期刊
JOURNAL OF CHEMICAL THERMODYNAMICS
卷 36, 期 9, 页码 731-742出版社
ACADEMIC PRESS LTD- ELSEVIER SCIENCE LTD
DOI: 10.1016/j.jct.2004.05.003
关键词
heat capacity; poly(lactic acid); heats of fusion; glass transition; melting; crystallinity; rigid-amorphous fraction
The heat capacity of poly(lactic acid) (PLA) is reported from T = (5 to 600) K as obtained by differential scanning calorimetry (d.s.c.) and adiabatic calorimetry. The heat capacity of solid PLA is linked to its group vibrational spectrum and the skeletal vibrations, the latter being described by a Tarasov equation with Theta(1) = 574 K, Theta(2) = Theta(3) = 52 K, and nine skeletal vibrations. The calculated and experimental heat capacities agree to +/- 3% between T= (5 and 300) K. The experimental heat capacity of liquid PLA can be expressed by C, (liquid) = (120.17 + 0.076T) J (.) K-1 (.) mol(-1) and has been compared to the ATHAS Data Bank, using contributions of other polymers with the same constituent groups. The glass transition temperature of amorphous PLA occurs at T = 332.5 K with a change in heat capacity of 43.8 J (.) K-1 (.) mol(-1). Depending on thermal history, semi-crystalline PLA has a melting endotherm between T= (418 and 432) K with variable heats of fusion. For 100% crystalline PLA, the heat of fusion is estimated to be (6.55 +/- 0.02) kJ (.) mol(-1) at T = 480 K. With these results, the enthalpy, entropy, and Gibbs function of crystalline and amorphous PLA were obtained. For semi-crystalline samples, one can check changes of crystallinity with temperature and judge the presence of rigid-amorphous fractions. (C) 2004 Elsevier Ltd. All rights reserved.
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