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Published on: June 20, 2019
The C36 Laves phase in diblock polymer melts.
Benjamin R Magruder1, Kevin D Dorfman1
1Department of Chemical Engineering and Materials Science, University of Minnesota, 421 Washington Ave SE, Minneapolis, MN 55455, USA. dorfman@umn.edu.
The C36 Laves phase is not observed in diblock polymers due to its free energy being an average of the C14 and C15 phases. Flexible diblock polymers favor C14 and C15 phases over C36.
Area of Science:
- Materials Science
- Polymer Physics
- Soft Matter Physics
Background:
- Laves phases (C14, C15) are common micelle packing structures in soft matter.
- The related C36 Laves phase, with alternating C14/C15 layers, has not been observed in diblock polymer systems.
Purpose of the Study:
- Investigate the absence of the C36 Laves phase in diblock polymers.
- Relate C36 morphology and energetics to other known mesophases using self-consistent field theory.
Main Methods:
- Self-consistent field theory simulations.
- Analysis of morphology and free energy in diblock polymer systems.
- Case studies: AB diblock/A homopolymer blends and neat AB diblock melts.
Main Results:
- C36 free energy is a near-perfect bisector of C14 and C15 free energies across all studied systems.
- This energetic symmetry arises from the intermediate packing structure of C36.
- C14 and C15 phases exhibit nearly identical micelle morphologies and degenerate free energies.
Conclusions:
- The intrinsic free energy symmetry explains the absence of C36 in flexible diblock polymers.
- C14 and C15 phases are thermodynamically favored over C36 due to facile mass transfer.
- C36 is not expected to form in flexible diblock polymer systems.
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