Sharp Stability of a String with Local Degenerate Kelvin-Voigt Damping

Abstract

This paper is on the asymptotic behavior of the elastic string equation with localized degenerate Kelvin--Voigt damping $$ u_{tt}(x,t)-[u_{x}(x,t)+b(x)u_{x,t}(x,t)]_{x}=0,\; x\in(-1,1),\; t>0,$$ where $b(x)=0$ on $x\in (-1,0]$, and $b(x)=x^\alpha>0$ on $x\in (0,1)$ for $\alpha\in(0,1)$. It is known that the optimal decay rate of solution is $t^{-2}$ in the limit case $\alpha=0$, and exponential decay rate for $\alpha\ge 1$. When $\alpha\in (0,1)$, the damping coefficient $b(x)$ is continuous, but its derivative has a singularity at the interface $x=0$. In this case, the best known decay rate is $t^{-\frac{3-\alpha}{2(1-\alpha)}}$. Although this rate is consistent with the exponential one at $\alpha=1$, it failed to match the optimal one at $\alpha=0$. In this paper, we obtain a sharper polynomial decay rate $t^{-\frac{2-\alpha}{1-\alpha}}$. More significantly, it is consistent with the optimal polynomial decay rate at $\alpha=0$ and the exponential decay rate at $\alpha = 1$.This is a big step toward the goal of obtaining eventually the optimal decay rate.