thermal nucleation
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2016 ◽  
Vol 30 (4) ◽  
pp. 2655-2661 ◽  
Author(s):  
Matthew T. Sullivan ◽  
Dan E. Angelescu

2014 ◽  
Vol 971-973 ◽  
pp. 103-106
Author(s):  
Xiao Hua Gu ◽  
Peng Zeng ◽  
Xi Wei Zhang ◽  
Xue Song

Abstract.In this paper, the nonisothermal crystallization kinetics was investigated by differential scanning calorimetry for the poly(m-xylylene adipamide) (MXD6) which were prepared by polymerization in reactor. The Avrami theory modified by Jeziorny and Z.S. Mo equation were used to describe the nonisothermal crystallization kinetics. The analysis based on the Avrami theory modified by Jeziorny shows that the Avrami exponent n of MXD6 ranges from 2.3 to 3.3, Moreover, both Avrami exponent (n) were around 3.0, which probably suggests a thermal nucleation and a three-dimensional crystal growth. The good linearity of the plots indicates the successful application of Z.S. Mo method in this case.


2014 ◽  
Vol 89 (3) ◽  
Author(s):  
Trung Dac Nguyen ◽  
Miguel Fuentes-Cabrera ◽  
Jason D. Fowlkes ◽  
Philip D. Rack

2012 ◽  
Vol 535-537 ◽  
pp. 1413-1416
Author(s):  
Tien Wei Shyr ◽  
Chia Hsin Tung ◽  
Yan Ting Liu

Poly(trimethylene terephthalate-co-isophthalate) (TI) copolyesters were synthesized using different ratios of isophthalic acid (IPA) and Terephthalic acid (TPA) with 1,3-propanediol (1,3-PDO). The compositions of TI copolyesters were analyzed using 1H nuclear magnetic resonance (NMR). Non-isothermal melt- and cold-crystallization and subsequent melting behaviors were investigated using differential scanning calorimetry (DSC). For TI0, TI10, and TI20, non-isothermal crystallization kinetics were analyzed using a modified Avrami equation. The results show that the reaction rate of TPA with 1,3-PDO was similar with that of IPA with 1,3-PDO in TI copolyesters. Crystallization exothermic peak and melting endothermic peak were not observed in DSC traces with an increase of the relative amount of PIP to 41%. The Avrami exponent n is in the range of 3.5-4.2 for melt-crystallized TI copolyesters and between 3.0-3.2 for cold-crystallized copolyesters. It suggests that the crystallization from melt state corresponds to thermal nucleation but the crystallization from glassy state originates from predeterminated nuclei.


2011 ◽  
Author(s):  
Bruno Werneck Mintz ◽  
Giuseppe Pagliara ◽  
Eduardo Souza Fraga ◽  
Juergen Schaffner-Bielich

2010 ◽  
Vol 37 (9) ◽  
pp. 094066 ◽  
Author(s):  
B W Mintz ◽  
E S Fraga ◽  
J Schaffner-Bielich ◽  
G Pagliara

e-Polymers ◽  
2007 ◽  
Vol 7 (1) ◽  
Author(s):  
Bo Yan ◽  
Yanmo Chen ◽  
Meifang Zhu ◽  
Ting Liu

AbstractThe non-isothermal crystallization behaviour of poly(phenylene sulfide) (PPS) in blends with hyperbranched poly(phenylene sulfide) (HPPS) was studied by means of differential scanning calorimetry (DSC). It was observed that the PPS crystallization temperature was found to decrease upon addition of the HPPS. It suggested that the crystallizability was reduced. The Ozawa equation was valid not only for neat PPS, but also for the blends. A notable reduction in Avrami exponents for the PPS/HPPS blend systems suggested that the nucleated process leads to rodshaped growth with thermal nucleation. The cooling crystallization function, which represents the rate of non-isothermal crystallization, was found to decrease with increase in HPPS content. The Ea value increases with the increase in HPPS content. Our results indicated that crystallization of the PPS was hampered by content of hyperbranched poly(phenylene sulfide).


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