Mp. Heitz et al., WATER CORE WITHIN PERFLUOROPOLYETHER-BASED MICROEMULSIONS FORMED IN SUPERCRITICAL CARBON-DIOXIDE, JOURNAL OF PHYSICAL CHEMISTRY B, 101(34), 1997, pp. 6707-6714
We report new experimental data on the ability of a perfluoropolyether
-based surfactant (PFPE) to form stable reverse micelles in supercriti
cal CO2. Previous work from our groups showed that PFPE reverse micell
es formed in CO2 can host a wide variety of hydrophiles and even provi
de an environment capable of solubilizing large proteins [Johnston, K.
P.; Harrison, K. L.; Clarke, M. J.; Howdle, S. M.; Heitz, M. P.; Brig
ht, F. V.; Carlier, C.; Randolph, T. W. Science 1996, 271, 624-626]. I
n the current work we report cloud point data for PFPE in CO2, X-band
EPR studies, and time-resolved anisotropy measurements. The cloud poin
t data show that a one-phase water-in-CO2 microemulsion can be formed
with a nominal molar water-to-surfactant ratio (R) of 20.7 at 45 degre
es C and 158.1 bar. EPR experiments on PFPE (with 4-hydroxy-TEMPO) and
Mn(PFPE)I show that PFPE aggregates in CO2 at pressures below which a
water pool can be formed. Stable Mn(PFPE)2 micelles can also be forme
d in supercritical CO2, and the internal water pool within these micel
les is able to ionize manganese, demonstrating that the water within t
his pool differs significantly from water within the CO2 bulk phase. E
PR results also suggest that these micelles exist in a nonspherical fo
rm. The rotational reorientation kinetics of two model fluorescent pro
bes, rhodamine 6G and lissamine rhodamine B sulfonyl hydrazine, are de
scribed well by a biexponential decay law. The faster rotational reori
entation time (phi(fast)) is approximately 100 ps and remains constant
regardless of CO2 continuous phase density or R. We interpret the flu
orophore rotational dynamics using three established models: a wobblin
g-in-a-cone model in which the fluorophore precesses about its emissio
n transition dipole, a lateral diffusion model wherein the probe diffu
ses along the reverse micelle headgroup/water core interface boundary,
and an anisotropic rotor model where the micelle shape itself is nons
pherical.