Activation parameters were determined for the dynamics of radicals formed by muonium addition to glycylglycine (GlyGly; H 3 N + CH 2 CONHCH 2 CO - 2 ) and the doubly protected alanylalanine derivative [Boc-AlaAla-Bz; Bu t OCONHCH(Me)CONHCH(Me)CO -O -CH 2 Ph]. GlyGly forms an adduct by muonium additi
Relaxation processes and molecular motion in a new semicrystalline polyimide
β Scribed by Stephen Z. D. Cheng; Tammy M. Chalmers; Yi Gu; Yeocheol Yoon; Frank W. Harris; Jinlong Cheng; Matilda Fone; Jack L. Koenig
- Publisher
- John Wiley and Sons
- Year
- 1995
- Tongue
- English
- Weight
- 637 KB
- Volume
- 196
- Category
- Article
- ISSN
- 1022-1352
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β¦ Synopsis
A new polyimide was synthesized from 3,3',4,4'-benzophenonetetracarboxylic dianhydride (BTDA) and 2,2-dimethyl-l,3-(4-aminophenoxy)propane (DMDA), and abbreviated to be BTDA-DMDA. This polymer possesses three relaxation processes which have been observed through dynamic mechanical and dielectric analyses above -150Β°C. The a relaxation process has been assigned to be the glass transition and occurs at about 250 "C with an apparent activation energy of 420 kJ/mol. Two subglass relaxation processes are aprelaxation process at around 100-170 "C in a frequency range from 0,l Hz to 100 kHz with an activation energy of 182 kJ/mol and a y relaxation process occurs at around -80 "C with an activation energy of 44 kJ/mol. Carbon-13 solid state nuclear magnetic resonance experiments were carried out for the study of molecular dynamics at different temperatures. The results indicate that the y relaxation is responsible for an oscillation and R flipping motion of the two phenoxy rings in the DMDA portion. Theprelaxation was shown to pertain to the kHz-motion of the aromatic imide rings in the BTDA portion. The molecular motion of the DMDA and BTDA portions are largely decoupled from each other in the frequency region studied.
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