# A Delayed Chemostat Model with Impulsive Diffusion and Input on Nutrients

- Jianjun Jiao
^{1}Email author and - Shaohong Cai
^{1}

**2009**:514240

**DOI: **10.1155/2009/514240

© J. Jiao and S. Cai. 2009

**Received: **21 August 2009

**Accepted: **30 November 2009

**Published: **10 January 2010

## Abstract

A chemostat model with delayed response in growth and impulsive diffusion and input on nutrients is considered. Using the discrete dynamical system determined by the stroboscopic map, we obtain a microorganism-extinction periodic solution. Further, it is globally attractive. The permanent condition of the investigated system is also obtained by the theory on impulsive delay differential equation. Finally, numerical analysis is inserted to illustrate dynamical behaviors of the chemostat system. Our results reveal that the impulsive input amount of nutrients plays an important role on the outcome of the chemostat. Our results provide strategy basis for biochemical reaction management.

## 1. Introduction

The theory of impulsive differential equation appears as a natural description of several real processes subject to certain perturbations whose duration is negligible in comparison with the duration of the process. Recently, equations of this kind are found in almost every domain of applied science. Many examples are given in [1]. Some impulsive differential equations have been recently introduced in population dynamics[2–7], pulse vaccination [8–11], and chemostat dynamics [12–15].

The chemostat is a basic piece of laboratory apparatus. The advantages are that certain of the biological parameters assumed to influence the outcomes can be controlled by the experimenters. The chemostat plays an important role in bioprocessing, such as ecology, microbiology, chemical engineering, and so forth. Smith and Waltman had made discussion about the chemostat model in [16]. The models contain discrete time delays which account for time which laps between uptaked of nutrient and the assimilation of nutrient into viable biomass. Smith, Waltman [17] and Kuang [18] discussed various aspects of models with discrete time delay. Freedman, So, and Waltman[19] were the first to incorporate time delay in chemostat models. Ellermeyer [20], Hsu et al. [21, 22], analyzed a discrete time delay model with two competitive microorganisms for a single nutrient in a chemostat. Hale, Somolinos [23] Hsu et al. [24], Wolkowicz, Zhao [25] investigated competition in chemostat. Ellermeyer et al. [26] did a theoretical and empirical investigation of delayed growth response in the continuous culture of bacteria. Delays occur naturally in biological system by two obvious sources of delays: delays due to the cell cycle; and delays due to the possibility the organism stores the nutrient. Delays appear in a chemostat model in Bush and Cook [27]. They have investigated a model of growth of one organism in the chemostat with a delay in the intrinsic growth rate of the microorganism but with no delay in the substrate equation.

In chemostat's simplest form, the system approximates conditions for plankton growth in lakes, where the limiting nutrients such as silica and phosphate are supplied from streams draining the watershed. In the lakes, the plankton population movements are subject to many factors, such as currents and turbulent lateral diffusion (cf. Levin and Segel [28], Mimura [29], Okubo [30], Freedman and Ruan [31]). Ruan [32] proposed a diffusive plankton-nutrient interaction model with delayed nutrient recycling and delayed growth response and studied Turing instability and the existence of travelling wave solutions. However, they did not investigate a chemostat model with delayed response in growth and impulsive diffusion on nutrients. Many researchers indicated that it was important to consider models with periodic perturbations, since these models may be quite naturally exposed in many real world phenomena, for instance, food supply, mating habits, cross flooding in rainstorm season. In fact, the perturbations such as cross flooding in rainstorm which are not suitable to be considered with continuity. These perturbations bring sudden changes to the system. Systems with sudden perturbations are involving an impulsive differential equations which have been studied intensively and systematically in [1, 2]. There are few papers [8, 12, 33, 34] research the chemostat model with impulsive perturbations on nutrients. In this paper, a chemostat model with delayed response in growth and impulsive diffusion on nutrients is investigated, we will obtain a microorganism-extinction periodic solution. Further, it is globally attractive. The permanent condition of the investigated system is also obtained.

The organizations of the paper are as following. In Section 2, we introduce a chemostat model with delayed response in growth and impulsive diffusion on nutrients. In Section 3, we present some preliminary results about the investigated model. Our main results are stated and proven in Section 4. Finally, the numerical analysis is inserted to illustrate the results, and conclude with a brief discussion in Section 5.

## 2. The Model

We investigate the following chemostat model with delayed response in growth and impulsive diffusion on nutrients:

where we suppose that the system is composed of two lakes connected by impulsive diffusion. denotes the concentration of the nutrient in th lake at time ( ). denotes the input nutrient concentration in th lake ( ). denotes the input rate from the lakes containing the substrate and the wash-out rate of substrate and microorganism by products from Lake . is diffusive rate between Lake and Lake . It is assumed here that the net exchange from patch to Lake is proportional to the difference of concentration of the nutrient. denotes the concentration of the the microorganism in the second lake at time . stands for the time delay in conversion of nutrient to biomass for the microorganism. As discussed in [20, 32], represents the biomass of those microorganisms that consume nutrient units of time prior to time and that survive in the chemostat the units of time necessary to complete the nutrient conversion process. indicates the consumption rate of nutrient by the microorganism. It is assumed that and . In particular, these hypotheses are satisfied by the Michaelis-Menten function here is the half-saturation constant or Michaelis-Menten constant. The impulsive diffusion occurs every period ( ), the system evolves from its initial state without being further affected by diffusion until the next pulse appears. and represents the concentration of the plankton in the th lake immediately after the th diffusion pulse at time , while represents the concentration of the microorganism in the th lake before the th diffusion pulse at time , . is the amount of the substrate concentration pulse at , in first lake. The purpose of this paper is to prove that the system (2.1) has a microorganism-extinction periodic solution, further, it is globally attractive, and also prove system (2.1) is permanent.

## 3. The Lemmas

The solution of (2.1), denoted by , is a piecewise continuous function : . is continuous on , and exists. Obviously the global existence and uniqueness of solutions of (2.1) is guaranteed by the smoothness properties of , which denotes the mapping defined by right-side of system (2.1) [1]. Before having the main results. we need some lemmas which will be used in the next.

According to the biological meanings, it is assumed that and . Now, we will show that all solutions of (2.1) are uniformly ultimately bounded.

Lemma.

There exists a constant such that for each solution of (2.1) with all large enough.

Proof.

So is uniformly ultimately bounded. Hence, by the definition of , there exists a constant such that for all large enough. The proof is complete.

If , the subsystem of (2.1) is written as

Integrating and solving the first two equations of system (3.3) between pulses, we have

Considering the last two equations of system (3.3), we have the stroboscopic map of system (3.3) as follows:

Equation (3.5) are difference equations. They describe the the concentration of the nutrients in the two lakes at a pulse in terms of values at the previous pulse. The dynamical behaviors of system (3.5) with equation (3.4) determine the dynamical behaviors of system (3.3). So we will devote to investigate system (3.5).

From system (3.5), we can easily have a unique fixed point of system (3.5) as follows

To write system (3.5) as a map, we define the map :

is the map evaluated at the point . Consequently, in system (3.4), describes the concentration of the nutrients in the time .

Doing similarly to [3, Lemma and Theorem ], and using iterative method, one can easily obtain Lemma 3.2 as follows:

Lemma.

Remark.

Lemma (see [18]).

where ; for . If ,

## 4. Dynamical Behaviors of (2.1)

From the above discussion, we know that there exists a microorganism-extinction boundary periodic solution of system (2.1). In this section, we will prove that the microorganism-extinction boundary periodic solution of system (2.1) is globally attractive.

Theorem.

holds, then the microorganism-extinction periodic solution of system (2.1) is globally attractive.

Proof.

we have . According to Lemma 3.4, we have .

Let be the solution of system (2.1) with initial conditions and , is the solution of system (4.10) with initial conditions . By the comparison theorem, we have

Incorporating into the positivity of , we know that Therefore, for any (sufficiently small), there exists an integer such that for all .

For system (2.1), we have

where denotes Therefore, for any . there exists a integer such that , Let , so we have , for large enough, which implies as . This completes the proof.

Definition 4.2.

System (2.1) is said to be permanent, if there are constants (independent of initial value) and a finite time such that for all solutions with all initial values , , , , , holds for all . Here may depend on the initial values .

Theorem.

Proof.

This is a contradiction. Thus, for all . As a consequence, Then for all . This implies that as , . It is a contradiction to . Hence, the claim is complete.

By the claim, we are left to consider two case. First, for all large enough. Second, oscillates about for large enough.

Define

where . We hope to show that for all large enough. The conclusion is evident in first case. For the second case, let and satisfy and for all where is sufficiently large such that for , is uniformly continuous. The positive solutions of (2.1) are ultimately bounded and is not affected by impulses. Hence, there is a and is dependent of the choice of such that for . If , there is nothing to prove. Let us consider the case . Since and , it is clear that for . Then, proceeding exactly as the proof for the above claim. We see that for . Because the kind of interval is chosen in an arbitrary way (we only need to be large). We conclude for all large . In the second case. In view of above discussion, the choice of is independent of the positive solution, and we proved that any positive solution of (2.1) satisfies for all sufficiently large . This completes the proof of the theorem.

Theorem 4.4.

then system (2.1) is permanent.

We can easily complete the proof of Theorem 4.4 by referring to Lemma 3.1, Theorems 4.1 and 4.3.

## 5. Discussion

## Declarations

### Acknowledgments

This work was supported by National Natural Science Foundation of China (10961008), the Nomarch Foundation of Guizhou Province (2008035), the Science Technology Foundation of Guizhou (2008J2250), the Science Technology Foundation of Guizhou Education Department (2008038), and the National Key Technology R&D Program of China (2006BAC01A09).

## Authors’ Affiliations

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