DIELECTRIC-SPECTROSCOPY ON DILUTE BLENDS OF POLYISOPRENE POLYBUTADIENE - EFFECTS OF MATRIX POLYBUTADIENE ON THE DYNAMICS OF PROBE POLYISOPRENE

Citation
K. Adachi et al., DIELECTRIC-SPECTROSCOPY ON DILUTE BLENDS OF POLYISOPRENE POLYBUTADIENE - EFFECTS OF MATRIX POLYBUTADIENE ON THE DYNAMICS OF PROBE POLYISOPRENE, Macromolecules, 28(10), 1995, pp. 3588-3596
Citations number
33
Categorie Soggetti
Polymer Sciences
Journal title
ISSN journal
00249297
Volume
28
Issue
10
Year of publication
1995
Pages
3588 - 3596
Database
ISI
SICI code
0024-9297(1995)28:10<3588:DODBOP>2.0.ZU;2-D
Abstract
Dielectric normal mode relaxation was studied on blends containing a s mall amount (similar to 5 wt %) of probe cis-polyisoprenes (PI) in a s eries of polybutadienes (PB) of different molecular weights M(B). Sinc e the PI chain has Stockmayer's type-A dipoles parallel to the chain c ontour, while PB chains do not, we can study global motion dynamics of the probe chain under various entanglement conditions between PI and PB chains. The dielectric normal-mode relaxation time tau of PI with m olecular weight M(I) followed a power law relation tau proportional to M(I)(a) with alpha varying from 2 to 3 depending on Mg: For M(B) < 30 00, alpha = 2.0 +/- 0.1 in agreement with the Rouse model, while for M (B) > 20 000, alpha = 3.0, conforming to the pure reptation model, and in the range 3000 < Mg < 12 000 a increased rather sharply with M(B). When tau was reduced to an isofriction state tau zeta, the log tau ze ta versus log M(I) plots for different M(B) converged at M(I) = 1900 ( congruent to the entanglement spacing M(eB) of bulk PB). The slope a o f each log tau zeta versus log M(I) plot at constant M(I)/M(B) (>1) wa s larger than 3 and became 3.7 (observed for monodisperse PI melts) at M(I)/M(B) congruent to 2-3. These findings were consistently interpre ted with Graessley's constraint release model. The shape of the dielec tric loss curves (reflecting the distribution of relaxation times) of the blends agreed rather well with the Rouse model when M(I)/M(B) > 10 and Mg < M(eB), but the loss curves became broader with decreasing M( I)/M(B) (or increasing M(B) > M(eB)) especially in the high-frequency tail, as usually observed in monodisperse P-I melts.