{"title":"The nonclassical diffusion equations with time-dependent memory kernels and a new class of nonlinearities","authors":"L. T. Thuy, N. Toan","doi":"10.1017/S0017089522000027","DOIUrl":null,"url":null,"abstract":"Abstract In this study, we consider the nonclassical diffusion equations with time-dependent memory kernels \n\\begin{equation*} u_{t} - \\Delta u_t - \\Delta u - \\int_0^\\infty k^{\\prime}_{t}(s) \\Delta u(t-s) ds + f( u) = g \\end{equation*}\n on a bounded domain \n$\\Omega \\subset \\mathbb{R}^N,\\, N\\geq 3$\n . Firstly, we study the existence and uniqueness of weak solutions and then, we investigate the existence of the time-dependent global attractors \n$\\mathcal{A}=\\{A_t\\}_{t\\in\\mathbb{R}}$\n in \n$H_0^1(\\Omega)\\times L^2_{\\mu_t}(\\mathbb{R}^+,H_0^1(\\Omega))$\n . Finally, we prove that the asymptotic dynamics of our problem, when \n$k_t$\n approaches a multiple \n$m\\delta_0$\n of the Dirac mass at zero as \n$t\\to \\infty$\n , is close to the one of its formal limit \n\\begin{equation*}u_{t} - \\Delta u_{t} - (1+m)\\Delta u + f( u) = g. \\end{equation*}\n The main novelty of our results is that no restriction on the upper growth of the nonlinearity is imposed and the memory kernel \n$k_t(\\!\\cdot\\!)$\n depends on time, which allows for instance to describe the dynamics of aging materials.","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2022-02-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1017/S0017089522000027","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
Abstract In this study, we consider the nonclassical diffusion equations with time-dependent memory kernels
\begin{equation*} u_{t} - \Delta u_t - \Delta u - \int_0^\infty k^{\prime}_{t}(s) \Delta u(t-s) ds + f( u) = g \end{equation*}
on a bounded domain
$\Omega \subset \mathbb{R}^N,\, N\geq 3$
. Firstly, we study the existence and uniqueness of weak solutions and then, we investigate the existence of the time-dependent global attractors
$\mathcal{A}=\{A_t\}_{t\in\mathbb{R}}$
in
$H_0^1(\Omega)\times L^2_{\mu_t}(\mathbb{R}^+,H_0^1(\Omega))$
. Finally, we prove that the asymptotic dynamics of our problem, when
$k_t$
approaches a multiple
$m\delta_0$
of the Dirac mass at zero as
$t\to \infty$
, is close to the one of its formal limit
\begin{equation*}u_{t} - \Delta u_{t} - (1+m)\Delta u + f( u) = g. \end{equation*}
The main novelty of our results is that no restriction on the upper growth of the nonlinearity is imposed and the memory kernel
$k_t(\!\cdot\!)$
depends on time, which allows for instance to describe the dynamics of aging materials.