AbstractA relationship has been found for OSA (olefin‐acrylonitrile‐styrene) polymers between normalized Izod impact strength (ΔI/N) or yield stress (Δσy/N) with mean particle radius. These normalized functions (which analytically include radius and rubbery phase volume) are representative of the toughening effect of a single particle with respect to the styrene‐acrylonitrile (SAN) rigid matrix. ΔI/Nand Δσy/Nincrease exponentially as a function of the radius. This approach, for Izod, was also applied to HIPS and toughened nylon reported in the literature and similar results were obtained. In the case of nylon, however, the ΔI/Nvalues are split in two different curves related to the tough‐brittle transition described in that literature. Referring to OSA, three samples (with the largest radii more than 0.22 μm) fail in a brittle manner and do not fit the curve of ΔI/N: they fit, however, that of Δσy/N. Further work must be done in order to investigate a decisive role either of interfacial adhesion (eventual lack for these three materials) or of tough‐brittle transition mentioned before for shear‐yielding deforming materials. In fact, OSA has behavior intermediate between that of nylon and HIPS wh
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