Global asymptotic stability of bifurcating, positive equilibria of p-Laplacian boundary value problems with p-concave nonlinearities

TL;DR

This paper studies the stability of positive equilibria in a p-Laplacian boundary value problem with nonlinearities, establishing conditions for global stability, instability, and blow-up based on the parameter .

Contribution

It provides a comprehensive analysis of the global asymptotic stability and blow-up phenomena for positive solutions of a nonlinear p-Laplacian problem, including bifurcation structure.

Findings

Global stability of trivial solution for <_{min}(g)

Global stability of positive equilibrium for _{min}(g)<<_{max}(g)

Finite-time blow-up for >_{max}(g)

Abstract

We consider the parabolic, initial value problem $$ v_t =\Delta_p(v)+\lambda g(x,v)\phi_p(v), \quad \text{in $\Omega \times (0,\infty),$} $$ \[ v =0, \text{in $\partial\Omega \times (0,\infty),$}\tag{IVP} v =v_0\ge0, \text{in $\Omega \times \{0\},$} \] where $\Omega$ is a bounded domain in ${\mathbb R}^N$, for some integer $N\ge1$, with smooth boundary $\partial\Omega$, $\phi_p(s):=|s|^{p-1} {\rm sgn}s$, $s\in{\mathbb R}$, $\Delta_p$ denotes the $p$-Laplacian, with $p>\max\{2,N\}$, $v_0\in C^0(\overline{\Omega})$, and $\lambda>0$. The function $g:\overline{\Omega } \times [0,\infty)\to(0,\infty)$ is $C^0$ and, for each $x\in\overline{\Omega }$, the function $g(x,\cdot):[0,\infty)\to(0,\infty)$ is Lipschitz continuous and strictly decreasing. Clearly, (IVP) has the trivial solution $v\equiv0$, for all $\lambda>0$. In addition, there exists $0<\lambda_{\rm min}(g)<\lambda_{\rm max}(g)$ ($\lambda_{\rm max}(g)$ may be $\infty$) such that: $(a)$ if $\lambda\not\in(\lambda_{\rm min}(g),\lambda_{\rm max}(g))$ then (IVP) has no non-trivial, positive equilibrium; $(b)$ if $\lambda\in(\lambda_{\rm min}(g),\lambda_{\rm max}(g))$ then (IVP) has a unique, non-trivial, positive equilibrium $e_\lambda\in W_0^{1,p}(\Omega)$. We prove the following results on the positive solutions of (IVP): $(a)$ if $0<\lambda<\lambda_{\rm min}(g)$ then the trivial solution is globally asymptotically stable; $(b)$ if $\lambda_{\rm min}(g)<\lambda<\lambda_{\rm max}(g)$ then $e_\lambda$ is globally asymptotically stable; $(c)$ if $\lambda_{\rm max}(g)<\lambda$ then any non-trivial solution blows up in finite time.