Layer-by-layer Assembly of Poly(lactic-co-glycolic acid)-b-poly(l-lysine) Copolymer Micelles

Biocompatible, biodegradable polyionic micelles were used as a building component for layer-by-layer (LbL) assembly that can produce drug-loaded nanolayers. To prepare the polycationic micelles, poly(lactic-co-glycolic acid)-b-poly(l-lysine) [PLGA-b-P(Lys)] copolymers were synthesized. In an aqueous phase, PLGA-b-P(Lys) copolymers were self-assembled to form spherical micelles with the inner core of poly(lactic-co-glycolic acid) (PLGA) and the cationic outer shell of P(Lys). The micelles were characterized by zeta potential, dynamic light scattering, and nuclear magnetic resonance. PLGA-b-P(Lys) micelles showed the positive zeta potential values in a broad range of pH (3–11), indicating the high stability of the polyionic micelles with the outer shell of positive charges. Cationic polymeric micelles were coated on the surface via electrostatic interactions with the oppositely charged polyelectrolyte, poly(sodium 4-styrenesulfonate). Formation of multiple micelle layers was monitored using quartz crystal microbalance in situ, and the surface topology of the layers was characterized by atomic force microscopy ex situ, as the number of micelle layer was increased. The multiple micelle layers were stable, and the thickness of micelle layer grew as the number of LbL coating increased. The approach described in this work can be used for the development of the biocompatible, biodegradable, drug-loaded bioactive nanocoatings.     

Electrosorption of pectin onto casein micelles

Pectin, a polysaccharide derived from plant cells of fruit, is commonly used as stabilizer in acidified milk drinks. To gain a better understanding of the way that pectin stabilizes these drinks, we studied the adsorption and layer thickness of pectin on casein micelles in skim milk dispersions. Dynamic light scattering was used to measure the layer thickness of adsorbed pectin onto casein micelles in situ during acidification. The results indicate that the adsorption of pectin onto casein micelles is multilayered and takes place at and below pH 5.0. Renneting, i.e., cleaving-off kappa-casein from the casein micelles, did not alter the adsorption pH. It did, however, show that pectin arrests the rennet-induced flocculation of casein micelles below pH 5.0. From the findings we concluded the attachment of pectin onto casein micelles is driven by electrosorption. Adsorption measurements confirmed the multilayered nature of the adsorption of pectin onto casein micelles. Both the adsorbed amount and the layer thickness increased with decreasing pH in the relevant range 3.5-5.0. The phase behavior of a casein micelles/pectin mixture was determined and could be explained in terms of thermodynamic incompatibility being relevant above pH 5.0 and adsorption, leading to either stabilization and bridging, being relevant below pH 5.0. The results confirm that electrosorption is the driving force for the adsorption of pectin onto casein micelles.     

Small and medium-angle X-ray analysis of bacterial lipoteichoic acid phase structure.

X-ray scattering analysis was performed on various types of bacterial lipoteichoic acid in solution. The X-ray data show that all samples investigated were characterized by a similar micellar ultrastructure (hydrophilic moiety on the outside) with a fatty acid chain conformation of the disordered, alpha-type at all temperatures between 5 degrees-53 degrees C. The size distribution of Staphylococcus aureus lipoteichoic acid micelles was sufficiently homogeneous to determine their size and some related molecular parameters by detailed small-angle X-ray scattering analysis. Nearly independent of the degree of D-alanine substitution and the ionic strength of the aqueous dispersion, an average micelle contained about 150 lipoteichoic acid molecules arranged in a spherical assembly with a diameter of about 22 nm, whereby the hydrophilic region occupied an outer shell of about 8.5 nm thickness. Based on the average chain length of lipoteichoic acid, it could be estimated that each glycerophosphate residue contributed by about 0.34 nm to the thickness of the hydrophilic shell as compared to a theoretical value of approximately 0.8 nm for a fully extended chain conformation, indicating a highly coiled conformation of the hydrophilic chain. The bearing of these findings on the properties of membrane-associated and secreted lipoteichoic acids is discussed.     

Bioprospecting for novel hydroxyoxylipins in fungi: presence of 3-hydroxy palmitic acid in Saccharomycopsis malanga

Electron microscopy studies indicated that the major oxylipin 3-hydroxy palmitic acid (16:0) was associated with aggregating vegetative cells and formed a web-like structure around these cells. Cross sections through this structure showed a hydrophilic outer layer and a more hydrophobic inner layer suggesting that the web-like structure is in fact tube-like micelles. This information sheds more light on the role of these hydroxyoxylipins in fungi.     

Bacterial amphiphiles as amyloid inducers: Effect of Rhamnolipid and Lipopolysaccharide on FapC fibrillation

Pseudomonas species export the amyloid-forming protein FapC to strengthen bacterial biofilm. P. species also produce the biosurfactant rhamnolipid (Rhl) and its outer membrane contains lipopolysaccharide (LPS). Given the possible contacts between FapC, Rhl and LPS, we here investigate how Rhl and LPS affect FapC fibrillation compared with SDS, known to promote fibrillation of proteins at sub-micellar concentrations. Micelles of all three surfactants help FapC bypass the nucleation lag phase, leading to rapid fibrillation, which persists even at high concentrations of micelles and incorporates almost all available FapC monomers. Fibrils formed at high micellar concentrations of Rhl and SDS seed fibrillation at low surfactant concentrations while retaining the original fibril structure. FapC interacts strongly with SDS to form a dense network of narrow fibrils. Small angle X-ray scattering (SAXS) analyses reveal that surfactants reduce the population of intermediates in the fibrillation process and detect a fast aggregation step over the first 2–4 h which precedes the main fibrillation monitored by Thioflavin T. An additional SAXS-detected rearrangement of early aggregates occurs after 4–10 h. At high Rhl concentrations, the micelles are decorated with protein fibrils. SDS induces FapC fibrillation so efficiently that epigallocatechin-3-gallate (EGCG) is unable to inhibit this process. However, EGCG stimulates FapC oligomer formation and inhibits fibrillation both on its own and in the presence of Rhl and LPS. This oligomer could be modelled as a compact core with a flexible shell. This suggests that EGCG can override the natural amyloid-stimulatory properties of these biosurfactants and thus target biofilm.     

Thermotropic phase behavior and stability of monosialoganglioside micelles in aqueous solution.

The thermotropic phase behavior of monosialoganglioside in a dilute aqueous dispersion at pH 6.8 was measured by using synchrotron radiation small-angle x-ray scattering and was analyzed by a shell-modeling method. Previous calorimetric studies on ganglioside systems have shown quite different thermotropic behaviors from other biological lipid systems, however, the details have still been ambiguous. Because of high statistical data and a shell-modeling analysis, we could elucidate the internal structural change of monosialoganglioside micelle induced by the elevation of temperature from 6 to 60 degrees C, that is, the shrinkage of the hydrophilic region and the slight expansion of the hydrophobic region occurring simultaneously, accompanying the elongation of the axial ratios of the ellipsoidal micelles. The model structures obtained explain the changes in the experimental scattering curves, the distance distribution functions, and the gyration radii. In addition we have also found an evident thermal hysteresis in the scattering curves and in the structural parameters. The present result suggests that the thickness of the hydrophilic region, namely, the conformation of oligosaccharide chains, is sensitive to a change of temperature.     

Effect of calcium concentration on the structure of casein micelles in thin films

The structure of thin casein films prepared with spin-coating is investigated as a function of the calcium concentration. Grazing incidence small-angle x-ray scattering and atomic force microscopy are used to probe the micelle structure. For comparison, the corresponding casein solutions are investigated with dynamic light-scattering experiments. In the thin films with added calcium three types of casein structures, aggregates, micelles, and mini-micelles, are observed in coexistence with atomic force microscopy and grazing incidence small-angle x-ray scattering. With increasing calcium concentration, the size of the aggregates strongly increases, while the size of micelles slightly decreases and the size of the mini-micelles increases. This effect is explained in the framework of the particle-stabilizing properties of the hairy layer of kappa-casein surrounding the casein micelles.     

Kinetic and structural aspects of reconstitution of phosphatidylcholine vesicles by dilution of phosphatidylcholine-sodium cholate mixed micelles

Dilution of mixed micellar dispersions of egg phosphatidylcholine (PC) and sodium cholate beyond a critical value results in formation of cholate-containing PC vesicles. The structure of the resultant vesicles and some mechanistic aspects of this process have been investigated by the use of light scattering and nuclear magnetic resonance techniques. The main findings and conclusions are the following: Both the state of aggregation (micellar or vesicular) and the apparent equilibrium size distribution of micelles or vesicles obtained by dilution of the PC-cholate mixed micellar dispersions are a function of the cholate to PC molar ratio in the mixed aggregates (micelles or vesicles). When this effective ratio (Re) is higher than 0.4, the dispersion is micellar, and the size of the mixed micelles increases with decreasing Re; when Re less than 0.3, the dispersion is essentially vesicular, and the mean hydrodynamic radius of the vesicles is an increasing function of Re; in dispersions with 0.3 less than Re less than 0.4, mixed micelles and vesicles coexist. Addition of cholate to vesicular dispersions, to Re values below 0.3, results in vesicle size growth through a concentration-independent lipid-exchange mechanism. Addition of cholate to higher Re values results in micellization (solubilization) of the vesicles. On the other hand, dilution of vesicular dispersions does not affect the size of the vesicles. Apparent equilibration of a mixed micellar dispersion following dilution to Re values below 0.3 is slow (many hours). The overall process involves a series of three subsequent categories of steps: (i) a rapid (approximately 1-2 min) prevesiculation equilibration of micellar sizes.(ABSTRACT TRUNCATED AT 250 WORDS)     

Exchangeability of Colloidal Calcium in Milk with Soluble Calcium

Approximately 40% of the calcium existing in colloidal phase of skimmilk was estimated to be hardly exchanged with the calcium psesent in soluble phase by applying a radioisotopic technique. This type of calcium was designated hard-to-exchange calcium. Hard-to-exchange calcium was absent or nearly zero in calcium caseinate dispersion or colloidal phosphate-free milk, but was present in composite calcium caseinate phosphate dispersion. It is suggested that hard-to-exchange calcium is present in a part of colloidal phosphate portion of casein micelles.     

Shape and size of bovine rhodopsin: A small-angle X-ray scattering study of a rhodopsin-detergent complex

Rhodopsin is extracted from rod outer segments of retinas with dodecyldimethylamine oxide (DDAO), a non-ionie detergent. The rhodopsin-DDAO complex is characterized by binding experiments, gel filtration, sedimentation, densimetry; its homogeneity, chemical composition, weight and partial specific volume are determined. The complex turns out to be a reasonably monodisperse association of one rhodopsin and 156 DDAO molecules. The rhodopsin-DDAO complex and the detergent micelles are studied by small-angle X-ray scattering techniques using a water/sucrose solvent of variable density. The experiments are performed on an absolute scale; mainly the value and curvature of the scattering curves at zero angle are exploited. The structure of the complex and of the micelles is shown to be independent of sucrose. Under these conditions the final result of the X-ray scattering study of each type of particle is the numerical value of a set of five parameters: molecular weight, volume and radius of gyration of the volume occupied by the particles, average electron density and second moment of the electron density fluctuations inside the particles. It is also shown that in the complex the centres of gravity of rhodopsin and of the detergent moiety are very near to each other. The analysis of these parameters leads to the determination of the size and shape of the detergent micelles and to an estimate of the size and shape of the volumes occupied by protein and by detergent in the complex. We find rhodopsin to be a very elongated molecule (maximum diameter ~95 Å) which spans a flat detergent micelle. These results suggest that in the rod outer segment discs the rhodopsin molecules span the membranes, that the rhodopsin molecules of the two opposite membranes of each disc come near to each other and that a high fraction of the intra-disc space is occupied by rhodopsin.     

Physicochemical studies of the interaction of the lipoheptapeptide surfactin with lipid bilayers of L-alpha-dimyristoyl phosphatidylcholine

To understand the biological action of surfactin from Bacillus subtilis we investigated its effects on the phase transition of L-alpha-dimyristoyl phosphatidylcholine (DMPC)-vesicles from the crystalline to the fluid state using differential scanning calorimetry; light scattering; small angle neutron scattering and cryo-electron microscopy. DSC-thermograms revealed two phase transition peaks. Light scattering profiles showed two branches with characteristic hysteresis phenomena. With both techniques the same values of the phase transition temperatures T(m1) and T(m2) of 23.5 and 23 degrees C were obtained indicating two forms of DMPC-surfactin aggregates which could be visualized by cryo-electron microscopy. Until 4 mol% surfactin the vesicular form predominated, but was accompanied by bilayered membrane fragments by increasing the biosurfactant concentrations. At surfactin concentrations higher than 15 mol% smaller DMPC-surfactin micelles of ellipsoidal conformation were formed, as demonstrated by small angle neutron scattering. In addition, by "Poor Man's" temperature-jump-relaxation spectroscopy slow transients in the phase transition of vesicular DMPC-surfactin aggregates with relaxation times of 20-30 s were detected which presumably indicate the slow dissipation of intermediate lipid-and surfactin domains formed after the main phase transition on the way to the fluid state. This process is accelerated by surfactin.     

Transmembrane movement of heme

Evidence for CO-heme partitioning into and across lipid bilayers was obtained by kinetic and chromatographic studies. Biphasic time courses were observed when CO-heme was rapidly mixed with unilamellar lipid vesicles in a stopped-flow spectrometer. The initial rapid phase depended linearly on lipid concentration and was assigned to heme partitioning between the external solvent phase and the outer lipid layer of the membranes. The rate of the second, much slower phase was independent of both heme and lipid concentration. The fraction of absorbance change associated with this slower phase increased with increasing heme to lipid ratios and reached a maximum of approximately 45%. A similar slow phase was observed when membrane-bound heme was reacted with apomyoglobin. In the presence of excess globin, all of the CO-heme was extracted from the membranes to form native CO myoglobin. Under these conditions, the fractional amount of absorbance change associated with the slow dissociation phase was approximately 45%, regardless of the heme to lipid ratio. These results suggest strongly that the slow phases represent transmembrane movement of heme, from the outer to the inner lipid layer in the association reactions and from the inner to the outer layer in dissociation reactions. The temperature dependence of the rate of CO-heme binding to the outer lipid layer was markedly different from that of transmembrane movement. The rate of the latter, slower process decreased greatly with increasing acyl chain length, whereas the rate of the initial binding process varied little with vesicle composition, as long as the membranes were examined above their melting temperatures. Finally, the two kinetically distinct bound heme fractions could be isolated directly by column chromatography.     

Cutinase-AOT interactions in reverse micelles: the effect of 1-hexanol

Cutinase encapsulated in dioctyl sulfosuccinate reverse micelles displays very low stability, undergoing fast denaturation due to an anchoring at the micellar interface. The denaturation process and the structure of the reverse micelle were characterized using biophysical techniques. The kinetics of denaturation observed from fluorescence match the increase of the hydrodynamic radius of reverse micelles. Denaturation in reverse micelles is mainly the unfolding of the three-dimensional structure since the decrease in the circular dichroism ellipticity in the far-UV range is very small. The process is accompanied by an increase in the steady-state anisotropy, as opposed to what happens for denaturation in aqueous solution.Since 1-hexanol used as co-surfactant in dioctyl sulfosuccinate reverse micelles slows or even prevents cutinase denaturation, its effect on cutinase conformation and on the size of reverse micelles was analyzed. When 1-hexanol is present, cutinase is encapsulated in a large reverse micelle, as deduced from dynamic light scattering. The large reverse micelle filled with cutinase was built from the fusion of reverse micelles according to a pseudo-unimolecular process ranging in time from a few minutes to 2h depending on the reverse micellar concentration. This slow equilibrium driven by the encapsulated cutinase has not been reported previously. The encapsulation of cutinase in dioctyl sulfosuccinate reverse micelles establishes a completely new equilibrium characterized by a bimodal population of empty and filled reverse micelles, whose characteristics depend greatly on the interfacial characteristics, that is, on the absence or presence of 1-hexanol.     

Behavior of cholesterol and spin-labeled cholestane in model bile systems studied by electron spin resonance and synchrotron x-ray.

The behavior of mixed bile salt micelles consisting of sodium taurocholate, egg phosphatidylcholine, and cholesterol has been studied by ESR spin labeling and synchrotron x-ray scattering. Consistent with published phase diagrams, pure and mixed bile salt micelles have a limited capacity to incorporate and, hence, solubilize cholesterol. Excess cholesterol crystallizes out, a process that is readily detected both by ESR spin labeling using 3-doxyl-5 alpha-cholestane as a probe for cholesterol and synchrotron x-ray scattering. Both methods yield entirely consistent results. The crystallization of cholesterol from mixed bile salt micelles is indicated by the appearance of a magnetically dilute powder spectrum that is readily detected by visual inspection of the ESR spectra. Both the absence of Heissenberg spin exchange and the observation of a magnetically dilute powder spectrum provide evidence for the spin label co-crystallizing with cholesterol. In mixed bile salt micelles containing egg phosphatidylcholine, the solubility of cholesterol is increased as detected by both methods. With increasing content of phosphatidylcholine and increasing mole ratio cholesterol/phosphatidylcholine, the anisotropy of motion of the spin probe increases. The spin label 3-doxyl-5 alpha-cholestane is a useful substitute for cholesterol provided that it is used in dilute mixtures with excess cholesterol: the cholesterol/spin label mole ratio in these mixtures should be greater than 100. Despite the structural similarity between the two compounds, there are still significant differences in their physico-chemical properties.(ABSTRACT TRUNCATED AT 250 WORDS)     

Structural phase relationships in lecthin-cholate-water systems

In the first part of this paperthe anomalies and discontinuities observed in different physical properties of the lecithin-cholate isotropic phase (light scattering, sodium ion activity, viscosity, conductivity) as well as the results of an enzymatic study are explained in terms of partial aggregation which sets in when the intermicellar solution is “unsaturated” in cholate.It is proposed that this aggregation process in the isotropic phase is exactly the inverse process of the disintegration of the hexagonal phase when the latter is diluted. The mixed micelles had previously been shown to be in the form of a bimolecular discs, both the cylindrical elements of the hexagonal phase and the entities in the aggregation process are stacks of mixed micellar discs, the existence of both of these states being governed by the same delicate hydrophilic-hydrophobic balance.The arguments in favour of this are discussed in the second part of the paper where in particular the model proposed for the hexagonal phase is verified by a detailed calculation from X-ray diffraction measurements. The variations of both the water layer between discs in the cylinder and of the intercylinder water volume were shown to be coherent with changes in lecithin concentration and the amount of water present, in agreement with the above mentioned balance.Finally having demonstrated the structural resemblance between these two phases and the mechanism of the passage from one phase to the other, an explanation of the inter-relationship of all phases in the system is attempted.     

Adsorption of an amphiphilic penicillin onto human serum albumin: characterisation of the complex

The complex formed by the interaction of the amphiphilic penicillin drug nafcillin and human serum albumin (HSA) in water at 25 degrees C has been characterised using a range of physicochemical techniques. Measurements of the solution conductivity and the electrophoretic mobility of the complexes have shown an ionic adsorption of the drug on the protein surface leading to a surface saturation at a nafcillin concentration of 0.012 mmol kg(-1) and subsequent formation of drug micelles in solutions of higher nafcillin concentration. Measurements of the size of the complex and the thickness of the adsorbed layer by static and dynamic light scattering have shown a gradual change in hydrodynamic radius of the complex with increasing drug concentration typical of a saturation rather than a denaturation process, the magnitude of the change being insufficient to account for any appreciable extension or unfolding of the HSA molecule. The interaction potential between the HSA/nafcillin complexes, and the stability of the complexes were determined from the dependence of diffusion coefficients on protein concentration by application of the DLVO colloidal stability theory. The results indicate decreasing stability of the colloidal dispersion of the drug/protein complexes with an increase in the concentration of added drug.     

Aggregation, lipid exchange, and metastable phases of dimyristoylphosphatidylethanolamine vesicles

A new fluorescent lipid analogue, bimanephosphatidylcholine, has been synthesized for use in lipid bilayers. This probe is well suited as an energy-transfer donor with N-(7-nitro-2,1,3-benzoxadiazol-4-yl)phosphatidylethanolamine as the acceptor. Dimyristoylphosphatidylethanolamine vesicles are prepared by sonication at pH 9 and characterized by electron microscopy and other methods. Resonance energy transfer between separately labeled donor and acceptor vesicles is monitored during HCl-induced aggregation to determine the kinetics of lipid randomization. Light scattering is also monitored to measure the kinetics of aggregation. The light scattering shows a marked reversal with NaOH while the energy transfer does not, indicating lipid exchange during a reversibly aggregated state; the extent of energy transfer suggests that only lipids in the outer monolayers exchange. The gel to liquid-crystalline phase transition temperature in HCl-treated vesicles is found to be 47 degrees C with diphenylhexatriene. The initial sonicated dispersion does not show a sharp phase transition. In vesicles labeled with both donor and acceptor probes, a small, irreversible increase in energy transfer is obtained upon lowering and then restoring the pH. These results suggest a metastable phase in the sonicated vesicles containing a randomized distribution of lipid and probes within the bilayers; the thermodynamically favored phase, whose formation is triggered by the pH shock, contains domains within which the probe lipids are more highly concentrated.     

The Submicroscopic Organization of the Cell Wall in Conifer Tracheides and Wood Fibres

The controversy concerning the details of structure in the wallsof conifer tracheides has been resolved by a study of the birefringenceobserved in sections cut at various angles to the radial longitudinalplane. It has been demonstrated that the optical heterogeneityobserved in transverse section is traceable to two factors:(i) The outer layer of each tracheide is composed of cellulosechains lying in a rather flat spiral, though not transverse,making an angle of some 50?, on an average, to cell length;in the thicker central layer the spiral is much steeper, withan angle of some 20?. (ii) At the same time the birefringenceof both layers is reduced in virtue of both high lignin contentand high angular dispersion, the dispersion being considerablygreater in the outer layer. It is presumed that this high angular dispersion in the outerlayer is responsible for the lack of any record of this layerin the X-ray diagram and its failure to make any marked contributionto the optical properties of the wall in face view.     

κ-Casein terminates casein micelle build-up by its “soft” secondary structure

In our previous paper (Nagy et?al. in J Biol Chem 285:38811–38817, 2010) by using a multilayered model system, we showed that, from α-casein, aggregates (similar to natural casein micelles) can be built up step by step if Ca-phosphate nanocluster incorporation is ensured between the protein adsorption steps. It remained, however, an open question whether the growth of the aggregates can be terminated, similarly to in nature with casein micelles. Here, we show that, in the presence of Ca-phosphate nanoclusters, upon adsorbing onto earlier α-casein surfaces, the secondary structure of α-casein remains practically unaffected, but κ-casein exhibits considerable changes in its secondary structure as manifested by a shift toward having more β-structures. In the absence of Ca-phosphate, only κ-casein can still adsorb onto the underlying casein surface; this κ-casein also expresses considerable shift toward β-structures. In addition, this κ-casein cover terminates casein aggregation; no further adsorption of either α- or κ-casein can be achieved. These results, while obtained on a model system, may show that the Ca-insensitive κ-casein can, indeed, be the outer layer of the casein micelles, not only because of its “hairy” extrusion into the water phase, but because of its “softer” secondary structure, which can “occlude” the interacting motifs serving casein aggregation. We think that the revealed nature of the molecular interactions, and the growth mechanism found here, might be useful to understand the aggregation process of casein micelles also in?vivo.     

Dynamic light scattering of cutinase in AOT reverse micelles

The fungal lipolytic enzyme cutinase, incorporated into sodium bis-(2ethylhexyl) sulfosuccinate reversed micelles has been investigated using dynamic light scattering. The reversed micelles form spontaneously when water is added to a solution of sodium bis-(2ethylhexyl) sulfosuccinate in isooctane. When an enzyme is previously dissolved in the water before its addition to the organic phase, the enzyme will be incorporated into the micelles. Enzyme encapsulation in reversed micelles can be advantageous namely to the conversion of water insoluble substrates and to carry out synthesis reactions. However protein unfolding occurs in several systems as for cutinase in sodium bis-(2ethylhexyl) sulfosuccinate reversed micelles. Dynamic light scattering measurements of sodium bis-(2ethylhexyl) sulfosuccinate reversed micelles with and without cutinase were taken at different water to surfactant ratios. The results indicate that cutinase was attached to the micellar wall and that might cause cutinase unfolding. The interactions between cutinase and the bis-(2ethylhexyl) sulfosuccinate interface are probably the driving force for cutinase unfolding at room temperature. Twenty-four hours after encapsulation, when cutinase is unfolded, a bimodal distribution was clearly observed. The radii of reversed micelles with unfolded cutinase were determined and found to be considerable larger than the radii of the empty reversed micelles. The majority of the reversed micelles were empty (90-96% of mass) and the remainder (4-10%) containing unfolded cutinase were larger by 26-89 A.