Stretching of material elements in time-periodic cavity flows is inves
tigated numerically. The spatial structure of the stretching field is
determined not only by nonchaotic islands and by unstable manifolds of
hyperbolic periodic points, but also by singularities of the flow fie
ld at the cavity corners. For the short time scales interesting to mos
t mixing applications, regions of very high stretching (good local mix
ing) are determined by unstable manifolds that pass close to the corne
rs of the cavity. Low stretching (poor local mixing) regions are usual
ly found both inside and near islands. In some cases, however, the uns
table manifolds wrap themselves around the islands, preventing the for
mation of segregated low stretching subregions within the chaotic regi
on.