Manifestation of phase separation processes in oscillatory shear: droplet-matrix systems versus co-continuous morphologies

Citation
I. Vinckier et Hm. Laun, Manifestation of phase separation processes in oscillatory shear: droplet-matrix systems versus co-continuous morphologies, RHEOL ACT, 38(4), 1999, pp. 274-286
Citations number
24
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
RHEOLOGICA ACTA
ISSN journal
00354511 → ACNP
Volume
38
Issue
4
Year of publication
1999
Pages
274 - 286
Database
ISI
SICI code
0035-4511(199910)38:4<274:MOPSPI>2.0.ZU;2-1
Abstract
Phase separation processes in mixtures of poly-alpha-methylstyrene-co-acryl onitrile (P alpha MSAN) and poly-methylmethacrylate (PMMA) with lower criti cal solution temperature (LCST) behavior have been studied, focusing on the manifestation of the interface in oscillatory shear measurements. By using blends of different composition, systems with a droplet-matrix morphology or a co-continuous structure are generated during the phase separation proc ess. The feasibility of probing this morphology development by rheological measurements has been investigated. The development of a disperse droplet p hase leads to an increase in the elasticity of the blend at low frequency, showing up as a shoulder in the plot of storage modulus versus frequency. H ere, the droplet growth is unaffected by the shear amplitude up to strains of 0.2; therefore the resulting dynamic data are suitable for quantitative analysis. In contrast, for blends in which phase separation leads to a co-c ontinuous structure, the storage modulus shows a power law behavior at low frequency and its value decreases as time proceeds. For the latter systems, effects of the dynamic measurement on the morphology development have been observed, even for strain amplitudes as low as 0.01. To probe the kinetics of morphology evolution in droplet-matrix systems, measurements of the tim e dependence of the dynamic moduli at fixed frequency should be performed ( for a whole series of frequencies). Only from such measurements, curves of the frequency dependence of the moduli at a well defined residence time can be constructed. From fitting these curves to the emulsion model of Paliern e, the droplet diameter distribution at that particular stage in the phase separation and growth process can be obtained. It is not appropriate to use a simplified version of the Palierne model containing only the average dro plet size, because a morphology with too broad a size distribution is gener ated.