A Lyapunov Function and Global Stability for a Class of Predator-Prey Models

We construct a new Lyapunov function for a class of predation models. Global stability of the positive equilibrium states of these systems can be established when the Lyapunov function is used.


Introduction
The dynamics of predator-prey systems are often described by differential equations, which represent time continuously.A common framework for such a model is 1-3 dN dt Nf N − Pg N, P , dP dt h g N, P , P P, where N and P are prey and predator densities, respectively, f N is the prey growth rate, g N is the functional response, for example, the prey consumption rate by an average single predator, and h g N , P the per capita growth rate of predators also known as the "predator numerical response" , which obviously increases with the prey consumption rate.The most widely accepted assumption for the numerical response with predator density restricting is as follows: h g N, P , P εg N, P − δP − β, 1.
where β is a per capita predator death rate, ε the conversion efficiency of food into offspring, δ the density dependent rate 2 .And prototype of the prey growth rate f N is the logistic growth where K > 0 is the carrying capacity of the prey.When where a is the efficiency of predator capture of prey, model 1.1 is called Ivlev-type predation model, due originally to Ivlev 4 .And Ivlev-type functional response is classified to the preydependent; that is, g is independent of predator P 2 .
Both ecologists and mathematicians are interested in the Ivlev-type predator-prey model and much progress has been seen in the study of the model 5-13 .Of them, Xiao 8 gave global analysis of the following model:

1.5
But, in paper 8 , the author gave complex process to prove the global asymptotical stability of the positive equilibrium.
In this paper, we will establish a new Lyapunov function to prove the global stability of the positive equilibrium of model 1.5 .
Our paper is organized as follows.In the next section, we discuss the existence, uniqueness of the positive equilibrium, and establish a new Lyapunov function to model 1.5 .In Section 3, we will give some examples to show the robustness of our Lyapunov function.

Main Results
First of all, it is easy to verify that model 1.5 has two trivial equilibria belonging to the boundary of R 2 , that is, at which one or more of populations has zero density or is extinct , namely, E 0 0, 0 and E 1 1, 0 .For the positive equilibrium, set We have the following Lemma regarding the existence of the positive equilibrium.
δ} is a region of attraction for all solutions of model 1.5 initiating in the interior of the positive quadrant R 2 .
Proof.Let N t , P t be any solution of model 1.5 with positive initial conditions.Note that dN/dt ≤ N 1 − N , by a standard comparison argument, we have Then, Similarly, since 1 − e −a > d, we have On the other hand, for all N, P ∈ Ω, we have dN/dt| N 0 0 and dP/dt| P 0 0. Hence, Ω is a region of attraction.As a consequence, we will focus on the stability of the positive equilibrium E * only in the region Ω.
In the following, we devote to the global stability of the positive equilibrium E * N * , P * for model 1.Substituting the expressions of dN/dt and dP/dt defined in 1.5 into 2.7 , we can obtain

2.10
So, Then we can get holds, which is equivalent to

2.16
In view of a ≤ 2, it follows that ψ N ≤ 0 and ψ N ≤ ψ 0 0 in the region Ω.Then ψ N ≤ 0 is always true.It follows that ϕ N ≤ 0, that is, V ≤ 0. Consequently, the function V N, P satisfies the asymptotic stability theorem 14 .Hence, E * N * , P * is globally asymptotically stable.This completes the proof.

Applications
In this paper, we construct a new Lyapunov function for proving the global asymptotical stability of model 1.5 .The new Lyapunov function is useful not only to model 1.5 , but also to other models.
In this section, we will give some examples to show the robustness of the Lyapunov function 2.6 .The parameters of the following models are positive and have the same ecological meanings with those of in model 1.5 .where m ∈ 0, 1 is a refuge protecting of the prey.We can choose a Lyapunov functional as follows: The proof is similar to that of the Section 2. where μ ∈ 0, 1 is the victim's competition constant.We can choose a Lyapunov functional as follows: V N, P

3.13
The remaining arguments are rather similar as Theorem 2.3.

Lemma 2 .1 see 8 .
Suppose 1 − e −a > d.Model 1.5 has a unique positive equilibrium E * N * , P * if either of the following inequalities holds:

Theorem 2 . 3 .
5 by constructing a new Lyapunov function which is motivated by the work of Hsu 3 .If a ≤ 2, the positive equilibrium E * N * , P * of model 1.5 is globally asymptotically stable in the region Ω.Proof.For model 1.5 , we construct a Lyapunov function of the form V N, P N N * 1 − e −aξ − d − δP * 1 − e −aξ dξ P P * η − P * η dη.2.6 Note that V N, P is non-negative, V N, P 0 if and only if N, P N * , P * .Furthermore, the time derivative of V along the solutions of 1.5 is dV dt 1 − e −aN − d − δP * 1 − e −aN

Example 3 . 2 .
Considering the following predator-prey model with Rosenzweig functional response see 10 : μ − δN − d P, 3.3 , respectively.∇ 2 ∂ 2 /∂x 2 ∂ 2 /∂y 2 , the usual Laplacian operator in two-dimensional space, is used to describe the Brownian random motion.In order to give the proof of the global stability, we construct a Lyapunov function: Example 3.4.Considering the following diffusive Ivlev-type predator-prey model see 13 :∂N dt rN 1 − N − 1 − e −aN P d 1 ∇ 2 N, ∂P dt ε 1 − e −aN − d P d 2 ∇ 2 P, 3.7where the nonnegative constants d 1 and d 2 are the diffusion coefficients of N and PIn the above, n is the outward unit normal vector of the boundary ∂Ω.