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Main‐Chain Chirality and Optical Activity in Polymers Consisting of CC Chains
Author(s) -
Wulff Günter
Publication year - 1989
Publication title -
angewandte chemie international edition in english
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 5.831
H-Index - 550
eISSN - 1521-3773
pISSN - 0570-0833
DOI - 10.1002/anie.198900211
Subject(s) - chirality (physics) , copolymer , polymer , enantiomer , styrene , optically active , polymer chemistry , materials science , methyl methacrylate , methacrylate , side chain , optical rotatory dispersion , chemistry , organic chemistry , circular dichroism , crystallography , chiral symmetry breaking , symmetry breaking , physics , quantum mechanics , nambu–jona lasinio model
Main‐chain chirality is the optical activity resulting from the configurational or conformational arrangement in the main chain of a polymer. The chirality of the most important types of structures has been investigated on the basis of systematic considerations of symmetry. This has led to the surprising result that even in polymers derived from 1‐substituted or nonsymmetric 1,1‐disubstituted olefins (the technologically most important polymers) several types of chiral structures exist, which are expected to result in optical activity if a particular enantiomer is favorably formed. By carrying out an asymmetric cyclopolymerization, it has been possible to obtain certain structural types in the form of optically active copolymers or homopolymers (e.g., copolymers of styrene with methyl methacrylate, or even the homopolymer of styrene). Another new group of optically active polymers consists of the atropisomeric helical polyisocyanides, poly(trityl methacrylates), and polychlorals. Optically active polymers are already used as adsorbents for the chromatographic separation of racemic mixtures. Further applications are likely to emerge.