Understanding the ionic activity and conductivity value differences between random copolymer electrolytes and block copolymer electrolytes of the same chemistry

  • Mario V. Ramos-Garcés
  • , Ke Li
  • , Qi Lei
  • , Deepra Bhattacharya
  • , Subarna Kole
  • , Qingteng Zhang
  • , Joseph Strzalka
  • , Polyxeni P. Angelopoulou
  • , Georgios Sakellariou
  • , Revati Kumar
  • , Christopher G. Arges

Research output: Contribution to journalArticlepeer-review

12 Scopus citations

Abstract

Herein, a systematic study where the macromolecular architectures of poly(styrene-block-2-vinyl pyridine) block copolymer electrolytes (BCE) are varied and their activity coefficients and ionic conductivities are compared and rationalized versus a random copolymer electrolyte (RCE) of the same repeat unit chemistry. By performing quartz crystal microbalance, ion-sorption, and ionic conductivity measurements of the thin film copolymer electrolytes, it is found that the RCE has higher ionic activity coefficients. This observation is ascribed to the fact that the ionic groups in the RCE are more spaced out, reducing the overall chain charge density. However, the ionic conductivity of the BCE is 50% higher and 17% higher after the conductivity is normalized by their ion exchange capacity values on a volumetric basis. This is attributed to the presence of percolated pathways in the BCE. To complement the experimental findings, molecular dynamics (MD) simulations showed that the BCE has larger water cluster sizes, rotational dynamics, and diffusion coefficients, which are contributing factors to the higher ionic conductivity of the BCE variant. The findings herein motivate the design of new polymer electrolyte chemistries that exploit the advantages of both RCEs and BCEs.

Original languageEnglish
Pages (from-to)15078-15084
Number of pages7
JournalRSC Advances
Volume11
Issue number25
DOIs
StatePublished - Apr 22 2021
Externally publishedYes

Funding

This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences Separation Science program under Award Number DESC0018989. This research used resources of the Advanced Photon Source, a U.S. Department of Energy (DOE) Office of Science User Facility operated for the DOE Office of Science by Argonne National Laboratory under Contract No. DE-AC02-06CH11357 (Beamline 8-ID-E for GI-SAXS experiments). LSU Shared Instrumentation and Nanofabrication Facilities were used for this work. R. K. and K. L. are grateful for computer time on the LSU-High Performance Computing (LSU-HPC) clusters as well as the clusters of the Louisiana Optical Network Initiative (LONI).

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