POLY(ETHYLENE OXIDE)-POLY(PROPYLENE OXIDE)-POLY(ETHYLENE OXIDE) BLOCK-COPOLYMER SURFACTANTS IN AQUEOUS-SOLUTIONS AND AT INTERFACES - THERMODYNAMICS, STRUCTURE, DYNAMICS, AND MODELING

Citation
P. Alexandridis et Ta. Hatton, POLY(ETHYLENE OXIDE)-POLY(PROPYLENE OXIDE)-POLY(ETHYLENE OXIDE) BLOCK-COPOLYMER SURFACTANTS IN AQUEOUS-SOLUTIONS AND AT INTERFACES - THERMODYNAMICS, STRUCTURE, DYNAMICS, AND MODELING, Colloids and surfaces. A, Physicochemical and engineering aspects, 96(1-2), 1995, pp. 1-46
Citations number
174
Categorie Soggetti
Chemistry Physical
ISSN journal
09277757
Volume
96
Issue
1-2
Year of publication
1995
Pages
1 - 46
Database
ISI
SICI code
0927-7757(1995)96:1-2<1:POOOB>2.0.ZU;2-8
Abstract
The association properties of poly(ethylene oxide)-block-poly(propylen e oxide)-block-poly(ethylene oxide) (PEO-PPO-PEO) copolymers (commerci ally available as Poloxamers and Pluronics) in aqueous solutions, and the adsorption of these copolymers at interfaces are reviewed. At low temperatures and/or concentrations the PEO-PPO-PEO copolymers exist in solution as individual coils (unimers). Thermodynamically stable mice lles are formed with increasing copolymer concentration and/or solutio n temperature, as revealed by surface tension, light scattering, and d ye solubilization experiments. The unimer-to-micelle transition is not sharp, but spans a concentration decade or 10 K. The critical micelli zation concentration (CMC) and temperature (CMT) decrease with an incr ease in the copolymer PPO content or molecular weight. The dependence of CMC on temperature, together with differential scanning calorimetry experiments, indicates that the micellization process of PEO-PPO-PEO copolymers in water is endothermic and driven by a decrease in the pol arity of ethylene oxide (EO) and propylene oxide (PO) segments as the temperature increases, and by the entropy gain in water when unimers a ggregate to form micelles (hydrophobic effect). The free energy and en thalpy of micellization can be correlated to the total number of EO an d PO segments in the copolymer and its molecular weight. The micelles have hydrodynamic radii of approximately 10 nm and aggregation numbers in the order of 50. The aggregation number is thought to be independe nt of the copolymer concentration and to increase with temperature. Ph enomenological and mean-field lattice models for the formation of mice lles can describe qualitatively the trends observed experimentally. In addition, the lattice models can provide information on the distribut ion of the EO and PO segments in the micelle. The PEO-PPO-PEO copolyme rs adsorb on both air-water and solid-water interfaces; the PPO block is located at the interface while the PEO block extends into the solut ion, when copolymers are adsorbed at hydrophobic interfaces. Gels are formed by certain PEO-PPO-PEO block copolymers at high concentrations, with the micelles remaining apparently intact in the form of a ''crys tal''. The gelation onset temperature and the thermal stability range of the gel increase with increasing PEO block length. A comparison of PEO-PPO copolymers with PEO-PBO and PEO-PS block copolymers and C(i)E( j) surfactants is made, and selected applications of PEO-PPO-PEO block copolymer solutions (such as solubilization of organics, protection o f microorganisms, and biomedical uses of micelles and gels) are presen ted.