Crystallization Behavior of Isotactic Propylene-1-Hexene Random Copolymer Revealed by Time-Resolved SAXS/WAXD Techniques

被引:12
作者
Mao, Yimin [1 ]
Zuo, Feng [1 ]
Keum, Jong Kahk [1 ]
Hsiao, Benjamin S. [1 ]
Thurman, Derek W. [2 ]
Tsou, Andy H. [3 ]
机构
[1] SUNY Stony Brook, Dept Chem, Stony Brook, NY 11794 USA
[2] ExxonMobil Chem Co, Baytown, TX 77520 USA
[3] ExxonMobil Res & Engn Co, Annandale, NJ 08801 USA
基金
美国国家科学基金会;
关键词
crystallization; morphology; propylene-1-hexene; random copolymer; SAXS; WAXD; X-RAY-SCATTERING; LIGHT-SCATTERING; STATISTICAL COPOLYMERS; DENSITY-FLUCTUATIONS; LINEAR POLYETHYLENE; PHASE-TRANSITIONS; LAMELLAR CRYSTALS; POLYPROPYLENE; MELTS; EVOLUTION;
D O I
10.1002/polb.21840
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
The crystallization behavior of isotactic propylene-1-hexene (PH) random copolymer having 5.7% mole fraction of hexene content was investigated using simultaneous time-resolved small-angle X-ray scattering (SAXS) and wide-angle X-ray diffraction (WAXD) techniques. For this copolymer, the hexene component cannot be incorporated into the unit cell structure of isotactic polypropylene (iPP). Only alpha-phase crystal form of iPP was observed when samples were melt crystallized at temperatures of 40 degrees C, 60 degrees C, 80 degrees C, and 100 degrees C. Comprehensive analysis of SAXS and WAXD profiles indicated that the crystalline morphology is correlated with crystallization temperature. At high temperatures (e.g., 100 degrees C) the dominant morphology is the lamellar structure; while at low temperatures (e.g., 40 degrees C) only highly disordered small crystal blocks can be formed. These morphologies are kinetically controlled. Under a small degree of supercooling (the corresponding iPP crystallization rate is slow), a segmental segregation between iPP and hexene components probably takes place, leading to the formation of iPP lamellar crystals with a higher degree of order. In contrast, under a large degree of supercooling (the corresponding iPP crystallization rate is fast), defective small crystal blocks are favored due to the large thermodynamic driving force and low chain mobility. (C) 2009 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 48:26-32,2010
引用
收藏
页码:26 / 32
页数:7
相关论文
共 34 条
[1]   Evolution of density fluctuations to lamellar crystals in linear polyethylene [J].
Akpalu, YA ;
Amis, EJ .
JOURNAL OF CHEMICAL PHYSICS, 1999, 111 (18) :8686-8695
[2]   Effect of polydispersity on the evolution of density fluctuations to lamellar crystals in linear polyethylene [J].
Akpalu, YA ;
Amis, EJ .
JOURNAL OF CHEMICAL PHYSICS, 2000, 113 (01) :392-403
[3]  
ANDREY VD, 1997, J CHEM PHYS, V107, P9234
[4]  
Brandrup J., 1999, Polymer Handbook, VII
[5]   Crystallization and melting of model ethylene-butene copolymers [J].
Crist, B ;
Howard, PR .
MACROMOLECULES, 1999, 32 (09) :3057-3067
[6]   Copolymer crystallization: Approaching equilibrium [J].
Crist, B ;
Finerman, TM .
POLYMER, 2005, 46 (20) :8745-8751
[7]   Thermodynamics of statistical copolymer melting [J].
Crist, B .
POLYMER, 2003, 44 (16) :4563-4572
[8]  
Crist B, 1999, J POLYM SCI POL PHYS, V37, P3131, DOI 10.1002/(SICI)1099-0488(19991101)37:21<3131::AID-POLB22>3.0.CO
[9]  
2-M
[10]   Weak segregation in molten statistical copolymers [J].
de Gennes, PG .
MACROMOLECULAR SYMPOSIA, 2003, 191 :7-9