Poly(9-undecyl-9-methyl-fluorene) and poly(9-pentadecyl-9-methyl-fluorene): Synthesis, solution structure, and effect of side chain asymmetry on aggregation behavior

Research output: Contribution to journalJournal article – Annual report year: 2019Researchpeer-review

DOI

  • Author: Knaapila, Matti

    Neutrons and X-rays for Materials Physics, Department of Physics, Technical University of Denmark, Fysikvej, 2800, Kgs. Lyngby, Denmark

  • Author: Stewart, Beverly

    University of Bradford, United Kingdom

  • Author: Garamus, Vasil M.

    Helmholtz-Zentrum Geesthacht - Centre for Materials and Coastal Research, Germany

  • Author: Ramos, M. Luísa

    Universidade de Coimbra, Portugal

  • Author: Cruz, Pedro F.

    Universidade de Coimbra, Portugal

  • Author: Brito, Rui M. M.

    Universidade de Coimbra, Portugal

  • Author: Justino, Licinia L. G.

    Universidade de Coimbra, Portugal

  • Author: Fausto, Rui

    Universidade de Coimbra, Portugal

  • Author: Napierala, Connor

    Technical University of Denmark, Denmark

  • Author: Forster, Michael

    Bergische Universität Wuppertal, Germany

  • Author: Burrows, Hugh D.

    University of Bradford, United Kingdom

  • Author: Scherf, Ullrich

    Bergische Universität Wuppertal, Germany

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We report on solution aggregates and backbone conformation of poly(9-undecyl-9-methyl-fluorene) (PF1-11) and poly(9-pentadecyl-9-methyl-fluorene) (PF1-15), having two different side chains compared with poly(9,9-dihexylfluorene) (PF6) and poly(9,9-dioctylfluorene) (PF8) with two identical side chains. In the poor solvent methylcyclohexane (MCH), X-ray scattering indicates that PF1-11 and PF1-15 appear as three-dimensional aggregates (5-10 nm wide and thick), forming ribbon-like agglomerates (correlation lengths of 100 nm). PF6 and PF8 appear as two-dimensional aggregates (>10 nm wide and 2-3 nm thick) involving ribbon-like agglomerates (correlation lengths much greater than 100?nm). Upon heating, all aggregates undergo a gel-sol transition which occurs at lower temperatures for PF1-11 and PF1-15 (80°C). In the good solvent toluene, PF1-11 and PF1-15 form networks of cylindrical particles. The mesh size and the cylinder radius are smaller in 24°C toluene (60 nm, 0.5 nm) than in 60°C MCH (300 nm, 1-2 nm). Nuclear magnetic resonance spectra in toluene-d8 together with density functional theory calculations suggest higher torsion angles between polymer repeat units for PF6, PF8, and PF1-11 (less planar conformation) and a gauche arrangement of the dihedral angles between the bridge carbon atom and the side chain methylene groups in PF1-15.
Original languageEnglish
JournalJournal of Polymer Science. Part B, Polymer Physics
Volume57
Issue number13
Pages (from-to)826-837
Number of pages12
ISSN0887-6266
DOIs
Publication statusPublished - 2019
CitationsWeb of Science® Times Cited: No match on DOI

    Research areas

  • Conjugated polymers, NMR, Polyfluorene, X-ray

ID: 184725600