THE VANISHING VISCOSITY LIMIT ON A MODEL OF KAREIVA-ODELL TYPE IN 2D

被引:0
|
作者
Luo, Yong [1 ]
Jin, Chunhua [1 ]
Yin, Jingxue [1 ]
机构
[1] South China Normal Univ, Sch Math Sci, Guangzhou 510631, Peoples R China
来源
关键词
Key veords and phrases; Prey-taxis; classical solution; strong solution; vanishing viscosity limit; PREDATOR-PREY MODEL; REACTION-DIFFUSION EQUATIONS; GLOBAL EXISTENCE; SPATIAL HETEROGENEITY; BLOW-UP; CLASSICAL-SOLUTIONS; HAPTOTAXIS MODEL; STEADY-STATES; SYSTEM; AGGREGATION;
D O I
10.3934/dcdsb.2023116
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
. In this paper we invoke the idea of vanishing viscosity limit to bridge the strong solutions of two models in 2D case, i.e., a model of KareivaOdell type in which predators have a remarkable tendency of moving towards diffusible prey, and a model of Stevens-Othmer type where a species has an oriented movement toward a nondiffusing signal. In more detail, we first give in L & INFIN;(& omega;) a uniform-in-& epsilon; upper bound of the unique (for each fixed diffusion coefficient & epsilon; of prey) classical solution of a model of Kareiva-Odell type for any & epsilon; & ISIN; (0, 1). Then we make Lp estimates on the classical solutions to derive a quantitative description in the sense of strong solution. Via the estimates made for the Kareiva-Odell type model, we use Aubin-Lions lemma to show a convergence as & epsilon; & RARR; 0. Finally, we find that the limit of this convergence is a strong solution and also a unique classical solution of a corresponding Stevens-Othmer type model.
引用
收藏
页码:833 / 874
页数:42
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