VISCOELASTIC CONTRAST AND KINETIC FRUSTRATION DURING POLY(ETHYLENE OXIDE) CRYSTALLIZATION IN A HOMOPOLYMER AND A TRIBLOCK COPOLYMER - COMPARISON OF ULTRASONIC AND LOW-FREQUENCY RHEOLOGY
I. Alig et al., VISCOELASTIC CONTRAST AND KINETIC FRUSTRATION DURING POLY(ETHYLENE OXIDE) CRYSTALLIZATION IN A HOMOPOLYMER AND A TRIBLOCK COPOLYMER - COMPARISON OF ULTRASONIC AND LOW-FREQUENCY RHEOLOGY, Macromolecules, 31(20), 1998, pp. 6917-6925
We report a combined study using an ultrasonic shear wave reflection t
echnique and conventional low-frequency rheology for the investigation
of the crystallization kinetics and melting of a poly(ethylene oxide)
(PEO) homopolymer and a poly(ethylene oxide)-polystyrene-poly(ethylen
e oxide) (PEO-PS-PEO) triblock copolymer. Both isochronal heating and
isothermal/isochronal kinetic measurements of the complex dynamic shea
r modulus G have been performed with high-frequency (ultrasonic) and
conventional low-frequency rheology at frequencies of 3.5 MHz and 0.16
Hz, respectively. The different frequencies create a different viscoe
lastic contrast between the two phases in the two experiments. In both
experiments the system can be regarded as a composite material made o
f spherulites within the amorphous matrix, and the increase of the she
ar modulus with time is attributed to the growing of spherulites at th
e expense of the amorphous matrix. The kinetics of crystallization are
analyzed in the framework of the Avrami equation using different mech
anical models that describe a two-phase composite. Although a simple p
arallel model composed of an amorphous and a spherulitic phase suffice
s to describe the ultrasonic shear experiment, a more complex model in
volving phase inversion is required to account for the abrupt dependen
ce of the shear modulus on time in rheology. The effect of external sh
ear is to speed up the kinetics. The ultrasonic shear experiments for
the homopolymer crystallization are compared with those of the tribloc
k copolymer, and it is found that the final modulus in the latter is c
onsiderably lower than that in the former experiment. This is explaine
d by the less perfect structure of the lamellae and/or the spherulites
in the copolymer and the kinetic frustration of the crystallization (
for low undercooling) due to the glassy PS microphase. It is shown tha
t the comparison of high and low-frequency rheology can provide new in
sights on the crystallization process and the final morphology in semi
crystalline polymers.