Influence of molecular weight on the phase behavior and structure formation of branched side-chain hairy-rod polyfluorene in bulk phase
Creators
- 1. Department of Physics, University of Durham, South Road, Durham DH1 3LE (United Kingdom)
- 2. Department of Applied Physics, University of Twente, P.O. Box 217, 7500 AE Enschede (Netherlands)
- 3. Department of Physical Sciences, P.O. Box 64, FI-00014, University of Helsinki (Finland)
- 4. Research Institute for Solid State Physics and Optics, P.O. Box 49, Budapest-1525 (Hungary)
- 5. Makromolekulare Chemie und Institut fuer Polymertechnologie, Bergische Universitaet Wuppertal, D-42097, Wuppertal (Germany)
Description
We report on an experimental study of the self-organization and phase behavior of hairy-rod π-conjugated branched side-chain polyfluorene, poly[9,9-bis(2-ethylhexyl)-fluorene-2,7-diyl] - i.e., poly[2,7-(9,9-bis(2-ethylhexyl)fluorene] (PF2/6) - as a function of molecular weight (Mn). The results have been compared to those of phenomenological theory. Samples for which Mn=3-147 kg/mol were used. First, the stiffness of PF2/6, the assumption of the theory, has been probed by small-angle neutron scattering in solution. Thermogravimetry has been used to show that PF2/6 is thermally stable over the conditions studied. Second, the existence of nematic and hexagonal phases has been phenomenologically identified for lower and higher Mn (LMW, MnMn*) regimes, respectively, based on free-energy argument of nematic and hexagonal hairy rods and found to correspond to the experimental x-ray diffraction (XRD) results for PF2/6. By using the lattice parameters of PF2/6 as an experimental input, the nematic-hexagonal transition has been predicted in the vicinity of glassification temperature (Tg) of PF2/6. Then, by taking the orientation parts of the free energies into account the nematic-hexagonal transition has been calculated as a function of temperature and Mn and a phase diagram has been formed. Below Tg of 80 deg. C only (frozen) nematic phase is observed for MnMn*. The nematic-hexagonal transition upon heating is observed for the HMW regime depending weakly on Mn, being at 140-165 deg. C for Mn>Mn*. Third, the phase behavior and structure formation as a function of Mn have been probed using powder and fiber XRD and differential scanning calorimetry and reasonable semiquantitative agreement with theory has been found for Mn≥3 kg/mol. Fourth, structural characteristics are widely discussed. The nematic phase of LMW materials has been observed to be denser than high-temperature nematic phase of HMW compounds. The hexagonal phase has been found to be paracrystalline in the (ab0) plane but a genuine crystal meridionally. We also find that all these materials including the shortest 10-mer possess the formerly observed rigid five-helix hairy-rod molecular structure
Additional details
Identifiers
Publishing Information
- Journal Title
- Physical Review. E, Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics
- Journal Volume
- 71
- Journal Issue
- 4
- Journal Page Range
- p. 041802-041802.13
- ISSN
- 1063-651X
- CODEN
- PLEEE8
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 36083380
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- CALORIMETRY; FLEXIBILITY; FLUORENE; FREE ENERGY; HEATING; LATTICE PARAMETERS; LIQUID CRYSTALS; MOLECULAR STRUCTURE; MOLECULAR WEIGHT; NEUTRON DIFFRACTION; PHASE DIAGRAMS; PHASE TRANSFORMATIONS; POLYMERS; POWDERS; SMALL ANGLE SCATTERING; SOLUTIONS; TEMPERATURE DEPENDENCE; TEMPERATURE RANGE 0273-0400 K; THERMAL GRAVIMETRIC ANALYSIS; X-RAY DIFFRACTION
- Descriptors DEC
- AROMATICS; CHEMICAL ANALYSIS; COHERENT SCATTERING; CONDENSED AROMATICS; CRYSTALS; DIAGRAMS; DIFFRACTION; DISPERSIONS; ENERGY; FLUIDS; GRAVIMETRIC ANALYSIS; HOMOGENEOUS MIXTURES; HYDROCARBONS; INFORMATION; LIQUIDS; MECHANICAL PROPERTIES; MIXTURES; ORGANIC COMPOUNDS; PHYSICAL PROPERTIES; QUANTITATIVE CHEMICAL ANALYSIS; SCATTERING; TEMPERATURE RANGE; TENSILE PROPERTIES; THERMAL ANALYSIS; THERMODYNAMIC PROPERTIES
Optional Information
- Notes
- (c) 2005 The American Physical Society