Y. Xiong et E. Kiran, Kinetics of pressure-induced phase separation (PIPS) in polystyrene plus methylcyclohexane solutions at high pressure, POLYMER, 41(10), 2000, pp. 3759-3777
Kinetics of pressure-induced phase separation in polystyrene + methylcycloh
exane solutions at high pressures (up to 25 MPa) have been studied as a fun
ction of polymer molecular weight (50 000 and 700 000), polymer concentrati
on (in the range from 4 to 16% by mass) and the quench depth (in the range
of 0.1-2 MPa), using time- and angle-resolved light scattering in a unique
high-pressure cell with a path length of 250 mu m.
The results show that phase separation in solutions at critical polymer con
centrations proceeds by spinodal decomposition which is displayed by a spin
odal ring or a maximum in the scattered light intensities with angle. The t
ime interval for the observation of spinodal ring was observed to depend on
the quench depth. The ring collapse was observed to take place within the
range of 3-160 s, shorter times being associated with deeper quenches. Phas
e separation in solutions at off-critical concentrations was observed to pr
oceeded by nucleation and growth mechanism for shallow quenches (as reflect
ed by the absence of a maximum in the angular variation of the scattered li
ght intensities), but by the spinodal decomposition process for deep quench
es.
The characteristic wave number q(m) corresponding to the maximum scattered
light intensity I,was observed to be non-stationary and moved to lower wave
numbers with time for all quenches leading to spinodal decomposition. The
time evolution of q(m) and I-m were observed to obey the power law approxim
ations q(m) similar to t(-alpha) and I-m similar to t(beta). The exponents
alpha and beta were found to increase with the quench depth, while however,
maintaining a beta similar or equal to 2 alpha relationship. The scaling c
haracteristics of the structure factor were also analyzed. It was found tha
t for a given quench depth the data at different times could be reduced to
a single master curve when normalized with respect to the maximum in the sc
attered light intensity and the corresponding wave number. Calculations of
the apparent diffusivity, based on the estimated values for the early stage
characteristic wave number q(m0), gave values around 10(-9) cm(2)/s. (C) 2
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