On the colloidal stability of water-in-oil emulsions a self-consistent field approach
β Scribed by F.A.M. Leermakers; Y.S. Sdranis; J. Lyklema; R.D. Groot
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 765 KB
- Volume
- 85
- Category
- Article
- ISSN
- 0927-7757
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β¦ Synopsis
We apply the self consistent field (SCF) theory for chain molecules in inhomogeneous systems, originated by Scheutjens and 1, l eer. t o study the interaction between Iwo water droplets in oil in the presence of surfactants . The modelling of interacting polymer-covered rigid interfaces is the classical application in the SCF approach . In this paper we study two surfactant-covered liquid-liquid interfaces near contact . This can he done by an osmotic pressure 'experiment'.
Our analysis indicates that for (surfactant-stabilised) water-in-oil emulsions two types of colloidal instability can be distinguished: (1) coalescence (flocculation in the primary minimum leading to a reduction of the number of droplets) and ( 2) aggregation (flocculation in secondary minimum . formation of clusters of droplets, i .e . a reduction of the number of kinetically active droplets but retaining their individuality) . The surfactant adsorbed at the water oil interface influences these two types of instabilities it) different ways . A high surfactant concentration effectively protects against coalescence, whereas, especially when the molecular weight of the oil molecules is larger than that of the surfactants. aggregation is promoted . Analysis of the interaction curves for lamellar interfaces enables the prediction of the macroscopic contact angle between two droplets . We show that this angle can vary strongly with the type of oil used . Protection against aggregation can be obtained by carefully choosing the surfactant in connection with the oil used .
π SIMILAR VOLUMES
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The interfacial rheological properties of the crude oil-water interface have been measured. It is found that the rheological properties are time dependent and the film takes at least 8 h to attain equilibrium. During this period the surface elasticity and viscosity increase markedly with time, with