English

Boundedness in a fully parabolic attraction-repulsion chemotaxis system with nonlinear diffusion and signal-dependent sensitivity

Analysis of PDEs 2021-08-10 v3

Abstract

This paper deals with the quasilinear fully parabolic attraction-repulsion chemotaxis system \begin{align*} u_t=\nabla \cdot (D(u)\nabla u) -\nabla \cdot (G(u)\chi(v)\nabla v) +\nabla\cdot(H(u)\xi(w)\nabla w), \quad v_t=d_1\Delta v+\alpha u-\beta v, \quad w_t=d_2\Delta w+\gamma u-\delta w, \quad x \in \Omega,\ t>0, \end{align*} under homogeneous Neumann boundary conditions and initial conditions, where ΩRn\Omega \subset \mathbb{R}^n (n1)(n \ge 1) is a bounded domain with smooth boundary, d1,d2,α,β,γ,δ>0d_1, d_2, \alpha, \beta, \gamma, \delta>0 are constants. Also, the diffusivity DD, the density-dependent sensitivities G,HG, H fulfill D(s)=a0(s+1)m1D(s)=a_0(s+1)^{m-1} with a0>0a_0>0 and mRm \in \mathbb{R}; 0G(s)b0(s+1)q10 \le G(s) \le b_0(s+1)^{q-1} with b0>0b_0>0 and q<min{2, m+1}q<\min\{2,\ m+1\}; 0H(s)c0(s+1)r10 \le H(s) \le c_0(s+1)^{r-1} with c0>0c_0>0 and r<min{2, m+1}r<\min\{2,\ m+1\}, and the signal-dependent sensitivities χ,ξ\chi, \xi satisfy 0<χ(s)χ0sk10<\chi(s)\le \frac{\chi_0}{s^{k_1}} with χ0>0\chi_0>0 and k1>1k_1>1; 0<ξ(s)ξ0sk20<\xi(s)\le \frac{\xi_0}{s^{k_2}} with ξ0>0\xi_0>0 and k2>1k_2>1. Global existence and boundedness in the case that w=0w=0 were proved by Ding (J. Math. Anal. Appl.; 2018;461;1260-1270) and Jia-Yang (J. Math. Anal. Appl.; 2019;475;139-153). However, there is no work on the above fully parabolic attraction-repulsion chemotaxis system with nonlinear diffusion and signal-dependent sensitivity. This paper develops global existence and boundedness of classical solutions to the above system by introducing a new test function.

Keywords

Cite

@article{arxiv.2103.02246,
  title  = {Boundedness in a fully parabolic attraction-repulsion chemotaxis system with nonlinear diffusion and signal-dependent sensitivity},
  author = {Yutaro Chiyo and Tomomi Yokota},
  journal= {arXiv preprint arXiv:2103.02246},
  year   = {2021}
}
R2 v1 2026-06-23T23:41:57.296Z