Abstract:The growth rate of isotactic polypropylene is deduced from microscopic observations during isothermal crystallizations. A change in the growth regime is observed at 138 ~ and interpreted as a Regime III --* Regime II transition, according to Hoffman's kinetic theory of polymer crystallization. A Regime II ~ Regime I transition is also theoretically predicted at 155 ~ i. e. at a temperature outside the investigated temperature range. The Regime III --, Regime II transition is related to the positive to negative change in the spherulite birefringence, which is generally attributed to a change in the organization of crystalline lamellae: quadritic arrays of intercrossing lamellae at Tc < 138 ~ (Regime III) and preferentially radiating lameUae at Tc > 138 ~ (Regime II). It is suggested that such a morphological change could be interpreted using the concept of "nonadjacent re-entry" introduced in Hoffman's kinetic theory. This interpretation could also explain the interspherulitic ruptures observed in negative spherulites.

International audienceThe crystallization kinetics of polypropylene was observed during shear and after shear experiments under isothermal condition. The crystallizations were performed in a plate-plate and a fiber pull-out device. The nucleation density, the crystalline growth and the overall kinetics were measured and compared with data obtained in a similar way but during static experiments. The morphologies are spherulitic and formed from nuclei which seem to be randomly distributed, α-phase spherulites are always observed but with a nucleation density and a growth rate which depend on shearrate. The nucleation density is strongly enhanced by shear and acts as the main factor on the overall kinetics. The overall kinetics can be analyzed with a two-step Avrami model, where an Avrami exponent n1 with a very high value is always observed first after shear and a more usual parameter n2 for the subsequent crystallization period. This high value of n1 seems to be related to the strong enhancement of nucleation density. The growth rate increases with the shear-rate, but the basic growth mechanisms do not seem to be modified. For crystallizations after shear the growth rate decreases with a long-time delay after shear but not down to the static value. The effect is characteristic of a partial relaxation of chain orientation after shear but with a very unusual time constant