水溶液
纤维素
化学
回转半径
尿素
再生纤维素
溶剂
特性粘度
持续时间
摩尔质量
粘度计
高分子化学
分析化学(期刊)
分子
粘度
材料科学
聚合物
有机化学
复合材料
作者
Jie Cai,Lei Zhu,Lina Zhang
摘要
Abstract Cellulose was dissolved rapidly in 4.6 wt % LiOH/15 wt % urea aqueous solution and precooled to –10 °C to create a colorless transparent solution. 13 C‐NMR spectrum proved that it is a direct solvent for cellulose rather than a derivative aqueous solution system. The result from transmission electron microscope showed a good dispersion of the cellulose molecules in the dilute solution at molecular level. Weight‐average molecular weight ( M w ), root mean square radius of gyration (〈 s 2 〉 z 1/2 ), and intrinsic viscosity ([η]) of cellulose in LiOH/urea aqueous solution were examined with laser light scattering and viscometry. The Mark–Houwink equation for cellulose in 4.6 wt % LiOH/15 wt % urea aqueous solution was established to be [η] = 3.72 × 10 −2 M in the M w region from 2.7 × 10 4 to 4.12 × 10 5 . The persistence length ( q ), molar mass per unit contour length ( M L ), and characteristic ratio ( C ∞ ) of cellulose in the dilute solution were given as 6.1 nm, 358 nm −1 , and 20.8, respectively. The experimental data of the molecular parameters of cellulose agreed with the Yamakawa–Fujii theory of the worm‐like chain, indicating that the LiOH/urea aqueous solution was a desirable solvent system of cellulose. The results revealed that the cellulose exists as semistiff‐chains in the LiOH/urea aqueous solution. The cellulose solution was stable during measurement and storage stage. This work provided a new colorless, easy‐to‐prepare, and nontoxic solvent system that can be used with facilities to investigate the chain conformation and molecular weight of cellulose. © 2006 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 44: 3093–3101, 2006
科研通智能强力驱动
Strongly Powered by AbleSci AI