ABSTRACT:Further comments on the analysis of dilute solution data are provided. Light-scattering and intrinsic-viscosity data used for this purpose are those obtained for monodisperse polystyrenes, prepared anionically in tetrahydrofuran, in benzene, toluene, and dichloroethane at 30°C and in cyclohexane at temperatures ranging from 32.2 to 60.1 °C. The value of [r;]o/M1/ 2 is somewhat greater than the corresponding value for Berry's polystyrenes prepared anionically in benzene, where [r;]o is the intrinsic viscosity at the theta temperature and M is the polymer molecular weight. This suggests that the two types of samples differ in microstructure, though the precise difference is unknown. However, it is shown that the two-parameter relationships established experimentally in the previous papers are well reproduced in the present data. The relationships are different from those determined by Kato, et al., for monodisperse poly(a-methylstyrene) prepared anionically. Since there is shown to be no essential difference between our and their methods of determining mean-square radii, it seems unlikely that the difference is related to measurements and subsequent treatments. It is suggested rather that the problem is related to Kato's samples.KEY WORDS Two-parameter Theory / Excluded-volume Effect / Mean-square Radius / Second Virial Coefficient / Intrinsic Viscosity / Expansion Factor / Scattering Function / Polystyrene / Anionic Polymerization / In the previous paper, 1 it has been pointed out that recent experimental studies on the ex-. eluded-volume effect in dilute polymer solutions may be classified into two groups with respect to the behavior of experimental data. The investigations of Berry,2 Norisuye, et a/., 3 ' 4 and Tanaka, et al., 1 ' 5 belong to the same category, which will be referred to as the first group, and the work of Kato, et al., 6 ' 7 is representative of the second group. There is fairly close agreement between the results of the two groups for theta-solvent systems, while the difference · between them is noticeable for good-solvent systems, i.e., for large expansion factor as, as defined by a 8 2 =(S 2 )/(S 2 ) 0 , where (S 2 ) is the mean-square radius of the polymer chain and (S 2 ) 0 is its unperturbed value in the theta state. for the chain of n effective bonds with /3 the binary-cluster integral for a pair of segments. Note that Berry's viscosity data 2 proved to belong rather to the first group after the reanalysis by 799