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Blow-up Prevention by Logistic Damping in a Chemotaxis-May-Nowak Model for Virus Infection

  • Yan Li,
  • Qingshan Zhang

摘要

In this paper, we study the no-flux boundary initial-boundary problem for a three-component reaction-diffusion system originating from the classical May-Nowak model for viral infection \(\begin{aligned} {\left\{ \begin{array}{ll} u_t=\Delta u-\chi \nabla \cdot (u\nabla v)+\kappa -u-uw-\mu u^{\alpha },\\ v_t=\Delta v-v+uw,\\ w_t=\Delta w-w+v \end{array}\right. } \end{aligned}\) u t = Δ u - χ · ( u v ) + κ - u - u w - μ u α , v t = Δ v - v + u w , w t = Δ w - w + v in a smoothly bounded domain \(\Omega \subset {\mathbb {R}}^n\) Ω R n , \(n\ge 1\) n 1 . It is shown that for any \(\kappa >0\) κ > 0 , \(\mu >0\) μ > 0 and sufficiently regular nonnegative initial data \((u_0,v_0,w_0)\) ( u 0 , v 0 , w 0 ) , the system possesses a unique nonnegative global bounded classical solution provided \(\begin{aligned} \alpha >\frac{n+2}{2}. \end{aligned}\) α > n + 2 2 . Moreover, we show the large time behavior of the solution with respect to the size of \(\kappa \) κ . More precisely, we prove that

if \(\kappa <1+\mu \) κ < 1 + μ , there exists \(\chi _1^*\) χ 1 such that if \(|\chi |\le \chi _1^*\) | χ | χ 1 , then the solution satisfies \(\begin{aligned} u(\cdot , t)\rightarrow u_*,\ v(\cdot , t)\rightarrow 0\ \text{ and }\ w(\cdot , t)\rightarrow 0\quad \text{ as }\ t\rightarrow \infty \end{aligned}\) u ( · , t ) u , v ( · , t ) 0 and w ( · , t ) 0 as t in \(L^{\infty }(\Omega )\) L ( Ω ) exponentially, where \(u_*\) u is the solution of algebraic equation \(\begin{aligned} \kappa -y-\mu y^{\alpha }=0; \end{aligned}\) κ - y - μ y α = 0 ;

if \(\kappa >1+\mu \) κ > 1 + μ , then there exists \(\chi _2^*\) χ 2 with the property that if \(|\chi |\le \chi _2^*\) | χ | χ 2 , then the solution fulfills that \(\begin{aligned} u(\cdot , t)\rightarrow 1,\ v(\cdot , t)\rightarrow \kappa -1-\mu \ \text{ and }\ w(\cdot , t)\rightarrow \kappa -1-\mu \quad \text{ as }\ t\rightarrow \infty \end{aligned}\) u ( · , t ) 1 , v ( · , t ) κ - 1 - μ and w ( · , t ) κ - 1 - μ as t in \(L^{\infty }(\Omega )\) L ( Ω ) .