Stabilität von Wasser-in-Öl-Emulsionen gegen Koaleszenz

Zusammenfassung Die Stabilität von Emulsionen von Wasser-in-Öl gegen Koaleszenz wurde untersucht. Diese Art von Emulsionen erfordert experimentell und auch theoretisch andere Methoden als Emulsionen von Öl-inWasser. In experimenteller Hinsicht werden zwei Methoden zur Messung der Koaleszenzgeschwindigkeit flokkulierter Emulsionen behandelt. Es werden mit beiden Methoden nicht der Absolutwert der Tröpfchenkonzentration, sondern zeitliche Änderungen dieser Größe gemessen.Nach einer Methode enthalten die Wassertröpfchen die farblosen Komponenten eines Farbstoffes. Nach Koaleszenz kommen diese Komponenten zur Reaktion und verursachen sodann eine Färbung des vergrößerten Tröpfchens.Nach der zweiten, genaueren, Methode enthalten alle Tröpfchen einen Farbstoff, und die Farbe der Emulsion im reflektierten Licht hängt dann in bekannter Weise mit der mittleren Tröpfchengröße zusammen.An Hand von Meßergebnissen wird die stabilisierende Wirkung von verschiedenen Emulgatoren diskutiert. Es werden sowohl öllösliche als feste Emulgatoren berücksichtigt.

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Summary The stability of emulsions of water in oil against coalescence was investigated. Both experimentally and theoretically, the investigation of this type of emulsion requires methods differing from those used for emulsions of oil in water. Two methods are discussed to measure the rate of coalescence in flocculated emulsions. Both methods measure changes in droplet concentration, and not the absolute value of this quantity.In one method, two types of water droplets are emulsified, each type containing one of the colourless components of a dye. Coalescence of two droplets brings the two components together so that a colour appears in the enlarged drop.In the second, more accurate, method all droplets contain a dye, and the colour of the emulsion in reflected light, then, depends in a known way on the average droplet size.The stabilization by several emulsifying agents, both solid and oilsoluble, was measured; the results are discussed.

     

Surface properties of mixed anionic/cationic surfactant solutions

Summary Published experimental surface pressures for mixtures of anionic and cationic surfactants are compared to what can be predicted from the surface behaviour of the separate constituents. Simple theory correctly predicts, for soluble surfactants, a large increase of surface pressure upon mixing an anionic and a cationic solution having the same surface pressure, and, for insoluble surfactants, a decrease of surface pressure upon mixing at a given area per long chain ion. These effects are due to the different adsorption characteristics of the four electroneutral combinations involved, and will occur even in the absence of specific surface interactions.

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Zusammenfassung Es wurden bekannte Oberflächendrucke für Mischfilme von Aniontensiden und Kationtensiden mit theoretischen Voraussagen, begründet auf dem Grenzflächenverhalten der einzelnen Komponenten, verglichen. Die einfache Theorie sagt richtig voraus, daß die Mischung zweier wäßriger Lösungen von Aniontensid bzw. Kationtensid mit gleichem Oberflächendruck, eine starke Erhöhung des Oberflächendruckes zur Folge haben muß, während die Mischung zweier unlöslicher Filme bei gegebener Tensidadsorption den Oberflächendruck herabsetzt. Dieses Verhalten wird aufgrund der verschiedenen Adsorptionseigenschaften der vier betreffenden Salze gedeutet, und ist von spezifischen Oberflächenwechselwirkungen unabhängig.

     

Dilational rheology of protein films adsorbed at fluid interfaces

This report aims at (i) presenting a quantitative interpretation of interfacial dilational moduli (|E|) for four proteins at three different interfaces and (ii) identifying the main parameters responsible. The proteins were adsorbed from aqueous solution against air, n-tetradecane and sunflower seed oil, as a function of protein concentration and adsorption time.Experimentally, a dynamic drop tensiometer is a convenient instrument to generate the required sinusoidal oscillations for compression/expansion of interfaces (Benjamins et al., 1996 [1]).Theoretically, a simple two-dimensional solution model with a constant molecular area of the protein described the data only at fairly low pressures. Much better agreement over the entire elastic range was found with a recent extension of the model. This extension accounted for adsorbed proteins adopting smaller molecular areas with increasing surface pressure.Three factors dominated the values of the dilational modulus: (i) rigidity of protein molecules, (ii) degree of interfacial non-ideality and (iii) tension of the clean interface (Benjamins et al., 2006 [2]). The last factor is clearly of great relevance to food emulsions.For each protein at different interfaces, the elasticity increased with the enthalpy parameter (Η^S) of the equation of state. Elasticity and Η^S both increased with the clean-interface tension, γ⁰, i.e., with decreasing polarity of the interface (Benjamins et al., 2006 [2]; Fainerman et al., 2003 [3]). The elasticity of the different proteins also increased with increasing rigidity of the molecules, indicating a lower compressibility of the molecular area at the interface.Pure viscosities were never observed in our experience. However, viscoelastic behaviour was found at high pressures, i.e., in densely packed surfaces. The measured viscous phase angles strongly decreased at still higher pressures, indicating that the active relaxation mechanism slowed down with increasing molecular packing density. Specific kinetic models are yet to be developed for such mechanisms.     

Surface-pressure isotherms of monolayers formed by microsize and nanosize particles

The thermodynamic model of a 2D solution developed earlier for protein monolayers at liquid interfaces is generalized for monolayers composed of micro- and nanoparticles. Surface pressure isotherms of particle monolayers published in the literature for a wide range of particles sizes (between 75 microm and 7.5 nm) are described by the theoretical model with one modification. The calculations of surface pressure pi on area A provide satisfactory agreement with the experimental data. The theory also yields reasonable cross-sectional area values of the solvent molecule water in the range between 0.12 and 0.18 nm2, which is almost independent of particle size. Also, the area per particle in a closely packed monolayer obtained from the theory is quite realistic.     

Substrate specificity analysis of protein kinase complex Dbf2-Mob1 by peptide library and proteome array screening

Background  

The mitotic exit network (MEN) is a group of proteins that form a signaling cascade that is essential for cells to exit mitosis in Saccharomyces cerevisiae. The MEN has also been implicated in playing a role in cytokinesis. Two components of this signaling pathway are the protein kinase Dbf2 and its binding partner essential for its kinase activity, Mob1. The components of MEN that act upstream of Dbf2-Mob1 have been characterized, but physiological substrates for Dbf2-Mob1 have yet to be identified.     

Steady streaming around a spherical drop displaced from the velocity antinode in an acoustic levitation field

The steady (acoustic) streaming associated with a sphericaldrop displaced from the velocity antinode of a standing waveis studied. The ratio of the particle size to the acoustic wavelengthis treated as small but non-zero, and the solution is developedin the form of a two-term expansion in terms of the correspondingsmallness parameter. The drop viscosity is assumed to be muchhigher than that of the surrounding fluid, which is the casefor a drop in a gas medium. There are essentially three distinctregions where the steady streaming flow is analysed: insidethe drop (internal circulation), in the Stokes shear-wave layerat the surface on the gas side, and the gas outside the Stokeslayer (the outer streaming region). Solutions for the internalcirculation and the outer streaming are obtained in the limitof small Reynolds number. Despite the gas-to-liquid viscosity ratio being small, the outerstreaming may be dramatically affected by the fact that thesphere is liquid as opposed to solid. The parameter that measuresthe effect of liquidity is essentially the viscosity ratio dividedby the relative (to the particle size) thickness of the Stokeslayer. The case of a solid sphere is recovered by letting thisparameter go to zero.