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Global boundedness of weak solutions for an attraction-repulsion chemotaxis system with p-Laplacian diffusion and nonlinear production

Zhe Jia

2023Discrete and Continuous Dynamical Systems - B18 citationsDOIOpen Access PDF

Abstract

This paper is concerned with the following attraction-repulsion chemotaxis system with p-Laplacian diffusion and nonlinear production: $ u_{t} = \nabla\cdot(|\nabla u|^{p-2}\nabla u)-\chi \nabla\cdot(u \nabla v)+\xi \nabla\cdot(u \nabla w)+f(u) $, $ v_{t} = \triangle v-\beta v+\alpha u^{k_{1}} $, $ w_{t} = \triangle w-\delta w+\gamma u^{k_{2}} $, under homogenous Neumann boundary condition in a bounded domain $ \Omega \subset \mathbb{R}^{n}(n\geq2) $, with $ \chi, \xi, \alpha,\beta,\gamma,\delta, k_{1}, k_{2} >0, p>1 $. In addition, the function $ f $ satisfying $ f(s)\equiv 0 $ or generalizing the logistic-type source $ f(s) = \kappa s-\mu s^{l} $ for all $ s\geq0 $ with $ \kappa\in \mathbb{R}, \mu>0, l>1 $. It is shown that (ⅰ) When $ f(u)\equiv0 $, if $ p>\frac{n(\max\{k_{1},k_{2}\}+2)}{n+1} $ or $ 1<p\leq\frac{n(\max\{k_{1},k_{2}\}+2)}{n+1} $ with $ \|u_{0}\|_{L^{\frac{(\max\{k_{1},k_{2}\}-p+2)n}{p}}(\Omega)} $ is small, the problem possesses a global bounded weak solution. (ⅱ) When $ f(u) = \kappa u-\mu u^{l} $, if $ \max\{k_{1},k_{2}\}< l-1 $ or $ \max\{k_{1},k_{2}\} = l-1 $ with large $ \mu>0 $, the problem possesses a global bounded weak solution.

Topics & Concepts

Nabla symbolCombinatoricsBounded functionPhysicsOmegaDomain (mathematical analysis)Neumann boundary conditionBoundary (topology)MathematicsMathematical analysisQuantum mechanicsMathematical Biology Tumor GrowthCellular Mechanics and InteractionsMathematical and Theoretical Epidemiology and Ecology Models
Global boundedness of weak solutions for an attraction-repulsion chemotaxis system with p-Laplacian diffusion and nonlinear production | Litcius