Poly(ethylene oxide-b-isoprene) diblock copolymer phase diagram

被引:132
作者
Floudas, G
Vazaiou, B
Schipper, F
Ulrich, R
Wiesner, U
Iatrou, H
Hadjichristidis, N
机构
[1] FORTH, Fdn Res & Technol Hellas, Inst Elect Struct & Laser, Heraklion 71110, Crete, Greece
[2] Univ Athens, Dept Chem, Athens 15771, Greece
[3] Max Planck Inst Polymerforsch, D-55021 Mainz, Germany
关键词
D O I
10.1021/ma001957p
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
The phase state of 25 poly(ethylene oxide-b-isoprene) (PEO-PI) diblock copolymers spanning the composition range 0.05 < f(PEO) < 0.8 has been studied using small-angle X-ray scattering and theology. In addition, the thermal and thermodynamic properties have been obtained from differential scanning calorimetry and pressure-volume-temperature measurements. Twenty of the diblocks exhibit at least one order-to-order transition, and two show four ordered phases. The phase diagram consists of four equilibrium phases in the melt; lamellar (Lam), hexagonally packed cylinders (Hex), spheres packed in a body centered cubic lattice (bcc) and a bicontinuous cubic phase with the Ia (3) over bard space group symmetry known as the gyroid phase. The latter is formed for the range of compositions 0.4 < f(PEO) < 0.45 which are the highest ever reported for a stable gyroid phase. The high asymmetry in the present phase diagram is attributed to the high conformational asymmetry of the PEO and PI (epsilon = 2.72). At low temperatures, upon PEO crystallization, all phases revert to the crystalline lamellar structure (L-c). Within the composition range 0.66 < f(PEO) < 0.7 another intermediate phase is formed known as perforated layers (PL) which is clearly not an equilibrium phase. The thermal expansion coefficient was found to be a sensitive probe of the ordered microstructures.
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收藏
页码:2947 / 2957
页数:11
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