Time-Resolved Synchrotron SAXS Observations on Sheared Syndiotactic Poly(propylene) Crystallization Process

2008 ◽  
Vol 209 (16) ◽  
pp. 1721-1729 ◽  
Author(s):  
Huiying Wen ◽  
Shichun Jiang ◽  
Yongfeng Men ◽  
Lijia An ◽  
Zhonghua Wu ◽  
...  
2002 ◽  
Vol 56 (4) ◽  
pp. 509-514 ◽  
Author(s):  
Xiaohua Yi ◽  
Karen Nerbonne ◽  
John Pellegrino

We present an experimental method for measuring diffusion of lubricants (or any highly viscous fluid) in polymers using Fourier transform infrared (FT-IR) attenuated total reflection (ATR) spectroscopy. Unlike the conventional FT-IR ATR diffusion measurement, in which a polymer sample is sandwiched between the penetrant and an internal reflection element (IRE), in this method, a thin layer of penetrant (for example, a lubricant) is sandwiched between the IRE and the polymer sample. This allows accurate control and measurement of the thickness of the lubricant layer, which, in turn, facilitates subsequent data analysis. The diffusion is studied by monitoring the time-resolved change in absorbance of either a unique polymer or penetrant band. A feature of this new method is that it can provide an estimate of solubility, as well as an estimate of the diffusivity of the penetrant in the polymer. Using this method, we studied the diffusion of mineral oil and a commercial fluorocarbon ether lubricant (Krytox® 143AC‡) in poly(propylene) (PP) film at room temperature. The experimental data was modeled using a Fickian model with impermeable and saturated boundary conditions applied at the IRE/lubricant and lubricant/polymer interfaces, respectively. The diffusivity and solubility of mineral oil in PP were found to be 1.34 ± 0.35 (×10−10) cm2/s and 0.77 ± 0.13 (×10−2) g/g of PP, respectively. The current model was unable to quantitatively describe the diffusion of the Krytox® 143AC in the PP, possibly due to excessive swelling.


2017 ◽  
Vol 62 ◽  
pp. 43-48 ◽  
Author(s):  
Qirong Kuang ◽  
Jinchuan Xu ◽  
Yongri Liang ◽  
Fengwei Xie ◽  
Feng Tian ◽  
...  

1984 ◽  
Vol 35 ◽  
Author(s):  
G.L. Olson ◽  
J.A. Roth ◽  
Y. Rytz-Froidevaux ◽  
J. Narayan

ABSTRACTThe temperature dependent competition between solid phase epitaxy and random crystallization in ion-implanted (As+, B+, F+, and BF2+) silicon films is investigated. Measurements of time-resolved reflectivity during cw laser heating show that in the As+, F+, and BF2+-implanted layers (conc 4×1020cm-3) epitaxial growth is disrupted at temperatures 1000°C. This effect is not observed in intrinsic films or in the B+-implanted layers. Correlation with results of microstructural analyses and computer simulation of the reflectivity experiment indicates that disruption of epitaxy is caused by enhancement of the random crystallization rate by arsenic and fluorine. Kinetics parameters for the enhanced crystallization process are determined; results are interpreted in terms of impurity-catalyzed nucleation during the random crystallization process.


2019 ◽  
Vol 52 (21) ◽  
pp. 8227-8237 ◽  
Author(s):  
Matthias Amann ◽  
Jakob Stensgaard Diget ◽  
Jeppe Lyngsø ◽  
Jan Skov Pedersen ◽  
Theyencheri Narayanan ◽  
...  

1996 ◽  
Vol 11 (8) ◽  
pp. 2104-2108 ◽  
Author(s):  
L. D. Carlos ◽  
M. Assunção

Time-resolved spectroscopy of poly(ethylene) oxide (PEO) and poly(propylene) oxide (PPO) electrolytes containing different concentrations of Eu3+ and Nd3+ ions is reported. A description of the main luminescence features of the Nd3+ electrolytes is also presented. Lifetimes regarding the main transitions of the luminescence spectra (5D0 → 7F1,2 and 4D3/2 → 4I11/2 for Eu3+ and Nd3+, respectively) are determined and are presented as a function of temperature in the range of 13 to 310 K. The order of magnitude of the values obtained at room temperature (0.2–0.6 ms and ≈0.7 ms for Eu3+ and Nd3+, respectively) is a further indication of the technological potential of these new polymeric materials. For the Eu3+ ion the thermally activated quenching of the 5D0 → 7F2 luminescence is discussed in terms of the observed energy superposition between the 5D0,1 levels and the ligands-to-metal charge-transfer states.


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