Radius of gyration of polystyrene combs and centipedes in solution

Citation
Y. Nakamura et al., Radius of gyration of polystyrene combs and centipedes in solution, MACROMOLEC, 33(22), 2000, pp. 8323-8328
Citations number
35
Categorie Soggetti
Organic Chemistry/Polymer Science
Journal title
MACROMOLECULES
ISSN journal
00249297 → ACNP
Volume
33
Issue
22
Year of publication
2000
Pages
8323 - 8328
Database
ISI
SICI code
0024-9297(20001031)33:22<8323:ROGOPC>2.0.ZU;2-6
Abstract
The method of Iatrou et al. (Macromolecules 1998, 31, 6697) was applied to synthesize a normal comb polystyrene sample with uniform side chains equall y spaced along the main chain but with the most probable distribution in th e main chain length. The molecular weights of the side chain and the connec tor (the part of the main chain between the neighboring side Chains) were 3 .5 x 10(4) and 2.3 x 104, respectively. The sample was analyzed using a gel -permeation chromatography system with a multiangle light scattering and re fractive index detector to determine the relationship between the z-average mean square radius of gyration [S-2] and the weight-average molecular weig ht M-W. Tetrahydrofuran (THF) was chosen as the solvent. The relation fell considerably below that for linear polystyrene. The slope of the plot of lo g [S2](1/2) vs log M-w for the comb polymer was 0.46, a value much smaller than the Flory exponent 0.6 for linear chains in good solvents. Similar mea surements were also made on polystyrene centipedes prepared by Iatrou et al ., which have two side chains at each junction point. As the ratio r of the molecular weight of the side chain to that of the connector increased, the [S-2] VS M-w relation was lowered. Comparison of the experimental relation ship with theoretical predictions for flexible discrete chains suggested th at the main chains of the two types of polymer are stiffened by the crowdin g of the side chains. To estimate the backbone stiffness, [S-2] was calcula ted on the basis of the wormlike comb model whose main and side chains have different Kuhn lengths lambda (-1) and lambda (-1)(s), respectively. With lambda (-1)(s) = 2 nm and the linear mass density = 390 nm(-1) (for both ma in chain and side chains), lambda (-1) was estimated so as to give the clos est agreement between the calculated and measured [S-2]. It was found that the calculated values for the comb polymer with lambda (-1) = 5.5 nm agree closely with the experimental data. The data for the centipedes were also e xplained by the theory, which showed the backbone stiffness to increase wit h increasing r.