Microdeformation in partially compatible blends of poly(styrene-acrylonitrile) and polycarbonate |
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Authors: | Larry L. Berger Edward J. Kramer |
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Affiliation: | (1) Department of Materials Science and Engineering and the Materials Science Center, Cornell University, 14853 Ithaca, New York, USA |
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Abstract: | Dilute 3-component 1-phase solutions in methylene chloride of poly(styrene-acrylonitrile) PSAN and polycarbonate PC are used to cast phase separated thin films. Films of pure PSAN, pure PC and five intermediate compositions are examined. The films are bonded to copper grids and strained at a constant rate of 4.1 × 10–6sec–1. The median tensile strainv for void formation is determined using an optical microscope and the regions surrounding the voids are examined by TEM. At room temperature and slow strain rates both PSAN and PC plastically deform by shear yielding. For pure PSANv was found to be 0.13 whereas for PCv exceeds 0.23. The addition of the more ductile polymer PC to PSAN at weight fractionsx forx 0.4 decreasesv. In this case voids form in crazes at the boundaries between the PC-rich inclusion and the PSAN-rich matrix. When the PC content is increased tox = 0.8,v approaches 0.23. The effect of physical ageing (annealing belowTg the glass transition temperature) on the mode of plastic deformation was also examined over the same compositional range. Physical ageing was found to suppress shear deformation and favour crazing in PSAN and PSAN-rich phases. Because crazes are more susceptible to breakdown than DZ's (shear deformation zones), physical ageing results in a marked decrease inv. The breakdown statistics of these phase separated partially compatible blends was found to follow a Weibull distribution in strain from which two parameters may be extracted: the Weibull modulus andw the Weibull scale parameter. is a measure of the breadth of distribution of void initiation andw is a measure of the median strain to void formation in the films. The behaviour ofw was found to approximately mirrorv. The Weibull modulus appears to be primarily controlled by the matrix phase. |
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