Glass Transition Temperature of Poly(tert-butyl methacrylate) Langmuir−Blodgett Film and Spin-Coated Film by X-ray Reflectivity and Ellipsometry

Langmuir ◽  
2000 ◽  
Vol 16 (5) ◽  
pp. 2351-2355 ◽  
Author(s):  
Yoon-Ki See ◽  
Junhoe Cha ◽  
Taihyun Chang ◽  
Moonhor Ree
Langmuir ◽  
1999 ◽  
Vol 15 (4) ◽  
pp. 1383-1387 ◽  
Author(s):  
Junhoe Cha ◽  
Yongjun Park ◽  
Ki-Bong Lee ◽  
Taihyun Chang

2002 ◽  
Vol 56 (12) ◽  
pp. 1568-1574 ◽  
Author(s):  
Young Mee Jung ◽  
Hyeon Suk Shin ◽  
Boguslawa Czarnik-Matusewicz ◽  
Isao Noda ◽  
Seung Bin Kim

External reflection FT-IR spectra of a Langmuir–Blodgett (LB) film of poly( tert-butyl methacrylate) (PtBMA) were measured at temperatures ranging from 26 to 136 °C. The glass transition temperature ( Tg) was determined from a two-dimensional (2D) mapping of the first derivative spectra of absorbance values against temperature over the wavenumber range 1100–1300 cm−1, which contains spectral features that are very sensitive to conformational changes. This mapping provides a surprisingly simple and direct method for detecting the value of Tg. The glass transition temperature determined from the 2D map was approximately 84 °C. Another transition at 103 °C, corresponding to the glass transition temperature of bulk PtBMA, was also detected from the 2D map. Principal component analysis (PCA) was employed to analyze the temperature-dependent FT-IR spectra. The glass transition temperatures (80 °C; 100 °C) of the PtBMA LB film determined by the score plot of PCA are consistent with those determined by the 2D map. Additionally, the loading vectors of PCA were found to give valuable insight into the molecular-level phenomena associated with the glass transition process. To gain more details about the polymer chain mobility, two-dimensional (2D) correlation analysis was performed on two sets of FT-IR spectra collected above and below Tg. In the synchronous 2D correlation spectrum obtained below the glass transition temperature (26–66 °C), the observation that the strongest intensity change occurs at 1137 cm−1 indicates that the reorganization of the bending mode of the bbC–C–O and bbC–C=O bonds connected to the backbone (bb) chain and coupled to the C–O stretching mode of the tert-butoxy group is potentially the mechanism underlying the β-transition. This result is in good agreement with the presence of a transition (β-transition) at approximately 43 °C obtained from the band around at 1137 cm−1 in the 2D mapping data.


1990 ◽  
Vol 215 ◽  
Author(s):  
G. D. Paiterson ◽  
P. K. Jue ◽  
J. R. Stevens

AbstractAn optically homogeneous sample of highly syndiotactic poly(n-butyl methacrylate) (PBMA) has been prepared. The glass transition temperature was observed to be Tg=55C. Measurements of the scattered intensity of the sample followed the expected behavior for a pure liquid above Tg. The intensity rose as the sample was cooled further towards the glass transition temperature for atactic PBMA. These results illuminate the importance of regions of different stereoisomers in methacrylate polymers. Measurements of the Rayleigh- Brillouin spectrum were carried out from -15 to 130 C. The ratio of the the central peak intensity to the Brillouin intensities at temperatures above Tg was consistent with a viscoelastic liquid and had a magnitude near 3. The Brillouin linewidth remained large near Tg. and decreased continuosly with no apparent change in slope in the glass transition region. The presence and importance of rapid motions in polymers near the glass transistion is demonstrated by these results. Slowly relaxing density fluctuations near Tg. were measured by photon correlation spectroscopy. Relaxation functions were obtained from 10−6 to 10 s. Average relaxation times <τ> were obtained from the integral of the relaxation function and were found to follow the relation <τ>=Aexp(B/(T−T0)), where for our sample B=2940K and T0=273K. The observed relaxation function decayed over a wider time range as the sample was cooled. Quantitative analysis of this effect using the Williams-Watts empirical function yielded a decrease in β from 0.35 at 90 C to 0.18 at 65 C. The relaxation functions were also analyzed to give a distribution of relaxation rates. The observed distributions were bimodal at 70 and 80 C. The two features behaved in a manner consistent with the primary and secondary relaxations observed for methacrylate polymers by other techniques.


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