The ionic conductivity and glass transition temperatures
of nanostructured
block copolymer electrolytes composed of polystyrene-b-poly(ethylene oxide) (SEO) doped with lithium bis(trifluoromethanesulfone)imide
(LiTFSI) were studied in the small molecular weight limit (between
2.7 and 13.7 kg mol–1). In this range, the annealed
conductivity exhibits a nonmonotonic dependence on molecular weight,
decreasing with increasing molecular weight in the small molecular
weight limit before increasing when molecular weight exceeds about
10 kg mol–1. We show that annealed electrolyte conductivity
is affected by two competing factors: the glass transition temperature
of the insulating polystyrene (PS) block and the width of the conducting
poly(ethylene oxide) (PEO) channel. In the low molecular weight limit,
all ions are in contact with both PS and PEO segments. The intermixing
between PS and PEO segments is restricted to an interfacial zone of
width, λ. Our experiments suggest that λ is about 5 nm.
The fraction of ions affected by the interfacial zone decreases as
the conducting channel width increases. We also study the effect of
thermal history on the conductivity of the block copolymer electrolytes.
Our data suggest that long-range order impedes ion transport.
PolyHIPEs are porous polymers synthesized within high internal phase emulsions (HIPEs). Recent research has shown that the locus of conventional free radical initiation (at the oil–water interface or in the organic phase) can affect the polyHIPE’s structure and properties. This paper is the first investigation of polyHIPE synthesis using activators generated by electron transfer for atom-transfer radical polymerization (AGET ATRP). Two different types of initiators (organic-phase-based and nanoparticle-based) were used to synthesize polyHIPEs within both surfactant-stabilized HIPEs and nanoparticle-stabilized Pickering HIPEs. The type and locus of initiation affected the macromolecular structure for all the polyHIPEs. Furthermore, the initiator also affected both the porous structure and the wall structure of polyHIPEs synthesized within Pickering HIPEs. Depending upon the initiator, either a polyhedral void shape or a nanoparticle assembly at the interface could become “locked in” at the very beginning of the polymerization.
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