Network phases in ABC triblock copolymers
Network phases in ABC triblock copolymers
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DOI:
10.1021/ma0493426
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发表时间:
2004-09-21
期刊:
影响因子:
5.5
通讯作者:
Bates, FS
中科院分区:
文献类型:
--
作者:
Epps, TH;Cochran, EW;Bates, FS
Many naturally occurring and engineered products are influenced by network structures. Collagen networks provide a scaffold for living tissue, while swollen arrays of physically cross-linked polypeptides constitute gelatin, the familiar dessert and electrophoresis medium. Although the associated mesh sizes differ by several orders of magnitude, these examples share a common feature: three-dimensional connectivity that imparts mechanical rigidity. Intercalating additional interconnected components can yield broader functions, eg, ionic or electrical conductivity, optical band gaps, and tailored heat and mass transfer. 1-3 At mesoscopic length scales (between roughly one nanometer and one micron) interfacial curvature and packing geometry often reflect self-assembly of molecules endowed with prescribed architectures and directed interactions. 4 Under the appropriate conditions, hydrated soaps, lipids, and surfactants form soft, permeable, bicontinuous solids, 5-7 some capable of templating hard mesoporous ceramic networks. 8, 9 Block copolymers provide even greater flexibility in manipulating the precise placement of engineering materials in a plethora of nanoscale configurations. 10, 11 However, aside from linear permutations of two block types (AB, ABA, ABAB, etc.) there is currently no reliable way to anticipate block copolymer morphologies from theory. This communication summarizes a comprehensive investigation of a homologous set of linear poly (isoprene-b-styrene-b-ethylene oxide)(ISO) triblock copolymers. We have synthesized and characterized more than eighty ISO triblock copolymers over the past 4 years, covering a wide range of compositions. Here we focus on a total of 43 model compounds (Mw/Mn< 1.08) with molecular weights 15< Mw< 25 kg/mol and compositions bounded by 0.20 e fI e 0.58, 0.25 e fS e 0.58, and 0 e fO e 0.37, where fi is the volume fraction of block i, calculated from the experimentally determined weight fractions and published homopolymer densities at 140 C: FI) 0.830, FS) 0.969, and FO) 1.064 g/mol. 12 The associated phases are identified in the triangular phase portrait illustrated in Figure 1. The experiments described here were conducted above 100 C, which exceeds the melting (Tm, O= 65 C) and glass transition (Tg, S= 90 C) temperatures. Most of the block copolymers exhibited an order-disorder transition temperature (TODT) above 100 C, and generally below 250 C. Ordered phases have been identified using a complement of four techniques: small-angle X-ray scattering (SAXS) performed at the Advanced Photon Source (APS, Argonne National Laboratory) or the University of Minnesota, transmission electron microscopy (TEM), light depolarization (birefringence), and dynamic mechanical spectroscopy (DMS). Previous experiments with a subset of the ISO polymers, located on the isopleth defined by fI) fS, indicated that a triply continuous network phase (tentatively associated with Fddd space group symmetry) separated the two-domain (I and S) and three-domain (I, S, and O) lamellar states. 13 A representative SAXS powder pattern, obtained from a specimen located in the composition window labeled O70 (see Figure 1), is