Effect of Hydrophobic Chain Length of Amphiphilic Silicone Oil (Copolymer) on the Nonionic Surfactant-Layer Curvature

Abstract

Phase behavior and formation of self-assemblies in ternary water/ penta(oxyethylene) dodecyl ether (C12EO5)/amphiphilic silicone copolymer, poly(dimethylsiloxane)−poly(oxyethylene) (Si m C3EO3.2) systems, were investigated. These silicone copolymers are very hydrophobic because of the short EO chain and are essentially water-insoluble amphiphilic oils, similar to high alcohols or fatty acids. In general, the surfactant layer curvature becomes less positive upon addition of amphiphilic oils, similar to what happens with high alcohols or fatty acids. This is what is observed for m = 5.8. However, in the ternary water/C12EO5/Si25C3EO3.2 system, the surfactant layer curvature becomes more positive, and micellar cubic, normal hexagonal, and bicontinuous cubic phases are also formed, although a lamellar liquid crystal forms only in the water−C12EO5 system. In the liquid crystal regions, it was found that Si25C3EO3.2 is not dissolved in the thin bilayer of the C12EO5 lamellar phase, whereas the long and bulky Si25C3 chain forms an oil core in those cubic, hexagonal, and bicontinuous cubic phases, in which the surfactant is absorbed at the hydrophobic interface of each aggregate. Then, this opposite effect of added amphiphilic silicone copolymer or oil to the surfactant solution is attributed to the long and flexible Si25C3 chain which makes an oil pool inside the aggregates. This different behavior of small and large Si m C3 chains is also observed in the cloud temperatures. In fact, the cloud temperature of C12EO5 aqueous solution decreases upon addition of Si5.8C3EO3.2, whereas it increases by adding a long hydrophobic chain, like Si14C3EO3.2 or Si25C3EO3.2 silicone oil. It was confirmed by DLS that long rod micelles, which are present in the water−C12EO5 system, become small spherical micelles upon addition of Si25C3EO3.2. Consequently, hydrophobic Si m C3EO3.2 changes the micellar shape in two different ways depending on the length of the Si m C3 chain. For small chains (e.g., m = 5.8), the surfactant−copolymer layer curvature changes to less positive by forming a mixed layer. Long and bulky chains (e.g., m = 14, 25) make an oil core and this tends to make the curvature more positive, being this effect pronounced with increasing the hydrophobic chain length.

Small-angle X-ray scattering (SAXS) study on nonionic fluorinated micelles in aqueous system

“…This is because the hydrophobic chain of the polymeric oil is longer than that of the host surfactant molecule. The present situation is somewhat similar to the report by Kaneko et al [44]. They reported the formation of hydrophobic oil pool in the micellar core upon adding silicon copolymer oils with longer hydrophobic part compared to the host surfactant molecule.…”

Phase behavior and preparation of mesoporous silica in aqueous mixtures of fluorinated surfactant and hydrophobic fluorinated polymer

“…Hence, two kinds of lamellar phases exist, one rich in surfactant and the other rich in polymer in the water/C 8 F 17 EO 10 /(C 3 F 6 O) n COOH system. This behavior has been previously found in several surfactant-polymer systems [36][37][38][39] and it is associated with packing restrictions, as will be discussed later.…”

Structure of Diglycerol Polyisostearate Nonionic Surfactant Micelles in Nonpolar Oil Hexadecane: A SAXS Study

“…Due to an unfavorable direct contact between the hydrophilic part and oils, reverse micelles are usually formed when an amphiphile is added into nonpolar solvents. Reverse micelles are mostly observed in the ternary mixtures of surfactant/water/oil, mostly in oil rich regions [11][12][13] . Furthermore, they have also been observed in aqueous systems of lipophilic surfactant in surfactant rich regions 14,15 .…”