X-RAY STRUCTURE OF POLYANILINE

被引:1299
作者
POUGET, JP
JOZEFOWICZ, ME
EPSTEIN, AJ
TANG, X
MACDIARMID, AG
机构
[1] OHIO STATE UNIV,DEPT PHYS,COLUMBUS,OH 43210
[2] OHIO STATE UNIV,DEPT CHEM,COLUMBUS,OH 43210
[3] UNIV PENN,DEPT CHEM,PHILADELPHIA,PA 19104
[4] UNIV PARIS 11,UTILISAT RAYONNEMENT ELECTROMAGNET LAB,F-91405 ORSAY,FRANCE
关键词
D O I
10.1021/ma00003a022
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
We distinguish between two classes of the emeraldine form of polyaniline. Class I emeraldine is that for which the conducting HCl salt exhibits ES-I crystal structure and the insulating base form is essentially amorphous EB-I. In general, class I materials are formed when the polymer is obtained from solution in the protonated form. Samples of polyaniline belonging to class II possess ES-II structure in the conducting HCl salt form and EB-II structure in the insulating base form. Emeraldine samples belonging to class II were prepared originally in the nonprotonated form. The crystalline components of ES-I, EB-II, and ES-II have been analyzed, and basic parameters of the structures have been derived from comparison between diffraction patterns and intensity calculations. EB-II has a structure similar to that of chemically analogous polymers such as poly(phenylene sulfide) and poly(phenylene oxide). ES-I and ES-II structures differ substantially in their compactness. In class I the increase of crystallite size and decrease in interchain separation with protonation correlate with increasing three-dimensional delocalization of charge with increasing protonation. In contrast, in partially crystalline EB-II, initially protonation occurs in amorphous regions with only subsequent doping into the crystalline areas.
引用
收藏
页码:779 / 789
页数:11
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