TY - JOUR
T1 - Conflicting Confinement Effects on the Tg, Diffusivity, and Effective Viscosity of Polymer Films
T2 - A Case Study with Poly(isobutyl methacrylate) on Silica and Possible Resolution
AU - Geng, Kun
AU - Katsumata, Reika
AU - Yu, Xuanji
AU - Ha, Heonjoo
AU - Dulaney, Austin R.
AU - Ellison, Christopher J.
AU - Tsui, Ophelia K.C.
N1 - Funding Information:
This work is funded by the National Science Foundation through the grant award DMR-1310536 and CAREER award DMR-1053293. R.K. appreciates the Takenaka Scholarship and Graduate Dean’s Prestigious Fellowship Supplement for financial support.
Publisher Copyright:
© 2017 American Chemical Society.
PY - 2017/1/24
Y1 - 2017/1/24
N2 - The glass transition temperature (Tg), in-plane diffusivity (D), and effective viscosity (ηeff) were measured for the same thin film system of poly(isobutyl methacrylate) supported by silica (PiBMA/SiOx). We found that both the Tg and D were independent of the film thickness (h0), but ηeff decreased with decreasing h0. We envisage the different h0 dependencies to be caused by Tg, D, and ηeff being different functions of the local Tg’s (Tg,i) or viscosities (ηi), which vary with the film depth. By assuming a three-layer model and that Tg(h0) = ⟨Tg,i⟩, D(h0) ∼ kBT/⟨ηi⟩, and ηeff(h0) = h03/3Mtot(ηi), where ⟨...⟩ denotes spatial averaging and Mtot is the mobility of the films, we were able to account for the experimental data. By extending these ideas to the analogous data of polystyrene supported by silica (PS/SiOx), a resolution was found for the long-standing inconsistency regarding the effects of confinement on the dynamics of polymer films.
AB - The glass transition temperature (Tg), in-plane diffusivity (D), and effective viscosity (ηeff) were measured for the same thin film system of poly(isobutyl methacrylate) supported by silica (PiBMA/SiOx). We found that both the Tg and D were independent of the film thickness (h0), but ηeff decreased with decreasing h0. We envisage the different h0 dependencies to be caused by Tg, D, and ηeff being different functions of the local Tg’s (Tg,i) or viscosities (ηi), which vary with the film depth. By assuming a three-layer model and that Tg(h0) = ⟨Tg,i⟩, D(h0) ∼ kBT/⟨ηi⟩, and ηeff(h0) = h03/3Mtot(ηi), where ⟨...⟩ denotes spatial averaging and Mtot is the mobility of the films, we were able to account for the experimental data. By extending these ideas to the analogous data of polystyrene supported by silica (PS/SiOx), a resolution was found for the long-standing inconsistency regarding the effects of confinement on the dynamics of polymer films.
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U2 - 10.1021/acs.macromol.6b01354
DO - 10.1021/acs.macromol.6b01354
M3 - Article
AN - SCOPUS:85018193029
SN - 0024-9297
VL - 50
SP - 609
EP - 617
JO - Macromolecules
JF - Macromolecules
IS - 2
ER -