ANOMALOUS SEGMENT DIFFUSION IN POLYMERS AND NMR RELAXATION SPECTROSCOPY

Citation
Hw. Weber et R. Kimmich, ANOMALOUS SEGMENT DIFFUSION IN POLYMERS AND NMR RELAXATION SPECTROSCOPY, Macromolecules, 26(10), 1993, pp. 2597-2606
Citations number
41
Categorie Soggetti
Polymer Sciences
Journal title
ISSN journal
00249297
Volume
26
Issue
10
Year of publication
1993
Pages
2597 - 2606
Database
ISI
SICI code
0024-9297(1993)26:10<2597:ASDIPA>2.0.ZU;2-#
Abstract
The dynamics of polymer chains in melts, solutions and networks was st udied by the aid of NMR relaxation spectroscopy. Proton data of the sp in-lattice relaxation curves are reported. Frequency, temperature, fra mes, T1 and T1rho, respectively, and of transverse relaxation curves a re reported. Frequency, temperature, concentration, molecular weight, and cross-link density dependences have been investigated. T1 was meas ured in a frequency range of 10(3) to 3 X 10(8) Hz predominantly using the field-cycling technique. The study refers to polyisoprene, polyis obutylene, poly(tetrahydrofuran), polystyrene, poly(ethylene oxide), p olyethylene, and poly(dimethylsiloxane). The range of molecular weight s was 10(3)-10(6). The power laws for the time dependence of the mean- square displacement, [r2] is-proportional-to t1/2 and [r2] is-proporti onal-to t1/4, predicted by the Doi/Edwards tube model for coil-interna l segment diffusion are shown to have their counterparts in the freque ncy dependence of the spin-lattice relaxation time which is characteri zed by power laws T1 is-proportional-to omega0.5 and T1 is-proportiona l-to omega0.25 in corresponding dynamic ranges. The experimental data can be interpreted on the basis of three components of segment fluctua tions. The crucial process is the reorientation of segments as a conse quence of translational displacements. The orientation correlation fun ction for this mechanism can be derived directly from limits of the ti me dependence of the mean-square segment displacements provided that t he displacements are guided by the chain contour. The experiments show , on the other hand, that the chain dynamics in length scales less tha n the Doi/Edwards tube diameter is not compatible with the Rouse model , whereas that of melts below the critical molecular weight and soluti ons is.