Strain state of poly(N‐isopropylacrylamide) in polystyrene‐b‐poly(N‐isopropylacrylamide) block copolymers and binary blends with polystyrene

M Rosales‐Guzmán, R Alexander‐Katz… - Journal of Polymer …, 2013 - Wiley Online Library
M Rosales‐Guzmán, R Alexander‐Katz, P Castillo‐Ocampo, A Vega‐Ríos, A Licea‐Claveríe
Journal of Polymer Science Part B: Polymer Physics, 2013Wiley Online Library
Three diblock copolymers of polystyrene‐b‐poly (N‐isopropylacrylamide)(PS‐b‐PNIPAM)
were prepared by reversible addition‐fragmentation chain transfer technique (RAFT) with
compositions fPS= 0.84, fPS= 0.29, and fPS= 0.33. Block copolymers rich in PNIPAM were
blended with polystyrene and its morphological effects were studied. The morphology of thin
films was induced by acetone vapor and determined in the dried state by means of TEM.
Copolymers with fPS= 0.84 and fPS= 0.29 form hexagonally packed cylinder (HPC) …
Abstract
Three diblock copolymers of polystyrene‐b‐poly(N‐isopropylacrylamide) (PS‐b‐PNIPAM) were prepared by reversible addition‐fragmentation chain transfer technique (RAFT) with compositions fPS = 0.84, fPS = 0.29, and fPS = 0.33. Block copolymers rich in PNIPAM were blended with polystyrene and its morphological effects were studied. The morphology of thin films was induced by acetone vapor and determined in the dried state by means of TEM. Copolymers with fPS = 0.84 and fPS = 0.29 form hexagonally packed cylinder (HPC) morphologies while that with fPS = 0.33 corresponds to a lamellar structure. In almost all cases where PNIPAM constitutes the continuous phase, a contraction of the PNIPAM blocks with respect to their average unperturbed dimension was observed, contrary to what one expects from the physics of self‐assembly of block copolymers. In contrast, for HPC morphology where PNIPAM is confined in a PS matrix, both blocks are highly extended. © 2013 Wiley Periodicals, Inc. J. Polym. Sci., Part B: Polym. Phys. 2013, 51, 1368–1376
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