Existence of positive periodic solution of n-dimensional Lotka–Volterra system with delays

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Abstract

With the help of a continuation theorem based on coincidence degree, easily verifiable criteria are established for the existence of positive periodic solutions of n-D Lotka–Volterra system with delays. And sufficient conditions are obtained for the persistence of the delay system. Finally, computer simulations are presented to illustrate the conclusions.

Introduction

Recently, more and more researchers have been studying the periodic solution of Lotka–Volterra system with delay owing to the application of the functional differential equation theory in math-biology and they obtained some results [1], [2], [3], [4], [5], [6], [7], [8], [9], [10], [11]. Wright [1] and Kuang [2], respectively, researched into the single population differential models with delays and acquired the sufficient conditions of global asymptotic stability of a positive equilibrium point. Goh [3] considered the sufficient condition of the global stability of a positive equilibrium point about the 2-D non-autonomous facultative mutualism system with delay. And the others, like Gopalsamy and He [4], he considered the sufficient condition of the global attractability of a positive equilibrium point about the 2-D autonomous facultative mutualism system with delay. Mukherjee [5] studied the persistence and global attractability of the 2-D autonomous facultative mutualism system with multiple delays. Lately, the persistence, boundedness and global attractability of a positive equilibrium point of the non-autonomous facultative mutualism system with multiple delays has been studied by Yang and Jiang [6]. Also Yang et al. [7] considered the existence of periodic positive solution of the non-autonomous facultative mutualism system with multiple delays, and Wang and Wang [8] discussed the existence of periodic positive solution of 2-D Lotka–Volterra system with multiple delays.

However, the variation of the environment plays an important role in many biological and ecological systems. In particular, the effects of a periodically varying environment are important for evolutionary theory as the selective forces on systems in a fluctuating environment differ from those in a stable environment. Thus, the assumption of periodicity of the parameters in a way incorporates the periodicity of the environment (e.g. seasonal effects of weather condition, food supplies, temperature, mating habits, harvesting etc.). In view of this, it is realistic to assume that the parameters in the models are periodic functions of period ω. Therefore, we discuss the following ns-D non-autonomous Lotka–Volterra system with multiple delays,xi(t)=xi(t)ri(t)-aii(t)xi(t-τii(t))+j=1jinaij(t)xj(t-τij(t)),i=1,2,,n,where xi(t) = φi(t)  0, t  [−τ, 0], τ = maxi,j=1,2,…,n{supt∈[0,ω]τij(t)}, φi  C([−τ, 0], R+), φi(0) > 0 and ri(t), aij(t), τij(t) are rigorous positive ω-periodic continuous bounded functions in R+.

The main purpose of this paper is to derive a set of easily verifiable sufficient conditions for the existence of positive periodic solution of (1), and the conditions of persistence. The method used here will be the coincidence degree theory developed by Gaines and Mawhin [12].

Definition 1

x(t) is said to be a positive solution of system (1) if x(t)=(x1(t),x2(t),,xn(t))T>0 in R+.

Lemma 1

The domain R+n={(x1,x2,,xn)T|xi>0,i=1,2,,n} is invariant with respect to (1).

In order to obtain the existence of a positive periodic solution of the system, we first make the following preparations.

Let X, Z be two real Banach space, Consider an operator equationLx=λNx,λ(0,1),where L : DomL  X  Z is a linear operator and λ is a parameter. Let P and Q denote two projectors such thatP:XDomLKerL,Q:ZZ/ImL.Denote by J : ImQ  KerL is an isomorphism of ImQ onto KerL. Recall that a linear operator L:DomL  X  Z with KerL = L−1(0) and ImL = L(DomL), will be called a Fredholm operator if the following two conditions hold: (I) KerL has a finite dimension; (II) ImL is closed and has a finite codimension.

We shall say that a mapping N is L compact on Ω if the mapping QN:Ω¯Z is continuous, QN(Ω¯) is bounded, and Kp(I-Q)N:Ω¯X is compact, i.e., it is continuous and Kp(I-Q)N(Ω¯) is relatively compact, where Kp : ImL  DomL  KerP is an inverse of the restriction Lp of L to DomL  KerP, so that LKp = I and KpL = I  P. In the sequel, we will use the following result of continuation theorem [12].

Lemma 2 Continuation Theorem

Let X, Z be two real Banach spaces and L a Fredholm mapping of index zero. Assume that N:Ω¯Z is L compact on Ω¯ with Ω open bounded in X. Furthermore suppose,

  • (a)

    for each λ  (0, 1), every solution x of Lx  λNx is such that x  DomL  ∂Ω;

  • (b)

    QNx  0 for each x  KerL  ∂Ω and Brouwer–Degree,deg{JQNx,ΩKerL,0}0.

Then operator equation Lx = Nx has at least one solution in DomLΩ¯.

Section snippets

Existence of positive periodic solution

Theorem 1

If system (1) satisfies the following conditions,

  • (a)

    aij=aij(ηij)1-τij(ηij),ηij=τij(ξij)[0,ω],ξij[-τij(0),ω-τij(0)],-a11a12a1na21-a22a2nan1an2-ann0;

  • (b)

    aijL=mint[0,ω]aij(t)1-τij(t),aijM=maxt[0,ω]aij(t)1-τij(t),ri¯=1ω0ωri(t)dt,τij(t)<1(i,j=1,2,,n);

  • (c)

    a11L-a12M-a1nM-a21Ma22L-a2nM-an1M-an2MannL is an M matrix [13], and |Ai|=a11Lr1¯-a1nM-a21Mr2¯-a2nM-an1Mrn¯annL>0.

Then (1) has at least one ω-periodic positive solution x(t).

Proof

Since the system (1) is equal to the following

Persistence of system

Definition 2

The system (1) is said to be persistent if every positive solution {(x1(t), x2(t),  , xn(t))T} satisfies limt→∞ inf xi(t) > 0. Furthermore, if there exist a constant mi > 0, such that limt→∞ inf xi(t)  mi > 0 (i = 1, 2,  , n), the system (1) is called uniform persistence.

Definition 3

The system (1) is said to be uniform persistent subsistent if there exist positive constants m, M, such thatMlimtsupxi(t)limtinfxi(t)mfor any positive solution {(x1(t), x2(t), …, xn(t))T} of system (1).

Theorem 2

Let (x1(t), x2(t),  , xn(t))T denote any

Numerical experiments

Consider the following systemsx1(t)=x1(t)[(1+0.5sint)-10x1(t-0.1esint)+(2+sint)x2(t-0.1ecost)],x2(t)=x2(t)[(1+0.5cost)+(2+cost)x1(t-0.1esint)-20x2(t-0.1ecost)]andx1(t)=x1(t)(1+0.5sint)-10x1(t-0.1esint)+(2+sint)x2(t-0.1ecost)+(2-cost)x3(t-0.0333esin2t),x2(t)=x2(t)(1+0.5cost)+(2+cost)x1(t-0.1esint)-20x2(t-0.1ecost)+(2+sint)x3(t-0.0333esin2t),x3(t)=x3(t)(1-0.5sint)+(2-cost)x1(t-0.1esint)+(2+sint)x2(t-0.1ecost)-30x3(t-0.0333esin2t).According to Theorem 1, we can obtain the positive periodic

Conclusion

In this paper, the existence of positive periodic solution and the persistence of a n-dimensional Lotka–Volterra system with delays are discussed. And we obtained the corresponding sufficient conditions of the existence of periodic solution of the system. At the same time, we give a theorem of the uniform persistence of this system. However, there are still many interesting and challenging mathematical question needing to be studied for system (1), for example, we do not discuss the

Acknowledgements

The authors are grateful to the referee for his/her helpful comments. This work was supported by the Research Foundation of Xijing University under Grant 100106.

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