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Abstract and Applied Analysis
Volume 2013 (2013), Article ID 939405, 9 pages
Global Solutions for an -Component System of Activator-Inhibitor Type
1Department of Mathematics, College of Sciences, Taibah University, Yanbu, Saudi Arabia
2Department of Mathematics, University of Tebessa, 12002 Tebessa, Algeria
3Department of Mathematics, University of Batna, 05000 Batna, Algeria
Received 15 May 2013; Accepted 17 July 2013
Academic Editor: Khalil Ezzinbi
Copyright © 2013 S. Abdelmalek et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
This paper deals with a reaction-diffusion system with fractional reactions modeling -substances into interaction following activator-inhibitor's scheme. The existence of global solutions is obtained via a judicious Lyapunov functional that generalizes the one introduced by Masuda and Takahashi.
In this paper, we are concerned with the existence of global solutions to a reaction-diffusion system with components generalizing the activator-inhibitor system: supplemented with Neumann boundary conditions and the positive initial data
Here , is an open bounded domain of class in , with boundary , and denotes the outward normal derivative on .
Throughout the paper, we make the following hypotheses:
The indexes , are nonnegative for all , with : we set for all . Let , be positive constants such that where where stands for the determinant of the -square symmetric matrix obtained from the matrix by removing the rows and the columns, where are the minors of the matrix . The elements of the matrix are as follows:
The main result of the paper is the following.
Theorem 1. Assume that condition (4) is satisfied. Let be a solution of (1)–(3) with positive and bounded initial data, and let Then the functional is uniformly bounded on the interval , , where denotes the eventual blow-up time.
Before we prove our results, let us dwell a while on the existing literature concerning Gierer-Meinhardt's type systems.
In 1972, following an ingenious idea of Turing , Gierer and Meinhardt  proposed a mathematical model for pattern formations of spatial tissue structures of hydra in morphogenesis. It is a system of reaction-diffusion equations of the form: with Neumann boundary conditions and initial conditions where ( in practice) is a bounded domain with smooth boundary , and , , and are non negative windexes with . Here is the activator, and is the inhibitor.
Global existence of solutions in was proved by Rothe , more than ten years after Gierer and Meinhardt's original paper with special choice of the parameters: , , , , and . Masuda and Takahashi  were able to prove global estimates and bounds of the solution for Gierer and Meinhardt's system in its general form. They proceeded by first proving lower bounds, then bounds (for any ), then uniform estimates and bounds in appropriate Sobolev spaces. The key point is represented by the bounds, which are derived using in a subtle way the specific structure of the equations.
Li et al.  also studied the activator-inhibitor model.
Very recently, Bernasconi  considered the larger system: and Meinhardt et al.  proposed activator-inhibitor models to describe a theory of biological pattern: which is Gierer and Meinhardt's system supplemented with a third equation, where is the activator, is the inhibitor, and is a source that acts as an inhomogeneous inhibitor.
Our paper generalizes the system in  to -components.
2. Preliminary Observations and Notations
The usual norms in the spaces , , and are denoted, respectively, by the following:
Our aim is to construct a Lyapunov functional that allows us to obtain -bounds on leading to global existence.
3. Preparatory Lemmas
For the proof of Theorem 1, we need some preparatory lemmas whose proofs will be in the appendix.
Lemma 3. Assume that the constants satisfy Then for all , , there exist and , such that , , , .
Lemma 4 (see ). Let . Then one has: where
Lemma 5. Let . One has where
Lemma 6 (see Masuda and Takahashi ). Let and let be a nonnegative integrable function on and (). Let be a positive function on satisfying the differential inequality Then, one has where is the maximal root of the algebraic equation:
Proof of Theorem 1. Since satisfies on , the maximum principle implies .
Differentiating with respect to yields Replacing , , by its expression from (1), we get where we have set Estimation of . We are going to show that .
Using Green's formula, we obtain where is defined in (8) and
The matrix is positive definite if and only if all its associated minor matrices are positive. To see this, we have the following.(1). Using (5), we get .(2) According to Lemma 4, we have Using (6) and (24) for , we get .(3) Again according to Lemma 4, we have But , thus . Using (6) and (24) for , we get .(4) We suppose that , and prove that ; thus
From Lemma 4,
This along with (37) yields But from (6) and (24) ; thus .
Consequently, we have .
Estimation of . We are going to estimate by a function of .
According to the maximum principle, there exists depending on , , such that , . We then have whereupon We have Using Lemma 3, we obtain Applying Hölder's inequality, we obtain So Also, we have So We then get which implies This yields the differential inequality: Thus under conditions (5), (6), and (8), we obtain ; using Lemma 6 we deduce that is bounded on ; that is, , where depends on , .
Proof of Corollary 2 (-bounds). By Theorem 1, we have , for all . By a simple argument relying on the variation-of-constants formula and the --estimate (Proposition 48.4 see ), we deduce that is uniformly bounded. Consequently, .
Proof of Lemma 4. We prove this lemma by induction.
For , we have .
We consider the case .
By using the well-known Dodgson condensation  for the symmetric -square matrix: But So Hence by using formula (20), formula (19) is correct for .
When , we suppose that formula (19) is correct for , and we prove it for .
It is sufficient to prove that By putting in formula (21), we get From the mathematical induction proof, we have By putting in formula (20), we get By replacing (A.9), (A.10), and (A.11) in (A.12), we obtain and thus formula (19) is correct for .
Now, we prove formula (A.9); we may generalize formula (A.9) as follows: Also, we prove formula (A.14) by induction. It is a second inductive proof included in the first one.
It is evident for .
For , formula (20) will be: Since we already know that simple substitution of these three formulas in the formula (A.15) followed by the application of the modified well-known Dodgson condensation which has been modified in  will lead to formula (A.14) for . directly.
When , we suppose that formula (A.14) is correct for , and we prove it for .
Formula (20) for reads
According to the first induction, we have According to the second induction, we have According to formula (21), we have: By replacing (A.18), (A.19), and (A.20) in (A.17) and by using the well-known Dodgson condensation, we obtain formula (A.14) for . Therefore, the second inductive proof is finished and consequently the first one.
Proof of Lemma 5. We prove this lemma by induction:
For , we have Because
Assuming , we suppose (24) is true for , and we prove it for . Hence, we aim to prove
Recall that It is then sufficient to prove which will satisfy the inequality
In order to prove (A.26), we first generalize it in the form This can be proven by mathematical induction. It is a secondary inductive proof inside the primary one. For , it is evident that For , the formula is evident too.
When , we suppose formula (A.28) true for : and we prove it for :
Accordingly, we have This finishes the proof.
The authors would like to express their deepest gratitude for Professor KIRANE (Université de la Rochelle, France) for all his valuable input and guidance throughout the research and authoring of this paper.
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