Convexity and Weighted Integral Inequalities for Energy Decay Rates of Nonlinear Dissipative Hyperbolic Systems

2004 ◽  
Vol 51 (1) ◽  
pp. 61-105 ◽  
Author(s):  
Fatiha Alabau-Boussouira
2020 ◽  
Vol 2020 ◽  
pp. 1-12
Author(s):  
Fengyun Zhang

This paper considers the fuzzy viscoelastic model with a nonlinear source u t t + L u + ∫ 0 t g t − ζ Δ u ζ d ζ − u γ u − η Δ u t = 0 in a bounded field Ω. Under weak assumptions of the function g t , with the aid of Mathematica software, the computational technique is used to construct the auxiliary functionals and precise priori estimates. As time goes to infinity, we prove that the solution is global and energy decays to zero in two different ways: the exponential form and the polynomial form.


2009 ◽  
Vol 25 (3) ◽  
pp. 797-821 ◽  
Author(s):  
Ruy Coimbra Charão ◽  
◽  
Jáuber Cavalcante Oliveira ◽  
Gustavo Alberto Perla Menzala ◽  

Author(s):  
J. R. Luo ◽  
T. J. Xiao

We consider an abstract second order non-autonomous evolution equation in a Hilbert space $H:$ $u''+Au+\gamma(t) u'+f(u)=0,$ where $A$ is a self-adjoint and nonnegative operator on $H$, $f$ is a conservative $H$-valued function with polynomial growth (not necessarily to be monotone), and $\gamma(t)u'$ is a time-dependent damping term. How exactly the decay of the energy is affected by the damping coefficient $\gamma(t)$ and the exponent associated with the nonlinear term $f$? There seems to be little development on the study of such problems, with regard to {\it non-autonomous} equations, even for strongly positive operator $A$. By an idea of asymptotic rate-sharpening (among others), we obtain the optimal decay rate of the energy of the non-autonomous evolution equation in terms of $\gamma(t)$ and $f$.  As a byproduct, we show the optimality of the energy decay rates obtained previously in the literature when $f$ is a monotone operator.


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