Volume 2012, Issue 1 678957
Research Article
Open Access

Qualitative Analysis for a Predator Prey System with Holling Type III Functional Response and Prey Refuge

Xia Liu

Corresponding Author

Xia Liu

College of Mathematics and Information Science, Henan Normal University, Xinxiang 453007, China htu.cn

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Yepeng Xing

Yepeng Xing

College of Mathematics and Science, Shanghai Normal University, Shanghai 200234, China shnu.edu.cn

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First published: 05 December 2012
Citations: 2
Academic Editor: Yonghui Xia

Abstract

A predator prey system with Holling III functional response and constant prey refuge is considered. By using the Dulac criterion, we discuss the global stability of the positive equilibrium of the system. By transforming the system to a Liénard system, the conditions for the existence of exactly one limit cycle for the system are given. Some numerical simulations are presented.

1. Introduction

Recently, the qualitative analysis of predator prey systems with Holling II or III types functional response and prey refuge has been done by several papers, see [15]. Their main objective is to discuss under what conditions the positive equilibrium of the corresponding system is stable or unstable and the existence of exactly one limit cycles. In general, the prey refuge has two types, one is the so-called constant proportion prey refuge: (1 − m)x, where m ∈ (0,1), the other type is called constant prey refuge: (xm).

In [2], the authors considered the following system with a constant proportion prey refuge:
(1.1)
where x and y denote the prey and predator density, respectively, at time t, the parameters a, b,  α,    β, c, k are positive constants, and their biological meanings can be seen in [2]. The main result is that when system (1.1) admits only one limit cycle which is globally asymptotically stable.
In paper [4], the authors only gave the local stability analysis to the following system with a constant prey refuge:
(1.2)
In this paper, we will research under what conditions that the positive equilibrium is globally asymptotically stable and the existence of exactly one stable limit cycle of system (1.2). For ecological reason, we only consider system (1.2) in Ω0 = {(x, y)∣x > m, y > 0} or .

It easy to obtain the following lemma.

Lemma 1.1. Any solution (x(t), y(t)) of system (1.2) with initial condition x(0) > m,   y(0) > 0 is positive and bounded for all t ≥ 0.

2. Basic Results

Let , then system (1.2) changes (still denote , as x,   y,   t)
(2.1)
Then Ω0 transforms to Ω = {(x, y)∣  x > 0,   y > 0} and system (2.1) is bounded.
Clearly, if (H1)  0 < m < a/b holds, system (2.1) has positive boundary equilibrium E0((a/b) − m, 0); if (H2)   kα > c,   0 < m < (abx*)/b, system (2.1) has a positive equilibrium E*(x*, y*), where
(2.2)

It is easy to obtain the following lemma.

Lemma 2.1. Let (H1) hold. Further assume that (H3)  kαc and (H4)  kα > c, m > max {0, (abx*)/b}. Then E0 is locally asymptotically stable, if any of (H3) and (H4) holds. When kα > c,   0 < m < (abx*)/b,   E0 is unstable, furthermore, E0 is a saddle point.

About the properties of the positive equilibrium, we have the following theorem.

Theorem 2.2. Assume kα > c. Then

  • (I)

    E* is locally asymptotically stable for 0 < m < (abx*)/b if a(2ckα) ≤ 2bcx* holds.

  • (II)

    E* is locally asymptotically stable for m1 < m < (abx*)/b and E* is locally unstable for 0 < m < m1 if a(2ckα) > 2bcx* holds, where

    (2.3)

  • (III)

    system (2.1) undergoes Hopf bifurcation at m = m1 if a(2ckα) > 2bcx* holds.

Proof. The Jacobian matrix of system (2.1) at E* is

(2.4)
where . Then tr (J(E*)) = −P/x*   = R(m)/x*, where , the discriminant of R(m) = 0 is . Hence, the equation R(m) = 0 has two roots m1 and m2, where .

Note that

(2.5)
and a(2ckα)>(≤)2bcx* implies m1 > (≤)0. Consider
(2.6)
Then
  • (I)

    If a(2ckα) ≤ 2bcx* holds, then m1 ≤ 0,   R(m) < 0 holds for m1 < m < m2. Considering (H2) and m2 > (abx*)/b, for 0 < m < (abx*)/b, tr (J(E*)) < 0, which implies E* is locally asymptotically stable.

  • (II)

    If a(2ckα) > 2bcx* holds, then m1 > 0, for m1 < m < m2,   R(m) < 0, since , by , we obtain m1 < (abx*)/b. Together with (H2), for m1 < m < (abx*)/b,   tr (J(E*)) < 0, which means E* is locally asymptotically stable. On the other hand, for 0 < m < m1,   tr (J(E*)) > 0,   E* is locally unstable.

  • (III)

    We have

    (2.7)
    these satisfy Liu’s Hopf bifurcation criterion (see [6], page 255); hence, the Hopf bifurcation occurs at m = m1. This ends the proof.

3. Global Stability of the Positive Equilibrium

Denote .

Theorem 3.1. If E*(x*, y*) is locally stable. Further assume that max {0, (a − 4bβ)/2b} < m < m4, then the positive equilibrium E*(x*, y*) of system (2.1) is globally asymptotically stable.

Proof. Take the Dulac function B(x, y) = x−2y−1, for system (2.1) we have

(3.1)
where
(3.2)

If a = 2bm, ϕ(x) = 2b(x4 + m2β2) > 0 for x > 0.

On the other hand, there exist

(3.3)
The equation ϕ(x) = 0 has two roots x1 = 0,   x2 = (a − 2bm)/4b.

Case  1. If a − 2bm > 0, then for 0 < x < x2, ϕ(x) < 0; for x > x2, ϕ(x) > 0. Hence, x = x2 is the least value of the function ϕ(x). If β > x2,   ϕ(x2) = (a − 2bm)(βx2)(β + x2) > 0, it has ϕ(x) > 0 for all x > 0, then ϕ(x) is increasing for x > 0, notice that ϕ(0) > 0. Therefore, ϕ(x) > 0 for x > 0. Since, T < 0 for x > 0, system (2.1) does not exist limit cycle.

Case  2. If bm < a < 2bm, then x2 < 0, for x > 0,   ϕ(x) > 0, hence, for x > 0,   ϕ(x) is increasing. Evidently, , then there exists such that ϕ(x0) = 0, where , hence, when 0 < x < x0,     ϕ(x) < 0, when x > x0,   ϕ(x) > 0. We know that ϕ(x) takes the least value at x = x0, that is, ϕ(x) > ϕ(x0). According to ϕ(x0) = 0, for x > 0 we obtain , where .

To prove ϕ(x) > 0 for x > 0, it suffices to prove for . Clearly, takes the least value at x = β, and is strictly decreasing at the interval (0, β). Hence, for holds. Since . Therefore, for holds if m3 < m < m4 holds, then for x > 0,   ϕ(x) > 0 holds.

In sum, if one of the following three conditions holds (1) m = a/2b; (2) 0 < m < a/2b,   x2 < β⇒max {0, (a − 4bβ)/2b} < m < a/2b; (3) a/2b < m < a/b, m3 < m < m4a/2b < m < m4, the function T does not change the sign for x > 0, then system (2.1) does not exist limit cycle. It is easy to see that the conditions (1), (2), and (3) are equal to max {0, (a − 4bβ)/2b} < m < m4. The proof is completed.

4. Existence and Uniqueness of Limit Cycle

Theorem 4.1. If a(2ckα) > 2bcx* holds, for 0 < m < m1 system (2.1) admits at least one limit cycle in Ω.

Proof. We construct a Bendixson loop which includes E* of system (2.1). Let be a length of the line L1: be a length of line L2:b(x + m) − a = 0. Define

(4.1)
where . The orbit of system (4.1) with initial value ((a/b) − m, a0) intersects with the line x = x* and the intersection point C(x*, y1), we obtain the orbit arc . Let be a length of line L3: be a length of line L4:x = 0. Because is a length of orbit line of system (2.1) and (dL2/dt)|(2.1)   = −b((a/b) − m) 2y < 0(y > 0), (dL3/dt)|(2.1) = y1(−cβ2 + (kαc)x2) < 0  (0 < x < x*),   (dL4/dt)|(2.1) = mβ2(abm) > 0, the orbits of system (2.1) tend to the interior of the Bendixson loop from the outer of , and , by comparing system (2.1) to system (4.1): dx/dt|(2.1) < dx/dt|(4.1) < 0 and dy/dt|(2.1) = dy/dt|(4.1) > 0. Then the orbits of system (2.1) tend to the interior of the Bendixson loop from the outer of . On the other hand, under the condition of Theorem 4.1, E*(x*, y*) is unstable, by Poincaré-Bendixson Theorem, system (2.1) admits at least one limit cycle in the region . This ends the proof.

Lemma 4.2 (see [7].)Let f(x), g(x) be continuously differentiable functions on the open interval (r1, r2), and φ(y) be continuously differentiable functions on R in

(4.2)
such that
  • (1)

    dφ(y)/dy > 0,

  • (2)

    having a unique x0 ∈ (r1, r2), such that (xx0)g(xx0) > 0 for xx0 and g(x0) = 0,

  • (3)

    f(x0)d/dx(f(x)/g(x)) < 0 for xx0,

then system (4.1) has at most one limit cycle.

Theorem 4.3. If a(2ckα) > 2bcx* holds, for system (2.1) exists exactly one limit cycle which is globally asymptotically stable in Ω.

Proof. Let u = x,   v = ln y,   τ = −x2t, still denote u, v, τ, as x,   y,    t, then system (2.1) becomes

(4.3)
the positive equilibrium E*(x*, y*) changes .

Let , then transform to the origin O(0,0), still denote , as x,   y yield

(4.4)
where F(x) = ((x + x* + m)(ab(x + x* + m))(β2 + (x + x*) 2))/(x + x*) 2y*.

Clearly, F(0) = 0. It is easy to see that the conditions (1) and (2) of Lemma 4.2 for x0 = 0 are satisfied. Consider

(4.5)
Note that by the assumption of Theorem 4.3, E* is unstable equilibrium and
(4.6)
then . Consider
(4.7)
where
(4.8)
where
(4.9)

Then, we have

(4.10)
where
(4.11)

By a simple computation, we obtain

(4.12)
It is easy to verify that and has two roots and defined by, respectively,
(4.13)
Obviously, . Therefore, for and for which indicates that is the minimum point of the function when x⩾−x*. Substituting into , we obtain
(4.14)
It is easy to see that if , then , which implies for all x⩾−x*. That is, the function is a strictly increasing function for x⩾−x*.

Note that for 0 < m < a/b and . It follows from (4.6) that

(4.15)

Hence, there exists a point , such that , that is,

(4.16)
This, together with the monotonicity of when x⩾−x*, we may conclude that for and for . Therefore, is the minimum point of the function for −x* < x < .

Together with (4.16), we obtain

(4.17)
It follows from (4.6), we have . This indicates for all x > −x*.

Then all the conditions of Lemma 4.2 are satisfied, considering Theorem 4.1, we obtain the conclusion of this theorem. The proof is completed.

5. Numerical Simulations

Take α = 0.5, k = 0.2, β = 0.5, a = 1, b = 0.1, and c = 0.09. Then a(2ckα) − 2bcx* = 0.053, and m1 ≈ 1.986121812. One can see a Hopf bifurcation occurring at m = 1.955 and the bifurcated periodic solution is stable in Figure 1.

Details are in the caption following the image
The bifurcated periodic solution is stable.

When taking m = 4.5, then x* = 1.5, y* ≈ 2.666666667, a(2ckα) − 2bcx* = 0.053,   m1 ≈ 1.986121812,(abx*)/b = 8.5,     (a − 4bβ)/2b = 4, a/2b = 5. Theorem 3.1 is satisfied; the equilibrium E* of system (2.1) is globally asymptotically stable. See Figure 2.

Details are in the caption following the image
The positive equilibrium E* of system (2.1) is globally asymptotically stable.

Take m = 1, we obtain E*(1.5,2.083333333), . The conditions in Theorem 4.1 are satisfied; hence, system (2.1) exists exactly one limit cycle which is globally asymptotically stable. One can see Figure 3.

Details are in the caption following the image
The dynamical behaviors of system (2.1) when α = 0.5, k = 0.2, β = 0.5, a = 1, b = 0.1, c = 0.09, m = 1. (a) The existence of unique limit cycle. (b) The global stability of the limit cycle.
Details are in the caption following the image
The dynamical behaviors of system (2.1) when α = 0.5, k = 0.2, β = 0.5, a = 1, b = 0.1, c = 0.09, m = 1. (a) The existence of unique limit cycle. (b) The global stability of the limit cycle.

Acknowledgments

This work is partially supported by the National Natural Science Foundation of China (11226142), Foundation of Henan Educational Committee (2012A110012), Youth Science Foundation of Henan Normal University (2011QK04), Natural Science Foundation of Shanghai (no. 12ZR1421600), and Shanghai Municipal Educational Committee (no. 10YZ74).

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