1 research outputs found
Influence of Counterions on Lauric Acid Vesicles and Theoretical Consideration of Vesicle Stability
The counterions, including inorganic cations, Na<sup>+</sup> and
Cs<sup>+</sup>, and organic cation, (C<sub>2</sub>H<sub>5</sub>)<sub>4</sub>N<sup>+</sup>, influence the phase behavior and self-assembled
structures of the lauric acid (LA) in water. Dissolving LA in NaOH,
CsOH, and (C<sub>2</sub>H<sub>5</sub>)<sub>4</sub>NOH (tetraethylammonium
hydroxide, TeAOH) solutions, respectively, we observed that the three
systems totally exhibited the same phase behavior, from birefringent
L<sub>α</sub> phase/precipitates (P) → L<sub>α</sub> phase → L<sub>α</sub> phase/L<sub>1</sub> (micelles)
→ L<sub>1</sub>. The temperature influence on phase behavior
was investigated, and with an increase of temperature, we observed
that less phase behavior change occurred in the systems of LA/CsOH/H<sub>2</sub>O and LA/TeAOH/H<sub>2</sub>O, while the phase behavior of
the LA/NaOH/H<sub>2</sub>O system exhibited an obvious change. Cryogenic
transmission electron microscopy (cryo-TEM) images demonstrated that
the different microstructures of L<sub>α</sub> phase samples
in the three systems existed. For the systems of LA/NaOH/H<sub>2</sub>O and LA/TeAOH/H<sub>2</sub>O, uni- and multilamellar vesicles coexist
for L<sub>α</sub> phase samples, as both the morphology and
size of these vesicles are polydisperse. The curvatures of the bilayer
membranes of the two systems are considered to vary from positive,
zero, and even negative. However, only spherically unilamellar vesicles
exist in the system of LA/CsOH/H<sub>2</sub>O, indicating that the
bilayers are more rigid than those in the LA/NaOH/H<sub>2</sub>O and
LA/TeAOH/H<sub>2</sub>O systems. Through the combination of the Helfrich
curvature energy theory and the mass-action model, the effective bending
constant <i>K</i> = 0.5 <i>k</i><sub>B</sub><i>T</i> in the LA/CsOH/H<sub>2</sub>O system was obtained, demonstrating
that the unilamellar vesicles are stabilized by thermal fluctuations.
A primary discussion for the effect of the nature of counterions on
the stability and deformation of the vesicles is presented