Phase behavior and aggregate formation for the aqueous monoolein system mixed with sodium oleate and oleic acid

Citation
J. Borne et al., Phase behavior and aggregate formation for the aqueous monoolein system mixed with sodium oleate and oleic acid, LANGMUIR, 17(25), 2001, pp. 7742-7751
Citations number
47
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
LANGMUIR
ISSN journal
07437463 → ACNP
Volume
17
Issue
25
Year of publication
2001
Pages
7742 - 7751
Database
ISI
SICI code
0743-7463(200112)17:25<7742:PBAAFF>2.0.ZU;2-3
Abstract
The phase behavior and microstructure of the two ternary systems monoolein (MO)-sodium oleate (NaO)-water ((H2O)-H-2) and MO-oleic acid (OA)-(H2O)-H-2 are studied by a combination of optical microscopy, cryo-transmission elec tron microscopy, small-angle X-ray diffraction, and NMR methods. The result s demonstrate significant differences in phase behavior between the two sys tems. The isothermal phase diagram of the MO-NaO-(H2O)-H-2 system is domina ted by a large lamellar liquid crystalline phase that shows an ideal swelli ng up to high water contents. Stable vesicles are the dominant aggregates a t water concentration > 90 wt%. The existence of a lamellar phase is, howev er, absent from the MO-OA-(H2O)-H-2 system, where the largest single-phase region is a reversed hexagonal liquid crystalline phase, HII, at low water content. A similar water-poor Hii phase is also identified for the MO-NaO-( H2O)-H-2 system. The two types of bicontinuous cubic structures, gyroid (C- G) and diamond (C-D), formed by the binary MO-(H2O)-H-2 system are also pre sent in the ternary systems. Part of the single C-G phase initially formed by the ternary system with NaO is found to be metastable and becomes destab ilized within a few weeks, leaving the rest of the C-G phase which is stabl e like other thermodynamically stable phases for the system. A cubic phase with a reversed micellar type structure is characterized for the oleic acid system. The experimentally determined phase diagrams and the phase structu res can be qualitatively understood in terms of the geometry of the lipid m olecule in combination with electrostatic effects.