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Colloids and Surfaces, 3-4(12), p. 213-225

DOI: 10.1016/0166-6622(84)80263-2

Colloids and Surfaces, (12), p. 213-225

DOI: 10.1016/0166-6622(84)80101-8

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Behaviour of a lyotropic-smectic liquid crystal between mica surfaces a study of the fully hydrated egg-lecithin

Journal article published in 1984 by Lisbeth Ter-Minassian-Saraga, Éric Perez
This paper was not found in any repository, but could be made available legally by the author.
This paper was not found in any repository, but could be made available legally by the author.

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Abstract

The behaviour of three egg-lecithin (EL)—water (W) mixtures, 60% (w/w):I, 50% (w/w):II and 30% (w/w):III, squeezed out or sucked in between two mica surfaces was investigated using an apparatus designed by J.N. Israelachvili. Mixture I is a lyotropic-smectic liquid crystal (LSLC), in contrast to II and III in which the LSLC is in equilibrium with a separated phase of excess water. The force F applied to the micasheet holders, the “separation” D between the mica surfaces and the average refractive index were measured for 1 < D < 200 nm.A stepwise-thinning process was mainly observed on compressing mixtures I and II from separation 30 < D < 60 nm down to the minimum reproducible separation Dmin, 9.0 ± 0.7 nm, which corresponded to the flattening of the mica surfaces. The steps ΔD were equal to multiples of λ = 5.5 ± 0.4 nm for sample I and of λ = 5.3 ± 0.3 nm for sample II.The contact area of the flattened-mica sheets increased with the force F at separation Dmin. Assuming that an effective elastic parameter can be defined for our composite system (mica sheet + glue), we interpret the F—contact-area dependence using the theory of Johnson et al. and deduce values of average normal pressures or stresses of the order of 10 mN m−2 on the flat mica—mica contact. At such pressures the values of λ and the repeat distance of the LSLC formed by EL + W and measured by X-ray diffraction are similar.The refractive index n of I is independent of separation for Dmin < D < 50 nm but its value increases when D decreases for II and III. It appears that excess water is selectively extruded when F increases and D decreases. We suggest that, at maximum stress and Dmin = 9 nm, the two mica surfaces are separated by two poorly hydrated EL bi-layers, while the EL polar groups in contact with the mica surface are almost completely dehydrated.