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 Open Access
Bifurcation analysis of a modified Leslie–Gower model with Holling typeIV functional response and nonlinear prey harvesting
 Zizhen Zhang^{1},
 Ranjit Kumar Upadhyay^{2}Email author and
 Jyotiska Datta^{3}
https://doi.org/10.1186/s1366201815813
© The Author(s) 2018
 Received: 23 January 2018
 Accepted: 1 April 2018
 Published: 10 April 2018
Abstract
In this work, an attempt is made to understand the dynamics of a modified Leslie–Gower model with nonlinear harvesting and Holling typeIV functional response. We study the model system using qualitative analysis, bifurcation theory and singular optimal control. We show that the interior equilibrium point is locally asymptotically stable and the system under goes a Hopf bifurcation with respect to the ratio of intrinsic growth of the predator and prey population as bifurcation parameter. The existence of bionomic equilibria is analyzed and the singular optimal control strategy is characterized using Pontryagin’s maximum principle. The existence of limit cycles appearing through local Hopf bifurcation and its stability is also examined and validated numerically by computing the first Lyapunov number. Optimal singular equilibrium points are obtained numerically for various discount rates.
Keywords
 Hopfbifurcation
 Saddlenode bifurcation
 Stable limit cycle
 Bionomic equilibria
 Singular optimal control
MSC
 34C15
 34C23
 37G15
 37N25
1 Introduction
The Leslie–Gower model [1, 2] (LG model) shows how asymptotic solutions converge to a stable equilibrium (independent of the initial conditions) state. The equilibrium point depends on the intrinsic factors which govern the system dynamics (in the sense of biology). It marks a significant improvement over the famous Lotka–Volterra model and it is limited in its explanatory capability [3]. Korobeinikov [4] established the global stability of a positive equilibrium point and showed that the limit cycle could be admitted by the model system. This limit cycle also exists if we take the Holling typeII or III functional response. Aziz and Okiye [5] have designed and studied the modified LG model with cyrtoid type functional response. Huang and Xiao [6] investigated a predator–prey system with Holling typeIV functional response. The qualitative analysis and bifurcation theory along with numerical simulations indicated that it has a unique stable limit cycle. Yafia et al. [7] studied the limit cycle in a modified LG model with Holling typeII scheme bifurcated from small and large time delays. Ji et al. [8] extended the study of the modified LG model designed by Aziz and Camara for stochastic perturbation. Huang et al. [9] studied controlling bifurcation in a delayed fractional predator–prey system with incommensurate orders. Rihan et al. [10] investigated fractionalorder delayed predator–prey systems with Holling typeII functional response. Song et al. [11] have studied dynamic analysis of a fractionalorder delayed predator–prey system with harvesting. Xu et al. [12] studied the stability and Hopf bifurcation of a population model with Holling typeIV functional response and time delay. Jana et al. [13] have studied a hybrid type tritrophic food chain model (Holling typeIV and Beddington–DeAngelis type functional responses) and try to understand the role of top predator interference and gestation delay and observed the subcritical Hopf bifurcation phenomena in the designed model system and the bifurcating periodic solution is unstable for the considered set of parameter values. Yu [14] studied the global stability of a modified LG model with Beddington–DeAngelis type functional response. Recently, Agrawal et al. [15] investigated the occurence of double Hopf bifurcation at positive equilibrium point when they choose appropriate measure of the tolerance of the prey. Furthermore, some dynamic behaviors, such as stability switches, chaos, bifurcation and double Hopf bifurcation scenarios are observed using numerical simulations.
Presently, the population dynamics is a very importance topic in the field of bioeconomics and related to the optimal management of renewable resources. It is more realistic to introduce the harvesting factor in the model system. We also introduce the idea of maximal sustainable yield in the management of renewable resources. It suggests exploiting the surplus production on the basis of biological growth model. Clark [16] reviewed how harvesting affects the fisheries management using ecological and economic models. Hoekstra et al. [17] studied the conservation and harvesting of a population dynamic model system and illustrated that several types of optimal harvesting solutions are possible and depend on both ecological parameters such as the predators search and handling time of prey and economic parameters (e.g., the maximum harvest rate, the discount rate and the cost of fishing). We know that mainly three types of harvesting have been reported in the literature: (i) constant rate of harvesting, (ii) proportional harvesting \(h(x)=qEx\), where q is the catch ability coefficient, E is the effort made for harvesting and the product qE is the fishing mortality [18], and (iii) nonlinear harvesting \(h(x)=qEx/(m_{1}E+m_{2}x)\), where \(m_{1}\) and \(m_{2}\) are suitable positive constants, proportional to the ratio of the stock level to the harvesting rate at high levels of effort and to the ratio of the effort level to the harvesting rate at high stock levels, respectively. Azar et al. [19] studied the Lotka–Volterra type two prey one predator model where the predator is harvested with two different schemes: (i) constant harvesting quota and (ii) constant harvesting effort, and one reported that a constant harvesting quota on the predator may destabilize the system. Zhu and Lan [20] made a Hopf bifurcation analysis of the LG model with constant prey harvesting. The dynamics of a model with proportionate harvesting has been studied by MenaLorca et al. [21]. Zhang et al. [22] studied the harvested LG model and found that harvesting has no influence on the persistence of the model system. So, the predator density strictly decreases with harvesting effort but it has no effect on the prey density. Kar and Ghorai [23] analyzed the dynamics of a delayed predator–prey model with harvesting in a modified LG model. Gupta et al. [24] studied the bifurcation analysis and control of the LG model with Michaelis–Menten type prey harvesting and observed that for a wide range of initial values the system goes to extinction. Recently, Huang et al. [25] studied the effect of constant yield predator harvesting on the dynamics of a LG model. The model exhibits different types of bifurcations including the saddlenode bifurcation, attracting and repelling Bogdanov–Takens bifurcations, and all types of Hopf bifurcation with the variation of the control parameters. Saleh [26] studied the dynamics of a modified LG model with quadratic predator harvesting.
We have proposed a new 2D modified Leslie–Gower type predator–prey model with Holling typeIV functional response in this manuscript. We have also incorporated the nonlinear harvesting in the prey population. Andrews [27] explored a function of the form \(f(x)=mx/((x^{2}/i)+x+a)\) and named it the Holling typeIV functional response or Monod–Haldane [28] function, which is similar to the Monod (i.e., the Michaelis–Menten) function for low concentration but includes the inhibitory effect at high concentrations. The parameters m and a can be interpreted as the maximum per capita predation rate and the half saturation constant in the absence of any inhibitory effect. The parameter i is a measure of the predator’s immunity from or tolerance of the prey. We have analyzed this model for its rich dynamics and studied the bioeconomic equilibria using singular optimal control strategies.
This work is organized as follows. In the next section, model formulation and biological meaning of the parameters are given. In Sect. 3, we presented the detail analysis of the model system. In Sect. 4, we discuss the linear stability analysis and Hopf bifurcation. Stability of the limit cycle is also presented in this section. Section 5 discusses the bionomic equilibria and optimal harvesting policy. In Sect. 6, some numerical simulation results are presented to illustrate or complement our mathematical findings. Conclusions and discussions are given in the final section which summarizes our findings.
2 Model formulation
Parameters and their biological meanings in this paper
Parameter  Description 

r  Intrinsic growth rate of the prey 
s  Intrinsic growth rates of the predator 
K  The environmental carrying capacity for prey 
m  The maximum per capita predation rate 
i  A direct measure of the predator’s immunity from or tolerance of the prey 
a  The half saturation constant in the absence of any inhibitory effect 
n  Number of prey required to support one predator at equilibrium 
The interaction between prey and predator is expressed by a Holling typeIV functional response, that is, \(f(u)= \frac{mu}{\frac{u^{2}}{i}+u+a}\) [3]. Taylor [30] has suggested that the subsistence of the predator depends on prey population therefore, the conventional environmental carrying capacity \(K_{v}\) of the predator is taken to be proportional to the prey abundance u, thus \(K_{v}= \frac{u}{n}\).
2.1 The model with prey harvesting
3 Analysis of the model system
3.1 Positivity and boundedness of solution
Lemma 1
(a) All solutions \((x(t), y(t))\) of system (4) with the initial condition (5) are positive for all \({t\geq 0}\). (b) All solutions \((x(t),y(t))\) of system (4) with the initial condition (5) are bounded for all \({t\geq 0}\).
Proof
Hence the whole solution starting in \(\operatorname {Int}(\Omega )=\{(x, y)\in R^{2}x>0, y>0\}\) remains in \(\operatorname {Int}(\Omega )\) for all \(t\geq 0\). Since the trajectories which start in positive direction of the xaxis and remain on it at all future time, the positive xaxis is an invariant set and similarly the positive yaxis is an invariant set for the system (4). Combining the two we observe that the set Ω defined in (2) is an invariant set for system (4).
Therefore, \(y(t)\leq \max\{\frac{M_{1}}{\beta }, y_{0}\}\equiv M_{2}\). This completes the proof of the boundedness of solutions and hence the system under consideration is a dissipative system. □
3.2 Equilibrium analysis
The roots of Eqs. (8) and (9) depend on the parameters h and c, so we shall consider the following cases.
Case I. When \(h>c\)
Axial Equilibria
The two real positive roots \(x_{1}\) and \(x_{2}\) will exist if \(c<1\) and \((1+c)^{2}4h>0\). Note that the other cases are not biologically feasible.
Interior Equilibria
From (9), it is obvious that \(P>0\) and \(T>0\). If either (i) \(Q, R, S<0\), or (ii) \(Q, S>0\), \(R<0\), or (iii) \(Q<0\), \(S, R>0\), or (iv) \(Q, R>0\), \(S<0\), or (v) \(Q>0\), \(S, R<0\), or (vi) \(Q, R<0\), \(S>0\), then by Descartes’ rule Eq. (9) has either two positive real roots or no real root and if either \(Q, S<0\), \(R>0\), then by Descartes’ rule Eq. (9) has either four positive real root or two positive real roots or no real root. Note that the other cases are not biologically feasible.
Case II. When \(h< c\)
Axial Equilibria
In this case \(x=\tilde{x}\) is the only positive real root of Eq. (8). For \(h< c\), the product of roots is negative. Therefore, the two roots are either of opposite sign or complex conjugates. The root \(\tilde{x}=\frac{(1c)+\sqrt{(1+c)^{2}4h}}{2}\) and the real positive root x̃ will exist if \(c<1\) and \((1+c)^{2}4h>0\). Hence the axial equilibria are \(\tilde{E}=( \tilde{x}, 0)\).
Interior Equilibria
From Eq. (9), obviously \(P>0\) and \(T<0\). If either (i) \(Q, R, S<0\), or (ii) \(Q, R, S>0\), then by Descartes’ rule Eq. (9) has only one positive real root and if either (i) \(Q>0\), \(R>0\), \(S<0\), or (ii) \(Q>0\), \(R<0\), \(S>0\), or (iii) \(Q<0\), \(R<0\), \(S>0\), or (iv) \(Q<0\), \(R>0\), \(S<0\), or (v) \(Q>0\), \(R<0\), \(S<0\), or (vi) \(Q<0\), \(R>0\), \(S>0\), then by Descartes’ rule Eq. (9) has either three positive real roots or one positive real root. Note that the other cases are not biologically feasible.
Case III. When \(h=c\)
Axial Equilibria
In this case \(x=1c\) is the only positive real root of Eq. (8). Therefore the axial equilibrium point is \(E=(1c, 0)\) provided \(c<1\).
Interior Equilibria
From Eq. (9), it is obvious that \(P>0\). If either (i) \(Q, R, S<0\), or (ii) \(Q>0\), \(R<0\), \(S<0\), or (iii) \(Q>0\), \(R>0\), \(S<0\), then by Descartes’ rule Eq. (9) has only one positive real root and if either \(Q<0\), \(R>0\), \(S<0\), then by Descartes’ rule Eq. (9) has either three positive real roots or one positive real root and if either (i) \(Q>0\), \(R<0\), \(S>0\), or (ii) \(Q<0\), \(R>0\), \(S>0\), or (iii) \(Q<0\), \(R<0\), \(S>0\), then by Descartes’ rule Eq. (9) has either two positive real roots or no positive real root. Note that the other cases are not biologically feasible.
4 Linear stability analysis and Hopf bifurcation
Theorem 1
 (a)
For \(h>c\), the axial equilibrium point \(E_{1}=(x_{1}, 0)\) is a repeller and \(E_{2}=(x_{2}, 0)\) is a saddle point.
 (b)
For \(h< c\), the axial equilibrium point \(\tilde{E}=(\tilde{x}, 0)\) is always a saddle point.
 (c)
For \(h=c\), the axial equilibrium point \(E=(1c, 0)\) is always a saddle point.
Proof
 (a)
For the equilibrium point \(E_{1}=(x_{1}, 0)\), the eigenvalues \(12x\frac{hc}{(c+x)^{2}}\) and δ are both positive and so the equilibrium point \(E_{1}\) is a repeller. Similarly at the equilibrium point \(E_{2}=(x_{2}, 0)\), the eigenvalue \(12x\frac{hc}{(c+x)^{2}}\) and \(\delta >0\) and the equilibrium point \(E_{2}\) is a saddle point.
 (b)
Since \(\tilde{E}=E_{2}\), Ẽ is saddle point.
 (c)
For the axial equilibrium point \(E=(1c, 0)\), the eigenvalues are \(12x\frac{hc}{(c+x)^{2}}=(1c)^{2}<0\) and \(\delta >0\) and the equilibrium point E is a saddle point.
Theorem 2
 (a)
The equilibrium point \(E_{*}(x_{*}, y_{*} )\) (for all three cases) is locally asymptotically stable if \(\frac{1}{2}< x_{*}<\sqrt{\alpha \gamma }\).
 (b)
System (4) undergoes a Hopf bifurcation with respect to the bifurcation parameter \(\delta =\tilde{\delta }\) around the equilibrium point \(E_{*} (x_{*}, y_{*})\) if \(x_{*}>\frac{1}{2}\) and \(\alpha \beta \tilde{\delta }(\frac{x^{2}}{\alpha }+x+\gamma )^{2}= \alpha (\frac{x^{2}}{\alpha }+x+\gamma )[\beta (12x_{*})(x_{*}+c)(\frac{x ^{2}}{\alpha }+x+\gamma )c\beta (1x_{*})(\frac{x^{2}}{\alpha }+x+ \gamma )+cx_{*}]x_{*}(\alpha \gamma x_{*}^{2}\beta )(x_{*}+c)\).
The proof is given in Appendix A1.
Theorem 3
 (i)
\(2\beta x_{*}^{5}+\beta (4\alpha +c1)x_{*}^{4}+\alpha \beta (2c+2 \alpha 2+4\gamma )x_{*}^{3} +\alpha (2c\beta \gamma \beta +c\alpha \beta +\alpha c+4\alpha \beta \gamma \beta \gamma )x_{*}^{2} +(c \beta \gamma \beta +2\beta \gamma^{2}\beta \gamma +2\gamma )x_{*}+ \alpha^{2}(\beta c\gamma +\beta \gamma +c\gamma )=0\),
 (ii)
\(2\beta x_{*}^{6}+\beta (4\alpha +c1+\delta )x_{*}^{5}+(2c \alpha \beta +2\alpha^{2}\beta +2\alpha \beta \delta \alpha +2\alpha \beta \gamma +c\beta \delta +2\alpha \beta \gamma 2\alpha \beta )x _{*}^{4} +\alpha (2c\beta \gamma +c\beta \beta \gamma \beta 2c+c \alpha \beta +4\alpha \beta \gamma \alpha \beta +\alpha \beta \delta 2c\beta \delta )x_{*}^{3} +\alpha (2c\alpha \beta \gamma 2\alpha \beta \gamma c\alpha +\alpha \beta \gamma^{2}+2\alpha \beta \gamma \delta +\alpha \gamma +2c\beta \gamma \delta +c\alpha \beta \delta )x _{*}^{2} +\alpha^{2}\beta (c\gamma^{2}+\gamma^{2}\delta +2c\gamma \delta \gamma^{2})x_{*}+c\alpha^{2}\beta \gamma^{2}\delta >0\), and
 (iii)
\(\sqrt{\frac{\alpha \gamma }{3}}< x_{*}<(2hc)^{1/3}c\).
The proof is given in Appendix A2.
4.1 Stability of limit cycles
Since the expression for the Lyapunov number σ is complicated we cannot say anything about the sign of σ and therefore we have analyzed it numerically.
5 Bionomic equilibria
Note that if the harvesting cost is greater than the revenue for prey species (i.e. \(C>\frac{pqx}{m_{1}E+m_{2}x}\)), then the harvesting in prey species is not profitable and it is of no interest. Hence, we consider that the cost must be less than the revenue for prey species (i.e. \(C<\frac{pqx}{m_{1}E+m_{2}x}\)).
Thus, the bionomic equilibria are the points of intersection of biological equilibrium line and zero profit line. Solving Eqs. (12) and (13), we obtain the value of \(x_{\infty }\) and \(y_{\infty }\) and from (14) we obtain \(E_{\infty }=\frac{pqCm_{2}}{cm_{1}}x_{\infty }\) if \(Cm_{2}< pq\).
5.1 Optimal harvesting policy
This shadow price \(\tau_{i}(t)=\lambda_{i}(t)e^{\mu t}\), \(i=1,2\), should remain constant over time in singular equilibrium to satisfy the transversality conditions at ∞ (i.e. \(\lim_{t\rightarrow \infty }\lambda_{i}(t)=0\) for \(i=1,2\)). Thus, the solution of Eq. (23) satisfying the transversality condition for the discounted autonomous infinite horizon problem (16) is \(\tau_{2}=\frac{R(x ^{*})}{(s+\mu )}\).
Thus, the maximized Hamiltonian \(H^{*}\) is concave in both x and y for all \(t\in [0, \infty )\) provided (27) and (28) are satisfied. Hence, the Arrow sufficiency condition for an infinite time horizon is satisfied [34] under certain constraints.
The generalized Legendre–Clebsch condition for the optimal control problem (16) is trivially satisfied as \(\frac{\partial H}{\partial E}=0\) for all \(t\in [0, \infty )\) along the optimal singular solution. Hence, from the Arrow sufficient conditions for infinite time horizon and generalized Legendre–Clebsch condition, the singular solution \((x^{*},y^{*},E^{*})\) is a part of the optimal solution (piecewise continuous curve) locally.
6 Numerical simulation results
 (i)
For \(\alpha =0.1\), \(\beta =2\), \(c=0.004\), \(\delta =0.5\), \(\gamma =1\), \(h=0.09\), the equilibrium points are \(E_{1}(0.101018, 0.050509)\) and \(E_{2}(0.847354, 0.423677)\).
For the equilibrium point \(E_{1}(0.101018, 0.050509)\), \(\operatorname {Tr}N=0.233986\) and \(\det N=0.346001\). For the equilibrium point \(E_{2}(0.847354, 0.423677)\), \(\operatorname {Tr}N=1.16308\) and \(\det N=0.355004\). The equilibrium point \(E_{1}(0.101018, 0.050509)\) is a saddle point and the equilibrium point \(E_{2}(0.847354, 0.423677)\) is a stable focus, which is shown in Fig. 1.  (ii)
For \(\alpha =0.2\), \(\beta =0.125\), \(c=0.049\), \(\delta =0.12\), \(\gamma =1\), \(h=0.05\), which gives the two equilibrium point \(E_{11}(0.0018, 0.0144)\) and \(E_{21}(0.0695, 0.556)\).
The equilibrium point \(E_{11}(0.0018, 0.0144)\) is a saddle point as the eigenvalues of Jacobian matrix are −0.107753 and 0.0208392. A stable limit cycle appears in a small neighborhood of \(E_{21}(0.0695, 0.556)\) as the Lyapunov number \(\sigma =30387.3\pi <0\) (see Fig. 2).  (iii)
For \(\alpha =0.5\), \(\beta =7.5\), \(c=0.1\), \(\delta =0.002\), \(\gamma =1\), \(h=0.05\), we have only one equilibrium point, \(E_{*}(0.9169, 0.1223)\).
For the equilibrium point \(E_{*}(0.9169, 0.1223)\), \(\operatorname {Tr}N=0.8342\) and \(\det N=0.0017\) and so the equilibrium point \(E_{*}(0.9169, 0.1223)\) is a stable focus, which is shown in Fig. 3.  (iv)
For \(\alpha =0.2\), \(\beta =0.125\), \(c=0.1\), \(\delta =0.12\), \(\gamma =1\), \(h=0.05\), the equilibrium point is \(E_{*}(0.09177, 0.73416)\).
An unstable limit cycles appears in a small neighborhood of \(E_{*}(0.09177, 0.73416)\) as the Lyapunov number \(\sigma =728.498 \pi >0\) (see Fig. 4).  (v)
For \(\alpha =0.5\), \(\beta =7.5\), \(c=0.1\), \(\delta =0.002\), \(\gamma =1\), \(h=0.1\), we have only one equilibrium point, which is \(E^{**}(0.8617, 0.1149)\).
For the equilibrium point \(E^{**}(0.8617, 0.1149)\), \(\operatorname {Tr}N=0.7312\) and \(\det N=0.0015\), so the equilibrium point \(E^{**}(0.8617, 0.1149)\) is a stable focus, which is shown in Fig. 5.  (vi)
For \(\alpha =0.2\), \(\beta =0.125\), \(c=0.01\), \(\delta =0.12\), \(\gamma =1\), \(h=0.01\), the equilibrium point is \(E_{3}(0.1196, 0.9568)\).
An unstable limit cycles appears in a small neighborhood of \(E_{3}(0.1196, 0.9568)\) as the Lyapunov number \(\sigma =330.29\pi >0\) (see Fig. 6).
 Case (i) :

For \(h>c\): For the parameters \(a=1\), \(n=1\), \(m=0.4\), \(s=0.01\), \(r=0.02\), \(i=0.1\), \(p=0.5\), \(q=0.9\), \(K=100\), \(C=0.03\), \(m_{1}=0.1\), \(m_{2}=0.03\), the optimal singular solutions for different rates of μ are given in Table 2.Table 2
Optimal singular solution for different discount rate μ
μ
\(x_{(1)}^{*}\)
\(x_{(2)}^{*}\)
\(x_{(3)}^{*}\)
\(x_{(4)}^{*}\)
\(x_{(5)}^{*}\)
\(E_{(1)}^{*}\)
\(E_{(2)}^{*}\)
\(E_{(3)}^{*}\)
\(E_{(4)}^{*}\)
\(E_{(5)}^{*}\)
0.0
0.46
4.61
−0.011
−0.41
−90.12
1.51
4.34
255.88
3.04
1.579
0.01
0.51
2.86
−0.017
−0.40
−138.43
1.29
6.30
153.04
3.095
1.26
0.02
0.57
1.96
−0.023
−0.39
−187.6
1.07
44.27
105.35
3.15
1.05
 Case (ii) :

For \(h< c\): For the parameters \(a=1\), \(n=1\), \(m=0.4\), \(s=0.01\), \(r=0.02\), \(i=0.1\), \(p=0.5\), \(q=0.0009\), \(K=100\), \(C=0.03\), \(m_{1}=0.1\), \(m_{2}=0.03\), the optimal singular solutions for different rates of μ are given in Table 3.Table 3
Optimal singular solution for different discount rate μ
μ
\(x_{(1)}^{*}\)
\(x_{(2)}^{*}\)
\(x_{(3)}^{*}\)
\(x_{(4)}^{*}\)
\(x_{(5)}^{*}\)
\(E_{(1)}^{*}\)
\(E_{(2)}^{*}\)
\(E_{(3)}^{*}\)
\(E_{(4)}^{*}\)
\(E_{(5)}^{*}\)
0.0
0.84
89.59
0.023
Complex
Complex
3.59
−0.417
−250.61
Complex
Complex
0.01
0.305
43.73
0.019
−0.40
−3.85
4.59
−0.14
−268.88
2.44
0.58
0.02
0.25
10.86
−0.006
−0.26
−21.05
5.86
−0.42
501.69
3.75
0.125
 Case (iii) :

For \(h=c\): For the parameters \(a=1\), \(n=1\), \(m=1.04\), \(s=0.1\), \(r=0.02\), \(i=0.9\), \(p=0.5\), \(q=0.002\), \(K=100\), \(C=0.003\), \(m_{1}=0.1\), \(m_{2}=0.03\), the optimal singular solutions for different rates of μ are given in Table 4.Table 4
Optimal singular solution for different discount rate μ
μ
\(x_{(1)}^{*}\)
\(x_{(2)}^{*}\)
\(x_{(3)}^{*}\)
\(x_{(4)}^{*}\)
\(x_{(5)}^{*}\)
\(E_{(1)}^{*}\)
\(E_{(2)}^{*}\)
\(E_{(3)}^{*}\)
\(E_{(4)}^{*}\)
\(E_{(5)}^{*}\)
0.0
94.52
0.014
−104.04
−0.338
−0.143
0.062
−783.5
0.016
1.37
4.55
0.01
73.24
0.071
−132.78
−0.306
−0.222
0.099
12.64
0.012
1.56
2.41
0.02
57.57
0.112
−167.12
Complex
Complex
0.124
3.44
0.009
Complex
Complex
Note that \(y_{(j)}^{*}=x_{(j)}^{*}\), \(j=1,2,3,4,5\), since in each case \(n=1\).
7 Conclusions and discussions
In this paper, a mathematical model to study the dynamical behavior of a modified Leslie–Gower model with Holling typeIV functional response and nonlinear prey harvesting has been proposed and analyzed. The existence of equilibrium points and their stability analysis have been discussed with the help of stability theory. The proposed model system undergoes a Hopf bifurcation and a saddlenode bifurcation around the equilibrium point for the control parameter δ, the ratio of intrinsic growth rates of the predator and prey population and \(h=\frac{qE}{rm_{2}K}\), respectively.
We have discussed the bionomical equilibrium of the model and explain the optimal harvesting policy to be adopted by a regulatory agency. By constructing an appropriate Hamiltonian function and using Pontryagin’s maximum principle, the optimal harvesting policy has been discussed. We also found an optimal equilibrium solution. The effect of harvesting the prey, predator or both on the stability of the system depends on a pretty finetuned balancing of the parameter values and also on which functions/functional responses are chosen to represent the ecological harvesting policy [39]. We have established the stability of a limit cycle using the first Lyapunov number around the equilibrium point. A stable limit cycle seems to be possible only when the per capita consumption of prey by the predator is bounded by some maximum value, as with the nonlinear prey harvesting. Optimal singular equilibrium points have been obtained numerically for various discount rate in various cases. Therefore, at least one optimum singular equilibrium point in each from which \((x_{(1)}^{*}, y_{(1)}^{*}, E_{(1)}^{*})\) is feasible from an ecological point of view.
Declarations
Acknowledgements
This work was supported by Project of Support Program for Excellent Youth Talent in Colleges and Universities of Anhui Province (No. gxyqZD2018044) and Anhui Provincial Natural Science Foundation (No. 1608085QF151, No. 1608085QF145).
Authors’ contributions
The authors read and approved the final manuscript.
Competing interests
The authors declare that they have no competing interests.
Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
Authors’ Affiliations
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