4.7 Article

Glass Transition Dynamics and Fragility of Ultrathin Miscible Polymer Blend Films

Journal

MACROMOLECULES
Volume 48, Issue 18, Pages 6682-6689

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acs.macromol.5b00979

Keywords

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Funding

  1. University of Pennsylvania
  2. MRSEC program of the National Science Foundation at the University of Pennsylvania [DMR-11-20901]
  3. National Science Foundation's Division of materials research, Polymers Programs [DMR-09-07493, PYI-DMR-91-58462]
  4. Direct For Mathematical & Physical Scien
  5. Division Of Materials Research [0907493, 1507713] Funding Source: National Science Foundation

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We use cooling-rate-dependent T-g measurements (CR-T-g) to indirectly probe the relaxation dynamics and fragility of thin films Of polystyrene (PS)/poly(2,6-dimethyl-1,4-phenylene oxide) (PPO) blends. Thin films of this miscible blend have a single glass transition temperature (T-g) that can be systematically shifted over 100 K simply by varying the composition of the blend. This study shows that the T-g of these blends decreases below the bulk T-g as the film thickness is decreased. Additionally, the degree of change in T-g strongly depends on the cooling rate of the experiment. We show that the T-g of 16 rim films of a 50% PS blend is 15 K lower than that of bulk at a cooling rate of 1 K/min but decreases only 4 K at a cooling rate of 120 K/min. By analyzing the cooling rate dependence of the T-g for various thicknesses of the 50% PS blend, we demonstrate that the fragility of these blends decreases with film thickness. This behavior is similar to what is observed in ultrathin films of polystyrene, which suggests that the deviations from bulk dynamics in PS/PPO blends are due to enhanced mobility near the free surface. Similar to pure PS, if extrapolated to higher temperatures, the dynamics of thin films intersect the bulk dynamics at a temperature a few degrees above bulk T-g. The presence of this temperature (T*) can help explain why some experiments fail to see T-g depression in thin films of these blends. Lastly, we show that while the fragility of the bulk blend changes due to differences in the fragility of the homopolymers, ultrathin films (h = 16 nm) have identical average dynamics and fragilities regardless of the blend composition at the same temperature relative to T-g. This result implies that enhanced mobility near the free surface affects the dynamics of these blend thin films similarly.

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