Diffusivity and viscosity of concentrated hydrogenated polybutadiene solutions

Citation
H. Tao et al., Diffusivity and viscosity of concentrated hydrogenated polybutadiene solutions, MACROMOLEC, 33(5), 2000, pp. 1747-1758
Citations number
75
Categorie Soggetti
Organic Chemistry/Polymer Science
Journal title
MACROMOLECULES
ISSN journal
00249297 → ACNP
Volume
33
Issue
5
Year of publication
2000
Pages
1747 - 1758
Database
ISI
SICI code
0024-9297(20000307)33:5<1747:DAVOCH>2.0.ZU;2-N
Abstract
We report measurements of diffusion (D) and viscosity (eta) in hydrogenated polybutadiene (hPB)/alkane solutions. The volume fractions (phi) extend fr om 0.20 up to the melt and the molecular weights (M) from 4900 up to 440 00 0; the number of entanglements per chain, M/M-e, ranges up to about 450. Th e temperature dependences of both D and eta are similar, consistent with li terature values, and independent of phi and M. We thus conclude that the mo nomeric friction factor is also independent of phi and M. For all samples w ith M/M-e greater than or equal to 3 the data are consistent with the scali ng relations D similar to M(-2.4+/-0.1)phi(-1/8+/-0.2) and eta similar to M (3.4+/-0.1)phi(3.8+/-0.2) within the precision of the data the M exponents do not depend on phi and the phi exponents do not depend on M. The M expone nt for D in solution is consistent with previously reported studies for phi less than or equal to 0.4 but apparently conflicts with the reptation valu e of -2.0 in the melt. However, by comparing with the literature melt self- diffusion data for hPB and six other polymers, it is clear that the exponen t is, in fact, universally stronger than -2.0. Furthermore, if a single uni versal exponent is assumed, the best value based on all the data is -2.28 /- 0.05. Our hPB data resolve the longstanding anomaly that the longest rel axation times tau(1) based on translation (similar to R-g(2)/D) and orienta tional relaxation (similar to eta) appeared to have different M dependences . The data also indicate that for both solutions and melts the dynamics are determined primarily by the number of entanglements per chain. The data ar e compared with current models of polymer dynamics, both reptative and nonr eptative. In the former case it is clear that a self-consistent theory inco rporating both "constraint release" and "contour length fluctuations" is re quired.