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Polycation radius of gyration in a polymeric ionic liquid (PIL): the PIL melt is not a theta solvent†
Lucas N. Wong,Seamus D. Jones,Kathleen Wood,Liliana de Campo,Tamim Darwish,Michael Moir,Hua Li,Rachel A. Segalman,Gregory G. Warr,Rob Atkin
Physical Chemistry Chemical Physics Pub Date : 01/25/2022 00:00:00 , DOI:10.1039/D1CP05354J
Abstract

The conformation of the polycation in the prototypical polymeric ionic liquid (PIL) poly(3-methyl-1-aminopropylimidazolylacrylamide) bis(trifluoromethylsulfonyl)imide (poly(3MAPIm)TFSI) was probed using small-angle neutron scattering (SANS) and ultra-small-angle neutron scattering (USANS) at 25 °C and 80 °C. Poly(3MAPIm)TFSI contains microvoids which lead to intense low q scattering that can be mitigated using mixtures of hydrogen- and deuterium-rich materials, allowing determination of the polycation conformation and radius of gyration (Rg). In the pure PIL, the polycation adopts a random coil conformation with Rg = 52 ± 0.5 Å. In contrast to conventional polymer melts, the pure PIL is not a theta solvent for the polycation. The TFSI anions, which comprise 48% v/v of the PIL, are strongly attracted to the polycation and act like small solvent molecules which leads to chain swelling analogous to an entangled, semi-dilute, or concentrated polymer solution in a good solvent.

Graphical abstract: Polycation radius of gyration in a polymeric ionic liquid (PIL): the PIL melt is not a theta solvent
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