Cd. Han et al., Lattice disordering/ordering and demicellization/micellization transitionsin highly asymmetric polystyrene-block-polyisoprene copolymers, MACROMOLEC, 33(10), 2000, pp. 3767-3780
Two kinds of transitions involving a change in molecular assembly, lattice
disordering/ordering transition (LDOT) and demicellization/micellization tr
ansition (DMT), in highly asymmetric polystyrene-bloch-polyisoprene (SI dib
lock) copolymers were investigated using oscillatory shear rheometry, trans
mission electron microscopy (TEM), and small-angle X-ray scattering (SAXS).
For the study, three highly asymmetric SI diblock copolymers having the vo
lume fractions of polystyrene (PS) block of 0.11, 0.13, and 0.16, respectiv
ely, were synthesized using anionic polymerization. In highly asymmetric bl
ock copolymer, LDOT is defined as a transition where the long-range order o
f microdomains is lost during heating, giving rise to a disordered arrangem
ent of spheres with short-range liquidlike order (termed disordered spheres
or micelles), and DMT is defined as a transition where all microdomains di
sappear during heating and are transformed into the micelle-free homogeneou
s state in which the component polymers are mixed on a molecular level and
only thermally induced composition fluctuations may exist DMT may be regard
ed as a pseudo-phase transition, involving effectively a finite number of m
olecules and hence occurring over a finite range (possibly a narrow range)
of temperatures. It was found that the three highly asymmetric SI diblock c
opolymers underwent, during heating, first lattice disordering and then dem
icellization transitions. The values of LDOT temperature (T-LDOT) and DMT t
emperature (T-DMT) for the highly asymmetric SI diblock copolymers were det
ermined by careful analysis of SAXS results, and the value T-DMT determined
by oscillatory shear rheometry was found in good agreement with SAXS resul
ts. The LDOT determined from SAXS was confirmed by TEM, showing the existen
ce of disordered spheres at thermal equilibrium at T-LDOT less than or equa
l to T less than or equal to T-DMT.