Flow birefringence is used to study stress relaxation following step strain deformations of a well entangled polyisoprene melt. The optical method employs multiple light paths to fully sample the three-dimensional stress tensor, and hence provides measurements of all three independent shear material
Atomic level picture of stress relaxation in polymer melts
β Scribed by G. Loriot; J. H. Weiner
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 273 KB
- Volume
- 36
- Category
- Article
- ISSN
- 0887-6266
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β¦ Synopsis
We have been developing a physical picture on the atomic level of stress relaxation in polymer melts by means of computer simulation of the process in model systems. In this article we treat a melt of freely jointed chains, each with N Γ 200 bonds and with excluded-volume interactions between all nonbonded atoms, that has been subjected to an initial constant-volume uniaxial extension. We consider both the stress relaxation history s(t) based on atomic interactions, and the stress history s e (t; N R ) based on subdividing the chain into segments with N R bonds each, with each segment regarded as an entropic spring. It is found that at early times s(t) ΓΊ s e (t; N R ) for all N R , and that, for the remainder of the simulation, there is no value of N R for which s(t) Γ s e (t; N R ) for an extended period; by the end of the simulation s(t) has fallen just below the value s e (t; 50). The decay of segment orientation, Β»P 2 (t; N R )β¦, and of bond orientation Β»P 2 (t; 1)β¦, is computed during the simulation. It is found that the decay of the atom-based stress s(t) is closely related to that of Β»P 2 (t; 1)β¦. This result may be understood through the concept of steric shielding. The change in local structure of the polymer melt during relaxation is also studied.
π SIMILAR VOLUMES
In order to evolve the methods of mechanical spectroscopy and find new methods of studying the rise of nonlinear viscoelasticity, periodic square and triangular stress functions have been used. A "new" viscoelastic function is defined, log JZ = g { log J1 1, where J1 and JZ are the compliances a t t