Volume 42, Issue 5 pp. 800-808
Article

Viscoelastic behaviors and molecular motions of highly syndiotactic poly(vinyl alcohol) fibers

Yasuo Gotoh

Corresponding Author

Yasuo Gotoh

Faculty of Textile Science and Technology, Shinshu University, 3-15-1, Tokida, Ueda 386-8567, Japan

Faculty of Textile Science and Technology, Shinshu University, 3-15-1, Tokida, Ueda 386-8567, JapanSearch for more papers by this author
Yoshitaka Nagara

Yoshitaka Nagara

Joint Research Center for Precision Polymerization, Japan Chemical Innovation Institute, Graduate School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan

Search for more papers by this author
Tamaki Nakano

Tamaki Nakano

Graduate School of Materials Science, Nara Institute of Science and Technology, Takayama-cho 8916-5, Ikoma, Nara 630-0101, Japan

Search for more papers by this author
Yoshio Okamoto

Yoshio Okamoto

Department of Applied Chemistry, Graduate School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan

Search for more papers by this author
Yutaka Ohkoshi

Yutaka Ohkoshi

Faculty of Textile Science and Technology, Shinshu University, 3-15-1, Tokida, Ueda 386-8567, Japan

Search for more papers by this author
Masanobu Nagura

Masanobu Nagura

Faculty of Textile Science and Technology, Shinshu University, 3-15-1, Tokida, Ueda 386-8567, Japan

Search for more papers by this author
First published: 21 January 2004
Citations: 4

Abstract

The viscoelastic behavior and molecular motion of highly syndiotactic poly(vinyl alcohol) (S-PVA) fibers with a dyad syndiotacticity (r) of 69% were studied by dynamic mechanical thermal analysis and wide-angle X-ray diffraction and compared with those of atactic poly(vinyl alcohol) (A-PVA) fibers with r = 54%. The βc dispersion, based on the molecular motion of the chain molecules in the crystalline regions, was observed for A-PVA around 120–140 °C, and the only primary (αc) dispersion was observed for S-PVA around 180 °C. The thermal expansion coefficients for the a and c axes of the A-PVA crystal changed discontinuously around 120 °C, which corresponded to the βc dispersion. For S-PVA, the coefficient for the (002) plane changed discontinuously around 100 °C, similarly to A-PVA, but that for the (100) plane remained unchanged between 20 and 220 °C. These results showed that the intermolecular hydrogen bonding of S-PVA was stronger in the direction of the a axis than in the other directions, suppressing the βc dispersion. The storage modulus and thermal expansion coefficient of the (020) plane (molecular axis) of S-PVA decreased markedly around 180 °C, and this indicated that the αc dispersion was due to the torsional motion of the molecular chains in the crystalline regions. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 800–808, 2004

The full text of this article hosted at iucr.org is unavailable due to technical difficulties.