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A fractional attraction-repulsion chemotaxis system with generalized logistic source and nonlinear productions

Liyan Song, Qingchun Li, Chengyuan Qu

Abstract

This paper studies a fractional attraction-repulsion system with generalized logistic source and nonlinear productions: \begin{equation*} \left\{ \begin{aligned} &u_t = -(-Δ)^αu - χ_1 \nabla \cdot (u \nabla v) + χ_2 \nabla \cdot (u \nabla w) + au - bu^γ, &x \in \mathbb{R}^N, \, t > 0, \\ &0 = Δv - λ_1 v + μ_1 u^k, &x \in \mathbb{R}^N, \, t > 0, \\ &0 = Δw - λ_2 w + μ_2 u^k, &x \in \mathbb{R}^N, \, t > 0. \end{aligned} \right. \end{equation*} We first establish the global boundedness of classical solutions with nonnegative bounded and uniformly continuous initial data in two different cases: $γ\geq k + 1$ and $γ< k + 1$, respectively. Next, we show the asymptotic behavior of the global solutions for both cases $γ= k + 1$ and $γ\neq k + 1$. Finally, we obtain the spreading speed of solutions. In particular, when $γ= k + 1$, the upper bound of the spreading speed increases monotonically with $k$. If the condition of balanced attraction-repulsion intensities is further specified, the spreading speed will be equal to $\frac{a}{N + 2α}$.

A fractional attraction-repulsion chemotaxis system with generalized logistic source and nonlinear productions

Abstract

This paper studies a fractional attraction-repulsion system with generalized logistic source and nonlinear productions: \begin{equation*} \left\{ \begin{aligned} &u_t = -(-Δ)^αu - χ_1 \nabla \cdot (u \nabla v) + χ_2 \nabla \cdot (u \nabla w) + au - bu^γ, &x \in \mathbb{R}^N, \, t > 0, \\ &0 = Δv - λ_1 v + μ_1 u^k, &x \in \mathbb{R}^N, \, t > 0, \\ &0 = Δw - λ_2 w + μ_2 u^k, &x \in \mathbb{R}^N, \, t > 0. \end{aligned} \right. \end{equation*} We first establish the global boundedness of classical solutions with nonnegative bounded and uniformly continuous initial data in two different cases: and , respectively. Next, we show the asymptotic behavior of the global solutions for both cases and . Finally, we obtain the spreading speed of solutions. In particular, when , the upper bound of the spreading speed increases monotonically with . If the condition of balanced attraction-repulsion intensities is further specified, the spreading speed will be equal to .

Paper Structure

This paper contains 4 sections, 8 theorems, 135 equations, 1 table.

Key Result

Proposition 1.1

Let $\gamma > 1$, $k\geq1$, $\alpha \in ( \frac{1}{2}, 1)$ and $0 \leq u_0 \in C_{unif}^b \left( \mathbb{R}^N \right)$. Then there exist a maximal existence time $T_{\max}$ and a unique nonnegative classical solution $(u, v, w)$ on $[0, T_{\max})$ such that $\lim_{t \to 0^+} u(\cdot, t) = u_0$ and Moreover, if $T_{\max} < \infty$, then

Theorems & Definitions (12)

  • Proposition 1.1
  • Theorem 1.1: Global Boundedness
  • Theorem 1.2: Asymptotic Behavior
  • Theorem 1.3: Spreading Speed
  • Lemma 2.1: ZZL, Lemma 4.2
  • Lemma 2.2
  • proof
  • Definition 2.3: PR
  • Lemma 3.1
  • proof
  • ...and 2 more