Orthogonal Crystal Orientation in Double-Crystalline Block Copolymer

In this study, we explore the orientation of crystals formed within the lamellar domains of a diblock copolymer composed of two crystallizable blocks, that is, poly(l-lactide)-block-polyethylene (PLLA-b-PE). The orientation of both PLLA and PE crystals with respect to the lamellar interface was exam...

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Veröffentlicht in:Macromolecules 2011-09, Vol.44 (17), p.6875-6884
Hauptverfasser: Lin, Ming-Champ, Wang, Yi-Chin, Chen, Jean-Hong, Chen, Hsin-Lung, Müller, Alejandro J, Su, Chun-Jen, Jeng, U-Ser
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Sprache:eng
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Zusammenfassung:In this study, we explore the orientation of crystals formed within the lamellar domains of a diblock copolymer composed of two crystallizable blocks, that is, poly(l-lactide)-block-polyethylene (PLLA-b-PE). The orientation of both PLLA and PE crystals with respect to the lamellar interface was examined under two types of crystallization condition with a broad range of crystallization temperatures (T c). The first type was the “two-stage crystallization”, where the PLLA block was allowed to crystallize before PE. The second was the “one-stage crystallization”, where PLLA and PE blocks competed to crystallize. A homeotropic crystal orientation was always observed for the PLLA crystals, with the crystalline stems lying parallel to the lamellar normal regardless of the crystallization condition, except when T c approached the glass-transition temperature of PLLA, where the orientation became random. A homogeneous crystal orientation with the PE crystalline stems oriented perpendicular to the lamellar normal was always identified at low-to-intermediate degree of undercooling, whereas at large undercooling, the crystals showed random orientation. The “orthogonal orientation” disclosed here was preserved over a broad range of undercooling. Our results further demonstrated that the orientation of both PLLA and PE crystals depended mainly on T c but was independent of the competitiveness of the two crystallization processes. This was a consequence of the strong segregation that made the two blocks crystallize independently within their respective microdomains.
ISSN:0024-9297
1520-5835
DOI:10.1021/ma201124u