Given a positive operator $A$ on some Hilbert space, and a nonnegative decreasing summable function $\mu$, we consider the abstract equation with memory $$ \ddot u(t)+ A u(t)- \int_0^t \mu(s)Au(t-s) ds=0 $$ modeling the dynamics of linearly viscoelastic solids. The purpose of this work is to provide numerical evidence of the fact that the energy $$\E(t)=\Big(1-\int_0^t\mu(s)ds\Big)\|u(t)\|^2_1+\|\dot u(t)\|^2 +\int_0^t\mu(s)\|u(t)-u(t-s)\|^2_1ds,$$ of any nontrivial solution cannot decay faster than exponential, no matter how fast might be the decay of the memory kernel $\mu$. This will be accomplished by simulating the integro-differential equation for different choices of the memory kernel $\mu$ and of the initial data.
Lack of superstable trajectories in linear viscoelasticity: a numerical approach
Antonietti, Paola F.;Liverani, Lorenzo;Pata, Vittorino
2023-01-01
Abstract
Given a positive operator $A$ on some Hilbert space, and a nonnegative decreasing summable function $\mu$, we consider the abstract equation with memory $$ \ddot u(t)+ A u(t)- \int_0^t \mu(s)Au(t-s) ds=0 $$ modeling the dynamics of linearly viscoelastic solids. The purpose of this work is to provide numerical evidence of the fact that the energy $$\E(t)=\Big(1-\int_0^t\mu(s)ds\Big)\|u(t)\|^2_1+\|\dot u(t)\|^2 +\int_0^t\mu(s)\|u(t)-u(t-s)\|^2_1ds,$$ of any nontrivial solution cannot decay faster than exponential, no matter how fast might be the decay of the memory kernel $\mu$. This will be accomplished by simulating the integro-differential equation for different choices of the memory kernel $\mu$ and of the initial data.File | Dimensione | Formato | |
---|---|---|---|
77438e01-2b2b-4bad-a522-fa9feb1336a7.pdf
accesso aperto
:
Publisher’s version
Dimensione
1.94 MB
Formato
Adobe PDF
|
1.94 MB | Adobe PDF | Visualizza/Apri |
I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.