Stress crazing is studied in crystalline, isotactic polypropylene (PP) at liquid nitrogen temperatures, in smectic PP as well as in monoclinic PP having spherulites of diameter 50–100 μm. The crazes are quite different in these two cases. In smectic PP they are extremely long, often traversing the entire width (0.5 cm) of the sample, straight, perpendicular to the stress direction, and generally very similar to crazes in glassy, amorphous polymers. In monoclinic PP, crazing occurs not along the boundaries between spherulites but along spherulite diameters that are only roughly perpendicular to the stress direction. In general, the length of a craze equals the spherulite diameter, although there is a tendency for crazes to run from one spherulite center to the next. A dramatic effect of gaseous environment on mechanical properties and the extent of crazing is observed. Gases near their condensation temperatures act as crazing agents in the sense that they reduce the stress required to promote crazing up to twofold as compared to the crazing stress in vacuum; also they increase the plastic strain due to crazing about tenfold in smectic, and somewhat less in monoclinic PP. The action of the gas is due to two mechanisms. First, the adsorbed gas reduces the surface energy of the polymer and so eases the creation of new surface in the holes and voids of the craze. Second, the gas becomes highly absorbed at the tip of an incidental flaw or of an existing craze, since these are regions of high dilatant stress; hence the gas acts as a plasticizer easing the flow involved in the nucleation and growth of the craze.
Read full abstract