HIPS/UHMWPE and HIPS/XL-UHMWPE containing carbon black (CB) are unique syst
ems in which CB is attracted to the PE, and thus structuring takes place af
fecting the morphology and the resultant electrical properties. UHMWPE, hav
ing a very high viscosity, was chosen as the dispersed phase within HIPS in
place of a conventional polymer in order to explore possibilities of obtai
ning unique structures that would induce the CB to segregate and form a con
ductive network. XL-UHMWPE particles also constitute an interesting dispers
ed phase, maintaining their highly porous and intricate structure even subs
equent to melt processing. In both cases the CB is located at the interface
; however, differences in resistivity values are observed. When low UHMWPE
or XL-UHMWPE contents are incorporated, the HIPS/XL-UHMWPE/CB compositions
have lower resistivities due to the heterogeneity of the interface, even at
high shear rates. When high UHMWPE or XL-UHMWPE contents are utilized, the
trends reverse: HIPS/UHMWPE/CB depict enhanced conductivity, due to the do
minance of UHMWPE particle coalescence and the resultant decrease in surfac
e area. This is contrary to what happens with the XL-UHMWPE particles, wher
e the surface area increases with their higher contents, since they do not
coalesce.