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Viscoelastic behavior of an amorphous polymer under oscillations of large amplitude

✍ Scribed by Vinogradov, G. V. ;Yanovsky, Yu. ;Isayev, A. I.


Publisher
Wiley (John Wiley & Sons)
Year
1970
Tongue
English
Weight
968 KB
Volume
8
Category
Article
ISSN
0449-2978

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✦ Synopsis


Abstract

The influence of periodic shear deformation and steady flow on a typical amorphous polymer is discussed. Forced sinusoidal vibrations were applied and the complex viscosity was determined. The action of a vibration of finite amplitude is equivalent to steady flow with a definite finite shear rate. Both processes cause truncation of the long‐time part of the relaxation specturm. It may be accepted to a first approximation that the long‐time boundary of the remaining part of the relaxation spectrum conforms to the long‐time part of the initial spectrum, even if the plateau region of the spectrum is truncated. The concept of limiting truncation of the short‐time part of the spectrum is introduced, this corresponding to the minimum absolute value of the complex viscosity versus reduced frequency and the lowest values of the dynamic and apparent viscosities. With an approximate representation of the relaxation spectrum, calculations were made of the maximum values of the viscosity and the coefficient relating the first difference of normal stresses to the square of the shear rate, and also of the apparent viscosity and normal stresses as functions of the shear rate. The calculated values are compared with experimental measurements, and it is shown that the correlation of the apparent viscosity and the absolute value of the complex viscosity is distributed at high frequencies, being superseded by a correlation between the apparent and dynamic viscosities.


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Behavior of concentrated polystyrene sol
✍ Pearson, Dale S. ;Rochefort, Willie E. πŸ“‚ Article πŸ“… 1982 πŸ› Wiley (John Wiley & Sons) 🌐 English βš– 980 KB

## Abstract The limits of linear viscoelastic behavior of polystyrene solutions have been investigated by subjecting them to large‐amplitude oscillatory strains, Ξ³~0~. At strains less than one we find that the dynamic storage modulus Gβ€²(Ο‰,Ξ³~0~) and the dynamic loss modulus Gβ€³(Ο‰,Ξ³~0~) decrease quadr