density classes. Evidence is presented which suggests that these density classes reflect different developmental age classes. The size differences between the pole cells and other embryonic cells contained in the enriched pole-cell fractions from the density gradients has enabled us to use sedimentation velocity centrifugation for additional enrichment. A distinct lower band of cells was obtained which consisted of 80% pole cells. Using these procedures, 1–2 × 10⁷ pole cells can be obtained daily.     

Macromolecular size-and-shape distributions by sedimentation velocity analytical ultracentrifugation

Sedimentation velocity analytical ultracentrifugation is an important tool in the characterization of macromolecules and nanoparticles in solution. The sedimentation coefficient distribution c(s) of Lamm equation solutions is based on the approximation of a single, weight-average frictional coefficient of all particles, determined from the experimental data, which scales the diffusion coefficient to the sedimentation coefficient consistent with the traditional s approximately M(2/3) power law. It provides a high hydrodynamic resolution, where diffusional broadening of the sedimentation boundaries is deconvoluted from the sedimentation coefficient distribution. The approximation of a single weight-average frictional ratio is favored by several experimental factors, and usually gives good results for chemically not too dissimilar macromolecules, such as mixtures of folded proteins. In this communication, we examine an extension to a two-dimensional distribution of sedimentation coefficient and frictional ratio, c(s,f(r)), which is representative of a more general set of size-and-shape distributions, including mass-Stokes radius distributions, c(M,R(S)), and sedimentation coefficient-molar mass distributions c(s,M). We show that this can be used to determine average molar masses of macromolecules and characterize macromolecular distributions, without the approximation of any scaling relationship between hydrodynamic and thermodynamic parameters.     

Membranes of Rhodopseudomonas sphaeroides. VI. Isolation of a fraction enriched in newly synthesized bacteriochlorophyll alpha-protein complexes.

Radioactivity eventually destined for the chromatophore membrane of Rhodopseudomonas sphaeroides was shown in pulse-chase studies to appear first in a distinct pigmented fraction. The material formed an upper pigmented band which sedimented more slowly than chromatophores when cell-free extracts were subjected directly to rate-zone sedimentation on sucrose density gradients. Sodium dodecyl sulfate-polyacrylamide gel electrophoresis indicated that the purified fraction contained polypeptide bands of the same mobility as light-harvesting bacteriochlorophyll alpha and reaction center-associated protein components of chromatophores; these were superimposed upon cytoplasmic membrane polypeptides. The pulse-chase relation was confined mainly to the polypeptide components of these pigment-protein complexes. It is suggested that the isolated fraction may be derived from sites at which new membrane invagination is initiated.