STRUCTURE AND MOLECULAR-CONFORMATION OF TUSSAH SILK FIBROIN FILMS TREATED WITH WATER-METHANOL SOLUTIONS - DYNAMIC-MECHANICAL AND THERMOMECHANICAL BEHAVIOR
M. Tsukada et al., STRUCTURE AND MOLECULAR-CONFORMATION OF TUSSAH SILK FIBROIN FILMS TREATED WITH WATER-METHANOL SOLUTIONS - DYNAMIC-MECHANICAL AND THERMOMECHANICAL BEHAVIOR, Journal of polymer science. Part B, Polymer physics, 36(15), 1998, pp. 2717-2724
The thermal response of tussah (Antheraea pernyi) silk fibroin films t
reated with different water-methanol solutions at 20 degrees C was stu
died by means of dynamic mechanical (DMA) and thermomechanical (TMA) a
nalyses as a function of methanol concentration and treatment time. Th
e DNLA. curves of alpha-helix films (treated with greater than or equa
l to 80% v/v methanol for 2 min and 100% methanol for 30 min) showed t
he sharp fall of storage modulus at about 190 degrees C, and the loss
peak in the range 207-213 degrees C. The TMA curves were characterized
by a thermal shrinkage at 209-211 degrees C, immediately followed by
an abrupt extension leading to film failure. Both storage and loss mod
ulus curves significantly shifted upwards for beta-sheet films, obtain
ed by treatment with less than or equal to 60% methanol for 30 min. Th
e loss peak exhibited a maximum at 236 degrees C. Accordingly, the TMA
shrinkage at above 200 degrees C disappeared. The films broke beyond
330 degrees C, failure being preceded by a broad contraction step. Int
ermediate DMA and TMA patterns were observed for the other solvent-tre
ated films. The loss peak shifted to higher temperature (219-220 degre
es C), and a minor loss modulus component appeared at about 230 degree
s C. This coincided with the onset of a plateau region in the storage
modulus curve. The TMA extension-contraction events in the range 200-3
00 degrees C weakened, and the samples displayed a final broad contrac
tion (peak temperature 326-338 degrees C) before breaking. The DMA and
TMA response of these films was attributed to partial annealing by so
lvent treatment, which resulted in the formation of nuclei of beta-she
et crystallization within the film matrix. The increased thermal stabi
lity was probably due to the small beta-sheet crystals formed, which a
cted as high-strength junctions between adjacent random coil and a-hel
ix domains. (C) 1998 John Wiley & Sons, Inc.