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Solubilization-emulsification mechanisms of detergency

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C.A. Miller and K.H. Raney/Colloids Surfaces A: Physicochem. Eng. Aspects 74 (1993) 169-215 173<br />

Fig. 2. Phase diagram <strong>of</strong> C 12E 5-water system [21]. L 1,<br />

L 2, and L 3 denote isotropic liquids; Lα, H 1, and V 1<br />

denote lamellar, hexagonal and viscous isotropic<br />

liquid crystalline phases, respectively. Reprinted with<br />

permission <strong>of</strong> the Royal Society <strong>of</strong> Chemistry.<br />

relatively low surfactant concentrations. As the<br />

particles <strong>of</strong> a liquid crystal do not coalesce as<br />

readily as liquid drops, the dispersions <strong>of</strong> La are<br />

frequently less turbid than those <strong>of</strong> L 3, a<br />

property which can be used to locate phase<br />

transition temperatures at which the La and L 3<br />

phases form [22]. At the highest temperatures<br />

shown in Fig. 2 the surfactant-rich liquid phase<br />

L 2 coexists with water.<br />

For more hydrophilic surfactants such as<br />

n-dodecyl hexaoxyethylene monoether (C 12E 6),<br />

clouding occurs at higher temperatures.<br />

Moreover, the Lα and L 3 phases do not appear<br />

at low surfactant concentrations; the La phase<br />

transforms continuously into L 2, and the cloud<br />

point curve is the only feature <strong>of</strong> this part <strong>of</strong> the<br />

phase diagram (see Fig.3). Phase diagrams for<br />

various binary nonionic surfactant-water<br />

systems are given by Mitchell et al. [23].<br />

Temperature effects are weaker for ionic<br />

surfactants and generally act in the opposite<br />

direction. Since the Debye length, a measure <strong>of</strong><br />

the electric double layer thickness, is<br />

proportional to (kT) 1/2 , where kT is the<br />

characteristic free energy <strong>of</strong> random thermal<br />

Fig. 3. Phase diagram <strong>of</strong> C 12E 6-water system [23].<br />

The symbols for the phases are as in Fig. 2 except<br />

that S is a solid phase and W is a water-rich liquid<br />

phase. Reprinted with permission <strong>of</strong> the Royal<br />

Society <strong>of</strong> Chemistry.<br />

motion, higher temperatures make ionic<br />

surfactant films more hydrophilic, with a greater<br />

tendency to curve toward an oil-in-water<br />

configuration. However, the addition <strong>of</strong><br />

inorganic salts has the opposite effect,<br />

compressing electric double layers and causing<br />

ionic surfactant films to become less<br />

hydrophilic. In some cases, a- second liquid<br />

phase is ultimately formed as salinity increases,<br />

i.e. the behavior is similar to clouding <strong>of</strong><br />

non-ionic surfactant solutions discussed above.<br />

This phenomenon was observed by McBain<br />

many years ago for aqueous soap solutions<br />

[23b]. Another example is shown along the<br />

upper boundary <strong>of</strong> Fig. 4 [24], with NaCl added<br />

to the sodium salt <strong>of</strong> a commercial ethoxylated<br />

sulfate based on a C 12-C 13 alcohol and<br />

containing an average <strong>of</strong> three ethylene oxide<br />

groups (Neodol 23-3S). As Fig. 4 indicates,<br />

multiphase regions involving the lamellar liquid<br />

crystal La are observed at even higher salinities.<br />

In other systems, for instance the Aerosol<br />

OT-NaCl-water system, the first phase formed<br />

upon increasing the salinity is the lamellar liquid<br />

crystalline phase [25,26]. Indeed, such behavior<br />

is typical for anionic surfactant-short-chain<br />

alcohol systems investigated for possible use in

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