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Thus, the ultimate capability for plastic deformation of the IA compatibilized blends is much larger than the overall elongation at break.
It was found that (i) Tg of crystallized blends is much lower than Tg of quenched blends, (ii) the semi-crystalline blends can only be described with a three-phase model.
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However, the model predictions for PS/PMMA (20/80, 30/70) blends are much higher than experimental results.
The particle dimension and its distribution of PA12 dispersed phase in these blends are much lower and narrower than that of the PP/PA12 blends.
The absolute viscosity and the intrinsic viscosity of solutions of blends are much higher than the weight average values of solutions of CDA and PVP.
DSC results show that the Tgs of the P4VP/PVPh blends are much higher than those of the calculated weight-average values.
PC with Mw = 30,000 g/mol formed miscible blends with PET only when PET had molecular weight <2800 g/mol, indicating PC/PET blends were much less miscible than RPC20/PET blends.
The PC/ABS blend was much less sensitive to notch tip radius and the Tbd was almost constant.
Under weak shear flow, the domain morphology of the OMMT filled blend was much thinner than that of the SiO2 filled blend.
Under strong shear flow, the string-like phase interface of the OMMT filled blend was much blurred compared with that of the SiO2 filled blend.
The mesophase content and degree of orientation of iPP matrix in iPP/OBC blend were much lower than that in neat iPP within the investigated strain range.
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