(ProQuest: ... denotes non-US-ASCII text omitted.)
Yang Gao 1,2 and Shengqiang Liu 1
Academic Editor:Weiming Wang
1, Academy of Fundamental and Interdisciplinary Science, Harbin Institute of Technology, Harbin 150080, China
2, Department of Mathematics, Daqing Normal University, Daqing, Heilongjiang 163712, China
Received 19 January 2014; Accepted 6 February 2014; 12 March 2014
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.
1. Introduction
In the literature of predator-prey population systems, both continuous reaction-diffusion systems and discrete patchy models are used to study the spatial heterogeneity [1, 2]; patchy models are often used to describe directed movement of population among niches or migration among habitats. It is naturally interesting problem to consider how the dispersal or migration of predator and prey influences the global dynamics of the interacting ecological system; thus patchy predator-prey model received lots of attentions [1, 3-6].
Since the discrete patchy models usually involve high-dimensional system, it is rather mathematically challenging to study the uniqueness and stability of the positive equilibrium of the predator-prey patchy models, and the available global dynamics criteria in the literatures mainly focus on the special case of two-patch [3] or on the permanence and existence of periodic solutions [4-6].
Recently, Li and Shuai [7] considered the following predator-prey model with dispersal for prey among n -patch: [figure omitted; refer to PDF] Here, xi , yi denote the densities of prey and predators on the patch i , respectively. The parameters ri , bi and γi , δi in the model are nonnegative constants. What is more, the parameters ei and [straight epsilon]i in the model are positive constants. Constant dijx is the dispersal rate of the prey from patch j to patch i and constants αijx can be selected to represent different boundary conditions in the continuous diffusion case.
In [7], the authors studied the global stability of the coexistence equilibrium of system (1), by considering (1) as a coupled n predator-prey submodels on networks. Using results from graph theory and a developed systematic approach that allows one to construct global Lyapunov functions for large-scale coupled systems from building blocks of individual vertex systems, Li and Shuai [7] obtain the following sharp results for (1).
Proposition 1 (see [7, Theorem 6.1]).
Assume that (dijx)n×n is irreducible. If there exists k such that bk >0 or δk >0 , then, whenever a positive equilibrium E* exists in (1), it is unique and globally asymptotically stable in the positive cone R2n+ .
Although well-improved results have been seen in the above work on dispersal predator-prey model, such models are not well studied yet in the sense that model (1) assumes no dispersal for predator, which is not realistic in many cases [1, 3]. Thus it is interesting for us to consider the global stability of the positive equilibrium for predator-prey model with dispersal for both predator and prey.
Motivated by the above work in [7], in this paper we generalize model (1) into the following predator-prey model with dispersal for both predator and prey: [figure omitted; refer to PDF] Here, the parameters ri , bi , ei , γi , δi , and [straight epsilon]i are defined the same as those in (1). The nonnegative constants dijy , αijy , and dijy are the dispersal rate of the predators from patch j to patch i , and αijy represents the different boundary conditions in the continuous diffusion case. Clearly, when dijy =0 for all i,j=1,...,n , model (2) directly reduces to (1); thus our model (2) directly extends model (1) in [7].
The main purpose of this paper is to obtain the global stability for the coexistence equilibrium of (2). We will engage the techniques of constructing Lyapunov function based on graph-theory which were well developed by Li et al. in [7-9]; we refer to [10-12] for recent applications. Our study seems to be the first attempt in applying the network method for coupled network systems of differential equations to address the predator-prey system with dispersal for both predator and prey among patches. Networked method has been extensively investigated in the several fields. For example, multiagent systems can be seen as complicated network systems. A lot of researchers take their interest in flocking and consensus of the multiagent systems [13-17]. What is more, neural network systems can be seen as complicated network systems. Over the past few decades, various neural network models have been extensively investigated [18-20].
A mathematical description of a network is a directed graph consisting of vertices and directed arcs connecting them. At each vertex, the local dynamics are given by a system of differential equations called the vertex system. The directed arcs indicate interconnections and interactions among vertex systems.
A digraph G with n vertices for the system (2) can be constructed as follows. Each vertex represents a patch and (j,i)∈E(G) if and only if dijx ,dijy >0 . At each vertex of G , the vertex dynamics is described by a predator-prey system. The coupling among these predator-prey systems is provided by dispersal of predator and prey among patches.
This paper is organized as follows. In the next section, we introduce preliminaries results on graph-theory based on coupled network models. In Section 3, we obtain the main result of system (2). This is followed by a brief conclusion section.
2. Preliminaries
In this section, we will list some definitions and Theorems that we will use in the later sections.
A directed graph or digraph G=(V,E) contains a set V={1,2,...,n} of vertices and a set E of arcs (i,j) leading from initial vertex i to terminal vertex j . A subgraph H of G is said to be spanning if H and G have the same vertex set. A digraph G is weighted if each arc (j,i) is assigned a positive weight. aij >0 if and only if there exists an arc from vertex j to vertex i in G .
The weight w(H) of a subgraph H is the product of the weights on all its arcs. A directed path P in G is a subgraph with distinct vertices i1 ,i2 ,...,im such that its set of arcs is {(ik ,ik+1 ):k=1,2,...,m} . If im =i1 , we call P a directed cycle.
A connected subgraph T is a tree if it contains no cycles, directed or undirected.
A tree T is rooted at vertex i , called the root, if i is not a terminal vertex of any arcs, and each of the remaining vertices is a terminal vertex of exactly one arc. A subgraph Q is unicyclic if it is a disjoint union of rooted trees whose roots form a directed cycle.
Given a weighted digraph G with n vertices, define the weight matrix A=(aij)n×n whose entry aij equals the weight of arc (j,i) if it exists, and 0 otherwise. For our purpose, we denote a weighted digraph as (G,A) . A digraph G is strongly connected if for any pair of distinct vertices, there exists a directed path from one to the other. A weighted digraph (G,A) is strongly connected if and only if the weight matrix A is irreducible.
The Laplacian matrix of (G,A) is denoted by L . Let ci denote the cofactor of the i th diagonal element of L . The following results are listed as follows from [7].
Proposition 2 (see [7]).
Assume n...5;2 . Then [figure omitted; refer to PDF] where Ti is the set of all spanning trees T of (G,A) that are rooted at vertex i , and w(T) is the weight of T . In particular, if (G,A) is strongly connected, then ci >0 for 1...4;i...4;n .
Theorem 3 (see [7]).
Assume n...5;2 . Let ci be given in Proposition 2. Then the following identity holds: [figure omitted; refer to PDF] where Fij (xi ,xj ) , 1...4;i , j...4;n , are arbitrary functions, Q is the set of all spanning unicyclic graphs of (G,A) , w(Q) is the weight of Q , and CQ denotes the directed cycle of Q .
Given a network represented by digraph G with n vertices, n...5;2 , a coupled system can be built on G by assigning each vertex its own internal dynamics and then coupling these vertex dynamics based on directed arcs in G . Assume that each vertex dynamics is described by a system of differential equations [figure omitted; refer to PDF] where ui ∈Rmi and fi :R×Rmi [arrow right]Rmi . Let gij :R×Rmi ×Rmj [arrow right]Rmi represent the influence of vertex j on vertex i , and let gij ...1;0 if there exists no arc from j to i in G . Then we obtain the following coupled system on graph G : [figure omitted; refer to PDF] Here functions fi , gij are such that initial-value problems have unique solutions.
We assume that each vertex system has a globally stable equilibrium and possesses a global Lyapunov function Vi .
Theorem 4 (see [7]).
Assume that the following assumptions are satisfied.
(1) There exist functions Vi (t,ui ) , Fij (t,ui ,uj ) and constants aij ...5;0 such that [figure omitted; refer to PDF]
(2) Along each directed cycle C of the weighted digraph (G,A) , A=(aij ) , [figure omitted; refer to PDF]
(3) Constants ci are given by the cofactor of the i th diagonal element of L .
Then the function V(t,u)=∑i=1n ...ciVi (t,ui ) satisfies V (t,u)...4;0 for t>0 , u∈D ; namely, V is a Lyapunov function for the system (6).
3. Main Results
In this section, the stability for the positive equilibrium of the n -patch predator-prey model (2) is considered. We regard (2) as a coupled system on a network. Using a Lyapunov function for the n -patch predator-prey model with dispersal and Theorem 4 of Section 2, we will establish that a positive equilibrium of the n -patch predator-prey model (2) with dispersal is globally asymptotically stable in R+2n as long as it exists.
First of all, we will give a lemma for the system (2).
Lemma 5.
The set R+2n is the positive invariant set for the system (2).
The next Theorem gives the globally asymptotically stable condition for the positive equilibrium of the system (2).
Theorem 6.
Assume that a positive equilibrium E* =(x1* ,y1* ,x2* ,y2* ,...,xn* ,yn* ) exists for the system (2) and the following assumptions hold.
(1) Dispersal matrixes (dijx)n×n , (dijy)n×n are irreducible; moreover there exists k such that bk >0 or δk >0 .
(2) There exists nonnegative constant λ such that λ·dijx[straight epsilon]ixj* =dijyeiyj* for 1...4;i , j...4;n , or dijx[straight epsilon]ixj* =λ·dijyeiyj* for 1...4;i , j...4;n .
Then, the positive equilibrium E* is unique and globally asymptotically stable in R+2n .
Proof.
Let [figure omitted; refer to PDF] In the sequel, we have [figure omitted; refer to PDF] Set Lyapunov functions as [figure omitted; refer to PDF] Direct differentiating Vi along the system (2), we have [figure omitted; refer to PDF] where [figure omitted; refer to PDF] Set aijx =dijx[straight epsilon]ixj* , bijy =dijyeiyj* ,A=(aijx)n×n , and B=(bijy)n×n . One has [figure omitted; refer to PDF]
Next, we have two cases to consider.
Case I. d i j x [straight epsilon] i x j * = λ · d i j y e i y j * for 1...4;i , j...4;n .
Case II. λ · d i j x [straight epsilon] i x j * = d i j y e i y j * for 1...4;i , j...4;n .
For Case I, from the fact that aijx =dijx[straight epsilon]ixj* and bijy =dijyeiyj* , we obtain that aijx =λbijy ; thus A=λ·B . Then we obtain that [figure omitted; refer to PDF] Let ciy denote the cofactor of the i th diagonal element of the matrix B . From the irreducible character of matrix B , we have ciy >0 .
Furthermore, set Lyapunov functions as [figure omitted; refer to PDF] Then differentiating V along the solution of the system (2), we obtain that [figure omitted; refer to PDF] Let G represent the directed graph associated with matrix B . Then G has vertices 1,2,...,n with a directed arc (k,j) from k to j if and only if bkjy ...0;0 . Then E(G) is the set of all directed arcs of G . By Kirchhoff's Matrix-Tree Theorem (see Proposition 2) we know that [upsilon]k =Ckk can be expressed as a sum of weights of all directed spanning subtrees T of G that are rooted at vertex k . Thus, each term in [upsilon]kakj is the weight ω(Q) of a unicyclic subgraph Q of G obtained from such a tree T by adding a directed arc (k,j) from the root k to vertex j . Because the arc (k,j) is a part of the unique cycle CQ of Q and that the same unicyclic graph Q can be formed when each arc of CQ is added to a corresponding rooted tree T , then the double sum can be expressed as a sum over all unicyclic subgraphs Q containing vertices 1,2,...,n . Therefore, following from the irreducible character of matrix B and Theorem 2.3 in [7], we obtain [figure omitted; refer to PDF] Combining with the fact that 1-a+ln...a...4;0 , therefore we have [figure omitted; refer to PDF] When we consider V (x,y)=0 , by condition 1, there exists k∈N+ such that [figure omitted; refer to PDF] It means that xk =xk* or yk =yk* .
If i and k can be connected with an arc from k to i in G , then we have aiky >0 and biky >0 . Furthermore, [figure omitted; refer to PDF] Because of 1-a+ln...a...4;0 and 1-a+ln...a=0,...a=0 . we deduce that [figure omitted; refer to PDF] From xk =xk* , or yk =yk* , we obtain that xi =xi* and yi /yi* =yk /yk* or yi =yi* and xi /xi* =xk /xk* .
By condition 1 and the definition of matrixes A , B , we get that B are irreducible. By strong connectivity of G , there exists a directed path P from any i to k . Then we have that, for any i=1,2,...,n , there must be [figure omitted; refer to PDF] or for any i=1,2,...,n , there must be [figure omitted; refer to PDF] Next, we will prove that the largest compact invariant subset of {(x,y)|"V (x,y)=0} is the singleton {E* } .
We only consider the case that [figure omitted; refer to PDF] The case that [figure omitted; refer to PDF] is similar to this case. So we omit it.
If μ=0 , we have yi =0 for any i=1,2,...,n , and then we have [figure omitted; refer to PDF] which contradicts to the fact that [figure omitted; refer to PDF]
If μ>0 and μ...0;1 , we have yi =μyi* for any i=1,2,...,n , and then we have [figure omitted; refer to PDF] which also contradicts to the fact that [figure omitted; refer to PDF] Therefore, we obtain that μ=1 , which means [figure omitted; refer to PDF] Namely, we get that the largest compact invariant subset of {(x,y)|"V (x,y)=0} is the singleton {E* } . Therefore, by the LaSalle Invariance Principle ([21]), E* is globally asymptotically stable in R+2n .
With the similar arguments to the Case I, we can prove that E* is globally asymptotically stable in R+2n for Case II. This completes the proof.
Remark 7.
Theorem 6 is applicable to model (1): consider model (2) with dijy =0 , i,j=1,...,n , and let λ=0 ; thus Theorem 6 directly reduces to Proposition 1 by Li and Shuai [7] for (1).
By Theorem 6 and similar arguments to Remark 7, we directly have the following global stability theorem for the predator-prey model with discrete dispersal of predator among patches.
Corollary 8.
Consider the model [figure omitted; refer to PDF] Assume that the matrix (dijy)n×n is irreducible. If there exists k such that bk >0 or δk >0 ; then, whenever a positive equilibrium E* exists in (32), it is unique and globally asymptotically stable in the positive cone R+2n .
4. Discussion
In this paper, we generalize the model of the n -patch predator-prey model of [7] to the general model (2) that both the prey and the predator have dispersal among n -patches. Based on the network method for coupled systems of differential equations developed in [7-9], we prove that the positive equilibrium of (2) is globally asymptotically stable given some conditions on the coupling (see Theorem 6). Our main theorem generalizes Theorem 6.1 in [7] and our results also cover the other case of (2) in that only the predators disperse among patches.
Biologically, our result of Theorem 6 implies that if predator-prey system is dispersing among strongly connected patches (which is equivalent to the irreducibility of the dispersal matrixes of predator and prey) and if the system is permanent (which guarantees the existence of positive equilibrium), then the numbers of both predators and prey in each patches will eventually be stable at some corresponding positive values given the well-coupled dispersal (condition 2 of Theorem 6).
We remark that our Theorem 6 requires the extra condition 2 for the coupling dispersal coefficients and that the global dynamics for the coexistence equilibrium of (2) without condition 2 of Theorem 6 are still unclear. It remains an interesting future problem for the patchy dispersal predator-prey model.
Acknowledgments
The first author is supported by the Natural Science Foundation for Doctor of Daqing Normal University (no. 12ZR09). Shengqiang Liu is supported by the NNSF of China (no. 10601042), the Fundamental Research Funds for the Central Universities (no. HIT.NSRIF.2010052), and Program of Excellent Team in Harbin Institute of Technology.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
[1] H. I. Freedman, Y. Takeuchi, "Global stability and predator dynamics in a model of prey dispersal in a patchy environment," Nonlinear Analysis: Theory, Methods & Applications , vol. 13, no. 8, pp. 993-1002, 1989.
[2] J. D. Murry Mathematical Biology , vol. 1-2, Springer, New York, NY, USA, 2002.
[3] Y. Kuang, Y. Takeuchi, "Predator-prey dynamics in models of prey dispersal in two-patch environments," Mathematical Biosciences , vol. 120, no. 1, pp. 77-98, 1994.
[4] J. Cui, "The effect of dispersal on permanence in a predator-prey population growth model," Computers & Mathematics with Applications , vol. 44, no. 8-9, pp. 1085-1097, 2002.
[5] R. Xu, M. A. J. Chaplain, F. A. Davidson, "Periodic solutions for a delayed predator-prey model of prey dispersal in two-patch environments," Nonlinear Analysis: Real World Applications , vol. 5, no. 1, pp. 183-206, 2004.
[6] L. Zhang, Z. Teng, "Permanence for a delayed periodic predator-prey model with prey dispersal in multi-patches and predator density-independent," Journal of Mathematical Analysis and Applications , vol. 338, no. 1, pp. 175-193, 2008.
[7] M. Y. Li, Z. Shuai, "Global-stability problem for coupled systems of differential equations on networks," Journal of Differential Equations , vol. 248, no. 1, pp. 1-20, 2010.
[8] H. Guo, M. Y. Li, Z. Shuai, "A graph-theoretic approach to the method of global Lyapunov functions," Proceedings of the American Mathematical Society , vol. 136, no. 8, pp. 2793-2802, 2008.
[9] M. Y. Li, Z. Shuai, "Global stability of an epidemic model in a patchy environment," Canadian Applied Mathematics Quarterly , vol. 17, no. 1, pp. 175-187, 2009.
[10] H. Shu, D. Fan, J. Wei, "Global stability of multi-group SEIR epidemic models with distributed delays and nonlinear transmission," Nonlinear Analysis: Real World Applications , vol. 13, no. 4, pp. 1581-1592, 2012.
[11] R. Sun, J. Shi, "Global stability of multigroup epidemic model with group mixing and nonlinear incidence rates," Applied Mathematics and Computation , vol. 218, no. 2, pp. 280-286, 2011.
[12] J. Wang, J. Zu, X. Liu, G. Huang, J. Zhang, "Global dynamics of a multi-group epidemic model with general relapse distribution and nonlinear incidence rate," The Journal of Biological Systems , vol. 20, no. 3, pp. 235-258, 2012.
[13] R. Olfati-Saber, "Flocking for multi-agent dynamic systems: algorithms and theory," IEEE Transactions on Automatic Control , vol. 51, no. 3, pp. 401-420, 2006.
[14] N. Moshtagh, A. Jadbabaie, K. Daniilidis, "Distributed geodesic control laws for flocking of nonholonomic agents," in Proceedings of the 44th IEEE Conference on Decision and Control, and the European Control Conference (CDC-ECC '05), pp. 2835-2840, December 2005.
[15] R. A. Freeman, Y. Peng, K. M. Lynch, "Distributed estimation and control of swarm formation statistics," in Proceedings of the American Control Conference, pp. 749-755, June 2006.
[16] Y. Hong, L. Gao, D. Cheng, J. Hu, "Lyapunov-based approach to multiagent systems with switching jointly connected interconnection," IEEE Transactions on Automatic Control , vol. 52, no. 5, pp. 943-948, 2007.
[17] R. Olfati-Saber, J. S. Shamma, "Consensus filters for sensor networks and distributed sensor fusion," in Proceedings of the 44th IEEE Conference on Decision and Control, and the European Control Conference (CDC-ECC '05), pp. 6698-6703, December 2005.
[18] M. T. Hagan, H. B. Demuth, M. H. Beale Neural Network Design , China Machine, Beijing, China, 2002.
[19] Z. H. Zhou, C. G. Cao Neural Network with Applications , Tsinghua University Press, Beijing, China, 2004.
[20] C. Hu, J. Yu, H. Jiang, Z. Teng, "Exponential stabilization and synchronization of neural networks with time-varying delays via periodically intermittent control," Nonlinearity , vol. 23, no. 10, pp. 2369-2391, 2010.
[21] H. K. Khalil Nonlinear Systems , Prentice Hall, 2002., 3rd.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Copyright © 2014 Yang Gao and Shengqiang Liu. Yang Gao 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.
Abstract
We investigate a predator-prey model with dispersal for both predator and prey among n patches; our main purpose is to extend the global stability criteria by Li and Shuai (2010) on a predator-prey model with dispersal for prey among n patches. By using the method of constructing Lyapunov functions based on graph-theoretical approach for coupled systems, we derive sufficient conditions under which the positive coexistence equilibrium of this model is unique and globally asymptotically stable if it exists.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer