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Optically active helical random copoly(phenylacetylene)s were prepared from structurally similar monomers, (+)-3-hexadecylcarbamoyl-5-[(( S )-1-phenylethyl)carbamoyl]phenylacetylene and 3-hexadecylcarbamoyl-5-(benzylcarbamoyl)phenylacetylene, under the catalysis of Rh[C(C 6 H 5 )═C(C 6 H 5 ) 2 ](nbd)(4-FC 6 H 4 ) 3 P (nbd = 2,5-norbornadiene). The chiral amplification followed either normal or abnormal “sergeants-and-soldiers” rule depending on the solvent nature. In apolar solvents (i.e., CHCl 3 and THF), contracted cis-cisoid M - and P -helices were selectively induced for the copolymers containing chiral units below or above 74 mol %, respectively. In polar solvent (i.e., CHCl 3 /CH 3 OH, 70/30, v/v), a cis-cisoid to cis-transoid transition occurred and stretched M -helices were dominantly formed, the optical activity of which scaled up nonlinearly with increasing chiral component. This unusual phenomenon was rationalized by the distinct competing interactions between the vicinal chiral/achiral and chiral/chiral unit pairs in the contracted and stretched helices according to the modified Ising model. It offers a promising design strategy to control macromolecular helicity.
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Wang et al. (2017) studied this question.
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