e c o l o g i c a l m o d e l l i n g 2 1 6 ( 2 0 0 8 ) 415–416 available at www.sciencedirect.com journal homepage: www.elsevier.com/locate/ecolmodel Letter to the Editor Stability condition for the predator-free equilibrium point of predator–prey systems with a class of functional response夽 Stability analysis of a predator–prey system incorporating a given functional response is a popular issue in mathematical ecology (Hogarth et al., 1992; Chattopadhyay et al., 2002; González-Olivares and Ramos-Jiliberto, 2003; Aghajani and Moradifam, 2006; Canan, 2008; Moghadas and Corbett, 2008; Wang, 2008). Hesaaraki and Moghadas (2001) have considered predator–prey systems with a class of functional response. They have obtained a sufficient and necessary condition for the existence of limit cycles around the interior equilibrium point of the considered system. They argue that “it is easy to check that (0,0) and (1,0) are both saddle points”. However, I find that the predator-free equilibrium point (1,0) can change from the locally unstable state to be locally asymptotically stable. Hence, it is partial to conclude that the equilibrium point (1,0) is a saddle point. Moreover, the existence of limit cycles around the equilibrium point E∗ = (x∗ , y∗ ) can be considered if and only if the predator-free equilibrium point is unstable. Because if it is locally asymptotically stable, the equilibrium point (x∗ , y∗ ) lies in the fourth quadrant. It has no ecological meanings. Therefore, we represent the following proposition Proposition 1. Assuming that (A1 ) − (A5 ) (see in Hesaaraki and Moghadas, 2001) hold, we can obtain that (1) If ϕ(1) > (D/), the equilibrium point (1,0) is a saddle point, and hence, is locally unstable. (2) If ϕ(1) < (D/), the equilibrium point (1,0) is locally asymptotically stable. Proof. The Jacobia matrix of the system (1.1) (see in Hesaaraki and Moghadas, 2001) at the equilibrium point (1,0) is J1 = 夽 −r −ϕ(1) 0 ϕ(1) − D It is easy to show that the two eigenvalues are 1 = −r and 2 = ϕ(1) − D. Clearly, the first one is negative. Hence, the stability of the equilibrium point (1,0) depends only on the sign of the second eigenvalue 2 = ϕ(1) − D. If 2 = ϕ(1) − D > 0, i.e. ϕ(1) > (D/), the equilibrium point (1,0) is a saddle point and locally unstable. According to the assumptions A1 and A2 , the response function ϕ(x) is increasing and positive. Thus we have ϕ(1) > 0. From the assumption A4 , the constant c is the maximum value of the response function ϕ(x). That is to say ϕ(1) < c. Hence, we obtain that 0 < ϕ(x∗ ) = D < ϕ(1) < c. Thus, x∗ < 1. The equilibrium point E∗ = (x∗ , y∗ ) lies in the first quadrant and is a positive point. Again, if 2 = ϕ(1) − D < 0, i.e. ϕ(1) < (D/), the equilibrium point (1,0) is locally asymptotically stable. Similarly, we have 0 < ϕ(1) < D = ϕ(x∗ ) < c Hence, x∗ > 1. The equilibrium point E∗ = (x∗ , y∗ ) lies in the forth quadrant. If the equilibrium point E∗ = (x∗ , y∗ ) is not a positive point, we do not think it has ecological meanings. Thus, we cannot consider its stability property and the existence of limit cycles around it. Therefore, the theorem 1.1 (see in Hesaaraki and Moghadas, 2001) should be proved if and only if the predatorfree equilibrium point is unstable. Supported by the National Natural Science Foundation of China (No. 30700100). 416 e c o l o g i c a l m o d e l l i n g 2 1 6 ( 2 0 0 8 ) 415–416 references Aghajani, A., Moradifam, A., 2006. Nonexistence of limit cycles in two classes of predator–prey systems. Appl. Math. Comput. 175, 356–365. Canan, C., 2008. The stability and Hopf bifurcation for a predator–prey system with time delay. Chaos, Solitons and Fractals 37, 87–99. Chattopadhyay, J., Sarkar, R.R., Ghosal, G., 2002. Removal of infected prey prevent limit cycle oscillations in an infected prey–predator system—a mathematical study. Ecol. Model. 156, 113–121. González-Olivares, E., Ramos-Jiliberto, R., 2003. Dynamic consequences of prey refuges in a simple model system: more prey, fewer predators and enhanced stability. Ecol. Model. 166, 135–146. Hesaaraki, M., Moghadas, S.M., 2001. Existence of limit cycles for predator–prey systems with a class of functional responses. Ecol. Model. 142, 1–9. Hogarth, W.L., Norbury, J., Cunning, I., Sommers, K., 1992. Stability of a predator–prey model with harvesting. Ecol. Model. 62, 83–106. Moghadas, S.M., Corbett, B.D., 2008. Limit cycles in a generalized Gause-type predator Cprey model. Chaos, Solitons and Fractals 37, 1343–1355. Wang, M.X., 2008. Stability and Hopf bifurcation for a prey–predator model with prey-stage structure and diffusion. Math. Biosci. 212, 149–160. Zhi-hui Ma ∗ Zi-zhen Li Key Laboratory of Arid and Grassland Agroecology of Ministry of Education, Lanzhou 730000, China ∗ Corresponding author. Tel.: +86 931 8913370; fax: +86 931 8912823. E-mail addresses: [email protected] (Z.-h. Ma), [email protected] (Z.-z. Li) 27 March 2008 Published on line 26 June 2008 0304-3800/$ – see front matter © 2008 Elsevier B.V. All rights reserved. doi:10.1016/j.ecolmodel.2008.05.002
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