1970
DOI: 10.1039/sd9700100118
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Interfacial energies of clean mica and of monomolecular films of fatty acids deposited on mica, in aqueous and non-aqueous media

Abstract: The influence of a variety of media on solid/fluid interfacial energies has been measured by a cleavage technique. The solid used was mica, chosen because of its near perfect cleavage and ideal bulk properties. Solid/vapour and solid/liquid interfacial energies, ysv and y s ~, were measured by cleaving specimens in the form of strips, first, in an atmosphere of the vapour and then with the specimens completely immersed in the corresponding liquid. Samples of mica coated with monomolecular films of fatty acids … Show more

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Cited by 16 publications
(4 citation statements)
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“…The interfacial energy of freshly cleaved mica in water is 107 mJ m −2 ; addition of an amphiphilic surfactant (lauryl acid) that coats the mica surface reduces it to 8 mJ m −2 . 27 A coacervate consisting of two polar polyelectrolytes - HA and fp-151-RGD - effectively decreases interfacial energy to <1 mJ m −2 . The low interfacial energy of coacervates (~0.1 mJ m −2 ) has recently been confirmed by another group using atomic force microscopy.…”
Section: Resultsmentioning
confidence: 99%
“…The interfacial energy of freshly cleaved mica in water is 107 mJ m −2 ; addition of an amphiphilic surfactant (lauryl acid) that coats the mica surface reduces it to 8 mJ m −2 . 27 A coacervate consisting of two polar polyelectrolytes - HA and fp-151-RGD - effectively decreases interfacial energy to <1 mJ m −2 . The low interfacial energy of coacervates (~0.1 mJ m −2 ) has recently been confirmed by another group using atomic force microscopy.…”
Section: Resultsmentioning
confidence: 99%
“…Measuring the γ associated with capillary/meniscus forces has garnered significant attention using the SFA and AFM and through theoretical models. ,, Once a capillary bridge between two surfaces is formed, as in the case of the experiments performed in this article, the surfaces are held together by the meniscus forces generated in the bridge. This adhesion corresponds to the γ of the aqueous/coacervate phase interface and is directly connected to the capillary pressure difference (Δ P ) across this interface, as defined by the Young–Laplace equation. normalΔ P = γ ( 1 r 1 + 1 r 2 ) …”
Section: Resultsmentioning
confidence: 99%
“…Freshly cleaved mica is one of the most suitable substrates for wetting experiments because the resulting surface is hard, homogeneous, impermeable, and atomically flat. As the surface energy of mica of about 300 mJ/m 2 (in air) is much higher than the surface tensions of hexane (18.6 mN/m) and the dendrimer (29.3 mN/m), it satisfies the macroscopic condition for spreading ( S > 0). However, this did not occur, as is shown in Figure a, where one can see droplets on top of a thin layer adsorbed directly on the substrate.…”
Section: Resultsmentioning
confidence: 99%