Gelatin-alpha olefin sulfonate interactions studied by dynamic light scattering

Dynamic light scattering (DLS) measurements were performed to study the binding of anionic surfactant alpha olefin sulfonate (AOS) to gelatin chains at various NaCl concentrations at 30 degrees C in aqueous sodium phosphate buffer (pH = 6.8) solutions. The surfactant concentration was varied from 0 to 80 mM and the NaCl concentrations chosen were 0.025, 0.05, and 0.1 M. AOS exhibited electrostatic binding to the positively charged sites of the polypeptide chain resulting in considerable reduction in its hydrodynamic radius up to critical micellar concentration (cmc = 8 mM for no salt, 0.01 and 0.025 M, and 5 mM for 0.05 M and 2 mM for 0.1 M solutions). The correlation function revealed the presence of two types of structures above cmc; namely the micelles of AOS and gelatin-AOS micelle complexes. The micellar radii (Rm), the effective gelatin-surfactant complex radii (Rc), have been determined as a function of salt concentration. No critical aggregation concentration (cac) was observed. The inter-gelatin-surfactant complex (kD1) and inter-micellar interactions (kD2), were determined by fitting the concentration dependence of Rm and Rc to a virial expansion in reduced concentration (c - cmc), which are compared. While kD1 showed strong ionic strength dependence, kD2 remained invariant of the same. The protein to surfactant binding ratio was found to be smaller than normal. Results have been discussed within the framework of the necklace-bead model of polymer-surfactant interactions.     

The onset of amelogenin nanosphere aggregation studied by small-angle X-ray scattering and dynamic light scattering

Proteins with predominantly hydrophobic character called amelogenins play a key role in the formation of the highly organized enamel tissue by forming nanospheres that interact with hydroxyapatite crystals. In the present investigation, we have studied the temperature and pH-dependent self-assembly of two recombinant mouse amelogenins, rM179 and rM166, the latter being an engineered version of the protein that lacks a 13 amino acid hydrophilic C-terminus. It has been postulated that this hydrophilic domain plays an important role in controlling the self-assembly behavior of rM179. By small-angle X-ray and neutron scattering, as well as by dynamic light scattering, we observed the onset of an aggregation of the rM179 protein nanospheres at pH 8. This behavior of the full-length recombinant protein is best explained by a core-shell model for the nanospheres, where hydrophilic and negatively charged side chains prevent the agglomeration of hydrophobic cores of the protein nanospheres at lower temperatures, while clusters consisting of several nanospheres start to form at elevated temperatures. In contrast, while capable of forming nanospheres, rM166 shows a very different aggregation behavior resulting in the formation of larger precipitates just above room temperature. These results, together with recent observations that rM179, unlike rM166, can regulate mineral organization in vitro, suggest that the aggregation of nanospheres of the full-length amelogenin rM179 is an important step in the self-assembly of the enamel matrix.     

Filipin and its interaction with cholesterol in aqueous media studied using static and dynamic light scattering

Aggregation of filipin in aqueous medium and filipin-induced changes in cholesterol micelles have been studied using intensity and dynamic light scattering. The dependencies of filipin aggregate dimensions on concentration, solvent, and temperature were studied, and revealed that the aggregates do not have a well-defined geometry, i.e., a critical micelle concentration cannot be detected and stable structures are not formed. The aggregates are of size R_g ≈ 110 nm and R_h ≈ 63 nm, referring to the radius of gyration and hydrodynamic radius, respectively. In the concentration range studied (1 μM < C < 30 μM), a low molecular weight species (monomer/dimer) is always present together with the aggregates. In ethanol/ water mixtures, large (R_g ≈ 500 nm), narrow distribution aggregates are formed in the water volume fraction range 0.45 < Φ_H2_O < 0.65. Aggregation also occurs on changing the temperature; In the range 7–37°C, smaller aggregates (10–30 nm) form and the process is only partially reversible. No pronounced effect of filipin on the structure of the cholesterol micelles was observed (a small increase in R_g and R_h is noted). These results rule out any “specificity” for the filipin interactions with cholesterol, which has been considered a key event in the filipin biochemical mode of action. A reevaluatiori Of this question is suggested and some alternatives are advanced. © 1994 John Wiley & Sons, Inc.     

Cell aggregation in cultures of Micrococcus luteus studied by dynamic light scattering

Cell aggregation was studied using the method of dynamic light scattering in the course of growth of Micrococcus luteus cultures in a liquid medium. The method detects particles ranging in size from 0.5 to 1000 microm in samples containing no more than 10(5) cells/ml. When grown in liquid media, M. luteus forms aggregates; during the lag phase, 80% of the cells are found in aggregates of 10 to 1000 microm, only minor amounts being represented by single cells. With the onset of exponential growth, the aggregates were decomposed, and single cells became prevalent in the culture liquid. This observation confirms that the aggregation of the cells during the lag phase is prerequisite to the initiation of bacterial growth. The method may be used in biotechnology for monitoring the state of bacterial cultures.     

Fusion induced aggregation of model vesicles studied by dynamic and static light scattering

Membrane fusion is a key step in the virus mediated cell fusion. The vesicular dispersion serves as a model system to study the membrane fusion. We employed dynamic and static light scattering to study the fusion of phosphatidylcholine vesicles in the presence of model fusion peptide fragments from the hemagglutinin HA2 protein. The fusion-induced aggregation under the present experimental setup exhibited strong pH dependence, similar to the parental viral protein. Replacement of the glycine residue at the extreme amino terminus by glutamic acid (G1E) abolished fusion activity. The average molecular mass and diameter of vesicular dispersion obtained from static and dynamic light scattering measurements respectively at neutral and acidic pH showed about three fold increase in acidic solution containing wild type fusion peptide. The light scattering data are consistent with lipid mixing results. The present work demonstrates the utility of light scattering as a facile means to monitor the fusion process.     

Size distribution of pressure-decomposed casein micelles studied by dynamic light scattering and AFM

Reversible and irreversible states of pressure-dissociated casein micelles were studied by in situ light scattering techniques and ex situ atomic force microscopy. AFM experiments performed at ambient pressure reveal heterogeneities across the micelle, suggesting a sub-structure on a 20 nm scale. At pressures between 50 and 250 MPa, the native micelles disintegrate into small fragments on the scale of the observed sub-structure. At pressures above 300 MPa the micelles fully decompose into their monomeric constituents. After pressure release two discrete populations of casein aggregates are observed, depending on the applied initial pressure: Between 160 and 240 MPa stable micelles with diameters near 100 nm without detectable sub-structures are formed. Casein micelles exposed to pressures above 280 MPa re-associate at ambient pressure yielding mini-micelles with diameters near 25 nm. The implications concerning structural models are discussed.     

Early stages of fibrinogen to fibrin conversion studied by static and dynamic light scattering

The early steps of fibrin aggregation induced by low Reptilase concentrations were studied by means of static and dynamic light scattering. In order to obtain information on the size and shape of the first oligomers, the angular dependence of the scattered intensity and the mean Rayleigh line width were measured. Under physiological pH and ionic strength, oligomer formation was detectable immediately after enzymatic activation. Comparison of the calculated data for different models with experimental results shows that the early fibrin polymerization proceeds as an end-to-end aggregation of elongated and possibly flexible molecules approximately 75 nm long.     

Internal dynamics of tRNA(Phe) studied by depolarized dynamic light scattering

The collective internal dynamics of transfer RNA(Phe) from brewer's yeast in solution was studied by depolarized dynamic light scattering (DDLS). Within the melting region of tRNA the depolarized spectra consist of two Lorentzian, where the narrow (slow) component describes the overall rotation of the macromolecule. The broad component is attributed to the collective reorientation of the bases within the biopolymer. At high temperature only this relaxation process is observed in the spectrum. The viscosity dependence of the collective internal relaxation process is described by the Stokes-Einstein-Debye equation for rotational diffusion. Estimates of the internal orientational pair correlation factor from the integral depolarized intensities of tRNA(Phe) solutions indicates that the observed dynamics correspond to the collective reorientation of approximately 5 bases. A comparison of the results presented with DDLS studies on the aggregation of the mononucleotide guanosine-5'-monophosphate confirms this result. For a further characterization of the relaxation process we studied the effect of hydrostatic pressure (1-1000 bar) on the depolarized spectra of tRNA. While other spectroscopic methods like nmr, fluorescence polarization anisotropy decay, or ESR give information about the very local motion of a single base within the DNA or RNA, this study shows that by DDLS one can characterize collective internal motions of macromolecules.     

Solution properties of starch nanoparticles in water and DMSO as studied by dynamic light scattering

Solution properties of starch nanoparticles dispersed in DMSO and in water were studied using dynamic light scattering. The particle size distribution had two main peaks in both solvents at all scattering angles studied. They were at around 40 and 300 nm, ascribed to isolated starch nanoparticles and their aggregates, respectively. From the excess scattering intensity by the 40-nm particles, the molecular weight of the nanoparticle was estimated as 2.2–2.6×10⁶ g/mol. When the concentration was increased, another peak appeared at around 1 μm. Raising the temperature from 25 to 65 °C did not change the distribution, indicating a purely entropic process in dynamic equilibrium of the aggregation. In DMSO, an oscillatory behavior was observed in the autocorrelation function at high temperatures.     

Desmin filaments studied by quasi-elastic light scattering.

We studied polymers of desmin, a muscle-specific type III intermediate filament protein, using quasi-elastic light scattering. Desmin was purified from chicken gizzard. Polymerization was induced either by 2 mM MgCl(2) or 150 mM NaCl. The polymer solutions were in the semidilute regime. We concluded that the persistence length of the filaments is between 0.1 and 1 microm. In all cases, we found a hydrodynamic diameter of desmin filaments of 16-18 nm. The filament dynamics exhibits a characteristic frequency in the sense that correlation functions measured on one sample but at different scattering vectors collapse onto a single master curve when time is normalized by the experimentally determined initial decay rate.     

Self-assembly of melanin studied by laser light scattering

The unknown molecular weight and chemical structure of melanin place the study of these pigments outside the range of the classical biochemical techniques; thus in this paper the problem of characterizing these heterogeneous biopolymers was approached by means of light scattering techniques, static and dynamic. The static technique allowed us to identify the macromolecular properties (MW and R(g)(2)(1/2)) of melanin extracted from sepia inksac and of two synthetic analogues: L-Dopa melanin obtained by autooxidation and by enzymatic oxidation by Tyrosinase. By dynamic light scattering (DLS), the hydrodynamic radius R(h) was measured to monitor the temporal behaviour of the polymerization and aggregation processes and R(h) variation by changing the chemical constraints of the polymerization medium, such as pH and ionic strength. The fractal dimension d of the aggregates of melanin, both natural and synthetic, in the past only recognized during the aggregation of the synthetic one by lowering the pH of the medium, was a useful parameter to further investigate and compare the structure of melanin granules of differing origins, revealing for the natural sample, a structure with clusters that are spherical, not largely hydrated and self-assembled, following a reaction limited aggregation kinetics (d=2.38).     

Fibrinogen and the early stages of polymerization to fibrin as studied by dynamic laser light scattering

Human fibrinogen and the polymerization of fibrin after activation by the enzymes, thrombin and Batroxobin, were studied by means of dynamic laser light scattering (DLS). The apparent diffusion constant, D, for fibrinogen was measured and has a value of (1.80 +/- 0.42) X 10(-7) cm2 X s-1. D was found to contain contributions from the translational diffusion constant (Dt) as well as from the rotational diffusion constant (Dr). A comparison between experimental and calculated values of Dr and Dt suggests that fibrinogen in the absence of added Ca2+ expresses a certain degree of flexibility, while it is straightened in the presence of added Ca2+. The time dependence of D showed periodic oscillations, while the average D values decreased with time. Thrombin and Batroxobin caused similar behaviour of D. The period length was related to the enzyme concentration, clotting time (Ct) and the rate of release of fibrinopeptide A (FPA). No periodic oscillations were observed in experiments where the enzyme was replaced by saline, or in experiments using a dysfunctional fibrinogen (fibrinogen Aarhus) which displayed slow rates of FPA-release and polymerization. We propose that the periodic oscillations in a system far from equilibrium may be explained by conformational changes occurring in the fibrinogen molecule during enzyme activation and polymerization.     

Structure of artificial cytoskeleton containing liposomes in aqueous solution studied by static and dynamic light scattering

The structure of three types of liposomes (egg yolk phosphatidylcholine (EPC) without modification and EPC vesicles containing cross-linked N-isopropylacrylamide (NIPAM) networks of low and a high concentration inside the vesicles) were analyzed by static and dynamic light scattering. Upon polymerization the network was assumed to become attached to the membrane by reactive anchoring monomers. For the sample of high poly(NIPAM) content the polymer network was assumed to fill the whole space in the vesicles. The issue of the present study was to examine hard and hollow sphere behavior of the liposomes with networks of high and low poly(NIPAM) content. The theoretical scattering curves differ markedly for uniform hard and uniform hollow spheres by the presence of specific peaks. However, polydispersity washed out the peaks and led to smoothed asymptotes with fractal dimensions of df = 2 for hollow and df = 4 for hard spheres. The experimental data could efficiently be fitted with weakly polydisperse hollow spheres. No clear conclusion could be drawn from the angular dependence alone for the liposome of high poly(NIPAM) content. The two wavelengths from the HeNe and Ar lasers proved to be too long for the studied liposomes of about 100 nm in radius. However, evidence for hollow sphere behavior was found for fractionated liposomes from the ratio rho = Rg/Rh = 1.04 +/- 0.02 (theory rho = 1.00 for hollow spheres). Finally, from the molar mass and the sphere radius, an apparent density was determined. The analysis gave the expected density for the pure EPC lecithin vesicles and a poly(NIPAM) network density of 0.244 g/mL. For the liposome of low poly(NIPAM) content the network appeared to be attached to the inner surface of the lecithin shell to form a layer of about 18 nm thickness.     

Denaturation and aggregation of hen egg lysozyme in aqueous ethanol solution studied by dynamic light scattering

We applied dynamic light scattering technique on the model system of hen egg lysozyme in salt-free aqueous ethanol solution to study the mechanism of denaturation and aggregation of protein. At low ethanol concentration [0-63% (v/v)], the fast relaxation mode was observed, which was caused by lysozyme molecules in the solution interacting with each other with strong repulsive electrostatic force. At 45 and 63% (v/v) ethanol, the slow relaxation mode was also observed, which showed translational diffusive nature, similar to that observed in salt-free polyelectrolyte solution. At 72 or 81% (v/v) ethanol, the slow mode disappeared, leaving only the fast mode. However, the mutual diffusion coefficients obtained from the fast mode at 72 and 81% (v/v) ethanol decreased by about one order of magnitude compared with those from the fast mode at 0-63% (v/v). The reported alcohol-induced conformational transformation of lysozyme molecules at >60% (v/v) ethanol from their native structure to an alpha-helix-rich structure might cause such drastic decrease in the mutual diffusion coefficients. At the highest ethanol concentration of 90% (v/v), the slow mode reappeared, and its relaxation rate was decreasing with elapsed time, which is possibly due to the growth of aggregates of lysozyme molecules. X-ray diffraction results suggested that the intermolecular beta-sheet formation caused the aggregation. Thus, our results indicated that the change in molecular structure of lysozyme closely relates to the diffusion of molecules and their aggregation.     

Effect of salt on sodium polystyrene sulfonate measured by light scattering

The quasielastic light scattering method was used to study the ionic strength dependence of the mutual diffusion coefficient of sodium polystyrene sulfonate (NaPSS) as a function of NaCl and CaCl₂ concentrations. The results indicate a splitting in the relaxation times that depends on the ratio C_p/C_s, where C_p and C_s are the polyion and added salt concentrations. A universal relationship taking into account Manning's theory of condensation and the Debye screening due to the added salt is proposed to characterize the fast–slow relaxation time transition.     

Effects of arginine on kinetics of protein aggregation studied by dynamic laser light scattering and tubidimetry techniques

Prevention of undesirable protein aggregation is an extremely important strategy in protein science, medicine, and biotechnology. Arginine is one of the most widely used low molecular weight solution additives effective in suppressing aggregation, assisting refolding of aggregated proteins, and enhancing the solubility of aggregation-prone unfolded molecules in vitro. However, the mechanism of suppression of protein aggregation by arginine is not well understood. To address the mechanism, two model systems have been investigated: protection of alcohol dehydrogenase (ADH) and insulin from heat- and dithiothreitol-induced aggregation, respectively, in the presence of arginine. Using dynamic light scattering (DLS) technique, we have demonstrated the concentration-dependent suppression of light scattering intensity of both ADH and insulin aggregates upon addition of arginine to the incubation medium, a significant effect being revealed in the physiological concentration range of arginine (1-10 mM). DLS studies showed that arginine shifted the populations of nanoparticles with higher hydrodynamic radii to the lower ones, suggesting that the preventive effect of arginine on the protein aggregation process arises because it suppresses intermolecular interactions among aggregation-prone molecules. The results of turbidity measurements were also shown to be consistent with these findings.     

Structure of aggregating kappa-carrageenan fractions studied by light scattering

We have studied kappa-carrageenan fractions with varying molar mass, obtained by sonication, using static and dynamic light scattering and polarimetry. The samples were characterised in 0.1 M NaCl and 0.1 M NaI, i.e. in the coil and helix conformation, respectively. We find that the molar mass and size of the untreated sample are the same in the coil and helix conformation. For the sonicated samples, we find larger average molar masses and sizes in the helix conformation. The critical temperature, T(c), below which the coil-helix transition sets in, decreases with decreasing molar mass. Aggregation is induced by lowering the temperature in the presence of 0.01 M KCl, which leads to the formation of locally rigid bundles of kappa-carrageenan chains. The thickness of the bundles increases slowly with time and we have not observed stabilisation, even after 24 h at 10 degrees C below T(c). The local structure of the aggregates is the same for all fractions, but at a given temperature, the rate of aggregation decreases with decreasing molar mass.     

Motility of bovine spermatozoa studied by laser light scattering

Laser light scattering has been employed to determine the swimming speed distribution and the fraction of motile cells in samples of bovine spermatozoa. As predicted from theory, average trajectory velocities determined by laser light scattering were approximately four times the average translational speed estimated using light microscopy. The proportion of motile spermatozoa decreased with time at the same rate when samples were prepared in either HEPES or phosphate buffers. However, whereas the mean swimming velocity declined slowly in HEPES buffer, it dropped rapidly when phosphate buffer was used. Dilution (in the range 40–0.4×10⁶ spermatozoa·ml^-1) in either of these two buffers reduced the fraction of motile spermatozoa in the sample, but the mean swimming velocity of the remaining active spermatozoa was unchanged. Lowering the temperature from 37° C to 15° C reduced the mean swimming speed by a factor of 2–3 and the fraction of motile cells by a factor of 4–5.