ABSTRACT

We study the global (in time) existence of nonnegative solutions of the Gierer-Meinhardt system with mixed boundary conditions. In the research, the Robin boundary and Neumann boundary conditions were used on the activator and the inhibitor conditions respectively. Based on the priori estimates of solutions, the considerable results were obtained.

Keywords:

Activator-Inhibitor System, Gierer-Meinhardt System, Robin and Neumann Boundary Conditions, Global Existence

1. Introduction

Biological spatial pattern formation is one area in applied mathematics under- going vivid investigations in recent years. Most models involved in biological phenomena are of the general reaction-diffusion type considered by Turing [1] . The distinctive attribute of Turing’s approach was the role of autocatalysis in coexistence with lateral inhibition. These studies led to the assumption of the existence of two chemical substances known as the activator and the inhibitor [2] [3] .

One of the famous studied models in biological spatial pattern formation is the Gierer-Meinhardt system which has received numerous attention and has been extensively studied [4] [5] [6] . The Gierer-Meinhardt system was used to model the head formation of a small, fresh-water animal called hydra [4] . We consider an activator concentration A and an inhibitor concentration H, satisfying the activator-inhibitor system given by

$(\begin{array}{ll}{A}_t={ϵ}^2\Delta A-A+\frac{A^p}{H^q+b},\hfill & \text{in}\Omega \times \left(0,T\right)\hfill \\ \tau H_t=D\Delta H-H+\frac{A^r}{H^s},\hfill & \text{in}\Omega \times \left(0,T\right)\hfill \\ ϵ\frac{\partial A}{\partial \nu }+aA=0=\frac{\partial H}{\partial \nu },\hfill & \text{on}\partial \Omega \times \left(0,T\right)\hfill \\ H\left(x,0\right)=H_0\left(x\right)>0,A\left(x,0\right)=A_0\left(x\right)\ge 0\hfill & \text{in}\bar{\Omega }\hfill \end{array}$ (1)

where $a\ge 0$ , $b\ge 0$ and $\Omega \subset {ℝ}^N$ is a bounded smooth domain; $\Delta$ is the Laplace or diffusion operator in ${ℝ}^N$ ; $\nu \left(x\right)$ is the unit outer normal at $x\in \partial \Omega$ , $\partial /\partial \nu :=\nabla \cdot \nu$ is the directional derivative in the direction of the vector $\nu$ . We assume that the reaction exponents $\left(p>1,q>0,r>0,s\ge 0\right)$ satisfy

$0<\frac{p-1}{r}<\frac{q}{s+1}.$ (2)

The diffusion constants are $ϵ>0$ and $D>0$ for the activator and inhibitor respectively. The time relaxation constant $\tau >0$ was mathematically intro- duced due to its usefulness on the stability of the system. The constant b provides additional support to the inhibitor and may be thought of as a measure of the effectiveness of the inhibitor in suppressing the production of the activator and that of its own. In [7] , the ratio in the middle of (2) is called net self-activation index, since it compares how strongly the activator activates the production of itself with how strongly it activates that of the inhibitor. On the other hand, they call the ratio on the right hand side of (2) net cross-inhibition index, since it compares how strongly the inhibitor suppresses the production of the activator with that of itself. For the the inequality in (2), we expect the production of the activator to be severely suppressed by the inhibitor.

In [4] , some biological applications such as modeling of skeletal limb development, Robin boundary conditions are more realistic since the Neumann boundary conditions. A comparative numerical study of a reaction-diffusion system was made in [8] with a range of different boundary conditions and it revealed that certain types of boundary conditions selected a particular pattern modes at the expense of others. It was shown that the robustness of certain patterns could be greatly enhanced and the authors showed a possible ap- plication to skeletal pattern of limb.

Special case was considered for the Neumann boundary condition (i.e. $a=0$ ) in [5] [9] . In [5] , Masuda and Takahashi proved the global solutions of the special case of (1) with b = 0 exists for $t>0$ provided in addition to (2) one has $\left(p-1\right)/r<2/\left(N+2\right)$ , we note the strict inequality here. In [9] , Jiang improved the net self-activation index noted in [5] to $\left(p-1\right)/r<1$ and showed that the solutions exists globally in time.

In this paper we consider the Robin boundary condition (a ≠ 0) on the activator and Neumann boundary condition on the inhibitor and study the global (in time) existence of solutions for the Gierer-Meinhardt system in (1). The theorem and lemmas in this current manuscript are inspired by [9] . We establish the global (in time) existence of (1) by proving the theorem below:

Theorem 1. Suppose $\Omega$ is a smooth bounded domain with a smooth

boundary $\partial \Omega$ in ${ℝ}^N$ . Assume that $\frac{p-1}{r}<\min \left\{1,\frac{q}{s+1}\right\}$ . Let $A_0$ and

$H_0\in W^{\mathrm{2,}\mathcal{l}}\left(\Omega \right)$ , $\mathcal{l}>\max \left\{N,2\right\}$ . Then every solution $\left(A\left(x\mathrm{,}t\right)\mathrm{,}H\left(x\mathrm{,}t\right)\right)$ of (1) exists globally in time.

2. Proof of Theorem 1

The local existence and uniqueness of (1) is standard and more details can be found in [10] [11] . A priori-estimates need to be ascertain in order to prove global in time existence of solutions. Let $\left(A\mathrm{,}H\right)$ be a solution of (1) in $\left[\mathrm{0,}T\right)$ . We want to ascertain that H is bounded away from zero. Let

$u\left(t\right)=\underset{x\in \Omega }{\inf }H\left(x,t\right),t\in \left[0,T\right)$

then

$u\left(0\right)=\underset{x\in \Omega }{\inf }{H}_0\left(x\right)>0$

Lemma 1. $u\left(t\right)\ge u\left(0\right){\text{e}}^{-\frac{t}{\tau }}$ for all $0\le t<T$ .

Proof. Let

$H^{*}\left(x,t\right)=H\left(x,t\right)-u\left(0\right){\text{e}}^{-\frac{t}{\tau }}$ (3)

then $H^{*}\left(x,t\right)$ satisfies

$\begin{array}{c}{H}_t^{*}=H_t-{\left[u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\right]}^{\prime }=\frac{1}{\tau }\left[D\Delta H-H+\frac{A^r}{H^s}\right]+\frac{1}{\tau }u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\\ =\frac{1}{\tau }\left[D\Delta H^{*}-\left(H^{*}+u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\right)+\frac{A^r}{H^s}\right]+\frac{1}{\tau }u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\\ =\frac{1}{\tau }\left[D\Delta H^{*}-H^{*}-u\left(0\right){\text{e}}^{-\frac{t}{\tau }}+\frac{A^r}{H^s}\right]+\frac{1}{\tau }u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\\ =\frac{1}{\tau }\left[D\Delta H^{*}-H^{*}+\frac{A^r}{H^s}\right]-\frac{1}{\tau }u\left(0\right){\text{e}}^{-\frac{t}{\tau }}+\frac{1}{\tau }u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\\ =\frac{1}{\tau }\left[D\Delta H^{*}-H^{*}+\frac{A^r}{H^s}\right]=\frac{1}{\tau }\left[D\Delta H^{*}-H^{*}\right]+\frac{A^r}{\tau H^s}\\ \ge \frac{1}{\tau }\left[D\Delta H^{*}-H^{*}\right]\text{in}\Omega \times \left[0,T\right)\end{array}$

and

$\frac{\partial H^{*}}{\partial \nu }=\frac{\partial }{\partial \nu }\left[H\left(x,t\right)-u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\right]=\frac{\partial }{\partial \nu }H\left(x,t\right)$

but

$\frac{\partial H}{\partial \nu }=0\text{on}\partial \Omega \times \left[0,T\right)$

thus

$\frac{\partial H^{*}}{\partial \nu }=0\text{on}\partial \Omega \times \left[0,T\right).$

Additionally at $t=0$ , from (3)

$H^{*}\left(x,0\right)=H\left(x,0\right)-u\left(0\right)=H\left(x,0\right)-\underset{x\in \Omega }{\inf }H\left(x,0\right)\ge 0$

So $H^{\mathrm{<mo>\; *\; </mo>}}\left(x\mathrm{,0}\right)\ge 0$ for any $x\in \Omega$ .

Hence from maximum principle, $H^{\mathrm{<mo>\; *\; </mo>}}\left(x\mathrm{,}t\right)\ge 0$ in $\bar{\Omega }\times \left[\mathrm{0,}T\right)$ and thus

$H\left(x\mathrm{,}t\right)-u\left(0\right){\text{e}}^{-\frac{t}{\tau }}\ge \mathrm{0,}$

$u\left(t\right)=\underset{x\in \Omega }{\inf }H\left(x,t\right)\ge u\left(0\right){\text{e}}^{-\frac{t}{\tau }},t\in \left[0,T\right)$

□

Lemma 2. For any two constants $\alpha >1,\beta \ge 0$ , let $\frac{p-1}{r}<\min \left\{1,\frac{q}{s+1}\right\}$ .

Define

$h_{\alpha ,\beta }\left(t\right)={\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }\left(x,t\right)}{H^{\beta }\left(x,t\right)}\text{d}x,0\le t<T$

Suppose

$2\epsilon \sqrt{\tau D\left(\alpha -1\right)\left(\beta +1\right)}\ge \left(\tau {ϵ}^2+D\right)\sqrt{\alpha \beta },$ (4)

then

${\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)\le \left(\frac{\beta }{\tau }-\alpha \right)h_{\alpha ,\beta }\left(t\right)+C{u}^{-\delta }{h}_{\alpha ,\beta }^{1-\vartheta }\left(t\right).$ (5)

Here

$\vartheta =\frac{\sigma }{\alpha }\left(\frac{r}{r-\left(p-1\right)-\sigma }\right)$ (6)

and

$\delta =\frac{r}{r-\left(p-1\right)-\sigma }\left[q-\frac{\left(s+1\right)\left(p-1\right)}{r}-\left(\frac{s+1}{r}-\frac{\beta }{\alpha }\right)\sigma \right]$ (7)

where $\delta >0$ , $\sigma >0$ , $\vartheta \in \left(\mathrm{0,1}\right)$ and

$C={\left[\alpha {\left(\beta /\tau \right)}^{-\frac{p-1+\sigma }{r}}\right]}^{\frac{r}{r-\left(p-1\right)-\sigma }}{\left|\Omega \right|}^{\vartheta }$

Proof. Let $\alpha >1$ and $\beta \ge 0$ ,

But

$\begin{array}{c}\alpha {ϵ}^2{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta }}\Delta A\text{d}x=\alpha {ϵ}^2{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha -1}}{H^{\beta }}\nabla A\cdot \nu \text{d}S-\alpha {ϵ}^2\left(\alpha -1\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -2}}{H^{\beta }}{\left|\nabla A\right|}^2\text{d}x\\ +\alpha {ϵ}^2\beta {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x\\ =\alpha {ϵ}^2{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha -1}}{H^{\beta }}\left(\frac{-aA}{ϵ}\right)\text{d}S-\alpha {\epsilon }^2\left(\alpha -1\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -2}}{H^{\beta }}{\left|\nabla A\right|}^2\text{d}x\\ +\alpha {ϵ}^2\beta {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x\\ =-\alpha ϵa{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}S-\alpha {ϵ}^2\left(\alpha -1\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -2}}{H^{\beta }}{\left|\nabla A\right|}^2\text{d}x\\ +\alpha {ϵ}^2\beta {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x\end{array}$

Additionally,

$\begin{array}{c}\frac{\beta D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta +1}}\Delta H\text{d}x=\frac{\beta D}{\tau }{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta +1}}\nabla H\cdot \nu \text{d}S+\frac{\beta \left(\beta +1\right)D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta +2}}{\left|\nabla H\right|}^2\text{d}x\\ -\frac{\alpha \beta D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x\\ =\frac{\beta D}{\tau }{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta +1}}\left(0\right)\text{d}S+\frac{\beta \left(\beta +1\right)D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta +2}}{\left|\nabla H\right|}^2\text{d}x\\ -\frac{\alpha \beta D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x\\ =\frac{\beta \left(\beta +1\right)D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta +2}}{\left|\nabla H\right|}^2\text{d}x-\frac{\alpha \beta D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x\end{array}$

now we have,

$\begin{array}{c}{\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)=\left(\frac{\beta }{\tau }-\alpha \right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}x-\alpha ϵa{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}S-\alpha {ϵ}^2\left(\alpha -1\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -2}}{H^{\beta }}{\left|\nabla A\right|}^2\text{d}x\\ +\alpha \beta \left({ϵ}^2+\frac{D}{\tau }\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha -1}}{H^{\beta +1}}\nabla A\nabla H\text{d}x-\frac{\beta \left(\beta +1\right)D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta +2}}{\left|\nabla H\right|}^2\text{d}x\\ +\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta +q}}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x.\\ =\left(\frac{\beta }{\tau }-\alpha \right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}x-\alpha ϵa{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}S-\alpha {ϵ}^2\left(\alpha -1\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}{\left|\frac{\nabla A}{A}\right|}^2\text{d}x\\ +\alpha \beta \left({ϵ}^2+\frac{D}{\tau }\right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\frac{\nabla H}{H}\frac{\nabla A}{A}\text{d}x-\frac{\beta \left(\beta +1\right)D}{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}{\left|\frac{\nabla H}{H}\right|}^2\text{d}x\\ +\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta +q}}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x.\\ =\left(\frac{\beta }{\tau }-\alpha \right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}x-\alpha ϵa{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}S+\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta +q}}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x\\ +{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}[-\alpha {ϵ}^2\left(\alpha -1\right){\left|\frac{\nabla A}{A}\right|}^2\text{d}x+\alpha \beta \left({ϵ}^2+\frac{D}{\tau }\right)\frac{\nabla H}{H}\frac{\nabla A}{A}\text{d}x\\ -\frac{\beta \left(\beta +1\right)D}{\tau }{\left|\frac{\nabla H}{H}\right|}^2\text{d}x].\end{array}$

We deduce from above a quadratic equation involving $\frac{\nabla A}{A}$ and $\frac{\nabla H}{H}$ . Let us

fix $\alpha >1$ and choose $\beta \ge 0$ , we have

$2ϵ\sqrt{\tau D\left(\alpha -1\right)\left(\beta +1\right)}\ge \left(\tau {ϵ}^2+D\right)\sqrt{\alpha \beta }\mathrm{,}$

therefore the quadratic form involving $\frac{\nabla A}{A}$ and $\frac{\nabla H}{H}$ in the inequality above

is non-positive since its determinant

${\left[\alpha \beta \left({ϵ}^2+\frac{D}{\tau }\right)\frac{\nabla H}{H}\right]}^2\le 4\left[-{ϵ}^2\alpha \left(\alpha -1\right)\right]\left[-\frac{\beta D}{\tau }\left(\beta +1\right){\left|\frac{\nabla H}{H}\right|}^2\right].$

Thus

$\begin{array}{c}{\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)\le \left(\frac{\beta }{\tau }-\alpha \right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}x-\alpha ϵa{\displaystyle {\int }_{\partial \Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}S+\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta +q}}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x\\ \le \left(\frac{\beta }{\tau }-\alpha \right){\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}x+\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta +q}}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x\\ =\left(\frac{\beta }{\tau }-\alpha \right)h_{\alpha \mathrm{,}\beta }\left(t\right)+\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta +q}}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x\mathrm{.}\end{array}$

We have

$\frac{p-1}{r}<1\Rightarrow r-\left(p-1\right)>0$

and

$\frac{p-1}{r}<\frac{q}{s+1}\Rightarrow q>\frac{\left(p-1\right)\left(s+1\right)}{r}$

we choose $\sigma >0$ sufficiently small such that

$r-\left(p-1\right)>\sigma$

and

$q>\frac{\left(p-1\right)\left(s+1\right)}{r}+\left(\frac{s+1}{r}-\frac{\beta }{\alpha }\right)\sigma .$

Now, we write

$\begin{array}{l}\frac{A^{\alpha +p-1}}{H^{\beta }\left(H^q+b\right)}\le \frac{A^{\alpha +p-1}}{H^{\beta }{H}^q}=\frac{A^{\alpha +p-1}}{H^{\beta }{H}^{\delta \left(\frac{r-\left(p-1\right)-\sigma }{r}\right)+\frac{\left(p-1\right)\left(s+1\right)}{r}+\left(\frac{s+1}{r}-\frac{\beta }{\alpha }\right)\sigma }}\\ =\frac{A^{\alpha +p-1}}{H^{\beta }{H}^{\delta \left(\frac{r-\left(p-1\right)-\sigma }{r}\right)}{H}^{\frac{\left(p-1\right)\left(s+1\right)}{r}}{H}^{\left(\frac{s+1}{r}-\frac{\beta }{\alpha }\right)\sigma }}=\frac{A^{\alpha +p-1}{H}^{\beta \frac{\sigma }{\alpha }}}{H^{\beta }{H}^{\delta \left(\frac{r-\left(p-1\right)-\sigma }{r}\right)}{H}^{\frac{\left(p-1\right)\left(s+1\right)}{r}}{H}^{\frac{s+1}{r}\sigma }}\\ =\frac{A^{\alpha +p-1}{H}^{\beta \frac{\sigma }{\alpha }}}{H^{\beta }{H}^{\delta \left(\frac{r-\left(p-1\right)-\sigma }{r}\right)}{H}^{\left(s+1\right)\frac{p-1+\sigma }{r}}}=\frac{A^{\alpha +p-1}{H}^{\beta \frac{\sigma }{\alpha }}}{H^{\beta }{H}^{\delta \left(\frac{r-\left(p-1\right)-\sigma }{r}\right)}{H}^{\left(s+1\right)\frac{p-1+\sigma }{r}}}\\ =\frac{A^{\alpha +p-1}{H}^{\beta \vartheta \left(1-\frac{p-1+\sigma }{r}\right)}}{H^{\beta -\beta \frac{p-1+\sigma }{r}+\beta \frac{p-1+\sigma }{r}}{H}^{\delta \left(1-\frac{p-1+\sigma }{r}\right)}{H}^{\left(s+1\right)\frac{p-1+\sigma }{r}}}=\frac{A^{\alpha +p-1}{H}^{\beta \vartheta \left(1-\frac{p-1+\sigma }{r}\right)}}{H^{\beta \left(1-\frac{p-1+\sigma }{r}\right)}{H}^{\delta \left(1-\frac{p-1+\sigma }{r}\right)}{H}^{(\beta +s+1)\frac{p-1+\sigma }{r}}}\end{array}$

but

$\begin{array}{c}{A}^{\alpha +p-1}=\frac{A^{\alpha }{A}^{p-1}{A}^{\sigma }}{A^{\sigma }}=\frac{A^{\alpha }{A}^{p-1+\sigma }}{A^{\alpha \vartheta \left(1-\frac{p-1+\sigma }{r}\right)}}\\ =\frac{A^{\alpha \left(1-\frac{p-1+\sigma }{r}+\frac{p-1+\sigma }{r}\right)}{A}^{r\frac{p-1+\sigma }{r}}}{A^{\alpha \vartheta \left(1-\frac{p-1+\sigma }{r}\right)}}\\ =\frac{A^{\alpha \left(1-\frac{p-1+\sigma }{r}\right)}{A}^{\alpha \frac{p-1+\sigma }{r}}{A}^{r\frac{p-1+\sigma }{r}}}{A^{\alpha \vartheta \left(1-\frac{p-1+\sigma }{r}\right)}}\\ =A^{\alpha \left(1-\vartheta \right)\left(1-\frac{p-1+\sigma }{r}\right)}{A}^{\left(\alpha +r\right)\frac{p-1+\sigma }{r}}\end{array}$

thus

$\begin{array}{c}\frac{A^{\alpha +p-1}}{H^{\beta +q}}=\frac{A^{\alpha \left(1-\vartheta \right)\left(1-\frac{p-1+\sigma }{r}\right)}{A}^{\left(\alpha +r\right)\frac{p-1+\sigma }{r}}{H}^{\beta \vartheta \left(1-\frac{p-1+\sigma }{r}\right)}}{H^{\beta \left(1-\frac{p-1+\sigma }{r}\right)}{H}^{\delta \left(1-\frac{p-1+\sigma }{r}\right)}{H}^{\left(\beta +s+1\right)\frac{p-1+\sigma }{r}}}\\ =\frac{H^{-\delta \left(1-\frac{p-1+\sigma }{r}\right)}{A}^{\alpha \left(1-\vartheta \right)\left(1-\frac{p-1+\sigma }{r}\right)}{A}^{\left(\alpha +r\right)\frac{p-1+\sigma }{r}}}{H^{\beta \left(1-\vartheta \right)\left(1-\frac{p-1+\sigma }{r}\right)}{H}^{\left(\beta +s+1\right)\frac{p-1+\sigma }{r}}}\\ ={\left[H^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }\right]}^{1-\frac{p-1+\sigma }{r}}{\left(\frac{A^{\alpha +r}}{H^{\beta +s+1}}\right)}^{\frac{p-1+\sigma }{r}}\end{array}$

where $\vartheta$ and $\delta$ are defined by (6) and (7)

$\begin{array}{c}\alpha \frac{A^{\alpha +p-1}}{H^{\beta }\left(H^q+b\right)}\le \alpha {\left[H^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }\right]}^{1-\frac{p-1+\sigma }{r}}{\left(\frac{A^{\alpha +r}}{H^{\beta +s+1}}\right)}^{\frac{p-1+\sigma }{r}}\\ \le \alpha {\left[u^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }\right]}^{1-\frac{p-1+\sigma }{r}}{\left(\frac{A^{\alpha +r}}{H^{\beta +s+1}}\right)}^{\frac{p-1+\sigma }{r}}\\ =\alpha {\left[u^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }\right]}^{1-\frac{p-1+\sigma }{r}}{\left(\frac{\beta {\tau }^{-1}}{\beta {\tau }^{-1}}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\right)}^{\frac{p-1+\sigma }{r}}\\ =\alpha {\left(\frac{\beta }{\tau }\right)}^{-\frac{p-1+\sigma }{r}}{\left[u^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }\right]}^{1-\frac{p-1+\sigma }{r}}{\left(\frac{\beta }{\tau }\frac{A^{\alpha +r}}{H^{\beta +s+1}}\right)}^{\frac{p-1+\sigma }{r}}\end{array}$

by Young’s inequality, we obtain

$\alpha \frac{A^{\alpha +p-1}}{H^{\beta }\left(H^q+b\right)}\le {\left[\alpha {\left(\frac{\beta }{\tau }\right)}^{-\frac{p-1+\sigma }{r}}\right]}^{\frac{r}{r-(p-1)-\sigma }}{u}^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }+\frac{\beta }{\tau }\frac{A^{\alpha +r}}{H^{\beta +s+1}}$

$\alpha \frac{A^{\alpha +p-1}}{H^{\beta }\left(H^q+b\right)}-\frac{\beta }{\tau }\frac{A^{\alpha +r}}{H^{\beta +s+1}}\le {\left[\alpha {\left(\frac{\beta }{\tau }\right)}^{-\frac{p-1+\sigma }{r}}\right]}^{\frac{r}{r-\left(p-1\right)-\sigma }}{u}^{-\delta }{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }.$

Therefore

$\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta }\left(H^q+b\right)}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x\le {\left[\alpha {\left(\frac{\beta }{\tau }\right)}^{-\frac{p-1+\sigma }{r}}\right]}^{\frac{r}{r-\left(p-1\right)-\sigma }}{u}^{-\delta }{\displaystyle {\int }_{\Omega }}{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }\text{d}x$

but by Hölder’s inequality

${\displaystyle {\int }_{\Omega }}{\left(\frac{A^{\alpha }}{H^{\beta }}\right)}^{1-\vartheta }dx\le {\left({\displaystyle {\int }_{\Omega }}\text{d}x\right)}^{\vartheta }{\left({\displaystyle {\int }_{\Omega }}\frac{A^{\alpha }}{H^{\beta }}\text{d}x\right)}^{1-\vartheta }={\left|\Omega \right|}^{\vartheta }{h}_{\alpha ,\beta }^{1-\vartheta }.$

Thus

$\begin{array}{l}\alpha {\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +p-1}}{H^{\beta }\left(H^q+b\right)}\text{d}x-\frac{\beta }{\tau }{\displaystyle {\int }_{\Omega }}\frac{A^{\alpha +r}}{H^{\beta +s+1}}\text{d}x\\ \le {\left[\alpha {\left(\frac{\beta }{\tau }\right)}^{-\frac{p-1+\sigma }{r}}\right]}^{\frac{r}{r-\left(p-1\right)-\sigma }}{u}^{-\delta }{\left|\Omega \right|}^{\vartheta }{h}_{\alpha ,\beta }^{1-\vartheta }=C{u}^{-\delta }{h}_{\alpha ,\beta }^{1-\vartheta }.\end{array}$

Finally,

${\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)\le \left(\frac{\beta }{\tau }-\alpha \right)h_{\alpha ,\beta }+C{u}^{-\delta }{h}_{\alpha ,\beta }^{1-\vartheta }.$

□

Remark 1. The condition in (4) is true for any

$\alpha \ge 2\text{and}0<\beta \le \frac{1}{2K}$

where $K\ge \max \left\{\frac{\tau {ϵ}^2}{D},\frac{D}{\tau {ϵ}^2}\right\}$

Lemma 3. Let $0\le \delta <1$ , $\theta >0$ and $\zeta >0$ on $\left(\mathrm{0,}T\right)$ be an integrable function. Let $h_{\alpha ,\beta }=h_{\alpha ,\beta }\left(t\right)$ be a nonnegative function on $\left[\mathrm{0,}T\right)$ satisfying the differential inequality

${\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)\le -\theta h_{\alpha ,\beta }+\zeta h_{\alpha ,\beta }^{\delta },0\le t<T.$ (8)

Then

$h_{\alpha ,\beta }\left(t\right)\le \kappa ,0\le t<T$ (9)

where $\kappa$ is the maximal root of the algebraic equation

$x-G\left(\zeta \right)x^{\delta }=h_{\alpha ,\beta }\left(0\right).$

Moreover, if $T=\infty$ , we have

$\underset{t\to \infty }{\lim \sup }{h}_{\alpha ,\beta }\left(t\right)\le {\kappa }_{\infty },$ (10)

where ${\kappa }_{\infty }$ is the maximal root of the algebraic equation

$x-G_{\infty }\left(\zeta \right)x^{\delta }=0.$

Proof.

${\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)\le -\theta h_{\alpha ,\beta }+\zeta h_{\alpha ,\beta }^{\delta }$

${\stackrel{\dot{}}{h}}_{\alpha \mathrm{,}\beta }\left(t\right)+\theta h_{\alpha \mathrm{,}\beta }\le \zeta h_{\alpha \mathrm{,}\beta }^{\delta }$

${\text{e}}^{\theta t}\left[{\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)+\theta h_{\alpha ,\beta }\right]\le {\text{e}}^{\theta t}\zeta h_{\alpha ,\beta }^{\delta }$

$\frac{\text{d}}{\text{d}t}\left[{\text{e}}^{\theta t}{h}_{\alpha ,\beta }\right]\le \zeta {\text{e}}^{\theta t}{h}_{\alpha ,\beta }^{\delta }$

${\displaystyle {\int }_0^t}\frac{\text{d}}{\text{d}t}\left[{\text{e}}^{\theta \chi }{h}_{\alpha ,\beta }\right]\text{d}\chi \le {\displaystyle {\int }_0^t}{\text{e}}^{\theta \chi }\zeta \left(\chi \right)h_{\alpha ,\beta }^{\delta }\left(\chi \right)\text{d}\chi$

${\text{e}}^{\theta t}{h}_{\alpha ,\beta }\left(t\right)-h_{\alpha ,\beta }\left(0\right)\le {\displaystyle {\int }_0^t}{\text{e}}^{\theta \chi }\zeta \left(\chi \right)h_{\alpha ,\beta }^{\delta }\left(\chi \right)\text{d}\chi$

${\text{e}}^{\theta t}{h}_{\alpha ,\beta }\left(t\right)\le h_{\alpha ,\beta }\left(0\right)+{\displaystyle {\int }_0^t}{\text{e}}^{\theta \chi }\zeta \left(\chi \right)h_{\alpha ,\beta }^{\delta }\left(\chi \right)\text{d}\chi$

$h_{\alpha ,\beta }\left(t\right)\le {\text{e}}^{-\theta t}{h}_{\alpha ,\beta }\left(0\right)+{\displaystyle {\int }_0^t}{\text{e}}^{-\theta \left(t-\chi \right)}\zeta \left(\chi \right)h_{\alpha ,\beta }^{\delta }\left(\chi \right)\text{d}\chi .$ (11)

Let

$\overline{h_{\alpha ,\beta }}\left(t\right)=\underset{0<\chi <t}{\sup }{h}_{\alpha ,\beta }\left(\chi \right),$

and

$G\left(\zeta \right):=\underset{0<t<T}{\sup }{\displaystyle {\int }_0^t}{\text{e}}^{-\theta \left(t-\chi \right)}\zeta \left(\chi \right)\text{d}\chi$

in particular, at $T=\infty$

$G_{\infty }\left(\zeta \right):=\underset{t\to \infty }{\lim \sup }{\displaystyle {\int }_0^t}{\text{e}}^{-\theta \left(t-\chi \right)}\zeta \left(\chi \right)\text{d}\chi$

we obtain now that

$\overline{h_{\alpha ,\beta }}\left(t\right)\le h_{\alpha ,\beta }\left(0\right)+G\left(\zeta \right)\overline{h_{\alpha ,\beta }^{\delta }}\left(t\right)$ (12)

Notice that the quantity $G\left(\zeta \right)$ is finite and hence (9) follows from (12). As $t\to \infty$ in (11), we ascertain

$\underset{t\to \infty }{\lim \sup }{h}_{\alpha ,\beta }\left(t\right)\le G_{\infty }\left(\zeta \right)\underset{t\to \infty }{\lim \sup }{h}_{\alpha ,\beta }^{\delta }\left(t\right)$

thus (10) follows since $G_{\infty }\left(\zeta \right)$ is finite. □

The next Lemma follows after applying Lemma 3 to (5).

Lemma 4. For any $\alpha ,\beta >0$ such that $\beta <\tau \alpha$ , and all conditions in Lemma 2 hold true. Then there exists a constant $C\left(T\right)=C_{\alpha ,\beta }\left(T\right)\le \infty$ such that

$h_{\alpha \mathrm{,}\beta }\left(t\right)\le C\left(T\right)$ (13)

for all $t\in \left[\mathrm{0,}T\right)$ .

Proof. For sufficiently small $\beta >0$ , such that $\beta <\tau \alpha$ with $\alpha >1$ , we obtain

$2ϵ\sqrt{\tau D\left(\alpha -1\right)\left(\beta +1\right)}\ge \left(\tau {ϵ}^2+D\right)\sqrt{\alpha \beta },\frac{\beta }{\tau }-\alpha <0,$

therefore we deduce from Lemma 2 that $h_{\alpha \mathrm{,}\beta }$ satisfies

${\stackrel{\dot{}}{h}}_{\alpha ,\beta }\left(t\right)\le \left(\frac{\beta }{\tau }-\alpha \right)h_{\alpha ,\beta }+C{u}^{-\delta }{h}_{\alpha ,\beta }^{1-\vartheta }.$

Since

$\frac{\beta }{\tau }-\alpha <0$

and

$u\left(t\right)\ge u\left(0\right){\text{e}}^{-\frac{t}{\tau }}$

for all $t\in \left[\mathrm{0,}T\right)$ , then from Lemma 3, (13) is true for $\alpha >1$ and sufficiently small $\beta$ such that $\beta <\tau \alpha$ . Since H is bounded away from zero, then (13) is true for any $\alpha ,\beta >0$ . □

From Lemma 1 and Lemma 4, we deduce the Corollary below.

Corollary 1. Let $\mathcal{l}\ge 1$ and all other assumptions in Theorem 1, Lemma 2, Lemma 3, and Lemma 4 hold true. Define

$g_1\left(A,H\right)=\frac{A^p}{H^q+b}$

$g_2\left(A,H\right)=\frac{A^r}{H^s}$

then there exist positive constant $C_{\mathcal{l}}\left(T\right)$ , such that

${\Vert g_j\left(A,H\right)\Vert }_{L^{\mathcal{l}}\left(\Omega \right)}\le C_{\mathcal{l}}\left(T\right),j=1,2$

for all $0\le t<T$ .

Proof. The proof to this Corollary follows from Lemma 3 and Lemma 4. □

3. Conclusion

In this paper, we have studied the Gierer-Meinhardt system with Robin boundary conditions and Neumann boundary conditions on the activator and inhibitor respectively. Global existence of solutions have been obtained under the mixed boundary conditions using a priori estimates of solutions.

Cite this paper

Antwi-Fordjour, K. and Nkashama, M. (2017) Global Existence of Solutions of the Gierer-Meinhardt System with Mixed Boundary Conditions. Applied Mathematics, 8, 857-867. https://doi.org/10.4236/am.2017.86067

References