English

The fast signal diffusion limit in a Keller-Segel system

Analysis of PDEs 2018-06-27 v2

Abstract

This paper deals with convergence of a solution for the parabolic-parabolic Keller-Segel system (uλ)t=Δuλχ(uλvλ),λ(vλ)t=Δvλvλ+uλ\mboxin Ω×(0,) (u_\lambda)_t = \Delta u_\lambda - \chi \nabla \cdot (u_\lambda \nabla v_\lambda), \quad \lambda (v_\lambda)_t = \Delta v_\lambda - v_\lambda + u_\lambda \quad \mbox{in} \ \Omega\times (0,\infty) to that for the parabolic-elliptic Keller-Segel system ut=Δuχ(uv),0=Δvv+u\mboxin Ω×(0,) u_t = \Delta u - \chi \nabla \cdot (u \nabla v), \quad 0= \Delta v -v +u \quad \mbox{in} \ \Omega\times (0,\infty) as λ0\lambda \searrow 0, where Ω\Omega is a bounded domain in Rn\mathbb{R}^n (n2n\ge 2) with smooth boundary, χ,λ>0\chi, \lambda>0 are constants. In chemotaxis systems parabolic-elliptic systems often provided some guide to methods and results for parabolic-parabolic systems. However, there have not been rich results on the relation between parabolic-elliptic systems and parabolic-parabolic systems. Namely, it still remains to analyze on the following question except some cases: Does a solution of the parabolic-parabolic system converge to that of the parabolic-elliptic system as λ0\lambda \searrow 0? In the case that Ω\Omega is the whole space Rn\mathbb{R}^n, or Ω\Omega is a bounded domain and χ\chi is a strong signal sensitivity, some positive answers were shown in the previous works. Therefore, one can expect a positive answer to this question also in the Keller-Segel system in a bounded domain Ω\Omega in some cases. This paper gives some positive answer in the 2-dimensional and the higher-dimensional Keller-Segel system.

Keywords

Cite

@article{arxiv.1711.04328,
  title  = {The fast signal diffusion limit in a Keller-Segel system},
  author = {Masaaki Mizukami},
  journal= {arXiv preprint arXiv:1711.04328},
  year   = {2018}
}

Comments

20 pages. arXiv admin note: text overlap with arXiv:1711.01677

R2 v1 2026-06-22T22:43:30.228Z