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In the past years, the asymptotic behavior of viscoelastic equations with past history has been studied by many authors (see [22 27]).
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Besides, Mustafa and Messaoudi [21, 22] investigated the general stability result of viscoelastic equation for relaxation function g satisfying (1.11).
Derived from the functional equation method and the standard solid model (shown in the 'Appendix'), the differential equation governing the contact behavior of viscoelastic bodies can be obtained as ∑ i = 0 2 A i ∂ i ∂ t i F t + 2 πwR = 4 R 3 ∑ i = 0 2 B i ∂ i ∂ t i δ 3 2 t (1).
This work deals with the behavior of viscoelastic jets under gravitational forces described by an asymptotic upper convected Maxwell (UCM) model, system of partial differential equations.
The mechanical behavior of viscoelastic materials combines elements of both viscous fluid and elastic solid responses.
In this paper, we consider the system of nonlinear viscoelastic equations.
The coefficient of determination R2 of the viscoelastic equation and the experimental data is ~0.9639.
The above proposed loss operator is equivalent to the loss operator of the viscoelastic equation for y = 2.
"Behavior control of viscoelastic surfactant system using additives," (Shaohua Lu and P. Somasundaran), oral presentation at the 234th ACS National Meeting, Boston, MA, August 23 , 2007
The stability result of viscoelastic wave equations without time delay has been studied by many authors.
Problem 1 is referred to as a system of viscoelastic wave equations.
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