Qualitative Analysis of a Diffusive Ratio-Dependent Holling-Tanner Predator-Prey Model with Smith Growth
Abstract
We investigated the dynamics of a diffusive ratio-dependent Holling-Tanner predator-prey model with Smith growth subject to zero-flux boundary condition. Some qualitative properties, including the dissipation, persistence, and local and global stability of positive constant solution, are discussed. Moreover, we give the refined a priori estimates of positive solutions and derive some results for the existence and nonexistence of nonconstant positive steady state.
1. Introduction
The dynamics of model (1) has been considered in many articles. For example, Hsu and Huang [7] obtained some results on the global stability of the positive equilibrium, more precisely, under the conditions which local stability of the positive equilibrium implies its global stability. Gasull and coworkers [8] investigated the conditions of the asymptotic stability of the positive equilibrium which does not imply global stability. Sáez and González-Olivares [9] showed the asymptotic stability of a positive equilibrium and gave a qualitative description of the bifurcation curve.
For model (2), in [13], the authors investigated the effect of time delays on the stability of the model and discussed the local asymptotic stability and the Hopf-bifurcation. Liang and Pan [16] have studied the local and global asymptotic stability of the coexisting equilibrium point and obtained the conditions for the Poincaré-Andronov-Hopf-bifurcating periodic solution. M. Banerjee and S. Banerjee [17] have studied the local asymptotic stability of the equilibrium point and obtained the conditions for the occurrence of the Turing-Hopf instability for PDE model. It is shown that prey and predator populations exhibit spatiotemporal chaos resulting from temporal oscillation of both the population and spatial instability.
The rest of the paper is organized as follows. In Section 2, we investigate the lager time behavior of model (6), including the dissipation, persistence property, and local and global stability of positive constant solution E*. In Section 3, we first give a priori upper and lower bounds for positive solutions of model (9), and then we deal with existence and nonexistence of nonconstant positive solutions of model (9), which imply some certain conditions under which the pattern happens or not.
2. Large Time Behavior of Solution to Model (6)
In this section, the dissipation and persistence properties are studied for solution of model (6). Moreover, the local and global asymptotic stability of positive constant solution E* = (N*, P*) are investigated.
2.1. The Properties of Dissipation and Persistence of Solution to Model (6)
Theorem 1. All the solutions of model (6) are nonnegative and defined for all t > 0. Furthermore, the nonnegative solution (N, P) of model (6) satisfies
Proof. The nonnegativity of the solution of model (6) is clear since the initial value is nonnegative. We only consider the latter of the theorem.
Note that N satisfies
Let z(t) be a solution of the ordinary differential equation:
As a result, for any ε > 0, there exists t0 > 0, such that N(x, t) ≤ K + ε for all and t ≥ t0. Hence, P(x, t) is a lower solution
Let P(t) be the unique positive solution of problem
Definition 2 (see [24].)The spatial model (6) is said to have the persistence property if for any nonnegative initial data (N0(x), P0(x)), there exists a positive constant ε = ε(N0, P0), such that the corresponding solution (N, P) of model (6) satisfies
Theorem 3. If m(1 + c) < ar, then model (6) has the persistence property.
Proof. Let N(x, t) be an upper solution of the following problem:
Let N(t) be the unique positive solution to the following problem:
Due to m(1 + c) < ar, we have that lim t→∞w(t) = K(ar − m(1 + c))/ar. By comparison, it follows that
Similarly, by the second equation of model (6), we have that P(x, t) is an upper solution of problem
Let P(t) be the unique positive solution to the following problem:
2.2. The Local Stability of the Constant Steady State
- (i)
Let 0 = μ0 < μ1 < μ2 < ⋯→∞ be the eigenvalues of the operator –Δ on Ω with the zero-flux boundary condition;
- (ii)
Let E(μ) = {ϕ∣ − Δϕ = μϕ in Ω, ∂ν ϕ = 0 on ∂Ω} with μ ∈ ℝ1;
- (iii)
Let {ϕij∣j = 1, …, dim E(μi)} be an orthonormal basis of E(μi), and Xij = {cϕij∣c ∈ ℝ2};
- (iv)
Let
(25) -
then
(26) -
where .
Theorem 4. Assume that
Proof. Define by
For each i = 0,1, 2, …, Xi is invariant under the operator ℒ, and λ is an eigenvalue of this operator on Xi if and only if it is an eigenvalue of the following matrix:
In view of (27) and (28), we have det (Ai) > 0 > tr (Ai) for any i ≥ 0. Therefore, the eigenvalues of the matrix Ai have negative real parts.
In the following, we prove that there exists δ > 0 such that
Let λ = μiξ, then
By the Routh-Hurwitz criterion, it follows that the two roots ξ1, ξ2 of all have negative real parts. Thus, let , we have that . By continuity, we see that there exists i0 such that the two roots ξi1, ξi2 of satisfy , , for all i ≥ i0. In turn, , for all i ≥ i0.
Let , then and (33) hold for . Consequently, the spectrum of ℒ which consists of eigenvalues, lies in {Reλ ≤ −δ}. In the sense of [25], we obtain that the positive constant solution E* = (N*, P*) of model (6) is uniformly asymptotically stable. This ends the proof.
2.3. The Global Stability of the Constant Solution
This subsection is devoted to the global stability of the constant solution E* for model (6).
Theorem 5. Assume that the following hold:
- (A1)
m(1 + c) < ar;
- (A2)
h(K + cN*)(N* + 2P*)+(K + cN*)(N* + aP*)(a + h) ≤ 2ηr(N* + aP*)(a + h);
- (A3)
hKN* ≤ η(2h − 1)(N* + aP*)(a + h),
Proof. In order to give the proof, we need to construct a Lyapunov function. Define
Set φ = N − N*, ϕ = P − P*. We have
By virtue of Theorems 1 and 3 and under the assumption of Theorem, we have
As a result, we have I(t) ≤ 0. Thus dE(t)/dt ≤ 0, which implies the desired assertion. The proof is completed.
3. A Priori Estimates and Existence of Nonconstant Positive Solution
In this section, we will deduce a priori estimates of positive upper and lower bounds for positive solution of model (9). Then, based on a priori estimates, we discuss the existence of nonconstant positive solution of model (9) for certain parameter ranges.
3.1. A Priori Estimates
In order to obtain the desired bound, we recall the following two lemmas which are due to Lin et al. [26] and Lou and Ni [27], respectively.
Lemma 6 (Harnack’s inequality [26]). Assume that and let be a positive solution to
Lemma 7 (maximum principle [27]). Let Ω be a bounded Lipschitz domain in ℝ2 and .
- (a)
Assume that and satisfies
(43) -
If , then g(x0, w(x0)) ≥ 0.
- (b)
Assume that and satisfies
(44) -
If , then g(x0, w(x0)) ≤ 0.
For convenience, let us denote the constants a, c, h, m, K, r, s collectively by Λ. The positive constants C, , , and so forth will depend only on the domain Ω and Λ. Now, we can state the main result which will play a critical role in Section 3.3.
Theorem 8. For any positive solution (N, P) of model (9),
Proof. Assume that (N, P) is a positive solution of model (9). Set
Since 0 < P(x)≤(1/h)∥N(x)∥∞, we have P(x) ≤ K/h in .
Theorem 9. Let d be a fix positive constant. Then there exists positive constant such that if d1, d2 > d, any positive solution (N, P) of model (6) satisfies
Proof. Let
By Lemma 7, it is clear that
Since m(K + cN(x0))/(N(x0) + aP(x0)) ≤ C with C > 0, then, by virtue of (52), we derive
3.2. Nonexistence of the Nonconstant Positive Solutions
Note that μ1 is the smallest positive eigenvalues of the operator –Δ in Ω subject to the zero-flux boundary condition. Now, using the energy estimates, we can claim the following results.
Theorem 10. Let D > s/μ1 be a fixed positive constant. Then there exists a positive constant d* = d*(Λ, D) such that model (9) has no positive nonconstant solution provided that d1 > d* and d2 > D.
Proof. Let (N, P) be any positive solution of model (9) and denote . Then
By the ε-Young inequality and the Poincaré inequality, we obtain that
In view of d2 > D > s/μ1, we can find a sufficiently small ϵ0 > 0 such that d2μ1 ≥ s + ϵ0M. Let d* = (1/μ1)(r + M/ϵ), then
3.3. Existence of the Nonconstant Positive Solutions
In this subsection, we shall discuss the existence of the positive nonconstant solution of model (9).
Unless otherwise specified, in this subsection, we always require that m < r(a + h) holds, which guarantees that model (9) has the unique positive constant solution E* = (N*, P*). From now on, we denote w = (N, P) T and w0 = E*.
On the other hand, using the decomposition (26), we have that Xi is an invariant space under ∇ℱ(w0) and ξ ∈ ℝ is an eigenvalue of ∇ℱ(w0) in Xi, if and only if, ξ is an eigenvalue of (μi + 1) −1(μiI − 𝒜). Therefore, ∇ℱ(w0) is invertible, if and only if, for any i ≥ 0 the matrix μiI − 𝒜 is invertible.
Lemma 11. Assume that, for all i ≥ 0, the matrix μiI − 𝒜 is nonsingular, then
Theorem 12. Assume that m(ar + cm + 2hr − acr) > r2(a + h) 2 and . If μ− ∈ (μi, μi+1) and μ+ ∈ (μj, μj+1) for some 0 ≤ i < j, and is odd, then model (9) has at least one nonconstant solution.
Proof. By Theorem 10, we can fix and such that model (9) with diffusion coefficients and has no nonconstant solutions.
By virtue of Theorems 8 and 9, there exists a positive constant , such that , .
Set
Since Ψ(w, t) is compact, the Leray-Schauder topological degree deg (I − Ψ(w, t), ℳ, 0) is well defined. From the invariance of Leray-Schauder degree at the homotopy, we deduce
Clearly, I − Ψ(w, 1) = ℱ. Thus, if model (9) has no other solutions except the constant one w0, then Lemma 11 shows that
On the contrary, by the choice of and , we have that w0 is the only solution of Ψ(w, 0) = 0. Furthermore, we have
From (79)–(81), we get a contradiction, and the proof is completed.
Acknowledgments
The authors would like to thank the anonymous referee for the very helpful suggestions and comments which led to improvements of our original paper. And this work is supported by the Cooperative Project of Yulin City (2011).