Curing of bisphenol M dicyanate ester under nanoscale constraint

被引:60
作者
Li, Qingxiu [1 ]
Simon, Sindee L. [1 ]
机构
[1] Texas Tech Univ, Dept Chem Engn, Lubbock, TX 79409 USA
关键词
D O I
10.1021/ma702144b
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
Nanoscale constraint is known to have a significant impact on the thermal properties of materials. Although thermosetting resins have been cured in the presence of nanoparticles and nanotubes, cure of thermosetting resins under the well-defined nanoscale constraints imposed by controlled pore glass (CPG) or similar matrices has not been previously documented. In this work, we investigate the isothermal curing under nanoscale constraint of a thermosetting resin, bisphenol M dicyanate ester (BMDC), which trimerizes to form a polycyanurate network material. Differential scanning calorimetry is used to monitor the evolution of the glass transition temperature (T-g) and the conversion during cure as a function of the diameter of the silanized control pore glass matrix which is used for confinement. A T-g depression is observed for both the bisphenol M dicyanate ester monomer and the polycyanurate networks; the depression is only a few degrees for the monomer, whereas a 56 K depression is observed for the "fully cured" network in 11.5 nm pores. The nanoscale constraint is also found to strongly increase the rate of cure of bisphenol M dicyanate ester, but it does not affect the normalized T-g vs conversion relationship. The appearance of a secondary T-g above the primary T-g in the smaller pores and the associated length scale are discussed.
引用
收藏
页码:1310 / 1317
页数:8
相关论文
共 80 条
[1]  
Ajayan PM, 2000, ADV MATER, V12, P750, DOI 10.1002/(SICI)1521-4095(200005)12:10<750::AID-ADMA750>3.0.CO
[2]  
2-6
[3]   Effects of confinement on freezing and melting [J].
Alba-Simionesco, C. ;
Coasne, B. ;
Dosseh, G. ;
Dudziak, G. ;
Gubbins, K. E. ;
Radhakrishnan, R. ;
Sliwinska-Bartkowiak, M. .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2006, 18 (06) :R15-R68
[4]   Effects of confinement on material behaviour at the nanometre size scale [J].
Alcoutlabi, M ;
McKenna, GB .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2005, 17 (15) :R461-R524
[5]   Length scale of cooperativity in the dynamic glass transition [J].
Arndt, M ;
Stannarius, R ;
Groothues, H ;
Hempel, E ;
Kremer, F .
PHYSICAL REVIEW LETTERS, 1997, 79 (11) :2077-2080
[6]   Dielectric investigations of the dynamic glass transition in nanopores [J].
Arndt, M ;
Stannarius, R ;
Gorbatschow, W ;
Kremer, F .
PHYSICAL REVIEW E, 1996, 54 (05) :5377-5390
[7]   Mechanical properties of Al2O3/polymethylmethacrylate nanocomposites [J].
Ash, BJ ;
Rogers, DF ;
Wiegand, CJ ;
Schadler, LS ;
Siegel, RW ;
Benicewicz, BC ;
Apple, T .
POLYMER COMPOSITES, 2002, 23 (06) :1014-1025
[8]   The glass transition temperature versus the fictive temperature [J].
Badrinarayanan, Prashanth ;
Zheng, Wei ;
Li, Qingxiu ;
Simon, Sindee L. .
JOURNAL OF NON-CRYSTALLINE SOLIDS, 2007, 353 (26) :2603-2612
[9]   Quantitative equivalence between polymer nanocomposites and thin polymer films [J].
Bansal, A ;
Yang, HC ;
Li, CZ ;
Cho, KW ;
Benicewicz, BC ;
Kumar, SK ;
Schadler, LS .
NATURE MATERIALS, 2005, 4 (09) :693-698
[10]   Controlling the thermornechanical properties of polymer nanocomposites by tailoring the polymer-particle interface [J].
Bansal, Amitabh ;
Yang, Hoichang ;
Li, Chunzhao ;
Benicewicz, Rian C. ;
Kumar, Sanat K. ;
Schadler, Linda S. .
JOURNAL OF POLYMER SCIENCE PART B-POLYMER PHYSICS, 2006, 44 (20) :2944-2950