ON THE STRUCTURE OF POLYMERIC MICELLES - SELF-CONSISTENT-FIELD THEORYAND UNIVERSAL PROPERTIES FOR VOLUME FRACTION PROFILES

Citation
Fam. Leermakers et al., ON THE STRUCTURE OF POLYMERIC MICELLES - SELF-CONSISTENT-FIELD THEORYAND UNIVERSAL PROPERTIES FOR VOLUME FRACTION PROFILES, Macromolecules, 28(9), 1995, pp. 3434-3443
Citations number
37
Categorie Soggetti
Polymer Sciences
Journal title
ISSN journal
00249297
Volume
28
Issue
9
Year of publication
1995
Pages
3434 - 3443
Database
ISI
SICI code
0024-9297(1995)28:9<3434:OTSOPM>2.0.ZU;2-R
Abstract
Polymeric micelles composed of asymmetric block copolymers of the type A(n)B(m) in a solvent S are analyzed by the self-consistent-field the ory due to Scheutjens and Fleer. Micelle formation is studied in a sph erical lattice geometry. An unfavorable mixing of A and S segments dri ves the self-assembly process, leading to micelles which can vary thei r aggregation number according to the conditions in solution. We study the micelle thermodynamics and the micelle structure as a function of the solvency of the B tails; the Flory-Huggins interaction parameter chi(SB) has been varied from 0 (good solvent) to 0.5 (Theta solvent). With decreasing solvency the critical micelle volume fraction (CMV) de creases and the micelle size increases. The micelles have a dense core and a more dilute brushlike corona structure. Our main interest is in the density profiles Of the corona. We distinguish four regimes in th ese profiles, denoted proximal, central, parabolic, and distal. The pr oximal part of the B profile is near the core and is nonuniversal, the central part is a power law which is in good agreement with the scali ng predictions of Daoud and Cotton, in the third regime the profile of the polymer segments is roughly parabolic, and in the distal regime a n exponential decay toward the bulk. solution occurs. The relative imp ortance of these regimes depends on the molecular architecture. For ex ample, increasing the number of core (A) segments causes the central p art first to grow and then to shrink in favor of the parabolic regime.