Optical anisotropies of para-halogenated polystyrenes and related molecules

Abstract
The optical anisotropies γ2 and molar Kerr constants mK of C6H5X, p-CH3—C6H4—X and p-(CH3)2CH—C6H4—X where X = Cl or Br, and of atactic poly(p-chlorostyrene) have been determined from depolarized Rayleigh scattering and electric birefringence measurements in CCl4 solutions at 25°C using λ= 633 nm radiation; γ2 for poly(p-bromostyrene) was determined in a mixture of CCl4 and CBr4. The anisotropic part of the polarizability tensors for C6H5Cl and C6H5Br are well defined by γ2 and the molar Cotton–Mouton constant mC, values of which are available from the work of LeFèvre and co-workers for these two compounds. Owing to the orientation of the dipole moment along one of the principal axes of , this tensor cannot be evaluated unambiguously from mK and γ2 for the other compounds. The anisotropy attributable to the arylene group about the axis joining the substituents appears to be little affected by substitution, however. Asymmetry of the arylene group perpendicular thereto depends appreciably on substitution; bond and group polarizabilities are not additive. The anisotropies of the polymers are formulated as the sums of tensors for the corresponding p-halogenocumenes. Averages 〈γ2〉 and 〈mK〉 over all conformations of the polymer chains are calculated as functions of the fraction wm of meso dyads. Values of 〈γ2〉 decrease about three-fold from syndiotactic (wm= 0) to isotactic (wm= 1). 〈mK〉 is extraordinarily sensitive to stereochemical composition; it decreases from a large positive value for wm= 0 to a large negative value for wm= 1. These results are interpreted in terms of structure and preferred conformations. Experimental measurements on atactic polymers support the calculations.